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37 #ifndef GMX_MDTYPES_TYPES_FORCEREC_H
38 #define GMX_MDTYPES_TYPES_FORCEREC_H
43 #include "gromacs/math/vectypes.h"
44 #include "gromacs/mdtypes/interaction_const.h"
45 #include "gromacs/mdtypes/md_enums.h"
46 #include "gromacs/utility/basedefinitions.h"
47 #include "gromacs/utility/real.h"
49 struct ForceProviders
;
51 /* Abstract type for PME that is defined only in the routine that use them. */
54 struct nonbonded_verlet_t
;
55 struct bonded_threading_t
;
66 /* macros for the cginfo data in forcerec
68 * Since the tpx format support max 256 energy groups, we do the same here.
69 * Note that we thus have bits 8-14 still unused.
71 * The maximum cg size in cginfo is 63
72 * because we only have space for 6 bits in cginfo,
73 * this cg size entry is actually only read with domain decomposition.
74 * But there is a smaller limit due to the t_excl data structure
75 * which is defined in nblist.h.
77 #define SET_CGINFO_GID(cgi, gid) (cgi) = (((cgi) & ~255) | (gid))
78 #define GET_CGINFO_GID(cgi) ( (cgi) & 255)
79 #define SET_CGINFO_FEP(cgi) (cgi) = ((cgi) | (1<<15))
80 #define GET_CGINFO_FEP(cgi) ( (cgi) & (1<<15))
81 #define SET_CGINFO_EXCL_INTRA(cgi) (cgi) = ((cgi) | (1<<16))
82 #define GET_CGINFO_EXCL_INTRA(cgi) ( (cgi) & (1<<16))
83 #define SET_CGINFO_EXCL_INTER(cgi) (cgi) = ((cgi) | (1<<17))
84 #define GET_CGINFO_EXCL_INTER(cgi) ( (cgi) & (1<<17))
85 #define SET_CGINFO_SOLOPT(cgi, opt) (cgi) = (((cgi) & ~(3<<18)) | ((opt)<<18))
86 #define GET_CGINFO_SOLOPT(cgi) (((cgi)>>18) & 3)
87 #define SET_CGINFO_CONSTR(cgi) (cgi) = ((cgi) | (1<<20))
88 #define GET_CGINFO_CONSTR(cgi) ( (cgi) & (1<<20))
89 #define SET_CGINFO_SETTLE(cgi) (cgi) = ((cgi) | (1<<21))
90 #define GET_CGINFO_SETTLE(cgi) ( (cgi) & (1<<21))
91 /* This bit is only used with bBondComm in the domain decomposition */
92 #define SET_CGINFO_BOND_INTER(cgi) (cgi) = ((cgi) | (1<<22))
93 #define GET_CGINFO_BOND_INTER(cgi) ( (cgi) & (1<<22))
94 #define SET_CGINFO_HAS_VDW(cgi) (cgi) = ((cgi) | (1<<23))
95 #define GET_CGINFO_HAS_VDW(cgi) ( (cgi) & (1<<23))
96 #define SET_CGINFO_HAS_Q(cgi) (cgi) = ((cgi) | (1<<24))
97 #define GET_CGINFO_HAS_Q(cgi) ( (cgi) & (1<<24))
98 #define SET_CGINFO_NATOMS(cgi, opt) (cgi) = (((cgi) & ~(63<<25)) | ((opt)<<25))
99 #define GET_CGINFO_NATOMS(cgi) (((cgi)>>25) & 63)
102 /* Value to be used in mdrun for an infinite cut-off.
103 * Since we need to compare with the cut-off squared,
104 * this value should be slighlty smaller than sqrt(GMX_FLOAT_MAX).
106 #define GMX_CUTOFF_INF 1E+18
108 /* enums for the neighborlist type */
110 enbvdwNONE
, enbvdwLJ
, enbvdwBHAM
, enbvdwTAB
, enbvdwNR
122 /* Forward declaration of type for managing Ewald tables */
123 struct gmx_ewald_tab_t
;
125 struct ewald_corr_thread_t
;
127 struct t_forcerec
{ // NOLINT (clang-analyzer-optin.performance.Padding)
128 struct interaction_const_t
*ic
;
132 //! Whether PBC must be considered for bonded interactions.
138 gmx_bool use_simd_kernels
;
140 /* Interaction for calculated in kernels. In many cases this is similar to
141 * the electrostatics settings in the inputrecord, but the difference is that
142 * these variables always specify the actual interaction in the kernel - if
143 * we are tabulating reaction-field the inputrec will say reaction-field, but
144 * the kernel interaction will say cubic-spline-table. To be safe we also
145 * have a kernel-specific setting for the modifiers - if the interaction is
146 * tabulated we already included the inputrec modification there, so the kernel
147 * modification setting will say 'none' in that case.
149 int nbkernel_elec_interaction
;
150 int nbkernel_vdw_interaction
;
151 int nbkernel_elec_modifier
;
152 int nbkernel_vdw_modifier
;
154 /* Use special N*N kernels? */
156 /* Private work data */
160 * Infinite cut-off's will be GMX_CUTOFF_INF (unlike in t_inputrec: 0).
164 /* Parameters for generalized reaction field */
167 /* Charge sum and dipole for topology A/B ([0]/[1]) for Ewald corrections */
173 /* Dispersion correction stuff */
175 int numAtomsForDispersionCorrection
;
176 struct t_forcetable
*dispersionCorrectionTable
;
178 /* The shift of the shift or user potentials */
180 real enershifttwelve
;
181 /* Integrated differces for energy and virial with cut-off functions */
186 /* Constant for long range dispersion correction (average dispersion)
187 * for topology A/B ([0]/[1]) */
189 /* Constant for long range repulsion term. Relative difference of about
190 * 0.1 percent with 0.8 nm cutoffs. But hey, it's cheap anyway...
200 /* The normal tables are in the nblists struct(s) below */
202 struct t_forcetable
*pairsTable
; /* for 1-4 interactions, [pairs] and [pairs_nb] */
215 /* solvent_opt contains the enum for the most common solvent
216 * in the system, which will be optimized.
217 * It can be set to esolNO to disable all water optimization */
221 gmx_bool bExcl_IntraCGAll_InterCGNone
;
222 struct cginfo_mb_t
*cginfo_mb
;
228 /* The neighborlists including tables */
231 struct t_nblists
*nblists
;
233 int cutoff_scheme
; /* group- or Verlet-style cutoff */
234 gmx_bool bNonbonded
; /* true if nonbonded calculations are *not* turned off */
235 struct nonbonded_verlet_t
*nbv
;
237 /* The wall tables (if used) */
239 struct t_forcetable
***wall_tab
;
241 /* The number of charge groups participating in do_force_lowlevel */
243 /* The number of atoms participating in do_force_lowlevel */
245 /* The number of atoms participating in force and constraints */
246 int natoms_force_constr
;
247 /* The allocation size of vectors of size natoms_force */
250 /* Forces that should not enter into the coord x force virial summation:
251 * PPPM/PME/Ewald/posres/ForceProviders
253 /* True when we have contributions that are directly added to the virial */
254 gmx_bool haveDirectVirialContributions
;
255 /* TODO: Replace the pointer by an object once we got rid of C */
256 std::vector
<gmx::RVec
> *forceBufferForDirectVirialContributions
;
258 /* Data for PPPM/PME/Ewald */
259 struct gmx_pme_t
*pmedata
;
260 int ljpme_combination_rule
;
262 /* PME/Ewald stuff */
263 struct gmx_ewald_tab_t
*ewald_table
;
265 /* Shift force array for computing the virial */
268 /* Non bonded Parameter lists */
269 int ntype
; /* Number of atom types */
272 real
*ljpme_c6grid
; /* C6-values used on grid in LJPME */
274 /* Energy group pair flags */
277 /* Shell molecular dynamics flexible constraints */
280 /* If > 0 signals Test Particle Insertion,
281 * the value is the number of atoms of the molecule to insert
282 * Only the energy difference due to the addition of the last molecule
283 * should be calculated.
287 /* Neighbor searching stuff */
292 struct t_QMMMrec
*qr
;
294 /* QM-MM neighborlists */
295 struct t_nblist
*QMMMlist
;
297 /* Limit for printing large forces, negative is don't print */
300 /* coarse load balancing time measurement */
305 /* User determined parameters, copied from the inputrec */
315 /* Pointer to struct for managing threading of bonded force calculation */
316 struct bonded_threading_t
*bondedThreading
;
318 /* TODO: Replace the pointer by an object once we got rid of C */
319 gmx::GpuBonded
*gpuBonded
;
321 /* Ewald correction thread local virial and energy data */
323 struct ewald_corr_thread_t
*ewc_t
;
325 struct ForceProviders
*forceProviders
;
328 /* Important: Starting with Gromacs-4.6, the values of c6 and c12 in the nbfp array have
329 * been scaled by 6.0 or 12.0 to save flops in the kernels. We have corrected this everywhere
330 * in the code, but beware if you are using these macros externally.
332 #define C6(nbfp, ntp, ai, aj) (nbfp)[2*((ntp)*(ai)+(aj))]
333 #define C12(nbfp, ntp, ai, aj) (nbfp)[2*((ntp)*(ai)+(aj))+1]
334 #define BHAMC(nbfp, ntp, ai, aj) (nbfp)[3*((ntp)*(ai)+(aj))]
335 #define BHAMA(nbfp, ntp, ai, aj) (nbfp)[3*((ntp)*(ai)+(aj))+1]
336 #define BHAMB(nbfp, ntp, ai, aj) (nbfp)[3*((ntp)*(ai)+(aj))+2]