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37 #ifndef GMX_MDTYPES_TYPES_FORCEREC_H
38 #define GMX_MDTYPES_TYPES_FORCEREC_H
40 #include "gromacs/math/vectypes.h"
42 #include "gromacs/math/paddedvector.h"
44 #include "gromacs/mdtypes/interaction_const.h"
45 #include "gromacs/mdtypes/md_enums.h"
46 #include "gromacs/topology/idef.h"
47 #include "gromacs/utility/basedefinitions.h"
48 #include "gromacs/utility/real.h"
57 /*! \libinternal \brief
58 * Interface for a component that provides forces during MD.
60 * This is typically part of a larger structure/class managing its own
61 * data, such that it has the information on what to do stored locally.
62 * \todo Implement returning of energy and dH/dlambda.
68 /*! \brief Compute forces
70 * \todo This is specific for electric fields and needs to be generalized.
71 * \param[in] cr Communication record for parallel operations
72 * \param[in] mdatoms Atom information
73 * \param[inout] force The forces
74 * \param[in] t The actual time in the simulation (ps)
76 virtual void calculateForces(const t_commrec
*cr
,
77 const t_mdatoms
*mdatoms
,
78 PaddedRVecVector
*force
,
86 /* Abstract type for PME that is defined only in the routine that use them. */
90 struct nonbonded_verlet_t
;
91 struct bonded_threading_t
;
99 /* macros for the cginfo data in forcerec
101 * Since the tpx format support max 256 energy groups, we do the same here.
102 * Note that we thus have bits 8-14 still unused.
104 * The maximum cg size in cginfo is 63
105 * because we only have space for 6 bits in cginfo,
106 * this cg size entry is actually only read with domain decomposition.
107 * But there is a smaller limit due to the t_excl data structure
108 * which is defined in nblist.h.
110 #define SET_CGINFO_GID(cgi, gid) (cgi) = (((cgi) & ~255) | (gid))
111 #define GET_CGINFO_GID(cgi) ( (cgi) & 255)
112 #define SET_CGINFO_FEP(cgi) (cgi) = ((cgi) | (1<<15))
113 #define GET_CGINFO_FEP(cgi) ( (cgi) & (1<<15))
114 #define SET_CGINFO_EXCL_INTRA(cgi) (cgi) = ((cgi) | (1<<16))
115 #define GET_CGINFO_EXCL_INTRA(cgi) ( (cgi) & (1<<16))
116 #define SET_CGINFO_EXCL_INTER(cgi) (cgi) = ((cgi) | (1<<17))
117 #define GET_CGINFO_EXCL_INTER(cgi) ( (cgi) & (1<<17))
118 #define SET_CGINFO_SOLOPT(cgi, opt) (cgi) = (((cgi) & ~(3<<18)) | ((opt)<<18))
119 #define GET_CGINFO_SOLOPT(cgi) (((cgi)>>18) & 3)
120 #define SET_CGINFO_CONSTR(cgi) (cgi) = ((cgi) | (1<<20))
121 #define GET_CGINFO_CONSTR(cgi) ( (cgi) & (1<<20))
122 #define SET_CGINFO_SETTLE(cgi) (cgi) = ((cgi) | (1<<21))
123 #define GET_CGINFO_SETTLE(cgi) ( (cgi) & (1<<21))
124 /* This bit is only used with bBondComm in the domain decomposition */
125 #define SET_CGINFO_BOND_INTER(cgi) (cgi) = ((cgi) | (1<<22))
126 #define GET_CGINFO_BOND_INTER(cgi) ( (cgi) & (1<<22))
127 #define SET_CGINFO_HAS_VDW(cgi) (cgi) = ((cgi) | (1<<23))
128 #define GET_CGINFO_HAS_VDW(cgi) ( (cgi) & (1<<23))
129 #define SET_CGINFO_HAS_Q(cgi) (cgi) = ((cgi) | (1<<24))
130 #define GET_CGINFO_HAS_Q(cgi) ( (cgi) & (1<<24))
131 #define SET_CGINFO_NATOMS(cgi, opt) (cgi) = (((cgi) & ~(63<<25)) | ((opt)<<25))
132 #define GET_CGINFO_NATOMS(cgi) (((cgi)>>25) & 63)
135 /* Value to be used in mdrun for an infinite cut-off.
136 * Since we need to compare with the cut-off squared,
137 * this value should be slighlty smaller than sqrt(GMX_FLOAT_MAX).
139 #define GMX_CUTOFF_INF 1E+18
141 /* enums for the neighborlist type */
143 enbvdwNONE
, enbvdwLJ
, enbvdwBHAM
, enbvdwTAB
, enbvdwNR
145 /* OOR is "one over r" -- standard coul */
147 enbcoulNONE
, enbcoulOOR
, enbcoulRF
, enbcoulTAB
, enbcoulGB
, enbcoulFEWALD
, enbcoulNR
151 egCOULSR
, egLJSR
, egBHAMSR
,
152 egCOUL14
, egLJ14
, egGB
, egNR
154 extern const char *egrp_nm
[egNR
+1];
156 typedef struct gmx_grppairener_t
{
157 int nener
; /* The number of energy group pairs */
158 real
*ener
[egNR
]; /* Energy terms for each pair of groups */
161 typedef struct gmx_enerdata_t
{
162 real term
[F_NRE
]; /* The energies for all different interaction types */
163 gmx_grppairener_t grpp
;
164 double dvdl_lin
[efptNR
]; /* Contributions to dvdl with linear lam-dependence */
165 double dvdl_nonlin
[efptNR
]; /* Idem, but non-linear dependence */
167 int fep_state
; /*current fep state -- just for printing */
168 double *enerpart_lambda
; /* Partial energy for lambda and flambda[] */
169 real foreign_term
[F_NRE
]; /* alternate array for storing foreign lambda energies */
170 gmx_grppairener_t foreign_grpp
; /* alternate array for storing foreign lambda energies */
172 /* The idea is that dvdl terms with linear lambda dependence will be added
173 * automatically to enerpart_lambda. Terms with non-linear lambda dependence
174 * should explicitly determine the energies at foreign lambda points
186 /* Forward declaration of type for managing Ewald tables */
187 struct gmx_ewald_tab_t
;
189 typedef struct ewald_corr_thread_t ewald_corr_thread_t
;
191 typedef struct t_forcerec
{
192 interaction_const_t
*ic
;
194 /* Domain Decomposition */
204 const struct gmx_hw_info_t
*hwinfo
;
205 const struct gmx_gpu_opt_t
*gpu_opt
;
206 gmx_bool use_simd_kernels
;
208 /* Interaction for calculated in kernels. In many cases this is similar to
209 * the electrostatics settings in the inputrecord, but the difference is that
210 * these variables always specify the actual interaction in the kernel - if
211 * we are tabulating reaction-field the inputrec will say reaction-field, but
212 * the kernel interaction will say cubic-spline-table. To be safe we also
213 * have a kernel-specific setting for the modifiers - if the interaction is
214 * tabulated we already included the inputrec modification there, so the kernel
215 * modification setting will say 'none' in that case.
217 int nbkernel_elec_interaction
;
218 int nbkernel_vdw_interaction
;
219 int nbkernel_elec_modifier
;
220 int nbkernel_vdw_modifier
;
222 /* Use special N*N kernels? */
224 /* Private work data */
226 void *AllvsAll_workgb
;
229 * Infinite cut-off's will be GMX_CUTOFF_INF (unlike in t_inputrec: 0).
233 /* Dielectric constant resp. multiplication factor for charges */
235 real epsilon_r
, epsilon_rf
, epsfac
;
237 /* Constants for reaction fields */
238 real kappa
, k_rf
, c_rf
;
240 /* Charge sum and dipole for topology A/B ([0]/[1]) for Ewald corrections */
246 /* Dispersion correction stuff */
248 int numAtomsForDispersionCorrection
;
249 struct t_forcetable
*dispersionCorrectionTable
;
251 /* The shift of the shift or user potentials */
253 real enershifttwelve
;
254 /* Integrated differces for energy and virial with cut-off functions */
259 /* Constant for long range dispersion correction (average dispersion)
260 * for topology A/B ([0]/[1]) */
262 /* Constant for long range repulsion term. Relative difference of about
263 * 0.1 percent with 0.8 nm cutoffs. But hey, it's cheap anyway...
273 /* The normal tables are in the nblists struct(s) below */
275 struct t_forcetable
*pairsTable
; /* for 1-4 interactions, [pairs] and [pairs_nb] */
277 /* PPPM & Shifting stuff */
278 int coulomb_modifier
;
279 real rcoulomb_switch
, rcoulomb
;
285 real rvdw_switch
, rvdw
;
301 /* solvent_opt contains the enum for the most common solvent
302 * in the system, which will be optimized.
303 * It can be set to esolNO to disable all water optimization */
307 gmx_bool bExcl_IntraCGAll_InterCGNone
;
308 cginfo_mb_t
*cginfo_mb
;
314 /* The neighborlists including tables */
317 struct t_nblists
*nblists
;
319 int cutoff_scheme
; /* group- or Verlet-style cutoff */
320 gmx_bool bNonbonded
; /* true if nonbonded calculations are *not* turned off */
321 struct nonbonded_verlet_t
*nbv
;
323 /* The wall tables (if used) */
325 struct t_forcetable
***wall_tab
;
327 /* The number of charge groups participating in do_force_lowlevel */
329 /* The number of atoms participating in do_force_lowlevel */
331 /* The number of atoms participating in force and constraints */
332 int natoms_force_constr
;
333 /* The allocation size of vectors of size natoms_force */
336 /* Forces that should not enter into the virial summation:
337 * PPPM/PME/Ewald/posres
338 * If such forces are present in the system, bF_NoVirSum=TRUE.
340 gmx_bool bF_NoVirSum
;
342 /* TODO: Replace the pointer by an object once we got rid of C */
343 PaddedRVecVector
*forceBufferNoVirialSummation
;
345 void *forceBufferNoVirialSummation_dummy
;
347 /* Pointer that points to forceNoVirialSummation when virial is calcaluted,
348 * points to the normal force vector when the virial is not requested
349 * or when bF_NoVirSum == FALSE.
352 PaddedRVecVector
*f_novirsum
;
354 void *f_novirsum_xdummy
;
357 /* Long-range forces and virial for PPPM/PME/Ewald */
358 struct gmx_pme_t
*pmedata
;
359 int ljpme_combination_rule
;
363 /* PME/Ewald stuff */
367 struct gmx_ewald_tab_t
*ewald_table
;
371 rvec vir_diag_posres
;
374 /* Non bonded Parameter lists */
375 int ntype
; /* Number of atom types */
378 real
*ljpme_c6grid
; /* C6-values used on grid in LJPME */
380 /* Energy group pair flags */
383 /* Shell molecular dynamics flexible constraints */
386 /* Generalized born implicit solvent */
388 /* Generalized born stuff */
389 real gb_epsilon_solvent
;
390 /* Table data for GB */
391 struct t_forcetable
*gbtab
;
392 /* VdW radius for each atomtype (dim is thus ntype) */
394 /* Effective radius (derived from effective volume) for each type */
396 /* Implicit solvent - surface tension for each atomtype */
397 real
*atype_surftens
;
398 /* Implicit solvent - radius for GB calculation */
399 real
*atype_gb_radius
;
400 /* Implicit solvent - overlap for HCT model */
402 /* Generalized born interaction data */
403 struct gmx_genborn_t
*born
;
405 /* Table scale for GB */
407 /* Table range for GB */
409 /* GB neighborlists (the sr list will contain for each atom all other atoms
410 * (for use in the SA calculation) and the lr list will contain
411 * for each atom all atoms 1-4 or greater (for use in the GB calculation)
413 struct t_nblist
*gblist_sr
;
414 struct t_nblist
*gblist_lr
;
415 struct t_nblist
*gblist
;
417 /* Inverse square root of the Born radii for implicit solvent */
419 /* Derivatives of the potential with respect to the Born radii */
421 /* Derivatives of the Born radii with respect to coordinates */
424 int nalloc_dadx
; /* Allocated size of dadx */
426 /* If > 0 signals Test Particle Insertion,
427 * the value is the number of atoms of the molecule to insert
428 * Only the energy difference due to the addition of the last molecule
429 * should be calculated.
433 /* Neighbor searching stuff */
438 struct t_QMMMrec
*qr
;
440 /* QM-MM neighborlists */
441 struct t_nblist
*QMMMlist
;
443 /* Limit for printing large forces, negative is don't print */
446 /* coarse load balancing time measurement */
451 /* User determined parameters, copied from the inputrec */
461 /* Pointer to struct for managing threading of bonded force calculation */
462 struct bonded_threading_t
*bonded_threading
;
464 /* Ewald correction thread local virial and energy data */
466 ewald_corr_thread_t
*ewc_t
;
468 struct IForceProvider
*efield
;
471 /* Important: Starting with Gromacs-4.6, the values of c6 and c12 in the nbfp array have
472 * been scaled by 6.0 or 12.0 to save flops in the kernels. We have corrected this everywhere
473 * in the code, but beware if you are using these macros externally.
475 #define C6(nbfp, ntp, ai, aj) (nbfp)[2*((ntp)*(ai)+(aj))]
476 #define C12(nbfp, ntp, ai, aj) (nbfp)[2*((ntp)*(ai)+(aj))+1]
477 #define BHAMC(nbfp, ntp, ai, aj) (nbfp)[3*((ntp)*(ai)+(aj))]
478 #define BHAMA(nbfp, ntp, ai, aj) (nbfp)[3*((ntp)*(ai)+(aj))+1]
479 #define BHAMB(nbfp, ntp, ai, aj) (nbfp)[3*((ntp)*(ai)+(aj))+2]