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41 #include<catamount/dclock.h>
47 #ifdef HAVE_SYS_TIME_H
60 #include "chargegroup.h"
84 #include "mpelogging.h"
87 #include "gmx_wallcycle.h"
100 typedef struct gmx_timeprint {
105 /* Portable version of ctime_r implemented in src/gmxlib/string2.c, but we do not want it declared in public installed headers */
107 gmx_ctime_r(const time_t *clock,char *buf, int n);
113 #ifdef HAVE_GETTIMEOFDAY
115 struct timezone tz = { 0,0 };
118 gettimeofday(&t,&tz);
120 seconds = (double) t.tv_sec + 1e-6*(double)t.tv_usec;
126 seconds = time(NULL);
133 #define difftime(end,start) ((double)(end)-(double)(start))
135 void print_time(FILE *out,gmx_runtime_t *runtime,gmx_large_int_t step,
136 t_inputrec *ir, t_commrec *cr)
139 char timebuf[STRLEN];
149 fprintf(out,"step %s",gmx_step_str(step,buf));
150 if ((step >= ir->nstlist))
152 if ((ir->nstlist == 0) || ((step % ir->nstlist) == 0))
154 /* We have done a full cycle let's update time_per_step */
155 runtime->last = gmx_gettime();
156 dt = difftime(runtime->last,runtime->real);
157 runtime->time_per_step = dt/(step - ir->init_step + 1);
159 dt = (ir->nsteps + ir->init_step - step)*runtime->time_per_step;
165 finish = (time_t) (runtime->last + dt);
166 gmx_ctime_r(&finish,timebuf,STRLEN);
167 sprintf(buf,"%s",timebuf);
168 buf[strlen(buf)-1]='\0';
169 fprintf(out,", will finish %s",buf);
172 fprintf(out,", remaining runtime: %5d s ",(int)dt);
176 fprintf(out," performance: %.1f ns/day ",
177 ir->delta_t/1000*24*60*60/runtime->time_per_step);
194 static double set_proctime(gmx_runtime_t *runtime)
200 prev = runtime->proc;
201 runtime->proc = dclock();
203 diff = runtime->proc - prev;
207 prev = runtime->proc;
208 runtime->proc = clock();
210 diff = (double)(runtime->proc - prev)/(double)CLOCKS_PER_SEC;
214 /* The counter has probably looped, ignore this data */
221 void runtime_start(gmx_runtime_t *runtime)
223 runtime->real = gmx_gettime();
225 set_proctime(runtime);
226 runtime->realtime = 0;
227 runtime->proctime = 0;
229 runtime->time_per_step = 0;
232 void runtime_end(gmx_runtime_t *runtime)
238 runtime->proctime += set_proctime(runtime);
239 runtime->realtime = now - runtime->real;
243 void runtime_upd_proc(gmx_runtime_t *runtime)
245 runtime->proctime += set_proctime(runtime);
248 void print_date_and_time(FILE *fplog,int nodeid,const char *title,
249 const gmx_runtime_t *runtime)
252 char timebuf[STRLEN];
253 char time_string[STRLEN];
260 tmptime = (time_t) runtime->real;
261 gmx_ctime_r(&tmptime,timebuf,STRLEN);
265 tmptime = (time_t) gmx_gettime();
266 gmx_ctime_r(&tmptime,timebuf,STRLEN);
268 for(i=0; timebuf[i]>=' '; i++)
270 time_string[i]=timebuf[i];
274 fprintf(fplog,"%s on node %d %s\n",title,nodeid,time_string);
278 static void sum_forces(int start,int end,rvec f[],rvec flr[])
283 pr_rvecs(debug,0,"fsr",f+start,end-start);
284 pr_rvecs(debug,0,"flr",flr+start,end-start);
286 for(i=start; (i<end); i++)
287 rvec_inc(f[i],flr[i]);
291 * calc_f_el calculates forces due to an electric field.
293 * force is kJ mol^-1 nm^-1 = e * kJ mol^-1 nm^-1 / e
295 * Et[] contains the parameters for the time dependent
296 * part of the field (not yet used).
297 * Ex[] contains the parameters for
298 * the spatial dependent part of the field. You can have cool periodic
299 * fields in principle, but only a constant field is supported
301 * The function should return the energy due to the electric field
302 * (if any) but for now returns 0.
305 * There can be problems with the virial.
306 * Since the field is not self-consistent this is unavoidable.
307 * For neutral molecules the virial is correct within this approximation.
308 * For neutral systems with many charged molecules the error is small.
309 * But for systems with a net charge or a few charged molecules
310 * the error can be significant when the field is high.
311 * Solution: implement a self-consitent electric field into PME.
313 static void calc_f_el(FILE *fp,int start,int homenr,
314 real charge[],rvec x[],rvec f[],
315 t_cosines Ex[],t_cosines Et[],double t)
321 for(m=0; (m<DIM); m++)
328 Ext[m] = cos(Et[m].a[0]*(t-t0))*exp(-sqr(t-t0)/(2.0*sqr(Et[m].a[2])));
332 Ext[m] = cos(Et[m].a[0]*t);
341 /* Convert the field strength from V/nm to MD-units */
342 Ext[m] *= Ex[m].a[0]*FIELDFAC;
343 for(i=start; (i<start+homenr); i++)
344 f[i][m] += charge[i]*Ext[m];
353 fprintf(fp,"%10g %10g %10g %10g #FIELD\n",t,
354 Ext[XX]/FIELDFAC,Ext[YY]/FIELDFAC,Ext[ZZ]/FIELDFAC);
358 static void calc_virial(FILE *fplog,int start,int homenr,rvec x[],rvec f[],
359 tensor vir_part,t_graph *graph,matrix box,
360 t_nrnb *nrnb,const t_forcerec *fr,int ePBC)
365 /* The short-range virial from surrounding boxes */
367 calc_vir(fplog,SHIFTS,fr->shift_vec,fr->fshift,vir_part,ePBC==epbcSCREW,box);
368 inc_nrnb(nrnb,eNR_VIRIAL,SHIFTS);
370 /* Calculate partial virial, for local atoms only, based on short range.
371 * Total virial is computed in global_stat, called from do_md
373 f_calc_vir(fplog,start,start+homenr,x,f,vir_part,graph,box);
374 inc_nrnb(nrnb,eNR_VIRIAL,homenr);
376 /* Add position restraint contribution */
377 for(i=0; i<DIM; i++) {
378 vir_part[i][i] += fr->vir_diag_posres[i];
381 /* Add wall contribution */
382 for(i=0; i<DIM; i++) {
383 vir_part[i][ZZ] += fr->vir_wall_z[i];
387 pr_rvecs(debug,0,"vir_part",vir_part,DIM);
390 static void print_large_forces(FILE *fp,t_mdatoms *md,t_commrec *cr,
391 gmx_large_int_t step,real pforce,rvec *x,rvec *f)
395 char buf[STEPSTRSIZE];
398 for(i=md->start; i<md->start+md->homenr; i++) {
400 /* We also catch NAN, if the compiler does not optimize this away. */
401 if (fn2 >= pf2 || fn2 != fn2) {
402 fprintf(fp,"step %s atom %6d x %8.3f %8.3f %8.3f force %12.5e\n",
403 gmx_step_str(step,buf),
404 ddglatnr(cr->dd,i),x[i][XX],x[i][YY],x[i][ZZ],sqrt(fn2));
409 void do_force(FILE *fplog,t_commrec *cr,
410 t_inputrec *inputrec,
411 gmx_large_int_t step,t_nrnb *nrnb,gmx_wallcycle_t wcycle,
414 gmx_groups_t *groups,
415 matrix box,rvec x[],history_t *hist,
419 gmx_enerdata_t *enerd,t_fcdata *fcd,
420 real lambda,t_graph *graph,
421 t_forcerec *fr,gmx_vsite_t *vsite,rvec mu_tot,
422 double t,FILE *field,gmx_edsam_t ed,
429 gmx_bool bSepDVDL,bStateChanged,bNS,bFillGrid,bCalcCGCM,bBS;
430 gmx_bool bDoLongRange,bDoForces,bSepLRF;
434 float cycles_ppdpme,cycles_pme,cycles_seppme,cycles_force;
436 start = mdatoms->start;
437 homenr = mdatoms->homenr;
439 bSepDVDL = (fr->bSepDVDL && do_per_step(step,inputrec->nstlog));
441 clear_mat(vir_force);
445 pd_cg_range(cr,&cg0,&cg1);
450 if (DOMAINDECOMP(cr))
452 cg1 = cr->dd->ncg_tot;
464 bStateChanged = (flags & GMX_FORCE_STATECHANGED);
465 bNS = (flags & GMX_FORCE_NS) && (fr->bAllvsAll==FALSE);
466 bFillGrid = (bNS && bStateChanged);
467 bCalcCGCM = (bFillGrid && !DOMAINDECOMP(cr));
468 bDoLongRange = (fr->bTwinRange && bNS && (flags & GMX_FORCE_DOLR));
469 bDoForces = (flags & GMX_FORCE_FORCES);
470 bSepLRF = (bDoLongRange && bDoForces && (flags & GMX_FORCE_SEPLRF));
474 update_forcerec(fplog,fr,box);
476 /* Calculate total (local) dipole moment in a temporary common array.
477 * This makes it possible to sum them over nodes faster.
479 calc_mu(start,homenr,
480 x,mdatoms->chargeA,mdatoms->chargeB,mdatoms->nChargePerturbed,
484 if (fr->ePBC != epbcNONE) {
485 /* Compute shift vectors every step,
486 * because of pressure coupling or box deformation!
488 if ((flags & GMX_FORCE_DYNAMICBOX) && bStateChanged)
489 calc_shifts(box,fr->shift_vec);
492 put_charge_groups_in_box(fplog,cg0,cg1,fr->ePBC,box,
493 &(top->cgs),x,fr->cg_cm);
494 inc_nrnb(nrnb,eNR_CGCM,homenr);
495 inc_nrnb(nrnb,eNR_RESETX,cg1-cg0);
497 else if (EI_ENERGY_MINIMIZATION(inputrec->eI) && graph) {
498 unshift_self(graph,box,x);
501 else if (bCalcCGCM) {
502 calc_cgcm(fplog,cg0,cg1,&(top->cgs),x,fr->cg_cm);
503 inc_nrnb(nrnb,eNR_CGCM,homenr);
508 move_cgcm(fplog,cr,fr->cg_cm);
511 pr_rvecs(debug,0,"cgcm",fr->cg_cm,top->cgs.nr);
515 if (!(cr->duty & DUTY_PME)) {
516 /* Send particle coordinates to the pme nodes.
517 * Since this is only implemented for domain decomposition
518 * and domain decomposition does not use the graph,
519 * we do not need to worry about shifting.
522 wallcycle_start(wcycle,ewcPP_PMESENDX);
523 GMX_MPE_LOG(ev_send_coordinates_start);
525 bBS = (inputrec->nwall == 2);
528 svmul(inputrec->wall_ewald_zfac,boxs[ZZ],boxs[ZZ]);
531 gmx_pme_send_x(cr,bBS ? boxs : box,x,
532 mdatoms->nChargePerturbed,lambda,
533 ( flags & GMX_FORCE_VIRIAL),step);
535 GMX_MPE_LOG(ev_send_coordinates_finish);
536 wallcycle_stop(wcycle,ewcPP_PMESENDX);
540 /* Communicate coordinates and sum dipole if necessary */
543 wallcycle_start(wcycle,ewcMOVEX);
544 if (DOMAINDECOMP(cr))
546 dd_move_x(cr->dd,box,x);
550 move_x(fplog,cr,GMX_LEFT,GMX_RIGHT,x,nrnb);
552 /* When we don't need the total dipole we sum it in global_stat */
553 if (bStateChanged && NEED_MUTOT(*inputrec))
555 gmx_sumd(2*DIM,mu,cr);
557 wallcycle_stop(wcycle,ewcMOVEX);
565 fr->mu_tot[i][j] = mu[i*DIM + j];
569 if (fr->efep == efepNO)
571 copy_rvec(fr->mu_tot[0],mu_tot);
578 (1.0 - lambda)*fr->mu_tot[0][j] + lambda*fr->mu_tot[1][j];
583 reset_enerdata(&(inputrec->opts),fr,bNS,enerd,MASTER(cr));
584 clear_rvecs(SHIFTS,fr->fshift);
588 wallcycle_start(wcycle,ewcNS);
590 if (graph && bStateChanged)
592 /* Calculate intramolecular shift vectors to make molecules whole */
593 mk_mshift(fplog,graph,fr->ePBC,box,x);
596 /* Reset long range forces if necessary */
599 /* Reset the (long-range) forces if necessary */
600 clear_rvecs(fr->natoms_force_constr,bSepLRF ? fr->f_twin : f);
603 /* Do the actual neighbour searching and if twin range electrostatics
604 * also do the calculation of long range forces and energies.
608 groups,&(inputrec->opts),top,mdatoms,
609 cr,nrnb,lambda,&dvdl,&enerd->grpp,bFillGrid,
610 bDoLongRange,bDoForces,bSepLRF ? fr->f_twin : f);
613 fprintf(fplog,sepdvdlformat,"LR non-bonded",0.0,dvdl);
615 enerd->dvdl_lin += dvdl;
617 wallcycle_stop(wcycle,ewcNS);
620 if (inputrec->implicit_solvent && bNS)
622 make_gb_nblist(cr,inputrec->gb_algorithm,inputrec->rlist,
623 x,box,fr,&top->idef,graph,fr->born);
626 if (DOMAINDECOMP(cr))
628 if (!(cr->duty & DUTY_PME))
630 wallcycle_start(wcycle,ewcPPDURINGPME);
631 dd_force_flop_start(cr->dd,nrnb);
635 /* Start the force cycle counter.
636 * This counter is stopped in do_forcelow_level.
637 * No parallel communication should occur while this counter is running,
638 * since that will interfere with the dynamic load balancing.
640 wallcycle_start(wcycle,ewcFORCE);
644 /* Reset forces for which the virial is calculated separately:
645 * PME/Ewald forces if necessary */
648 if (flags & GMX_FORCE_VIRIAL)
650 fr->f_novirsum = fr->f_novirsum_alloc;
651 GMX_BARRIER(cr->mpi_comm_mygroup);
654 clear_rvecs(fr->f_novirsum_n,fr->f_novirsum);
658 clear_rvecs(homenr,fr->f_novirsum+start);
660 GMX_BARRIER(cr->mpi_comm_mygroup);
664 /* We are not calculating the pressure so we do not need
665 * a separate array for forces that do not contribute
674 /* Add the long range forces to the short range forces */
675 for(i=0; i<fr->natoms_force_constr; i++)
677 copy_rvec(fr->f_twin[i],f[i]);
680 else if (!(fr->bTwinRange && bNS))
682 /* Clear the short-range forces */
683 clear_rvecs(fr->natoms_force_constr,f);
686 clear_rvec(fr->vir_diag_posres);
688 GMX_BARRIER(cr->mpi_comm_mygroup);
690 if (inputrec->ePull == epullCONSTRAINT)
692 clear_pull_forces(inputrec->pull);
695 /* update QMMMrec, if necessary */
698 update_QMMMrec(cr,fr,x,mdatoms,box,top);
701 if ((flags & GMX_FORCE_BONDED) && top->idef.il[F_POSRES].nr > 0)
703 /* Position restraints always require full pbc */
704 set_pbc(&pbc,inputrec->ePBC,box);
705 v = posres(top->idef.il[F_POSRES].nr,top->idef.il[F_POSRES].iatoms,
706 top->idef.iparams_posres,
707 (const rvec*)x,fr->f_novirsum,fr->vir_diag_posres,
708 inputrec->ePBC==epbcNONE ? NULL : &pbc,lambda,&dvdl,
709 fr->rc_scaling,fr->ePBC,fr->posres_com,fr->posres_comB);
712 fprintf(fplog,sepdvdlformat,
713 interaction_function[F_POSRES].longname,v,dvdl);
715 enerd->term[F_POSRES] += v;
716 /* This linear lambda dependence assumption is only correct
717 * when only k depends on lambda,
718 * not when the reference position depends on lambda.
719 * grompp checks for this.
721 enerd->dvdl_lin += dvdl;
722 inc_nrnb(nrnb,eNR_POSRES,top->idef.il[F_POSRES].nr/2);
725 /* Compute the bonded and non-bonded energies and optionally forces */
726 do_force_lowlevel(fplog,step,fr,inputrec,&(top->idef),
727 cr,nrnb,wcycle,mdatoms,&(inputrec->opts),
728 x,hist,f,enerd,fcd,mtop,top,fr->born,
729 &(top->atomtypes),bBornRadii,box,
730 lambda,graph,&(top->excls),fr->mu_tot,
733 cycles_force = wallcycle_stop(wcycle,ewcFORCE);
734 GMX_BARRIER(cr->mpi_comm_mygroup);
738 do_flood(fplog,cr,x,f,ed,box,step);
741 if (DOMAINDECOMP(cr))
743 dd_force_flop_stop(cr->dd,nrnb);
746 dd_cycles_add(cr->dd,cycles_force-cycles_pme,ddCyclF);
752 if (IR_ELEC_FIELD(*inputrec))
754 /* Compute forces due to electric field */
755 calc_f_el(MASTER(cr) ? field : NULL,
756 start,homenr,mdatoms->chargeA,x,fr->f_novirsum,
757 inputrec->ex,inputrec->et,t);
760 /* Communicate the forces */
763 wallcycle_start(wcycle,ewcMOVEF);
764 if (DOMAINDECOMP(cr))
766 dd_move_f(cr->dd,f,fr->fshift);
767 /* Do we need to communicate the separate force array
768 * for terms that do not contribute to the single sum virial?
769 * Position restraints and electric fields do not introduce
770 * inter-cg forces, only full electrostatics methods do.
771 * When we do not calculate the virial, fr->f_novirsum = f,
772 * so we have already communicated these forces.
774 if (EEL_FULL(fr->eeltype) && cr->dd->n_intercg_excl &&
775 (flags & GMX_FORCE_VIRIAL))
777 dd_move_f(cr->dd,fr->f_novirsum,NULL);
781 /* We should not update the shift forces here,
782 * since f_twin is already included in f.
784 dd_move_f(cr->dd,fr->f_twin,NULL);
789 pd_move_f(cr,f,nrnb);
792 pd_move_f(cr,fr->f_twin,nrnb);
795 wallcycle_stop(wcycle,ewcMOVEF);
798 /* If we have NoVirSum forces, but we do not calculate the virial,
799 * we sum fr->f_novirum=f later.
801 if (vsite && !(fr->bF_NoVirSum && !(flags & GMX_FORCE_VIRIAL)))
803 wallcycle_start(wcycle,ewcVSITESPREAD);
804 spread_vsite_f(fplog,vsite,x,f,fr->fshift,nrnb,
805 &top->idef,fr->ePBC,fr->bMolPBC,graph,box,cr);
806 wallcycle_stop(wcycle,ewcVSITESPREAD);
810 wallcycle_start(wcycle,ewcVSITESPREAD);
811 spread_vsite_f(fplog,vsite,x,fr->f_twin,NULL,
813 &top->idef,fr->ePBC,fr->bMolPBC,graph,box,cr);
814 wallcycle_stop(wcycle,ewcVSITESPREAD);
818 if (flags & GMX_FORCE_VIRIAL)
820 /* Calculation of the virial must be done after vsites! */
821 calc_virial(fplog,mdatoms->start,mdatoms->homenr,x,f,
822 vir_force,graph,box,nrnb,fr,inputrec->ePBC);
826 if (inputrec->ePull == epullUMBRELLA || inputrec->ePull == epullCONST_F)
828 /* Calculate the center of mass forces, this requires communication,
829 * which is why pull_potential is called close to other communication.
830 * The virial contribution is calculated directly,
831 * which is why we call pull_potential after calc_virial.
833 set_pbc(&pbc,inputrec->ePBC,box);
835 enerd->term[F_COM_PULL] =
836 pull_potential(inputrec->ePull,inputrec->pull,mdatoms,&pbc,
837 cr,t,lambda,x,f,vir_force,&dvdl);
840 fprintf(fplog,sepdvdlformat,"Com pull",enerd->term[F_COM_PULL],dvdl);
842 enerd->dvdl_lin += dvdl;
845 if (PAR(cr) && !(cr->duty & DUTY_PME))
847 cycles_ppdpme = wallcycle_stop(wcycle,ewcPPDURINGPME);
848 dd_cycles_add(cr->dd,cycles_ppdpme,ddCyclPPduringPME);
850 /* In case of node-splitting, the PP nodes receive the long-range
851 * forces, virial and energy from the PME nodes here.
853 wallcycle_start(wcycle,ewcPP_PMEWAITRECVF);
855 gmx_pme_receive_f(cr,fr->f_novirsum,fr->vir_el_recip,&e,&dvdl,
859 fprintf(fplog,sepdvdlformat,"PME mesh",e,dvdl);
861 enerd->term[F_COUL_RECIP] += e;
862 enerd->dvdl_lin += dvdl;
865 dd_cycles_add(cr->dd,cycles_seppme,ddCyclPME);
867 wallcycle_stop(wcycle,ewcPP_PMEWAITRECVF);
870 if (bDoForces && fr->bF_NoVirSum)
874 /* Spread the mesh force on virtual sites to the other particles...
875 * This is parallellized. MPI communication is performed
876 * if the constructing atoms aren't local.
878 wallcycle_start(wcycle,ewcVSITESPREAD);
879 spread_vsite_f(fplog,vsite,x,fr->f_novirsum,NULL,nrnb,
880 &top->idef,fr->ePBC,fr->bMolPBC,graph,box,cr);
881 wallcycle_stop(wcycle,ewcVSITESPREAD);
883 if (flags & GMX_FORCE_VIRIAL)
885 /* Now add the forces, this is local */
888 sum_forces(0,fr->f_novirsum_n,f,fr->f_novirsum);
892 sum_forces(start,start+homenr,f,fr->f_novirsum);
894 if (EEL_FULL(fr->eeltype))
896 /* Add the mesh contribution to the virial */
897 m_add(vir_force,fr->vir_el_recip,vir_force);
901 pr_rvecs(debug,0,"vir_force",vir_force,DIM);
906 /* Sum the potential energy terms from group contributions */
907 sum_epot(&(inputrec->opts),enerd);
909 if (fr->print_force >= 0 && bDoForces)
911 print_large_forces(stderr,mdatoms,cr,step,fr->print_force,x,f);
915 void do_constrain_first(FILE *fplog,gmx_constr_t constr,
916 t_inputrec *ir,t_mdatoms *md,
917 t_state *state,rvec *f,
918 t_graph *graph,t_commrec *cr,t_nrnb *nrnb,
919 t_forcerec *fr, gmx_localtop_t *top, tensor shake_vir)
922 gmx_large_int_t step;
923 double mass,tmass,vcm[4];
928 snew(savex,state->natoms);
931 end = md->homenr + start;
934 fprintf(debug,"vcm: start=%d, homenr=%d, end=%d\n",
935 start,md->homenr,end);
936 /* Do a first constrain to reset particles... */
937 step = ir->init_step;
940 char buf[STEPSTRSIZE];
941 fprintf(fplog,"\nConstraining the starting coordinates (step %s)\n",
942 gmx_step_str(step,buf));
946 /* constrain the current position */
947 constrain(NULL,TRUE,FALSE,constr,&(top->idef),
948 ir,NULL,cr,step,0,md,
949 state->x,state->x,NULL,
950 state->box,state->lambda,&dvdlambda,
951 NULL,NULL,nrnb,econqCoord,ir->epc==epcMTTK,state->veta,state->veta);
954 /* constrain the inital velocity, and save it */
955 /* also may be useful if we need the ekin from the halfstep for velocity verlet */
956 /* might not yet treat veta correctly */
957 constrain(NULL,TRUE,FALSE,constr,&(top->idef),
958 ir,NULL,cr,step,0,md,
959 state->x,state->v,state->v,
960 state->box,state->lambda,&dvdlambda,
961 NULL,NULL,nrnb,econqVeloc,ir->epc==epcMTTK,state->veta,state->veta);
963 /* constrain the inital velocities at t-dt/2 */
964 if (EI_STATE_VELOCITY(ir->eI) && ir->eI!=eiVV)
966 for(i=start; (i<end); i++)
968 for(m=0; (m<DIM); m++)
970 /* Reverse the velocity */
971 state->v[i][m] = -state->v[i][m];
972 /* Store the position at t-dt in buf */
973 savex[i][m] = state->x[i][m] + dt*state->v[i][m];
976 /* Shake the positions at t=-dt with the positions at t=0
977 * as reference coordinates.
981 char buf[STEPSTRSIZE];
982 fprintf(fplog,"\nConstraining the coordinates at t0-dt (step %s)\n",
983 gmx_step_str(step,buf));
986 constrain(NULL,TRUE,FALSE,constr,&(top->idef),
987 ir,NULL,cr,step,-1,md,
989 state->box,state->lambda,&dvdlambda,
990 state->v,NULL,nrnb,econqCoord,ir->epc==epcMTTK,state->veta,state->veta);
992 for(i=start; i<end; i++) {
993 for(m=0; m<DIM; m++) {
994 /* Re-reverse the velocities */
995 state->v[i][m] = -state->v[i][m];
1000 for(m=0; (m<4); m++)
1002 for(i=start; i<end; i++) {
1003 mass = md->massT[i];
1004 for(m=0; m<DIM; m++) {
1005 vcm[m] += state->v[i][m]*mass;
1010 if (ir->nstcomm != 0 || debug) {
1011 /* Compute the global sum of vcm */
1013 fprintf(debug,"vcm: %8.3f %8.3f %8.3f,"
1014 " total mass = %12.5e\n",vcm[XX],vcm[YY],vcm[ZZ],vcm[3]);
1018 for(m=0; (m<DIM); m++)
1021 fprintf(debug,"vcm: %8.3f %8.3f %8.3f,"
1022 " total mass = %12.5e\n",vcm[XX],vcm[YY],vcm[ZZ],tmass);
1023 if (ir->nstcomm != 0) {
1024 /* Now we have the velocity of center of mass, let's remove it */
1025 for(i=start; (i<end); i++) {
1026 for(m=0; (m<DIM); m++)
1027 state->v[i][m] -= vcm[m];
1035 void calc_enervirdiff(FILE *fplog,int eDispCorr,t_forcerec *fr)
1037 double eners[2],virs[2],enersum,virsum,y0,f,g,h;
1038 double r0,r1,r,rc3,rc9,ea,eb,ec,pa,pb,pc,pd;
1039 double invscale,invscale2,invscale3;
1040 int ri0,ri1,ri,i,offstart,offset;
1043 fr->enershiftsix = 0;
1044 fr->enershifttwelve = 0;
1045 fr->enerdiffsix = 0;
1046 fr->enerdifftwelve = 0;
1048 fr->virdifftwelve = 0;
1050 if (eDispCorr != edispcNO) {
1051 for(i=0; i<2; i++) {
1055 if ((fr->vdwtype == evdwSWITCH) || (fr->vdwtype == evdwSHIFT)) {
1056 if (fr->rvdw_switch == 0)
1058 "With dispersion correction rvdw-switch can not be zero "
1059 "for vdw-type = %s",evdw_names[fr->vdwtype]);
1061 scale = fr->nblists[0].tab.scale;
1062 vdwtab = fr->nblists[0].vdwtab;
1064 /* Round the cut-offs to exact table values for precision */
1065 ri0 = floor(fr->rvdw_switch*scale);
1066 ri1 = ceil(fr->rvdw*scale);
1072 if (fr->vdwtype == evdwSHIFT) {
1073 /* Determine the constant energy shift below rvdw_switch */
1074 fr->enershiftsix = (real)(-1.0/(rc3*rc3)) - vdwtab[8*ri0];
1075 fr->enershifttwelve = (real)( 1.0/(rc9*rc3)) - vdwtab[8*ri0 + 4];
1077 /* Add the constant part from 0 to rvdw_switch.
1078 * This integration from 0 to rvdw_switch overcounts the number
1079 * of interactions by 1, as it also counts the self interaction.
1080 * We will correct for this later.
1082 eners[0] += 4.0*M_PI*fr->enershiftsix*rc3/3.0;
1083 eners[1] += 4.0*M_PI*fr->enershifttwelve*rc3/3.0;
1085 invscale = 1.0/(scale);
1086 invscale2 = invscale*invscale;
1087 invscale3 = invscale*invscale2;
1089 /* following summation derived from cubic spline definition,
1090 Numerical Recipies in C, second edition, p. 113-116. Exact
1091 for the cubic spline. We first calculate the negative of
1092 the energy from rvdw to rvdw_switch, assuming that g(r)=1,
1093 and then add the more standard, abrupt cutoff correction to
1094 that result, yielding the long-range correction for a
1095 switched function. We perform both the pressure and energy
1096 loops at the same time for simplicity, as the computational
1100 enersum = 0.0; virsum = 0.0;
1105 for (ri=ri0; ri<ri1; ri++) {
1108 eb = 2.0*invscale2*r;
1112 pb = 3.0*invscale2*r;
1113 pc = 3.0*invscale*r*r;
1116 /* this "8" is from the packing in the vdwtab array - perhaps
1117 should be #define'ed? */
1118 offset = 8*ri + offstart;
1119 y0 = vdwtab[offset];
1120 f = vdwtab[offset+1];
1121 g = vdwtab[offset+2];
1122 h = vdwtab[offset+3];
1124 enersum += y0*(ea/3 + eb/2 + ec) + f*(ea/4 + eb/3 + ec/2)+
1125 g*(ea/5 + eb/4 + ec/3) + h*(ea/6 + eb/5 + ec/4);
1126 virsum += f*(pa/4 + pb/3 + pc/2 + pd) +
1127 2*g*(pa/5 + pb/4 + pc/3 + pd/2) + 3*h*(pa/6 + pb/5 + pc/4 + pd/3);
1130 enersum *= 4.0*M_PI;
1132 eners[i] -= enersum;
1136 /* now add the correction for rvdw_switch to infinity */
1137 eners[0] += -4.0*M_PI/(3.0*rc3);
1138 eners[1] += 4.0*M_PI/(9.0*rc9);
1139 virs[0] += 8.0*M_PI/rc3;
1140 virs[1] += -16.0*M_PI/(3.0*rc9);
1142 else if ((fr->vdwtype == evdwCUT) || (fr->vdwtype == evdwUSER)) {
1143 if (fr->vdwtype == evdwUSER && fplog)
1145 "WARNING: using dispersion correction with user tables\n");
1146 rc3 = fr->rvdw*fr->rvdw*fr->rvdw;
1148 eners[0] += -4.0*M_PI/(3.0*rc3);
1149 eners[1] += 4.0*M_PI/(9.0*rc9);
1150 virs[0] += 8.0*M_PI/rc3;
1151 virs[1] += -16.0*M_PI/(3.0*rc9);
1154 "Dispersion correction is not implemented for vdw-type = %s",
1155 evdw_names[fr->vdwtype]);
1157 fr->enerdiffsix = eners[0];
1158 fr->enerdifftwelve = eners[1];
1159 /* The 0.5 is due to the Gromacs definition of the virial */
1160 fr->virdiffsix = 0.5*virs[0];
1161 fr->virdifftwelve = 0.5*virs[1];
1165 void calc_dispcorr(FILE *fplog,t_inputrec *ir,t_forcerec *fr,
1166 gmx_large_int_t step,int natoms,
1167 matrix box,real lambda,tensor pres,tensor virial,
1168 real *prescorr, real *enercorr, real *dvdlcorr)
1170 gmx_bool bCorrAll,bCorrPres;
1171 real dvdlambda,invvol,dens,ninter,avcsix,avctwelve,enerdiff,svir=0,spres=0;
1181 if (ir->eDispCorr != edispcNO) {
1182 bCorrAll = (ir->eDispCorr == edispcAllEner ||
1183 ir->eDispCorr == edispcAllEnerPres);
1184 bCorrPres = (ir->eDispCorr == edispcEnerPres ||
1185 ir->eDispCorr == edispcAllEnerPres);
1187 invvol = 1/det(box);
1190 /* Only correct for the interactions with the inserted molecule */
1191 dens = (natoms - fr->n_tpi)*invvol;
1196 dens = natoms*invvol;
1197 ninter = 0.5*natoms;
1200 if (ir->efep == efepNO)
1202 avcsix = fr->avcsix[0];
1203 avctwelve = fr->avctwelve[0];
1207 avcsix = (1 - lambda)*fr->avcsix[0] + lambda*fr->avcsix[1];
1208 avctwelve = (1 - lambda)*fr->avctwelve[0] + lambda*fr->avctwelve[1];
1211 enerdiff = ninter*(dens*fr->enerdiffsix - fr->enershiftsix);
1212 *enercorr += avcsix*enerdiff;
1214 if (ir->efep != efepNO)
1216 dvdlambda += (fr->avcsix[1] - fr->avcsix[0])*enerdiff;
1220 enerdiff = ninter*(dens*fr->enerdifftwelve - fr->enershifttwelve);
1221 *enercorr += avctwelve*enerdiff;
1222 if (fr->efep != efepNO)
1224 dvdlambda += (fr->avctwelve[1] - fr->avctwelve[0])*enerdiff;
1230 svir = ninter*dens*avcsix*fr->virdiffsix/3.0;
1231 if (ir->eDispCorr == edispcAllEnerPres)
1233 svir += ninter*dens*avctwelve*fr->virdifftwelve/3.0;
1235 /* The factor 2 is because of the Gromacs virial definition */
1236 spres = -2.0*invvol*svir*PRESFAC;
1238 for(m=0; m<DIM; m++) {
1239 virial[m][m] += svir;
1240 pres[m][m] += spres;
1245 /* Can't currently control when it prints, for now, just print when degugging */
1249 fprintf(debug,"Long Range LJ corr.: <C6> %10.4e, <C12> %10.4e\n",
1255 "Long Range LJ corr.: Epot %10g, Pres: %10g, Vir: %10g\n",
1256 *enercorr,spres,svir);
1260 fprintf(debug,"Long Range LJ corr.: Epot %10g\n",*enercorr);
1264 if (fr->bSepDVDL && do_per_step(step,ir->nstlog))
1266 fprintf(fplog,sepdvdlformat,"Dispersion correction",
1267 *enercorr,dvdlambda);
1269 if (fr->efep != efepNO)
1271 *dvdlcorr += dvdlambda;
1276 void do_pbc_first(FILE *fplog,matrix box,t_forcerec *fr,
1277 t_graph *graph,rvec x[])
1280 fprintf(fplog,"Removing pbc first time\n");
1281 calc_shifts(box,fr->shift_vec);
1283 mk_mshift(fplog,graph,fr->ePBC,box,x);
1285 p_graph(debug,"do_pbc_first 1",graph);
1286 shift_self(graph,box,x);
1287 /* By doing an extra mk_mshift the molecules that are broken
1288 * because they were e.g. imported from another software
1289 * will be made whole again. Such are the healing powers
1292 mk_mshift(fplog,graph,fr->ePBC,box,x);
1294 p_graph(debug,"do_pbc_first 2",graph);
1297 fprintf(fplog,"Done rmpbc\n");
1300 static void low_do_pbc_mtop(FILE *fplog,int ePBC,matrix box,
1301 gmx_mtop_t *mtop,rvec x[],
1306 gmx_molblock_t *molb;
1308 if (bFirst && fplog)
1309 fprintf(fplog,"Removing pbc first time\n");
1313 for(mb=0; mb<mtop->nmolblock; mb++) {
1314 molb = &mtop->molblock[mb];
1315 if (molb->natoms_mol == 1 ||
1316 (!bFirst && mtop->moltype[molb->type].cgs.nr == 1)) {
1317 /* Just one atom or charge group in the molecule, no PBC required */
1318 as += molb->nmol*molb->natoms_mol;
1320 /* Pass NULL iso fplog to avoid graph prints for each molecule type */
1321 mk_graph_ilist(NULL,mtop->moltype[molb->type].ilist,
1322 0,molb->natoms_mol,FALSE,FALSE,graph);
1324 for(mol=0; mol<molb->nmol; mol++) {
1325 mk_mshift(fplog,graph,ePBC,box,x+as);
1327 shift_self(graph,box,x+as);
1328 /* The molecule is whole now.
1329 * We don't need the second mk_mshift call as in do_pbc_first,
1330 * since we no longer need this graph.
1333 as += molb->natoms_mol;
1341 void do_pbc_first_mtop(FILE *fplog,int ePBC,matrix box,
1342 gmx_mtop_t *mtop,rvec x[])
1344 low_do_pbc_mtop(fplog,ePBC,box,mtop,x,TRUE);
1347 void do_pbc_mtop(FILE *fplog,int ePBC,matrix box,
1348 gmx_mtop_t *mtop,rvec x[])
1350 low_do_pbc_mtop(fplog,ePBC,box,mtop,x,FALSE);
1353 void finish_run(FILE *fplog,t_commrec *cr,const char *confout,
1354 t_inputrec *inputrec,
1355 t_nrnb nrnb[],gmx_wallcycle_t wcycle,
1356 gmx_runtime_t *runtime,
1357 gmx_bool bWriteStat)
1360 t_nrnb *nrnb_tot=NULL;
1363 double cycles[ewcNR];
1365 wallcycle_sum(cr,wcycle,cycles);
1367 if (cr->nnodes > 1) {
1371 MPI_Reduce(nrnb->n,nrnb_tot->n,eNRNB,MPI_DOUBLE,MPI_SUM,
1372 MASTERRANK(cr),cr->mpi_comm_mysim);
1378 if (SIMMASTER(cr)) {
1379 print_flop(fplog,nrnb_tot,&nbfs,&mflop);
1380 if (cr->nnodes > 1) {
1385 if ((cr->duty & DUTY_PP) && DOMAINDECOMP(cr)) {
1386 print_dd_statistics(cr,inputrec,fplog);
1398 snew(nrnb_all,cr->nnodes);
1399 nrnb_all[0] = *nrnb;
1400 for(s=1; s<cr->nnodes; s++)
1402 MPI_Recv(nrnb_all[s].n,eNRNB,MPI_DOUBLE,s,0,
1403 cr->mpi_comm_mysim,&stat);
1405 pr_load(fplog,cr,nrnb_all);
1410 MPI_Send(nrnb->n,eNRNB,MPI_DOUBLE,MASTERRANK(cr),0,
1411 cr->mpi_comm_mysim);
1416 if (SIMMASTER(cr)) {
1417 wallcycle_print(fplog,cr->nnodes,cr->npmenodes,runtime->realtime,
1420 if (EI_DYNAMICS(inputrec->eI)) {
1421 delta_t = inputrec->delta_t;
1427 print_perf(fplog,runtime->proctime,runtime->realtime,
1428 cr->nnodes-cr->npmenodes,
1429 runtime->nsteps_done,delta_t,nbfs,mflop);
1432 print_perf(stderr,runtime->proctime,runtime->realtime,
1433 cr->nnodes-cr->npmenodes,
1434 runtime->nsteps_done,delta_t,nbfs,mflop);
1438 runtime=inputrec->nsteps*inputrec->delta_t;
1440 if (cr->nnodes == 1)
1441 fprintf(stderr,"\n\n");
1442 print_perf(stderr,nodetime,realtime,runtime,&ntot,
1443 cr->nnodes-cr->npmenodes,FALSE);
1445 wallcycle_print(fplog,cr->nnodes,cr->npmenodes,realtime,wcycle,cycles);
1446 print_perf(fplog,nodetime,realtime,runtime,&ntot,cr->nnodes-cr->npmenodes,
1449 pr_load(fplog,cr,nrnb_all);
1456 void init_md(FILE *fplog,
1457 t_commrec *cr,t_inputrec *ir,const output_env_t oenv,
1458 double *t,double *t0,
1459 real *lambda,double *lam0,
1460 t_nrnb *nrnb,gmx_mtop_t *mtop,
1462 int nfile,const t_filenm fnm[],
1463 gmx_mdoutf_t **outf,t_mdebin **mdebin,
1464 tensor force_vir,tensor shake_vir,rvec mu_tot,
1465 gmx_bool *bSimAnn,t_vcm **vcm, t_state *state, unsigned long Flags)
1470 /* Initial values */
1471 *t = *t0 = ir->init_t;
1472 if (ir->efep != efepNO)
1474 *lam0 = ir->init_lambda;
1475 *lambda = *lam0 + ir->init_step*ir->delta_lambda;
1479 *lambda = *lam0 = 0.0;
1483 for(i=0;i<ir->opts.ngtc;i++)
1485 /* set bSimAnn if any group is being annealed */
1486 if(ir->opts.annealing[i]!=eannNO)
1493 update_annealing_target_temp(&(ir->opts),ir->init_t);
1498 *upd = init_update(fplog,ir);
1503 *vcm = init_vcm(fplog,&mtop->groups,ir);
1506 if (EI_DYNAMICS(ir->eI) && !(Flags & MD_APPENDFILES))
1508 if (ir->etc == etcBERENDSEN)
1510 please_cite(fplog,"Berendsen84a");
1512 if (ir->etc == etcVRESCALE)
1514 please_cite(fplog,"Bussi2007a");
1522 *outf = init_mdoutf(nfile,fnm,Flags,cr,ir,oenv);
1524 *mdebin = init_mdebin((Flags & MD_APPENDFILES) ? NULL : (*outf)->fp_ene,
1525 mtop,ir, (*outf)->fp_dhdl);
1528 /* Initiate variables */
1529 clear_mat(force_vir);
1530 clear_mat(shake_vir);