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39 #include "gromacs/legacyheaders/force.h"
47 #include "gromacs/domdec/domdec.h"
48 #include "gromacs/ewald/ewald.h"
49 #include "gromacs/ewald/long-range-correction.h"
50 #include "gromacs/ewald/pme.h"
51 #include "gromacs/legacyheaders/gmx_omp_nthreads.h"
52 #include "gromacs/legacyheaders/macros.h"
53 #include "gromacs/legacyheaders/mdrun.h"
54 #include "gromacs/legacyheaders/names.h"
55 #include "gromacs/legacyheaders/network.h"
56 #include "gromacs/legacyheaders/nonbonded.h"
57 #include "gromacs/legacyheaders/nrnb.h"
58 #include "gromacs/legacyheaders/ns.h"
59 #include "gromacs/legacyheaders/qmmm.h"
60 #include "gromacs/legacyheaders/txtdump.h"
61 #include "gromacs/legacyheaders/typedefs.h"
62 #include "gromacs/legacyheaders/types/commrec.h"
63 #include "gromacs/listed-forces/listed-forces.h"
64 #include "gromacs/math/vec.h"
65 #include "gromacs/mdlib/forcerec-threading.h"
66 #include "gromacs/pbcutil/ishift.h"
67 #include "gromacs/pbcutil/mshift.h"
68 #include "gromacs/pbcutil/pbc.h"
69 #include "gromacs/timing/wallcycle.h"
70 #include "gromacs/utility/cstringutil.h"
71 #include "gromacs/utility/fatalerror.h"
72 #include "gromacs/utility/smalloc.h"
83 gmx_bool bDoLongRangeNS)
88 if (!fr->ns.nblist_initialized)
90 init_neighbor_list(fp, fr, md->homenr);
98 nsearch = search_neighbours(fp, fr, box, top, groups, cr, nrnb, md,
99 bFillGrid, bDoLongRangeNS);
102 fprintf(debug, "nsearch = %d\n", nsearch);
105 /* Check whether we have to do dynamic load balancing */
106 /*if ((nsb->nstDlb > 0) && (mod(step,nsb->nstDlb) == 0))
107 count_nb(cr,nsb,&(top->blocks[ebCGS]),nns,fr->nlr,
108 &(top->idef),opts->ngener);
110 if (fr->ns.dump_nl > 0)
112 dump_nblist(fp, cr, fr, fr->ns.dump_nl);
116 static void reduce_thread_energies(tensor vir_q, tensor vir_lj,
117 real *Vcorr_q, real *Vcorr_lj,
118 real *dvdl_q, real *dvdl_lj,
120 ewald_corr_thread_t *ewc_t)
124 for (t = 1; t < nthreads; t++)
126 *Vcorr_q += ewc_t[t].Vcorr_q;
127 *Vcorr_lj += ewc_t[t].Vcorr_lj;
128 *dvdl_q += ewc_t[t].dvdl[efptCOUL];
129 *dvdl_lj += ewc_t[t].dvdl[efptVDW];
130 m_add(vir_q, ewc_t[t].vir_q, vir_q);
131 m_add(vir_lj, ewc_t[t].vir_lj, vir_lj);
135 void do_force_lowlevel(t_forcerec *fr, t_inputrec *ir,
136 t_idef *idef, t_commrec *cr,
137 t_nrnb *nrnb, gmx_wallcycle_t wcycle,
139 rvec x[], history_t *hist,
142 gmx_enerdata_t *enerd,
163 real dvdl_dum[efptNR], dvdl_nb[efptNR];
166 double t0 = 0.0, t1, t2, t3; /* time measurement for coarse load balancing */
169 set_pbc(&pbc, fr->ePBC, box);
171 /* reset free energy components */
172 for (i = 0; i < efptNR; i++)
179 for (i = 0; (i < DIM); i++)
181 box_size[i] = box[i][i];
186 /* do QMMM first if requested */
189 enerd->term[F_EQM] = calculate_QMMM(cr, x, f, fr);
192 /* Call the short range functions all in one go. */
195 /*#define TAKETIME ((cr->npmenodes) && (fr->timesteps < 12))*/
196 #define TAKETIME FALSE
199 MPI_Barrier(cr->mpi_comm_mygroup);
206 /* foreign lambda component for walls */
207 real dvdl_walls = do_walls(ir, fr, box, md, x, f, lambda[efptVDW],
208 enerd->grpp.ener[egLJSR], nrnb);
209 enerd->dvdl_lin[efptVDW] += dvdl_walls;
212 /* If doing GB, reset dvda and calculate the Born radii */
213 if (ir->implicit_solvent)
215 wallcycle_sub_start(wcycle, ewcsNONBONDED);
217 for (i = 0; i < born->nr; i++)
224 calc_gb_rad(cr, fr, ir, top, x, &(fr->gblist), born, md, nrnb);
227 wallcycle_sub_stop(wcycle, ewcsNONBONDED);
231 /* We only do non-bonded calculation with group scheme here, the verlet
232 * calls are done from do_force_cutsVERLET(). */
233 if (fr->cutoff_scheme == ecutsGROUP && (flags & GMX_FORCE_NONBONDED))
236 /* Add short-range interactions */
237 donb_flags |= GMX_NONBONDED_DO_SR;
239 /* Currently all group scheme kernels always calculate (shift-)forces */
240 if (flags & GMX_FORCE_FORCES)
242 donb_flags |= GMX_NONBONDED_DO_FORCE;
244 if (flags & GMX_FORCE_VIRIAL)
246 donb_flags |= GMX_NONBONDED_DO_SHIFTFORCE;
248 if (flags & GMX_FORCE_ENERGY)
250 donb_flags |= GMX_NONBONDED_DO_POTENTIAL;
252 if (flags & GMX_FORCE_DO_LR)
254 donb_flags |= GMX_NONBONDED_DO_LR;
257 wallcycle_sub_start(wcycle, ewcsNONBONDED);
258 do_nonbonded(fr, x, f, f_longrange, md, excl,
260 lambda, dvdl_nb, -1, -1, donb_flags);
262 /* If we do foreign lambda and we have soft-core interactions
263 * we have to recalculate the (non-linear) energies contributions.
265 if (fepvals->n_lambda > 0 && (flags & GMX_FORCE_DHDL) && fepvals->sc_alpha != 0)
267 for (i = 0; i < enerd->n_lambda; i++)
271 for (j = 0; j < efptNR; j++)
273 lam_i[j] = (i == 0 ? lambda[j] : fepvals->all_lambda[j][i-1]);
275 reset_foreign_enerdata(enerd);
276 do_nonbonded(fr, x, f, f_longrange, md, excl,
277 &(enerd->foreign_grpp), nrnb,
278 lam_i, dvdl_dum, -1, -1,
279 (donb_flags & ~GMX_NONBONDED_DO_FORCE) | GMX_NONBONDED_DO_FOREIGNLAMBDA);
280 sum_epot(&(enerd->foreign_grpp), enerd->foreign_term);
281 enerd->enerpart_lambda[i] += enerd->foreign_term[F_EPOT];
284 wallcycle_sub_stop(wcycle, ewcsNONBONDED);
288 /* If we are doing GB, calculate bonded forces and apply corrections
289 * to the solvation forces */
290 /* MRS: Eventually, many need to include free energy contribution here! */
291 if (ir->implicit_solvent)
293 wallcycle_sub_start(wcycle, ewcsLISTED);
294 calc_gb_forces(cr, md, born, top, x, f, fr, idef,
295 ir->gb_algorithm, ir->sa_algorithm, nrnb, &pbc, graph, enerd);
296 wallcycle_sub_stop(wcycle, ewcsLISTED);
307 if (fepvals->sc_alpha != 0)
309 enerd->dvdl_nonlin[efptVDW] += dvdl_nb[efptVDW];
313 enerd->dvdl_lin[efptVDW] += dvdl_nb[efptVDW];
316 if (fepvals->sc_alpha != 0)
318 /* even though coulomb part is linear, we already added it, beacuse we
319 need to go through the vdw calculation anyway */
321 enerd->dvdl_nonlin[efptCOUL] += dvdl_nb[efptCOUL];
325 enerd->dvdl_lin[efptCOUL] += dvdl_nb[efptCOUL];
333 pr_rvecs(debug, 0, "fshift after SR", fr->fshift, SHIFTS);
336 /* Shift the coordinates. Must be done before listed forces and PPPM,
337 * but is also necessary for SHAKE and update, therefore it can NOT
338 * go when no listed forces have to be evaluated.
340 * The shifting and PBC code is deliberately not timed, since with
341 * the Verlet scheme it only takes non-zero time with triclinic
342 * boxes, and even then the time is around a factor of 100 less
343 * than the next smallest counter.
347 /* Here sometimes we would not need to shift with NBFonly,
348 * but we do so anyhow for consistency of the returned coordinates.
352 shift_self(graph, box, x);
355 inc_nrnb(nrnb, eNR_SHIFTX, 2*graph->nnodes);
359 inc_nrnb(nrnb, eNR_SHIFTX, graph->nnodes);
362 /* Check whether we need to do listed interactions or correct for exclusions */
364 ((flags & GMX_FORCE_LISTED)
365 || EEL_RF(fr->eeltype) || EEL_FULL(fr->eeltype) || EVDW_PME(fr->vdwtype)))
367 /* TODO There are no electrostatics methods that require this
368 transformation, when using the Verlet scheme, so update the
369 above conditional. */
370 /* Since all atoms are in the rectangular or triclinic unit-cell,
371 * only single box vector shifts (2 in x) are required.
373 set_pbc_dd(&pbc, fr->ePBC, cr->dd, TRUE, box);
377 do_force_listed(wcycle, box, ir->fepvals, cr->ms,
378 idef, (const rvec *) x, hist, f, fr,
379 &pbc, graph, enerd, nrnb, lambda, md, fcd,
380 DOMAINDECOMP(cr) ? cr->dd->gatindex : NULL,
386 clear_mat(fr->vir_el_recip);
387 clear_mat(fr->vir_lj_recip);
389 /* Do long-range electrostatics and/or LJ-PME, including related short-range
392 if (EEL_FULL(fr->eeltype) || EVDW_PME(fr->vdwtype))
395 real Vlr_q = 0, Vlr_lj = 0, Vcorr_q = 0, Vcorr_lj = 0;
396 real dvdl_long_range_q = 0, dvdl_long_range_lj = 0;
398 bSB = (ir->nwall == 2);
402 svmul(ir->wall_ewald_zfac, boxs[ZZ], boxs[ZZ]);
403 box_size[ZZ] *= ir->wall_ewald_zfac;
406 if (EEL_PME_EWALD(fr->eeltype) || EVDW_PME(fr->vdwtype))
408 real dvdl_long_range_correction_q = 0;
409 real dvdl_long_range_correction_lj = 0;
410 /* With the Verlet scheme exclusion forces are calculated
411 * in the non-bonded kernel.
413 /* The TPI molecule does not have exclusions with the rest
414 * of the system and no intra-molecular PME grid
415 * contributions will be calculated in
416 * gmx_pme_calc_energy.
418 if ((ir->cutoff_scheme == ecutsGROUP && fr->n_tpi == 0) ||
419 ir->ewald_geometry != eewg3D ||
420 ir->epsilon_surface != 0)
424 wallcycle_sub_start(wcycle, ewcsEWALD_CORRECTION);
428 gmx_fatal(FARGS, "TPI with PME currently only works in a 3D geometry with tin-foil boundary conditions");
431 nthreads = fr->nthread_ewc;
432 #pragma omp parallel for num_threads(nthreads) schedule(static)
433 for (t = 0; t < nthreads; t++)
435 tensor *vir_q, *vir_lj;
436 real *Vcorrt_q, *Vcorrt_lj, *dvdlt_q, *dvdlt_lj;
439 vir_q = &fr->vir_el_recip;
440 vir_lj = &fr->vir_lj_recip;
442 Vcorrt_lj = &Vcorr_lj;
443 dvdlt_q = &dvdl_long_range_correction_q;
444 dvdlt_lj = &dvdl_long_range_correction_lj;
448 vir_q = &fr->ewc_t[t].vir_q;
449 vir_lj = &fr->ewc_t[t].vir_lj;
450 Vcorrt_q = &fr->ewc_t[t].Vcorr_q;
451 Vcorrt_lj = &fr->ewc_t[t].Vcorr_lj;
452 dvdlt_q = &fr->ewc_t[t].dvdl[efptCOUL];
453 dvdlt_lj = &fr->ewc_t[t].dvdl[efptVDW];
460 /* Threading is only supported with the Verlet cut-off
461 * scheme and then only single particle forces (no
462 * exclusion forces) are calculated, so we can store
463 * the forces in the normal, single fr->f_novirsum array.
465 ewald_LRcorrection(fr->excl_load[t], fr->excl_load[t+1],
467 md->chargeA, md->chargeB,
468 md->sqrt_c6A, md->sqrt_c6B,
469 md->sigmaA, md->sigmaB,
470 md->sigma3A, md->sigma3B,
471 md->nChargePerturbed || md->nTypePerturbed,
472 ir->cutoff_scheme != ecutsVERLET,
473 excl, x, bSB ? boxs : box, mu_tot,
476 fr->f_novirsum, *vir_q, *vir_lj,
478 lambda[efptCOUL], lambda[efptVDW],
483 reduce_thread_energies(fr->vir_el_recip, fr->vir_lj_recip,
485 &dvdl_long_range_correction_q,
486 &dvdl_long_range_correction_lj,
487 nthreads, fr->ewc_t);
489 wallcycle_sub_stop(wcycle, ewcsEWALD_CORRECTION);
492 if (EEL_PME_EWALD(fr->eeltype) && fr->n_tpi == 0)
494 /* This is not in a subcounter because it takes a
495 negligible and constant-sized amount of time */
496 Vcorr_q += ewald_charge_correction(cr, fr, lambda[efptCOUL], box,
497 &dvdl_long_range_correction_q,
501 enerd->dvdl_lin[efptCOUL] += dvdl_long_range_correction_q;
502 enerd->dvdl_lin[efptVDW] += dvdl_long_range_correction_lj;
504 if ((EEL_PME(fr->eeltype) || EVDW_PME(fr->vdwtype)) && (cr->duty & DUTY_PME))
506 /* Do reciprocal PME for Coulomb and/or LJ. */
507 assert(fr->n_tpi >= 0);
508 if (fr->n_tpi == 0 || (flags & GMX_FORCE_STATECHANGED))
510 pme_flags = GMX_PME_SPREAD | GMX_PME_SOLVE;
511 if (EEL_PME(fr->eeltype))
513 pme_flags |= GMX_PME_DO_COULOMB;
515 if (EVDW_PME(fr->vdwtype))
517 pme_flags |= GMX_PME_DO_LJ;
519 if (flags & GMX_FORCE_FORCES)
521 pme_flags |= GMX_PME_CALC_F;
523 if (flags & GMX_FORCE_VIRIAL)
525 pme_flags |= GMX_PME_CALC_ENER_VIR;
529 /* We don't calculate f, but we do want the potential */
530 pme_flags |= GMX_PME_CALC_POT;
532 wallcycle_start(wcycle, ewcPMEMESH);
533 status = gmx_pme_do(fr->pmedata,
534 0, md->homenr - fr->n_tpi,
536 md->chargeA, md->chargeB,
537 md->sqrt_c6A, md->sqrt_c6B,
538 md->sigmaA, md->sigmaB,
539 bSB ? boxs : box, cr,
540 DOMAINDECOMP(cr) ? dd_pme_maxshift_x(cr->dd) : 0,
541 DOMAINDECOMP(cr) ? dd_pme_maxshift_y(cr->dd) : 0,
543 fr->vir_el_recip, fr->ewaldcoeff_q,
544 fr->vir_lj_recip, fr->ewaldcoeff_lj,
546 lambda[efptCOUL], lambda[efptVDW],
547 &dvdl_long_range_q, &dvdl_long_range_lj, pme_flags);
548 *cycles_pme = wallcycle_stop(wcycle, ewcPMEMESH);
551 gmx_fatal(FARGS, "Error %d in reciprocal PME routine", status);
553 /* We should try to do as little computation after
554 * this as possible, because parallel PME synchronizes
555 * the nodes, so we want all load imbalance of the
556 * rest of the force calculation to be before the PME
557 * call. DD load balancing is done on the whole time
558 * of the force call (without PME).
563 if (EVDW_PME(ir->vdwtype))
566 gmx_fatal(FARGS, "Test particle insertion not implemented with LJ-PME");
568 /* Determine the PME grid energy of the test molecule
569 * with the PME grid potential of the other charges.
571 gmx_pme_calc_energy(fr->pmedata, fr->n_tpi,
572 x + md->homenr - fr->n_tpi,
573 md->chargeA + md->homenr - fr->n_tpi,
579 if (!EEL_PME(fr->eeltype) && EEL_PME_EWALD(fr->eeltype))
581 Vlr_q = do_ewald(ir, x, fr->f_novirsum,
582 md->chargeA, md->chargeB,
583 box_size, cr, md->homenr,
584 fr->vir_el_recip, fr->ewaldcoeff_q,
585 lambda[efptCOUL], &dvdl_long_range_q, fr->ewald_table);
588 /* Note that with separate PME nodes we get the real energies later */
589 enerd->dvdl_lin[efptCOUL] += dvdl_long_range_q;
590 enerd->dvdl_lin[efptVDW] += dvdl_long_range_lj;
591 enerd->term[F_COUL_RECIP] = Vlr_q + Vcorr_q;
592 enerd->term[F_LJ_RECIP] = Vlr_lj + Vcorr_lj;
595 fprintf(debug, "Vlr_q = %g, Vcorr_q = %g, Vlr_corr_q = %g\n",
596 Vlr_q, Vcorr_q, enerd->term[F_COUL_RECIP]);
597 pr_rvecs(debug, 0, "vir_el_recip after corr", fr->vir_el_recip, DIM);
598 pr_rvecs(debug, 0, "fshift after LR Corrections", fr->fshift, SHIFTS);
599 fprintf(debug, "Vlr_lj: %g, Vcorr_lj = %g, Vlr_corr_lj = %g\n",
600 Vlr_lj, Vcorr_lj, enerd->term[F_LJ_RECIP]);
601 pr_rvecs(debug, 0, "vir_lj_recip after corr", fr->vir_lj_recip, DIM);
606 /* Is there a reaction-field exclusion correction needed? */
607 if (EEL_RF(fr->eeltype) && eelRF_NEC != fr->eeltype)
609 /* With the Verlet scheme, exclusion forces are calculated
610 * in the non-bonded kernel.
612 if (ir->cutoff_scheme != ecutsVERLET)
614 real dvdl_rf_excl = 0;
615 enerd->term[F_RF_EXCL] =
616 RF_excl_correction(fr, graph, md, excl, x, f,
617 fr->fshift, &pbc, lambda[efptCOUL], &dvdl_rf_excl);
619 enerd->dvdl_lin[efptCOUL] += dvdl_rf_excl;
628 print_nrnb(debug, nrnb);
636 MPI_Barrier(cr->mpi_comm_mygroup);
639 if (fr->timesteps == 11)
642 fprintf(stderr, "* PP load balancing info: rank %d, step %s, rel wait time=%3.0f%% , load string value: %7.2f\n",
643 cr->nodeid, gmx_step_str(fr->timesteps, buf),
644 100*fr->t_wait/(fr->t_wait+fr->t_fnbf),
645 (fr->t_fnbf+fr->t_wait)/fr->t_fnbf);
653 pr_rvecs(debug, 0, "fshift after bondeds", fr->fshift, SHIFTS);
658 void init_enerdata(int ngener, int n_lambda, gmx_enerdata_t *enerd)
662 for (i = 0; i < F_NRE; i++)
665 enerd->foreign_term[i] = 0;
669 for (i = 0; i < efptNR; i++)
671 enerd->dvdl_lin[i] = 0;
672 enerd->dvdl_nonlin[i] = 0;
678 fprintf(debug, "Creating %d sized group matrix for energies\n", n2);
680 enerd->grpp.nener = n2;
681 enerd->foreign_grpp.nener = n2;
682 for (i = 0; (i < egNR); i++)
684 snew(enerd->grpp.ener[i], n2);
685 snew(enerd->foreign_grpp.ener[i], n2);
690 enerd->n_lambda = 1 + n_lambda;
691 snew(enerd->enerpart_lambda, enerd->n_lambda);
699 void destroy_enerdata(gmx_enerdata_t *enerd)
703 for (i = 0; (i < egNR); i++)
705 sfree(enerd->grpp.ener[i]);
708 for (i = 0; (i < egNR); i++)
710 sfree(enerd->foreign_grpp.ener[i]);
715 sfree(enerd->enerpart_lambda);
719 static real sum_v(int n, real v[])
725 for (i = 0; (i < n); i++)
733 void sum_epot(gmx_grppairener_t *grpp, real *epot)
737 /* Accumulate energies */
738 epot[F_COUL_SR] = sum_v(grpp->nener, grpp->ener[egCOULSR]);
739 epot[F_LJ] = sum_v(grpp->nener, grpp->ener[egLJSR]);
740 epot[F_LJ14] = sum_v(grpp->nener, grpp->ener[egLJ14]);
741 epot[F_COUL14] = sum_v(grpp->nener, grpp->ener[egCOUL14]);
742 epot[F_COUL_LR] = sum_v(grpp->nener, grpp->ener[egCOULLR]);
743 epot[F_LJ_LR] = sum_v(grpp->nener, grpp->ener[egLJLR]);
744 /* We have already added 1-2,1-3, and 1-4 terms to F_GBPOL */
745 epot[F_GBPOL] += sum_v(grpp->nener, grpp->ener[egGB]);
747 /* lattice part of LR doesnt belong to any group
748 * and has been added earlier
750 epot[F_BHAM] = sum_v(grpp->nener, grpp->ener[egBHAMSR]);
751 epot[F_BHAM_LR] = sum_v(grpp->nener, grpp->ener[egBHAMLR]);
754 for (i = 0; (i < F_EPOT); i++)
756 if (i != F_DISRESVIOL && i != F_ORIRESDEV)
758 epot[F_EPOT] += epot[i];
763 void sum_dhdl(gmx_enerdata_t *enerd, real *lambda, t_lambda *fepvals)
768 enerd->dvdl_lin[efptVDW] += enerd->term[F_DVDL_VDW]; /* include dispersion correction */
769 enerd->term[F_DVDL] = 0.0;
770 for (i = 0; i < efptNR; i++)
772 if (fepvals->separate_dvdl[i])
774 /* could this be done more readably/compactly? */
787 index = F_DVDL_BONDED;
789 case (efptRESTRAINT):
790 index = F_DVDL_RESTRAINT;
796 enerd->term[index] = enerd->dvdl_lin[i] + enerd->dvdl_nonlin[i];
799 fprintf(debug, "dvdl-%s[%2d]: %f: non-linear %f + linear %f\n",
800 efpt_names[i], i, enerd->term[index], enerd->dvdl_nonlin[i], enerd->dvdl_lin[i]);
805 enerd->term[F_DVDL] += enerd->dvdl_lin[i] + enerd->dvdl_nonlin[i];
808 fprintf(debug, "dvd-%sl[%2d]: %f: non-linear %f + linear %f\n",
809 efpt_names[0], i, enerd->term[F_DVDL], enerd->dvdl_nonlin[i], enerd->dvdl_lin[i]);
814 /* Notes on the foreign lambda free energy difference evaluation:
815 * Adding the potential and ekin terms that depend linearly on lambda
816 * as delta lam * dvdl to the energy differences is exact.
817 * For the constraints this is not exact, but we have no other option
818 * without literally changing the lengths and reevaluating the energies at each step.
819 * (try to remedy this post 4.6 - MRS)
820 * For the non-bonded LR term we assume that the soft-core (if present)
821 * no longer affects the energy beyond the short-range cut-off,
822 * which is a very good approximation (except for exotic settings).
823 * (investigate how to overcome this post 4.6 - MRS)
825 if (fepvals->separate_dvdl[efptBONDED])
827 enerd->term[F_DVDL_BONDED] += enerd->term[F_DVDL_CONSTR];
831 enerd->term[F_DVDL] += enerd->term[F_DVDL_CONSTR];
833 enerd->term[F_DVDL_CONSTR] = 0;
835 for (i = 0; i < fepvals->n_lambda; i++)
837 /* note we are iterating over fepvals here!
838 For the current lam, dlam = 0 automatically,
839 so we don't need to add anything to the
840 enerd->enerpart_lambda[0] */
842 /* we don't need to worry about dvdl_lin contributions to dE at
843 current lambda, because the contributions to the current
844 lambda are automatically zeroed */
846 for (j = 0; j < efptNR; j++)
848 /* Note that this loop is over all dhdl components, not just the separated ones */
849 dlam = (fepvals->all_lambda[j][i]-lambda[j]);
850 enerd->enerpart_lambda[i+1] += dlam*enerd->dvdl_lin[j];
853 fprintf(debug, "enerdiff lam %g: (%15s), non-linear %f linear %f*%f\n",
854 fepvals->all_lambda[j][i], efpt_names[j],
855 (enerd->enerpart_lambda[i+1] - enerd->enerpart_lambda[0]),
856 dlam, enerd->dvdl_lin[j]);
863 void reset_foreign_enerdata(gmx_enerdata_t *enerd)
867 /* First reset all foreign energy components. Foreign energies always called on
868 neighbor search steps */
869 for (i = 0; (i < egNR); i++)
871 for (j = 0; (j < enerd->grpp.nener); j++)
873 enerd->foreign_grpp.ener[i][j] = 0.0;
877 /* potential energy components */
878 for (i = 0; (i <= F_EPOT); i++)
880 enerd->foreign_term[i] = 0.0;
884 void reset_enerdata(t_forcerec *fr, gmx_bool bNS,
885 gmx_enerdata_t *enerd,
891 /* First reset all energy components, except for the long range terms
892 * on the master at non neighbor search steps, since the long range
893 * terms have already been summed at the last neighbor search step.
895 bKeepLR = (fr->bTwinRange && !bNS);
896 for (i = 0; (i < egNR); i++)
898 if (!(bKeepLR && bMaster && (i == egCOULLR || i == egLJLR)))
900 for (j = 0; (j < enerd->grpp.nener); j++)
902 enerd->grpp.ener[i][j] = 0.0;
906 for (i = 0; i < efptNR; i++)
908 enerd->dvdl_lin[i] = 0.0;
909 enerd->dvdl_nonlin[i] = 0.0;
912 /* Normal potential energy components */
913 for (i = 0; (i <= F_EPOT); i++)
915 enerd->term[i] = 0.0;
917 /* Initialize the dVdlambda term with the long range contribution */
918 /* Initialize the dvdl term with the long range contribution */
919 enerd->term[F_DVDL] = 0.0;
920 enerd->term[F_DVDL_COUL] = 0.0;
921 enerd->term[F_DVDL_VDW] = 0.0;
922 enerd->term[F_DVDL_BONDED] = 0.0;
923 enerd->term[F_DVDL_RESTRAINT] = 0.0;
924 enerd->term[F_DKDL] = 0.0;
925 if (enerd->n_lambda > 0)
927 for (i = 0; i < enerd->n_lambda; i++)
929 enerd->enerpart_lambda[i] = 0.0;
932 /* reset foreign energy data - separate function since we also call it elsewhere */
933 reset_foreign_enerdata(enerd);