From d5c099deb3ccf39e92e83a49024bdde61ca7ef4a Mon Sep 17 00:00:00 2001
From: Jon Doe <cgeuzaine@uliege.be>
Date: Sun, 1 Apr 2018 10:07:50 +0200
Subject: [PATCH] pp
---
Magnetodynamics/Lib_MagStaDyn_av_2D_Cir.pro | 545 --------------------
1 file changed, 545 deletions(-)
delete mode 100644 Magnetodynamics/Lib_MagStaDyn_av_2D_Cir.pro
diff --git a/Magnetodynamics/Lib_MagStaDyn_av_2D_Cir.pro b/Magnetodynamics/Lib_MagStaDyn_av_2D_Cir.pro
deleted file mode 100644
index aedde5b..0000000
--- a/Magnetodynamics/Lib_MagStaDyn_av_2D_Cir.pro
+++ /dev/null
@@ -1,545 +0,0 @@
-// This is a template .pro file containing a general formulation for 2D
-// magnetostatic and magnetodynamic problems in terms of the magnetic vector
-// potential a (potentially coupled with the electric scalar potential v), with
-// optional circuit coupling.
-
-// Below are definitions of the constants (inside "DefineConstant"), groups
-// (inside "DefineGroup") and functions (inside "DefineFunction") that can be
-// redefined from outside this template.
-
-DefineConstant[
- Flag_FrequencyDomain = 1, // frequency-domain or time-domain simulation
- Flag_CircuitCoupling = 0, // consider coupling with external electric circuit
- Flag_NewtonRaphson = 1, // Newton-Raphson or Picard method for nonlinear iterations
- CoefPower = 0.5, // coefficient for power calculations
- Freq = 50, // frequency (for harmonic simulations)
- TimeInit = 0, // intial time (for time-domain simulations)
- TimeFinal = 1/50, // final time (for time-domain simulations)
- DeltaTime = 1/500, // time step (for time-domain simulations)
- FE_Order = 1, // finite element order
- Val_Rint = 0, // interior radius of annulus shell transformation region (Vol_Inf_Mag)
- Val_Rext = 0 // exterior radius of annulus shell transformation region (Vol_Inf_Mag)
- NL_tol_abs = 1e-6, // absolute tolerance on residual for noninear iterations
- NL_tol_rel = 1e-6, // relative tolerance on residual for noninear iterations
- NL_iter_max = 20 // maximum number of noninear iterations
-];
-
-Group {
- DefineGroup[
- // The full magnetic domain:
- Vol_Mag,
-
- // Subsets of Vol_Mag:
- Vol_C_Mag, // massive conductors
- Vol_S0_Mag, // stranded conductors with imposed current densities js0
- Vol_S_Mag, // stranded conductors with imposed current, voltage or circuit coupling
- Vol_NL_Mag, // nonlinear magnetic materials
- Vol_V_Mag, // moving massive conducting parts (with invariant mesh)
- Vol_M_Mag, // permanent magnets
- Vol_Inf_Mag, // annulus where a infinite shell transformation is applied
-
- // Boundaries:
- Sur_FluxTube_Mag, // boundary with Neumann BC
- Sur_Perfect_Mag, // boundary of perfect conductors (non-meshed)
- Sur_Imped_Mag // boundary of conductors approximated by a surface impedance
- // (non-meshed)
- ];
- If(Flag_CircuitCoupling)
- DefineGroup[
- SourceV_Cir, // voltage sources
- SourceI_Cir, // current sources
- Resistance_Cir, // resistors (linear)
- Inductance_Cir, // inductors
- Capacitance_Cir, // capacitors
- Diode_Cir // diodes (treated as nonlinear resistors)
- ];
- EndIf
-}
-
-Function {
- DefineFunction[
- nu, // reluctivity (in Vol_Mag)
- sigma, // conductivity (in Vol_C_Mag and Vol_S_Mag)
- br, // remanent magnetic flux density (in Vol_M_Mag)
- js0, // source current density (in Vol_S0_Mag)
- dhdb, // Jacobian for Newton-Raphson method (in Vol_NL_Mag)
- nxh, // n x magnetic field (on Sur_FluxTube_Mag)
- Velocity, // velocity of moving part (in Vol_V_Mag)
- Ns, // number of turns (in Vol_S_Mag)
- Sc, // cross-section of windings (in Vol_S_Mag)
- CoefGeos, // geometrical coefficient for 2D or 2D axi model (in Vol_Mag)
- Ysur // surface admittance (on Sur_Imped_Mag)
- ];
- If(Flag_CircuitCoupling)
- DefineFunction[
- Resistance, // resistance values
- Inductance, // inductance values
- Capacitance // capacitance values
- ];
- EndIf
-}
-
-// End of definitions.
-
-Group{
- // all linear materials
- Vol_L_Mag = Region[ {Vol_Mag, -Vol_NL_Mag} ];
- // all volumes + surfaces on which integrals will be computed
- Dom_Mag = Region[ {Vol_Mag, Sur_FluxTube_Mag, Sur_Perfect_Mag, Sur_Imped_Mag} ];
- If(Flag_CircuitCoupling)
- // all circuit impedances
- DomainZ_Cir = Region[ {Resistance_Cir, Inductance_Cir, Capacitance_Cir} ];
- // all circuit sources
- DomainSource_Cir = Region[ {SourceV_Cir, SourceI_Cir} ];
- // all circuit elements
- Domain_Cir = Region[ {DomainZ_Cir, DomainSource_Cir} ];
- EndIf
-}
-
-Jacobian {
- { Name Vol;
- Case {
- { Region Vol_Inf_Mag ;
- Jacobian VolSphShell {Val_Rint, Val_Rext} ; }
- { Region All; Jacobian Vol; }
- }
- }
- { Name Sur;
- Case {
- { Region All; Jacobian Sur; }
- }
- }
-}
-
-Integration {
- { Name Gauss_v;
- Case {
- { Type Gauss;
- Case {
- { GeoElement Point; NumberOfPoints 1; }
- { GeoElement Line; NumberOfPoints 5; }
- { GeoElement Triangle; NumberOfPoints 7; }
- { GeoElement Quadrangle; NumberOfPoints 4; }
- { GeoElement Tetrahedron; NumberOfPoints 15; }
- { GeoElement Hexahedron; NumberOfPoints 14; }
- { GeoElement Prism; NumberOfPoints 21; }
- }
- }
- }
- }
-}
-
-// Same FunctionSpace for both static and dynamic formulations
-FunctionSpace {
- { Name Hcurl_a_2D; Type Form1P; // 1-form (circulations) on edges
- // perpendicular to the plane of study
- BasisFunction {
- // \vec{a}(x) = \sum_{n \in N(Domain)} a_n \vec{s}_n(x)
- // without nodes on perfect conductors (where a is constant)
- { Name s_n; NameOfCoef a_n; Function BF_PerpendicularEdge;
- Support Dom_Mag; Entity NodesOf[All, Not Sur_Perfect_Mag]; }
-
- // global basis function on boundary of perfect conductors
- { Name s_skin; NameOfCoef a_skin; Function BF_GroupOfPerpendicularEdges;
- Support Dom_Mag; Entity GroupsOfNodesOf[Sur_Perfect_Mag]; }
-
- // additional basis functions for 2nd order interpolation
- If(FE_Order == 2)
- { Name s_e; NameOfCoef a_e; Function BF_PerpendicularEdge_2E;
- Support Vol_Mag; Entity EdgesOf[All]; }
- EndIf
- }
- GlobalQuantity {
- { Name A; Type AliasOf; NameOfCoef a_skin; }
- { Name I; Type AssociatedWith; NameOfCoef a_skin; }
- }
- Constraint {
- { NameOfCoef a_n;
- EntityType NodesOf; NameOfConstraint MagneticVectorPotential_2D; }
-
- { NameOfCoef I;
- EntityType GroupsOfNodesOf; NameOfConstraint Current_2D; }
-
- If(FE_Order == 2)
- { NameOfCoef a_e;
- EntityType EdgesOf; NameOfConstraint MagneticVectorPotential_2D_0; }
- EndIf
- }
- }
-}
-
-FunctionSpace {
- // Gradient of Electric scalar potential (2D)
- { Name Hregion_u_2D; Type Form1P; // same as for \vec{a}
- BasisFunction {
- { Name sr; NameOfCoef ur; Function BF_RegionZ;
- // constant vector (over the region) with nonzero z-component only
- Support Region[{Vol_C_Mag, Sur_Imped_Mag}];
- Entity Region[{Vol_C_Mag, Sur_Imped_Mag}]; }
- }
- GlobalQuantity {
- { Name U; Type AliasOf; NameOfCoef ur; }
- { Name I; Type AssociatedWith; NameOfCoef ur; }
- }
- Constraint {
- { NameOfCoef U;
- EntityType Region; NameOfConstraint Voltage_2D; }
- { NameOfCoef I;
- EntityType Region; NameOfConstraint Current_2D; }
- }
- }
-
- // Current in stranded coil (2D)
- { Name Hregion_i_2D; Type Vector;
- BasisFunction {
- { Name sr; NameOfCoef ir; Function BF_RegionZ;
- Support Vol_S_Mag; Entity Vol_S_Mag; }
- }
- GlobalQuantity {
- { Name Is; Type AliasOf; NameOfCoef ir; }
- { Name Us; Type AssociatedWith; NameOfCoef ir; }
- }
- Constraint {
- { NameOfCoef Us;
- EntityType Region; NameOfConstraint Voltage_2D; }
- { NameOfCoef Is;
- EntityType Region; NameOfConstraint Current_2D; }
- }
- }
-}
-
-If(Flag_CircuitCoupling)
- // UZ and IZ for impedances
- FunctionSpace {
- { Name Hregion_Z; Type Scalar;
- BasisFunction {
- { Name sr; NameOfCoef ir; Function BF_Region;
- Support Domain_Cir; Entity Domain_Cir; }
- }
- GlobalQuantity {
- { Name Iz; Type AliasOf; NameOfCoef ir; }
- { Name Uz; Type AssociatedWith; NameOfCoef ir; }
- }
- Constraint {
- { NameOfCoef Uz;
- EntityType Region; NameOfConstraint Voltage_Cir; }
- { NameOfCoef Iz;
- EntityType Region; NameOfConstraint Current_Cir; }
- }
- }
- }
-EndIf
-
-
-// Static Formulation
-Formulation {
- { Name MagSta_a_2D; Type FemEquation;
- Quantity {
- { Name a; Type Local; NameOfSpace Hcurl_a_2D; }
- { Name ir; Type Local; NameOfSpace Hregion_i_2D; }
- }
- Equation {
- Integral { [ nu[] * Dof{d a} , {d a} ];
- In Vol_L_Mag; Jacobian Vol; Integration Gauss_v; }
-
- If(Flag_NewtonRaphson)
- Integral { [ nu[{d a}] * {d a} , {d a} ];
- In Vol_NL_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ dhdb[{d a}] * Dof{d a} , {d a} ];
- In Vol_NL_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ - dhdb[{d a}] * {d a} , {d a} ];
- In Vol_NL_Mag; Jacobian Vol; Integration Gauss_v; }
- Else
- Integral { [ nu[{d a}] * Dof{d a}, {d a} ];
- In Vol_NL_Mag; Jacobian Vol; Integration Gauss_v; }
- EndIf
-
- Integral { [ - nu[] * br[] , {d a} ];
- In Vol_M_Mag; Jacobian Vol; Integration Gauss_v; }
-
- Integral { [ - js0[] , {a} ];
- In Vol_S0_Mag; Jacobian Vol; Integration Gauss_v; }
-
- Integral { [ - (js0[]*Vector[0,0,1]) * Dof{ir} , {a} ];
- In Vol_S_Mag; Jacobian Vol; Integration Gauss_v; }
-
- Integral { [ nxh[] , {a} ];
- In Sur_FluxTube_Mag; Jacobian Sur; Integration Gauss_v; }
- }
- }
-}
-
-// Dynamic Formulation (eddy currents)
-Formulation {
- { Name MagDyn_a_2D; Type FemEquation;
- Quantity {
- { Name a; Type Local; NameOfSpace Hcurl_a_2D; }
- { Name A_floating; Type Global; NameOfSpace Hcurl_a_2D [A]; }
- { Name I_perfect; Type Global; NameOfSpace Hcurl_a_2D [I]; }
-
- { Name ur; Type Local; NameOfSpace Hregion_u_2D; }
- { Name I; Type Global; NameOfSpace Hregion_u_2D [I]; }
- { Name U; Type Global; NameOfSpace Hregion_u_2D [U]; }
-
- { Name ir; Type Local; NameOfSpace Hregion_i_2D; }
- { Name Us; Type Global; NameOfSpace Hregion_i_2D [Us]; }
- { Name Is; Type Global; NameOfSpace Hregion_i_2D [Is]; }
-
- If(Flag_CircuitCoupling)
- { Name Uz; Type Global; NameOfSpace Hregion_Z [Uz]; }
- { Name Iz; Type Global; NameOfSpace Hregion_Z [Iz]; }
- EndIf
- }
- Equation {
- Integral { [ nu[] * Dof{d a} , {d a} ];
- In Vol_L_Mag; Jacobian Vol; Integration Gauss_v; }
-
- If(Flag_NewtonRaphson)
- Integral { [ nu[{d a}] * {d a} , {d a} ];
- In Vol_NL_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ dhdb[{d a}] * Dof{d a} , {d a} ];
- In Vol_NL_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ - dhdb[{d a}] * {d a} , {d a} ];
- In Vol_NL_Mag; Jacobian Vol; Integration Gauss_v; }
- Else
- Integral { [ nu[{d a}] * Dof{d a}, {d a} ];
- In Vol_NL_Mag; Jacobian Vol; Integration Gauss_v; }
- EndIf
-
- Integral { [ - nu[] * br[] , {d a} ];
- In Vol_M_Mag; Jacobian Vol; Integration Gauss_v; }
-
- // Electric field e = -Dt[{a}]-{ur},
- // with {ur} = Grad v constant in each region of Vol_C_Mag
- Integral { DtDof [ sigma[] * Dof{a} , {a} ];
- In Vol_C_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ sigma[] * Dof{ur} / CoefGeos[] , {a} ];
- In Vol_C_Mag; Jacobian Vol; Integration Gauss_v; }
-
- Integral { [ - sigma[] * (Velocity[] /\ Dof{d a}) , {a} ];
- In Vol_V_Mag; Jacobian Vol; Integration Gauss_v; }
-
- Integral { [ - js0[] , {a} ];
- In Vol_S0_Mag; Jacobian Vol; Integration Gauss_v; }
-
- Integral { [ nxh[] , {a} ];
- In Sur_FluxTube_Mag; Jacobian Sur; Integration Gauss_v; }
-
- Integral { DtDof [ Ysur[] * Dof{a} , {a} ];
- In Sur_Imped_Mag; Jacobian Sur; Integration Gauss_v; }
- Integral { [ Ysur[] * Dof{ur} / CoefGeos[] , {a} ];
- In Sur_Imped_Mag; Jacobian Sur; Integration Gauss_v; }
-
- // When {ur} act as a test function, one obtains the circuits relations,
- // relating the voltage and the current of each region in Vol_C_Mag
- Integral { DtDof [ sigma[] * Dof{a} , {ur} ];
- In Vol_C_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ sigma[] * Dof{ur} / CoefGeos[] , {ur} ];
- In Vol_C_Mag; Jacobian Vol; Integration Gauss_v; }
- GlobalTerm { [ Dof{I} *(CoefGeos[]/Fabs[CoefGeos[]]) , {U} ]; In Vol_C_Mag; }
-
- Integral { DtDof [ Ysur[] * Dof{a} , {ur} ];
- In Sur_Imped_Mag; Jacobian Sur; Integration Gauss_v; }
- Integral { [ Ysur[] * Dof{ur} / CoefGeos[] , {ur} ];
- In Sur_Imped_Mag; Jacobian Sur; Integration Gauss_v; }
- GlobalTerm { [ Dof{I} *(CoefGeos[]/Fabs[CoefGeos[]]) , {U} ]; In Sur_Imped_Mag; }
-
- // js[0] should be of the form: Ns[]/Sc[] * Vector[0,0,1]
- Integral { [ - (js0[]*Vector[0,0,1]) * Dof{ir} , {a} ];
- In Vol_S_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { DtDof [ Ns[]/Sc[] * Dof{a} , {ir} ];
- In Vol_S_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ Ns[]/Sc[] / sigma[] * (js0[]*Vector[0,0,1]) * Dof{ir} , {ir} ];
- In Vol_S_Mag; Jacobian Vol; Integration Gauss_v; }
- GlobalTerm { [ Dof{Us} / CoefGeos[] , {Is} ]; In Vol_S_Mag; }
- // Attention: CoefGeo[.] = 2*Pi for Axi
-
- GlobalTerm { [ - Dof{I_perfect} , {A_floating} ]; In Sur_Perfect_Mag; }
-
- If(Flag_CircuitCoupling)
- GlobalTerm { NeverDt[ Dof{Uz} , {Iz} ]; In Resistance_Cir; }
- GlobalTerm { NeverDt[ Resistance[] * Dof{Iz} , {Iz} ]; In Resistance_Cir; }
-
- GlobalTerm { [ Dof{Uz} , {Iz} ]; In Inductance_Cir; }
- GlobalTerm { DtDof [ Inductance[] * Dof{Iz} , {Iz} ]; In Inductance_Cir; }
-
- GlobalTerm { NeverDt[ Dof{Iz} , {Iz} ]; In Capacitance_Cir; }
- GlobalTerm { DtDof [ Capacitance[] * Dof{Uz} , {Iz} ]; In Capacitance_Cir; }
-
- GlobalTerm { NeverDt[ Dof{Uz} , {Iz} ]; In Diode_Cir; }
- GlobalTerm { NeverDt[ Resistance[{Uz}] * Dof{Iz} , {Iz} ]; In Diode_Cir; }
-
- GlobalTerm { [ 0. * Dof{Iz} , {Iz} ]; In DomainSource_Cir; }
-
- GlobalEquation {
- Type Network; NameOfConstraint ElectricalCircuit;
- { Node {I}; Loop {U}; Equation {I}; In Vol_C_Mag; }
- { Node {Is}; Loop {Us}; Equation {Us}; In Vol_S_Mag; }
- { Node {Iz}; Loop {Uz}; Equation {Uz}; In Domain_Cir; }
- }
- EndIf
-
- }
- }
-}
-
-Resolution {
- { Name MagDyn_a_2D;
- System {
- { Name Sys; NameOfFormulation MagDyn_a_2D;
- If(Flag_FrequencyDomain)
- Type ComplexValue; Frequency Freq;
- EndIf
- }
- }
- Operation {
- If(Flag_FrequencyDomain)
- Generate[Sys]; Solve[Sys]; SaveSolution[Sys];
- Else
- InitSolution[Sys]; // provide initial condition
- TimeLoopTheta[TimeInit, TimeFinal, DeltaTime, 1.]{
- // Euler implicit (1) -- Crank-Nicolson (0.5)
- Generate[Sys]; Solve[Sys];
- If(NbrRegions[Vol_NL_Mag])
- Generate[Sys]; GetResidual[Sys, $res0];
- Evaluate[ $res = $res0, $iter = 0 ];
- Print[{$iter, $res, $res / $res0},
- Format "Residual %03g: abs %14.12e rel %14.12e"];
- While[$res > NL_tol_abs && $res / $res0 > NL_tol_rel &&
- $res / $res0 <= 1 && $iter < NL_iter_max]{
- Solve[Sys]; Generate[Sys]; GetResidual[Sys, $res];
- Evaluate[ $iter = $iter + 1 ];
- Print[{$iter, $res, $res / $res0},
- Format "Residual %03g: abs %14.12e rel %14.12e"];
- }
- EndIf
- SaveSolution[Sys];
- }
- EndIf
- }
- }
- { Name MagSta_a_2D;
- System {
- { Name Sys; NameOfFormulation MagSta_a_2D; }
- }
- Operation {
- InitSolution[Sys];
- Generate[Sys]; Solve[Sys];
- If(NbrRegions[Vol_NL_Mag])
- Generate[Sys]; GetResidual[Sys, $res0];
- Evaluate[ $res = $res0, $iter = 0 ];
- Print[{$iter, $res, $res / $res0},
- Format "Residual %03g: abs %14.12e rel %14.12e"];
- While[$res > NL_tol_abs && $res / $res0 > NL_tol_rel &&
- $res / $res0 <= 1 && $iter < NL_iter_max]{
- Solve[Sys]; Generate[Sys]; GetResidual[Sys, $res];
- Evaluate[ $iter = $iter + 1 ];
- Print[{$iter, $res, $res / $res0},
- Format "Residual %03g: abs %14.12e rel %14.12e"];
- }
- EndIf
- SaveSolution[Sys];
- }
- }
-}
-
-// Same PostProcessing for both static and dynamic formulations (both refer to
-// the same FunctionSpace from which the solution is obtained)
-PostProcessing {
- { Name MagDyn_a_2D; NameOfFormulation MagDyn_a_2D;
- PostQuantity {
- // In 2D, a is a vector with only a z-component: (0,0,az)
- { Name a; Value {
- Term { [ {a} ]; In Vol_Mag; Jacobian Vol; }
- }
- }
- // The equilines of az are field lines (giving the magnetic field direction)
- { Name az; Value {
- Term { [ CompZ[{a}] ]; In Vol_Mag; Jacobian Vol; }
- }
- }
- { Name b; Value {
- Term { [ {d a} ]; In Vol_Mag; Jacobian Vol; }
- }
- }
- { Name norm_of_b; Value {
- Term { [ Norm[{d a}] ]; In Vol_Mag; Jacobian Vol; }
- }
- }
- { Name h; Value {
- Term { [ nu[] * {d a} ]; In Vol_Mag; Jacobian Vol; }
- Term { [ -nu[] * br[] ]; In Vol_M_Mag; Jacobian Vol; }
- }
- }
- { Name js; Value {
- Term { [ js0[] ]; In Vol_S0_Mag; Jacobian Vol; }
- Term { [ (js0[]*Vector[0,0,1])*{ir} ]; In Vol_S_Mag; Jacobian Vol; }
- Term { [ Vector[0,0,0] ]; In Vol_Mag; Jacobian Vol; } // to force a vector result out of sources
- }
- }
- { Name j; Value {
- Term { [ -sigma[] * (Dt[{a}]+{ur}/CoefGeos[]) ]; In Vol_C_Mag; Jacobian Vol; }
- Term { [ js0[] ]; In Vol_S0_Mag; Jacobian Vol; }
- Term { [ (js0[]*Vector[0,0,1])*{ir} ]; In Vol_S_Mag; Jacobian Vol; }
- Term { [ Vector[0,0,0] ]; In Vol_Mag; Jacobian Vol; }
- // Current density in A/m
- Term { [ -Ysur[] * (Dt[{a}]+{ur}/CoefGeos[]) ]; In Sur_Imped_Mag; Jacobian Sur; }
- }
- }
- { Name JouleLosses; Value {
- Integral { [ CoefPower * sigma[]*SquNorm[Dt[{a}]+{ur}/CoefGeos[]] ];
- In Vol_C_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ CoefPower * 1./sigma[]*SquNorm[js0[]] ];
- In Vol_S0_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ CoefPower * 1./sigma[]*SquNorm[(js0[]*Vector[0,0,1])*{ir}] ];
- In Vol_S_Mag; Jacobian Vol; Integration Gauss_v; }
- Integral { [ CoefPower * Ysur[]*SquNorm[Dt[{a}]+{ur}/CoefGeos[]] ];
- In Sur_Imped_Mag; Jacobian Sur; Integration Gauss_v; }
- }
- }
- { Name U; Value {
- Term { [ {U} ]; In Vol_C_Mag; }
- Term { [ {Us} ]; In Vol_S_Mag; }
- If(Flag_CircuitCoupling)
- Term { [ {Uz} ]; In Domain_Cir; }
- EndIf
- }
- }
- { Name I; Value {
- Term { [ {I} ]; In Vol_C_Mag; }
- Term { [ {Is} ]; In Vol_S_Mag; }
- If(Flag_CircuitCoupling)
- Term { [ {Iz} ]; In Domain_Cir; }
- EndIf
- }
- }
- }
- }
-
- { Name MagSta_a_2D; NameOfFormulation MagSta_a_2D;
- PostQuantity {
- { Name a; Value {
- Term { [ {a} ]; In Vol_Mag; Jacobian Vol; }
- }
- }
- { Name az; Value {
- Term { [ CompZ[{a}] ]; In Vol_Mag; Jacobian Vol; }
- }
- }
- { Name b; Value {
- Term { [ {d a} ]; In Vol_Mag; Jacobian Vol; }
- }
- }
- { Name h; Value {
- Term { [ nu[] * {d a} ]; In Vol_Mag; Jacobian Vol; }
- }
- }
- { Name j; Value {
- Term { [ js0[] ]; In Vol_S0_Mag; Jacobian Vol; }
- Term { [ (js0[]*Vector[0,0,1])*{ir} ]; In Vol_S_Mag; Jacobian Vol; }
- Term { [ Vector[0,0,0] ]; In Vol_Mag; Jacobian Vol; }
- }
- }
- }
- }
-}
--
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