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35 /* This file is completely threadsafe - keep it that way! */
52 #include "mtop_util.h"
53 #include "gmx_omp_nthreads.h"
55 static void init_grptcstat(int ngtc
,t_grp_tcstat tcstat
[])
59 for(i
=0; (i
<ngtc
); i
++) {
61 clear_mat(tcstat
[i
].ekinh
);
62 clear_mat(tcstat
[i
].ekinh_old
);
63 clear_mat(tcstat
[i
].ekinf
);
67 static void init_grpstat(FILE *log
,
68 gmx_mtop_t
*mtop
,int ngacc
,t_grp_acc gstat
[])
71 gmx_mtop_atomloop_all_t aloop
;
76 groups
= &mtop
->groups
;
77 aloop
= gmx_mtop_atomloop_all_init(mtop
);
78 while (gmx_mtop_atomloop_all_next(aloop
,&i
,&atom
))
80 grp
= ggrpnr(groups
,egcACC
,i
);
81 if ((grp
< 0) && (grp
>= ngacc
))
83 gmx_incons("Input for acceleration groups wrong");
86 /* This will not work for integrator BD */
87 gstat
[grp
].mA
+= atom
->m
;
88 gstat
[grp
].mB
+= atom
->mB
;
93 void init_ekindata(FILE *log
,gmx_mtop_t
*mtop
,t_grpopts
*opts
,
94 gmx_ekindata_t
*ekind
)
99 fprintf(log
,"ngtc: %d, ngacc: %d, ngener: %d\n",opts
->ngtc
,opts
->ngacc
,
103 /* bNEMD tells if we should remove remove the COM velocity
104 * from the velocities during velocity scaling in T-coupling.
105 * Turn this on when we have multiple acceleration groups
106 * or one accelerated group.
108 ekind
->bNEMD
= (opts
->ngacc
> 1 || norm(opts
->acc
[0]) > 0);
110 ekind
->ngtc
= opts
->ngtc
;
111 snew(ekind
->tcstat
,opts
->ngtc
);
112 init_grptcstat(opts
->ngtc
,ekind
->tcstat
);
113 /* Set Berendsen tcoupl lambda's to 1,
114 * so runs without Berendsen coupling are not affected.
116 for(i
=0; i
<opts
->ngtc
; i
++)
118 ekind
->tcstat
[i
].lambda
= 1.0;
119 ekind
->tcstat
[i
].vscale_nhc
= 1.0;
120 ekind
->tcstat
[i
].ekinscaleh_nhc
= 1.0;
121 ekind
->tcstat
[i
].ekinscalef_nhc
= 1.0;
124 nthread
= gmx_omp_nthreads_get(emntUpdate
);
126 snew(ekind
->ekin_work_alloc
,nthread
);
127 snew(ekind
->ekin_work
,nthread
);
128 #pragma omp parallel for num_threads(nthread) schedule(static)
129 for(thread
=0; thread
<nthread
; thread
++)
131 /* Allocate 2 elements extra on both sides,
132 * so in single precision we have 2*3*3*4=72 bytes buffer
133 * on both sides to avoid cache pollution.
135 snew(ekind
->ekin_work_alloc
[thread
],ekind
->ngtc
+4);
136 ekind
->ekin_work
[thread
] = ekind
->ekin_work_alloc
[thread
] + 2;
139 ekind
->ngacc
= opts
->ngacc
;
140 snew(ekind
->grpstat
,opts
->ngacc
);
141 init_grpstat(log
,mtop
,opts
->ngacc
,ekind
->grpstat
);
144 void accumulate_u(t_commrec
*cr
,t_grpopts
*opts
,gmx_ekindata_t
*ekind
)
146 /* This routine will only be called when it's necessary */
152 for(g
=0; (g
<opts
->ngacc
); g
++)
154 add_binr(rb
,DIM
,ekind
->grpstat
[g
].u
);
158 for(g
=0; (g
<opts
->ngacc
); g
++)
160 extract_binr(rb
,DIM
*g
,DIM
,ekind
->grpstat
[g
].u
);
165 /* I don't think accumulate_ekin is used anymore? */
168 static void accumulate_ekin(t_commrec
*cr
,t_grpopts
*opts
,
169 gmx_ekindata_t
*ekind
)
175 for(g
=0; (g
<opts
->ngtc
); g
++)
177 gmx_sum(DIM
*DIM
,ekind
->tcstat
[g
].ekinf
[0],cr
);
183 void update_ekindata(int start
,int homenr
,gmx_ekindata_t
*ekind
,
184 t_grpopts
*opts
,rvec v
[],t_mdatoms
*md
,real lambda
)
189 /* calculate mean velocities at whole timestep */
190 for(g
=0; (g
<opts
->ngtc
); g
++) {
191 ekind
->tcstat
[g
].T
= 0;
195 for (g
=0; (g
<opts
->ngacc
); g
++)
196 clear_rvec(ekind
->grpstat
[g
].u
);
199 for(n
=start
; (n
<start
+homenr
); n
++) {
202 for(d
=0; (d
<DIM
);d
++) {
203 mv
= md
->massT
[n
]*v
[n
][d
];
204 ekind
->grpstat
[g
].u
[d
] += mv
;
208 for (g
=0; (g
< opts
->ngacc
); g
++) {
209 for(d
=0; (d
<DIM
);d
++) {
210 ekind
->grpstat
[g
].u
[d
] /=
211 (1-lambda
)*ekind
->grpstat
[g
].mA
+ lambda
*ekind
->grpstat
[g
].mB
;
217 real
sum_ekin(t_grpopts
*opts
,gmx_ekindata_t
*ekind
,real
*dekindlambda
,
218 gmx_bool bEkinAveVel
, gmx_bool bSaveEkinOld
, gmx_bool bScaleEkin
)
222 t_grp_tcstat
*tcstat
;
231 clear_mat(ekind
->ekin
);
233 for(i
=0; (i
<ngtc
); i
++)
237 tcstat
= &ekind
->tcstat
[i
];
238 /* Sometimes a group does not have degrees of freedom, e.g.
239 * when it consists of shells and virtual sites, then we just
240 * set the temperatue to 0 and also neglect the kinetic
241 * energy, which should be zero anyway.
249 /* in this case, kinetic energy is from the current velocities already */
250 msmul(tcstat
->ekinf
,tcstat
->ekinscalef_nhc
,tcstat
->ekinf
);
256 /* Calculate the full step Ekin as the average of the half steps */
257 for(j
=0; (j
<DIM
); j
++)
259 for(m
=0; (m
<DIM
); m
++)
261 tcstat
->ekinf
[j
][m
] =
262 0.5*(tcstat
->ekinh
[j
][m
]*tcstat
->ekinscaleh_nhc
+ tcstat
->ekinh_old
[j
][m
]);
266 m_add(tcstat
->ekinf
,ekind
->ekin
,ekind
->ekin
);
268 tcstat
->Th
= calc_temp(trace(tcstat
->ekinh
),nd
);
269 tcstat
->T
= calc_temp(trace(tcstat
->ekinf
),nd
);
271 /* after the scaling factors have been multiplied in, we can remove them */
274 tcstat
->ekinscalef_nhc
= 1.0;
278 tcstat
->ekinscaleh_nhc
= 1.0;
295 *dekindlambda
= 0.5*(ekind
->dekindl
+ ekind
->dekindl_old
);