git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@8795 f3b2605a-c512-4ea7-a41b-209d697bcdaa
This commit is contained in:
@ -22,8 +22,10 @@
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#include "force.h"
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#include "memory.h"
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#include "error.h"
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#include "math_const.h"
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using namespace LAMMPS_NS;
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using namespace MathConst;
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#define OFFSET 16384
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@ -38,7 +40,7 @@ using namespace LAMMPS_NS;
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/* ---------------------------------------------------------------------- */
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PPPMTIP4P::PPPMTIP4P(LAMMPS *lmp, int narg, char **arg) :
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PPPMOld(lmp, narg, arg) {}
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PPPM(lmp, narg, arg) {}
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/* ---------------------------------------------------------------------- */
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@ -49,7 +51,7 @@ void PPPMTIP4P::init()
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if (force->newton == 0)
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error->all(FLERR,"Kspace style pppm/tip4p requires newton on");
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PPPMOld::init();
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PPPM::init();
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}
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/* ----------------------------------------------------------------------
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@ -162,6 +164,16 @@ void PPPMTIP4P::make_rho()
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------------------------------------------------------------------------- */
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void PPPMTIP4P::fieldforce()
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{
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if (differentiation_flag == 1) fieldforce_ad();
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else fieldforce_ik();
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}
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/* ----------------------------------------------------------------------
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interpolate from grid to get electric field & force on my particles for ik
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------------------------------------------------------------------------- */
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void PPPMTIP4P::fieldforce_ik()
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{
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int i,l,m,n,nx,ny,nz,mx,my,mz;
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FFT_SCALAR dx,dy,dz,x0,y0,z0;
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@ -170,14 +182,12 @@ void PPPMTIP4P::fieldforce()
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int iH1,iH2;
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double xM[3];
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double fx,fy,fz;
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double ddotf, rOMx, rOMy, rOMz, f1x, f1y, f1z;
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// loop over my charges, interpolate electric field from nearby grid points
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// (nx,ny,nz) = global coords of grid pt to "lower left" of charge
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// (dx,dy,dz) = distance to "lower left" grid pt
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// (mx,my,mz) = global coords of moving stencil pt
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// ek = 3 components of E-field on particle
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double *q = atom->q;
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double **x = atom->x;
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double **f = atom->f;
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@ -231,27 +241,245 @@ void PPPMTIP4P::fieldforce()
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fz = qfactor * ekz;
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find_M(i,iH1,iH2,xM);
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rOMx = xM[0] - x[i][0];
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rOMy = xM[1] - x[i][1];
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rOMz = xM[2] - x[i][2];
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f[i][0] += fx*(1 - alpha);
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f[i][1] += fy*(1 - alpha);
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f[i][2] += fz*(1 - alpha);
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ddotf = (rOMx * fx + rOMy * fy + rOMz * fz) / (qdist * qdist);
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f[iH1][0] += 0.5*alpha*fx;
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f[iH1][1] += 0.5*alpha*fy;
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f[iH1][2] += 0.5*alpha*fz;
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f1x = ddotf * rOMx;
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f1y = ddotf * rOMy;
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f1z = ddotf * rOMz;
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f[iH2][0] += 0.5*alpha*fx;
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f[iH2][1] += 0.5*alpha*fy;
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f[iH2][2] += 0.5*alpha*fz;
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}
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}
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}
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f[i][0] += fx - alpha * (fx - f1x);
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f[i][1] += fy - alpha * (fy - f1y);
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f[i][2] += fz - alpha * (fz - f1z);
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/* ----------------------------------------------------------------------
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interpolate from grid to get electric field & force on my particles for ad
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------------------------------------------------------------------------- */
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f[iH1][0] += 0.5*alpha*(fx - f1x);
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f[iH1][1] += 0.5*alpha*(fy - f1y);
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f[iH1][2] += 0.5*alpha*(fz - f1z);
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void PPPMTIP4P::fieldforce_ad()
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{
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int i,l,m,n,nx,ny,nz,mx,my,mz;
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FFT_SCALAR dx,dy,dz,x0,y0,z0,dx0,dy0,dz0;
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FFT_SCALAR ekx,eky,ekz;
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double *xi;
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int iH1,iH2;
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double xM[3];
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double s1,s2,s3;
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double sf;
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double *prd;
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double fx,fy,fz;
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f[iH2][0] += 0.5*alpha*(fx - f1x);
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f[iH2][1] += 0.5*alpha*(fy - f1y);
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f[iH2][2] += 0.5*alpha*(fz - f1z);
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if (triclinic == 0) prd = domain->prd;
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else prd = domain->prd_lamda;
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double xprd = prd[0];
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double yprd = prd[1];
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double zprd = prd[2];
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double zprd_slab = zprd*slab_volfactor;
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double hx_inv = nx_pppm/xprd;
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double hy_inv = ny_pppm/yprd;
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double hz_inv = nz_pppm/zprd;
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// loop over my charges, interpolate electric field from nearby grid points
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// (nx,ny,nz) = global coords of grid pt to "lower left" of charge
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// (dx,dy,dz) = distance to "lower left" grid pt
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// (mx,my,mz) = global coords of moving stencil pt
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// ek = 3 components of E-field on particle
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double *q = atom->q;
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double **x = atom->x;
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double **f = atom->f;
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int *type = atom->type;
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int nlocal = atom->nlocal;
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for (i = 0; i < nlocal; i++) {
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if (type[i] == typeO) {
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find_M(i,iH1,iH2,xM);
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xi = xM;
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} else xi = x[i];
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nx = part2grid[i][0];
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ny = part2grid[i][1];
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nz = part2grid[i][2];
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dx = nx+shiftone - (x[i][0]-boxlo[0])*delxinv;
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dy = ny+shiftone - (x[i][1]-boxlo[1])*delyinv;
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dz = nz+shiftone - (x[i][2]-boxlo[2])*delzinv;
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compute_rho1d(dx,dy,dz);
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compute_drho1d(dx,dy,dz);
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ekx = eky = ekz = ZEROF;
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for (n = nlower; n <= nupper; n++) {
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mz = n+nz;
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for (m = nlower; m <= nupper; m++) {
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my = m+ny;
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for (l = nlower; l <= nupper; l++) {
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mx = l+nx;
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ekx += drho1d[0][l]*rho1d[1][m]*rho1d[2][n]*u_brick[mz][my][mx];
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eky += rho1d[0][l]*drho1d[1][m]*rho1d[2][n]*u_brick[mz][my][mx];
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ekz += rho1d[0][l]*rho1d[1][m]*drho1d[2][n]*u_brick[mz][my][mx];
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}
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}
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}
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ekx *= hx_inv;
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eky *= hy_inv;
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ekz *= hz_inv;
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// convert E-field to force and substract self forces
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const double qfactor = force->qqrd2e * scale;
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s1 = x[i][0]*hx_inv;
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s2 = x[i][1]*hy_inv;
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s3 = x[i][2]*hz_inv;
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sf = sf_coeff[0]*sin(2*MY_PI*s1);
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sf += sf_coeff[1]*sin(4*MY_PI*s1);
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sf *= 2*q[i]*q[i];
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fx = qfactor*(ekx*q[i] - sf);
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sf = sf_coeff[2]*sin(2*MY_PI*s2);
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sf += sf_coeff[3]*sin(4*MY_PI*s2);
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sf *= 2*q[i]*q[i];
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fy = qfactor*(eky*q[i] - sf);
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sf = sf_coeff[4]*sin(2*MY_PI*s3);
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sf += sf_coeff[5]*sin(4*MY_PI*s3);
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sf *= 2*q[i]*q[i];
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fz = qfactor*(ekz*q[i] - sf);
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if (type[i] != typeO) {
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f[i][0] += fx;
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f[i][1] += fy;
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f[i][2] += fz;
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} else {
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find_M(i,iH1,iH2,xM);
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f[i][0] += fx*(1 - alpha);
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f[i][1] += fy*(1 - alpha);
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f[i][2] += fz*(1 - alpha);
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f[iH1][0] += 0.5*alpha*fx;
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f[iH1][1] += 0.5*alpha*fy;
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f[iH1][2] += 0.5*alpha*fz;
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f[iH2][0] += 0.5*alpha*fx;
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f[iH2][1] += 0.5*alpha*fy;
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f[iH2][2] += 0.5*alpha*fz;
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}
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}
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}
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/* ----------------------------------------------------------------------
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interpolate from grid to get electric field & force on my particles
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------------------------------------------------------------------------- */
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void PPPMTIP4P::fieldforce_peratom()
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{
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int i,l,m,n,nx,ny,nz,mx,my,mz;
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FFT_SCALAR dx,dy,dz,x0,y0,z0;
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double *xi;
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int iH1,iH2;
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double xM[3];
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FFT_SCALAR u_pa,v0,v1,v2,v3,v4,v5;
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// loop over my charges, interpolate electric field from nearby grid points
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// (nx,ny,nz) = global coords of grid pt to "lower left" of charge
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// (dx,dy,dz) = distance to "lower left" grid pt
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// (mx,my,mz) = global coords of moving stencil pt
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// ek = 3 components of E-field on particle
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double *q = atom->q;
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double **x = atom->x;
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double **f = atom->f;
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int *type = atom->type;
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int nlocal = atom->nlocal;
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for (i = 0; i < nlocal; i++) {
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if (type[i] == typeO) {
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find_M(i,iH1,iH2,xM);
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xi = xM;
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} else xi = x[i];
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nx = part2grid[i][0];
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ny = part2grid[i][1];
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nz = part2grid[i][2];
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dx = nx+shiftone - (xi[0]-boxlo[0])*delxinv;
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dy = ny+shiftone - (xi[1]-boxlo[1])*delyinv;
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dz = nz+shiftone - (xi[2]-boxlo[2])*delzinv;
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compute_rho1d(dx,dy,dz);
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u_pa = v0 = v1 = v2 = v3 = v4 = v5 = ZEROF;
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for (n = nlower; n <= nupper; n++) {
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mz = n+nz;
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z0 = rho1d[2][n];
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for (m = nlower; m <= nupper; m++) {
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my = m+ny;
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y0 = z0*rho1d[1][m];
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for (l = nlower; l <= nupper; l++) {
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mx = l+nx;
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x0 = y0*rho1d[0][l];
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if (eflag_atom) u_pa += x0*u_brick[mz][my][mx];
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if (vflag_atom) {
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v0 += x0*v0_brick[mz][my][mx];
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v1 += x0*v1_brick[mz][my][mx];
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v2 += x0*v2_brick[mz][my][mx];
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v3 += x0*v3_brick[mz][my][mx];
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v4 += x0*v4_brick[mz][my][mx];
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v5 += x0*v5_brick[mz][my][mx];
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}
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}
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}
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}
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if (eflag_atom) {
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if (type[i] != typeO) {
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eatom[i] += q[i]*u_pa;
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} else {
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eatom[i] += q[i]*u_pa*(1-alpha);
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eatom[iH1] += q[i]*u_pa*alpha*0.5;
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eatom[iH2] += q[i]*u_pa*alpha*0.5;
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}
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}
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if (vflag_atom) {
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if (type[i] != typeO) {
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vatom[i][0] += v0*q[i];
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vatom[i][1] += v1*q[i];
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vatom[i][2] += v2*q[i];
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vatom[i][3] += v3*q[i];
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vatom[i][4] += v4*q[i];
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vatom[i][5] += v5*q[i];
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} else {
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vatom[i][0] += v0*(1-alpha)*q[i];
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vatom[i][1] += v1*(1-alpha)*q[i];
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vatom[i][2] += v2*(1-alpha)*q[i];
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vatom[i][3] += v3*(1-alpha)*q[i];
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vatom[i][4] += v4*(1-alpha)*q[i];
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vatom[i][5] += v5*(1-alpha)*q[i];
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vatom[iH1][0] += v0*alpha*0.5*q[i];
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vatom[iH1][1] += v1*alpha*0.5*q[i];
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vatom[iH1][2] += v2*alpha*0.5*q[i];
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vatom[iH1][3] += v3*alpha*0.5*q[i];
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vatom[iH1][4] += v4*alpha*0.5*q[i];
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vatom[iH1][5] += v5*alpha*0.5*q[i];
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vatom[iH2][0] += v0*alpha*0.5*q[i];
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vatom[iH2][1] += v1*alpha*0.5*q[i];
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vatom[iH2][2] += v2*alpha*0.5*q[i];
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vatom[iH2][3] += v3*alpha*0.5*q[i];
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vatom[iH2][4] += v4*alpha*0.5*q[i];
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vatom[iH2][5] += v5*alpha*0.5*q[i];
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}
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}
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}
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}
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