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);
}
double do_tpi(FILE *fplog, t_commrec *cr,
int nfile, const t_filenm fnm[],
const output_env_t oenv, gmx_bool bVerbose, gmx_bool gmx_unused bCompact,
int gmx_unused nstglobalcomm,
gmx_vsite_t gmx_unused *vsite, gmx_constr_t gmx_unused constr,
int gmx_unused stepout,
t_inputrec *inputrec,
gmx_mtop_t *top_global, t_fcdata *fcd,
t_state *state,
t_mdatoms *mdatoms,
t_nrnb *nrnb, gmx_wallcycle_t wcycle,
gmx_edsam_t gmx_unused ed,
t_forcerec *fr,
int gmx_unused repl_ex_nst, int gmx_unused repl_ex_nex, int gmx_unused repl_ex_seed,
gmx_membed_t gmx_unused membed,
real gmx_unused cpt_period, real gmx_unused max_hours,
const char gmx_unused *deviceOptions,
int gmx_unused imdport,
unsigned long gmx_unused Flags,
gmx_walltime_accounting_t walltime_accounting)
{
const char *TPI = "Test Particle Insertion";
gmx_localtop_t *top;
gmx_groups_t *groups;
gmx_enerdata_t *enerd;
rvec *f;
real lambda, t, temp, beta, drmax, epot;
double embU, sum_embU, *sum_UgembU, V, V_all, VembU_all;
t_trxstatus *status;
t_trxframe rerun_fr;
gmx_bool bDispCorr, bCharge, bRFExcl, bNotLastFrame, bStateChanged, bNS;
tensor force_vir, shake_vir, vir, pres;
int cg_tp, a_tp0, a_tp1, ngid, gid_tp, nener, e;
rvec *x_mol;
rvec mu_tot, x_init, dx, x_tp;
int nnodes, frame;
gmx_int64_t frame_step_prev, frame_step;
gmx_int64_t nsteps, stepblocksize = 0, step;
gmx_int64_t rnd_count_stride, rnd_count;
gmx_int64_t seed;
double rnd[4];
int i, start, end;
FILE *fp_tpi = NULL;
char *ptr, *dump_pdb, **leg, str[STRLEN], str2[STRLEN];
double dbl, dump_ener;
gmx_bool bCavity;
int nat_cavity = 0, d;
real *mass_cavity = NULL, mass_tot;
int nbin;
double invbinw, *bin, refvolshift, logV, bUlogV;
real dvdl, prescorr, enercorr, dvdlcorr;
gmx_bool bEnergyOutOfBounds;
const char *tpid_leg[2] = {"direct", "reweighted"};
/* Since there is no upper limit to the insertion energies,
* we need to set an upper limit for the distribution output.
*/
real bU_bin_limit = 50;
real bU_logV_bin_limit = bU_bin_limit + 10;
nnodes = cr->nnodes;
top = gmx_mtop_generate_local_top(top_global, inputrec);
groups = &top_global->groups;
bCavity = (inputrec->eI == eiTPIC);
if (bCavity)
{
ptr = getenv("GMX_TPIC_MASSES");
if (ptr == NULL)
{
nat_cavity = 1;
}
else
{
/* Read (multiple) masses from env var GMX_TPIC_MASSES,
* The center of mass of the last atoms is then used for TPIC.
*/
nat_cavity = 0;
while (sscanf(ptr, "%lf%n", &dbl, &i) > 0)
{
srenew(mass_cavity, nat_cavity+1);
mass_cavity[nat_cavity] = dbl;
fprintf(fplog, "mass[%d] = %f\n",
nat_cavity+1, mass_cavity[nat_cavity]);
nat_cavity++;
ptr += i;
}
if (nat_cavity == 0)
{
gmx_fatal(FARGS, "Found %d masses in GMX_TPIC_MASSES", nat_cavity);
}
}
}
/*
init_em(fplog,TPI,inputrec,&lambda,nrnb,mu_tot,
state->box,fr,mdatoms,top,cr,nfile,fnm,NULL,NULL);*/
/* We never need full pbc for TPI */
fr->ePBC = epbcXYZ;
/* Determine the temperature for the Boltzmann weighting */
temp = inputrec->opts.ref_t[0];
if (fplog)
{
for (i = 1; (i < inputrec->opts.ngtc); i++)
{
if (inputrec->opts.ref_t[i] != temp)
{
fprintf(fplog, "\nWARNING: The temperatures of the different temperature coupling groups are not identical\n\n");
fprintf(stderr, "\nWARNING: The temperatures of the different temperature coupling groups are not identical\n\n");
}
}
fprintf(fplog,
"\n The temperature for test particle insertion is %.3f K\n\n",
temp);
}
beta = 1.0/(BOLTZ*temp);
/* Number of insertions per frame */
nsteps = inputrec->nsteps;
/* Use the same neighborlist with more insertions points
* in a sphere of radius drmax around the initial point
*/
/* This should be a proper mdp parameter */
drmax = inputrec->rtpi;
/* An environment variable can be set to dump all configurations
* to pdb with an insertion energy <= this value.
*/
dump_pdb = getenv("GMX_TPI_DUMP");
dump_ener = 0;
if (dump_pdb)
{
sscanf(dump_pdb, "%lf", &dump_ener);
}
atoms2md(top_global, inputrec, 0, NULL, top_global->natoms, mdatoms);
update_mdatoms(mdatoms, inputrec->fepvals->init_lambda);
snew(enerd, 1);
init_enerdata(groups->grps[egcENER].nr, inputrec->fepvals->n_lambda, enerd);
snew(f, top_global->natoms);
/* Print to log file */
walltime_accounting_start(walltime_accounting);
wallcycle_start(wcycle, ewcRUN);
print_start(fplog, cr, walltime_accounting, "Test Particle Insertion");
/* The last charge group is the group to be inserted */
cg_tp = top->cgs.nr - 1;
a_tp0 = top->cgs.index[cg_tp];
a_tp1 = top->cgs.index[cg_tp+1];
if (debug)
{
fprintf(debug, "TPI cg %d, atoms %d-%d\n", cg_tp, a_tp0, a_tp1);
}
if (a_tp1 - a_tp0 > 1 &&
(inputrec->rlist < inputrec->rcoulomb ||
inputrec->rlist < inputrec->rvdw))
{
gmx_fatal(FARGS, "Can not do TPI for multi-atom molecule with a twin-range cut-off");
}
snew(x_mol, a_tp1-a_tp0);
bDispCorr = (inputrec->eDispCorr != edispcNO);
bCharge = FALSE;
for (i = a_tp0; i < a_tp1; i++)
{
/* Copy the coordinates of the molecule to be insterted */
copy_rvec(state->x[i], x_mol[i-a_tp0]);
/* Check if we need to print electrostatic energies */
bCharge |= (mdatoms->chargeA[i] != 0 ||
(mdatoms->chargeB && mdatoms->chargeB[i] != 0));
}
bRFExcl = (bCharge && EEL_RF(fr->eeltype) && fr->eeltype != eelRF_NEC);
calc_cgcm(fplog, cg_tp, cg_tp+1, &(top->cgs), state->x, fr->cg_cm);
if (bCavity)
{
if (norm(fr->cg_cm[cg_tp]) > 0.5*inputrec->rlist && fplog)
{
fprintf(fplog, "WARNING: Your TPI molecule is not centered at 0,0,0\n");
fprintf(stderr, "WARNING: Your TPI molecule is not centered at 0,0,0\n");
}
}
else
{
/* Center the molecule to be inserted at zero */
for (i = 0; i < a_tp1-a_tp0; i++)
{
rvec_dec(x_mol[i], fr->cg_cm[cg_tp]);
}
}
if (fplog)
{
fprintf(fplog, "\nWill insert %d atoms %s partial charges\n",
a_tp1-a_tp0, bCharge ? "with" : "without");
fprintf(fplog, "\nWill insert %d times in each frame of %s\n",
(int)nsteps, opt2fn("-rerun", nfile, fnm));
}
if (!bCavity)
{
if (inputrec->nstlist > 1)
{
if (drmax == 0 && a_tp1-a_tp0 == 1)
{
gmx_fatal(FARGS, "Re-using the neighborlist %d times for insertions of a single atom in a sphere of radius %f does not make sense", inputrec->nstlist, drmax);
}
if (fplog)
{
fprintf(fplog, "Will use the same neighborlist for %d insertions in a sphere of radius %f\n", inputrec->nstlist, drmax);
}
}
}
else
{
if (fplog)
{
fprintf(fplog, "Will insert randomly in a sphere of radius %f around the center of the cavity\n", drmax);
}
}
ngid = groups->grps[egcENER].nr;
gid_tp = GET_CGINFO_GID(fr->cginfo[cg_tp]);
nener = 1 + ngid;
if (bDispCorr)
{
nener += 1;
}
if (bCharge)
{
nener += ngid;
if (bRFExcl)
{
nener += 1;
}
if (EEL_FULL(fr->eeltype))
{
nener += 1;
}
}
snew(sum_UgembU, nener);
/* Copy the random seed set by the user */
seed = inputrec->ld_seed;
/* We use the frame step number as one random counter.
* The second counter use the insertion (step) count. But we
* need multiple random numbers per insertion. This number is
* not fixed, since we generate random locations in a sphere
* by putting locations in a cube and some of these fail.
* A count of 20 is already extremely unlikely, so 10000 is
* a safe margin for random numbers per insertion.
*/
rnd_count_stride = 10000;
if (MASTER(cr))
{
fp_tpi = xvgropen(opt2fn("-tpi", nfile, fnm),
"TPI energies", "Time (ps)",
"(kJ mol\\S-1\\N) / (nm\\S3\\N)", oenv);
xvgr_subtitle(fp_tpi, "f. are averages over one frame", oenv);
snew(leg, 4+nener);
e = 0;
sprintf(str, "-kT log(<Ve\\S-\\betaU\\N>/<V>)");
leg[e++] = strdup(str);
sprintf(str, "f. -kT log<e\\S-\\betaU\\N>");
leg[e++] = strdup(str);
sprintf(str, "f. <e\\S-\\betaU\\N>");
leg[e++] = strdup(str);
sprintf(str, "f. V");
leg[e++] = strdup(str);
sprintf(str, "f. <Ue\\S-\\betaU\\N>");
leg[e++] = strdup(str);
for (i = 0; i < ngid; i++)
{
sprintf(str, "f. <U\\sVdW %s\\Ne\\S-\\betaU\\N>",
*(groups->grpname[groups->grps[egcENER].nm_ind[i]]));
leg[e++] = strdup(str);
}
if (bDispCorr)
{
sprintf(str, "f. <U\\sdisp c\\Ne\\S-\\betaU\\N>");
leg[e++] = strdup(str);
}
if (bCharge)
{
for (i = 0; i < ngid; i++)
{
sprintf(str, "f. <U\\sCoul %s\\Ne\\S-\\betaU\\N>",
*(groups->grpname[groups->grps[egcENER].nm_ind[i]]));
leg[e++] = strdup(str);
}
if (bRFExcl)
{
sprintf(str, "f. <U\\sRF excl\\Ne\\S-\\betaU\\N>");
leg[e++] = strdup(str);
}
if (EEL_FULL(fr->eeltype))
{
sprintf(str, "f. <U\\sCoul recip\\Ne\\S-\\betaU\\N>");
leg[e++] = strdup(str);
}
}
xvgr_legend(fp_tpi, 4+nener, (const char**)leg, oenv);
for (i = 0; i < 4+nener; i++)
{
sfree(leg[i]);
}
sfree(leg);
}
clear_rvec(x_init);
V_all = 0;
VembU_all = 0;
invbinw = 10;
nbin = 10;
snew(bin, nbin);
/* Avoid frame step numbers <= -1 */
frame_step_prev = -1;
bNotLastFrame = read_first_frame(oenv, &status, opt2fn("-rerun", nfile, fnm),
&rerun_fr, TRX_NEED_X);
frame = 0;
if (rerun_fr.natoms - (bCavity ? nat_cavity : 0) !=
mdatoms->nr - (a_tp1 - a_tp0))
{
gmx_fatal(FARGS, "Number of atoms in trajectory (%d)%s "
"is not equal the number in the run input file (%d) "
"minus the number of atoms to insert (%d)\n",
rerun_fr.natoms, bCavity ? " minus one" : "",
mdatoms->nr, a_tp1-a_tp0);
}
refvolshift = log(det(rerun_fr.box));
switch (inputrec->eI)
{
case eiTPI:
stepblocksize = inputrec->nstlist;
break;
case eiTPIC:
stepblocksize = 1;
break;
default:
gmx_fatal(FARGS, "Unknown integrator %s", ei_names[inputrec->eI]);
}
#ifdef GMX_SIMD
/* Make sure we don't detect SIMD overflow generated before this point */
gmx_simd_check_and_reset_overflow();
#endif
while (bNotLastFrame)
{
frame_step = rerun_fr.step;
if (frame_step <= frame_step_prev)
{
/* We don't have step number in the trajectory file,
* or we have constant or decreasing step numbers.
* Ensure we have increasing step numbers, since we use
* the step numbers as a counter for random numbers.
*/
frame_step = frame_step_prev + 1;
}
frame_step_prev = frame_step;
lambda = rerun_fr.lambda;
t = rerun_fr.time;
sum_embU = 0;
for (e = 0; e < nener; e++)
{
sum_UgembU[e] = 0;
}
/* Copy the coordinates from the input trajectory */
for (i = 0; i < rerun_fr.natoms; i++)
{
copy_rvec(rerun_fr.x[i], state->x[i]);
}
copy_mat(rerun_fr.box, state->box);
V = det(state->box);
logV = log(V);
bStateChanged = TRUE;
bNS = TRUE;
step = cr->nodeid*stepblocksize;
while (step < nsteps)
{
/* Initialize the second counter for random numbers using
* the insertion step index. This ensures that we get
* the same random numbers independently of how many
* MPI ranks we use. Also for the same seed, we get
* the same initial random sequence for different nsteps.
*/
rnd_count = step*rnd_count_stride;
if (!bCavity)
{
/* Random insertion in the whole volume */
bNS = (step % inputrec->nstlist == 0);
if (bNS)
{
/* Generate a random position in the box */
gmx_rng_cycle_2uniform(frame_step, rnd_count++, seed, RND_SEED_TPI, rnd);
gmx_rng_cycle_2uniform(frame_step, rnd_count++, seed, RND_SEED_TPI, rnd+2);
for (d = 0; d < DIM; d++)
{
x_init[d] = rnd[d]*state->box[d][d];
}
}
if (inputrec->nstlist == 1)
{
copy_rvec(x_init, x_tp);
}
else
{
/* Generate coordinates within |dx|=drmax of x_init */
do
{
gmx_rng_cycle_2uniform(frame_step, rnd_count++, seed, RND_SEED_TPI, rnd);
gmx_rng_cycle_2uniform(frame_step, rnd_count++, seed, RND_SEED_TPI, rnd+2);
for (d = 0; d < DIM; d++)
{
dx[d] = (2*rnd[d] - 1)*drmax;
}
}
while (norm2(dx) > drmax*drmax);
rvec_add(x_init, dx, x_tp);
}
}
else
{
/* Random insertion around a cavity location
* given by the last coordinate of the trajectory.
*/
if (step == 0)
{
if (nat_cavity == 1)
{
/* Copy the location of the cavity */
copy_rvec(rerun_fr.x[rerun_fr.natoms-1], x_init);
}
else
{
/* Determine the center of mass of the last molecule */
clear_rvec(x_init);
mass_tot = 0;
for (i = 0; i < nat_cavity; i++)
{
for (d = 0; d < DIM; d++)
{
x_init[d] +=
mass_cavity[i]*rerun_fr.x[rerun_fr.natoms-nat_cavity+i][d];
}
mass_tot += mass_cavity[i];
}
for (d = 0; d < DIM; d++)
{
x_init[d] /= mass_tot;
}
}
}
/* Generate coordinates within |dx|=drmax of x_init */
do
{
gmx_rng_cycle_2uniform(frame_step, rnd_count++, seed, RND_SEED_TPI, rnd);
gmx_rng_cycle_2uniform(frame_step, rnd_count++, seed, RND_SEED_TPI, rnd+2);
for (d = 0; d < DIM; d++)
{
dx[d] = (2*rnd[d] - 1)*drmax;
}
}
while (norm2(dx) > drmax*drmax);
rvec_add(x_init, dx, x_tp);
}
if (a_tp1 - a_tp0 == 1)
{
/* Insert a single atom, just copy the insertion location */
copy_rvec(x_tp, state->x[a_tp0]);
}
else
{
/* Copy the coordinates from the top file */
for (i = a_tp0; i < a_tp1; i++)
{
copy_rvec(x_mol[i-a_tp0], state->x[i]);
}
/* Rotate the molecule randomly */
gmx_rng_cycle_2uniform(frame_step, rnd_count++, seed, RND_SEED_TPI, rnd);
gmx_rng_cycle_2uniform(frame_step, rnd_count++, seed, RND_SEED_TPI, rnd+2);
rotate_conf(a_tp1-a_tp0, state->x+a_tp0, NULL,
2*M_PI*rnd[0],
2*M_PI*rnd[1],
2*M_PI*rnd[2]);
/* Shift to the insertion location */
for (i = a_tp0; i < a_tp1; i++)
{
rvec_inc(state->x[i], x_tp);
}
}
/* Clear some matrix variables */
clear_mat(force_vir);
clear_mat(shake_vir);
clear_mat(vir);
clear_mat(pres);
/* Set the charge group center of mass of the test particle */
copy_rvec(x_init, fr->cg_cm[top->cgs.nr-1]);
/* Calc energy (no forces) on new positions.
* Since we only need the intermolecular energy
* and the RF exclusion terms of the inserted molecule occur
* within a single charge group we can pass NULL for the graph.
* This also avoids shifts that would move charge groups
* out of the box.
*
* Some checks above ensure than we can not have
* twin-range interactions together with nstlist > 1,
* therefore we do not need to remember the LR energies.
*/
/* Make do_force do a single node force calculation */
cr->nnodes = 1;
do_force(fplog, cr, inputrec,
step, nrnb, wcycle, top, &top_global->groups,
state->box, state->x, &state->hist,
f, force_vir, mdatoms, enerd, fcd,
state->lambda,
NULL, fr, NULL, mu_tot, t, NULL, NULL, FALSE,
GMX_FORCE_NONBONDED | GMX_FORCE_ENERGY |
(bNS ? GMX_FORCE_DYNAMICBOX | GMX_FORCE_NS | GMX_FORCE_DO_LR : 0) |
(bStateChanged ? GMX_FORCE_STATECHANGED : 0));
cr->nnodes = nnodes;
bStateChanged = FALSE;
bNS = FALSE;
/* Calculate long range corrections to pressure and energy */
calc_dispcorr(fplog, inputrec, fr, step, top_global->natoms, state->box,
lambda, pres, vir, &prescorr, &enercorr, &dvdlcorr);
/* figure out how to rearrange the next 4 lines MRS 8/4/2009 */
enerd->term[F_DISPCORR] = enercorr;
enerd->term[F_EPOT] += enercorr;
enerd->term[F_PRES] += prescorr;
enerd->term[F_DVDL_VDW] += dvdlcorr;
epot = enerd->term[F_EPOT];
bEnergyOutOfBounds = FALSE;
#ifdef GMX_SIMD_X86_SSE2_OR_HIGHER
/* With SSE the energy can overflow, check for this */
if (gmx_mm_check_and_reset_overflow())
{
if (debug)
{
fprintf(debug, "Found an SSE overflow, assuming the energy is out of bounds\n");
}
bEnergyOutOfBounds = TRUE;
}
#endif
/* If the compiler doesn't optimize this check away
* we catch the NAN energies.
* The epot>GMX_REAL_MAX check catches inf values,
* which should nicely result in embU=0 through the exp below,
* but it does not hurt to check anyhow.
*/
/* Non-bonded Interaction usually diverge at r=0.
* With tabulated interaction functions the first few entries
* should be capped in a consistent fashion between
* repulsion, dispersion and Coulomb to avoid accidental
* negative values in the total energy.
* The table generation code in tables.c does this.
* With user tbales the user should take care of this.
*/
if (epot != epot || epot > GMX_REAL_MAX)
{
bEnergyOutOfBounds = TRUE;
}
if (bEnergyOutOfBounds)
{
if (debug)
{
fprintf(debug, "\n time %.3f, step %d: non-finite energy %f, using exp(-bU)=0\n", t, (int)step, epot);
}
embU = 0;
}
else
{
embU = exp(-beta*epot);
sum_embU += embU;
/* Determine the weighted energy contributions of each energy group */
e = 0;
sum_UgembU[e++] += epot*embU;
if (fr->bBHAM)
{
for (i = 0; i < ngid; i++)
{
sum_UgembU[e++] +=
(enerd->grpp.ener[egBHAMSR][GID(i, gid_tp, ngid)] +
enerd->grpp.ener[egBHAMLR][GID(i, gid_tp, ngid)])*embU;
}
}
else
{
for (i = 0; i < ngid; i++)
{
sum_UgembU[e++] +=
(enerd->grpp.ener[egLJSR][GID(i, gid_tp, ngid)] +
enerd->grpp.ener[egLJLR][GID(i, gid_tp, ngid)])*embU;
}
}
if (bDispCorr)
{
sum_UgembU[e++] += enerd->term[F_DISPCORR]*embU;
}
if (bCharge)
{
for (i = 0; i < ngid; i++)
{
sum_UgembU[e++] +=
(enerd->grpp.ener[egCOULSR][GID(i, gid_tp, ngid)] +
enerd->grpp.ener[egCOULLR][GID(i, gid_tp, ngid)])*embU;
}
if (bRFExcl)
{
sum_UgembU[e++] += enerd->term[F_RF_EXCL]*embU;
}
if (EEL_FULL(fr->eeltype))
{
sum_UgembU[e++] += enerd->term[F_COUL_RECIP]*embU;
}
}
}
if (embU == 0 || beta*epot > bU_bin_limit)
{
bin[0]++;
}
else
{
i = (int)((bU_logV_bin_limit
- (beta*epot - logV + refvolshift))*invbinw
+ 0.5);
if (i < 0)
{
i = 0;
}
if (i >= nbin)
{
realloc_bins(&bin, &nbin, i+10);
}
bin[i]++;
}
if (debug)
{
fprintf(debug, "TPI %7d %12.5e %12.5f %12.5f %12.5f\n",
(int)step, epot, x_tp[XX], x_tp[YY], x_tp[ZZ]);
}
if (dump_pdb && epot <= dump_ener)
{
sprintf(str, "t%g_step%d.pdb", t, (int)step);
sprintf(str2, "t: %f step %d ener: %f", t, (int)step, epot);
write_sto_conf_mtop(str, str2, top_global, state->x, state->v,
inputrec->ePBC, state->box);
}
step++;
if ((step/stepblocksize) % cr->nnodes != cr->nodeid)
{
/* Skip all steps assigned to the other MPI ranks */
step += (cr->nnodes - 1)*stepblocksize;
}
}
if (PAR(cr))
{
/* When running in parallel sum the energies over the processes */
gmx_sumd(1, &sum_embU, cr);
gmx_sumd(nener, sum_UgembU, cr);
}
frame++;
V_all += V;
VembU_all += V*sum_embU/nsteps;
if (fp_tpi)
{
if (bVerbose || frame%10 == 0 || frame < 10)
{
fprintf(stderr, "mu %10.3e <mu> %10.3e\n",
-log(sum_embU/nsteps)/beta, -log(VembU_all/V_all)/beta);
}
fprintf(fp_tpi, "%10.3f %12.5e %12.5e %12.5e %12.5e",
t,
VembU_all == 0 ? 20/beta : -log(VembU_all/V_all)/beta,
sum_embU == 0 ? 20/beta : -log(sum_embU/nsteps)/beta,
sum_embU/nsteps, V);
for (e = 0; e < nener; e++)
{
fprintf(fp_tpi, " %12.5e", sum_UgembU[e]/nsteps);
}
fprintf(fp_tpi, "\n");
fflush(fp_tpi);
}
bNotLastFrame = read_next_frame(oenv, status, &rerun_fr);
} /* End of the loop */
walltime_accounting_end(walltime_accounting);
close_trj(status);
if (fp_tpi != NULL)
{
gmx_fio_fclose(fp_tpi);
}
if (fplog != NULL)
{
fprintf(fplog, "\n");
fprintf(fplog, " <V> = %12.5e nm^3\n", V_all/frame);
fprintf(fplog, " <mu> = %12.5e kJ/mol\n", -log(VembU_all/V_all)/beta);
}
/* Write the Boltzmann factor histogram */
if (PAR(cr))
{
/* When running in parallel sum the bins over the processes */
i = nbin;
global_max(cr, &i);
realloc_bins(&bin, &nbin, i);
gmx_sumd(nbin, bin, cr);
}
if (MASTER(cr))
{
fp_tpi = xvgropen(opt2fn("-tpid", nfile, fnm),
"TPI energy distribution",
"\\betaU - log(V/<V>)", "count", oenv);
sprintf(str, "number \\betaU > %g: %9.3e", bU_bin_limit, bin[0]);
xvgr_subtitle(fp_tpi, str, oenv);
xvgr_legend(fp_tpi, 2, (const char **)tpid_leg, oenv);
for (i = nbin-1; i > 0; i--)
{
bUlogV = -i/invbinw + bU_logV_bin_limit - refvolshift + log(V_all/frame);
fprintf(fp_tpi, "%6.2f %10d %12.5e\n",
bUlogV,
(int)(bin[i]+0.5),
bin[i]*exp(-bUlogV)*V_all/VembU_all);
}
gmx_fio_fclose(fp_tpi);
}
sfree(bin);
sfree(sum_UgembU);
walltime_accounting_set_nsteps_done(walltime_accounting, frame*inputrec->nsteps);
return 0;
}
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);
}
