Fixed typos in GB inner dielectric commit for some kernels.
[gromacs.git] / src / mdlib / forcerec.c
blobb8775b9efac9ee43a0e1a26c53f4259bd1dc4029
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36 #ifdef HAVE_CONFIG_H
37 #include <config.h>
38 #endif
40 #include <math.h>
41 #include <string.h>
42 #include "sysstuff.h"
43 #include "typedefs.h"
44 #include "macros.h"
45 #include "smalloc.h"
46 #include "macros.h"
47 #include "physics.h"
48 #include "force.h"
49 #include "nonbonded.h"
50 #include "invblock.h"
51 #include "names.h"
52 #include "network.h"
53 #include "pbc.h"
54 #include "ns.h"
55 #include "mshift.h"
56 #include "txtdump.h"
57 #include "coulomb.h"
58 #include "mdrun.h"
59 #include "domdec.h"
60 #include "partdec.h"
61 #include "qmmm.h"
62 #include "copyrite.h"
63 #include "mtop_util.h"
65 t_forcerec *mk_forcerec(void)
67 t_forcerec *fr;
69 snew(fr,1);
71 return fr;
74 #ifdef DEBUG
75 static void pr_nbfp(FILE *fp,real *nbfp,bool bBHAM,int atnr)
77 int i,j;
79 for(i=0; (i<atnr); i++) {
80 for(j=0; (j<atnr); j++) {
81 fprintf(fp,"%2d - %2d",i,j);
82 if (bBHAM)
83 fprintf(fp," a=%10g, b=%10g, c=%10g\n",BHAMA(nbfp,atnr,i,j),
84 BHAMB(nbfp,atnr,i,j),BHAMC(nbfp,atnr,i,j));
85 else
86 fprintf(fp," c6=%10g, c12=%10g\n",C6(nbfp,atnr,i,j),
87 C12(nbfp,atnr,i,j));
91 #endif
93 static real *mk_nbfp(const gmx_ffparams_t *idef,bool bBHAM)
95 real *nbfp;
96 int i,j,k,atnr;
98 atnr=idef->atnr;
99 if (bBHAM) {
100 snew(nbfp,3*atnr*atnr);
101 for(i=k=0; (i<atnr); i++) {
102 for(j=0; (j<atnr); j++,k++) {
103 BHAMA(nbfp,atnr,i,j) = idef->iparams[k].bham.a;
104 BHAMB(nbfp,atnr,i,j) = idef->iparams[k].bham.b;
105 BHAMC(nbfp,atnr,i,j) = idef->iparams[k].bham.c;
109 else {
110 snew(nbfp,2*atnr*atnr);
111 for(i=k=0; (i<atnr); i++) {
112 for(j=0; (j<atnr); j++,k++) {
113 C6(nbfp,atnr,i,j) = idef->iparams[k].lj.c6;
114 C12(nbfp,atnr,i,j) = idef->iparams[k].lj.c12;
118 return nbfp;
121 /* This routine sets fr->solvent_opt to the most common solvent in the
122 * system, e.g. esolSPC or esolTIP4P. It will also mark each charge group in
123 * the fr->solvent_type array with the correct type (or esolNO).
125 * Charge groups that fulfill the conditions but are not identical to the
126 * most common one will be marked as esolNO in the solvent_type array.
128 * TIP3p is identical to SPC for these purposes, so we call it
129 * SPC in the arrays (Apologies to Bill Jorgensen ;-)
131 * NOTE: QM particle should not
132 * become an optimized solvent. Not even if there is only one charge
133 * group in the Qm
136 typedef struct
138 int model;
139 int count;
140 int vdwtype[4];
141 real charge[4];
142 } solvent_parameters_t;
144 static void
145 check_solvent_cg(const gmx_moltype_t *molt,
146 int cg0,
147 int nmol,
148 const unsigned char *qm_grpnr,
149 const t_grps *qm_grps,
150 t_forcerec * fr,
151 int *n_solvent_parameters,
152 solvent_parameters_t **solvent_parameters_p,
153 int cginfo,
154 int *cg_sp)
156 const t_blocka * excl;
157 t_atom *atom;
158 int j,k;
159 int j0,j1,nj;
160 bool perturbed;
161 bool has_vdw[4];
162 bool match;
163 real tmp_charge[4];
164 int tmp_vdwtype[4];
165 int tjA;
166 bool qm;
167 solvent_parameters_t *solvent_parameters;
169 /* We use a list with parameters for each solvent type.
170 * Every time we discover a new molecule that fulfills the basic
171 * conditions for a solvent we compare with the previous entries
172 * in these lists. If the parameters are the same we just increment
173 * the counter for that type, and otherwise we create a new type
174 * based on the current molecule.
176 * Once we've finished going through all molecules we check which
177 * solvent is most common, and mark all those molecules while we
178 * clear the flag on all others.
181 solvent_parameters = *solvent_parameters_p;
183 /* Mark the cg first as non optimized */
184 *cg_sp = -1;
186 /* Check if this cg has no exclusions with atoms in other charge groups
187 * and all atoms inside the charge group excluded.
188 * We only have 3 or 4 atom solvent loops.
190 if (GET_CGINFO_EXCL_INTER(cginfo) ||
191 !GET_CGINFO_EXCL_INTRA(cginfo))
193 return;
196 /* Get the indices of the first atom in this charge group */
197 j0 = molt->cgs.index[cg0];
198 j1 = molt->cgs.index[cg0+1];
200 /* Number of atoms in our molecule */
201 nj = j1 - j0;
203 if (debug) {
204 fprintf(debug,
205 "Moltype '%s': there are %d atoms in this charge group\n",
206 *molt->name,nj);
209 /* Check if it could be an SPC (3 atoms) or TIP4p (4) water,
210 * otherwise skip it.
212 if (nj<3 || nj>4)
214 return;
217 /* Check if we are doing QM on this group */
218 qm = FALSE;
219 if (qm_grpnr != NULL)
221 for(j=j0 ; j<j1 && !qm; j++)
223 qm = (qm_grpnr[j] < qm_grps->nr - 1);
226 /* Cannot use solvent optimization with QM */
227 if (qm)
229 return;
232 atom = molt->atoms.atom;
234 /* Still looks like a solvent, time to check parameters */
236 /* If it is perturbed (free energy) we can't use the solvent loops,
237 * so then we just skip to the next molecule.
239 perturbed = FALSE;
241 for(j=j0; j<j1 && !perturbed; j++)
243 perturbed = PERTURBED(atom[j]);
246 if (perturbed)
248 return;
251 /* Now it's only a question if the VdW and charge parameters
252 * are OK. Before doing the check we compare and see if they are
253 * identical to a possible previous solvent type.
254 * First we assign the current types and charges.
256 for(j=0; j<nj; j++)
258 tmp_vdwtype[j] = atom[j0+j].type;
259 tmp_charge[j] = atom[j0+j].q;
262 /* Does it match any previous solvent type? */
263 for(k=0 ; k<*n_solvent_parameters; k++)
265 match = TRUE;
268 /* We can only match SPC with 3 atoms and TIP4p with 4 atoms */
269 if( (solvent_parameters[k].model==esolSPC && nj!=3) ||
270 (solvent_parameters[k].model==esolTIP4P && nj!=4) )
271 match = FALSE;
273 /* Check that types & charges match for all atoms in molecule */
274 for(j=0 ; j<nj && match==TRUE; j++)
276 if (tmp_vdwtype[j] != solvent_parameters[k].vdwtype[j])
278 match = FALSE;
280 if(tmp_charge[j] != solvent_parameters[k].charge[j])
282 match = FALSE;
285 if (match == TRUE)
287 /* Congratulations! We have a matched solvent.
288 * Flag it with this type for later processing.
290 *cg_sp = k;
291 solvent_parameters[k].count += nmol;
293 /* We are done with this charge group */
294 return;
298 /* If we get here, we have a tentative new solvent type.
299 * Before we add it we must check that it fulfills the requirements
300 * of the solvent optimized loops. First determine which atoms have
301 * VdW interactions.
303 for(j=0; j<nj; j++)
305 has_vdw[j] = FALSE;
306 tjA = tmp_vdwtype[j];
308 /* Go through all other tpes and see if any have non-zero
309 * VdW parameters when combined with this one.
311 for(k=0; k<fr->ntype && (has_vdw[j]==FALSE); k++)
313 /* We already checked that the atoms weren't perturbed,
314 * so we only need to check state A now.
316 if (fr->bBHAM)
318 has_vdw[j] = (has_vdw[j] ||
319 (BHAMA(fr->nbfp,fr->ntype,tjA,k) != 0.0) ||
320 (BHAMB(fr->nbfp,fr->ntype,tjA,k) != 0.0) ||
321 (BHAMC(fr->nbfp,fr->ntype,tjA,k) != 0.0));
323 else
325 /* Standard LJ */
326 has_vdw[j] = (has_vdw[j] ||
327 (C6(fr->nbfp,fr->ntype,tjA,k) != 0.0) ||
328 (C12(fr->nbfp,fr->ntype,tjA,k) != 0.0));
333 /* Now we know all we need to make the final check and assignment. */
334 if (nj == 3)
336 /* So, is it an SPC?
337 * For this we require thatn all atoms have charge,
338 * the charges on atom 2 & 3 should be the same, and only
339 * atom 1 should have VdW.
341 if (has_vdw[0] == TRUE &&
342 has_vdw[1] == FALSE &&
343 has_vdw[2] == FALSE &&
344 tmp_charge[0] != 0 &&
345 tmp_charge[1] != 0 &&
346 tmp_charge[2] == tmp_charge[1])
348 srenew(solvent_parameters,*n_solvent_parameters+1);
349 solvent_parameters[*n_solvent_parameters].model = esolSPC;
350 solvent_parameters[*n_solvent_parameters].count = nmol;
351 for(k=0;k<3;k++)
353 solvent_parameters[*n_solvent_parameters].vdwtype[k] = tmp_vdwtype[k];
354 solvent_parameters[*n_solvent_parameters].charge[k] = tmp_charge[k];
357 *cg_sp = *n_solvent_parameters;
358 (*n_solvent_parameters)++;
361 else if (nj==4)
363 /* Or could it be a TIP4P?
364 * For this we require thatn atoms 2,3,4 have charge, but not atom 1.
365 * Only atom 1 should have VdW.
367 if(has_vdw[0] == TRUE &&
368 has_vdw[1] == FALSE &&
369 has_vdw[2] == FALSE &&
370 has_vdw[3] == FALSE &&
371 tmp_charge[0] == 0 &&
372 tmp_charge[1] != 0 &&
373 tmp_charge[2] == tmp_charge[1] &&
374 tmp_charge[3] != 0)
376 srenew(solvent_parameters,*n_solvent_parameters+1);
377 solvent_parameters[*n_solvent_parameters].model = esolTIP4P;
378 solvent_parameters[*n_solvent_parameters].count = nmol;
379 for(k=0;k<4;k++)
381 solvent_parameters[*n_solvent_parameters].vdwtype[k] = tmp_vdwtype[k];
382 solvent_parameters[*n_solvent_parameters].charge[k] = tmp_charge[k];
385 *cg_sp = *n_solvent_parameters;
386 (*n_solvent_parameters)++;
390 *solvent_parameters_p = solvent_parameters;
393 static void
394 check_solvent(FILE * fp,
395 const gmx_mtop_t * mtop,
396 t_forcerec * fr,
397 cginfo_mb_t *cginfo_mb)
399 const t_block * cgs;
400 const t_block * mols;
401 const gmx_moltype_t *molt;
402 int mb,mol,cg_mol,at_offset,cg_offset,am,cgm,i,nmol_ch,nmol;
403 int n_solvent_parameters;
404 solvent_parameters_t *solvent_parameters;
405 int **cg_sp;
406 int bestsp,bestsol;
408 if (debug)
410 fprintf(debug,"Going to determine what solvent types we have.\n");
413 mols = &mtop->mols;
415 n_solvent_parameters = 0;
416 solvent_parameters = NULL;
417 /* Allocate temporary array for solvent type */
418 snew(cg_sp,mtop->nmolblock);
420 cg_offset = 0;
421 at_offset = 0;
422 for(mb=0; mb<mtop->nmolblock; mb++)
424 molt = &mtop->moltype[mtop->molblock[mb].type];
425 cgs = &molt->cgs;
426 /* Here we have to loop over all individual molecules
427 * because we need to check for QMMM particles.
429 snew(cg_sp[mb],cginfo_mb[mb].cg_mod);
430 nmol_ch = cginfo_mb[mb].cg_mod/cgs->nr;
431 nmol = mtop->molblock[mb].nmol/nmol_ch;
432 for(mol=0; mol<nmol_ch; mol++)
434 cgm = mol*cgs->nr;
435 am = mol*cgs->index[cgs->nr];
436 for(cg_mol=0; cg_mol<cgs->nr; cg_mol++)
438 check_solvent_cg(molt,cg_mol,nmol,
439 mtop->groups.grpnr[egcQMMM] ?
440 mtop->groups.grpnr[egcQMMM]+at_offset+am : 0,
441 &mtop->groups.grps[egcQMMM],
443 &n_solvent_parameters,&solvent_parameters,
444 cginfo_mb[mb].cginfo[cgm+cg_mol],
445 &cg_sp[mb][cgm+cg_mol]);
448 cg_offset += cgs->nr;
449 at_offset += cgs->index[cgs->nr];
452 /* Puh! We finished going through all charge groups.
453 * Now find the most common solvent model.
456 /* Most common solvent this far */
457 bestsp = -2;
458 for(i=0;i<n_solvent_parameters;i++)
460 if (bestsp == -2 ||
461 solvent_parameters[i].count > solvent_parameters[bestsp].count)
463 bestsp = i;
467 if (bestsp >= 0)
469 bestsol = solvent_parameters[bestsp].model;
471 else
473 bestsol = esolNO;
476 #ifdef DISABLE_WATER_NLIST
477 bestsol = esolNO;
478 #endif
480 fr->nWatMol = 0;
481 for(mb=0; mb<mtop->nmolblock; mb++)
483 cgs = &mtop->moltype[mtop->molblock[mb].type].cgs;
484 nmol = (mtop->molblock[mb].nmol*cgs->nr)/cginfo_mb[mb].cg_mod;
485 for(i=0; i<cginfo_mb[mb].cg_mod; i++)
487 if (cg_sp[mb][i] == bestsp)
489 SET_CGINFO_SOLOPT(cginfo_mb[mb].cginfo[i],bestsol);
490 fr->nWatMol += nmol;
492 else
494 SET_CGINFO_SOLOPT(cginfo_mb[mb].cginfo[i],esolNO);
497 sfree(cg_sp[mb]);
499 sfree(cg_sp);
501 if (bestsol != esolNO && fp!=NULL)
503 fprintf(fp,"\nEnabling %s-like water optimization for %d molecules.\n\n",
504 esol_names[bestsol],
505 solvent_parameters[bestsp].count);
508 sfree(solvent_parameters);
509 fr->solvent_opt = bestsol;
512 static cginfo_mb_t *init_cginfo_mb(FILE *fplog,const gmx_mtop_t *mtop,
513 t_forcerec *fr,bool bNoSolvOpt)
515 const t_block *cgs;
516 const t_blocka *excl;
517 const gmx_moltype_t *molt;
518 const gmx_molblock_t *molb;
519 cginfo_mb_t *cginfo_mb;
520 int *cginfo;
521 int cg_offset,a_offset,cgm,am;
522 int mb,m,ncg_tot,cg,a0,a1,gid,ai,j,aj,excl_nalloc;
523 bool bId,*bExcl,bExclIntraAll,bExclInter;
525 ncg_tot = ncg_mtop(mtop);
526 snew(cginfo_mb,mtop->nmolblock);
528 excl_nalloc = 10;
529 snew(bExcl,excl_nalloc);
530 cg_offset = 0;
531 a_offset = 0;
532 for(mb=0; mb<mtop->nmolblock; mb++)
534 molb = &mtop->molblock[mb];
535 molt = &mtop->moltype[molb->type];
536 cgs = &molt->cgs;
537 excl = &molt->excls;
539 /* Check if the cginfo is identical for all molecules in this block.
540 * If so, we only need an array of the size of one molecule.
541 * Otherwise we make an array of #mol times #cgs per molecule.
543 bId = TRUE;
544 am = 0;
545 for(m=0; m<molb->nmol; m++)
547 am = m*cgs->index[cgs->nr];
548 for(cg=0; cg<cgs->nr; cg++)
550 a0 = cgs->index[cg];
551 a1 = cgs->index[cg+1];
552 if (ggrpnr(&mtop->groups,egcENER,a_offset+am+a0) !=
553 ggrpnr(&mtop->groups,egcENER,a_offset +a0))
555 bId = FALSE;
557 if (mtop->groups.grpnr[egcQMMM] != NULL)
559 for(ai=a0; ai<a1; ai++)
561 if (mtop->groups.grpnr[egcQMMM][a_offset+am+ai] !=
562 mtop->groups.grpnr[egcQMMM][a_offset +ai])
564 bId = FALSE;
571 cginfo_mb[mb].cg_start = cg_offset;
572 cginfo_mb[mb].cg_end = cg_offset + molb->nmol*cgs->nr;
573 cginfo_mb[mb].cg_mod = (bId ? 1 : molb->nmol)*cgs->nr;
574 snew(cginfo_mb[mb].cginfo,cginfo_mb[mb].cg_mod);
575 cginfo = cginfo_mb[mb].cginfo;
577 for(m=0; m<(bId ? 1 : molb->nmol); m++)
579 cgm = m*cgs->nr;
580 am = m*cgs->index[cgs->nr];
581 for(cg=0; cg<cgs->nr; cg++)
583 a0 = cgs->index[cg];
584 a1 = cgs->index[cg+1];
586 /* Store the energy group in cginfo */
587 gid = ggrpnr(&mtop->groups,egcENER,a_offset+am+a0);
588 SET_CGINFO_GID(cginfo[cgm+cg],gid);
590 /* Check the intra/inter charge group exclusions */
591 if (a1-a0 > excl_nalloc) {
592 excl_nalloc = a1 - a0;
593 srenew(bExcl,excl_nalloc);
595 /* bExclIntraAll: all intra cg interactions excluded
596 * bExclInter: any inter cg interactions excluded
598 bExclIntraAll = TRUE;
599 bExclInter = FALSE;
600 for(ai=a0; ai<a1; ai++) {
601 /* Clear the exclusion list for atom ai */
602 for(aj=a0; aj<a1; aj++) {
603 bExcl[aj-a0] = FALSE;
605 /* Loop over all the exclusions of atom ai */
606 for(j=excl->index[ai]; j<excl->index[ai+1]; j++)
608 aj = excl->a[j];
609 if (aj < a0 || aj >= a1)
611 bExclInter = TRUE;
613 else
615 bExcl[aj-a0] = TRUE;
618 /* Check if ai excludes a0 to a1 */
619 for(aj=a0; aj<a1; aj++)
621 if (!bExcl[aj-a0])
623 bExclIntraAll = FALSE;
627 if (bExclIntraAll)
629 SET_CGINFO_EXCL_INTRA(cginfo[cgm+cg]);
631 if (bExclInter)
633 SET_CGINFO_EXCL_INTER(cginfo[cgm+cg]);
635 if (a1 - a0 > MAX_CHARGEGROUP_SIZE)
637 /* The size in cginfo is currently only read with DD */
638 gmx_fatal(FARGS,"A charge group has size %d which is larger than the limit of %d atoms",a1-a0,MAX_CHARGEGROUP_SIZE);
640 SET_CGINFO_NATOMS(cginfo[cgm+cg],a1-a0);
643 cg_offset += molb->nmol*cgs->nr;
644 a_offset += molb->nmol*cgs->index[cgs->nr];
646 sfree(bExcl);
648 /* the solvent optimizer is called after the QM is initialized,
649 * because we don't want to have the QM subsystemto become an
650 * optimized solvent
653 check_solvent(fplog,mtop,fr,cginfo_mb);
655 if (getenv("GMX_NO_SOLV_OPT"))
657 if (fplog)
659 fprintf(fplog,"Found environment variable GMX_NO_SOLV_OPT.\n"
660 "Disabling all solvent optimization\n");
662 fr->solvent_opt = esolNO;
664 if (bNoSolvOpt)
666 fr->solvent_opt = esolNO;
668 if (!fr->solvent_opt)
670 for(mb=0; mb<mtop->nmolblock; mb++)
672 for(cg=0; cg<cginfo_mb[mb].cg_mod; cg++)
674 SET_CGINFO_SOLOPT(cginfo_mb[mb].cginfo[cg],esolNO);
679 return cginfo_mb;
682 static int *cginfo_expand(int nmb,cginfo_mb_t *cgi_mb)
684 int ncg,mb,cg;
685 int *cginfo;
687 ncg = cgi_mb[nmb-1].cg_end;
688 snew(cginfo,ncg);
689 mb = 0;
690 for(cg=0; cg<ncg; cg++)
692 while (cg >= cgi_mb[mb].cg_end)
694 mb++;
696 cginfo[cg] =
697 cgi_mb[mb].cginfo[(cg - cgi_mb[mb].cg_start) % cgi_mb[mb].cg_mod];
700 return cginfo;
703 static void set_chargesum(FILE *log,t_forcerec *fr,const gmx_mtop_t *mtop)
705 double qsum;
706 int mb,nmol,i;
707 const t_atoms *atoms;
709 qsum = 0;
710 for(mb=0; mb<mtop->nmolblock; mb++)
712 nmol = mtop->molblock[mb].nmol;
713 atoms = &mtop->moltype[mtop->molblock[mb].type].atoms;
714 for(i=0; i<atoms->nr; i++)
716 qsum += nmol*atoms->atom[i].q;
719 fr->qsum[0] = qsum;
720 if (fr->efep != efepNO)
722 qsum = 0;
723 for(mb=0; mb<mtop->nmolblock; mb++)
725 nmol = mtop->molblock[mb].nmol;
726 atoms = &mtop->moltype[mtop->molblock[mb].type].atoms;
727 for(i=0; i<atoms->nr; i++)
729 qsum += nmol*atoms->atom[i].qB;
731 fr->qsum[1] = qsum;
734 else
736 fr->qsum[1] = fr->qsum[0];
738 if (log) {
739 if (fr->efep == efepNO)
740 fprintf(log,"System total charge: %.3f\n",fr->qsum[0]);
741 else
742 fprintf(log,"System total charge, top. A: %.3f top. B: %.3f\n",
743 fr->qsum[0],fr->qsum[1]);
747 void update_forcerec(FILE *log,t_forcerec *fr,matrix box)
749 if (fr->eeltype == eelGRF)
751 calc_rffac(NULL,fr->eeltype,fr->epsilon_r,fr->epsilon_rf,
752 fr->rcoulomb,fr->temp,fr->zsquare,box,
753 &fr->kappa,&fr->k_rf,&fr->c_rf);
757 void set_avcsixtwelve(FILE *fplog,t_forcerec *fr,const gmx_mtop_t *mtop)
759 const t_atoms *atoms;
760 const t_blocka *excl;
761 int mb,nmol,nmolc,i,j,tpi,tpj,j1,j2,k,n,nexcl,q;
762 #if (defined SIZEOF_LONG_LONG_INT) && (SIZEOF_LONG_LONG_INT >= 8)
763 long long int npair,npair_ij,tmpi,tmpj;
764 #else
765 double npair, npair_ij,tmpi,tmpj;
766 #endif
767 double csix,ctwelve;
768 int ntp,*typecount;
769 bool bBHAM;
770 real *nbfp;
772 ntp = fr->ntype;
773 bBHAM = fr->bBHAM;
774 nbfp = fr->nbfp;
776 for(q=0; q<(fr->efep==efepNO ? 1 : 2); q++) {
777 csix = 0;
778 ctwelve = 0;
779 npair = 0;
780 nexcl = 0;
781 if (!fr->n_tpi) {
782 /* Count the types so we avoid natoms^2 operations */
783 snew(typecount,ntp);
784 for(mb=0; mb<mtop->nmolblock; mb++) {
785 nmol = mtop->molblock[mb].nmol;
786 atoms = &mtop->moltype[mtop->molblock[mb].type].atoms;
787 for(i=0; i<atoms->nr; i++) {
788 if (q == 0)
790 tpi = atoms->atom[i].type;
792 else
794 tpi = atoms->atom[i].typeB;
796 typecount[tpi] += nmol;
799 for(tpi=0; tpi<ntp; tpi++) {
800 for(tpj=tpi; tpj<ntp; tpj++) {
801 tmpi = typecount[tpi];
802 tmpj = typecount[tpj];
803 if (tpi != tpj)
805 npair_ij = tmpi*tmpj;
807 else
809 npair_ij = tmpi*(tmpi - 1)/2;
811 if (bBHAM) {
812 csix += npair_ij*BHAMC(nbfp,ntp,tpi,tpj);
813 } else {
814 csix += npair_ij* C6(nbfp,ntp,tpi,tpj);
815 ctwelve += npair_ij* C12(nbfp,ntp,tpi,tpj);
817 npair += npair_ij;
820 sfree(typecount);
821 /* Subtract the excluded pairs.
822 * The main reason for substracting exclusions is that in some cases
823 * some combinations might never occur and the parameters could have
824 * any value. These unused values should not influence the dispersion
825 * correction.
827 for(mb=0; mb<mtop->nmolblock; mb++) {
828 nmol = mtop->molblock[mb].nmol;
829 atoms = &mtop->moltype[mtop->molblock[mb].type].atoms;
830 excl = &mtop->moltype[mtop->molblock[mb].type].excls;
831 for(i=0; (i<atoms->nr); i++) {
832 if (q == 0)
834 tpi = atoms->atom[i].type;
836 else
838 tpi = atoms->atom[i].typeB;
840 j1 = excl->index[i];
841 j2 = excl->index[i+1];
842 for(j=j1; j<j2; j++) {
843 k = excl->a[j];
844 if (k > i)
846 if (q == 0)
848 tpj = atoms->atom[k].type;
850 else
852 tpj = atoms->atom[k].typeB;
854 if (bBHAM) {
855 csix -= nmol*BHAMC(nbfp,ntp,tpi,tpj);
856 } else {
857 csix -= nmol*C6 (nbfp,ntp,tpi,tpj);
858 ctwelve -= nmol*C12(nbfp,ntp,tpi,tpj);
860 nexcl += nmol;
865 } else {
866 /* Only correct for the interaction of the test particle
867 * with the rest of the system.
869 atoms = &mtop->moltype[mtop->molblock[mtop->nmolblock-1].type].atoms;
870 if (q == 0)
872 tpi = atoms->atom[atoms->nr-1].type;
874 else
876 tpi = atoms->atom[atoms->nr-1].typeB;
878 npair = 0;
879 for(mb=0; mb<mtop->nmolblock; mb++) {
880 nmol = mtop->molblock[mb].nmol;
881 atoms = &mtop->moltype[mtop->molblock[mb].type].atoms;
882 for(j=0; j<atoms->nr; j++) {
883 nmolc = nmol;
884 /* Remove the interaction of the test charge group
885 * with itself.
887 if (mb == mtop->nmolblock-1 && j >= atoms->nr - fr->n_tpi)
889 nmolc--;
891 if (q == 0)
893 tpj = atoms->atom[j].type;
895 else
897 tpj = atoms->atom[j].typeB;
899 if (bBHAM)
901 csix += nmolc*BHAMC(nbfp,ntp,tpi,tpj);
903 else
905 csix += nmolc*C6 (nbfp,ntp,tpi,tpj);
906 ctwelve += nmolc*C12(nbfp,ntp,tpi,tpj);
908 npair += nmolc;
912 if (npair - nexcl <= 0 && fplog) {
913 fprintf(fplog,"\nWARNING: There are no atom pairs for dispersion correction\n\n");
914 csix = 0;
915 ctwelve = 0;
916 } else {
917 csix /= npair - nexcl;
918 ctwelve /= npair - nexcl;
920 if (debug) {
921 fprintf(debug,"Counted %d exclusions\n",nexcl);
922 fprintf(debug,"Average C6 parameter is: %10g\n",(double)csix);
923 fprintf(debug,"Average C12 parameter is: %10g\n",(double)ctwelve);
925 fr->avcsix[q] = csix;
926 fr->avctwelve[q] = ctwelve;
928 if (fplog != NULL)
930 if (fr->eDispCorr == edispcAllEner ||
931 fr->eDispCorr == edispcAllEnerPres)
933 fprintf(fplog,"Long Range LJ corr.: <C6> %10.4e, <C12> %10.4e\n",
934 fr->avcsix[0],fr->avctwelve[0]);
936 else
938 fprintf(fplog,"Long Range LJ corr.: <C6> %10.4e\n",fr->avcsix[0]);
944 static void set_bham_b_max(FILE *fplog,t_forcerec *fr,
945 const gmx_mtop_t *mtop)
947 const t_atoms *at1,*at2;
948 int mt1,mt2,i,j,tpi,tpj,ntypes;
949 real b,bmin;
950 real *nbfp;
952 if (fplog)
954 fprintf(fplog,"Determining largest Buckingham b parameter for table\n");
956 nbfp = fr->nbfp;
957 ntypes = fr->ntype;
959 bmin = -1;
960 fr->bham_b_max = 0;
961 for(mt1=0; mt1<mtop->nmoltype; mt1++)
963 at1 = &mtop->moltype[mt1].atoms;
964 for(i=0; (i<at1->nr); i++)
966 tpi = at1->atom[i].type;
967 if (tpi >= ntypes)
968 gmx_fatal(FARGS,"Atomtype[%d] = %d, maximum = %d",i,tpi,ntypes);
970 for(mt2=mt1; mt2<mtop->nmoltype; mt2++)
972 at2 = &mtop->moltype[mt2].atoms;
973 for(j=0; (j<at2->nr); j++) {
974 tpj = at2->atom[j].type;
975 if (tpj >= ntypes)
977 gmx_fatal(FARGS,"Atomtype[%d] = %d, maximum = %d",j,tpj,ntypes);
979 b = BHAMB(nbfp,ntypes,tpi,tpj);
980 if (b > fr->bham_b_max)
982 fr->bham_b_max = b;
984 if ((b < bmin) || (bmin==-1))
986 bmin = b;
992 if (fplog)
994 fprintf(fplog,"Buckingham b parameters, min: %g, max: %g\n",
995 bmin,fr->bham_b_max);
999 static void make_nbf_tables(FILE *fp,const output_env_t oenv,
1000 t_forcerec *fr,real rtab,
1001 const t_commrec *cr,
1002 const char *tabfn,char *eg1,char *eg2,
1003 t_nblists *nbl)
1005 char buf[STRLEN];
1006 int i,j;
1007 void * p_tmp;
1009 if (tabfn == NULL) {
1010 if (debug)
1011 fprintf(debug,"No table file name passed, can not read table, can not do non-bonded interactions\n");
1012 return;
1015 sprintf(buf,"%s",tabfn);
1016 if (eg1 && eg2)
1017 /* Append the two energy group names */
1018 sprintf(buf + strlen(tabfn) - strlen(ftp2ext(efXVG)) - 1,"_%s_%s.%s",
1019 eg1,eg2,ftp2ext(efXVG));
1020 nbl->tab = make_tables(fp,oenv,fr,MASTER(cr),buf,rtab,0);
1021 /* Copy the contents of the table to separate coulomb and LJ tables too,
1022 * to improve cache performance.
1025 /* For performance reasons we want
1026 * the table data to be aligned to 16-byte. This is accomplished
1027 * by allocating 16 bytes extra to a temporary pointer, and then
1028 * calculating an aligned pointer. This new pointer must not be
1029 * used in a free() call, but thankfully we're sloppy enough not
1030 * to do this...
1033 /* 8 fp entries per vdw table point, n+1 points, and 16 bytes extra to align it. */
1034 p_tmp = malloc(8*(nbl->tab.n+1)*sizeof(real)+16);
1036 /* align it - size_t has the same same as a pointer */
1037 nbl->vdwtab = (real *) (((size_t) p_tmp + 16) & (~((size_t) 15)));
1039 /* 4 fp entries per coul table point, n+1 points, and 16 bytes extra to align it. */
1040 p_tmp = malloc(4*(nbl->tab.n+1)*sizeof(real)+16);
1042 /* align it - size_t has the same same as a pointer */
1043 nbl->coultab = (real *) (((size_t) p_tmp + 16) & (~((size_t) 15)));
1046 for(i=0; i<=nbl->tab.n; i++) {
1047 for(j=0; j<4; j++)
1048 nbl->coultab[4*i+j] = nbl->tab.tab[12*i+j];
1049 for(j=0; j<8; j++)
1050 nbl->vdwtab [8*i+j] = nbl->tab.tab[12*i+4+j];
1054 static void count_tables(int ftype1,int ftype2,const gmx_mtop_t *mtop,
1055 int *ncount,int **count)
1057 const gmx_moltype_t *molt;
1058 const t_ilist *il;
1059 int mt,ftype,stride,i,j,tabnr;
1061 for(mt=0; mt<mtop->nmoltype; mt++)
1063 molt = &mtop->moltype[mt];
1064 for(ftype=0; ftype<F_NRE; ftype++)
1066 if (ftype == ftype1 || ftype == ftype2) {
1067 il = &molt->ilist[ftype];
1068 stride = 1 + NRAL(ftype);
1069 for(i=0; i<il->nr; i+=stride) {
1070 tabnr = mtop->ffparams.iparams[il->iatoms[i]].tab.table;
1071 if (tabnr < 0)
1072 gmx_fatal(FARGS,"A bonded table number is smaller than 0: %d\n",tabnr);
1073 if (tabnr >= *ncount) {
1074 srenew(*count,tabnr+1);
1075 for(j=*ncount; j<tabnr+1; j++)
1076 (*count)[j] = 0;
1077 *ncount = tabnr+1;
1079 (*count)[tabnr]++;
1086 static bondedtable_t *make_bonded_tables(FILE *fplog,
1087 int ftype1,int ftype2,
1088 const gmx_mtop_t *mtop,
1089 const char *basefn,const char *tabext)
1091 int i,ncount,*count;
1092 char tabfn[STRLEN];
1093 bondedtable_t *tab;
1095 tab = NULL;
1097 ncount = 0;
1098 count = NULL;
1099 count_tables(ftype1,ftype2,mtop,&ncount,&count);
1101 if (ncount > 0) {
1102 snew(tab,ncount);
1103 for(i=0; i<ncount; i++) {
1104 if (count[i] > 0) {
1105 sprintf(tabfn,"%s",basefn);
1106 sprintf(tabfn + strlen(basefn) - strlen(ftp2ext(efXVG)) - 1,"_%s%d.%s",
1107 tabext,i,ftp2ext(efXVG));
1108 tab[i] = make_bonded_table(fplog,tabfn,NRAL(ftype1)-2);
1111 sfree(count);
1114 return tab;
1117 void forcerec_set_ranges(t_forcerec *fr,
1118 int ncg_home,int ncg_force,
1119 int natoms_force,int natoms_f_novirsum)
1121 fr->cg0 = 0;
1122 fr->hcg = ncg_home;
1124 /* fr->ncg_force is unused in the standard code,
1125 * but it can be useful for modified code dealing with charge groups.
1127 fr->ncg_force = ncg_force;
1128 fr->natoms_force = natoms_force;
1130 if (fr->natoms_force > fr->nalloc_force)
1132 fr->nalloc_force = over_alloc_dd(fr->natoms_force);
1134 if (fr->bTwinRange)
1136 srenew(fr->f_twin,fr->nalloc_force);
1140 if (fr->bF_NoVirSum)
1142 fr->f_novirsum_n = natoms_f_novirsum;
1143 if (fr->f_novirsum_n > fr->f_novirsum_nalloc)
1145 fr->f_novirsum_nalloc = over_alloc_dd(fr->f_novirsum_n);
1146 srenew(fr->f_novirsum_alloc,fr->f_novirsum_nalloc);
1149 else
1151 fr->f_novirsum_n = 0;
1155 static real cutoff_inf(real cutoff)
1157 if (cutoff == 0)
1159 cutoff = GMX_CUTOFF_INF;
1162 return cutoff;
1165 void init_forcerec(FILE *fp,
1166 const output_env_t oenv,
1167 t_forcerec *fr,
1168 t_fcdata *fcd,
1169 const t_inputrec *ir,
1170 const gmx_mtop_t *mtop,
1171 const t_commrec *cr,
1172 matrix box,
1173 bool bMolEpot,
1174 const char *tabfn,
1175 const char *tabpfn,
1176 const char *tabbfn,
1177 bool bNoSolvOpt,
1178 real print_force)
1180 int i,j,m,natoms,ngrp,negp_pp,negptable,egi,egj;
1181 real rtab;
1182 rvec box_size;
1183 const t_block *cgs;
1184 bool bTab,bSep14tab,bNormalnblists;
1185 t_nblists *nbl;
1186 int *nm_ind,egp_flags;
1188 fr->bDomDec = DOMAINDECOMP(cr);
1190 natoms = mtop->natoms;
1192 if (check_box(ir->ePBC,box))
1194 gmx_fatal(FARGS,check_box(ir->ePBC,box));
1197 /* Test particle insertion ? */
1198 if (EI_TPI(ir->eI)) {
1199 /* Set to the size of the molecule to be inserted (the last one) */
1200 /* Because of old style topologies, we have to use the last cg
1201 * instead of the last molecule type.
1203 cgs = &mtop->moltype[mtop->molblock[mtop->nmolblock-1].type].cgs;
1204 fr->n_tpi = cgs->index[cgs->nr] - cgs->index[cgs->nr-1];
1205 if (fr->n_tpi != mtop->mols.index[mtop->mols.nr] - mtop->mols.index[mtop->mols.nr-1]) {
1206 gmx_fatal(FARGS,"The molecule to insert can not consist of multiple charge groups.\nMake it a single charge group.");
1208 } else {
1209 fr->n_tpi = 0;
1212 /* Copy the user determined parameters */
1213 fr->userint1 = ir->userint1;
1214 fr->userint2 = ir->userint2;
1215 fr->userint3 = ir->userint3;
1216 fr->userint4 = ir->userint4;
1217 fr->userreal1 = ir->userreal1;
1218 fr->userreal2 = ir->userreal2;
1219 fr->userreal3 = ir->userreal3;
1220 fr->userreal4 = ir->userreal4;
1222 /* Shell stuff */
1223 fr->fc_stepsize = ir->fc_stepsize;
1225 /* Free energy */
1226 fr->efep = ir->efep;
1227 fr->sc_alpha = ir->sc_alpha;
1228 fr->sc_power = ir->sc_power;
1229 fr->sc_sigma6 = pow(ir->sc_sigma,6);
1231 /* Check if we can/should do all-vs-all kernels */
1232 #ifdef GMX_DOUBLE
1233 /* double not done yet */
1234 fr->bAllvsAll = FALSE;
1235 #else
1236 fr->bAllvsAll = (ir->rlist==0 &&
1237 ir->rcoulomb==0 &&
1238 ir->rvdw==0 &&
1239 ir->ePBC==epbcNONE &&
1240 ir->vdwtype==evdwCUT &&
1241 ir->coulombtype==eelCUT &&
1242 ir->efep==efepNO &&
1243 (ir->implicit_solvent == eisNO ||
1244 (ir->implicit_solvent==eisGBSA && (ir->gb_algorithm==egbSTILL ||
1245 ir->gb_algorithm==egbHCT ||
1246 ir->gb_algorithm==egbOBC)))
1248 if (fr->bAllvsAll && ir->opts.ngener > 1)
1250 const char *note="NOTE: Can not use all-vs-all force loops, because there are multiple energy monitor groups; you might get significantly higher performance when using only a single energy monitor group.\n";
1251 if (MASTER(cr))
1253 fprintf(stderr,"\n%s\n",note);
1255 if (fp != NULL)
1257 fprintf(fp,"\n%s\n",note);
1259 fr->bAllvsAll = FALSE;
1261 #endif
1262 fr->AllvsAll_work = NULL;
1263 fr->AllvsAll_workgb = NULL;
1265 /* Neighbour searching stuff */
1266 fr->bGrid = (ir->ns_type == ensGRID);
1267 fr->ePBC = ir->ePBC;
1268 fr->bMolPBC = ir->bPeriodicMols;
1269 fr->rc_scaling = ir->refcoord_scaling;
1270 copy_rvec(ir->posres_com,fr->posres_com);
1271 copy_rvec(ir->posres_comB,fr->posres_comB);
1272 fr->rlist = cutoff_inf(ir->rlist);
1273 fr->rlistlong = cutoff_inf(ir->rlistlong);
1274 fr->eeltype = ir->coulombtype;
1275 fr->vdwtype = ir->vdwtype;
1277 fr->bTwinRange = fr->rlistlong > fr->rlist;
1278 fr->bEwald = (EEL_PME(fr->eeltype) || fr->eeltype==eelEWALD);
1280 fr->reppow = mtop->ffparams.reppow;
1281 fr->bvdwtab = (fr->vdwtype != evdwCUT ||
1282 !gmx_within_tol(fr->reppow,12.0,10*GMX_DOUBLE_EPS));
1283 fr->bcoultab = (!(fr->eeltype == eelCUT || EEL_RF(fr->eeltype)) ||
1284 fr->eeltype == eelRF_ZERO);
1286 if (getenv("GMX_FORCE_TABLES"))
1288 fr->bvdwtab = TRUE;
1289 fr->bcoultab = TRUE;
1292 if (fp) {
1293 fprintf(fp,"Table routines are used for coulomb: %s\n",bool_names[fr->bcoultab]);
1294 fprintf(fp,"Table routines are used for vdw: %s\n",bool_names[fr->bvdwtab ]);
1297 /* Tables are used for direct ewald sum */
1298 if(fr->bEwald)
1300 if (EEL_PME(ir->coulombtype))
1302 if (fp)
1303 fprintf(fp,"Will do PME sum in reciprocal space.\n");
1304 please_cite(fp,"Essman95a");
1306 if (ir->ewald_geometry == eewg3DC)
1308 if (fp)
1310 fprintf(fp,"Using the Ewald3DC correction for systems with a slab geometry.\n");
1312 please_cite(fp,"In-Chul99a");
1315 fr->ewaldcoeff=calc_ewaldcoeff(ir->rcoulomb, ir->ewald_rtol);
1316 init_ewald_tab(&(fr->ewald_table), cr, ir, fp);
1317 if (fp)
1319 fprintf(fp,"Using a Gaussian width (1/beta) of %g nm for Ewald\n",
1320 1/fr->ewaldcoeff);
1324 /* Electrostatics */
1325 fr->epsilon_r = ir->epsilon_r;
1326 fr->epsilon_rf = ir->epsilon_rf;
1327 fr->fudgeQQ = mtop->ffparams.fudgeQQ;
1328 fr->rcoulomb_switch = ir->rcoulomb_switch;
1329 fr->rcoulomb = cutoff_inf(ir->rcoulomb);
1331 /* Parameters for generalized RF */
1332 fr->zsquare = 0.0;
1333 fr->temp = 0.0;
1335 if (fr->eeltype == eelGRF)
1337 init_generalized_rf(fp,mtop,ir,fr);
1339 else if (EEL_FULL(fr->eeltype) || (fr->eeltype == eelSHIFT) ||
1340 (fr->eeltype == eelUSER) || (fr->eeltype == eelSWITCH))
1342 /* We must use the long range cut-off for neighboursearching...
1343 * An extra range of e.g. 0.1 nm (half the size of a charge group)
1344 * is necessary for neighboursearching. This allows diffusion
1345 * into the cut-off range (between neighborlist updates),
1346 * and gives more accurate forces because all atoms within the short-range
1347 * cut-off rc must be taken into account, while the ns criterium takes
1348 * only those with the center of geometry within the cut-off.
1349 * (therefore we have to add half the size of a charge group, plus
1350 * something to account for diffusion if we have nstlist > 1)
1352 for(m=0; (m<DIM); m++)
1353 box_size[m]=box[m][m];
1355 if (fr->eeltype == eelPPPM && fr->phi == NULL)
1356 snew(fr->phi,natoms);
1358 if ((fr->eeltype==eelPPPM) || (fr->eeltype==eelPOISSON) ||
1359 (fr->eeltype == eelSHIFT && fr->rcoulomb > fr->rcoulomb_switch))
1360 set_shift_consts(fp,fr->rcoulomb_switch,fr->rcoulomb,box_size,fr);
1363 fr->bF_NoVirSum = (EEL_FULL(fr->eeltype) ||
1364 gmx_mtop_ftype_count(mtop,F_POSRES) > 0 ||
1365 IR_ELEC_FIELD(*ir));
1367 /* Mask that says whether or not this NBF list should be computed */
1368 /* if (fr->bMask == NULL) {
1369 ngrp = ir->opts.ngener*ir->opts.ngener;
1370 snew(fr->bMask,ngrp);*/
1371 /* Defaults to always */
1372 /* for(i=0; (i<ngrp); i++)
1373 fr->bMask[i] = TRUE;
1376 if (ncg_mtop(mtop) > fr->cg_nalloc && !DOMAINDECOMP(cr)) {
1377 /* Count the total number of charge groups */
1378 fr->cg_nalloc = ncg_mtop(mtop);
1379 srenew(fr->cg_cm,fr->cg_nalloc);
1381 if (fr->shift_vec == NULL)
1382 snew(fr->shift_vec,SHIFTS);
1384 if (fr->fshift == NULL)
1385 snew(fr->fshift,SHIFTS);
1387 if (fr->nbfp == NULL) {
1388 fr->ntype = mtop->ffparams.atnr;
1389 fr->bBHAM = (mtop->ffparams.functype[0] == F_BHAM);
1390 fr->nbfp = mk_nbfp(&mtop->ffparams,fr->bBHAM);
1393 /* Copy the energy group exclusions */
1394 fr->egp_flags = ir->opts.egp_flags;
1396 /* Van der Waals stuff */
1397 fr->rvdw = cutoff_inf(ir->rvdw);
1398 fr->rvdw_switch = ir->rvdw_switch;
1399 if ((fr->vdwtype != evdwCUT) && (fr->vdwtype != evdwUSER) && !fr->bBHAM) {
1400 if (fr->rvdw_switch >= fr->rvdw)
1401 gmx_fatal(FARGS,"rvdw_switch (%f) must be < rvdw (%f)",
1402 fr->rvdw_switch,fr->rvdw);
1403 if (fp)
1404 fprintf(fp,"Using %s Lennard-Jones, switch between %g and %g nm\n",
1405 (fr->eeltype==eelSWITCH) ? "switched":"shifted",
1406 fr->rvdw_switch,fr->rvdw);
1409 if (fr->bBHAM && (fr->vdwtype == evdwSHIFT || fr->vdwtype == evdwSWITCH))
1410 gmx_fatal(FARGS,"Switch/shift interaction not supported with Buckingham");
1412 if (fp)
1413 fprintf(fp,"Cut-off's: NS: %g Coulomb: %g %s: %g\n",
1414 fr->rlist,fr->rcoulomb,fr->bBHAM ? "BHAM":"LJ",fr->rvdw);
1416 fr->eDispCorr = ir->eDispCorr;
1417 if (ir->eDispCorr != edispcNO)
1419 set_avcsixtwelve(fp,fr,mtop);
1422 if (fr->bBHAM)
1424 set_bham_b_max(fp,fr,mtop);
1427 fr->bGB = (ir->implicit_solvent == eisGBSA);
1428 fr->gb_epsilon_solvent = ir->gb_epsilon_solvent;
1430 /* Copy the GBSA data (radius, volume and surftens for each
1431 * atomtype) from the topology atomtype section to forcerec.
1433 snew(fr->atype_radius,fr->ntype);
1434 snew(fr->atype_vol,fr->ntype);
1435 snew(fr->atype_surftens,fr->ntype);
1436 snew(fr->atype_gb_radius,fr->ntype);
1437 snew(fr->atype_S_hct,fr->ntype);
1439 if (mtop->atomtypes.nr > 0)
1441 for(i=0;i<fr->ntype;i++)
1442 fr->atype_radius[i] =mtop->atomtypes.radius[i];
1443 for(i=0;i<fr->ntype;i++)
1444 fr->atype_vol[i] = mtop->atomtypes.vol[i];
1445 for(i=0;i<fr->ntype;i++)
1446 fr->atype_surftens[i] = mtop->atomtypes.surftens[i];
1447 for(i=0;i<fr->ntype;i++)
1448 fr->atype_gb_radius[i] = mtop->atomtypes.gb_radius[i];
1449 for(i=0;i<fr->ntype;i++)
1450 fr->atype_S_hct[i] = mtop->atomtypes.S_hct[i];
1453 /* Generate the GB table if needed */
1454 if(fr->bGB)
1456 #ifdef GMX_DOUBLE
1457 fr->gbtabscale=2000;
1458 #else
1459 fr->gbtabscale=500;
1460 #endif
1462 fr->gbtabr=100;
1463 fr->gbtab=make_gb_table(fp,oenv,fr,tabpfn,fr->gbtabscale);
1465 init_gb(&fr->born,cr,fr,ir,mtop,ir->rgbradii,ir->gb_algorithm);
1467 /* Copy local gb data (for dd, this is done in dd_partition_system) */
1468 if (!DOMAINDECOMP(cr))
1470 make_local_gb(cr,fr->born,ir->gb_algorithm);
1474 /* Set the charge scaling */
1475 if (fr->epsilon_r != 0)
1476 fr->epsfac = ONE_4PI_EPS0/fr->epsilon_r;
1477 else
1478 /* eps = 0 is infinite dieletric: no coulomb interactions */
1479 fr->epsfac = 0;
1481 /* Reaction field constants */
1482 if (EEL_RF(fr->eeltype))
1483 calc_rffac(fp,fr->eeltype,fr->epsilon_r,fr->epsilon_rf,
1484 fr->rcoulomb,fr->temp,fr->zsquare,box,
1485 &fr->kappa,&fr->k_rf,&fr->c_rf);
1487 set_chargesum(fp,fr,mtop);
1489 /* if we are using LR electrostatics, and they are tabulated,
1490 * the tables will contain modified coulomb interactions.
1491 * Since we want to use the non-shifted ones for 1-4
1492 * coulombic interactions, we must have an extra set of tables.
1495 /* Construct tables.
1496 * A little unnecessary to make both vdw and coul tables sometimes,
1497 * but what the heck... */
1499 bTab = fr->bcoultab || fr->bvdwtab;
1501 bSep14tab = ((!bTab || fr->eeltype!=eelCUT || fr->vdwtype!=evdwCUT ||
1502 fr->bBHAM) &&
1503 (gmx_mtop_ftype_count(mtop,F_LJ14) > 0 ||
1504 gmx_mtop_ftype_count(mtop,F_LJC14_Q) > 0 ||
1505 gmx_mtop_ftype_count(mtop,F_LJC_PAIRS_NB) > 0));
1507 negp_pp = ir->opts.ngener - ir->nwall;
1508 negptable = 0;
1509 if (!bTab) {
1510 bNormalnblists = TRUE;
1511 fr->nnblists = 1;
1512 } else {
1513 bNormalnblists = (ir->eDispCorr != edispcNO);
1514 for(egi=0; egi<negp_pp; egi++) {
1515 for(egj=egi; egj<negp_pp; egj++) {
1516 egp_flags = ir->opts.egp_flags[GID(egi,egj,ir->opts.ngener)];
1517 if (!(egp_flags & EGP_EXCL)) {
1518 if (egp_flags & EGP_TABLE) {
1519 negptable++;
1520 } else {
1521 bNormalnblists = TRUE;
1526 if (bNormalnblists) {
1527 fr->nnblists = negptable + 1;
1528 } else {
1529 fr->nnblists = negptable;
1531 if (fr->nnblists > 1)
1532 snew(fr->gid2nblists,ir->opts.ngener*ir->opts.ngener);
1534 snew(fr->nblists,fr->nnblists);
1536 /* This code automatically gives table length tabext without cut-off's,
1537 * in that case grompp should already have checked that we do not need
1538 * normal tables and we only generate tables for 1-4 interactions.
1540 rtab = ir->rlistlong + ir->tabext;
1542 if (bTab) {
1543 /* make tables for ordinary interactions */
1544 if (bNormalnblists) {
1545 make_nbf_tables(fp,oenv,fr,rtab,cr,tabfn,NULL,NULL,&fr->nblists[0]);
1546 if (!bSep14tab)
1547 fr->tab14 = fr->nblists[0].tab;
1548 m = 1;
1549 } else {
1550 m = 0;
1552 if (negptable > 0) {
1553 /* Read the special tables for certain energy group pairs */
1554 nm_ind = mtop->groups.grps[egcENER].nm_ind;
1555 for(egi=0; egi<negp_pp; egi++) {
1556 for(egj=egi; egj<negp_pp; egj++) {
1557 egp_flags = ir->opts.egp_flags[GID(egi,egj,ir->opts.ngener)];
1558 if ((egp_flags & EGP_TABLE) && !(egp_flags & EGP_EXCL)) {
1559 nbl = &(fr->nblists[m]);
1560 if (fr->nnblists > 1) {
1561 fr->gid2nblists[GID(egi,egj,ir->opts.ngener)] = m;
1563 /* Read the table file with the two energy groups names appended */
1564 make_nbf_tables(fp,oenv,fr,rtab,cr,tabfn,
1565 *mtop->groups.grpname[nm_ind[egi]],
1566 *mtop->groups.grpname[nm_ind[egj]],
1567 &fr->nblists[m]);
1568 m++;
1569 } else if (fr->nnblists > 1) {
1570 fr->gid2nblists[GID(egi,egj,ir->opts.ngener)] = 0;
1576 if (bSep14tab)
1578 /* generate extra tables with plain Coulomb for 1-4 interactions only */
1579 fr->tab14 = make_tables(fp,oenv,fr,MASTER(cr),tabpfn,rtab,
1580 GMX_MAKETABLES_14ONLY);
1583 /* Wall stuff */
1584 fr->nwall = ir->nwall;
1585 if (ir->nwall && ir->wall_type==ewtTABLE)
1587 make_wall_tables(fp,oenv,ir,tabfn,&mtop->groups,fr);
1590 if (fcd && tabbfn) {
1591 fcd->bondtab = make_bonded_tables(fp,
1592 F_TABBONDS,F_TABBONDSNC,
1593 mtop,tabbfn,"b");
1594 fcd->angletab = make_bonded_tables(fp,
1595 F_TABANGLES,-1,
1596 mtop,tabbfn,"a");
1597 fcd->dihtab = make_bonded_tables(fp,
1598 F_TABDIHS,-1,
1599 mtop,tabbfn,"d");
1600 } else {
1601 if (debug)
1602 fprintf(debug,"No fcdata or table file name passed, can not read table, can not do bonded interactions\n");
1605 if (ir->eDispCorr != edispcNO)
1607 calc_enervirdiff(fp,ir->eDispCorr,fr);
1610 /* QM/MM initialization if requested
1612 if (ir->bQMMM)
1614 fprintf(stderr,"QM/MM calculation requested.\n");
1617 fr->bQMMM = ir->bQMMM;
1618 fr->qr = mk_QMMMrec();
1620 /* Set all the static charge group info */
1621 fr->cginfo_mb = init_cginfo_mb(fp,mtop,fr,bNoSolvOpt);
1622 if (DOMAINDECOMP(cr)) {
1623 fr->cginfo = NULL;
1624 } else {
1625 fr->cginfo = cginfo_expand(mtop->nmolblock,fr->cginfo_mb);
1628 if (!DOMAINDECOMP(cr))
1630 /* When using particle decomposition, the effect of the second argument,
1631 * which sets fr->hcg, is corrected later in do_md and init_em.
1633 forcerec_set_ranges(fr,ncg_mtop(mtop),ncg_mtop(mtop),
1634 mtop->natoms,mtop->natoms);
1637 fr->print_force = print_force;
1640 /* coarse load balancing vars */
1641 fr->t_fnbf=0.;
1642 fr->t_wait=0.;
1643 fr->timesteps=0;
1645 /* Initialize neighbor search */
1646 init_ns(fp,cr,&fr->ns,fr,mtop,box);
1648 if (cr->duty & DUTY_PP)
1649 gmx_setup_kernels(fp);
1652 #define pr_real(fp,r) fprintf(fp,"%s: %e\n",#r,r)
1653 #define pr_int(fp,i) fprintf((fp),"%s: %d\n",#i,i)
1654 #define pr_bool(fp,b) fprintf((fp),"%s: %s\n",#b,bool_names[b])
1656 void pr_forcerec(FILE *fp,t_forcerec *fr,t_commrec *cr)
1658 int i;
1660 pr_real(fp,fr->rlist);
1661 pr_real(fp,fr->rcoulomb);
1662 pr_real(fp,fr->fudgeQQ);
1663 pr_bool(fp,fr->bGrid);
1664 pr_bool(fp,fr->bTwinRange);
1665 /*pr_int(fp,fr->cg0);
1666 pr_int(fp,fr->hcg);*/
1667 for(i=0; i<fr->nnblists; i++)
1668 pr_int(fp,fr->nblists[i].tab.n);
1669 pr_real(fp,fr->rcoulomb_switch);
1670 pr_real(fp,fr->rcoulomb);
1672 fflush(fp);