void do_pbc_first(FILE *log,t_parm *parm,rvec box_size,t_forcerec *fr,
t_graph *graph,rvec x[])
{
char *pbcenv;
if(log)
fprintf(log,"Removing pbc first time\n");
calc_shifts(parm->box,box_size,fr->shift_vec);
mk_mshift(log,graph,parm->box,x);
#ifdef SPEC_CPU
pbcenv = NULL;
#else
pbcenv = getenv ("NOPBC");
#endif
if (pbcenv == NULL)
shift_self(graph,parm->box,x);
else
{
if(log)
fprintf(log,"Not doing first shift_self\n");
}
if(log)
fprintf(log,"Done rmpbc\n");
}
void gmx_rmpbc(gmx_rmpbc_t gpbc, int natoms, matrix box, rvec x[])
{
int ePBC;
t_graph *gr;
ePBC = gmx_rmpbc_ePBC(gpbc, box);
gr = gmx_rmpbc_get_graph(gpbc, ePBC, natoms);
if (gr != NULL)
{
mk_mshift(stdout, gr, ePBC, box, x);
shift_self(gr, box, x);
}
}
void do_pbc_first(FILE *fplog,matrix box,t_forcerec *fr,
t_graph *graph,rvec x[])
{
if (fplog)
fprintf(fplog,"Removing pbc first time\n");
calc_shifts(box,fr->shift_vec);
if (graph) {
mk_mshift(fplog,graph,fr->ePBC,box,x);
if (gmx_debug_at)
p_graph(debug,"do_pbc_first 1",graph);
shift_self(graph,box,x);
/* By doing an extra mk_mshift the molecules that are broken
* because they were e.g. imported from another software
* will be made whole again. Such are the healing powers
* of GROMACS.
*/
mk_mshift(fplog,graph,fr->ePBC,box,x);
if (gmx_debug_at)
p_graph(debug,"do_pbc_first 2",graph);
}
if (fplog)
fprintf(fplog,"Done rmpbc\n");
}
void gmx_rmpbc_trxfr(gmx_rmpbc_t gpbc, t_trxframe *fr)
{
int ePBC;
t_graph *gr;
if (fr->bX && fr->bBox)
{
ePBC = gmx_rmpbc_ePBC(gpbc, fr->box);
gr = gmx_rmpbc_get_graph(gpbc, ePBC, fr->natoms);
if (gr != NULL)
{
mk_mshift(stdout, gr, ePBC, fr->box, fr->x);
shift_self(gr, fr->box, fr->x);
}
}
}
void gmx_rmpbc_copy(gmx_rmpbc_t gpbc, int natoms, matrix box, rvec x[], rvec x_s[])
{
int ePBC;
t_graph *gr;
int i;
ePBC = gmx_rmpbc_ePBC(gpbc, box);
gr = gmx_rmpbc_get_graph(gpbc, ePBC, natoms);
if (gr != NULL)
{
mk_mshift(stdout, gr, ePBC, box, x);
shift_x(gr, box, x, x_s);
}
else
{
for (i = 0; i < natoms; i++)
{
copy_rvec(x[i], x_s[i]);
}
}
}
static void low_do_pbc_mtop(FILE *fplog,int ePBC,matrix box,
gmx_mtop_t *mtop,rvec x[],
bool bFirst)
{
t_graph *graph;
int mb,as,mol;
gmx_molblock_t *molb;
if (bFirst && fplog)
fprintf(fplog,"Removing pbc first time\n");
snew(graph,1);
as = 0;
for(mb=0; mb<mtop->nmolblock; mb++) {
molb = &mtop->molblock[mb];
if (molb->natoms_mol == 1 ||
(!bFirst && mtop->moltype[molb->type].cgs.nr == 1)) {
/* Just one atom or charge group in the molecule, no PBC required */
as += molb->nmol*molb->natoms_mol;
} else {
/* Pass NULL iso fplog to avoid graph prints for each molecule type */
mk_graph_ilist(NULL,mtop->moltype[molb->type].ilist,
0,molb->natoms_mol,FALSE,FALSE,graph);
for(mol=0; mol<molb->nmol; mol++) {
mk_mshift(fplog,graph,ePBC,box,x+as);
shift_self(graph,box,x+as);
/* The molecule is whole now.
* We don't need the second mk_mshift call as in do_pbc_first,
* since we no longer need this graph.
*/
as += molb->natoms_mol;
}
done_graph(graph);
}
}
sfree(graph);
}
int relax_shell_flexcon(FILE *fplog, t_commrec *cr, gmx_bool bVerbose,
gmx_int64_t mdstep, t_inputrec *inputrec,
gmx_bool bDoNS, int force_flags,
gmx_localtop_t *top,
gmx_constr_t constr,
gmx_enerdata_t *enerd, t_fcdata *fcd,
t_state *state, rvec f[],
tensor force_vir,
t_mdatoms *md,
t_nrnb *nrnb, gmx_wallcycle_t wcycle,
t_graph *graph,
gmx_groups_t *groups,
struct gmx_shellfc *shfc,
t_forcerec *fr,
gmx_bool bBornRadii,
double t, rvec mu_tot,
gmx_bool *bConverged,
gmx_vsite_t *vsite,
FILE *fp_field)
{
int nshell;
t_shell *shell;
t_idef *idef;
rvec *pos[2], *force[2], *acc_dir = NULL, *x_old = NULL;
real Epot[2], df[2];
rvec dx;
real sf_dir, invdt;
real ftol, xiH, xiS, dum = 0;
char sbuf[22];
gmx_bool bCont, bInit;
int nat, dd_ac0, dd_ac1 = 0, i;
int start = 0, homenr = md->homenr, end = start+homenr, cg0, cg1;
int nflexcon, g, number_steps, d, Min = 0, count = 0;
#define Try (1-Min) /* At start Try = 1 */
bCont = (mdstep == inputrec->init_step) && inputrec->bContinuation;
bInit = (mdstep == inputrec->init_step) || shfc->bRequireInit;
ftol = inputrec->em_tol;
number_steps = inputrec->niter;
nshell = shfc->nshell;
shell = shfc->shell;
nflexcon = shfc->nflexcon;
idef = &top->idef;
if (DOMAINDECOMP(cr))
{
nat = dd_natoms_vsite(cr->dd);
if (nflexcon > 0)
{
dd_get_constraint_range(cr->dd, &dd_ac0, &dd_ac1);
nat = max(nat, dd_ac1);
}
}
else
{
nat = state->natoms;
}
if (nat > shfc->x_nalloc)
{
/* Allocate local arrays */
shfc->x_nalloc = over_alloc_dd(nat);
for (i = 0; (i < 2); i++)
{
srenew(shfc->x[i], shfc->x_nalloc);
srenew(shfc->f[i], shfc->x_nalloc);
}
}
for (i = 0; (i < 2); i++)
{
pos[i] = shfc->x[i];
force[i] = shfc->f[i];
}
/* When we had particle decomposition, this code only worked with
* PD when all particles involved with each shell were in the same
* charge group. Not sure if this is still relevant. */
if (bDoNS && inputrec->ePBC != epbcNONE && !DOMAINDECOMP(cr))
{
/* This is the only time where the coordinates are used
* before do_force is called, which normally puts all
* charge groups in the box.
*/
cg0 = 0;
cg1 = top->cgs.nr;
put_charge_groups_in_box(fplog, cg0, cg1, fr->ePBC, state->box,
&(top->cgs), state->x, fr->cg_cm);
if (graph)
{
mk_mshift(fplog, graph, fr->ePBC, state->box, state->x);
}
}
/* After this all coordinate arrays will contain whole molecules */
if (graph)
{
shift_self(graph, state->box, state->x);
}
if (nflexcon)
{
if (nat > shfc->flex_nalloc)
{
shfc->flex_nalloc = over_alloc_dd(nat);
srenew(shfc->acc_dir, shfc->flex_nalloc);
srenew(shfc->x_old, shfc->flex_nalloc);
}
acc_dir = shfc->acc_dir;
x_old = shfc->x_old;
for (i = 0; i < homenr; i++)
{
for (d = 0; d < DIM; d++)
{
shfc->x_old[i][d] =
state->x[start+i][d] - state->v[start+i][d]*inputrec->delta_t;
}
}
}
/* Do a prediction of the shell positions */
if (shfc->bPredict && !bCont)
{
predict_shells(fplog, state->x, state->v, inputrec->delta_t, nshell, shell,
md->massT, NULL, bInit);
}
/* do_force expected the charge groups to be in the box */
if (graph)
{
unshift_self(graph, state->box, state->x);
}
/* Calculate the forces first time around */
if (gmx_debug_at)
{
pr_rvecs(debug, 0, "x b4 do_force", state->x + start, homenr);
}
do_force(fplog, cr, inputrec, mdstep, nrnb, wcycle, top, groups,
state->box, state->x, &state->hist,
force[Min], force_vir, md, enerd, fcd,
state->lambda, graph,
fr, vsite, mu_tot, t, fp_field, NULL, bBornRadii,
(bDoNS ? GMX_FORCE_NS : 0) | force_flags);
sf_dir = 0;
if (nflexcon)
{
init_adir(fplog, shfc,
constr, idef, inputrec, cr, dd_ac1, mdstep, md, start, end,
shfc->x_old-start, state->x, state->x, force[Min],
shfc->acc_dir-start,
fr->bMolPBC, state->box, state->lambda, &dum, nrnb);
for (i = start; i < end; i++)
{
sf_dir += md->massT[i]*norm2(shfc->acc_dir[i-start]);
}
}
Epot[Min] = enerd->term[F_EPOT];
df[Min] = rms_force(cr, shfc->f[Min], nshell, shell, nflexcon, &sf_dir, &Epot[Min]);
df[Try] = 0;
if (debug)
{
fprintf(debug, "df = %g %g\n", df[Min], df[Try]);
}
if (gmx_debug_at)
{
pr_rvecs(debug, 0, "force0", force[Min], md->nr);
}
if (nshell+nflexcon > 0)
{
/* Copy x to pos[Min] & pos[Try]: during minimization only the
* shell positions are updated, therefore the other particles must
* be set here.
*/
memcpy(pos[Min], state->x, nat*sizeof(state->x[0]));
memcpy(pos[Try], state->x, nat*sizeof(state->x[0]));
}
if (bVerbose && MASTER(cr))
{
print_epot(stdout, mdstep, 0, Epot[Min], df[Min], nflexcon, sf_dir);
}
if (debug)
{
fprintf(debug, "%17s: %14.10e\n",
interaction_function[F_EKIN].longname, enerd->term[F_EKIN]);
fprintf(debug, "%17s: %14.10e\n",
interaction_function[F_EPOT].longname, enerd->term[F_EPOT]);
fprintf(debug, "%17s: %14.10e\n",
interaction_function[F_ETOT].longname, enerd->term[F_ETOT]);
fprintf(debug, "SHELLSTEP %s\n", gmx_step_str(mdstep, sbuf));
}
/* First check whether we should do shells, or whether the force is
* low enough even without minimization.
*/
*bConverged = (df[Min] < ftol);
for (count = 1; (!(*bConverged) && (count < number_steps)); count++)
{
if (vsite)
{
construct_vsites(vsite, pos[Min], inputrec->delta_t, state->v,
idef->iparams, idef->il,
fr->ePBC, fr->bMolPBC, cr, state->box);
}
if (nflexcon)
{
init_adir(fplog, shfc,
constr, idef, inputrec, cr, dd_ac1, mdstep, md, start, end,
x_old-start, state->x, pos[Min], force[Min], acc_dir-start,
fr->bMolPBC, state->box, state->lambda, &dum, nrnb);
directional_sd(pos[Min], pos[Try], acc_dir-start, start, end,
fr->fc_stepsize);
}
/* New positions, Steepest descent */
shell_pos_sd(pos[Min], pos[Try], force[Min], nshell, shell, count);
/* do_force expected the charge groups to be in the box */
if (graph)
{
unshift_self(graph, state->box, pos[Try]);
}
if (gmx_debug_at)
{
pr_rvecs(debug, 0, "RELAX: pos[Min] ", pos[Min] + start, homenr);
pr_rvecs(debug, 0, "RELAX: pos[Try] ", pos[Try] + start, homenr);
}
/* Try the new positions */
do_force(fplog, cr, inputrec, 1, nrnb, wcycle,
top, groups, state->box, pos[Try], &state->hist,
force[Try], force_vir,
md, enerd, fcd, state->lambda, graph,
fr, vsite, mu_tot, t, fp_field, NULL, bBornRadii,
force_flags);
if (gmx_debug_at)
{
pr_rvecs(debug, 0, "RELAX: force[Min]", force[Min] + start, homenr);
pr_rvecs(debug, 0, "RELAX: force[Try]", force[Try] + start, homenr);
}
sf_dir = 0;
if (nflexcon)
{
init_adir(fplog, shfc,
constr, idef, inputrec, cr, dd_ac1, mdstep, md, start, end,
x_old-start, state->x, pos[Try], force[Try], acc_dir-start,
fr->bMolPBC, state->box, state->lambda, &dum, nrnb);
for (i = start; i < end; i++)
{
sf_dir += md->massT[i]*norm2(acc_dir[i-start]);
}
}
Epot[Try] = enerd->term[F_EPOT];
df[Try] = rms_force(cr, force[Try], nshell, shell, nflexcon, &sf_dir, &Epot[Try]);
if (debug)
{
fprintf(debug, "df = %g %g\n", df[Min], df[Try]);
}
if (debug)
{
if (gmx_debug_at)
{
pr_rvecs(debug, 0, "F na do_force", force[Try] + start, homenr);
}
if (gmx_debug_at)
{
fprintf(debug, "SHELL ITER %d\n", count);
dump_shells(debug, pos[Try], force[Try], ftol, nshell, shell);
}
}
if (bVerbose && MASTER(cr))
{
print_epot(stdout, mdstep, count, Epot[Try], df[Try], nflexcon, sf_dir);
}
*bConverged = (df[Try] < ftol);
if ((df[Try] < df[Min]))
{
if (debug)
{
fprintf(debug, "Swapping Min and Try\n");
}
if (nflexcon)
{
/* Correct the velocities for the flexible constraints */
invdt = 1/inputrec->delta_t;
for (i = start; i < end; i++)
{
for (d = 0; d < DIM; d++)
{
state->v[i][d] += (pos[Try][i][d] - pos[Min][i][d])*invdt;
}
}
}
Min = Try;
}
else
{
decrease_step_size(nshell, shell);
}
}
if (MASTER(cr) && !(*bConverged))
{
/* Note that the energies and virial are incorrect when not converged */
if (fplog)
{
fprintf(fplog,
"step %s: EM did not converge in %d iterations, RMS force %.3f\n",
gmx_step_str(mdstep, sbuf), number_steps, df[Min]);
}
fprintf(stderr,
"step %s: EM did not converge in %d iterations, RMS force %.3f\n",
gmx_step_str(mdstep, sbuf), number_steps, df[Min]);
}
/* Copy back the coordinates and the forces */
memcpy(state->x, pos[Min], nat*sizeof(state->x[0]));
memcpy(f, force[Min], nat*sizeof(f[0]));
return count;
}
void do_force(FILE *fplog,t_commrec *cr,
t_inputrec *inputrec,
int step,t_nrnb *nrnb,gmx_wallcycle_t wcycle,
gmx_localtop_t *top,
gmx_groups_t *groups,
matrix box,rvec x[],history_t *hist,
rvec f[],rvec buf[],
tensor vir_force,
t_mdatoms *mdatoms,
gmx_enerdata_t *enerd,t_fcdata *fcd,
real lambda,t_graph *graph,
t_forcerec *fr,gmx_vsite_t *vsite,rvec mu_tot,
real t,FILE *field,gmx_edsam_t ed,
int flags)
{
static rvec box_size;
int cg0,cg1,i,j;
int start,homenr;
static double mu[2*DIM];
rvec mu_tot_AB[2];
bool bSepDVDL,bStateChanged,bNS,bFillGrid,bCalcCGCM,bBS,bDoForces;
matrix boxs;
real e,v,dvdl;
t_pbc pbc;
float cycles_ppdpme,cycles_pme,cycles_force;
start = mdatoms->start;
homenr = mdatoms->homenr;
bSepDVDL = (fr->bSepDVDL && do_per_step(step,inputrec->nstlog));
clear_mat(vir_force);
if (PARTDECOMP(cr)) {
pd_cg_range(cr,&cg0,&cg1);
} else {
cg0 = 0;
if (DOMAINDECOMP(cr))
cg1 = cr->dd->ncg_tot;
else
cg1 = top->cgs.nr;
if (fr->n_tpi > 0)
cg1--;
}
bStateChanged = (flags & GMX_FORCE_STATECHANGED);
bNS = (flags & GMX_FORCE_NS);
bFillGrid = (bNS && bStateChanged);
bCalcCGCM = (bFillGrid && !DOMAINDECOMP(cr));
bDoForces = (flags & GMX_FORCE_FORCES);
if (bStateChanged) {
update_forcerec(fplog,fr,box);
/* Calculate total (local) dipole moment in a temporary common array.
* This makes it possible to sum them over nodes faster.
*/
calc_mu(start,homenr,
x,mdatoms->chargeA,mdatoms->chargeB,mdatoms->nChargePerturbed,
mu,mu+DIM);
}
if (fr->ePBC != epbcNONE) {
/* Compute shift vectors every step,
* because of pressure coupling or box deformation!
*/
if (DYNAMIC_BOX(*inputrec) && bStateChanged)
calc_shifts(box,fr->shift_vec);
if (bCalcCGCM) {
put_charge_groups_in_box(fplog,cg0,cg1,fr->ePBC,box,
&(top->cgs),x,fr->cg_cm);
inc_nrnb(nrnb,eNR_CGCM,homenr);
inc_nrnb(nrnb,eNR_RESETX,cg1-cg0);
}
else if (EI_ENERGY_MINIMIZATION(inputrec->eI) && graph) {
unshift_self(graph,box,x);
}
}
else if (bCalcCGCM) {
calc_cgcm(fplog,cg0,cg1,&(top->cgs),x,fr->cg_cm);
inc_nrnb(nrnb,eNR_CGCM,homenr);
}
if (bCalcCGCM) {
if (PAR(cr)) {
move_cgcm(fplog,cr,fr->cg_cm);
}
if (gmx_debug_at)
pr_rvecs(debug,0,"cgcm",fr->cg_cm,top->cgs.nr);
}
#ifdef GMX_MPI
if (!(cr->duty & DUTY_PME)) {
/* Send particle coordinates to the pme nodes.
* Since this is only implemented for domain decomposition
* and domain decomposition does not use the graph,
* we do not need to worry about shifting.
*/
wallcycle_start(wcycle,ewcPP_PMESENDX);
GMX_MPE_LOG(ev_send_coordinates_start);
bBS = (inputrec->nwall == 2);
if (bBS) {
copy_mat(box,boxs);
svmul(inputrec->wall_ewald_zfac,boxs[ZZ],boxs[ZZ]);
}
gmx_pme_send_x(cr,bBS ? boxs : box,x,mdatoms->nChargePerturbed,lambda);
GMX_MPE_LOG(ev_send_coordinates_finish);
wallcycle_stop(wcycle,ewcPP_PMESENDX);
}
#endif /* GMX_MPI */
/* Communicate coordinates and sum dipole if necessary */
if (PAR(cr)) {
wallcycle_start(wcycle,ewcMOVEX);
if (DOMAINDECOMP(cr)) {
dd_move_x(cr->dd,box,x,buf);
} else {
move_x(fplog,cr,GMX_LEFT,GMX_RIGHT,x,nrnb);
}
/* When we don't need the total dipole we sum it in global_stat */
if (NEED_MUTOT(*inputrec))
gmx_sumd(2*DIM,mu,cr);
wallcycle_stop(wcycle,ewcMOVEX);
}
for(i=0; i<2; i++)
for(j=0;j<DIM;j++)
mu_tot_AB[i][j] = mu[i*DIM + j];
if (fr->efep == efepNO)
copy_rvec(mu_tot_AB[0],mu_tot);
else
for(j=0; j<DIM; j++)
mu_tot[j] = (1.0 - lambda)*mu_tot_AB[0][j] + lambda*mu_tot_AB[1][j];
/* Reset energies */
reset_energies(&(inputrec->opts),fr,bNS,enerd,MASTER(cr));
if (bNS) {
wallcycle_start(wcycle,ewcNS);
if (graph && bStateChanged)
/* Calculate intramolecular shift vectors to make molecules whole */
mk_mshift(fplog,graph,fr->ePBC,box,x);
/* Reset long range forces if necessary */
if (fr->bTwinRange) {
clear_rvecs(fr->f_twin_n,fr->f_twin);
clear_rvecs(SHIFTS,fr->fshift_twin);
}
/* Do the actual neighbour searching and if twin range electrostatics
* also do the calculation of long range forces and energies.
*/
dvdl = 0;
ns(fplog,fr,x,f,box,groups,&(inputrec->opts),top,mdatoms,
cr,nrnb,step,lambda,&dvdl,&enerd->grpp,bFillGrid,bDoForces);
if (bSepDVDL)
fprintf(fplog,sepdvdlformat,"LR non-bonded",0,dvdl);
enerd->dvdl_lr = dvdl;
enerd->term[F_DVDL] += dvdl;
wallcycle_stop(wcycle,ewcNS);
}
if (DOMAINDECOMP(cr)) {
if (!(cr->duty & DUTY_PME)) {
wallcycle_start(wcycle,ewcPPDURINGPME);
dd_force_flop_start(cr->dd,nrnb);
}
}
/* Start the force cycle counter.
* This counter is stopped in do_forcelow_level.
* No parallel communication should occur while this counter is running,
* since that will interfere with the dynamic load balancing.
*/
wallcycle_start(wcycle,ewcFORCE);
if (bDoForces) {
/* Reset PME/Ewald forces if necessary */
if (fr->bF_NoVirSum)
{
GMX_BARRIER(cr->mpi_comm_mygroup);
if (fr->bDomDec)
clear_rvecs(fr->f_novirsum_n,fr->f_novirsum);
else
clear_rvecs(homenr,fr->f_novirsum+start);
GMX_BARRIER(cr->mpi_comm_mygroup);
}
/* Copy long range forces into normal buffers */
if (fr->bTwinRange) {
for(i=0; i<fr->f_twin_n; i++)
copy_rvec(fr->f_twin[i],f[i]);
for(i=0; i<SHIFTS; i++)
copy_rvec(fr->fshift_twin[i],fr->fshift[i]);
}
else {
if (DOMAINDECOMP(cr))
clear_rvecs(cr->dd->nat_tot,f);
else
clear_rvecs(mdatoms->nr,f);
clear_rvecs(SHIFTS,fr->fshift);
}
clear_rvec(fr->vir_diag_posres);
GMX_BARRIER(cr->mpi_comm_mygroup);
}
if (inputrec->ePull == epullCONSTRAINT)
clear_pull_forces(inputrec->pull);
/* update QMMMrec, if necessary */
if(fr->bQMMM)
update_QMMMrec(cr,fr,x,mdatoms,box,top);
if ((flags & GMX_FORCE_BONDED) && top->idef.il[F_POSRES].nr > 0) {
/* Position restraints always require full pbc */
set_pbc(&pbc,inputrec->ePBC,box);
v = posres(top->idef.il[F_POSRES].nr,top->idef.il[F_POSRES].iatoms,
top->idef.iparams_posres,
(const rvec*)x,fr->f_novirsum,fr->vir_diag_posres,
inputrec->ePBC==epbcNONE ? NULL : &pbc,lambda,&dvdl,
fr->rc_scaling,fr->ePBC,fr->posres_com,fr->posres_comB);
if (bSepDVDL) {
fprintf(fplog,sepdvdlformat,
interaction_function[F_POSRES].longname,v,dvdl);
}
enerd->term[F_POSRES] += v;
enerd->term[F_DVDL] += dvdl;
inc_nrnb(nrnb,eNR_POSRES,top->idef.il[F_POSRES].nr/2);
}
/* Compute the bonded and non-bonded forces */
do_force_lowlevel(fplog,step,fr,inputrec,&(top->idef),
cr,nrnb,wcycle,mdatoms,&(inputrec->opts),
x,hist,f,enerd,fcd,box,lambda,graph,&(top->excls),mu_tot_AB,
flags,&cycles_force);
GMX_BARRIER(cr->mpi_comm_mygroup);
if (ed) {
do_flood(fplog,cr,x,f,ed,box,step);
}
if (DOMAINDECOMP(cr)) {
dd_force_flop_stop(cr->dd,nrnb);
if (wcycle)
dd_cycles_add(cr->dd,cycles_force,ddCyclF);
}
if (bDoForces) {
/* Compute forces due to electric field */
calc_f_el(MASTER(cr) ? field : NULL,
start,homenr,mdatoms->chargeA,x,f,inputrec->ex,inputrec->et,t);
/* When using PME/Ewald we compute the long range virial there.
* otherwise we do it based on long range forces from twin range
* cut-off based calculation (or not at all).
*/
/* Communicate the forces */
if (PAR(cr)) {
wallcycle_start(wcycle,ewcMOVEF);
if (DOMAINDECOMP(cr)) {
dd_move_f(cr->dd,f,buf,fr->fshift);
/* Position restraint do not introduce inter-cg forces */
if (EEL_FULL(fr->eeltype) && cr->dd->n_intercg_excl)
dd_move_f(cr->dd,fr->f_novirsum,buf,NULL);
} else {
move_f(fplog,cr,GMX_LEFT,GMX_RIGHT,f,buf,nrnb);
}
wallcycle_stop(wcycle,ewcMOVEF);
}
}
if (bDoForces) {
if (vsite) {
wallcycle_start(wcycle,ewcVSITESPREAD);
spread_vsite_f(fplog,vsite,x,f,fr->fshift,nrnb,
&top->idef,fr->ePBC,fr->bMolPBC,graph,box,cr);
wallcycle_stop(wcycle,ewcVSITESPREAD);
}
/* Calculation of the virial must be done after vsites! */
calc_virial(fplog,mdatoms->start,mdatoms->homenr,x,f,
vir_force,graph,box,nrnb,fr,inputrec->ePBC);
}
if (inputrec->ePull == epullUMBRELLA || inputrec->ePull == epullCONST_F) {
/* Calculate the center of mass forces, this requires communication,
* which is why pull_potential is called close to other communication.
* The virial contribution is calculated directly,
* which is why we call pull_potential after calc_virial.
*/
set_pbc(&pbc,inputrec->ePBC,box);
dvdl = 0;
enerd->term[F_COM_PULL] =
pull_potential(inputrec->ePull,inputrec->pull,mdatoms,&pbc,
cr,t,lambda,x,f,vir_force,&dvdl);
if (bSepDVDL)
fprintf(fplog,sepdvdlformat,"Com pull",enerd->term[F_COM_PULL],dvdl);
enerd->term[F_DVDL] += dvdl;
}
if (!(cr->duty & DUTY_PME)) {
cycles_ppdpme = wallcycle_stop(wcycle,ewcPPDURINGPME);
dd_cycles_add(cr->dd,cycles_ppdpme,ddCyclPPduringPME);
}
#ifdef GMX_MPI
if (PAR(cr) && !(cr->duty & DUTY_PME)) {
/* In case of node-splitting, the PP nodes receive the long-range
* forces, virial and energy from the PME nodes here.
*/
wallcycle_start(wcycle,ewcPP_PMEWAITRECVF);
dvdl = 0;
gmx_pme_receive_f(cr,fr->f_novirsum,fr->vir_el_recip,&e,&dvdl,
&cycles_pme);
if (bSepDVDL)
fprintf(fplog,sepdvdlformat,"PME mesh",e,dvdl);
enerd->term[F_COUL_RECIP] += e;
enerd->term[F_DVDL] += dvdl;
if (wcycle)
dd_cycles_add(cr->dd,cycles_pme,ddCyclPME);
wallcycle_stop(wcycle,ewcPP_PMEWAITRECVF);
}
#endif
if (bDoForces && fr->bF_NoVirSum) {
if (vsite) {
/* Spread the mesh force on virtual sites to the other particles...
* This is parallellized. MPI communication is performed
* if the constructing atoms aren't local.
*/
wallcycle_start(wcycle,ewcVSITESPREAD);
spread_vsite_f(fplog,vsite,x,fr->f_novirsum,NULL,nrnb,
&top->idef,fr->ePBC,fr->bMolPBC,graph,box,cr);
wallcycle_stop(wcycle,ewcVSITESPREAD);
}
/* Now add the forces, this is local */
if (fr->bDomDec) {
sum_forces(0,fr->f_novirsum_n,f,fr->f_novirsum);
} else {
sum_forces(start,start+homenr,f,fr->f_novirsum);
}
if (EEL_FULL(fr->eeltype)) {
/* Add the mesh contribution to the virial */
m_add(vir_force,fr->vir_el_recip,vir_force);
}
if (debug)
pr_rvecs(debug,0,"vir_force",vir_force,DIM);
}
/* Sum the potential energy terms from group contributions */
sum_epot(&(inputrec->opts),enerd);
if (fr->print_force >= 0 && bDoForces)
print_large_forces(stderr,mdatoms,cr,step,fr->print_force,x,f);
}
void do_force(FILE *log,t_commrec *cr,t_commrec *mcr,
t_parm *parm,t_nsborder *nsb,tensor vir_part,tensor pme_vir,
int step,t_nrnb *nrnb,t_topology *top,t_groups *grps,
rvec x[],rvec v[],rvec f[],rvec buf[],
t_mdatoms *mdatoms,real ener[],t_fcdata *fcd,bool bVerbose,
real lambda,t_graph *graph,
bool bNS,bool bNBFonly,t_forcerec *fr, rvec mu_tot,
bool bGatherOnly)
{
static rvec box_size;
static real dvdl_lr = 0;
int cg0,cg1,i,j;
int start,homenr;
static real mu_and_q[DIM+1];
real qsum;
start = START(nsb);
homenr = HOMENR(nsb);
cg0 = CG0(nsb);
cg1 = CG1(nsb);
update_forcerec(log,fr,parm->box);
/* Calculate total (local) dipole moment in a temporary common array.
* This makes it possible to sum them over nodes faster.
*/
calc_mu_and_q(nsb,x,mdatoms->chargeT,mu_and_q,mu_and_q+DIM);
if (fr->ePBC != epbcNONE) {
/* Compute shift vectors every step, because of pressure coupling! */
if (parm->ir.epc != epcNO)
calc_shifts(parm->box,box_size,fr->shift_vec);
if (bNS) {
put_charge_groups_in_box(log,cg0,cg1,parm->box,box_size,
&(top->blocks[ebCGS]),x,fr->cg_cm);
inc_nrnb(nrnb,eNR_RESETX,homenr);
} else if (parm->ir.eI==eiSteep || parm->ir.eI==eiCG)
unshift_self(graph,parm->box,x);
}
else if (bNS)
calc_cgcm(log,cg0,cg1,&(top->blocks[ebCGS]),x,fr->cg_cm);
if (bNS) {
inc_nrnb(nrnb,eNR_CGCM,cg1-cg0);
if (PAR(cr))
move_cgcm(log,cr,fr->cg_cm,nsb->workload);
if (debug)
pr_rvecs(debug,0,"cgcm",fr->cg_cm,nsb->cgtotal);
}
/* Communicate coordinates and sum dipole and net charge if necessary */
if (PAR(cr)) {
move_x(log,cr->left,cr->right,x,nsb,nrnb);
gmx_sum(DIM+1,mu_and_q,cr);
}
for(i=0;i<DIM;i++)
mu_tot[i]=mu_and_q[i];
qsum=mu_and_q[DIM];
/* Reset energies */
reset_energies(&(parm->ir.opts),grps,fr,bNS,ener);
if (bNS) {
if (fr->ePBC != epbcNONE)
/* Calculate intramolecular shift vectors to make molecules whole */
mk_mshift(log,graph,parm->box,x);
/* Reset long range forces if necessary */
if (fr->bTwinRange) {
clear_rvecs(nsb->natoms,fr->f_twin);
clear_rvecs(SHIFTS,fr->fshift_twin);
}
/* Do the actual neighbour searching and if twin range electrostatics
* also do the calculation of long range forces and energies.
*/
dvdl_lr = 0;
ns(log,fr,x,f,parm->box,grps,&(parm->ir.opts),top,mdatoms,
cr,nrnb,nsb,step,lambda,&dvdl_lr);
}
/* Reset PME/Ewald forces if necessary */
if (EEL_LR(fr->eeltype))
clear_rvecs(homenr,fr->f_pme+start);
/* Copy long range forces into normal buffers */
if (fr->bTwinRange) {
for(i=0; i<nsb->natoms; i++)
copy_rvec(fr->f_twin[i],f[i]);
for(i=0; i<SHIFTS; i++)
copy_rvec(fr->fshift_twin[i],fr->fshift[i]);
}
else {
clear_rvecs(nsb->natoms,f);
clear_rvecs(SHIFTS,fr->fshift);
}
/* Compute the forces */
force(log,step,fr,&(parm->ir),&(top->idef),nsb,cr,mcr,nrnb,grps,mdatoms,
top->atoms.grps[egcENER].nr,&(parm->ir.opts),
x,f,ener,fcd,bVerbose,parm->box,lambda,graph,&(top->atoms.excl),
bNBFonly,pme_vir,mu_tot,qsum,bGatherOnly);
/* Take long range contribution to free energy into account */
ener[F_DVDL] += dvdl_lr;
#ifdef DEBUG
if (bNS)
print_nrnb(log,nrnb);
#endif
/* The short-range virial from surrounding boxes */
clear_mat(vir_part);
calc_vir(log,SHIFTS,fr->shift_vec,fr->fshift,vir_part);
inc_nrnb(nrnb,eNR_VIRIAL,SHIFTS);
if (debug)
pr_rvecs(debug,0,"vir_shifts",vir_part,DIM);
/* Compute forces due to electric field */
calc_f_el(start,homenr,mdatoms->chargeT,f,parm->ir.ex);
/* When using PME/Ewald we compute the long range virial (pme_vir) there.
* otherwise we do it based on long range forces from twin range
* cut-off based calculation (or not at all).
*/
/* Communicate the forces */
if (PAR(cr))
move_f(log,cr->left,cr->right,f,buf,nsb,nrnb);
}