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37 #ifndef GMX_MDTYPES_TYPES_FORCEREC_H
38 #define GMX_MDTYPES_TYPES_FORCEREC_H
44 #include "gromacs/math/vectypes.h"
45 #include "gromacs/mdtypes/interaction_const.h"
46 #include "gromacs/mdtypes/md_enums.h"
47 #include "gromacs/utility/basedefinitions.h"
48 #include "gromacs/utility/real.h"
50 struct ForceProviders
;
52 /* Abstract type for PME that is defined only in the routine that use them. */
55 struct nonbonded_verlet_t
;
56 struct bonded_threading_t
;
57 class DispersionCorrection
;
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.
75 #define SET_CGINFO_GID(cgi, gid) (cgi) = (((cgi) & ~255) | (gid))
76 #define GET_CGINFO_GID(cgi) ( (cgi) & 255)
77 #define SET_CGINFO_FEP(cgi) (cgi) = ((cgi) | (1<<15))
78 #define GET_CGINFO_FEP(cgi) ( (cgi) & (1<<15))
79 #define SET_CGINFO_EXCL_INTRA(cgi) (cgi) = ((cgi) | (1<<16))
80 #define GET_CGINFO_EXCL_INTRA(cgi) ( (cgi) & (1<<16))
81 #define SET_CGINFO_EXCL_INTER(cgi) (cgi) = ((cgi) | (1<<17))
82 #define GET_CGINFO_EXCL_INTER(cgi) ( (cgi) & (1<<17))
83 #define SET_CGINFO_SOLOPT(cgi, opt) (cgi) = (((cgi) & ~(3<<18)) | ((opt)<<18))
84 #define GET_CGINFO_SOLOPT(cgi) (((cgi)>>18) & 3)
85 #define SET_CGINFO_CONSTR(cgi) (cgi) = ((cgi) | (1<<20))
86 #define GET_CGINFO_CONSTR(cgi) ( (cgi) & (1<<20))
87 #define SET_CGINFO_SETTLE(cgi) (cgi) = ((cgi) | (1<<21))
88 #define GET_CGINFO_SETTLE(cgi) ( (cgi) & (1<<21))
89 /* This bit is only used with bBondComm in the domain decomposition */
90 #define SET_CGINFO_BOND_INTER(cgi) (cgi) = ((cgi) | (1<<22))
91 #define GET_CGINFO_BOND_INTER(cgi) ( (cgi) & (1<<22))
92 #define SET_CGINFO_HAS_VDW(cgi) (cgi) = ((cgi) | (1<<23))
93 #define GET_CGINFO_HAS_VDW(cgi) ( (cgi) & (1<<23))
94 #define SET_CGINFO_HAS_Q(cgi) (cgi) = ((cgi) | (1<<24))
95 #define GET_CGINFO_HAS_Q(cgi) ( (cgi) & (1<<24))
96 #define SET_CGINFO_NATOMS(cgi, opt) (cgi) = (((cgi) & ~(63<<25)) | ((opt)<<25))
97 #define GET_CGINFO_NATOMS(cgi) (((cgi)>>25) & 63)
100 /* Value to be used in mdrun for an infinite cut-off.
101 * Since we need to compare with the cut-off squared,
102 * this value should be slighlty smaller than sqrt(GMX_FLOAT_MAX).
104 #define GMX_CUTOFF_INF 1E+18
106 /* enums for the neighborlist type */
108 enbvdwNONE
, enbvdwLJ
, enbvdwBHAM
, enbvdwTAB
, enbvdwNR
120 /* Forward declaration of type for managing Ewald tables */
121 struct gmx_ewald_tab_t
;
123 struct ewald_corr_thread_t
;
125 struct t_forcerec
{ // NOLINT (clang-analyzer-optin.performance.Padding)
126 struct interaction_const_t
*ic
= nullptr;
130 //! Tells whether atoms inside a molecule can be in different periodic images,
131 // i.e. whether we need to take into account PBC when computing distances inside molecules.
132 // This determines whether PBC must be considered for e.g. bonded interactions.
133 gmx_bool bMolPBC
= FALSE
;
135 rvec posres_com
= { 0 };
136 rvec posres_comB
= { 0 };
138 gmx_bool use_simd_kernels
= FALSE
;
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
= 0;
150 int nbkernel_vdw_interaction
= 0;
151 int nbkernel_elec_modifier
= 0;
152 int nbkernel_vdw_modifier
= 0;
155 * Infinite cut-off's will be GMX_CUTOFF_INF (unlike in t_inputrec: 0).
159 /* Charge sum and dipole for topology A/B ([0]/[1]) for Ewald corrections */
160 double qsum
[2] = { 0 };
161 double q2sum
[2] = { 0 };
162 double c6sum
[2] = { 0 };
163 rvec mu_tot
[2] = { { 0 } };
165 /* Dispersion correction stuff */
166 std::unique_ptr
<DispersionCorrection
> dispersionCorrection
;
172 gmx_bool bcoultab
= FALSE
;
173 gmx_bool bvdwtab
= FALSE
;
175 t_forcetable
*pairsTable
= nullptr; /* for 1-4 interactions, [pairs] and [pairs_nb] */
179 real sc_alphavdw
= 0;
180 real sc_alphacoul
= 0;
183 real sc_sigma6_def
= 0;
184 real sc_sigma6_min
= 0;
189 /* solvent_opt contains the enum for the most common solvent
190 * in the system, which will be optimized.
191 * It can be set to esolNO to disable all water optimization */
194 gmx_bool bGrid
= FALSE
;
195 gmx_bool bExcl_IntraCGAll_InterCGNone
= FALSE
;
196 struct cginfo_mb_t
*cginfo_mb
= nullptr;
197 std::vector
<int> cginfo
;
198 rvec
*shift_vec
= nullptr;
200 int cutoff_scheme
= 0; /* group- or Verlet-style cutoff */
201 gmx_bool bNonbonded
= FALSE
; /* true if nonbonded calculations are *not* turned off */
203 /* The Nbnxm Verlet non-bonded machinery */
204 std::unique_ptr
<nonbonded_verlet_t
> nbv
;
206 /* The wall tables (if used) */
208 t_forcetable
***wall_tab
= nullptr;
210 /* The number of charge groups participating in do_force_lowlevel */
212 /* The number of atoms participating in do_force_lowlevel */
213 int natoms_force
= 0;
214 /* The number of atoms participating in force and constraints */
215 int natoms_force_constr
= 0;
216 /* The allocation size of vectors of size natoms_force */
217 int nalloc_force
= 0;
219 /* Forces that should not enter into the coord x force virial summation:
220 * PPPM/PME/Ewald/posres/ForceProviders
222 /* True when we have contributions that are directly added to the virial */
223 bool haveDirectVirialContributions
= false;
224 /* Force buffer for force computation with direct virial contributions */
225 std::vector
<gmx::RVec
> forceBufferForDirectVirialContributions
;
227 /* Data for PPPM/PME/Ewald */
228 struct gmx_pme_t
*pmedata
= nullptr;
229 int ljpme_combination_rule
= 0;
231 /* PME/Ewald stuff */
232 struct gmx_ewald_tab_t
*ewald_table
= nullptr;
234 /* Shift force array for computing the virial */
235 rvec
*fshift
= nullptr;
237 /* Non bonded Parameter lists */
238 int ntype
= 0; /* Number of atom types */
239 gmx_bool bBHAM
= FALSE
;
240 real
*nbfp
= nullptr;
241 real
*ljpme_c6grid
= nullptr; /* C6-values used on grid in LJPME */
243 /* Energy group pair flags */
244 int *egp_flags
= nullptr;
246 /* Shell molecular dynamics flexible constraints */
247 real fc_stepsize
= 0;
249 /* If > 0 signals Test Particle Insertion,
250 * the value is the number of atoms of the molecule to insert
251 * Only the energy difference due to the addition of the last molecule
252 * should be calculated.
257 gmx_bool bQMMM
= FALSE
;
258 struct t_QMMMrec
*qr
= nullptr;
260 /* QM-MM neighborlists */
261 struct t_nblist
*QMMMlist
= nullptr;
263 /* Limit for printing large forces, negative is don't print */
264 real print_force
= 0;
266 /* User determined parameters, copied from the inputrec */
276 /* Pointer to struct for managing threading of bonded force calculation */
277 struct bonded_threading_t
*bondedThreading
= nullptr;
279 /* TODO: Replace the pointer by an object once we got rid of C */
280 gmx::GpuBonded
*gpuBonded
= nullptr;
282 /* Ewald correction thread local virial and energy data */
284 struct ewald_corr_thread_t
*ewc_t
= nullptr;
286 struct ForceProviders
*forceProviders
= nullptr;
289 /* Important: Starting with Gromacs-4.6, the values of c6 and c12 in the nbfp array have
290 * been scaled by 6.0 or 12.0 to save flops in the kernels. We have corrected this everywhere
291 * in the code, but beware if you are using these macros externally.
293 #define C6(nbfp, ntp, ai, aj) (nbfp)[2*((ntp)*(ai)+(aj))]
294 #define C12(nbfp, ntp, ai, aj) (nbfp)[2*((ntp)*(ai)+(aj))+1]
295 #define BHAMC(nbfp, ntp, ai, aj) (nbfp)[3*((ntp)*(ai)+(aj))]
296 #define BHAMA(nbfp, ntp, ai, aj) (nbfp)[3*((ntp)*(ai)+(aj))+1]
297 #define BHAMB(nbfp, ntp, ai, aj) (nbfp)[3*((ntp)*(ai)+(aj))+2]