pyoculus 0.1.1
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Class that used to setup the cylindrical bfield problem used in ODE solver. More...
Public Member Functions | |
__init__ (self, R0, Z0, Nfp=1) | |
Set up the problem. | |
f_RZ (self, phi, RZ, *args) | |
Returns ODE RHS. | |
Public Member Functions inherited from pyoculus.problems.cylindrical_problem.CylindricalProblem | |
f_RZ_tangent (self, phi, RZ, *args) | |
Returns ODE RHS, with tangent. | |
f (self, zeta, y, *args) | |
Returns ODE RHS. | |
f_tangent (self, zeta, y, *args) | |
Returns ODE RHS. | |
set_axis (self, R0, Z0) | |
Set the axis. | |
Public Member Functions inherited from pyoculus.problems.base_problem.BaseProblem | |
convert_coords (self, coord1) | |
Converts coordinates (for example \(s,\theta,\zeta\) to \(R,Z,\varphi\)) | |
Public Member Functions inherited from pyoculus.problems.bfield_problem.BfieldProblem | |
B (self, coords, *args) | |
Returns magnetic fields. | |
dBdX (self, coords, *args) | |
Returns magnetic fields. | |
B_many (self, x1arr, x2arr, x3arr, input1D=True, *args) | |
Returns magnetic fields, with multipy coordinate inputs. | |
dBdX_many (self, x1arr, x2arr, x3arr, input1D=True, *args) | |
Returns magnetic fields. | |
Additional Inherited Members | |
Public Attributes inherited from pyoculus.problems.cylindrical_problem.CylindricalProblem | |
int | problem_size = 2 |
str | poincare_plot_type = "RZ" |
str | poincare_plot_xlabel = "R(m)" |
str | poincare_plot_ylabel = "Z(m)" |
Nfp = Nfp | |
Public Attributes inherited from pyoculus.problems.base_problem.BaseProblem | |
int | problem_size = 2 |
str | poincare_plot_type = "yx" |
str | poincare_plot_xlabel = "y" |
str | poincare_plot_ylabel = "x" |
Public Attributes inherited from pyoculus.problems.bfield_problem.BfieldProblem | |
bool | has_jacobian = False |
if the output magnetic field contains the jacobian factor or not | |
Protected Attributes inherited from pyoculus.problems.cylindrical_problem.CylindricalProblem | |
_R0 = R0 | |
_Z0 = Z0 | |
Class that used to setup the cylindrical bfield problem used in ODE solver.
The system of ODEs is given by
\[ \frac{dR}{d\phi} = \frac{B^{R}}{B^{\phi}} \]
\[ \frac{dZ}{d\phi} = \frac{B^{Z}}{B^{\phi}} \]
pyoculus.problems.cylindrical_bfield.CylindricalBfield.__init__ | ( | self, | |
R0, | |||
Z0, | |||
Nfp = 1 ) |
Set up the problem.
R0 | the R coordinate of the magnetic axis |
Z0 | the Z coordinate of the magnetic axis |
Reimplemented from pyoculus.problems.cylindrical_problem.CylindricalProblem.
Reimplemented in pyoculus.problems.m3dc1_bfield.M3DC1Bfield.
pyoculus.problems.cylindrical_bfield.CylindricalBfield.f_RZ | ( | self, | |
phi, | |||
RZ, | |||
* | args ) |
Returns ODE RHS.
phi | cylindrical angle in ODE |
RZ | \((R, Z)\) in ODE |
*args | parameter for the ODE |
Reimplemented from pyoculus.problems.cylindrical_problem.CylindricalProblem.