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authorGravatar Dave Grote <grote1@llnl.gov> 2019-08-19 16:53:48 -0700
committerGravatar Dave Grote <grote1@llnl.gov> 2019-08-19 16:53:48 -0700
commitefbcd1b41c98d317b25a88e4099364c1ee95b0a1 (patch)
tree3689071c050cb948c80f7f82b1007015c031b460 /Source/FieldSolver/WarpXPushFieldsEM.cpp
parent982bfb591e90c2dc1ecf319ff6af917f1a199ea1 (diff)
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Implemented inverse volume scaling of J for RZ multimode in C++
Diffstat (limited to '')
-rw-r--r--Source/FieldSolver/WarpXPushFieldsEM.cpp81
1 files changed, 73 insertions, 8 deletions
diff --git a/Source/FieldSolver/WarpXPushFieldsEM.cpp b/Source/FieldSolver/WarpXPushFieldsEM.cpp
index dfb9f0211..0455762d6 100644
--- a/Source/FieldSolver/WarpXPushFieldsEM.cpp
+++ b/Source/FieldSolver/WarpXPushFieldsEM.cpp
@@ -616,6 +616,8 @@ WarpX::ApplyInverseVolumeScalingToCurrentDensity (MultiFab* Jx, MultiFab* Jy, Mu
const Real rmin = xyzmin[0];
const int irmin = lo.x;
+ const long nmodes = n_rz_azimuthal_modes;
+
// Rescale current in r-z mode since the inverse volume factor was not
// included in the current deposition.
amrex::ParallelFor(tbr,
@@ -625,13 +627,30 @@ WarpX::ApplyInverseVolumeScalingToCurrentDensity (MultiFab* Jx, MultiFab* Jy, Mu
// to the cells above the axis.
// Note that Jr(i==0) is at 1/2 dr.
if (rmin == 0. && 0 <= i && i < ngJ) {
- Jr_arr(i,j,0) -= Jr_arr(-1-i,j,0);
+ Jr_arr(i,j,0,0) -= Jr_arr(-1-i,j,0,0);
}
// Apply the inverse volume scaling
// Since Jr is not cell centered in r, no need for distinction
// between on axis and off-axis factors
const amrex::Real r = std::abs(rmin + (i - irmin + 0.5)*dr);
- Jr_arr(i,j,0) /= (2.*MathConst::pi*r);
+ Jr_arr(i,j,0,0) /= (2.*MathConst::pi*r);
+
+ for (int imode=1 ; imode < nmodes ; imode++) {
+ const Real ifact = ( (imode%2) == 0 ? +1. : -1.);
+ // Wrap the current density deposited in the guard cells around
+ // to the cells above the axis.
+ // Note that Jr(i==0) is at 1/2 dr.
+ if (rmin == 0. && 0 <= i && i < ngJ) {
+ Jr_arr(i,j,0,2*imode) -= ifact*Jr_arr(-1-i,j,0,2*imode);
+ Jr_arr(i,j,0,2*imode+1) -= ifact*Jr_arr(-1-i,j,0,2*imode+1);
+ }
+ // Apply the inverse volume scaling
+ // Since Jr is not cell centered in r, no need for distinction
+ // between on axis and off-axis factors
+ Jr_arr(i,j,0,2*imode) /= (2.*MathConst::pi*r);
+ Jr_arr(i,j,0,2*imode+1) /= (2.*MathConst::pi*r);
+ }
+
});
amrex::ParallelFor(tbt,
[=] AMREX_GPU_DEVICE (int i, int j, int k)
@@ -640,17 +659,40 @@ WarpX::ApplyInverseVolumeScalingToCurrentDensity (MultiFab* Jx, MultiFab* Jy, Mu
// to the cells above the axis.
// Jt is located on the boundary
if (rmin == 0. && 0 < i && i <= ngJ) {
- Jt_arr(i,j,0) += Jt_arr(-i,j,0);
+ Jt_arr(i,j,0,0) += Jt_arr(-i,j,0,0);
}
// Apply the inverse volume scaling
// Jt is forced to zero on axis.
const amrex::Real r = std::abs(rmin + (i - irmin)*dr);
if (r == 0.) {
- Jt_arr(i,j,0) = 0.;
+ Jt_arr(i,j,0,0) = 0.;
} else {
- Jt_arr(i,j,0) /= (2.*MathConst::pi*r);
+ Jt_arr(i,j,0,0) /= (2.*MathConst::pi*r);
+ }
+
+ for (int imode=1 ; imode < nmodes ; imode++) {
+ const Real ifact = ( (imode%2) == 0 ? +1. : -1.);
+ // Wrap the current density deposited in the guard cells around
+ // to the cells above the axis.
+ // Jt is located on the boundary
+ if (rmin == 0. && 0 < i && i <= ngJ) {
+ Jt_arr(i,j,0,2*imode) += ifact*Jt_arr(-i,j,0,2*imode);
+ Jt_arr(i,j,0,2*imode+1) += ifact*Jt_arr(-i,j,0,2*imode+1);
+ }
+
+ // Apply the inverse volume scaling
+ // Jt is forced to zero on axis.
+ const amrex::Real r = std::abs(rmin + (i - irmin)*dr);
+ if (r == 0.) {
+ Jt_arr(i,j,0,2*imode) = 0.;
+ Jt_arr(i,j,0,2*imode+1) = 0.;
+ } else {
+ Jt_arr(i,j,0,2*imode) /= (2.*MathConst::pi*r);
+ Jt_arr(i,j,0,2*imode+1) /= (2.*MathConst::pi*r);
+ }
}
+
});
amrex::ParallelFor(tbz,
[=] AMREX_GPU_DEVICE (int i, int j, int k)
@@ -659,17 +701,40 @@ WarpX::ApplyInverseVolumeScalingToCurrentDensity (MultiFab* Jx, MultiFab* Jy, Mu
// to the cells above the axis.
// Jz is located on the boundary
if (rmin == 0. && 0 < i && i <= ngJ) {
- Jz_arr(i,j,0) += Jz_arr(-i,j,0);
+ Jz_arr(i,j,0,0) += Jz_arr(-i,j,0,0);
}
// Apply the inverse volume scaling
const amrex::Real r = std::abs(rmin + (i - irmin)*dr);
if (r == 0.) {
// Verboncoeur JCP 164, 421-427 (2001) : corrected volume on axis
- Jz_arr(i,j,0) /= (MathConst::pi*dr/3.);
+ Jz_arr(i,j,0,0) /= (MathConst::pi*dr/3.);
} else {
- Jz_arr(i,j,0) /= (2.*MathConst::pi*r);
+ Jz_arr(i,j,0,0) /= (2.*MathConst::pi*r);
+ }
+
+ for (int imode=1 ; imode < nmodes ; imode++) {
+ const Real ifact = ( (imode%2) == 0 ? +1. : -1.);
+ // Wrap the current density deposited in the guard cells around
+ // to the cells above the axis.
+ // Jz is located on the boundary
+ if (rmin == 0. && 0 < i && i <= ngJ) {
+ Jz_arr(i,j,0,2*imode) += Jz_arr(-i,j,0,2*imode);
+ Jz_arr(i,j,0,2*imode+1) += Jz_arr(-i,j,0,2*imode+1);
+ }
+
+ // Apply the inverse volume scaling
+ const amrex::Real r = std::abs(rmin + (i - irmin)*dr);
+ if (r == 0.) {
+ // Verboncoeur JCP 164, 421-427 (2001) : corrected volume on axis
+ Jz_arr(i,j,0,2*imode) /= (MathConst::pi*dr/3.);
+ Jz_arr(i,j,0,2*imode+1) /= (MathConst::pi*dr/3.);
+ } else {
+ Jz_arr(i,j,0,2*imode) /= (2.*MathConst::pi*r);
+ Jz_arr(i,j,0,2*imode+1) /= (2.*MathConst::pi*r);
+ }
}
+
});
}
}