-
Notifications
You must be signed in to change notification settings - Fork 47
Commit
This commit does not belong to any branch on this repository, and may belong to a fork outside of the repository.
Merge pull request #19 from bendudson/coils
MultiCoil and ShapedCoil types
- Loading branch information
Showing
12 changed files
with
1,179 additions
and
226 deletions.
There are no files selected for viewing
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,255 @@ | ||
""" | ||
Poloidal field coil | ||
Used in machine to define coils. Can also be a base class for other coil types. | ||
License | ||
------- | ||
Copyright 2016-2019 Ben Dudson, University of York. Email: benjamin.dudson@york.ac.uk | ||
This file is part of FreeGS. | ||
FreeGS is free software: you can redistribute it and/or modify | ||
it under the terms of the GNU Lesser General Public License as published by | ||
the Free Software Foundation, either version 3 of the License, or | ||
(at your option) any later version. | ||
FreeGS is distributed in the hope that it will be useful, | ||
but WITHOUT ANY WARRANTY; without even the implied warranty of | ||
MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the | ||
GNU Lesser General Public License for more details. | ||
You should have received a copy of the GNU Lesser General Public License | ||
along with FreeGS. If not, see <http://www.gnu.org/licenses/>. | ||
""" | ||
|
||
from .gradshafranov import Greens, GreensBr, GreensBz, mu0 | ||
import numpy as np | ||
import numbers | ||
|
||
class AreaCurrentLimit: | ||
""" | ||
Calculate the coil area based on a fixed current density limit | ||
""" | ||
def __init__(self, current_density = 3.5e9): | ||
""" | ||
current_density - Maximum current density in A/m^2 | ||
Limits in general depend on the magnetic field | ||
Typical values Nb3Sn ~ 3.5e9 A/m^2 | ||
https://doi.org/10.1016/0167-899X(86)90010-8 | ||
""" | ||
self._current_density = current_density | ||
|
||
def __call__(self, coil): | ||
""" | ||
Return the area in m^2, given a Coil object | ||
""" | ||
return abs(coil.current * coil.turns) / self._current_density | ||
|
||
class Coil: | ||
""" | ||
Represents a poloidal field coil | ||
public members | ||
-------------- | ||
R, Z - Location of the coil | ||
current - current in the coil in Amps | ||
turns - Number of turns | ||
control - enable or disable control system | ||
area - Cross-section area in m^2 | ||
The total toroidal current carried by the coil is current * turns | ||
""" | ||
|
||
# A dtype for converting to Numpy array and storing in HDF5 files | ||
dtype = np.dtype([ | ||
(str("R"), np.float64), | ||
(str("Z"), np.float64), | ||
(str("current"), np.float64), | ||
(str("turns"), np.int), | ||
(str("control"), np.bool), | ||
]) | ||
|
||
def __init__(self, R, Z, current=0.0, turns=1, control=True, area=AreaCurrentLimit()): | ||
""" | ||
R, Z - Location of the coil | ||
current - current in each turn of the coil in Amps | ||
turns - Number of turns. Total coil current is current * turns | ||
control - enable or disable control system | ||
area - Cross-section area in m^2 | ||
Area can be a fixed value (e.g. 0.025 for 5x5cm coil), or can be specified | ||
using a function which takes a coil as an input argument. | ||
To specify a current density limit, use: | ||
area = AreaCurrentLimit(current_density) | ||
where current_density is in A/m^2. The area of the coil will be recalculated | ||
as the coil current is changed. | ||
The most important effect of the area is on the coil self-force: | ||
The smaller the area the larger the hoop force for a given current. | ||
""" | ||
self.R = R | ||
self.Z = Z | ||
|
||
self.current = current | ||
self.turns = turns | ||
self.control = control | ||
self.area = area | ||
|
||
def psi(self, R, Z): | ||
""" | ||
Calculate poloidal flux at (R,Z) | ||
""" | ||
return self.controlPsi(R,Z) * self.current | ||
|
||
def createPsiGreens(self, R, Z): | ||
""" | ||
Calculate the Greens function at every point, and return | ||
array. This will be passed back to evaluate Psi in | ||
calcPsiFromGreens() | ||
""" | ||
return self.controlPsi(R,Z) | ||
|
||
def calcPsiFromGreens(self, pgreen): | ||
""" | ||
Calculate plasma psi from Greens functions and current | ||
""" | ||
return self.current * pgreen | ||
|
||
def Br(self, R, Z): | ||
""" | ||
Calculate radial magnetic field Br at (R,Z) | ||
""" | ||
return self.controlBr(R,Z) * self.current | ||
|
||
def Bz(self, R, Z): | ||
""" | ||
Calculate vertical magnetic field Bz at (R,Z) | ||
""" | ||
return self.controlBz(R,Z) * self.current | ||
|
||
def controlPsi(self, R, Z): | ||
""" | ||
Calculate poloidal flux at (R,Z) due to a unit current | ||
""" | ||
return Greens(self.R, self.Z, R, Z) * self.turns | ||
|
||
def controlBr(self, R, Z): | ||
""" | ||
Calculate radial magnetic field Br at (R,Z) due to a unit current | ||
""" | ||
return GreensBr(self.R,self.Z, R, Z) * self.turns | ||
|
||
def controlBz(self, R, Z): | ||
""" | ||
Calculate vertical magnetic field Bz at (R,Z) due to a unit current | ||
""" | ||
return GreensBz(self.R,self.Z, R, Z) * self.turns | ||
|
||
def getForces(self, equilibrium): | ||
""" | ||
Calculate forces on the coils in Newtons | ||
Returns an array of two elements: [ Fr, Fz ] | ||
Force on coil due to its own current: | ||
Lorentz self‐forces on curved current loops | ||
Physics of Plasmas 1, 3425 (1998); https://doi.org/10.1063/1.870491 | ||
David A. Garren and James Chen | ||
""" | ||
current = self.current # current per turn | ||
total_current = current * self.turns # Total toroidal current | ||
|
||
# Calculate field at this coil due to all other coils | ||
# and plasma. Need to zero this coil's current | ||
self.current = 0.0 | ||
Br = equilibrium.Br(self.R, self.Z) | ||
Bz = equilibrium.Bz(self.R, self.Z) | ||
self.current = current | ||
|
||
# Assume circular cross-section for hoop (self) force | ||
minor_radius = np.sqrt(self.area / np.pi) | ||
|
||
# Self inductance factor, depending on internal current | ||
# distribution. 0.5 for uniform current, 0 for surface current | ||
self_inductance = 0.5 | ||
|
||
# Force per unit length. | ||
# In cgs units f = I^2/(c^2 * R) * (ln(8*R/a) - 1 + xi/2) | ||
# In SI units f = mu0 * I^2 / (4*pi*R) * (ln(8*R/a) - 1 + xi/2) | ||
self_fr = (mu0 * total_current**2 / (4.*np.pi*self.R)) * (np.log(8.*self.R/minor_radius) - 1 + self_inductance/2.) | ||
|
||
Ltor = 2*np.pi*self.R # Length of coil | ||
return np.array([ (total_current * Bz + self_fr) * Ltor, # Jphi x Bz = Fr, self force always outwards | ||
-total_current * Br * Ltor]) # Jphi x Br = - Fz | ||
|
||
def __repr__(self): | ||
return ("Coil(R={0}, Z={1}, current={2:.1f}, turns={3}, control={4})" | ||
.format(self.R, self.Z, self.current, self.turns, self.control)) | ||
|
||
def __eq__(self, other): | ||
return (self.R == other.R | ||
and self.Z == other.Z | ||
and self.current == other.current | ||
and self.turns == other.turns | ||
and self.control == other.control) | ||
|
||
def __ne__(self, other): | ||
return not self == other | ||
|
||
def to_numpy_array(self): | ||
""" | ||
Helper method for writing output | ||
""" | ||
return np.array((self.R, self.Z, self.current, self.turns, self.control), | ||
dtype=self.dtype) | ||
|
||
@classmethod | ||
def from_numpy_array(cls, value): | ||
if value.dtype != cls.dtype: | ||
raise ValueError("Can't create {this} from dtype: {got} (expected: {dtype})" | ||
.format(this=type(cls), got=value.dtype, dtype=cls.dtype)) | ||
return Coil(*value[()]) | ||
|
||
@property | ||
def area(self): | ||
""" | ||
The cross-section area of the coil in m^2 | ||
""" | ||
if isinstance(self._area, numbers.Number): | ||
assert self._area > 0 | ||
return self._area | ||
# Calculate using functor | ||
area = self._area(self) | ||
assert area > 0 | ||
return area | ||
|
||
@area.setter | ||
def area(self, area): | ||
self._area = area | ||
|
||
def plot(self, axis=None, show=False): | ||
""" | ||
Plot the coil location, using axis if given | ||
The area of the coil is used to set the radius | ||
""" | ||
minor_radius = np.sqrt(self.area / np.pi) | ||
|
||
import matplotlib.pyplot as plt | ||
|
||
if axis is None: | ||
fig = plt.figure() | ||
axis = fig.add_subplot(111) | ||
|
||
circle = plt.Circle((self.R, self.Z), minor_radius, color='b') | ||
axis.add_artist(circle) | ||
return axis |
Oops, something went wrong.