Update check_response_functions.ipynb

call plt.show() such that readthedocs shows figures. figures are not shown in readthedocs otherwise because black formatting does not accept a semicolumn.
pastas · Jan 19, 2023 · ef922dc · ef922dc
1 parent eab10c9
commit ef922dc
Showing 1 changed file with 33 additions and 26 deletions.
diff --git a/doc/concepts/check_response_functions.ipynb b/doc/concepts/check_response_functions.ipynb
@@ -19,7 +19,7 @@
     "import numpy as np\n",
     "import matplotlib.pyplot as plt\n",
     "from scipy.integrate import quad\n",
-    "import pastas as ps"
+    "import pastas as ps\n"
    ]
   },
   {
@@ -37,7 +37,7 @@
    "metadata": {},
    "outputs": [],
    "source": [
-    "ps.Gamma.impulse"
+    "ps.Gamma.impulse\n"
    ]
   },
   {
@@ -59,7 +59,7 @@
     "step = gamma.step(p)\n",
     "stepnum = np.zeros(len(t))\n",
     "for i in range(1, len(t)):\n",
-    "    stepnum[i] = quad(gamma.impulse, 0, t[i], args=(p))[0]"
+    "    stepnum[i] = quad(gamma.impulse, 0, t[i], args=(p))[0]\n"
    ]
   },
   {
@@ -74,7 +74,8 @@
     "plt.xlabel(\"time (d)\")\n",
     "plt.ylabel(\"step (m)\")\n",
     "plt.grid()\n",
-    "plt.legend()"
+    "plt.legend()\n",
+    "plt.show()\n"
    ]
   },
   {
@@ -92,7 +93,7 @@
    "metadata": {},
    "outputs": [],
    "source": [
-    "ps.Exponential.impulse"
+    "ps.Exponential.impulse\n"
    ]
   },
   {
@@ -113,7 +114,7 @@
     "step = exponential.step(p)\n",
     "stepnum = np.zeros(len(t))\n",
     "for i in range(1, len(t)):\n",
-    "    stepnum[i] = quad(exponential.impulse, 0, t[i], args=(p))[0]"
+    "    stepnum[i] = quad(exponential.impulse, 0, t[i], args=(p))[0]\n"
    ]
   },
   {
@@ -128,7 +129,8 @@
     "plt.xlabel(\"time (d)\")\n",
     "plt.ylabel(\"step (m)\")\n",
     "plt.grid()\n",
-    "plt.legend()"
+    "plt.legend()\n",
+    "plt.show()\n"
    ]
   },
   {
@@ -146,7 +148,7 @@
    "metadata": {},
    "outputs": [],
    "source": [
-    "ps.Hantush.impulse"
+    "ps.Hantush.impulse\n"
    ]
   },
   {
@@ -168,7 +170,7 @@
     "step = hantush.step(p)\n",
     "stepnum = np.zeros(len(t))\n",
     "for i in range(1, len(t)):\n",
-    "    stepnum[i] = quad(hantush.impulse, 0, t[i], args=(p))[0]"
+    "    stepnum[i] = quad(hantush.impulse, 0, t[i], args=(p))[0]\n"
    ]
   },
   {
@@ -183,7 +185,8 @@
     "plt.xlabel(\"time (d)\")\n",
     "plt.ylabel(\"step (m)\")\n",
     "plt.grid()\n",
-    "plt.legend()"
+    "plt.legend()\n",
+    "plt.show()\n"
    ]
   },
   {
@@ -201,7 +204,7 @@
    "metadata": {},
    "outputs": [],
    "source": [
-    "ps.Polder.impulse"
+    "ps.Polder.impulse\n"
    ]
   },
   {
@@ -223,7 +226,7 @@
     "step = polder.step(p)\n",
     "stepnum = np.zeros(len(t))\n",
     "for i in range(1, len(t)):\n",
-    "    stepnum[i] = quad(polder.impulse, 0, t[i], args=(p))[0]"
+    "    stepnum[i] = quad(polder.impulse, 0, t[i], args=(p))[0]\n"
    ]
   },
   {
@@ -238,7 +241,8 @@
     "plt.xlabel(\"time (d)\")\n",
     "plt.ylabel(\"step (m)\")\n",
     "plt.grid()\n",
-    "plt.legend()"
+    "plt.legend()\n",
+    "plt.show()\n"
    ]
   },
   {
@@ -256,7 +260,7 @@
    "metadata": {},
    "outputs": [],
    "source": [
-    "ps.FourParam.impulse"
+    "ps.FourParam.impulse\n"
    ]
   },
   {
@@ -270,7 +274,7 @@
     "n = 1.5\n",
     "a = 50\n",
     "b = 10\n",
-    "p = [A, n, a, b]\n",
+    "p = [n, a, b]\n",
     "\n",
     "fourparam = ps.FourParam(quad=False)  # use simple integration\n",
     "tmax = fourparam.get_tmax(p)\n",
@@ -282,7 +286,7 @@
     "    stepnum[i] = quad(fourparam.impulse, 0, t[i], args=(p))[0]\n",
     "stepnum = (\n",
     "    stepnum / quad(fourparam.impulse, 0, np.inf, args=p)[0]\n",
-    ")  # four param is scaled at the end"
+    ")  # four param is scaled at the end\n"
    ]
   },
   {
@@ -297,7 +301,8 @@
     "plt.xlabel(\"time (d)\")\n",
     "plt.ylabel(\"step (m)\")\n",
     "plt.grid()\n",
-    "plt.legend()"
+    "plt.legend()\n",
+    "plt.show()\n"
    ]
   },
   {
@@ -315,7 +320,7 @@
    "metadata": {},
    "outputs": [],
    "source": [
-    "ps.DoubleExponential.impulse"
+    "ps.DoubleExponential.impulse\n"
    ]
   },
   {
@@ -338,7 +343,7 @@
     "step = doubexp.step(p)\n",
     "stepnum = np.zeros(len(t))\n",
     "for i in range(1, len(t)):\n",
-    "    stepnum[i] = quad(doubexp.impulse, 0, t[i], args=(p))[0]"
+    "    stepnum[i] = quad(doubexp.impulse, 0, t[i], args=(p))[0]\n"
    ]
   },
   {
@@ -353,7 +358,8 @@
     "plt.xlabel(\"time (d)\")\n",
     "plt.ylabel(\"step (m)\")\n",
     "plt.grid()\n",
-    "plt.legend()"
+    "plt.legend()\n",
+    "plt.show()\n"
    ]
   },
   {
@@ -371,7 +377,7 @@
    "metadata": {},
    "outputs": [],
    "source": [
-    "# ps.Edelman.impulse"
+    "# ps.Edelman.impulse\n"
    ]
   },
   {
@@ -391,7 +397,7 @@
     "# #step = edel.step(p)\n",
     "# stepnum = np.zeros(len(t))\n",
     "# for i in range(1, len(t)):\n",
-    "#     stepnum[i] = quad(edel.impulse, 1e-3, t[i], args=(p))[0]"
+    "#     stepnum[i] = quad(edel.impulse, 1e-3, t[i], args=(p))[0]\n"
    ]
   },
   {
@@ -406,7 +412,7 @@
     "# plt.xlabel(\"time (d)\")\n",
     "# plt.ylabel(\"step (m)\")\n",
     "# plt.grid()\n",
-    "# plt.legend();"
+    "# plt.legend();\n"
    ]
   },
   {
@@ -493,7 +499,7 @@
    "metadata": {},
    "outputs": [],
    "source": [
-    "ps.Kraijenhoff.impulse"
+    "ps.Kraijenhoff.impulse\n"
    ]
   },
   {
@@ -516,7 +522,7 @@
     "stepnum_brug = np.zeros(len(t))\n",
     "\n",
     "for i in range(1, len(t)):\n",
-    "    stepnum_brug[i] = quad(khoff.impulse, 0, t[i], args=(p))[0]"
+    "    stepnum_brug[i] = quad(khoff.impulse, 0, t[i], args=(p))[0]\n"
    ]
   },
   {
@@ -531,7 +537,8 @@
     "plt.xlabel(\"time (d)\")\n",
     "plt.ylabel(\"step (m)\")\n",
     "plt.grid()\n",
-    "plt.legend()"
+    "plt.legend()\n",
+    "plt.show()\n"
    ]
   }
  ],