601 lines
17 KiB
C++
601 lines
17 KiB
C++
// clang-format off
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/* ----------------------------------------------------------------------
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LAMMPS - Large-scale Atomic/Molecular Massively Parallel Simulator
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https://www.lammps.org/, Sandia National Laboratories
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Steve Plimpton, sjplimp@sandia.gov
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Copyright (2003) Sandia Corporation. Under the terms of Contract
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DE-AC04-94AL85000 with Sandia Corporation, the U.S. Government retains
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certain rights in this software. This software is distributed under
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the GNU General Public License.
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See the README file in the top-level LAMMPS directory.
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------------------------------------------------------------------------- */
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/* ----------------------------------------------------------------------
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Contributing authors: Amalie Frischknecht and Ahmed Ismail (SNL)
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------------------------------------------------------------------------- */
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#include "pppm_tip4p.h"
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#include <mpi.h>
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#include <cmath>
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#include "atom.h"
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#include "domain.h"
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#include "force.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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#ifdef FFT_SINGLE
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#define ZEROF 0.0f
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#define ONEF 1.0f
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#else
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#define ZEROF 0.0
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#define ONEF 1.0
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#endif
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/* ---------------------------------------------------------------------- */
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PPPMTIP4P::PPPMTIP4P(LAMMPS *lmp) : PPPM(lmp)
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{
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triclinic_support = 1;
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tip4pflag = 1;
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}
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/* ---------------------------------------------------------------------- */
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void PPPMTIP4P::init()
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{
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// TIP4P PPPM requires newton on, b/c it computes forces on ghost atoms
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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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PPPM::init();
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}
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/* ----------------------------------------------------------------------
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find center grid pt for each of my particles
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check that full stencil for the particle will fit in my 3d brick
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store central grid pt indices in part2grid array
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------------------------------------------------------------------------- */
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void PPPMTIP4P::particle_map()
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{
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int nx,ny,nz,iH1,iH2;
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double *xi,xM[3];
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int *type = atom->type;
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double **x = atom->x;
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int nlocal = atom->nlocal;
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if (!std::isfinite(boxlo[0]) || !std::isfinite(boxlo[1]) || !std::isfinite(boxlo[2]))
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error->one(FLERR,"Non-numeric box dimensions - simulation unstable");
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int flag = 0;
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for (int 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,ny,nz) = global coords of grid pt to "lower left" of charge
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// current particle coord can be outside global and local box
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// add/subtract OFFSET to avoid int(-0.75) = 0 when want it to be -1
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nx = static_cast<int> ((xi[0]-boxlo[0])*delxinv+shift) - OFFSET;
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ny = static_cast<int> ((xi[1]-boxlo[1])*delyinv+shift) - OFFSET;
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nz = static_cast<int> ((xi[2]-boxlo[2])*delzinv+shift) - OFFSET;
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part2grid[i][0] = nx;
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part2grid[i][1] = ny;
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part2grid[i][2] = nz;
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// check that entire stencil around nx,ny,nz will fit in my 3d brick
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if (nx+nlower < nxlo_out || nx+nupper > nxhi_out ||
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ny+nlower < nylo_out || ny+nupper > nyhi_out ||
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nz+nlower < nzlo_out || nz+nupper > nzhi_out) flag++;
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}
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int flag_all;
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MPI_Allreduce(&flag,&flag_all,1,MPI_INT,MPI_SUM,world);
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if (flag_all) error->all(FLERR,"Out of range atoms - cannot compute PPPM");
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}
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/* ----------------------------------------------------------------------
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create discretized "density" on section of global grid due to my particles
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density(x,y,z) = charge "density" at grid points of my 3d brick
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(nxlo:nxhi,nylo:nyhi,nzlo:nzhi) is extent of my brick (including ghosts)
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in global grid
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------------------------------------------------------------------------- */
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void PPPMTIP4P::make_rho()
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{
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int i,l,m,n,nx,ny,nz,mx,my,mz,iH1,iH2;
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FFT_SCALAR dx,dy,dz,x0,y0,z0;
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double *xi,xM[3];
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// clear 3d density array
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FFT_SCALAR *vec = &density_brick[nzlo_out][nylo_out][nxlo_out];
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for (i = 0; i < ngrid; i++) vec[i] = ZEROF;
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// loop over my charges, add their contribution to 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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int *type = atom->type;
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double *q = atom->q;
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double **x = atom->x;
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int nlocal = atom->nlocal;
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for (int 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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z0 = delvolinv * q[i];
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for (n = nlower; n <= nupper; n++) {
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mz = n+nz;
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y0 = 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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x0 = y0*rho1d[1][m];
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for (l = nlower; l <= nupper; l++) {
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mx = l+nx;
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density_brick[mz][my][mx] += x0*rho1d[0][l];
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}
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}
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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 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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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 fx,fy,fz;
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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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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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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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ekx -= x0*vdx_brick[mz][my][mx];
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eky -= x0*vdy_brick[mz][my][mx];
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ekz -= x0*vdz_brick[mz][my][mx];
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}
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}
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}
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// convert E-field to force
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const double qfactor = qqrd2e * scale * q[i];
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if (type[i] != typeO) {
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f[i][0] += qfactor*ekx;
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f[i][1] += qfactor*eky;
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if (slabflag != 2) f[i][2] += qfactor*ekz;
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} else {
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fx = qfactor * ekx;
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fy = qfactor * eky;
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fz = qfactor * ekz;
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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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if (slabflag != 2) 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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if (slabflag != 2) 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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if (slabflag != 2) 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 for ad
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------------------------------------------------------------------------- */
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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;
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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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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 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 - (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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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 subtract self forces
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const double qfactor = qqrd2e * scale;
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s1 = xi[0]*hx_inv;
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s2 = xi[1]*hy_inv;
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s3 = xi[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 *= 2.0*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 *= 2.0*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 *= 2.0*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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if (slabflag != 2) 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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if (slabflag != 2) 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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if (slabflag != 2) 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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if (slabflag != 2) 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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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];
|
|
vatom[i][4] += v4*(1-alpha)*q[i];
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|
vatom[i][5] += v5*(1-alpha)*q[i];
|
|
vatom[iH1][0] += v0*alpha*0.5*q[i];
|
|
vatom[iH1][1] += v1*alpha*0.5*q[i];
|
|
vatom[iH1][2] += v2*alpha*0.5*q[i];
|
|
vatom[iH1][3] += v3*alpha*0.5*q[i];
|
|
vatom[iH1][4] += v4*alpha*0.5*q[i];
|
|
vatom[iH1][5] += v5*alpha*0.5*q[i];
|
|
vatom[iH2][0] += v0*alpha*0.5*q[i];
|
|
vatom[iH2][1] += v1*alpha*0.5*q[i];
|
|
vatom[iH2][2] += v2*alpha*0.5*q[i];
|
|
vatom[iH2][3] += v3*alpha*0.5*q[i];
|
|
vatom[iH2][4] += v4*alpha*0.5*q[i];
|
|
vatom[iH2][5] += v5*alpha*0.5*q[i];
|
|
}
|
|
}
|
|
}
|
|
}
|
|
|
|
/* ----------------------------------------------------------------------
|
|
find 2 H atoms bonded to O atom i
|
|
compute position xM of fictitious charge site for O atom
|
|
also return local indices iH1,iH2 of H atoms
|
|
------------------------------------------------------------------------- */
|
|
|
|
void PPPMTIP4P::find_M(int i, int &iH1, int &iH2, double *xM)
|
|
{
|
|
double **x = atom->x;
|
|
|
|
iH1 = atom->map(atom->tag[i] + 1);
|
|
iH2 = atom->map(atom->tag[i] + 2);
|
|
|
|
if (iH1 == -1 || iH2 == -1) error->one(FLERR,"TIP4P hydrogen is missing");
|
|
if (atom->type[iH1] != typeH || atom->type[iH2] != typeH)
|
|
error->one(FLERR,"TIP4P hydrogen has incorrect atom type");
|
|
|
|
if (triclinic) {
|
|
|
|
// need to use custom code to find the closest image for triclinic,
|
|
// since local atoms are in lambda coordinates, but ghosts are not.
|
|
|
|
int *sametag = atom->sametag;
|
|
double xo[3],xh1[3],xh2[3],xm[3];
|
|
const int nlocal = atom->nlocal;
|
|
|
|
for (int ii = 0; ii < 3; ++ii) {
|
|
xo[ii] = x[i][ii];
|
|
xh1[ii] = x[iH1][ii];
|
|
xh2[ii] = x[iH2][ii];
|
|
}
|
|
|
|
if (i < nlocal) domain->lamda2x(x[i],xo);
|
|
if (iH1 < nlocal) domain->lamda2x(x[iH1],xh1);
|
|
if (iH2 < nlocal) domain->lamda2x(x[iH2],xh2);
|
|
|
|
double delx = xo[0] - xh1[0];
|
|
double dely = xo[1] - xh1[1];
|
|
double delz = xo[2] - xh1[2];
|
|
double rsqmin = delx*delx + dely*dely + delz*delz;
|
|
double rsq;
|
|
int closest = iH1;
|
|
|
|
// no need to run lamda2x() here -> ghost atoms
|
|
|
|
while (sametag[iH1] >= 0) {
|
|
iH1 = sametag[iH1];
|
|
delx = xo[0] - x[iH1][0];
|
|
dely = xo[1] - x[iH1][1];
|
|
delz = xo[2] - x[iH1][2];
|
|
rsq = delx*delx + dely*dely + delz*delz;
|
|
if (rsq < rsqmin) {
|
|
rsqmin = rsq;
|
|
closest = iH1;
|
|
xh1[0] = x[iH1][0];
|
|
xh1[1] = x[iH1][1];
|
|
xh1[2] = x[iH1][2];
|
|
}
|
|
}
|
|
iH1 = closest;
|
|
|
|
closest = iH2;
|
|
delx = xo[0] - xh2[0];
|
|
dely = xo[1] - xh2[1];
|
|
delz = xo[2] - xh2[2];
|
|
rsqmin = delx*delx + dely*dely + delz*delz;
|
|
|
|
while (sametag[iH2] >= 0) {
|
|
iH2 = sametag[iH2];
|
|
delx = xo[0] - x[iH2][0];
|
|
dely = xo[1] - x[iH2][1];
|
|
delz = xo[2] - x[iH2][2];
|
|
rsq = delx*delx + dely*dely + delz*delz;
|
|
if (rsq < rsqmin) {
|
|
rsqmin = rsq;
|
|
closest = iH2;
|
|
xh2[0] = x[iH2][0];
|
|
xh2[1] = x[iH2][1];
|
|
xh2[2] = x[iH2][2];
|
|
}
|
|
}
|
|
iH2 = closest;
|
|
|
|
// finally compute M in real coordinates ...
|
|
|
|
double delx1 = xh1[0] - xo[0];
|
|
double dely1 = xh1[1] - xo[1];
|
|
double delz1 = xh1[2] - xo[2];
|
|
|
|
double delx2 = xh2[0] - xo[0];
|
|
double dely2 = xh2[1] - xo[1];
|
|
double delz2 = xh2[2] - xo[2];
|
|
|
|
xm[0] = xo[0] + alpha * 0.5 * (delx1 + delx2);
|
|
xm[1] = xo[1] + alpha * 0.5 * (dely1 + dely2);
|
|
xm[2] = xo[2] + alpha * 0.5 * (delz1 + delz2);
|
|
|
|
// ... and convert M to lamda space for PPPM
|
|
|
|
domain->x2lamda(xm,xM);
|
|
|
|
} else {
|
|
|
|
// set iH1,iH2 to index of closest image to O
|
|
|
|
iH1 = domain->closest_image(i,iH1);
|
|
iH2 = domain->closest_image(i,iH2);
|
|
|
|
double delx1 = x[iH1][0] - x[i][0];
|
|
double dely1 = x[iH1][1] - x[i][1];
|
|
double delz1 = x[iH1][2] - x[i][2];
|
|
|
|
double delx2 = x[iH2][0] - x[i][0];
|
|
double dely2 = x[iH2][1] - x[i][1];
|
|
double delz2 = x[iH2][2] - x[i][2];
|
|
|
|
xM[0] = x[i][0] + alpha * 0.5 * (delx1 + delx2);
|
|
xM[1] = x[i][1] + alpha * 0.5 * (dely1 + dely2);
|
|
xM[2] = x[i][2] + alpha * 0.5 * (delz1 + delz2);
|
|
}
|
|
}
|