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/*
* $Id$
*
* This source code is part of
*
* G R O M A C S
*
* GROningen MAchine for Chemical Simulations
*
* VERSION 3.2.0
* Written by David van der Spoel, Erik Lindahl, Berk Hess, and others.
* Copyright (c) 1991-2000, University of Groningen, The Netherlands.
* Copyright (c) 2001-2004, The GROMACS development team,
* check out http://www.gromacs.org for more information.
* This program is free software; you can redistribute it and/or
* modify it under the terms of the GNU General Public License
* as published by the Free Software Foundation; either version 2
* of the License, or (at your option) any later version.
*
* If you want to redistribute modifications, please consider that
* scientific software is very special. Version control is crucial -
* bugs must be traceable. We will be happy to consider code for
* inclusion in the official distribution, but derived work must not
* be called official GROMACS. Details are found in the README & COPYING
* files - if they are missing, get the official version at www.gromacs.org.
*
* To help us fund GROMACS development, we humbly ask that you cite
* the papers on the package - you can find them in the top README file.
*
* For more info, check our website at http://www.gromacs.org
*
* And Hey:
* GRoups of Organic Molecules in ACtion for Science
*/
#ifdef HAVE_CONFIG_H
#include <config.h>
#endif
#include "ns.h"
#include "qmmmrec.h"
/* Abstract type for PME that is defined only in the routine that use them. */
typedef struct gmx_pme *gmx_pme_t;
typedef struct {
real r; /* range of the table */
int n; /* n+1 is the number of points */
real scale; /* distance between two points */
real scale_exp; /* distance for exponential Buckingham table */
real *tab; /* the actual tables, per point there are 4 numbers for
* Coulomb, dispersion and repulsion (in total 12 numbers)
*/
} t_forcetable;
typedef struct {
t_forcetable tab;
/* We duplicate tables for cache optimization purposes */
real *coultab; /* Coul only */
real *vdwtab; /* Vdw only */
/* The actual neighbor lists, short and long range, see enum above
* for definition of neighborlist indices.
*/
t_nblist nlist_sr[eNL_NR];
t_nblist nlist_lr[eNL_NR];
} t_nblists;
/* macros for the cginfo data in forcerec */
#define SET_CGINFO_GID(cgi,gid) (cgi) = (((cgi) & ~65535) | (gid) )
#define GET_CGINFO_GID(cgi) ( (cgi) & 65535)
#define SET_CGINFO_EXCL_INTRA(cgi) (cgi) = ((cgi) | (1<<16))
#define GET_CGINFO_EXCL_INTRA(cgi) ( (cgi) & (1<<16))
#define SET_CGINFO_EXCL_INTER(cgi) (cgi) = ((cgi) | (1<<17))
#define GET_CGINFO_EXCL_INTER(cgi) ( (cgi) & (1<<17))
#define SET_CGINFO_SOLOPT(cgi,opt) (cgi) = (((cgi) & ~(15<<18)) | ((opt)<<18))
#define GET_CGINFO_SOLOPT(cgi) (((cgi)>>18) & 15)
/* This bit is only used with bBondComm in the domain decomposition */
#define SET_CGINFO_BOND_INTER(cgi) (cgi) = ((cgi) | (1<<22))
#define GET_CGINFO_BOND_INTER(cgi) ( (cgi) & (1<<22))
enum { egCOULSR, egLJSR, egBHAMSR, egCOULLR, egLJLR, egBHAMLR,
egCOUL14, egLJ14, egNR };
typedef struct {
int nener; /* The number of energy group pairs */
real *ener[egNR]; /* Energy terms for each pair of groups */
} gmx_grppairener_t;
typedef struct {
real term[F_NRE]; /* The energies for all different interaction types */
gmx_grppairener_t grpp;
real dvdl_lr;
} gmx_enerdata_t;
typedef struct {
/* Domain Decomposition */
bool bDomDec;
/* PBC stuff */
int ePBC;
bool bMolPBC;
int rc_scaling;
rvec posres_com;
rvec posres_comB;
/* Cut-Off stuff */
real rlist,rlistlong;
/* Dielectric constant resp. multiplication factor for charges */
real zsquare,temp;
real epsilon_r,epsilon_rf,epsfac;
/* Constants for reaction fields */
real kappa,k_rf,c_rf;
/* Charge sum for topology A/B ([0]/[1]) for Ewald corrections */
double qsum[2];
/* The shift of the shift or user potentials */
real enershiftsix;
real enershifttwelve;
/* Integrated differces for energy and virial with cut-off functions */
real enerdiffsix;
real enerdifftwelve;
real virdiffsix;
real virdifftwelve;
/* Constant for long range dispersion correction (average dispersion)
* for topology A/B ([0]/[1]) */
real avcsix[2];
/* Constant for long range repulsion term. Relative difference of about
* 0.1 percent with 0.8 nm cutoffs. But hey, it's cheap anyway...
*/
real avctwelve[2];
/* Fudge factors */
real fudgeQQ;
/* Table stuff */
bool bcoultab;
bool bvdwtab;
/* The normal tables are in the nblists struct(s) below */
t_forcetable tab14; /* for 1-4 interactions only */
/* PPPM & Shifting stuff */
real rcoulomb_switch,rcoulomb;
real *phi;
/* VdW stuff */
real rvdw_switch,rvdw;
real bham_b_max;
/* Free energy ? */
int efep;
real sc_alpha;
int sc_power;
real sc_sigma6;
bool bSepDVDL;
/* NS Stuff */
int eeltype;
int vdwtype;
int cg0,hcg;
/* solvent_opt contains the enum for the most common solvent
* in the system, which will be optimized.
* It can be set to esolNO to disable all water optimization */
int solvent_opt;
int nWatMol;
bool bGrid;
int *cginfo_global;
int *cginfo;
rvec *cg_cm;
int cg_nalloc;
rvec *shift_vec;
/* The neighborlists including tables */
int nnblists;
int *gid2nblists;
t_nblists *nblists;
/* The wall tables (if used) */
int nwall;
t_forcetable **wall_tab;
/* This mask array of length nn determines whether or not this bit of the
* neighbourlists should be computed. Usually all these are true of course,
* but not when shells are used. During minimisation all the forces that
* include shells are done, then after minimsation is converged the remaining
* forces are computed.
*/
/* bool *bMask; */
/* Twin Range stuff. */
bool bTwinRange;
int nlr;
int f_twin_n;
int f_twin_nalloc;
rvec *f_twin;
rvec *fshift_twin;
/* Forces that should not enter into the virial summation:
* PPPM/PME/Ewald/posres
*/
bool bF_NoVirSum;
int f_novirsum_n;
int f_novirsum_nalloc;
rvec *f_novirsum;
/* Long-range forces and virial for PPPM/PME/Ewald */
gmx_pme_t pmedata;
tensor vir_el_recip;
/* PME/Ewald stuff */
bool bEwald;
real ewaldcoeff;
/* Virial Stuff */
rvec *fshift;
rvec vir_diag_posres;
dvec vir_wall_z;
/* Non bonded Parameter lists */
int ntype; /* Number of atom types */
bool bBHAM;
real *nbfp;
/* Energy group pair flags */
int *egp_flags;
/* xmdrun flexible constraints */
real fc_stepsize;
/* Generalized born stuff */
/* VdW radius for each atomtype (dim is thus ntype) */
real *atype_radius;
/* Effective radius (derived from effective volume) for each type */
real *atype_vol;
/* Implicit solvent - surface tension for each atomtype */
real *atype_surftens;
/* If > 0 signals Test Particle Insertion,
* the value is the number of atoms of the molecule to insert
* Only the energy difference due to the addition of the last molecule
* should be calculated.
*/
bool n_tpi;
/* Neighbor searching stuff */
gmx_ns_t ns;
/* QMMM stuff */
bool bQMMM;
t_QMMMrec *qr;
/* QM-MM neighborlists */
t_nblist QMMMlist_sr;
t_nblist QMMMlist_lr; /* not needed, one QMMM list suffices */
/* Limit for printing large forces, negative is don't print */
real print_force;
/* User determined parameters, copied from the inputrec */
int userint1;
int userint2;
int userint3;
int userint4;
real userreal1;
real userreal2;
real userreal3;
real userreal4;
} t_forcerec;
#define C6(nbfp,ntp,ai,aj) (nbfp)[2*((ntp)*(ai)+(aj))]
#define C12(nbfp,ntp,ai,aj) (nbfp)[2*((ntp)*(ai)+(aj))+1]
#define BHAMC(nbfp,ntp,ai,aj) (nbfp)[3*((ntp)*(ai)+(aj))]
#define BHAMA(nbfp,ntp,ai,aj) (nbfp)[3*((ntp)*(ai)+(aj))+1]
#define BHAMB(nbfp,ntp,ai,aj) (nbfp)[3*((ntp)*(ai)+(aj))+2]
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