Fixed precision in thermal expansion coefficient calc.
[gromacs.git] / include / pull_rotation.h
blob9b9c33046d2e6e60dc48241c2414f500c709d22a
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39 /*! \file pull_rotation.h
41 * @brief Enforced rotation of protein parts or other groups of particles.
43 * This file contains routines that are used to enforce rotational motion
44 * upon a subgroup of particles.
48 #ifndef _pull_rotation_h
49 #define _pull_rotation_h
50 #include "visibility.h"
51 #include "vec.h"
52 #include "typedefs.h"
55 #ifdef __cplusplus
56 extern "C" {
57 #endif
60 /*! \brief Initialize the enforced rotation groups.
62 * This routine does the memory allocation for various helper arrays, opens
63 * the output files etc.
65 * \param fplog General output file, normally md.log.
66 * \param ir Struct containing MD input parameters, among those
67 * also the enforced rotation parameters.
68 * \param nfile Number of entries in the fnm structure.
69 * \param fnm The filenames struct containing also the names
70 * of the rotation output files.
71 * \param cr Pointer to MPI communication data.
72 * \param x The positions of all MD particles.
73 * \param box The simulation box.
74 * \param mtop Molecular topology.
75 * \param oenv Needed to open the rotation output xvgr file.
76 * \param Flags Flags passed over from main, used to determine
77 * whether or not we are doing a rerun.
79 GMX_LIBMD_EXPORT
80 extern void init_rot(FILE *fplog, t_inputrec *ir, int nfile, const t_filenm fnm[],
81 t_commrec *cr, rvec *x, matrix box, gmx_mtop_t *mtop, const output_env_t oenv,
82 gmx_bool bVerbose, unsigned long Flags);
85 /*! \brief Make a selection of the home atoms for all enforced rotation groups.
87 * This routine is similar to dd_make_local_pull_groups, but works only with
88 * domain decomposition. It should be called at every domain decomposition.
90 * \param dd Structure containing domain decomposition data.
91 * \param rot Pointer to all the enforced rotation data.
93 extern void dd_make_local_rotation_groups(gmx_domdec_t *dd, t_rot *rot);
96 /*! \brief Calculation of the enforced rotation potential.
98 * This is the main enforced rotation module which is called during every time
99 * step. Here the rotation potential as well as the resulting forces are
100 * calculated.
102 * \param cr Pointer to MPI communication data.
103 * \param ir Struct containing MD input parameters, among those
104 * \param box Simulation box, needed to make group whole.
105 * \param x The positions of all the local particles.
106 * \param t Time.
107 * \param step The time step.
108 * \param wcycle During the potential calculation the wallcycles are
109 * counted. Later they enter the dynamic load balancing.
110 * \param bNS After domain decomposition / neighborsearching several
111 * local arrays have to be updated (masses, shifts)
113 extern void do_rotation(t_commrec *cr, t_inputrec *ir, matrix box, rvec x[], real t,
114 gmx_large_int_t step, gmx_wallcycle_t wcycle, gmx_bool bNS);
117 /*! \brief Add the enforced rotation forces to the official force array.
119 * Adds the forces from enforced rotation potential to the local forces and
120 * sums up the contributions to the rotation potential from all the nodes. Since
121 * this needs communication, this routine should be called after the SR forces
122 * have been evaluated (in order not to spoil cycle counts).
123 * This routine also outputs data to the various rotation output files (e.g.
124 * the potential, the angle of the group, torques and more).
126 * \param rot Pointer to all the enforced rotation data.
127 * \param f The local forces to which the rotational forces have
128 * to be added.
129 * \param cr Pointer to MPI communication data.
130 * \param step The time step, used for output.
131 * \param t Time, used for output.
133 extern real add_rot_forces(t_rot *rot, rvec f[], t_commrec *cr, gmx_large_int_t step, real t);
136 /*! \brief Close the enforced rotation output files.
138 * \param rot Pointer to all the enforced rotation data.
140 GMX_LIBMD_EXPORT
141 extern void finish_rot(t_rot *rot);
144 #ifdef __cplusplus
146 #endif
149 #endif