t_mdebin *init_mdebin(ener_file_t fp_ene,
const gmx_mtop_t *mtop,
const t_inputrec *ir,
FILE *fp_dhdl)
{
const char *ener_nm[F_NRE];
static const char *vir_nm[] = {
"Vir-XX", "Vir-XY", "Vir-XZ",
"Vir-YX", "Vir-YY", "Vir-YZ",
"Vir-ZX", "Vir-ZY", "Vir-ZZ"
};
static const char *sv_nm[] = {
"ShakeVir-XX", "ShakeVir-XY", "ShakeVir-XZ",
"ShakeVir-YX", "ShakeVir-YY", "ShakeVir-YZ",
"ShakeVir-ZX", "ShakeVir-ZY", "ShakeVir-ZZ"
};
static const char *fv_nm[] = {
"ForceVir-XX", "ForceVir-XY", "ForceVir-XZ",
"ForceVir-YX", "ForceVir-YY", "ForceVir-YZ",
"ForceVir-ZX", "ForceVir-ZY", "ForceVir-ZZ"
};
static const char *pres_nm[] = {
"Pres-XX", "Pres-XY", "Pres-XZ",
"Pres-YX", "Pres-YY", "Pres-YZ",
"Pres-ZX", "Pres-ZY", "Pres-ZZ"
};
static const char *surft_nm[] = {
"#Surf*SurfTen"
};
static const char *mu_nm[] = {
"Mu-X", "Mu-Y", "Mu-Z"
};
static const char *vcos_nm[] = {
"2CosZ*Vel-X"
};
static const char *visc_nm[] = {
"1/Viscosity"
};
static const char *baro_nm[] = {
"Barostat"
};
char **grpnms;
const gmx_groups_t *groups;
char **gnm;
char buf[256];
const char *bufi;
t_mdebin *md;
int i, j, ni, nj, n, k, kk, ncon, nset;
gmx_bool bBHAM, b14;
snew(md, 1);
if (EI_DYNAMICS(ir->eI))
{
md->delta_t = ir->delta_t;
}
else
{
md->delta_t = 0;
}
groups = &mtop->groups;
bBHAM = (mtop->ffparams.functype[0] == F_BHAM);
b14 = (gmx_mtop_ftype_count(mtop, F_LJ14) > 0 ||
gmx_mtop_ftype_count(mtop, F_LJC14_Q) > 0);
ncon = gmx_mtop_ftype_count(mtop, F_CONSTR);
nset = gmx_mtop_ftype_count(mtop, F_SETTLE);
md->bConstr = (ncon > 0 || nset > 0);
md->bConstrVir = FALSE;
if (md->bConstr)
{
if (ncon > 0 && ir->eConstrAlg == econtLINCS)
{
md->nCrmsd = 1;
}
md->bConstrVir = (getenv("GMX_CONSTRAINTVIR") != NULL);
}
else
{
md->nCrmsd = 0;
}
/* Energy monitoring */
for (i = 0; i < egNR; i++)
{
md->bEInd[i] = FALSE;
}
for (i = 0; i < F_NRE; i++)
{
md->bEner[i] = FALSE;
if (i == F_LJ)
{
md->bEner[i] = !bBHAM;
}
else if (i == F_BHAM)
{
md->bEner[i] = bBHAM;
}
else if (i == F_EQM)
{
md->bEner[i] = ir->bQMMM;
}
else if (i == F_RF_EXCL)
{
md->bEner[i] = (EEL_RF(ir->coulombtype) && ir->cutoff_scheme == ecutsGROUP);
}
else if (i == F_COUL_RECIP)
{
md->bEner[i] = EEL_FULL(ir->coulombtype);
}
else if (i == F_LJ_RECIP)
{
md->bEner[i] = EVDW_PME(ir->vdwtype);
}
else if (i == F_LJ14)
{
md->bEner[i] = b14;
}
else if (i == F_COUL14)
{
md->bEner[i] = b14;
}
else if (i == F_LJC14_Q || i == F_LJC_PAIRS_NB)
{
md->bEner[i] = FALSE;
}
else if ((i == F_DVDL_COUL && ir->fepvals->separate_dvdl[efptCOUL]) ||
(i == F_DVDL_VDW && ir->fepvals->separate_dvdl[efptVDW]) ||
(i == F_DVDL_BONDED && ir->fepvals->separate_dvdl[efptBONDED]) ||
(i == F_DVDL_RESTRAINT && ir->fepvals->separate_dvdl[efptRESTRAINT]) ||
(i == F_DKDL && ir->fepvals->separate_dvdl[efptMASS]) ||
(i == F_DVDL && ir->fepvals->separate_dvdl[efptFEP]))
{
md->bEner[i] = (ir->efep != efepNO);
}
else if ((interaction_function[i].flags & IF_VSITE) ||
(i == F_CONSTR) || (i == F_CONSTRNC) || (i == F_SETTLE))
{
md->bEner[i] = FALSE;
}
else if ((i == F_COUL_SR) || (i == F_EPOT) || (i == F_PRES) || (i == F_EQM))
{
md->bEner[i] = TRUE;
}
else if ((i == F_GBPOL) && ir->implicit_solvent == eisGBSA)
{
md->bEner[i] = TRUE;
}
else if ((i == F_NPSOLVATION) && ir->implicit_solvent == eisGBSA && (ir->sa_algorithm != esaNO))
{
md->bEner[i] = TRUE;
}
else if ((i == F_GB12) || (i == F_GB13) || (i == F_GB14))
{
md->bEner[i] = FALSE;
}
else if ((i == F_ETOT) || (i == F_EKIN) || (i == F_TEMP))
{
md->bEner[i] = EI_DYNAMICS(ir->eI);
}
else if (i == F_DISPCORR || i == F_PDISPCORR)
{
md->bEner[i] = (ir->eDispCorr != edispcNO);
}
else if (i == F_DISRESVIOL)
{
md->bEner[i] = (gmx_mtop_ftype_count(mtop, F_DISRES) > 0);
}
else if (i == F_ORIRESDEV)
{
md->bEner[i] = (gmx_mtop_ftype_count(mtop, F_ORIRES) > 0);
}
else if (i == F_CONNBONDS)
{
md->bEner[i] = FALSE;
}
else if (i == F_COM_PULL)
{
md->bEner[i] = (ir->bPull && pull_have_potential(ir->pull_work));
}
else if (i == F_ECONSERVED)
{
md->bEner[i] = ((ir->etc == etcNOSEHOOVER || ir->etc == etcVRESCALE) &&
(ir->epc == epcNO || ir->epc == epcMTTK));
}
else
{
md->bEner[i] = (gmx_mtop_ftype_count(mtop, i) > 0);
}
}
md->f_nre = 0;
for (i = 0; i < F_NRE; i++)
{
if (md->bEner[i])
{
ener_nm[md->f_nre] = interaction_function[i].longname;
md->f_nre++;
}
}
md->epc = ir->epc;
md->bDiagPres = !TRICLINIC(ir->ref_p);
md->ref_p = (ir->ref_p[XX][XX]+ir->ref_p[YY][YY]+ir->ref_p[ZZ][ZZ])/DIM;
md->bTricl = TRICLINIC(ir->compress) || TRICLINIC(ir->deform);
md->bDynBox = inputrecDynamicBox(ir);
md->etc = ir->etc;
md->bNHC_trotter = inputrecNvtTrotter(ir);
md->bPrintNHChains = ir->bPrintNHChains;
md->bMTTK = (inputrecNptTrotter(ir) || inputrecNphTrotter(ir));
md->bMu = inputrecNeedMutot(ir);
md->ebin = mk_ebin();
/* Pass NULL for unit to let get_ebin_space determine the units
* for interaction_function[i].longname
*/
md->ie = get_ebin_space(md->ebin, md->f_nre, ener_nm, NULL);
if (md->nCrmsd)
{
/* This should be called directly after the call for md->ie,
* such that md->iconrmsd follows directly in the list.
*/
md->iconrmsd = get_ebin_space(md->ebin, md->nCrmsd, conrmsd_nm, "");
}
if (md->bDynBox)
{
md->ib = get_ebin_space(md->ebin,
md->bTricl ? NTRICLBOXS : NBOXS,
md->bTricl ? tricl_boxs_nm : boxs_nm,
unit_length);
md->ivol = get_ebin_space(md->ebin, 1, vol_nm, unit_volume);
md->idens = get_ebin_space(md->ebin, 1, dens_nm, unit_density_SI);
if (md->bDiagPres)
{
md->ipv = get_ebin_space(md->ebin, 1, pv_nm, unit_energy);
md->ienthalpy = get_ebin_space(md->ebin, 1, enthalpy_nm, unit_energy);
}
}
if (md->bConstrVir)
{
md->isvir = get_ebin_space(md->ebin, asize(sv_nm), sv_nm, unit_energy);
md->ifvir = get_ebin_space(md->ebin, asize(fv_nm), fv_nm, unit_energy);
}
md->ivir = get_ebin_space(md->ebin, asize(vir_nm), vir_nm, unit_energy);
md->ipres = get_ebin_space(md->ebin, asize(pres_nm), pres_nm, unit_pres_bar);
md->isurft = get_ebin_space(md->ebin, asize(surft_nm), surft_nm,
unit_surft_bar);
if (md->epc == epcPARRINELLORAHMAN || md->epc == epcMTTK)
{
md->ipc = get_ebin_space(md->ebin, md->bTricl ? 6 : 3,
boxvel_nm, unit_vel);
}
if (md->bMu)
{
md->imu = get_ebin_space(md->ebin, asize(mu_nm), mu_nm, unit_dipole_D);
}
if (ir->cos_accel != 0)
{
md->ivcos = get_ebin_space(md->ebin, asize(vcos_nm), vcos_nm, unit_vel);
md->ivisc = get_ebin_space(md->ebin, asize(visc_nm), visc_nm,
unit_invvisc_SI);
}
/* Energy monitoring */
for (i = 0; i < egNR; i++)
{
md->bEInd[i] = FALSE;
}
md->bEInd[egCOULSR] = TRUE;
md->bEInd[egLJSR ] = TRUE;
if (bBHAM)
{
md->bEInd[egLJSR] = FALSE;
md->bEInd[egBHAMSR] = TRUE;
}
if (b14)
{
md->bEInd[egLJ14] = TRUE;
md->bEInd[egCOUL14] = TRUE;
}
md->nEc = 0;
for (i = 0; (i < egNR); i++)
{
if (md->bEInd[i])
{
md->nEc++;
}
}
n = groups->grps[egcENER].nr;
md->nEg = n;
md->nE = (n*(n+1))/2;
snew(md->igrp, md->nE);
if (md->nE > 1)
{
n = 0;
snew(gnm, md->nEc);
for (k = 0; (k < md->nEc); k++)
{
snew(gnm[k], STRLEN);
}
for (i = 0; (i < groups->grps[egcENER].nr); i++)
{
ni = groups->grps[egcENER].nm_ind[i];
for (j = i; (j < groups->grps[egcENER].nr); j++)
{
nj = groups->grps[egcENER].nm_ind[j];
for (k = kk = 0; (k < egNR); k++)
{
if (md->bEInd[k])
{
sprintf(gnm[kk], "%s:%s-%s", egrp_nm[k],
*(groups->grpname[ni]), *(groups->grpname[nj]));
kk++;
}
}
md->igrp[n] = get_ebin_space(md->ebin, md->nEc,
(const char **)gnm, unit_energy);
n++;
}
}
for (k = 0; (k < md->nEc); k++)
{
sfree(gnm[k]);
}
sfree(gnm);
if (n != md->nE)
{
gmx_incons("Number of energy terms wrong");
}
}
md->nTC = groups->grps[egcTC].nr;
md->nNHC = ir->opts.nhchainlength; /* shorthand for number of NH chains */
if (md->bMTTK)
{
md->nTCP = 1; /* assume only one possible coupling system for barostat
for now */
}
else
{
md->nTCP = 0;
}
if (md->etc == etcNOSEHOOVER)
{
if (md->bNHC_trotter)
{
md->mde_n = 2*md->nNHC*md->nTC;
}
else
{
md->mde_n = 2*md->nTC;
}
if (md->epc == epcMTTK)
{
md->mdeb_n = 2*md->nNHC*md->nTCP;
}
}
else
{
md->mde_n = md->nTC;
md->mdeb_n = 0;
}
snew(md->tmp_r, md->mde_n);
snew(md->tmp_v, md->mde_n);
snew(md->grpnms, md->mde_n);
grpnms = md->grpnms;
for (i = 0; (i < md->nTC); i++)
{
ni = groups->grps[egcTC].nm_ind[i];
sprintf(buf, "T-%s", *(groups->grpname[ni]));
grpnms[i] = gmx_strdup(buf);
}
md->itemp = get_ebin_space(md->ebin, md->nTC, (const char **)grpnms,
unit_temp_K);
if (md->etc == etcNOSEHOOVER)
{
if (md->bPrintNHChains)
{
if (md->bNHC_trotter)
{
for (i = 0; (i < md->nTC); i++)
{
ni = groups->grps[egcTC].nm_ind[i];
bufi = *(groups->grpname[ni]);
for (j = 0; (j < md->nNHC); j++)
{
sprintf(buf, "Xi-%d-%s", j, bufi);
grpnms[2*(i*md->nNHC+j)] = gmx_strdup(buf);
sprintf(buf, "vXi-%d-%s", j, bufi);
grpnms[2*(i*md->nNHC+j)+1] = gmx_strdup(buf);
}
}
md->itc = get_ebin_space(md->ebin, md->mde_n,
(const char **)grpnms, unit_invtime);
if (md->bMTTK)
{
for (i = 0; (i < md->nTCP); i++)
{
bufi = baro_nm[0]; /* All barostat DOF's together for now. */
for (j = 0; (j < md->nNHC); j++)
{
sprintf(buf, "Xi-%d-%s", j, bufi);
grpnms[2*(i*md->nNHC+j)] = gmx_strdup(buf);
sprintf(buf, "vXi-%d-%s", j, bufi);
grpnms[2*(i*md->nNHC+j)+1] = gmx_strdup(buf);
}
}
md->itcb = get_ebin_space(md->ebin, md->mdeb_n,
(const char **)grpnms, unit_invtime);
}
}
else
{
for (i = 0; (i < md->nTC); i++)
{
ni = groups->grps[egcTC].nm_ind[i];
bufi = *(groups->grpname[ni]);
sprintf(buf, "Xi-%s", bufi);
grpnms[2*i] = gmx_strdup(buf);
sprintf(buf, "vXi-%s", bufi);
grpnms[2*i+1] = gmx_strdup(buf);
}
md->itc = get_ebin_space(md->ebin, md->mde_n,
(const char **)grpnms, unit_invtime);
}
}
}
else if (md->etc == etcBERENDSEN || md->etc == etcYES ||
md->etc == etcVRESCALE)
{
for (i = 0; (i < md->nTC); i++)
{
ni = groups->grps[egcTC].nm_ind[i];
sprintf(buf, "Lamb-%s", *(groups->grpname[ni]));
grpnms[i] = gmx_strdup(buf);
}
md->itc = get_ebin_space(md->ebin, md->mde_n, (const char **)grpnms, "");
}
sfree(grpnms);
md->nU = groups->grps[egcACC].nr;
if (md->nU > 1)
{
snew(grpnms, 3*md->nU);
for (i = 0; (i < md->nU); i++)
{
ni = groups->grps[egcACC].nm_ind[i];
sprintf(buf, "Ux-%s", *(groups->grpname[ni]));
grpnms[3*i+XX] = gmx_strdup(buf);
sprintf(buf, "Uy-%s", *(groups->grpname[ni]));
grpnms[3*i+YY] = gmx_strdup(buf);
sprintf(buf, "Uz-%s", *(groups->grpname[ni]));
grpnms[3*i+ZZ] = gmx_strdup(buf);
}
md->iu = get_ebin_space(md->ebin, 3*md->nU, (const char **)grpnms, unit_vel);
sfree(grpnms);
}
if (fp_ene)
{
do_enxnms(fp_ene, &md->ebin->nener, &md->ebin->enm);
}
md->print_grpnms = NULL;
/* check whether we're going to write dh histograms */
md->dhc = NULL;
if (ir->fepvals->separate_dhdl_file == esepdhdlfileNO)
{
/* Currently dh histograms are only written with dynamics */
if (EI_DYNAMICS(ir->eI))
{
snew(md->dhc, 1);
mde_delta_h_coll_init(md->dhc, ir);
}
md->fp_dhdl = NULL;
snew(md->dE, ir->fepvals->n_lambda);
}
else
{
md->fp_dhdl = fp_dhdl;
snew(md->dE, ir->fepvals->n_lambda);
}
if (ir->bSimTemp)
{
int i;
snew(md->temperatures, ir->fepvals->n_lambda);
for (i = 0; i < ir->fepvals->n_lambda; i++)
{
md->temperatures[i] = ir->simtempvals->temperatures[i];
}
}
return md;
}
void count_bonded_distances(gmx_mtop_t *mtop, const t_inputrec *ir,
double *ndistance_c, double *ndistance_simd)
{
gmx_bool bExcl;
int nst_ener_or_vir;
double nonsimd_step_frac;
int mb, nmol, ftype;
gmx_moltype_t *molt;
double ndtot_c, ndtot_simd;
#ifdef GMX_SIMD_HAVE_REAL
gmx_bool bSimdBondeds = TRUE;
#else
gmx_bool bSimdBondeds = FALSE;
#endif
bExcl = (ir->cutoff_scheme == ecutsGROUP && IR_EXCL_FORCES(*ir)
&& !EEL_FULL(ir->coulombtype));
if (bSimdBondeds)
{
/* We only have SIMD versions of these bondeds without energy and
* without shift-forces, we take that into account here.
*/
if (ir->nstcalcenergy > 0)
{
nonsimd_step_frac = 1.0/ir->nstcalcenergy;
}
else
{
nonsimd_step_frac = 0;
}
if (ir->epc != epcNO && 1.0/ir->nstpcouple > nonsimd_step_frac)
{
nonsimd_step_frac = 1.0/ir->nstpcouple;
}
}
else
{
nonsimd_step_frac = 1;
}
/* Count the number of pbc_rvec_sub calls required for bonded interactions.
* This number is also roughly proportional to the computational cost.
*/
ndtot_c = 0;
ndtot_simd = 0;
#if defined _ICC && __ICC == 1400 || defined __ICL && __ICL == 1400
#pragma novector /* Work-around for incorrect vectorization */
#endif
for (mb = 0; mb < mtop->nmolblock; mb++)
{
molt = &mtop->moltype[mtop->molblock[mb].type];
nmol = mtop->molblock[mb].nmol;
for (ftype = 0; ftype < F_NRE; ftype++)
{
int nbonds;
if (interaction_function[ftype].flags & IF_BOND)
{
double nd_c, nd_simd;
nd_c = 0;
nd_simd = 0;
/* For all interactions, except for the three exceptions
* in the switch below, #distances = #atoms - 1.
*/
switch (ftype)
{
case F_POSRES:
case F_FBPOSRES:
nd_c = 1;
break;
case F_CONNBONDS:
break;
/* These bonded potentially use SIMD */
case F_ANGLES:
case F_PDIHS:
case F_RBDIHS:
nd_c = nonsimd_step_frac *(NRAL(ftype) - 1);
nd_simd = (1 - nonsimd_step_frac)*(NRAL(ftype) - 1);
break;
default:
nd_c = NRAL(ftype) - 1;
break;
}
nbonds = nmol*molt->ilist[ftype].nr/(1 + NRAL(ftype));
ndtot_c += nbonds*nd_c;
ndtot_simd += nbonds*nd_simd;
}
}
if (bExcl)
{
ndtot_c += nmol*(molt->excls.nra - molt->atoms.nr)/2;
}
}
if (debug)
{
fprintf(debug, "nr. of distance calculations in bondeds: C %.1f SIMD %.1f\n", ndtot_c, ndtot_simd);
}
if (ndistance_c != NULL)
{
*ndistance_c = ndtot_c;
}
if (ndistance_simd != NULL)
{
*ndistance_simd = ndtot_simd;
}
}
void do_force_lowlevel(t_forcerec *fr, t_inputrec *ir,
t_idef *idef, t_commrec *cr,
t_nrnb *nrnb, gmx_wallcycle_t wcycle,
t_mdatoms *md,
rvec x[], history_t *hist,
rvec f[],
rvec f_longrange[],
gmx_enerdata_t *enerd,
t_fcdata *fcd,
gmx_localtop_t *top,
gmx_genborn_t *born,
gmx_bool bBornRadii,
matrix box,
t_lambda *fepvals,
real *lambda,
t_graph *graph,
t_blocka *excl,
rvec mu_tot[],
int flags,
float *cycles_pme)
{
int i, j;
int donb_flags;
gmx_bool bSB;
int pme_flags;
matrix boxs;
rvec box_size;
t_pbc pbc;
real dvdl_dum[efptNR], dvdl_nb[efptNR];
#ifdef GMX_MPI
double t0 = 0.0, t1, t2, t3; /* time measurement for coarse load balancing */
#endif
set_pbc(&pbc, fr->ePBC, box);
/* reset free energy components */
for (i = 0; i < efptNR; i++)
{
dvdl_nb[i] = 0;
dvdl_dum[i] = 0;
}
/* Reset box */
for (i = 0; (i < DIM); i++)
{
box_size[i] = box[i][i];
}
debug_gmx();
/* do QMMM first if requested */
if (fr->bQMMM)
{
enerd->term[F_EQM] = calculate_QMMM(cr, x, f, fr);
}
/* Call the short range functions all in one go. */
#ifdef GMX_MPI
/*#define TAKETIME ((cr->npmenodes) && (fr->timesteps < 12))*/
#define TAKETIME FALSE
if (TAKETIME)
{
MPI_Barrier(cr->mpi_comm_mygroup);
t0 = MPI_Wtime();
}
#endif
if (ir->nwall)
{
/* foreign lambda component for walls */
real dvdl_walls = do_walls(ir, fr, box, md, x, f, lambda[efptVDW],
enerd->grpp.ener[egLJSR], nrnb);
enerd->dvdl_lin[efptVDW] += dvdl_walls;
}
/* If doing GB, reset dvda and calculate the Born radii */
if (ir->implicit_solvent)
{
wallcycle_sub_start(wcycle, ewcsNONBONDED);
for (i = 0; i < born->nr; i++)
{
fr->dvda[i] = 0;
}
if (bBornRadii)
{
calc_gb_rad(cr, fr, ir, top, x, &(fr->gblist), born, md, nrnb);
}
wallcycle_sub_stop(wcycle, ewcsNONBONDED);
}
where();
/* We only do non-bonded calculation with group scheme here, the verlet
* calls are done from do_force_cutsVERLET(). */
if (fr->cutoff_scheme == ecutsGROUP && (flags & GMX_FORCE_NONBONDED))
{
donb_flags = 0;
/* Add short-range interactions */
donb_flags |= GMX_NONBONDED_DO_SR;
/* Currently all group scheme kernels always calculate (shift-)forces */
if (flags & GMX_FORCE_FORCES)
{
donb_flags |= GMX_NONBONDED_DO_FORCE;
}
if (flags & GMX_FORCE_VIRIAL)
{
donb_flags |= GMX_NONBONDED_DO_SHIFTFORCE;
}
if (flags & GMX_FORCE_ENERGY)
{
donb_flags |= GMX_NONBONDED_DO_POTENTIAL;
}
if (flags & GMX_FORCE_DO_LR)
{
donb_flags |= GMX_NONBONDED_DO_LR;
}
wallcycle_sub_start(wcycle, ewcsNONBONDED);
do_nonbonded(fr, x, f, f_longrange, md, excl,
&enerd->grpp, nrnb,
lambda, dvdl_nb, -1, -1, donb_flags);
/* If we do foreign lambda and we have soft-core interactions
* we have to recalculate the (non-linear) energies contributions.
*/
if (fepvals->n_lambda > 0 && (flags & GMX_FORCE_DHDL) && fepvals->sc_alpha != 0)
{
for (i = 0; i < enerd->n_lambda; i++)
{
real lam_i[efptNR];
for (j = 0; j < efptNR; j++)
{
lam_i[j] = (i == 0 ? lambda[j] : fepvals->all_lambda[j][i-1]);
}
reset_foreign_enerdata(enerd);
do_nonbonded(fr, x, f, f_longrange, md, excl,
&(enerd->foreign_grpp), nrnb,
lam_i, dvdl_dum, -1, -1,
(donb_flags & ~GMX_NONBONDED_DO_FORCE) | GMX_NONBONDED_DO_FOREIGNLAMBDA);
sum_epot(&(enerd->foreign_grpp), enerd->foreign_term);
enerd->enerpart_lambda[i] += enerd->foreign_term[F_EPOT];
}
}
wallcycle_sub_stop(wcycle, ewcsNONBONDED);
where();
}
/* If we are doing GB, calculate bonded forces and apply corrections
* to the solvation forces */
/* MRS: Eventually, many need to include free energy contribution here! */
if (ir->implicit_solvent)
{
wallcycle_sub_start(wcycle, ewcsLISTED);
calc_gb_forces(cr, md, born, top, x, f, fr, idef,
ir->gb_algorithm, ir->sa_algorithm, nrnb, &pbc, graph, enerd);
wallcycle_sub_stop(wcycle, ewcsLISTED);
}
#ifdef GMX_MPI
if (TAKETIME)
{
t1 = MPI_Wtime();
fr->t_fnbf += t1-t0;
}
#endif
if (fepvals->sc_alpha != 0)
{
enerd->dvdl_nonlin[efptVDW] += dvdl_nb[efptVDW];
}
else
{
enerd->dvdl_lin[efptVDW] += dvdl_nb[efptVDW];
}
if (fepvals->sc_alpha != 0)
/* even though coulomb part is linear, we already added it, beacuse we
need to go through the vdw calculation anyway */
{
enerd->dvdl_nonlin[efptCOUL] += dvdl_nb[efptCOUL];
}
else
{
enerd->dvdl_lin[efptCOUL] += dvdl_nb[efptCOUL];
}
debug_gmx();
if (debug)
{
pr_rvecs(debug, 0, "fshift after SR", fr->fshift, SHIFTS);
}
/* Shift the coordinates. Must be done before listed forces and PPPM,
* but is also necessary for SHAKE and update, therefore it can NOT
* go when no listed forces have to be evaluated.
*
* The shifting and PBC code is deliberately not timed, since with
* the Verlet scheme it only takes non-zero time with triclinic
* boxes, and even then the time is around a factor of 100 less
* than the next smallest counter.
*/
/* Here sometimes we would not need to shift with NBFonly,
* but we do so anyhow for consistency of the returned coordinates.
*/
if (graph)
{
shift_self(graph, box, x);
if (TRICLINIC(box))
{
inc_nrnb(nrnb, eNR_SHIFTX, 2*graph->nnodes);
}
else
{
inc_nrnb(nrnb, eNR_SHIFTX, graph->nnodes);
}
}
/* Check whether we need to do listed interactions or correct for exclusions */
if (fr->bMolPBC &&
((flags & GMX_FORCE_LISTED)
|| EEL_RF(fr->eeltype) || EEL_FULL(fr->eeltype) || EVDW_PME(fr->vdwtype)))
{
/* TODO There are no electrostatics methods that require this
transformation, when using the Verlet scheme, so update the
above conditional. */
/* Since all atoms are in the rectangular or triclinic unit-cell,
* only single box vector shifts (2 in x) are required.
*/
set_pbc_dd(&pbc, fr->ePBC, cr->dd, TRUE, box);
}
debug_gmx();
do_force_listed(wcycle, box, ir->fepvals, cr->ms,
idef, (const rvec *) x, hist, f, fr,
&pbc, graph, enerd, nrnb, lambda, md, fcd,
DOMAINDECOMP(cr) ? cr->dd->gatindex : NULL,
flags);
where();
*cycles_pme = 0;
clear_mat(fr->vir_el_recip);
clear_mat(fr->vir_lj_recip);
/* Do long-range electrostatics and/or LJ-PME, including related short-range
* corrections.
*/
if (EEL_FULL(fr->eeltype) || EVDW_PME(fr->vdwtype))
{
int status = 0;
real Vlr_q = 0, Vlr_lj = 0, Vcorr_q = 0, Vcorr_lj = 0;
real dvdl_long_range_q = 0, dvdl_long_range_lj = 0;
bSB = (ir->nwall == 2);
if (bSB)
{
copy_mat(box, boxs);
svmul(ir->wall_ewald_zfac, boxs[ZZ], boxs[ZZ]);
box_size[ZZ] *= ir->wall_ewald_zfac;
}
if (EEL_PME_EWALD(fr->eeltype) || EVDW_PME(fr->vdwtype))
{
real dvdl_long_range_correction_q = 0;
real dvdl_long_range_correction_lj = 0;
/* With the Verlet scheme exclusion forces are calculated
* in the non-bonded kernel.
*/
/* The TPI molecule does not have exclusions with the rest
* of the system and no intra-molecular PME grid
* contributions will be calculated in
* gmx_pme_calc_energy.
*/
if ((ir->cutoff_scheme == ecutsGROUP && fr->n_tpi == 0) ||
ir->ewald_geometry != eewg3D ||
ir->epsilon_surface != 0)
{
int nthreads, t;
wallcycle_sub_start(wcycle, ewcsEWALD_CORRECTION);
if (fr->n_tpi > 0)
{
gmx_fatal(FARGS, "TPI with PME currently only works in a 3D geometry with tin-foil boundary conditions");
}
nthreads = fr->nthread_ewc;
#pragma omp parallel for num_threads(nthreads) schedule(static)
for (t = 0; t < nthreads; t++)
{
try
{
tensor *vir_q, *vir_lj;
real *Vcorrt_q, *Vcorrt_lj, *dvdlt_q, *dvdlt_lj;
if (t == 0)
{
vir_q = &fr->vir_el_recip;
vir_lj = &fr->vir_lj_recip;
Vcorrt_q = &Vcorr_q;
Vcorrt_lj = &Vcorr_lj;
dvdlt_q = &dvdl_long_range_correction_q;
dvdlt_lj = &dvdl_long_range_correction_lj;
}
else
{
vir_q = &fr->ewc_t[t].vir_q;
vir_lj = &fr->ewc_t[t].vir_lj;
Vcorrt_q = &fr->ewc_t[t].Vcorr_q;
Vcorrt_lj = &fr->ewc_t[t].Vcorr_lj;
dvdlt_q = &fr->ewc_t[t].dvdl[efptCOUL];
dvdlt_lj = &fr->ewc_t[t].dvdl[efptVDW];
clear_mat(*vir_q);
clear_mat(*vir_lj);
}
*dvdlt_q = 0;
*dvdlt_lj = 0;
/* Threading is only supported with the Verlet cut-off
* scheme and then only single particle forces (no
* exclusion forces) are calculated, so we can store
* the forces in the normal, single fr->f_novirsum array.
*/
ewald_LRcorrection(fr->excl_load[t], fr->excl_load[t+1],
cr, t, fr,
md->chargeA, md->chargeB,
md->sqrt_c6A, md->sqrt_c6B,
md->sigmaA, md->sigmaB,
md->sigma3A, md->sigma3B,
md->nChargePerturbed || md->nTypePerturbed,
ir->cutoff_scheme != ecutsVERLET,
excl, x, bSB ? boxs : box, mu_tot,
ir->ewald_geometry,
ir->epsilon_surface,
fr->f_novirsum, *vir_q, *vir_lj,
Vcorrt_q, Vcorrt_lj,
lambda[efptCOUL], lambda[efptVDW],
dvdlt_q, dvdlt_lj);
}
GMX_CATCH_ALL_AND_EXIT_WITH_FATAL_ERROR;
}
if (nthreads > 1)
{
reduce_thread_energies(fr->vir_el_recip, fr->vir_lj_recip,
&Vcorr_q, &Vcorr_lj,
&dvdl_long_range_correction_q,
&dvdl_long_range_correction_lj,
nthreads, fr->ewc_t);
}
wallcycle_sub_stop(wcycle, ewcsEWALD_CORRECTION);
}
void do_force_lowlevel(FILE *fplog, gmx_large_int_t step,
t_forcerec *fr, t_inputrec *ir,
t_idef *idef, t_commrec *cr,
t_nrnb *nrnb, gmx_wallcycle_t wcycle,
t_mdatoms *md,
t_grpopts *opts,
rvec x[], history_t *hist,
rvec f[],
rvec f_longrange[],
gmx_enerdata_t *enerd,
t_fcdata *fcd,
gmx_mtop_t *mtop,
gmx_localtop_t *top,
gmx_genborn_t *born,
t_atomtypes *atype,
gmx_bool bBornRadii,
matrix box,
t_lambda *fepvals,
real *lambda,
t_graph *graph,
t_blocka *excl,
rvec mu_tot[],
int flags,
float *cycles_pme)
{
int i, j, status;
int donb_flags;
gmx_bool bDoEpot, bSepDVDL, bSB;
int pme_flags;
matrix boxs;
rvec box_size;
real Vsr, Vlr, Vcorr = 0;
t_pbc pbc;
real dvdgb;
char buf[22];
double clam_i, vlam_i;
real dvdl_dum[efptNR], dvdl, dvdl_nb[efptNR], lam_i[efptNR];
real dvdlsum;
#ifdef GMX_MPI
double t0 = 0.0, t1, t2, t3; /* time measurement for coarse load balancing */
#endif
#define PRINT_SEPDVDL(s, v, dvdlambda) if (bSepDVDL) {fprintf(fplog, sepdvdlformat, s, v, dvdlambda); }
GMX_MPE_LOG(ev_force_start);
set_pbc(&pbc, fr->ePBC, box);
/* reset free energy components */
for (i = 0; i < efptNR; i++)
{
dvdl_nb[i] = 0;
dvdl_dum[i] = 0;
}
/* Reset box */
for (i = 0; (i < DIM); i++)
{
box_size[i] = box[i][i];
}
bSepDVDL = (fr->bSepDVDL && do_per_step(step, ir->nstlog));
debug_gmx();
/* do QMMM first if requested */
if (fr->bQMMM)
{
enerd->term[F_EQM] = calculate_QMMM(cr, x, f, fr, md);
}
if (bSepDVDL)
{
fprintf(fplog, "Step %s: non-bonded V and dVdl for node %d:\n",
gmx_step_str(step, buf), cr->nodeid);
}
/* Call the short range functions all in one go. */
GMX_MPE_LOG(ev_do_fnbf_start);
#ifdef GMX_MPI
/*#define TAKETIME ((cr->npmenodes) && (fr->timesteps < 12))*/
#define TAKETIME FALSE
if (TAKETIME)
{
MPI_Barrier(cr->mpi_comm_mygroup);
t0 = MPI_Wtime();
}
#endif
if (ir->nwall)
{
/* foreign lambda component for walls */
dvdl = do_walls(ir, fr, box, md, x, f, lambda[efptVDW],
enerd->grpp.ener[egLJSR], nrnb);
PRINT_SEPDVDL("Walls", 0.0, dvdl);
enerd->dvdl_lin[efptVDW] += dvdl;
}
/* If doing GB, reset dvda and calculate the Born radii */
if (ir->implicit_solvent)
{
wallcycle_sub_start(wcycle, ewcsNONBONDED);
for (i = 0; i < born->nr; i++)
{
fr->dvda[i] = 0;
}
if (bBornRadii)
{
calc_gb_rad(cr, fr, ir, top, atype, x, &(fr->gblist), born, md, nrnb);
}
wallcycle_sub_stop(wcycle, ewcsNONBONDED);
}
where();
/* We only do non-bonded calculation with group scheme here, the verlet
* calls are done from do_force_cutsVERLET(). */
if (fr->cutoff_scheme == ecutsGROUP && (flags & GMX_FORCE_NONBONDED))
{
donb_flags = 0;
/* Add short-range interactions */
donb_flags |= GMX_NONBONDED_DO_SR;
if (flags & GMX_FORCE_FORCES)
{
donb_flags |= GMX_NONBONDED_DO_FORCE;
}
if (flags & GMX_FORCE_ENERGY)
{
donb_flags |= GMX_NONBONDED_DO_POTENTIAL;
}
if (flags & GMX_FORCE_DO_LR)
{
donb_flags |= GMX_NONBONDED_DO_LR;
}
wallcycle_sub_start(wcycle, ewcsNONBONDED);
do_nonbonded(cr, fr, x, f, f_longrange, md, excl,
&enerd->grpp, box_size, nrnb,
lambda, dvdl_nb, -1, -1, donb_flags);
/* If we do foreign lambda and we have soft-core interactions
* we have to recalculate the (non-linear) energies contributions.
*/
if (fepvals->n_lambda > 0 && (flags & GMX_FORCE_DHDL) && fepvals->sc_alpha != 0)
{
for (i = 0; i < enerd->n_lambda; i++)
{
for (j = 0; j < efptNR; j++)
{
lam_i[j] = (i == 0 ? lambda[j] : fepvals->all_lambda[j][i-1]);
}
reset_foreign_enerdata(enerd);
do_nonbonded(cr, fr, x, f, f_longrange, md, excl,
&(enerd->foreign_grpp), box_size, nrnb,
lam_i, dvdl_dum, -1, -1,
(donb_flags & ~GMX_NONBONDED_DO_FORCE) | GMX_NONBONDED_DO_FOREIGNLAMBDA);
sum_epot(&ir->opts, &(enerd->foreign_grpp), enerd->foreign_term);
enerd->enerpart_lambda[i] += enerd->foreign_term[F_EPOT];
}
}
wallcycle_sub_stop(wcycle, ewcsNONBONDED);
where();
}
/* If we are doing GB, calculate bonded forces and apply corrections
* to the solvation forces */
/* MRS: Eventually, many need to include free energy contribution here! */
if (ir->implicit_solvent)
{
wallcycle_sub_start(wcycle, ewcsBONDED);
calc_gb_forces(cr, md, born, top, atype, x, f, fr, idef,
ir->gb_algorithm, ir->sa_algorithm, nrnb, bBornRadii, &pbc, graph, enerd);
wallcycle_sub_stop(wcycle, ewcsBONDED);
}
#ifdef GMX_MPI
if (TAKETIME)
{
t1 = MPI_Wtime();
fr->t_fnbf += t1-t0;
}
#endif
if (fepvals->sc_alpha != 0)
{
enerd->dvdl_nonlin[efptVDW] += dvdl_nb[efptVDW];
}
else
{
enerd->dvdl_lin[efptVDW] += dvdl_nb[efptVDW];
}
if (fepvals->sc_alpha != 0)
/* even though coulomb part is linear, we already added it, beacuse we
need to go through the vdw calculation anyway */
{
enerd->dvdl_nonlin[efptCOUL] += dvdl_nb[efptCOUL];
}
else
{
enerd->dvdl_lin[efptCOUL] += dvdl_nb[efptCOUL];
}
Vsr = 0;
if (bSepDVDL)
{
for (i = 0; i < enerd->grpp.nener; i++)
{
Vsr +=
(fr->bBHAM ?
enerd->grpp.ener[egBHAMSR][i] :
enerd->grpp.ener[egLJSR][i])
+ enerd->grpp.ener[egCOULSR][i] + enerd->grpp.ener[egGB][i];
}
dvdlsum = dvdl_nb[efptVDW] + dvdl_nb[efptCOUL];
PRINT_SEPDVDL("VdW and Coulomb SR particle-p.", Vsr, dvdlsum);
}
debug_gmx();
GMX_MPE_LOG(ev_do_fnbf_finish);
if (debug)
{
pr_rvecs(debug, 0, "fshift after SR", fr->fshift, SHIFTS);
}
/* Shift the coordinates. Must be done before bonded forces and PPPM,
* but is also necessary for SHAKE and update, therefore it can NOT
* go when no bonded forces have to be evaluated.
*/
/* Here sometimes we would not need to shift with NBFonly,
* but we do so anyhow for consistency of the returned coordinates.
*/
if (graph)
{
shift_self(graph, box, x);
if (TRICLINIC(box))
{
inc_nrnb(nrnb, eNR_SHIFTX, 2*graph->nnodes);
}
else
{
inc_nrnb(nrnb, eNR_SHIFTX, graph->nnodes);
}
}
/* Check whether we need to do bondeds or correct for exclusions */
if (fr->bMolPBC &&
((flags & GMX_FORCE_BONDED)
|| EEL_RF(fr->eeltype) || EEL_FULL(fr->eeltype)))
{
/* Since all atoms are in the rectangular or triclinic unit-cell,
* only single box vector shifts (2 in x) are required.
*/
set_pbc_dd(&pbc, fr->ePBC, cr->dd, TRUE, box);
}
debug_gmx();
if (flags & GMX_FORCE_BONDED)
{
GMX_MPE_LOG(ev_calc_bonds_start);
wallcycle_sub_start(wcycle, ewcsBONDED);
calc_bonds(fplog, cr->ms,
idef, x, hist, f, fr, &pbc, graph, enerd, nrnb, lambda, md, fcd,
DOMAINDECOMP(cr) ? cr->dd->gatindex : NULL, atype, born,
flags,
fr->bSepDVDL && do_per_step(step, ir->nstlog), step);
/* Check if we have to determine energy differences
* at foreign lambda's.
*/
if (fepvals->n_lambda > 0 && (flags & GMX_FORCE_DHDL) &&
idef->ilsort != ilsortNO_FE)
{
if (idef->ilsort != ilsortFE_SORTED)
{
gmx_incons("The bonded interactions are not sorted for free energy");
}
for (i = 0; i < enerd->n_lambda; i++)
{
reset_foreign_enerdata(enerd);
for (j = 0; j < efptNR; j++)
{
lam_i[j] = (i == 0 ? lambda[j] : fepvals->all_lambda[j][i-1]);
}
calc_bonds_lambda(fplog, idef, x, fr, &pbc, graph, &(enerd->foreign_grpp), enerd->foreign_term, nrnb, lam_i, md,
fcd, DOMAINDECOMP(cr) ? cr->dd->gatindex : NULL);
sum_epot(&ir->opts, &(enerd->foreign_grpp), enerd->foreign_term);
enerd->enerpart_lambda[i] += enerd->foreign_term[F_EPOT];
}
}
debug_gmx();
GMX_MPE_LOG(ev_calc_bonds_finish);
wallcycle_sub_stop(wcycle, ewcsBONDED);
}
where();
*cycles_pme = 0;
if (EEL_FULL(fr->eeltype))
{
bSB = (ir->nwall == 2);
if (bSB)
{
copy_mat(box, boxs);
svmul(ir->wall_ewald_zfac, boxs[ZZ], boxs[ZZ]);
box_size[ZZ] *= ir->wall_ewald_zfac;
}
clear_mat(fr->vir_el_recip);
if (fr->bEwald)
{
Vcorr = 0;
dvdl = 0;
/* With the Verlet scheme exclusion forces are calculated
* in the non-bonded kernel.
*/
/* The TPI molecule does not have exclusions with the rest
* of the system and no intra-molecular PME grid contributions
* will be calculated in gmx_pme_calc_energy.
*/
if ((ir->cutoff_scheme == ecutsGROUP && fr->n_tpi == 0) ||
ir->ewald_geometry != eewg3D ||
ir->epsilon_surface != 0)
{
int nthreads, t;
wallcycle_sub_start(wcycle, ewcsEWALD_CORRECTION);
if (fr->n_tpi > 0)
{
gmx_fatal(FARGS, "TPI with PME currently only works in a 3D geometry with tin-foil boundary conditions");
}
nthreads = gmx_omp_nthreads_get(emntBonded);
#pragma omp parallel for num_threads(nthreads) schedule(static)
for (t = 0; t < nthreads; t++)
{
int s, e, i;
rvec *fnv;
tensor *vir;
real *Vcorrt, *dvdlt;
if (t == 0)
{
fnv = fr->f_novirsum;
vir = &fr->vir_el_recip;
Vcorrt = &Vcorr;
dvdlt = &dvdl;
}
else
{
fnv = fr->f_t[t].f;
vir = &fr->f_t[t].vir;
Vcorrt = &fr->f_t[t].Vcorr;
dvdlt = &fr->f_t[t].dvdl[efptCOUL];
for (i = 0; i < fr->natoms_force; i++)
{
clear_rvec(fnv[i]);
}
clear_mat(*vir);
}
*dvdlt = 0;
*Vcorrt =
ewald_LRcorrection(fplog,
fr->excl_load[t], fr->excl_load[t+1],
cr, t, fr,
md->chargeA,
md->nChargePerturbed ? md->chargeB : NULL,
ir->cutoff_scheme != ecutsVERLET,
excl, x, bSB ? boxs : box, mu_tot,
ir->ewald_geometry,
ir->epsilon_surface,
fnv, *vir,
lambda[efptCOUL], dvdlt);
}
if (nthreads > 1)
{
reduce_thread_forces(fr->natoms_force, fr->f_novirsum,
fr->vir_el_recip,
&Vcorr, efptCOUL, &dvdl,
nthreads, fr->f_t);
}
wallcycle_sub_stop(wcycle, ewcsEWALD_CORRECTION);
}
if (fr->n_tpi == 0)
{
Vcorr += ewald_charge_correction(cr, fr, lambda[efptCOUL], box,
&dvdl, fr->vir_el_recip);
}
PRINT_SEPDVDL("Ewald excl./charge/dip. corr.", Vcorr, dvdl);
enerd->dvdl_lin[efptCOUL] += dvdl;
}
status = 0;
Vlr = 0;
dvdl = 0;
switch (fr->eeltype)
{
case eelPME:
case eelPMESWITCH:
case eelPMEUSER:
case eelPMEUSERSWITCH:
case eelP3M_AD:
if (cr->duty & DUTY_PME)
{
assert(fr->n_tpi >= 0);
if (fr->n_tpi == 0 || (flags & GMX_FORCE_STATECHANGED))
{
pme_flags = GMX_PME_SPREAD_Q | GMX_PME_SOLVE;
if (flags & GMX_FORCE_FORCES)
{
pme_flags |= GMX_PME_CALC_F;
}
if (flags & (GMX_FORCE_VIRIAL | GMX_FORCE_ENERGY))
{
pme_flags |= GMX_PME_CALC_ENER_VIR;
}
if (fr->n_tpi > 0)
{
/* We don't calculate f, but we do want the potential */
pme_flags |= GMX_PME_CALC_POT;
}
wallcycle_start(wcycle, ewcPMEMESH);
status = gmx_pme_do(fr->pmedata,
md->start, md->homenr - fr->n_tpi,
x, fr->f_novirsum,
md->chargeA, md->chargeB,
bSB ? boxs : box, cr,
DOMAINDECOMP(cr) ? dd_pme_maxshift_x(cr->dd) : 0,
DOMAINDECOMP(cr) ? dd_pme_maxshift_y(cr->dd) : 0,
nrnb, wcycle,
fr->vir_el_recip, fr->ewaldcoeff,
&Vlr, lambda[efptCOUL], &dvdl,
pme_flags);
*cycles_pme = wallcycle_stop(wcycle, ewcPMEMESH);
/* We should try to do as little computation after
* this as possible, because parallel PME synchronizes
* the nodes, so we want all load imbalance of the rest
* of the force calculation to be before the PME call.
* DD load balancing is done on the whole time of
* the force call (without PME).
*/
}
if (fr->n_tpi > 0)
{
/* Determine the PME grid energy of the test molecule
* with the PME grid potential of the other charges.
*/
gmx_pme_calc_energy(fr->pmedata, fr->n_tpi,
x + md->homenr - fr->n_tpi,
md->chargeA + md->homenr - fr->n_tpi,
&Vlr);
}
PRINT_SEPDVDL("PME mesh", Vlr, dvdl);
}
break;
case eelEWALD:
Vlr = do_ewald(fplog, FALSE, ir, x, fr->f_novirsum,
md->chargeA, md->chargeB,
box_size, cr, md->homenr,
fr->vir_el_recip, fr->ewaldcoeff,
lambda[efptCOUL], &dvdl, fr->ewald_table);
PRINT_SEPDVDL("Ewald long-range", Vlr, dvdl);
break;
default:
gmx_fatal(FARGS, "No such electrostatics method implemented %s",
eel_names[fr->eeltype]);
}
if (status != 0)
{
gmx_fatal(FARGS, "Error %d in long range electrostatics routine %s",
status, EELTYPE(fr->eeltype));
}
/* Note that with separate PME nodes we get the real energies later */
enerd->dvdl_lin[efptCOUL] += dvdl;
enerd->term[F_COUL_RECIP] = Vlr + Vcorr;
if (debug)
{
fprintf(debug, "Vlr = %g, Vcorr = %g, Vlr_corr = %g\n",
Vlr, Vcorr, enerd->term[F_COUL_RECIP]);
pr_rvecs(debug, 0, "vir_el_recip after corr", fr->vir_el_recip, DIM);
pr_rvecs(debug, 0, "fshift after LR Corrections", fr->fshift, SHIFTS);
}
}
else
{
if (EEL_RF(fr->eeltype))
{
/* With the Verlet scheme exclusion forces are calculated
* in the non-bonded kernel.
*/
if (ir->cutoff_scheme != ecutsVERLET && fr->eeltype != eelRF_NEC)
{
dvdl = 0;
enerd->term[F_RF_EXCL] =
RF_excl_correction(fplog, fr, graph, md, excl, x, f,
fr->fshift, &pbc, lambda[efptCOUL], &dvdl);
}
enerd->dvdl_lin[efptCOUL] += dvdl;
PRINT_SEPDVDL("RF exclusion correction",
enerd->term[F_RF_EXCL], dvdl);
}
}
where();
debug_gmx();
if (debug)
{
print_nrnb(debug, nrnb);
}
debug_gmx();
#ifdef GMX_MPI
if (TAKETIME)
{
t2 = MPI_Wtime();
MPI_Barrier(cr->mpi_comm_mygroup);
t3 = MPI_Wtime();
fr->t_wait += t3-t2;
if (fr->timesteps == 11)
{
fprintf(stderr, "* PP load balancing info: node %d, step %s, rel wait time=%3.0f%% , load string value: %7.2f\n",
cr->nodeid, gmx_step_str(fr->timesteps, buf),
100*fr->t_wait/(fr->t_wait+fr->t_fnbf),
(fr->t_fnbf+fr->t_wait)/fr->t_fnbf);
}
fr->timesteps++;
}
#endif
if (debug)
{
pr_rvecs(debug, 0, "fshift after bondeds", fr->fshift, SHIFTS);
}
GMX_MPE_LOG(ev_force_finish);
}
static real optimize_ncells(FILE *fplog,
int nnodes_tot,int npme_only,
bool bDynLoadBal,real dlb_scale,
gmx_mtop_t *mtop,matrix box,gmx_ddbox_t *ddbox,
t_inputrec *ir,
gmx_domdec_t *dd,
real cellsize_limit,real cutoff,
bool bInterCGBondeds,bool bInterCGMultiBody,
ivec nc)
{
int npp,npme,ndiv,*div,*mdiv,d,nmax;
bool bExcl_pbcdx;
float pbcdxr;
real limit;
ivec itry;
limit = cellsize_limit;
dd->nc[XX] = 1;
dd->nc[YY] = 1;
dd->nc[ZZ] = 1;
npp = nnodes_tot - npme_only;
if (EEL_PME(ir->coulombtype))
{
npme = (npme_only > 0 ? npme_only : npp);
}
else
{
npme = 0;
}
if (bInterCGBondeds)
{
/* For Ewald exclusions pbc_dx is not called */
bExcl_pbcdx =
(EEL_EXCL_FORCES(ir->coulombtype) && !EEL_FULL(ir->coulombtype));
pbcdxr = (double)n_bonded_dx(mtop,bExcl_pbcdx)/(double)mtop->natoms;
}
else
{
/* Every molecule is a single charge group: no pbc required */
pbcdxr = 0;
}
/* Add a margin for DLB and/or pressure scaling */
if (bDynLoadBal)
{
if (dlb_scale >= 1.0)
{
gmx_fatal(FARGS,"The value for option -dds should be smaller than 1");
}
if (fplog)
{
fprintf(fplog,"Scaling the initial minimum size with 1/%g (option -dds) = %g\n",dlb_scale,1/dlb_scale);
}
limit /= dlb_scale;
}
else if (ir->epc != epcNO)
{
if (fplog)
{
fprintf(fplog,"To account for pressure scaling, scaling the initial minimum size with %g\n",DD_GRID_MARGIN_PRES_SCALE);
limit *= DD_GRID_MARGIN_PRES_SCALE;
}
}
if (fplog)
{
fprintf(fplog,"Optimizing the DD grid for %d cells with a minimum initial size of %.3f nm\n",npp,limit);
if (limit > 0)
{
fprintf(fplog,"The maximum allowed number of cells is:");
for(d=0; d<DIM; d++)
{
nmax = (int)(ddbox->box_size[d]*ddbox->skew_fac[d]/limit);
if (d >= ddbox->npbcdim && nmax < 2)
{
nmax = 2;
}
fprintf(fplog," %c %d",'X' + d,nmax);
}
fprintf(fplog,"\n");
}
}
if (debug)
{
fprintf(debug,"Average nr of pbc_dx calls per atom %.2f\n",pbcdxr);
}
/* Decompose npp in factors */
ndiv = factorize(npp,&div,&mdiv);
itry[XX] = 1;
itry[YY] = 1;
itry[ZZ] = 1;
clear_ivec(nc);
assign_factors(dd,limit,cutoff,box,ddbox,ir,pbcdxr,
npme,ndiv,div,mdiv,itry,nc);
sfree(div);
sfree(mdiv);
return limit;
}
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_lowlevel(t_forcerec *fr, t_inputrec *ir,
t_idef *idef, t_commrec *cr,
t_nrnb *nrnb, gmx_wallcycle_t wcycle,
t_mdatoms *md,
rvec x[], history_t *hist,
rvec f[],
rvec f_longrange[],
gmx_enerdata_t *enerd,
t_fcdata *fcd,
gmx_localtop_t *top,
gmx_genborn_t *born,
gmx_bool bBornRadii,
matrix box,
t_lambda *fepvals,
real *lambda,
t_graph *graph,
t_blocka *excl,
rvec mu_tot[],
int flags,
float *cycles_pme)
{
int i, j;
int donb_flags;
gmx_bool bSB;
int pme_flags;
matrix boxs;
rvec box_size;
t_pbc pbc;
real dvdl_dum[efptNR], dvdl_nb[efptNR];
#ifdef GMX_MPI
double t0 = 0.0, t1, t2, t3; /* time measurement for coarse load balancing */
#endif
set_pbc(&pbc, fr->ePBC, box);
/* reset free energy components */
for (i = 0; i < efptNR; i++)
{
dvdl_nb[i] = 0;
dvdl_dum[i] = 0;
}
/* Reset box */
for (i = 0; (i < DIM); i++)
{
box_size[i] = box[i][i];
}
debug_gmx();
/* do QMMM first if requested */
if (fr->bQMMM)
{
enerd->term[F_EQM] = calculate_QMMM(cr, x, f, fr);
}
/* Call the short range functions all in one go. */
#ifdef GMX_MPI
/*#define TAKETIME ((cr->npmenodes) && (fr->timesteps < 12))*/
#define TAKETIME FALSE
if (TAKETIME)
{
MPI_Barrier(cr->mpi_comm_mygroup);
t0 = MPI_Wtime();
}
#endif
if (ir->nwall)
{
/* foreign lambda component for walls */
real dvdl_walls = do_walls(ir, fr, box, md, x, f, lambda[efptVDW],
enerd->grpp.ener[egLJSR], nrnb);
enerd->dvdl_lin[efptVDW] += dvdl_walls;
}
/* If doing GB, reset dvda and calculate the Born radii */
if (ir->implicit_solvent)
{
wallcycle_sub_start(wcycle, ewcsNONBONDED);
for (i = 0; i < born->nr; i++)
{
fr->dvda[i] = 0;
}
if (bBornRadii)
{
calc_gb_rad(cr, fr, ir, top, x, &(fr->gblist), born, md, nrnb);
}
wallcycle_sub_stop(wcycle, ewcsNONBONDED);
}
where();
/* We only do non-bonded calculation with group scheme here, the verlet
* calls are done from do_force_cutsVERLET(). */
if (fr->cutoff_scheme == ecutsGROUP && (flags & GMX_FORCE_NONBONDED))
{
donb_flags = 0;
/* Add short-range interactions */
donb_flags |= GMX_NONBONDED_DO_SR;
/* Currently all group scheme kernels always calculate (shift-)forces */
if (flags & GMX_FORCE_FORCES)
{
donb_flags |= GMX_NONBONDED_DO_FORCE;
}
if (flags & GMX_FORCE_VIRIAL)
{
donb_flags |= GMX_NONBONDED_DO_SHIFTFORCE;
}
if (flags & GMX_FORCE_ENERGY)
{
donb_flags |= GMX_NONBONDED_DO_POTENTIAL;
}
if (flags & GMX_FORCE_DO_LR)
{
donb_flags |= GMX_NONBONDED_DO_LR;
}
wallcycle_sub_start(wcycle, ewcsNONBONDED);
do_nonbonded(fr, x, f, f_longrange, md, excl,
&enerd->grpp, nrnb,
lambda, dvdl_nb, -1, -1, donb_flags);
/* If we do foreign lambda and we have soft-core interactions
* we have to recalculate the (non-linear) energies contributions.
*/
if (fepvals->n_lambda > 0 && (flags & GMX_FORCE_DHDL) && fepvals->sc_alpha != 0)
{
for (i = 0; i < enerd->n_lambda; i++)
{
real lam_i[efptNR];
for (j = 0; j < efptNR; j++)
{
lam_i[j] = (i == 0 ? lambda[j] : fepvals->all_lambda[j][i-1]);
}
reset_foreign_enerdata(enerd);
do_nonbonded(fr, x, f, f_longrange, md, excl,
&(enerd->foreign_grpp), nrnb,
lam_i, dvdl_dum, -1, -1,
(donb_flags & ~GMX_NONBONDED_DO_FORCE) | GMX_NONBONDED_DO_FOREIGNLAMBDA);
sum_epot(&(enerd->foreign_grpp), enerd->foreign_term);
enerd->enerpart_lambda[i] += enerd->foreign_term[F_EPOT];
}
}
wallcycle_sub_stop(wcycle, ewcsNONBONDED);
where();
}
/* If we are doing GB, calculate bonded forces and apply corrections
* to the solvation forces */
/* MRS: Eventually, many need to include free energy contribution here! */
if (ir->implicit_solvent)
{
wallcycle_sub_start(wcycle, ewcsLISTED);
calc_gb_forces(cr, md, born, top, x, f, fr, idef,
ir->gb_algorithm, ir->sa_algorithm, nrnb, &pbc, graph, enerd);
wallcycle_sub_stop(wcycle, ewcsLISTED);
}
#ifdef GMX_MPI
if (TAKETIME)
{
t1 = MPI_Wtime();
fr->t_fnbf += t1-t0;
}
#endif
if (fepvals->sc_alpha != 0)
{
enerd->dvdl_nonlin[efptVDW] += dvdl_nb[efptVDW];
}
else
{
enerd->dvdl_lin[efptVDW] += dvdl_nb[efptVDW];
}
if (fepvals->sc_alpha != 0)
/* even though coulomb part is linear, we already added it, beacuse we
need to go through the vdw calculation anyway */
{
enerd->dvdl_nonlin[efptCOUL] += dvdl_nb[efptCOUL];
}
else
{
enerd->dvdl_lin[efptCOUL] += dvdl_nb[efptCOUL];
}
debug_gmx();
if (debug)
{
pr_rvecs(debug, 0, "fshift after SR", fr->fshift, SHIFTS);
}
/* Shift the coordinates. Must be done before listed forces and PPPM,
* but is also necessary for SHAKE and update, therefore it can NOT
* go when no listed forces have to be evaluated.
*
* The shifting and PBC code is deliberately not timed, since with
* the Verlet scheme it only takes non-zero time with triclinic
* boxes, and even then the time is around a factor of 100 less
* than the next smallest counter.
*/
/* Here sometimes we would not need to shift with NBFonly,
* but we do so anyhow for consistency of the returned coordinates.
*/
if (graph)
{
shift_self(graph, box, x);
if (TRICLINIC(box))
{
inc_nrnb(nrnb, eNR_SHIFTX, 2*graph->nnodes);
}
else
{
inc_nrnb(nrnb, eNR_SHIFTX, graph->nnodes);
}
}
/* Check whether we need to do listed interactions or correct for exclusions */
if (fr->bMolPBC &&
((flags & GMX_FORCE_LISTED)
|| EEL_RF(fr->eeltype) || EEL_FULL(fr->eeltype) || EVDW_PME(fr->vdwtype)))
{
/* TODO There are no electrostatics methods that require this
transformation, when using the Verlet scheme, so update the
above conditional. */
/* Since all atoms are in the rectangular or triclinic unit-cell,
* only single box vector shifts (2 in x) are required.
*/
set_pbc_dd(&pbc, fr->ePBC, cr->dd, TRUE, box);
}
debug_gmx();
do_force_listed(wcycle, box, ir->fepvals, cr->ms,
idef, (const rvec *) x, hist, f, fr,
&pbc, graph, enerd, nrnb, lambda, md, fcd,
DOMAINDECOMP(cr) ? cr->dd->gatindex : NULL,
flags);
where();
*cycles_pme = 0;
clear_mat(fr->vir_el_recip);
clear_mat(fr->vir_lj_recip);
/* Do long-range electrostatics and/or LJ-PME, including related short-range
* corrections.
*/
if (EEL_FULL(fr->eeltype) || EVDW_PME(fr->vdwtype))
{
int status = 0;
real Vlr_q = 0, Vlr_lj = 0, Vcorr_q = 0, Vcorr_lj = 0;
real dvdl_long_range_q = 0, dvdl_long_range_lj = 0;
bSB = (ir->nwall == 2);
if (bSB)
{
copy_mat(box, boxs);
svmul(ir->wall_ewald_zfac, boxs[ZZ], boxs[ZZ]);
box_size[ZZ] *= ir->wall_ewald_zfac;
}
if (EEL_PME_EWALD(fr->eeltype) || EVDW_PME(fr->vdwtype))
{
real dvdl_long_range_correction_q = 0;
real dvdl_long_range_correction_lj = 0;
/* With the Verlet scheme exclusion forces are calculated
* in the non-bonded kernel.
*/
/* The TPI molecule does not have exclusions with the rest
* of the system and no intra-molecular PME grid
* contributions will be calculated in
* gmx_pme_calc_energy.
*/
if ((ir->cutoff_scheme == ecutsGROUP && fr->n_tpi == 0) ||
ir->ewald_geometry != eewg3D ||
ir->epsilon_surface != 0)
{
int nthreads, t;
wallcycle_sub_start(wcycle, ewcsEWALD_CORRECTION);
if (fr->n_tpi > 0)
{
gmx_fatal(FARGS, "TPI with PME currently only works in a 3D geometry with tin-foil boundary conditions");
}
nthreads = gmx_omp_nthreads_get(emntBonded);
#pragma omp parallel for num_threads(nthreads) schedule(static)
for (t = 0; t < nthreads; t++)
{
int i;
rvec *fnv;
tensor *vir_q, *vir_lj;
real *Vcorrt_q, *Vcorrt_lj, *dvdlt_q, *dvdlt_lj;
if (t == 0)
{
fnv = fr->f_novirsum;
vir_q = &fr->vir_el_recip;
vir_lj = &fr->vir_lj_recip;
Vcorrt_q = &Vcorr_q;
Vcorrt_lj = &Vcorr_lj;
dvdlt_q = &dvdl_long_range_correction_q;
dvdlt_lj = &dvdl_long_range_correction_lj;
}
else
{
fnv = fr->f_t[t].f;
vir_q = &fr->f_t[t].vir_q;
vir_lj = &fr->f_t[t].vir_lj;
Vcorrt_q = &fr->f_t[t].Vcorr_q;
Vcorrt_lj = &fr->f_t[t].Vcorr_lj;
dvdlt_q = &fr->f_t[t].dvdl[efptCOUL];
dvdlt_lj = &fr->f_t[t].dvdl[efptVDW];
for (i = 0; i < fr->natoms_force; i++)
{
clear_rvec(fnv[i]);
}
clear_mat(*vir_q);
clear_mat(*vir_lj);
}
*dvdlt_q = 0;
*dvdlt_lj = 0;
ewald_LRcorrection(fr->excl_load[t], fr->excl_load[t+1],
cr, t, fr,
md->chargeA, md->chargeB,
md->sqrt_c6A, md->sqrt_c6B,
md->sigmaA, md->sigmaB,
md->sigma3A, md->sigma3B,
md->nChargePerturbed || md->nTypePerturbed,
ir->cutoff_scheme != ecutsVERLET,
excl, x, bSB ? boxs : box, mu_tot,
ir->ewald_geometry,
ir->epsilon_surface,
fnv, *vir_q, *vir_lj,
Vcorrt_q, Vcorrt_lj,
lambda[efptCOUL], lambda[efptVDW],
dvdlt_q, dvdlt_lj);
}
if (nthreads > 1)
{
reduce_thread_forces(fr->natoms_force, fr->f_novirsum,
fr->vir_el_recip, fr->vir_lj_recip,
&Vcorr_q, &Vcorr_lj,
&dvdl_long_range_correction_q,
&dvdl_long_range_correction_lj,
nthreads, fr->f_t);
}
wallcycle_sub_stop(wcycle, ewcsEWALD_CORRECTION);
}
if (EEL_PME_EWALD(fr->eeltype) && fr->n_tpi == 0)
{
/* This is not in a subcounter because it takes a
negligible and constant-sized amount of time */
Vcorr_q += ewald_charge_correction(cr, fr, lambda[efptCOUL], box,
&dvdl_long_range_correction_q,
fr->vir_el_recip);
}
enerd->dvdl_lin[efptCOUL] += dvdl_long_range_correction_q;
enerd->dvdl_lin[efptVDW] += dvdl_long_range_correction_lj;
if ((EEL_PME(fr->eeltype) || EVDW_PME(fr->vdwtype)) && (cr->duty & DUTY_PME))
{
/* Do reciprocal PME for Coulomb and/or LJ. */
assert(fr->n_tpi >= 0);
if (fr->n_tpi == 0 || (flags & GMX_FORCE_STATECHANGED))
{
pme_flags = GMX_PME_SPREAD | GMX_PME_SOLVE;
if (EEL_PME(fr->eeltype))
{
pme_flags |= GMX_PME_DO_COULOMB;
}
if (EVDW_PME(fr->vdwtype))
{
pme_flags |= GMX_PME_DO_LJ;
}
if (flags & GMX_FORCE_FORCES)
{
pme_flags |= GMX_PME_CALC_F;
}
if (flags & GMX_FORCE_VIRIAL)
{
pme_flags |= GMX_PME_CALC_ENER_VIR;
}
if (fr->n_tpi > 0)
{
/* We don't calculate f, but we do want the potential */
pme_flags |= GMX_PME_CALC_POT;
}
wallcycle_start(wcycle, ewcPMEMESH);
status = gmx_pme_do(fr->pmedata,
0, md->homenr - fr->n_tpi,
x, fr->f_novirsum,
md->chargeA, md->chargeB,
md->sqrt_c6A, md->sqrt_c6B,
md->sigmaA, md->sigmaB,
bSB ? boxs : box, cr,
DOMAINDECOMP(cr) ? dd_pme_maxshift_x(cr->dd) : 0,
DOMAINDECOMP(cr) ? dd_pme_maxshift_y(cr->dd) : 0,
nrnb, wcycle,
fr->vir_el_recip, fr->ewaldcoeff_q,
fr->vir_lj_recip, fr->ewaldcoeff_lj,
&Vlr_q, &Vlr_lj,
lambda[efptCOUL], lambda[efptVDW],
&dvdl_long_range_q, &dvdl_long_range_lj, pme_flags);
*cycles_pme = wallcycle_stop(wcycle, ewcPMEMESH);
if (status != 0)
{
gmx_fatal(FARGS, "Error %d in reciprocal PME routine", status);
}
/* We should try to do as little computation after
* this as possible, because parallel PME synchronizes
* the nodes, so we want all load imbalance of the
* rest of the force calculation to be before the PME
* call. DD load balancing is done on the whole time
* of the force call (without PME).
*/
}
if (fr->n_tpi > 0)
{
if (EVDW_PME(ir->vdwtype))
{
gmx_fatal(FARGS, "Test particle insertion not implemented with LJ-PME");
}
/* Determine the PME grid energy of the test molecule
* with the PME grid potential of the other charges.
*/
gmx_pme_calc_energy(fr->pmedata, fr->n_tpi,
x + md->homenr - fr->n_tpi,
md->chargeA + md->homenr - fr->n_tpi,
&Vlr_q);
}
}
}
if (!EEL_PME(fr->eeltype) && EEL_PME_EWALD(fr->eeltype))
{
Vlr_q = do_ewald(ir, x, fr->f_novirsum,
md->chargeA, md->chargeB,
box_size, cr, md->homenr,
fr->vir_el_recip, fr->ewaldcoeff_q,
lambda[efptCOUL], &dvdl_long_range_q, fr->ewald_table);
}
/* Note that with separate PME nodes we get the real energies later */
enerd->dvdl_lin[efptCOUL] += dvdl_long_range_q;
enerd->dvdl_lin[efptVDW] += dvdl_long_range_lj;
enerd->term[F_COUL_RECIP] = Vlr_q + Vcorr_q;
enerd->term[F_LJ_RECIP] = Vlr_lj + Vcorr_lj;
if (debug)
{
fprintf(debug, "Vlr_q = %g, Vcorr_q = %g, Vlr_corr_q = %g\n",
Vlr_q, Vcorr_q, enerd->term[F_COUL_RECIP]);
pr_rvecs(debug, 0, "vir_el_recip after corr", fr->vir_el_recip, DIM);
pr_rvecs(debug, 0, "fshift after LR Corrections", fr->fshift, SHIFTS);
fprintf(debug, "Vlr_lj: %g, Vcorr_lj = %g, Vlr_corr_lj = %g\n",
Vlr_lj, Vcorr_lj, enerd->term[F_LJ_RECIP]);
pr_rvecs(debug, 0, "vir_lj_recip after corr", fr->vir_lj_recip, DIM);
}
}
else
{
/* Is there a reaction-field exclusion correction needed? */
if (EEL_RF(fr->eeltype) && eelRF_NEC != fr->eeltype)
{
/* With the Verlet scheme, exclusion forces are calculated
* in the non-bonded kernel.
*/
if (ir->cutoff_scheme != ecutsVERLET)
{
real dvdl_rf_excl = 0;
enerd->term[F_RF_EXCL] =
RF_excl_correction(fr, graph, md, excl, x, f,
fr->fshift, &pbc, lambda[efptCOUL], &dvdl_rf_excl);
enerd->dvdl_lin[efptCOUL] += dvdl_rf_excl;
}
}
}
where();
debug_gmx();
if (debug)
{
print_nrnb(debug, nrnb);
}
debug_gmx();
#ifdef GMX_MPI
if (TAKETIME)
{
t2 = MPI_Wtime();
MPI_Barrier(cr->mpi_comm_mygroup);
t3 = MPI_Wtime();
fr->t_wait += t3-t2;
if (fr->timesteps == 11)
{
char buf[22];
fprintf(stderr, "* PP load balancing info: rank %d, step %s, rel wait time=%3.0f%% , load string value: %7.2f\n",
cr->nodeid, gmx_step_str(fr->timesteps, buf),
100*fr->t_wait/(fr->t_wait+fr->t_fnbf),
(fr->t_fnbf+fr->t_wait)/fr->t_fnbf);
}
fr->timesteps++;
}
#endif
if (debug)
{
pr_rvecs(debug, 0, "fshift after bondeds", fr->fshift, SHIFTS);
}
}
void do_force_lowlevel(FILE *fplog, gmx_large_int_t step,
t_forcerec *fr, t_inputrec *ir,
t_idef *idef, t_commrec *cr,
t_nrnb *nrnb, gmx_wallcycle_t wcycle,
t_mdatoms *md,
t_grpopts *opts,
rvec x[], history_t *hist,
rvec f[],
gmx_enerdata_t *enerd,
t_fcdata *fcd,
gmx_mtop_t *mtop,
gmx_localtop_t *top,
gmx_genborn_t *born,
t_atomtypes *atype,
gmx_bool bBornRadii,
matrix box,
real lambda,
t_graph *graph,
t_blocka *excl,
rvec mu_tot[],
int flags,
float *cycles_pme)
{
int i,status;
int donb_flags;
gmx_bool bDoEpot,bSepDVDL,bSB;
int pme_flags;
matrix boxs;
rvec box_size;
real dvdlambda,Vsr,Vlr,Vcorr=0,vdip,vcharge;
t_pbc pbc;
real dvdgb;
char buf[22];
gmx_enerdata_t ed_lam;
double lam_i;
real dvdl_dum;
#ifdef GMX_MPI
double t0=0.0,t1,t2,t3; /* time measurement for coarse load balancing */
#endif
#define PRINT_SEPDVDL(s,v,dvdl) if (bSepDVDL) fprintf(fplog,sepdvdlformat,s,v,dvdl);
GMX_MPE_LOG(ev_force_start);
set_pbc(&pbc,fr->ePBC,box);
/* Reset box */
for(i=0; (i<DIM); i++)
{
box_size[i]=box[i][i];
}
bSepDVDL=(fr->bSepDVDL && do_per_step(step,ir->nstlog));
debug_gmx();
/* do QMMM first if requested */
if(fr->bQMMM)
{
enerd->term[F_EQM] = calculate_QMMM(cr,x,f,fr,md);
}
if (bSepDVDL)
{
fprintf(fplog,"Step %s: non-bonded V and dVdl for node %d:\n",
gmx_step_str(step,buf),cr->nodeid);
}
/* Call the short range functions all in one go. */
GMX_MPE_LOG(ev_do_fnbf_start);
dvdlambda = 0;
#ifdef GMX_MPI
/*#define TAKETIME ((cr->npmenodes) && (fr->timesteps < 12))*/
#define TAKETIME FALSE
if (TAKETIME)
{
MPI_Barrier(cr->mpi_comm_mygroup);
t0=MPI_Wtime();
}
#endif
if (ir->nwall)
{
dvdlambda = do_walls(ir,fr,box,md,x,f,lambda,
enerd->grpp.ener[egLJSR],nrnb);
PRINT_SEPDVDL("Walls",0.0,dvdlambda);
enerd->dvdl_lin += dvdlambda;
}
/* If doing GB, reset dvda and calculate the Born radii */
if (ir->implicit_solvent)
{
/* wallcycle_start(wcycle,ewcGB); */
for(i=0; i<born->nr; i++)
{
fr->dvda[i]=0;
}
if(bBornRadii)
{
calc_gb_rad(cr,fr,ir,top,atype,x,&(fr->gblist),born,md,nrnb);
}
/* wallcycle_stop(wcycle, ewcGB); */
}
where();
donb_flags = 0;
if (flags & GMX_FORCE_FORCES)
{
donb_flags |= GMX_DONB_FORCES;
}
do_nonbonded(cr,fr,x,f,md,excl,
fr->bBHAM ?
enerd->grpp.ener[egBHAMSR] :
enerd->grpp.ener[egLJSR],
enerd->grpp.ener[egCOULSR],
enerd->grpp.ener[egGB],box_size,nrnb,
lambda,&dvdlambda,-1,-1,donb_flags);
/* If we do foreign lambda and we have soft-core interactions
* we have to recalculate the (non-linear) energies contributions.
*/
if (ir->n_flambda > 0 && (flags & GMX_FORCE_DHDL) && ir->sc_alpha != 0)
{
init_enerdata(mtop->groups.grps[egcENER].nr,ir->n_flambda,&ed_lam);
for(i=0; i<enerd->n_lambda; i++)
{
lam_i = (i==0 ? lambda : ir->flambda[i-1]);
dvdl_dum = 0;
reset_enerdata(&ir->opts,fr,TRUE,&ed_lam,FALSE);
do_nonbonded(cr,fr,x,f,md,excl,
fr->bBHAM ?
ed_lam.grpp.ener[egBHAMSR] :
ed_lam.grpp.ener[egLJSR],
ed_lam.grpp.ener[egCOULSR],
enerd->grpp.ener[egGB], box_size,nrnb,
lam_i,&dvdl_dum,-1,-1,
GMX_DONB_FOREIGNLAMBDA);
sum_epot(&ir->opts,&ed_lam);
enerd->enerpart_lambda[i] += ed_lam.term[F_EPOT];
}
destroy_enerdata(&ed_lam);
}
where();
/* If we are doing GB, calculate bonded forces and apply corrections
* to the solvation forces */
if (ir->implicit_solvent) {
calc_gb_forces(cr,md,born,top,atype,x,f,fr,idef,
ir->gb_algorithm,ir->sa_algorithm,nrnb,bBornRadii,&pbc,graph,enerd);
}
#ifdef GMX_MPI
if (TAKETIME)
{
t1=MPI_Wtime();
fr->t_fnbf += t1-t0;
}
#endif
if (ir->sc_alpha != 0)
{
enerd->dvdl_nonlin += dvdlambda;
}
else
{
enerd->dvdl_lin += dvdlambda;
}
Vsr = 0;
if (bSepDVDL)
{
for(i=0; i<enerd->grpp.nener; i++)
{
Vsr +=
(fr->bBHAM ?
enerd->grpp.ener[egBHAMSR][i] :
enerd->grpp.ener[egLJSR][i])
+ enerd->grpp.ener[egCOULSR][i] + enerd->grpp.ener[egGB][i];
}
}
PRINT_SEPDVDL("VdW and Coulomb SR particle-p.",Vsr,dvdlambda);
debug_gmx();
GMX_MPE_LOG(ev_do_fnbf_finish);
if (debug)
{
pr_rvecs(debug,0,"fshift after SR",fr->fshift,SHIFTS);
}
/* Shift the coordinates. Must be done before bonded forces and PPPM,
* but is also necessary for SHAKE and update, therefore it can NOT
* go when no bonded forces have to be evaluated.
*/
/* Here sometimes we would not need to shift with NBFonly,
* but we do so anyhow for consistency of the returned coordinates.
*/
if (graph)
{
shift_self(graph,box,x);
if (TRICLINIC(box))
{
inc_nrnb(nrnb,eNR_SHIFTX,2*graph->nnodes);
}
else
{
inc_nrnb(nrnb,eNR_SHIFTX,graph->nnodes);
}
}
/* Check whether we need to do bondeds or correct for exclusions */
if (fr->bMolPBC &&
((flags & GMX_FORCE_BONDED)
|| EEL_RF(fr->eeltype) || EEL_FULL(fr->eeltype)))
{
/* Since all atoms are in the rectangular or triclinic unit-cell,
* only single box vector shifts (2 in x) are required.
*/
set_pbc_dd(&pbc,fr->ePBC,cr->dd,TRUE,box);
}
debug_gmx();
if (flags & GMX_FORCE_BONDED)
{
GMX_MPE_LOG(ev_calc_bonds_start);
calc_bonds(fplog,cr->ms,
idef,x,hist,f,fr,&pbc,graph,enerd,nrnb,lambda,md,fcd,
DOMAINDECOMP(cr) ? cr->dd->gatindex : NULL, atype, born,
fr->bSepDVDL && do_per_step(step,ir->nstlog),step);
/* Check if we have to determine energy differences
* at foreign lambda's.
*/
if (ir->n_flambda > 0 && (flags & GMX_FORCE_DHDL) &&
idef->ilsort != ilsortNO_FE)
{
if (idef->ilsort != ilsortFE_SORTED)
{
gmx_incons("The bonded interactions are not sorted for free energy");
}
init_enerdata(mtop->groups.grps[egcENER].nr,ir->n_flambda,&ed_lam);
for(i=0; i<enerd->n_lambda; i++)
{
lam_i = (i==0 ? lambda : ir->flambda[i-1]);
dvdl_dum = 0;
reset_enerdata(&ir->opts,fr,TRUE,&ed_lam,FALSE);
calc_bonds_lambda(fplog,
idef,x,fr,&pbc,graph,&ed_lam,nrnb,lam_i,md,
fcd,
DOMAINDECOMP(cr) ? cr->dd->gatindex : NULL);
sum_epot(&ir->opts,&ed_lam);
enerd->enerpart_lambda[i] += ed_lam.term[F_EPOT];
}
destroy_enerdata(&ed_lam);
}
debug_gmx();
GMX_MPE_LOG(ev_calc_bonds_finish);
}
where();
*cycles_pme = 0;
if (EEL_FULL(fr->eeltype))
{
bSB = (ir->nwall == 2);
if (bSB)
{
copy_mat(box,boxs);
svmul(ir->wall_ewald_zfac,boxs[ZZ],boxs[ZZ]);
box_size[ZZ] *= ir->wall_ewald_zfac;
}
clear_mat(fr->vir_el_recip);
if (fr->bEwald)
{
if (fr->n_tpi == 0)
{
dvdlambda = 0;
Vcorr = ewald_LRcorrection(fplog,md->start,md->start+md->homenr,
cr,fr,
md->chargeA,
md->nChargePerturbed ? md->chargeB : NULL,
excl,x,bSB ? boxs : box,mu_tot,
ir->ewald_geometry,
ir->epsilon_surface,
lambda,&dvdlambda,&vdip,&vcharge);
PRINT_SEPDVDL("Ewald excl./charge/dip. corr.",Vcorr,dvdlambda);
enerd->dvdl_lin += dvdlambda;
}
else
{
if (ir->ewald_geometry != eewg3D || ir->epsilon_surface != 0)
{
gmx_fatal(FARGS,"TPI with PME currently only works in a 3D geometry with tin-foil boundary conditions");
}
/* The TPI molecule does not have exclusions with the rest
* of the system and no intra-molecular PME grid contributions
* will be calculated in gmx_pme_calc_energy.
*/
Vcorr = 0;
}
}
else
{
Vcorr = shift_LRcorrection(fplog,md->start,md->homenr,cr,fr,
md->chargeA,excl,x,TRUE,box,
fr->vir_el_recip);
}
dvdlambda = 0;
status = 0;
switch (fr->eeltype)
{
case eelPPPM:
status = gmx_pppm_do(fplog,fr->pmedata,FALSE,x,fr->f_novirsum,
md->chargeA,
box_size,fr->phi,cr,md->start,md->homenr,
nrnb,ir->pme_order,&Vlr);
break;
case eelPME:
case eelPMESWITCH:
case eelPMEUSER:
case eelPMEUSERSWITCH:
if (cr->duty & DUTY_PME)
{
if (fr->n_tpi == 0 || (flags & GMX_FORCE_STATECHANGED))
{
pme_flags = GMX_PME_SPREAD_Q | GMX_PME_SOLVE;
if (flags & GMX_FORCE_FORCES)
{
pme_flags |= GMX_PME_CALC_F;
}
if (flags & GMX_FORCE_VIRIAL)
{
pme_flags |= GMX_PME_CALC_ENER_VIR;
}
if (fr->n_tpi > 0)
{
/* We don't calculate f, but we do want the potential */
pme_flags |= GMX_PME_CALC_POT;
}
wallcycle_start(wcycle,ewcPMEMESH);
status = gmx_pme_do(fr->pmedata,
md->start,md->homenr - fr->n_tpi,
x,fr->f_novirsum,
md->chargeA,md->chargeB,
bSB ? boxs : box,cr,
DOMAINDECOMP(cr) ? dd_pme_maxshift_x(cr->dd) : 0,
DOMAINDECOMP(cr) ? dd_pme_maxshift_y(cr->dd) : 0,
nrnb,wcycle,
fr->vir_el_recip,fr->ewaldcoeff,
&Vlr,lambda,&dvdlambda,
pme_flags);
*cycles_pme = wallcycle_stop(wcycle,ewcPMEMESH);
/* We should try to do as little computation after
* this as possible, because parallel PME synchronizes
* the nodes, so we want all load imbalance of the rest
* of the force calculation to be before the PME call.
* DD load balancing is done on the whole time of
* the force call (without PME).
*/
}
if (fr->n_tpi > 0)
{
/* Determine the PME grid energy of the test molecule
* with the PME grid potential of the other charges.
*/
gmx_pme_calc_energy(fr->pmedata,fr->n_tpi,
x + md->homenr - fr->n_tpi,
md->chargeA + md->homenr - fr->n_tpi,
&Vlr);
}
PRINT_SEPDVDL("PME mesh",Vlr,dvdlambda);
}
else
{
/* Energies and virial are obtained later from the PME nodes */
/* but values have to be zeroed out here */
Vlr=0.0;
}
break;
case eelEWALD:
Vlr = do_ewald(fplog,FALSE,ir,x,fr->f_novirsum,
md->chargeA,md->chargeB,
box_size,cr,md->homenr,
fr->vir_el_recip,fr->ewaldcoeff,
lambda,&dvdlambda,fr->ewald_table);
PRINT_SEPDVDL("Ewald long-range",Vlr,dvdlambda);
break;
default:
Vlr = 0;
gmx_fatal(FARGS,"No such electrostatics method implemented %s",
eel_names[fr->eeltype]);
}
if (status != 0)
{
gmx_fatal(FARGS,"Error %d in long range electrostatics routine %s",
status,EELTYPE(fr->eeltype));
}
enerd->dvdl_lin += dvdlambda;
enerd->term[F_COUL_RECIP] = Vlr + Vcorr;
if (debug)
{
fprintf(debug,"Vlr = %g, Vcorr = %g, Vlr_corr = %g\n",
Vlr,Vcorr,enerd->term[F_COUL_RECIP]);
pr_rvecs(debug,0,"vir_el_recip after corr",fr->vir_el_recip,DIM);
pr_rvecs(debug,0,"fshift after LR Corrections",fr->fshift,SHIFTS);
}
}
else
{
if (EEL_RF(fr->eeltype))
{
dvdlambda = 0;
if (fr->eeltype != eelRF_NEC)
{
enerd->term[F_RF_EXCL] =
RF_excl_correction(fplog,fr,graph,md,excl,x,f,
fr->fshift,&pbc,lambda,&dvdlambda);
}
enerd->dvdl_lin += dvdlambda;
PRINT_SEPDVDL("RF exclusion correction",
enerd->term[F_RF_EXCL],dvdlambda);
}
}
where();
debug_gmx();
if (debug)
{
print_nrnb(debug,nrnb);
}
debug_gmx();
#ifdef GMX_MPI
if (TAKETIME)
{
t2=MPI_Wtime();
MPI_Barrier(cr->mpi_comm_mygroup);
t3=MPI_Wtime();
fr->t_wait += t3-t2;
if (fr->timesteps == 11)
{
fprintf(stderr,"* PP load balancing info: node %d, step %s, rel wait time=%3.0f%% , load string value: %7.2f\n",
cr->nodeid, gmx_step_str(fr->timesteps,buf),
100*fr->t_wait/(fr->t_wait+fr->t_fnbf),
(fr->t_fnbf+fr->t_wait)/fr->t_fnbf);
}
fr->timesteps++;
}
#endif
if (debug)
{
pr_rvecs(debug,0,"fshift after bondeds",fr->fshift,SHIFTS);
}
GMX_MPE_LOG(ev_force_finish);
}
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);
}
t_mdebin *init_mdebin(ener_file_t fp_ene,
const gmx_mtop_t *mtop,
const t_inputrec *ir,
FILE *fp_dhdl)
{
const char *ener_nm[F_NRE];
static const char *vir_nm[] = {
"Vir-XX", "Vir-XY", "Vir-XZ",
"Vir-YX", "Vir-YY", "Vir-YZ",
"Vir-ZX", "Vir-ZY", "Vir-ZZ"
};
static const char *sv_nm[] = {
"ShakeVir-XX", "ShakeVir-XY", "ShakeVir-XZ",
"ShakeVir-YX", "ShakeVir-YY", "ShakeVir-YZ",
"ShakeVir-ZX", "ShakeVir-ZY", "ShakeVir-ZZ"
};
static const char *fv_nm[] = {
"ForceVir-XX", "ForceVir-XY", "ForceVir-XZ",
"ForceVir-YX", "ForceVir-YY", "ForceVir-YZ",
"ForceVir-ZX", "ForceVir-ZY", "ForceVir-ZZ"
};
static const char *pres_nm[] = {
"Pres-XX","Pres-XY","Pres-XZ",
"Pres-YX","Pres-YY","Pres-YZ",
"Pres-ZX","Pres-ZY","Pres-ZZ"
};
static const char *surft_nm[] = {
"#Surf*SurfTen"
};
static const char *mu_nm[] = {
"Mu-X", "Mu-Y", "Mu-Z"
};
static const char *vcos_nm[] = {
"2CosZ*Vel-X"
};
static const char *visc_nm[] = {
"1/Viscosity"
};
static const char *baro_nm[] = {
"Barostat"
};
char **grpnms;
const gmx_groups_t *groups;
char **gnm;
char buf[256];
const char *bufi;
t_mdebin *md;
int i,j,ni,nj,n,nh,k,kk,ncon,nset;
gmx_bool bBHAM,bNoseHoover,b14;
snew(md,1);
if (EI_DYNAMICS(ir->eI))
{
md->delta_t = ir->delta_t;
}
else
{
md->delta_t = 0;
}
groups = &mtop->groups;
bBHAM = (mtop->ffparams.functype[0] == F_BHAM);
b14 = (gmx_mtop_ftype_count(mtop,F_LJ14) > 0 ||
gmx_mtop_ftype_count(mtop,F_LJC14_Q) > 0);
ncon = gmx_mtop_ftype_count(mtop,F_CONSTR);
nset = gmx_mtop_ftype_count(mtop,F_SETTLE);
md->bConstr = (ncon > 0 || nset > 0);
md->bConstrVir = FALSE;
if (md->bConstr) {
if (ncon > 0 && ir->eConstrAlg == econtLINCS) {
if (ir->eI == eiSD2)
md->nCrmsd = 2;
else
md->nCrmsd = 1;
}
md->bConstrVir = (getenv("GMX_CONSTRAINTVIR") != NULL);
} else {
md->nCrmsd = 0;
}
/* Energy monitoring */
for(i=0;i<egNR;i++)
{
md->bEInd[i]=FALSE;
}
#ifndef GMX_OPENMM
for(i=0; i<F_NRE; i++)
{
md->bEner[i] = FALSE;
if (i == F_LJ)
md->bEner[i] = !bBHAM;
else if (i == F_BHAM)
md->bEner[i] = bBHAM;
else if (i == F_EQM)
md->bEner[i] = ir->bQMMM;
else if (i == F_COUL_LR)
md->bEner[i] = (ir->rcoulomb > ir->rlist);
else if (i == F_LJ_LR)
md->bEner[i] = (!bBHAM && ir->rvdw > ir->rlist);
else if (i == F_BHAM_LR)
md->bEner[i] = (bBHAM && ir->rvdw > ir->rlist);
else if (i == F_RF_EXCL)
md->bEner[i] = (EEL_RF(ir->coulombtype) && ir->coulombtype != eelRF_NEC);
else if (i == F_COUL_RECIP)
md->bEner[i] = EEL_FULL(ir->coulombtype);
else if (i == F_LJ14)
md->bEner[i] = b14;
else if (i == F_COUL14)
md->bEner[i] = b14;
else if (i == F_LJC14_Q || i == F_LJC_PAIRS_NB)
md->bEner[i] = FALSE;
else if ((i == F_DVDL) || (i == F_DKDL))
md->bEner[i] = (ir->efep != efepNO);
else if (i == F_DHDL_CON)
md->bEner[i] = (ir->efep != efepNO && md->bConstr);
else if ((interaction_function[i].flags & IF_VSITE) ||
(i == F_CONSTR) || (i == F_CONSTRNC) || (i == F_SETTLE))
md->bEner[i] = FALSE;
else if ((i == F_COUL_SR) || (i == F_EPOT) || (i == F_PRES) || (i==F_EQM))
md->bEner[i] = TRUE;
else if ((i == F_GBPOL) && ir->implicit_solvent==eisGBSA)
md->bEner[i] = TRUE;
else if ((i == F_NPSOLVATION) && ir->implicit_solvent==eisGBSA && (ir->sa_algorithm != esaNO))
md->bEner[i] = TRUE;
else if ((i == F_GB12) || (i == F_GB13) || (i == F_GB14))
md->bEner[i] = FALSE;
else if ((i == F_ETOT) || (i == F_EKIN) || (i == F_TEMP))
md->bEner[i] = EI_DYNAMICS(ir->eI);
else if (i==F_VTEMP)
md->bEner[i] = (EI_DYNAMICS(ir->eI) && getenv("GMX_VIRIAL_TEMPERATURE"));
else if (i == F_DISPCORR || i == F_PDISPCORR)
md->bEner[i] = (ir->eDispCorr != edispcNO);
else if (i == F_DISRESVIOL)
md->bEner[i] = (gmx_mtop_ftype_count(mtop,F_DISRES) > 0);
else if (i == F_ORIRESDEV)
md->bEner[i] = (gmx_mtop_ftype_count(mtop,F_ORIRES) > 0);
else if (i == F_CONNBONDS)
md->bEner[i] = FALSE;
else if (i == F_COM_PULL)
md->bEner[i] = (ir->ePull == epullUMBRELLA || ir->ePull == epullCONST_F);
else if (i == F_ECONSERVED)
md->bEner[i] = ((ir->etc == etcNOSEHOOVER || ir->etc == etcVRESCALE) &&
(ir->epc == epcNO || ir->epc==epcMTTK));
else
md->bEner[i] = (gmx_mtop_ftype_count(mtop,i) > 0);
}
#else
/* OpenMM always produces only the following 4 energy terms */
md->bEner[F_EPOT] = TRUE;
md->bEner[F_EKIN] = TRUE;
md->bEner[F_ETOT] = TRUE;
md->bEner[F_TEMP] = TRUE;
#endif
md->f_nre=0;
for(i=0; i<F_NRE; i++)
{
if (md->bEner[i])
{
/* FIXME: The constness should not be cast away */
/*ener_nm[f_nre]=(char *)interaction_function[i].longname;*/
ener_nm[md->f_nre]=interaction_function[i].longname;
md->f_nre++;
}
}
md->epc = ir->epc;
for (i=0;i<DIM;i++)
{
for (j=0;j<DIM;j++)
{
md->ref_p[i][j] = ir->ref_p[i][j];
}
}
md->bTricl = TRICLINIC(ir->compress) || TRICLINIC(ir->deform);
md->bDynBox = DYNAMIC_BOX(*ir);
md->etc = ir->etc;
md->bNHC_trotter = IR_NVT_TROTTER(ir);
md->bMTTK = IR_NPT_TROTTER(ir);
md->ebin = mk_ebin();
/* Pass NULL for unit to let get_ebin_space determine the units
* for interaction_function[i].longname
*/
md->ie = get_ebin_space(md->ebin,md->f_nre,ener_nm,NULL);
if (md->nCrmsd)
{
/* This should be called directly after the call for md->ie,
* such that md->iconrmsd follows directly in the list.
*/
md->iconrmsd = get_ebin_space(md->ebin,md->nCrmsd,conrmsd_nm,"");
}
if (md->bDynBox)
{
md->ib = get_ebin_space(md->ebin,
md->bTricl ? NTRICLBOXS : NBOXS,
md->bTricl ? tricl_boxs_nm : boxs_nm,
unit_length);
md->ivol = get_ebin_space(md->ebin, 1, vol_nm, unit_volume);
md->idens = get_ebin_space(md->ebin, 1, dens_nm, unit_density_SI);
md->ipv = get_ebin_space(md->ebin, 1, pv_nm, unit_energy);
md->ienthalpy = get_ebin_space(md->ebin, 1, enthalpy_nm, unit_energy);
}
if (md->bConstrVir)
{
md->isvir = get_ebin_space(md->ebin,asize(sv_nm),sv_nm,unit_energy);
md->ifvir = get_ebin_space(md->ebin,asize(fv_nm),fv_nm,unit_energy);
}
md->ivir = get_ebin_space(md->ebin,asize(vir_nm),vir_nm,unit_energy);
md->ipres = get_ebin_space(md->ebin,asize(pres_nm),pres_nm,unit_pres_bar);
md->isurft = get_ebin_space(md->ebin,asize(surft_nm),surft_nm,
unit_surft_bar);
if (md->epc == epcPARRINELLORAHMAN || md->epc == epcMTTK)
{
md->ipc = get_ebin_space(md->ebin,md->bTricl ? 6 : 3,
boxvel_nm,unit_vel);
}
md->imu = get_ebin_space(md->ebin,asize(mu_nm),mu_nm,unit_dipole_D);
if (ir->cos_accel != 0)
{
md->ivcos = get_ebin_space(md->ebin,asize(vcos_nm),vcos_nm,unit_vel);
md->ivisc = get_ebin_space(md->ebin,asize(visc_nm),visc_nm,
unit_invvisc_SI);
}
/* Energy monitoring */
for(i=0;i<egNR;i++)
{
md->bEInd[i] = FALSE;
}
md->bEInd[egCOULSR] = TRUE;
md->bEInd[egLJSR ] = TRUE;
if (ir->rcoulomb > ir->rlist)
{
md->bEInd[egCOULLR] = TRUE;
}
if (!bBHAM)
{
if (ir->rvdw > ir->rlist)
{
md->bEInd[egLJLR] = TRUE;
}
}
else
{
md->bEInd[egLJSR] = FALSE;
md->bEInd[egBHAMSR] = TRUE;
if (ir->rvdw > ir->rlist)
{
md->bEInd[egBHAMLR] = TRUE;
}
}
if (b14)
{
md->bEInd[egLJ14] = TRUE;
md->bEInd[egCOUL14] = TRUE;
}
md->nEc=0;
for(i=0; (i<egNR); i++)
{
if (md->bEInd[i])
{
md->nEc++;
}
}
n=groups->grps[egcENER].nr;
md->nEg=n;
md->nE=(n*(n+1))/2;
snew(md->igrp,md->nE);
if (md->nE > 1)
{
n=0;
snew(gnm,md->nEc);
for(k=0; (k<md->nEc); k++)
{
snew(gnm[k],STRLEN);
}
for(i=0; (i<groups->grps[egcENER].nr); i++)
{
ni=groups->grps[egcENER].nm_ind[i];
for(j=i; (j<groups->grps[egcENER].nr); j++)
{
nj=groups->grps[egcENER].nm_ind[j];
for(k=kk=0; (k<egNR); k++)
{
if (md->bEInd[k])
{
sprintf(gnm[kk],"%s:%s-%s",egrp_nm[k],
*(groups->grpname[ni]),*(groups->grpname[nj]));
kk++;
}
}
md->igrp[n]=get_ebin_space(md->ebin,md->nEc,
(const char **)gnm,unit_energy);
n++;
}
}
for(k=0; (k<md->nEc); k++)
{
sfree(gnm[k]);
}
sfree(gnm);
if (n != md->nE)
{
gmx_incons("Number of energy terms wrong");
}
}
md->nTC=groups->grps[egcTC].nr;
md->nNHC = ir->opts.nhchainlength; /* shorthand for number of NH chains */
if (md->bMTTK)
{
md->nTCP = 1; /* assume only one possible coupling system for barostat
for now */
}
else
{
md->nTCP = 0;
}
if (md->etc == etcNOSEHOOVER) {
if (md->bNHC_trotter) {
md->mde_n = 2*md->nNHC*md->nTC;
}
else
{
md->mde_n = 2*md->nTC;
}
if (md->epc == epcMTTK)
{
md->mdeb_n = 2*md->nNHC*md->nTCP;
}
} else {
md->mde_n = md->nTC;
md->mdeb_n = 0;
}
snew(md->tmp_r,md->mde_n);
snew(md->tmp_v,md->mde_n);
snew(md->grpnms,md->mde_n);
grpnms = md->grpnms;
for(i=0; (i<md->nTC); i++)
{
ni=groups->grps[egcTC].nm_ind[i];
sprintf(buf,"T-%s",*(groups->grpname[ni]));
grpnms[i]=strdup(buf);
}
md->itemp=get_ebin_space(md->ebin,md->nTC,(const char **)grpnms,
unit_temp_K);
bNoseHoover = (getenv("GMX_NOSEHOOVER_CHAINS") != NULL); /* whether to print Nose-Hoover chains */
if (md->etc == etcNOSEHOOVER)
{
if (bNoseHoover)
{
if (md->bNHC_trotter)
{
for(i=0; (i<md->nTC); i++)
{
ni=groups->grps[egcTC].nm_ind[i];
bufi = *(groups->grpname[ni]);
for(j=0; (j<md->nNHC); j++)
{
sprintf(buf,"Xi-%d-%s",j,bufi);
grpnms[2*(i*md->nNHC+j)]=strdup(buf);
sprintf(buf,"vXi-%d-%s",j,bufi);
grpnms[2*(i*md->nNHC+j)+1]=strdup(buf);
}
}
md->itc=get_ebin_space(md->ebin,md->mde_n,
(const char **)grpnms,unit_invtime);
if (md->bMTTK)
{
for(i=0; (i<md->nTCP); i++)
{
bufi = baro_nm[0]; /* All barostat DOF's together for now. */
for(j=0; (j<md->nNHC); j++)
{
sprintf(buf,"Xi-%d-%s",j,bufi);
grpnms[2*(i*md->nNHC+j)]=strdup(buf);
sprintf(buf,"vXi-%d-%s",j,bufi);
grpnms[2*(i*md->nNHC+j)+1]=strdup(buf);
}
}
md->itcb=get_ebin_space(md->ebin,md->mdeb_n,
(const char **)grpnms,unit_invtime);
}
}
else
{
for(i=0; (i<md->nTC); i++)
{
ni=groups->grps[egcTC].nm_ind[i];
bufi = *(groups->grpname[ni]);
sprintf(buf,"Xi-%s",bufi);
grpnms[2*i]=strdup(buf);
sprintf(buf,"vXi-%s",bufi);
grpnms[2*i+1]=strdup(buf);
}
md->itc=get_ebin_space(md->ebin,md->mde_n,
(const char **)grpnms,unit_invtime);
}
}
}
else if (md->etc == etcBERENDSEN || md->etc == etcYES ||
md->etc == etcVRESCALE)
{
for(i=0; (i<md->nTC); i++)
{
ni=groups->grps[egcTC].nm_ind[i];
sprintf(buf,"Lamb-%s",*(groups->grpname[ni]));
grpnms[i]=strdup(buf);
}
md->itc=get_ebin_space(md->ebin,md->mde_n,(const char **)grpnms,"");
}
sfree(grpnms);
md->nU=groups->grps[egcACC].nr;
if (md->nU > 1)
{
snew(grpnms,3*md->nU);
for(i=0; (i<md->nU); i++)
{
ni=groups->grps[egcACC].nm_ind[i];
sprintf(buf,"Ux-%s",*(groups->grpname[ni]));
grpnms[3*i+XX]=strdup(buf);
sprintf(buf,"Uy-%s",*(groups->grpname[ni]));
grpnms[3*i+YY]=strdup(buf);
sprintf(buf,"Uz-%s",*(groups->grpname[ni]));
grpnms[3*i+ZZ]=strdup(buf);
}
md->iu=get_ebin_space(md->ebin,3*md->nU,(const char **)grpnms,unit_vel);
sfree(grpnms);
}
if ( fp_ene )
{
do_enxnms(fp_ene,&md->ebin->nener,&md->ebin->enm);
}
md->print_grpnms=NULL;
/* check whether we're going to write dh histograms */
md->dhc=NULL;
if (ir->separate_dhdl_file == sepdhdlfileNO )
{
int i;
snew(md->dhc, 1);
mde_delta_h_coll_init(md->dhc, ir);
md->fp_dhdl = NULL;
}
else
{
md->fp_dhdl = fp_dhdl;
}
md->dhdl_derivatives = (ir->dhdl_derivatives==dhdlderivativesYES);
return md;
}
int main (int argc, char *argv[])
{
static const char *desc[] = {
"The gromacs preprocessor",
"reads a molecular topology file, checks the validity of the",
"file, expands the topology from a molecular description to an atomic",
"description. The topology file contains information about",
"molecule types and the number of molecules, the preprocessor",
"copies each molecule as needed. ",
"There is no limitation on the number of molecule types. ",
"Bonds and bond-angles can be converted into constraints, separately",
"for hydrogens and heavy atoms.",
"Then a coordinate file is read and velocities can be generated",
"from a Maxwellian distribution if requested.",
"grompp also reads parameters for the mdrun ",
"(eg. number of MD steps, time step, cut-off), and others such as",
"NEMD parameters, which are corrected so that the net acceleration",
"is zero.",
"Eventually a binary file is produced that can serve as the sole input",
"file for the MD program.[PAR]",
"grompp uses the atom names from the topology file. The atom names",
"in the coordinate file (option [TT]-c[tt]) are only read to generate",
"warnings when they do not match the atom names in the topology.",
"Note that the atom names are irrelevant for the simulation as",
"only the atom types are used for generating interaction parameters.[PAR]",
"grompp calls a preprocessor to resolve includes, macros ",
"etcetera. By default we use the cpp in your path. To specify a "
"different macro-preprocessor (e.g. m4) or alternative location",
"you can put a line in your parameter file specifying the path",
"to that program. Specifying [TT]-pp[tt] will get the pre-processed",
"topology file written out.[PAR]",
"If your system does not have a c-preprocessor, you can still",
"use grompp, but you do not have access to the features ",
"from the cpp. Command line options to the c-preprocessor can be given",
"in the [TT].mdp[tt] file. See your local manual (man cpp).[PAR]",
"When using position restraints a file with restraint coordinates",
"can be supplied with [TT]-r[tt], otherwise restraining will be done",
"with respect to the conformation from the [TT]-c[tt] option.",
"For free energy calculation the the coordinates for the B topology",
"can be supplied with [TT]-rb[tt], otherwise they will be equal to",
"those of the A topology.[PAR]",
"Starting coordinates can be read from trajectory with [TT]-t[tt].",
"The last frame with coordinates and velocities will be read,",
"unless the [TT]-time[tt] option is used.",
"Note that these velocities will not be used when [TT]gen_vel = yes[tt]",
"in your [TT].mdp[tt] file. An energy file can be supplied with",
"[TT]-e[tt] to have exact restarts when using pressure and/or",
"Nose-Hoover temperature coupling. For an exact restart do not forget",
"to turn off velocity generation and turn on unconstrained starting",
"when constraints are present in the system.",
"If you want to continue a crashed run, it is",
"easier to use [TT]tpbconv[tt].[PAR]",
"Using the [TT]-morse[tt] option grompp can convert the harmonic bonds",
"in your topology to morse potentials. This makes it possible to break",
"bonds. For this option to work you need an extra file in your $GMXLIB",
"with dissociation energy. Use the -debug option to get more information",
"on the workings of this option (look for MORSE in the grompp.log file",
"using less or something like that).[PAR]",
"By default all bonded interactions which have constant energy due to",
"virtual site constructions will be removed. If this constant energy is",
"not zero, this will result in a shift in the total energy. All bonded",
"interactions can be kept by turning off [TT]-rmvsbds[tt]. Additionally,",
"all constraints for distances which will be constant anyway because",
"of virtual site constructions will be removed. If any constraints remain",
"which involve virtual sites, a fatal error will result.[PAR]"
"To verify your run input file, please make notice of all warnings",
"on the screen, and correct where necessary. Do also look at the contents",
"of the [TT]mdout.mdp[tt] file, this contains comment lines, as well as",
"the input that [TT]grompp[tt] has read. If in doubt you can start grompp",
"with the [TT]-debug[tt] option which will give you more information",
"in a file called grompp.log (along with real debug info). Finally, you",
"can see the contents of the run input file with the [TT]gmxdump[tt]",
"program."
};
t_gromppopts *opts;
gmx_mtop_t *sys;
int nmi;
t_molinfo *mi;
gpp_atomtype_t atype;
t_inputrec *ir;
int natoms,nvsite,comb,mt;
t_params *plist;
t_state state;
matrix box;
real max_spacing,fudgeQQ;
double reppow;
char fn[STRLEN],fnB[STRLEN],*mdparin;
int nerror,ntype;
bool bNeedVel,bGenVel;
bool have_radius,have_vol,have_surftens,have_gb_radius,have_S_hct;
bool have_atomnumber;
int n12,n13,n14;
t_params *gb_plist = NULL;
gmx_genborn_t *born = NULL;
t_filenm fnm[] = {
{ efMDP, NULL, NULL, ffOPTRD },
{ efMDP, "-po", "mdout", ffWRITE },
{ efSTX, "-c", NULL, ffREAD },
{ efSTX, "-r", NULL, ffOPTRD },
{ efSTX, "-rb", NULL, ffOPTRD },
{ efNDX, NULL, NULL, ffOPTRD },
{ efTOP, NULL, NULL, ffREAD },
{ efTOP, "-pp", "processed", ffOPTWR },
{ efTPX, "-o", NULL, ffWRITE },
{ efTRN, "-t", NULL, ffOPTRD },
{ efEDR, "-e", NULL, ffOPTRD }
};
#define NFILE asize(fnm)
/* Command line options */
static bool bVerbose=TRUE,bRenum=TRUE;
static bool bRmVSBds=TRUE,bZero=FALSE;
static int i,maxwarn=0;
static real fr_time=-1;
t_pargs pa[] = {
{ "-v", FALSE, etBOOL, {&bVerbose},
"Be loud and noisy" },
{ "-time", FALSE, etREAL, {&fr_time},
"Take frame at or first after this time." },
{ "-rmvsbds",FALSE, etBOOL, {&bRmVSBds},
"Remove constant bonded interactions with virtual sites" },
{ "-maxwarn", FALSE, etINT, {&maxwarn},
"Number of allowed warnings during input processing" },
{ "-zero", FALSE, etBOOL, {&bZero},
"Set parameters for bonded interactions without defaults to zero instead of generating an error" },
{ "-renum", FALSE, etBOOL, {&bRenum},
"Renumber atomtypes and minimize number of atomtypes" }
};
CopyRight(stdout,argv[0]);
/* Initiate some variables */
nerror=0;
snew(ir,1);
snew(opts,1);
init_ir(ir,opts);
/* Parse the command line */
parse_common_args(&argc,argv,0,NFILE,fnm,asize(pa),pa,
asize(desc),desc,0,NULL);
init_warning(maxwarn);
/* PARAMETER file processing */
mdparin = opt2fn("-f",NFILE,fnm);
set_warning_line(mdparin,-1);
get_ir(mdparin,opt2fn("-po",NFILE,fnm),ir,opts,&nerror);
if (bVerbose)
fprintf(stderr,"checking input for internal consistency...\n");
check_ir(mdparin,ir,opts,&nerror);
if (ir->ld_seed == -1) {
ir->ld_seed = make_seed();
fprintf(stderr,"Setting the LD random seed to %d\n",ir->ld_seed);
}
bNeedVel = EI_STATE_VELOCITY(ir->eI);
bGenVel = (bNeedVel && opts->bGenVel);
snew(plist,F_NRE);
init_plist(plist);
snew(sys,1);
atype = init_atomtype();
if (debug)
pr_symtab(debug,0,"Just opened",&sys->symtab);
strcpy(fn,ftp2fn(efTOP,NFILE,fnm));
if (!gmx_fexist(fn))
gmx_fatal(FARGS,"%s does not exist",fn);
new_status(fn,opt2fn_null("-pp",NFILE,fnm),opt2fn("-c",NFILE,fnm),
opts,ir,bZero,bGenVel,bVerbose,&state,
atype,sys,&nmi,&mi,plist,&comb,&reppow,&fudgeQQ,
opts->bMorse,
&nerror);
if (debug)
pr_symtab(debug,0,"After new_status",&sys->symtab);
if (count_constraints(sys,mi) && (ir->eConstrAlg == econtSHAKE)) {
if (ir->eI == eiCG || ir->eI == eiLBFGS) {
fprintf(stderr,
"ERROR: Can not do %s with %s, use %s\n",
EI(ir->eI),econstr_names[econtSHAKE],econstr_names[econtLINCS]);
nerror++;
}
if (ir->bPeriodicMols) {
fprintf(stderr,
"ERROR: can not do periodic molecules with %s, use %s\n",
econstr_names[econtSHAKE],econstr_names[econtLINCS]);
nerror++;
}
}
/* If we are doing GBSA, check that we got the parameters we need
* This checking is to see if there are GBSA paratmeters for all
* atoms in the force field. To go around this for testing purposes
* comment out the nerror++ counter temporarliy
*/
have_radius=have_vol=have_surftens=have_gb_radius=have_S_hct=TRUE;
for(i=0;i<get_atomtype_ntypes(atype);i++) {
have_radius=have_radius && (get_atomtype_radius(i,atype) > 0);
have_vol=have_vol && (get_atomtype_vol(i,atype) > 0);
have_surftens=have_surftens && (get_atomtype_surftens(i,atype) > 0);
have_gb_radius=have_gb_radius && (get_atomtype_gb_radius(i,atype) > 0);
have_S_hct=have_S_hct && (get_atomtype_S_hct(i,atype) > 0);
}
if(!have_radius && ir->implicit_solvent==eisGBSA) {
fprintf(stderr,"Can't do GB electrostatics; the forcefield is missing values for\n"
"atomtype radii, or they might be zero\n.");
/* nerror++; */
}
/*
if(!have_surftens && ir->implicit_solvent!=eisNO) {
fprintf(stderr,"Can't do implicit solvent; the forcefield is missing values\n"
" for atomtype surface tension\n.");
nerror++;
}
*/
/* If we are doing QM/MM, check that we got the atom numbers */
have_atomnumber = TRUE;
for (i=0; i<get_atomtype_ntypes(atype); i++) {
have_atomnumber = have_atomnumber && (get_atomtype_atomnumber(i,atype) >= 0);
}
if (!have_atomnumber && ir->bQMMM)
{
fprintf(stderr,"\n"
"It appears as if you are trying to run a QM/MM calculation, but the force\n"
"field you are using does not contain atom numbers fields. This is an\n"
"optional field (introduced in Gromacs 3.3) for general runs, but mandatory\n"
"for QM/MM. The good news is that it is easy to add - put the atom number as\n"
"an integer just before the mass column in ffXXXnb.itp.\n"
"NB: United atoms have the same atom numbers as normal ones.\n\n");
nerror++;
}
if (nerror) {
print_warn_num(FALSE);
gmx_fatal(FARGS,"There were %d error(s) processing your input",nerror);
}
if (opt2bSet("-r",NFILE,fnm))
sprintf(fn,"%s",opt2fn("-r",NFILE,fnm));
else
sprintf(fn,"%s",opt2fn("-c",NFILE,fnm));
if (opt2bSet("-rb",NFILE,fnm))
sprintf(fnB,"%s",opt2fn("-rb",NFILE,fnm));
else
strcpy(fnB,fn);
if (nint_ftype(sys,mi,F_POSRES) > 0) {
if (bVerbose) {
fprintf(stderr,"Reading position restraint coords from %s",fn);
if (strcmp(fn,fnB) == 0) {
fprintf(stderr,"\n");
} else {
fprintf(stderr," and %s\n",fnB);
if (ir->efep != efepNO && ir->n_flambda > 0) {
fprintf(stderr,"ERROR: can not change the position restraint reference coordinates with lambda togther with foreign lambda calculation.\n");
nerror++;
}
}
}
gen_posres(sys,mi,fn,fnB,
ir->refcoord_scaling,ir->ePBC,
ir->posres_com,ir->posres_comB);
}
nvsite = 0;
/* set parameters for virtual site construction (not for vsiten) */
for(mt=0; mt<sys->nmoltype; mt++) {
nvsite +=
set_vsites(bVerbose, &sys->moltype[mt].atoms, atype, mi[mt].plist);
}
/* now throw away all obsolete bonds, angles and dihedrals: */
/* note: constraints are ALWAYS removed */
if (nvsite) {
for(mt=0; mt<sys->nmoltype; mt++) {
clean_vsite_bondeds(mi[mt].plist,sys->moltype[mt].atoms.nr,bRmVSBds);
}
}
/* If we are using CMAP, setup the pre-interpolation grid */
if(plist->ncmap>0)
{
init_cmap_grid(&sys->cmap_grid, plist->nc, plist->grid_spacing);
setup_cmap(plist->grid_spacing, plist->nc, plist->cmap,&sys->cmap_grid);
}
set_wall_atomtype(atype,opts,ir);
if (bRenum) {
renum_atype(plist, sys, ir->wall_atomtype, atype, bVerbose);
ntype = get_atomtype_ntypes(atype);
}
/* PELA: Copy the atomtype data to the topology atomtype list */
copy_atomtype_atomtypes(atype,&(sys->atomtypes));
if (debug)
pr_symtab(debug,0,"After renum_atype",&sys->symtab);
if (bVerbose)
fprintf(stderr,"converting bonded parameters...\n");
ntype = get_atomtype_ntypes(atype);
convert_params(ntype, plist, mi, comb, reppow, fudgeQQ, sys);
if(ir->implicit_solvent)
{
printf("Constructing Generalized Born topology...\n");
/* Check for -normvsbds switch to grompp, necessary for gb together with vsites */
if(bRmVSBds && nvsite)
{
fprintf(stderr, "ERROR: Must use -normvsbds switch to grompp when doing Generalized Born\n"
"together with virtual sites\n");
nerror++;
}
if (nerror)
{
print_warn_num(FALSE);
gmx_fatal(FARGS,"There were %d error(s) processing your input",nerror);
}
generate_gb_topology(sys,mi);
}
if (debug)
pr_symtab(debug,0,"After convert_params",&sys->symtab);
/* set ptype to VSite for virtual sites */
for(mt=0; mt<sys->nmoltype; mt++) {
set_vsites_ptype(FALSE,&sys->moltype[mt]);
}
if (debug) {
pr_symtab(debug,0,"After virtual sites",&sys->symtab);
}
/* Check velocity for virtual sites and shells */
if (bGenVel) {
check_vel(sys,state.v);
}
/* check masses */
check_mol(sys);
for(i=0; i<sys->nmoltype; i++) {
check_cg_sizes(ftp2fn(efTOP,NFILE,fnm),&sys->moltype[i].cgs);
}
check_warning_error(FARGS);
if (bVerbose)
fprintf(stderr,"initialising group options...\n");
do_index(mdparin,ftp2fn_null(efNDX,NFILE,fnm),
sys,bVerbose,ir,
bGenVel ? state.v : NULL);
/* Init the temperature coupling state */
init_gtc_state(&state,ir->opts.ngtc);
if (bVerbose)
fprintf(stderr,"Checking consistency between energy and charge groups...\n");
check_eg_vs_cg(sys);
if (debug)
pr_symtab(debug,0,"After index",&sys->symtab);
triple_check(mdparin,ir,sys,&nerror);
close_symtab(&sys->symtab);
if (debug)
pr_symtab(debug,0,"After close",&sys->symtab);
/* make exclusions between QM atoms */
if (ir->bQMMM) {
generate_qmexcl(sys,ir);
}
if (ftp2bSet(efTRN,NFILE,fnm)) {
if (bVerbose)
fprintf(stderr,"getting data from old trajectory ...\n");
cont_status(ftp2fn(efTRN,NFILE,fnm),ftp2fn_null(efEDR,NFILE,fnm),
bNeedVel,bGenVel,fr_time,ir,&state,sys);
}
if (ir->ePBC==epbcXY && ir->nwall!=2)
clear_rvec(state.box[ZZ]);
if (EEL_FULL(ir->coulombtype)) {
/* Calculate the optimal grid dimensions */
copy_mat(state.box,box);
if (ir->ePBC==epbcXY && ir->nwall==2)
svmul(ir->wall_ewald_zfac,box[ZZ],box[ZZ]);
max_spacing = calc_grid(stdout,box,opts->fourierspacing,
&(ir->nkx),&(ir->nky),&(ir->nkz),1);
if ((ir->coulombtype == eelPPPM) && (max_spacing > 0.1)) {
set_warning_line(mdparin,-1);
sprintf(warn_buf,"Grid spacing larger then 0.1 while using PPPM.");
warning_note(NULL);
}
}
if (ir->ePull != epullNO)
set_pull_init(ir,sys,state.x,state.box,opts->pull_start);
/* reset_multinr(sys); */
if (EEL_PME(ir->coulombtype)) {
float ratio = pme_load_estimate(sys,ir,state.box);
fprintf(stderr,"Estimate for the relative computational load of the PME mesh part: %.2f\n",ratio);
if (ratio > 0.5)
warning_note("The optimal PME mesh load for parallel simulations is below 0.5\n"
"and for highly parallel simulations between 0.25 and 0.33,\n"
"for higher performance, increase the cut-off and the PME grid spacing");
}
{
double cio = compute_io(ir,sys->natoms,&sys->groups,F_NRE,1);
sprintf(warn_buf,"This run will generate roughly %.0f Mb of data",cio);
if (cio > 2000) {
set_warning_line(mdparin,-1);
warning_note(NULL);
} else {
printf("%s\n",warn_buf);
}
}
if (bVerbose)
fprintf(stderr,"writing run input file...\n");
print_warn_num(TRUE);
state.lambda = ir->init_lambda;
write_tpx_state(ftp2fn(efTPX,NFILE,fnm),ir,&state,sys);
thanx(stderr);
return 0;
}
void
nbnxn_kernel_simd_2xnn(nbnxn_pairlist_set_t *nbl_list,
const nbnxn_atomdata_t *nbat,
const interaction_const_t *ic,
int ewald_excl,
rvec *shift_vec,
int force_flags,
int clearF,
real *fshift,
real *Vc,
real *Vvdw)
#ifdef GMX_NBNXN_SIMD_2XNN
{
int nnbl;
nbnxn_pairlist_t **nbl;
int coult;
int nb;
nnbl = nbl_list->nnbl;
nbl = nbl_list->nbl;
if (EEL_RF(ic->eeltype) || ic->eeltype == eelCUT)
{
coult = coultRF;
}
else
{
if (ewald_excl == ewaldexclTable)
{
if (ic->rcoulomb == ic->rvdw)
{
coult = coultTAB;
}
else
{
coult = coultTAB_TWIN;
}
}
else
{
if (ic->rcoulomb == ic->rvdw)
{
coult = coultEWALD;
}
else
{
coult = coultEWALD_TWIN;
}
}
}
#pragma omp parallel for schedule(static) num_threads(gmx_omp_nthreads_get(emntNonbonded))
for (nb = 0; nb < nnbl; nb++)
{
nbnxn_atomdata_output_t *out;
real *fshift_p;
out = &nbat->out[nb];
if (clearF == enbvClearFYes)
{
clear_f(nbat, nb, out->f);
}
if ((force_flags & GMX_FORCE_VIRIAL) && nnbl == 1)
{
fshift_p = fshift;
}
else
{
fshift_p = out->fshift;
if (clearF == enbvClearFYes)
{
clear_fshift(fshift_p);
}
}
/* With Ewald type electrostatics we the forces for excluded atom pairs
* should not contribute to the virial sum. The exclusion forces
* are not calculate in the energy kernels, but are in _noener.
*/
if (!((force_flags & GMX_FORCE_ENERGY) ||
(EEL_FULL(ic->eeltype) && (force_flags & GMX_FORCE_VIRIAL))))
{
/* Don't calculate energies */
p_nbk_noener[coult][nbat->comb_rule](nbl[nb], nbat,
ic,
shift_vec,
out->f,
fshift_p);
}
else if (out->nV == 1 || !(force_flags & GMX_FORCE_ENERGY))
{
/* No energy groups */
out->Vvdw[0] = 0;
out->Vc[0] = 0;
p_nbk_ener[coult][nbat->comb_rule](nbl[nb], nbat,
ic,
shift_vec,
out->f,
fshift_p,
out->Vvdw,
out->Vc);
}
else
{
/* Calculate energy group contributions */
int i;
for (i = 0; i < out->nVS; i++)
{
out->VSvdw[i] = 0;
}
for (i = 0; i < out->nVS; i++)
{
out->VSc[i] = 0;
}
p_nbk_energrp[coult][nbat->comb_rule](nbl[nb], nbat,
ic,
shift_vec,
out->f,
fshift_p,
out->VSvdw,
out->VSc);
reduce_group_energies(nbat->nenergrp, nbat->neg_2log,
out->VSvdw, out->VSc,
out->Vvdw, out->Vc);
}
}
if (force_flags & GMX_FORCE_ENERGY)
{
reduce_energies_over_lists(nbat, nnbl, Vvdw, Vc);
}
}
t_mdebin *init_mdebin(int fp_ene,
const gmx_mtop_t *mtop,
const t_inputrec *ir)
{
char *ener_nm[F_NRE];
static char *vir_nm[] = {
"Vir-XX", "Vir-XY", "Vir-XZ",
"Vir-YX", "Vir-YY", "Vir-YZ",
"Vir-ZX", "Vir-ZY", "Vir-ZZ"
};
static char *sv_nm[] = {
"ShakeVir-XX", "ShakeVir-XY", "ShakeVir-XZ",
"ShakeVir-YX", "ShakeVir-YY", "ShakeVir-YZ",
"ShakeVir-ZX", "ShakeVir-ZY", "ShakeVir-ZZ"
};
static char *fv_nm[] = {
"ForceVir-XX", "ForceVir-XY", "ForceVir-XZ",
"ForceVir-YX", "ForceVir-YY", "ForceVir-YZ",
"ForceVir-ZX", "ForceVir-ZY", "ForceVir-ZZ"
};
static char *pres_nm[] = {
"Pres-XX (bar)","Pres-XY (bar)","Pres-XZ (bar)",
"Pres-YX (bar)","Pres-YY (bar)","Pres-YZ (bar)",
"Pres-ZX (bar)","Pres-ZY (bar)","Pres-ZZ (bar)"
};
static char *surft_nm[] = {
"#Surf*SurfTen"
};
static char *mu_nm[] = {
"Mu-X", "Mu-Y", "Mu-Z"
};
static char *vcos_nm[] = {
"2CosZ*Vel-X"
};
static char *visc_nm[] = {
"1/Viscosity (SI)"
};
static char **grpnms;
const gmx_groups_t *groups;
char **gnm;
char buf[256];
t_mdebin *md;
int i,j,ni,nj,n,k,kk,ncon,nset;
bool bBHAM,b14;
f_nre = 0; // otherwise, multiple calls to mdrunner_integrate are not possible!NnCrmsd;
groups = &mtop->groups;
bBHAM = (mtop->ffparams.functype[0] == F_BHAM);
b14 = (gmx_mtop_ftype_count(mtop,F_LJ14) > 0 ||
gmx_mtop_ftype_count(mtop,F_LJC14_Q) > 0);
ncon = gmx_mtop_ftype_count(mtop,F_CONSTR);
nset = gmx_mtop_ftype_count(mtop,F_SETTLE);
bConstr = (ncon > 0 || nset > 0);
bConstrVir = FALSE;
if (bConstr) {
if (ncon > 0 && ir->eConstrAlg == econtLINCS) {
if (ir->eI == eiSD2)
nCrmsd = 2;
else
nCrmsd = 1;
}
bConstrVir = (getenv("GMX_CONSTRAINTVIR") != NULL);
} else {
nCrmsd = 0;
}
for(i=0; i<F_NRE; i++) {
bEner[i] = FALSE;
if (i == F_LJ)
bEner[i] = !bBHAM;
else if (i == F_BHAM)
bEner[i] = bBHAM;
else if (i == F_EQM)
bEner[i] = ir->bQMMM;
else if (i == F_COUL_LR)
bEner[i] = (ir->rcoulomb > ir->rlist);
else if (i == F_LJ_LR)
bEner[i] = (!bBHAM && ir->rvdw > ir->rlist);
else if (i == F_BHAM_LR)
bEner[i] = (bBHAM && ir->rvdw > ir->rlist);
else if (i == F_RF_EXCL)
bEner[i] = (EEL_RF(ir->coulombtype) && ir->coulombtype != eelRF_NEC);
else if (i == F_COUL_RECIP)
bEner[i] = EEL_FULL(ir->coulombtype);
else if (i == F_LJ14)
bEner[i] = b14;
else if (i == F_COUL14)
bEner[i] = b14;
else if (i == F_LJC14_Q || i == F_LJC_PAIRS_NB)
bEner[i] = FALSE;
else if ((i == F_DVDL) || (i == F_DKDL))
bEner[i] = (ir->efep != efepNO);
else if (i == F_DGDL_CON)
bEner[i] = (ir->efep != efepNO && bConstr);
else if ((interaction_function[i].flags & IF_VSITE) ||
(i == F_CONSTR) || (i == F_SETTLE))
bEner[i] = FALSE;
else if ((i == F_COUL_SR) || (i == F_EPOT) || (i == F_PRES) || (i==F_EQM))
bEner[i] = TRUE;
else if ((i == F_ETOT) || (i == F_EKIN) || (i == F_TEMP))
bEner[i] = EI_DYNAMICS(ir->eI);
else if (i == F_DISPCORR)
bEner[i] = (ir->eDispCorr != edispcNO);
else if (i == F_DISRESVIOL)
bEner[i] = (gmx_mtop_ftype_count(mtop,F_DISRES) > 0);
else if (i == F_ORIRESDEV)
bEner[i] = (gmx_mtop_ftype_count(mtop,F_ORIRES) > 0);
else if (i == F_CONNBONDS)
bEner[i] = FALSE;
else if (i == F_COM_PULL)
bEner[i] = (ir->ePull == epullUMBRELLA || ir->ePull == epullCONST_F);
else if (i == F_ECONSERVED)
bEner[i] = ((ir->etc == etcNOSEHOOVER || ir->etc == etcVRESCALE) &&
ir->epc == epcNO);
else
bEner[i] = (gmx_mtop_ftype_count(mtop,i) > 0);
}
for(i=0; i<F_NRE; i++)
if (bEner[i]) {
ener_nm[f_nre]=interaction_function[i].longname;
f_nre++;
}
epc = ir->epc;
bTricl = TRICLINIC(ir->compress) || TRICLINIC(ir->deform);
bDynBox = DYNAMIC_BOX(*ir);
etc = ir->etc;
/* Energy monitoring */
snew(md,1);
md->ebin = mk_ebin();
md->ie = get_ebin_space(md->ebin,f_nre,ener_nm);
if (nCrmsd) {
/* This should be called directly after the call for md->ie,
* such that md->iconrmsd follows directly in the list.
*/
md->iconrmsd = get_ebin_space(md->ebin,nCrmsd,conrmsd_nm);
}
if (bDynBox)
md->ib = get_ebin_space(md->ebin, bTricl ? NTRICLBOXS :
NBOXS, bTricl ? tricl_boxs_nm : boxs_nm);
if (bConstrVir) {
md->isvir = get_ebin_space(md->ebin,asize(sv_nm),sv_nm);
md->ifvir = get_ebin_space(md->ebin,asize(fv_nm),fv_nm);
}
md->ivir = get_ebin_space(md->ebin,asize(vir_nm),vir_nm);
md->ipres = get_ebin_space(md->ebin,asize(pres_nm),pres_nm);
md->isurft = get_ebin_space(md->ebin,asize(surft_nm),surft_nm);
if (epc == epcPARRINELLORAHMAN) {
md->ipc = get_ebin_space(md->ebin,bTricl ? 6 : 3,boxvel_nm);
}
md->imu = get_ebin_space(md->ebin,asize(mu_nm),mu_nm);
if (ir->cos_accel != 0) {
md->ivcos = get_ebin_space(md->ebin,asize(vcos_nm),vcos_nm);
md->ivisc = get_ebin_space(md->ebin,asize(visc_nm),visc_nm);
}
if (ir->rcoulomb > ir->rlist)
bEInd[egCOULLR] = TRUE;
if (!bBHAM) {
if (ir->rvdw > ir->rlist)
bEInd[egLJLR] = TRUE;
} else {
bEInd[egLJSR] = FALSE;
bEInd[egBHAMSR] = TRUE;
if (ir->rvdw > ir->rlist)
bEInd[egBHAMLR] = TRUE;
}
if (b14) {
bEInd[egLJ14] = TRUE;
bEInd[egCOUL14] = TRUE;
}
md->nEc=0;
for(i=0; (i<egNR); i++)
if (bEInd[i])
md->nEc++;
n=groups->grps[egcENER].nr;
md->nEg=n;
md->nE=(n*(n+1))/2;
snew(md->igrp,md->nE);
if (md->nE > 1) {
n=0;
snew(gnm,md->nEc);
for(k=0; (k<md->nEc); k++)
snew(gnm[k],STRLEN);
for(i=0; (i<groups->grps[egcENER].nr); i++) {
ni=groups->grps[egcENER].nm_ind[i];
for(j=i; (j<groups->grps[egcENER].nr); j++) {
nj=groups->grps[egcENER].nm_ind[j];
for(k=kk=0; (k<egNR); k++) {
if (bEInd[k]) {
sprintf(gnm[kk],"%s:%s-%s",egrp_nm[k],
*(groups->grpname[ni]),*(groups->grpname[nj]));
kk++;
}
}
md->igrp[n]=get_ebin_space(md->ebin,md->nEc,gnm);
n++;
}
}
for(k=0; (k<md->nEc); k++)
sfree(gnm[k]);
sfree(gnm);
if (n != md->nE)
gmx_incons("Number of energy terms wrong");
}
md->nTC=groups->grps[egcTC].nr;
snew(grpnms,md->nTC);
for(i=0; (i<md->nTC); i++) {
ni=groups->grps[egcTC].nm_ind[i];
sprintf(buf,"T-%s",*(groups->grpname[ni]));
grpnms[i]=strdup(buf);
}
md->itemp=get_ebin_space(md->ebin,md->nTC,grpnms);
sfree(*grpnms);
if (etc == etcNOSEHOOVER) {
for(i=0; (i<md->nTC); i++) {
ni=groups->grps[egcTC].nm_ind[i];
sprintf(buf,"Xi-%s",*(groups->grpname[ni]));
grpnms[i]=strdup(buf);
}
md->itc=get_ebin_space(md->ebin,md->nTC,grpnms);
sfree(*grpnms);
} else if (etc == etcBERENDSEN || etc == etcYES || etc == etcVRESCALE) {
for(i=0; (i<md->nTC); i++) {
ni=groups->grps[egcTC].nm_ind[i];
sprintf(buf,"Lamb-%s",*(groups->grpname[ni]));
grpnms[i]=strdup(buf);
}
md->itc=get_ebin_space(md->ebin,md->nTC,grpnms);
sfree(*grpnms);
}
sfree(grpnms);
md->nU=groups->grps[egcACC].nr;
if (md->nU > 1) {
snew(grpnms,3*md->nU);
for(i=0; (i<md->nU); i++) {
ni=groups->grps[egcACC].nm_ind[i];
sprintf(buf,"Ux-%s",*(groups->grpname[ni]));
grpnms[3*i+XX]=strdup(buf);
sprintf(buf,"Uy-%s",*(groups->grpname[ni]));
grpnms[3*i+YY]=strdup(buf);
sprintf(buf,"Uz-%s",*(groups->grpname[ni]));
grpnms[3*i+ZZ]=strdup(buf);
}
md->iu=get_ebin_space(md->ebin,3*md->nU,grpnms);
sfree(*grpnms);
sfree(grpnms);
}
if (fp_ene != -1)
do_enxnms(fp_ene,&md->ebin->nener,&md->ebin->enm);
return md;
}
