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50 #include "nonbonded.h"
65 #include "gmx_omp_nthreads.h"
80 gmx_grppairener_t *grppener,
82 gmx_bool bDoLongRangeNS)
88 if (!fr->ns.nblist_initialized)
90 init_neighbor_list(fp, fr, md->homenr);
96 nsearch = search_neighbours(fp,fr,x,box,top,groups,cr,nrnb,md,
97 lambda,dvdlambda,grppener,
98 bFillGrid,bDoLongRangeNS,TRUE);
100 fprintf(debug,"nsearch = %d\n",nsearch);
102 /* Check whether we have to do dynamic load balancing */
103 /*if ((nsb->nstDlb > 0) && (mod(step,nsb->nstDlb) == 0))
104 count_nb(cr,nsb,&(top->blocks[ebCGS]),nns,fr->nlr,
105 &(top->idef),opts->ngener);
107 if (fr->ns.dump_nl > 0)
108 dump_nblist(fp,cr,fr,fr->ns.dump_nl);
111 static void reduce_thread_forces(int n,rvec *f,
114 int efpt_ind,real *dvdl,
115 int nthreads,f_thread_t *f_t)
119 /* This reduction can run over any number of threads */
120 #pragma omp parallel for num_threads(gmx_omp_nthreads_get(emntBonded)) private(t) schedule(static)
123 for(t=1; t<nthreads; t++)
125 rvec_inc(f[i],f_t[t].f[i]);
128 for(t=1; t<nthreads; t++)
130 *Vcorr += f_t[t].Vcorr;
131 *dvdl += f_t[t].dvdl[efpt_ind];
132 m_add(vir,f_t[t].vir,vir);
136 void do_force_lowlevel(FILE *fplog, gmx_large_int_t step,
137 t_forcerec *fr, t_inputrec *ir,
138 t_idef *idef, t_commrec *cr,
139 t_nrnb *nrnb, gmx_wallcycle_t wcycle,
142 rvec x[], history_t *hist,
145 gmx_enerdata_t *enerd,
163 gmx_bool bDoEpot,bSepDVDL,bSB;
167 real Vsr,Vlr,Vcorr=0;
171 gmx_enerdata_t ed_lam;
172 double clam_i,vlam_i;
173 real dvdl_dum[efptNR], dvdl, dvdl_nb[efptNR], lam_i[efptNR];
177 double t0=0.0,t1,t2,t3; /* time measurement for coarse load balancing */
180 #define PRINT_SEPDVDL(s,v,dvdlambda) if (bSepDVDL) fprintf(fplog,sepdvdlformat,s,v,dvdlambda);
183 set_pbc(&pbc,fr->ePBC,box);
185 /* reset free energy components */
186 for (i=0;i<efptNR;i++)
193 for(i=0; (i<DIM); i++)
195 box_size[i]=box[i][i];
198 bSepDVDL=(fr->bSepDVDL && do_per_step(step,ir->nstlog));
201 /* do QMMM first if requested */
204 enerd->term[F_EQM] = calculate_QMMM(cr,x,f,fr,md);
209 fprintf(fplog,"Step %s: non-bonded V and dVdl for node %d:\n",
210 gmx_step_str(step,buf),cr->nodeid);
213 /* Call the short range functions all in one go. */
216 /*#define TAKETIME ((cr->npmenodes) && (fr->timesteps < 12))*/
217 #define TAKETIME FALSE
220 MPI_Barrier(cr->mpi_comm_mygroup);
227 /* foreign lambda component for walls */
228 dvdl = do_walls(ir,fr,box,md,x,f,lambda[efptVDW],
229 enerd->grpp.ener[egLJSR],nrnb);
230 PRINT_SEPDVDL("Walls",0.0,dvdl);
231 enerd->dvdl_lin[efptVDW] += dvdl;
234 /* If doing GB, reset dvda and calculate the Born radii */
235 if (ir->implicit_solvent)
237 wallcycle_sub_start(wcycle, ewcsNONBONDED);
239 for(i=0;i<born->nr;i++)
246 calc_gb_rad(cr,fr,ir,top,atype,x,&(fr->gblist),born,md,nrnb);
249 wallcycle_sub_stop(wcycle, ewcsNONBONDED);
253 /* We only do non-bonded calculation with group scheme here, the verlet
254 * calls are done from do_force_cutsVERLET(). */
255 if (fr->cutoff_scheme == ecutsGROUP && (flags & GMX_FORCE_NONBONDED))
258 /* Add short-range interactions */
259 donb_flags |= GMX_NONBONDED_DO_SR;
261 if (flags & GMX_FORCE_FORCES)
263 donb_flags |= GMX_NONBONDED_DO_FORCE;
265 if (flags & GMX_FORCE_ENERGY)
267 donb_flags |= GMX_NONBONDED_DO_POTENTIAL;
269 if (flags & GMX_FORCE_DO_LR)
271 donb_flags |= GMX_NONBONDED_DO_LR;
274 wallcycle_sub_start(wcycle, ewcsNONBONDED);
275 do_nonbonded(cr,fr,x,f,f_longrange,md,excl,
276 &enerd->grpp,box_size,nrnb,
277 lambda,dvdl_nb,-1,-1,donb_flags);
278 wallcycle_sub_stop(wcycle, ewcsNONBONDED);
281 /* If we do foreign lambda and we have soft-core interactions
282 * we have to recalculate the (non-linear) energies contributions.
284 if (fepvals->n_lambda > 0 && (flags & GMX_FORCE_DHDL) && fepvals->sc_alpha != 0)
286 wallcycle_sub_start(wcycle, ewcsNONBONDED);
287 init_enerdata(mtop->groups.grps[egcENER].nr,fepvals->n_lambda,&ed_lam);
289 for(i=0; i<enerd->n_lambda; i++)
291 for (j=0;j<efptNR;j++)
293 lam_i[j] = (i==0 ? lambda[j] : fepvals->all_lambda[j][i-1]);
295 reset_enerdata(&ir->opts,fr,TRUE,&ed_lam,FALSE);
296 do_nonbonded(cr,fr,x,f,f_longrange,md,excl,
297 &(ed_lam.grpp), box_size,nrnb,
298 lam_i,dvdl_dum,-1,-1,
299 GMX_NONBONDED_DO_FOREIGNLAMBDA | GMX_NONBONDED_DO_SR);
300 sum_epot(&ir->opts,&ed_lam);
301 enerd->enerpart_lambda[i] += ed_lam.term[F_EPOT];
303 destroy_enerdata(&ed_lam);
304 wallcycle_sub_stop(wcycle, ewcsNONBONDED);
308 /* If we are doing GB, calculate bonded forces and apply corrections
309 * to the solvation forces */
310 /* MRS: Eventually, many need to include free energy contribution here! */
311 if (ir->implicit_solvent)
313 wallcycle_sub_start(wcycle, ewcsBONDED);
314 calc_gb_forces(cr,md,born,top,atype,x,f,fr,idef,
315 ir->gb_algorithm,ir->sa_algorithm,nrnb,bBornRadii,&pbc,graph,enerd);
316 wallcycle_sub_stop(wcycle, ewcsBONDED);
327 if (fepvals->sc_alpha!=0)
329 enerd->dvdl_nonlin[efptVDW] += dvdl_nb[efptVDW];
333 enerd->dvdl_lin[efptVDW] += dvdl_nb[efptVDW];
336 if (fepvals->sc_alpha!=0)
338 /* even though coulomb part is linear, we already added it, beacuse we
339 need to go through the vdw calculation anyway */
341 enerd->dvdl_nonlin[efptCOUL] += dvdl_nb[efptCOUL];
345 enerd->dvdl_lin[efptCOUL] += dvdl_nb[efptCOUL];
351 for(i=0; i<enerd->grpp.nener; i++)
355 enerd->grpp.ener[egBHAMSR][i] :
356 enerd->grpp.ener[egLJSR][i])
357 + enerd->grpp.ener[egCOULSR][i] + enerd->grpp.ener[egGB][i];
359 dvdlsum = dvdl_nb[efptVDW] + dvdl_nb[efptCOUL];
360 PRINT_SEPDVDL("VdW and Coulomb SR particle-p.",Vsr,dvdlsum);
367 pr_rvecs(debug,0,"fshift after SR",fr->fshift,SHIFTS);
370 /* Shift the coordinates. Must be done before bonded forces and PPPM,
371 * but is also necessary for SHAKE and update, therefore it can NOT
372 * go when no bonded forces have to be evaluated.
375 /* Here sometimes we would not need to shift with NBFonly,
376 * but we do so anyhow for consistency of the returned coordinates.
380 shift_self(graph,box,x);
383 inc_nrnb(nrnb,eNR_SHIFTX,2*graph->nnodes);
387 inc_nrnb(nrnb,eNR_SHIFTX,graph->nnodes);
390 /* Check whether we need to do bondeds or correct for exclusions */
392 ((flags & GMX_FORCE_BONDED)
393 || EEL_RF(fr->eeltype) || EEL_FULL(fr->eeltype)))
395 /* Since all atoms are in the rectangular or triclinic unit-cell,
396 * only single box vector shifts (2 in x) are required.
398 set_pbc_dd(&pbc,fr->ePBC,cr->dd,TRUE,box);
402 if (flags & GMX_FORCE_BONDED)
404 wallcycle_sub_start(wcycle, ewcsBONDED);
405 calc_bonds(fplog,cr->ms,
406 idef,x,hist,f,fr,&pbc,graph,enerd,nrnb,lambda,md,fcd,
407 DOMAINDECOMP(cr) ? cr->dd->gatindex : NULL, atype, born,
409 fr->bSepDVDL && do_per_step(step,ir->nstlog),step);
411 /* Check if we have to determine energy differences
412 * at foreign lambda's.
414 if (fepvals->n_lambda > 0 && (flags & GMX_FORCE_DHDL) &&
415 idef->ilsort != ilsortNO_FE)
417 if (idef->ilsort != ilsortFE_SORTED)
419 gmx_incons("The bonded interactions are not sorted for free energy");
421 init_enerdata(mtop->groups.grps[egcENER].nr,fepvals->n_lambda,&ed_lam);
423 for(i=0; i<enerd->n_lambda; i++)
425 reset_enerdata(&ir->opts,fr,TRUE,&ed_lam,FALSE);
426 for (j=0;j<efptNR;j++)
428 lam_i[j] = (i==0 ? lambda[j] : fepvals->all_lambda[j][i-1]);
430 calc_bonds_lambda(fplog,idef,x,fr,&pbc,graph,&ed_lam,nrnb,lam_i,md,
431 fcd,DOMAINDECOMP(cr) ? cr->dd->gatindex : NULL);
432 sum_epot(&ir->opts,&ed_lam);
433 enerd->enerpart_lambda[i] += ed_lam.term[F_EPOT];
435 destroy_enerdata(&ed_lam);
439 wallcycle_sub_stop(wcycle, ewcsBONDED);
445 if (EEL_FULL(fr->eeltype))
447 bSB = (ir->nwall == 2);
451 svmul(ir->wall_ewald_zfac,boxs[ZZ],boxs[ZZ]);
452 box_size[ZZ] *= ir->wall_ewald_zfac;
455 clear_mat(fr->vir_el_recip);
462 /* With the Verlet scheme exclusion forces are calculated
463 * in the non-bonded kernel.
465 /* The TPI molecule does not have exclusions with the rest
466 * of the system and no intra-molecular PME grid contributions
467 * will be calculated in gmx_pme_calc_energy.
469 if ((ir->cutoff_scheme == ecutsGROUP && fr->n_tpi == 0) ||
470 ir->ewald_geometry != eewg3D ||
471 ir->epsilon_surface != 0)
475 wallcycle_sub_start(wcycle, ewcsEWALD_CORRECTION);
479 gmx_fatal(FARGS,"TPI with PME currently only works in a 3D geometry with tin-foil boundary conditions");
482 nthreads = gmx_omp_nthreads_get(emntBonded);
483 #pragma omp parallel for num_threads(nthreads) schedule(static)
484 for(t=0; t<nthreads; t++)
492 fnv = fr->f_novirsum;
493 vir = &fr->vir_el_recip;
500 vir = &fr->f_t[t].vir;
501 Vcorrt = &fr->f_t[t].Vcorr;
502 dvdlt = &fr->f_t[t].dvdl[efptCOUL];
503 for(i=0; i<fr->natoms_force; i++)
511 ewald_LRcorrection(fplog,
512 fr->excl_load[t],fr->excl_load[t+1],
515 md->nChargePerturbed ? md->chargeB : NULL,
516 ir->cutoff_scheme != ecutsVERLET,
517 excl,x,bSB ? boxs : box,mu_tot,
521 lambda[efptCOUL],dvdlt);
525 reduce_thread_forces(fr->natoms_force,fr->f_novirsum,
527 &Vcorr,efptCOUL,&dvdl,
531 wallcycle_sub_stop(wcycle, ewcsEWALD_CORRECTION);
536 Vcorr += ewald_charge_correction(cr,fr,lambda[efptCOUL],box,
537 &dvdl,fr->vir_el_recip);
540 PRINT_SEPDVDL("Ewald excl./charge/dip. corr.",Vcorr,dvdl);
541 enerd->dvdl_lin[efptCOUL] += dvdl;
552 case eelPMEUSERSWITCH:
554 if (cr->duty & DUTY_PME)
556 assert(fr->n_tpi >= 0);
557 if (fr->n_tpi == 0 || (flags & GMX_FORCE_STATECHANGED))
559 pme_flags = GMX_PME_SPREAD_Q | GMX_PME_SOLVE;
560 if (flags & GMX_FORCE_FORCES)
562 pme_flags |= GMX_PME_CALC_F;
564 if (flags & (GMX_FORCE_VIRIAL | GMX_FORCE_ENERGY))
566 pme_flags |= GMX_PME_CALC_ENER_VIR;
570 /* We don't calculate f, but we do want the potential */
571 pme_flags |= GMX_PME_CALC_POT;
573 wallcycle_start(wcycle,ewcPMEMESH);
574 status = gmx_pme_do(fr->pmedata,
575 md->start,md->homenr - fr->n_tpi,
577 md->chargeA,md->chargeB,
579 DOMAINDECOMP(cr) ? dd_pme_maxshift_x(cr->dd) : 0,
580 DOMAINDECOMP(cr) ? dd_pme_maxshift_y(cr->dd) : 0,
582 fr->vir_el_recip,fr->ewaldcoeff,
583 &Vlr,lambda[efptCOUL],&dvdl,
585 *cycles_pme = wallcycle_stop(wcycle,ewcPMEMESH);
587 /* We should try to do as little computation after
588 * this as possible, because parallel PME synchronizes
589 * the nodes, so we want all load imbalance of the rest
590 * of the force calculation to be before the PME call.
591 * DD load balancing is done on the whole time of
592 * the force call (without PME).
597 /* Determine the PME grid energy of the test molecule
598 * with the PME grid potential of the other charges.
600 gmx_pme_calc_energy(fr->pmedata,fr->n_tpi,
601 x + md->homenr - fr->n_tpi,
602 md->chargeA + md->homenr - fr->n_tpi,
605 PRINT_SEPDVDL("PME mesh",Vlr,dvdl);
609 Vlr = do_ewald(fplog,FALSE,ir,x,fr->f_novirsum,
610 md->chargeA,md->chargeB,
611 box_size,cr,md->homenr,
612 fr->vir_el_recip,fr->ewaldcoeff,
613 lambda[efptCOUL],&dvdl,fr->ewald_table);
614 PRINT_SEPDVDL("Ewald long-range",Vlr,dvdl);
617 gmx_fatal(FARGS,"No such electrostatics method implemented %s",
618 eel_names[fr->eeltype]);
622 gmx_fatal(FARGS,"Error %d in long range electrostatics routine %s",
623 status,EELTYPE(fr->eeltype));
625 /* Note that with separate PME nodes we get the real energies later */
626 enerd->dvdl_lin[efptCOUL] += dvdl;
627 enerd->term[F_COUL_RECIP] = Vlr + Vcorr;
630 fprintf(debug,"Vlr = %g, Vcorr = %g, Vlr_corr = %g\n",
631 Vlr,Vcorr,enerd->term[F_COUL_RECIP]);
632 pr_rvecs(debug,0,"vir_el_recip after corr",fr->vir_el_recip,DIM);
633 pr_rvecs(debug,0,"fshift after LR Corrections",fr->fshift,SHIFTS);
638 if (EEL_RF(fr->eeltype))
640 /* With the Verlet scheme exclusion forces are calculated
641 * in the non-bonded kernel.
643 if (ir->cutoff_scheme != ecutsVERLET && fr->eeltype != eelRF_NEC)
646 enerd->term[F_RF_EXCL] =
647 RF_excl_correction(fplog,fr,graph,md,excl,x,f,
648 fr->fshift,&pbc,lambda[efptCOUL],&dvdl);
651 enerd->dvdl_lin[efptCOUL] += dvdl;
652 PRINT_SEPDVDL("RF exclusion correction",
653 enerd->term[F_RF_EXCL],dvdl);
661 print_nrnb(debug,nrnb);
669 MPI_Barrier(cr->mpi_comm_mygroup);
672 if (fr->timesteps == 11)
674 fprintf(stderr,"* PP load balancing info: node %d, step %s, rel wait time=%3.0f%% , load string value: %7.2f\n",
675 cr->nodeid, gmx_step_str(fr->timesteps,buf),
676 100*fr->t_wait/(fr->t_wait+fr->t_fnbf),
677 (fr->t_fnbf+fr->t_wait)/fr->t_fnbf);
685 pr_rvecs(debug,0,"fshift after bondeds",fr->fshift,SHIFTS);
690 void init_enerdata(int ngener,int n_lambda,gmx_enerdata_t *enerd)
694 for(i=0; i<F_NRE; i++)
700 for(i=0; i<efptNR; i++) {
701 enerd->dvdl_lin[i] = 0;
702 enerd->dvdl_nonlin[i] = 0;
708 fprintf(debug,"Creating %d sized group matrix for energies\n",n2);
710 enerd->grpp.nener = n2;
711 for(i=0; (i<egNR); i++)
713 snew(enerd->grpp.ener[i],n2);
718 enerd->n_lambda = 1 + n_lambda;
719 snew(enerd->enerpart_lambda,enerd->n_lambda);
727 void destroy_enerdata(gmx_enerdata_t *enerd)
731 for(i=0; (i<egNR); i++)
733 sfree(enerd->grpp.ener[i]);
738 sfree(enerd->enerpart_lambda);
742 static real sum_v(int n,real v[])
754 void sum_epot(t_grpopts *opts,gmx_enerdata_t *enerd)
756 gmx_grppairener_t *grpp;
763 /* Accumulate energies */
764 epot[F_COUL_SR] = sum_v(grpp->nener,grpp->ener[egCOULSR]);
765 epot[F_LJ] = sum_v(grpp->nener,grpp->ener[egLJSR]);
766 epot[F_LJ14] = sum_v(grpp->nener,grpp->ener[egLJ14]);
767 epot[F_COUL14] = sum_v(grpp->nener,grpp->ener[egCOUL14]);
768 epot[F_COUL_LR] = sum_v(grpp->nener,grpp->ener[egCOULLR]);
769 epot[F_LJ_LR] = sum_v(grpp->nener,grpp->ener[egLJLR]);
770 /* We have already added 1-2,1-3, and 1-4 terms to F_GBPOL */
771 epot[F_GBPOL] += sum_v(grpp->nener,grpp->ener[egGB]);
773 /* lattice part of LR doesnt belong to any group
774 * and has been added earlier
776 epot[F_BHAM] = sum_v(grpp->nener,grpp->ener[egBHAMSR]);
777 epot[F_BHAM_LR] = sum_v(grpp->nener,grpp->ener[egBHAMLR]);
780 for(i=0; (i<F_EPOT); i++)
782 if (i != F_DISRESVIOL && i != F_ORIRESDEV)
784 epot[F_EPOT] += epot[i];
789 void sum_dhdl(gmx_enerdata_t *enerd, real *lambda, t_lambda *fepvals)
794 enerd->dvdl_lin[efptVDW] += enerd->term[F_DVDL_VDW]; /* include dispersion correction */
795 enerd->term[F_DVDL] = 0.0;
796 for (i=0;i<efptNR;i++)
798 if (fepvals->separate_dvdl[i])
800 /* could this be done more readably/compactly? */
809 index = F_DVDL_BONDED;
811 case (efptRESTRAINT):
812 index = F_DVDL_RESTRAINT;
821 enerd->term[index] = enerd->dvdl_lin[i] + enerd->dvdl_nonlin[i];
824 fprintf(debug,"dvdl-%s[%2d]: %f: non-linear %f + linear %f\n",
825 efpt_names[i],i,enerd->term[index],enerd->dvdl_nonlin[i],enerd->dvdl_lin[i]);
830 enerd->term[F_DVDL] += enerd->dvdl_lin[i] + enerd->dvdl_nonlin[i];
833 fprintf(debug,"dvd-%sl[%2d]: %f: non-linear %f + linear %f\n",
834 efpt_names[0],i,enerd->term[F_DVDL],enerd->dvdl_nonlin[i],enerd->dvdl_lin[i]);
839 /* Notes on the foreign lambda free energy difference evaluation:
840 * Adding the potential and ekin terms that depend linearly on lambda
841 * as delta lam * dvdl to the energy differences is exact.
842 * For the constraints this is not exact, but we have no other option
843 * without literally changing the lengths and reevaluating the energies at each step.
844 * (try to remedy this post 4.6 - MRS)
845 * For the non-bonded LR term we assume that the soft-core (if present)
846 * no longer affects the energy beyond the short-range cut-off,
847 * which is a very good approximation (except for exotic settings).
848 * (investigate how to overcome this post 4.6 - MRS)
851 for(i=0; i<fepvals->n_lambda; i++)
852 { /* note we are iterating over fepvals here!
853 For the current lam, dlam = 0 automatically,
854 so we don't need to add anything to the
855 enerd->enerpart_lambda[0] */
857 /* we don't need to worry about dvdl contributions to the current lambda, because
858 it's automatically zero */
860 /* first kinetic energy term */
861 dlam = (fepvals->all_lambda[efptMASS][i] - lambda[efptMASS]);
863 enerd->enerpart_lambda[i+1] += enerd->term[F_DKDL]*dlam;
865 for (j=0;j<efptNR;j++)
867 if (j==efptMASS) {continue;} /* no other mass term to worry about */
869 dlam = (fepvals->all_lambda[j][i]-lambda[j]);
870 enerd->enerpart_lambda[i+1] += dlam*enerd->dvdl_lin[j];
873 fprintf(debug,"enerdiff lam %g: (%15s), non-linear %f linear %f*%f\n",
874 fepvals->all_lambda[j][i],efpt_names[j],
875 (enerd->enerpart_lambda[i+1] - enerd->enerpart_lambda[0]),
876 dlam,enerd->dvdl_lin[j]);
882 void reset_enerdata(t_grpopts *opts,
883 t_forcerec *fr,gmx_bool bNS,
884 gmx_enerdata_t *enerd,
890 /* First reset all energy components, except for the long range terms
891 * on the master at non neighbor search steps, since the long range
892 * terms have already been summed at the last neighbor search step.
894 bKeepLR = (fr->bTwinRange && !bNS);
895 for(i=0; (i<egNR); i++) {
896 if (!(bKeepLR && bMaster && (i == egCOULLR || i == egLJLR))) {
897 for(j=0; (j<enerd->grpp.nener); j++)
898 enerd->grpp.ener[i][j] = 0.0;
901 for (i=0;i<efptNR;i++)
903 enerd->dvdl_lin[i] = 0.0;
904 enerd->dvdl_nonlin[i] = 0.0;
907 /* Normal potential energy components */
908 for(i=0; (i<=F_EPOT); i++) {
909 enerd->term[i] = 0.0;
911 /* Initialize the dVdlambda term with the long range contribution */
912 /* Initialize the dvdl term with the long range contribution */
913 enerd->term[F_DVDL] = 0.0;
914 enerd->term[F_DVDL_COUL] = 0.0;
915 enerd->term[F_DVDL_VDW] = 0.0;
916 enerd->term[F_DVDL_BONDED] = 0.0;
917 enerd->term[F_DVDL_RESTRAINT] = 0.0;
918 enerd->term[F_DKDL] = 0.0;
919 if (enerd->n_lambda > 0)
921 for(i=0; i<enerd->n_lambda; i++)
923 enerd->enerpart_lambda[i] = 0.0;