本文整理汇总了C++中parse_common_args函数的典型用法代码示例。如果您正苦于以下问题:C++ parse_common_args函数的具体用法?C++ parse_common_args怎么用?C++ parse_common_args使用的例子?那么恭喜您, 这里精选的函数代码示例或许可以为您提供帮助。
在下文中一共展示了parse_common_args函数的20个代码示例,这些例子默认根据受欢迎程度排序。您可以为喜欢或者感觉有用的代码点赞,您的评价将有助于我们的系统推荐出更棒的C++代码示例。
示例1: gmx_make_ndx
int gmx_make_ndx(int argc, char *argv[])
{
const char *desc[] = {
"Index groups are necessary for almost every GROMACS program.",
"All these programs can generate default index groups. You ONLY",
"have to use [THISMODULE] when you need SPECIAL index groups.",
"There is a default index group for the whole system, 9 default",
"index groups for proteins, and a default index group",
"is generated for every other residue name.",
"",
"When no index file is supplied, also [THISMODULE] will generate the",
"default groups.",
"With the index editor you can select on atom, residue and chain names",
"and numbers.",
"When a run input file is supplied you can also select on atom type.",
"You can use boolean operations, you can split groups",
"into chains, residues or atoms. You can delete and rename groups.",
"Type 'h' in the editor for more details.",
"",
"The atom numbering in the editor and the index file starts at 1.",
"",
"The [TT]-twin[tt] switch duplicates all index groups with an offset of",
"[TT]-natoms[tt], which is useful for Computational Electrophysiology",
"double-layer membrane setups.",
"",
"See also [gmx-select] [TT]-on[tt], which provides an alternative way",
"for constructing index groups. It covers nearly all of [THISMODULE]",
"functionality, and in many cases much more."
};
static int natoms = 0;
static gmx_bool bVerbose = FALSE;
static gmx_bool bDuplicate = FALSE;
t_pargs pa[] = {
{ "-natoms", FALSE, etINT, {&natoms},
"set number of atoms (default: read from coordinate or index file)" },
{ "-twin", FALSE, etBOOL, {&bDuplicate},
"Duplicate all index groups with an offset of -natoms" },
{ "-verbose", FALSE, etBOOL, {&bVerbose},
"HIDDENVerbose output" }
};
#define NPA asize(pa)
gmx_output_env_t *oenv;
const char *stxfile;
const char *ndxoutfile;
gmx_bool bNatoms;
int j;
t_atoms *atoms;
rvec *x, *v;
int ePBC;
matrix box;
t_blocka *block, *block2;
char **gnames, **gnames2;
t_filenm fnm[] = {
{ efSTX, "-f", nullptr, ffOPTRD },
{ efNDX, "-n", nullptr, ffOPTRDMULT },
{ efNDX, "-o", nullptr, ffWRITE }
};
#define NFILE asize(fnm)
if (!parse_common_args(&argc, argv, 0, NFILE, fnm, NPA, pa, asize(desc), desc,
0, nullptr, &oenv))
{
return 0;
}
stxfile = ftp2fn_null(efSTX, NFILE, fnm);
gmx::ArrayRef<const std::string> ndxInFiles = opt2fnsIfOptionSet("-n", NFILE, fnm);
ndxoutfile = opt2fn("-o", NFILE, fnm);
bNatoms = opt2parg_bSet("-natoms", NPA, pa);
if (!stxfile && ndxInFiles.empty())
{
gmx_fatal(FARGS, "No input files (structure or index)");
}
if (stxfile)
{
t_topology *top;
snew(top, 1);
fprintf(stderr, "\nReading structure file\n");
read_tps_conf(stxfile, top, &ePBC, &x, &v, box, FALSE);
atoms = &top->atoms;
if (atoms->pdbinfo == nullptr)
{
snew(atoms->pdbinfo, atoms->nr);
}
natoms = atoms->nr;
bNatoms = TRUE;
}
else
{
atoms = nullptr;
x = nullptr;
}
/* read input file(s) */
block = new_blocka();
gnames = nullptr;
//.........这里部分代码省略.........
开发者ID:friforever,项目名称:gromacs,代码行数:101,代码来源:gmx_make_ndx.cpp
示例2: gmx_spatial
//.........这里部分代码省略.........
t_trxframe fr;
rvec *xtop;
matrix box, box_pbc;
t_trxstatus *status;
int flags = TRX_READ_X;
t_pbc pbc;
t_atoms *atoms;
int natoms;
char *grpnm, *grpnmp;
int *index, *indexp;
int i, nidx, nidxp;
int v;
int j, k;
int ***bin = NULL;
int nbin[3];
FILE *flp;
int x, y, z, minx, miny, minz, maxx, maxy, maxz;
int numfr, numcu;
int tot, maxval, minval;
double norm;
gmx_output_env_t *oenv;
gmx_rmpbc_t gpbc = NULL;
t_filenm fnm[] = {
{ efTPS, NULL, NULL, ffREAD }, /* this is for the topology */
{ efTRX, "-f", NULL, ffREAD }, /* and this for the trajectory */
{ efNDX, NULL, NULL, ffOPTRD }
};
#define NFILE asize(fnm)
/* This is the routine responsible for adding default options,
* calling the X/motif interface, etc. */
if (!parse_common_args(&argc, argv, PCA_CAN_TIME | PCA_CAN_VIEW,
NFILE, fnm, asize(pa), pa, asize(desc), desc, asize(bugs), bugs, &oenv))
{
return 0;
}
read_tps_conf(ftp2fn(efTPS, NFILE, fnm), &top, &ePBC, &xtop, NULL, box, TRUE);
sfree(xtop);
atoms = &(top.atoms);
printf("Select group to generate SDF:\n");
get_index(atoms, ftp2fn_null(efNDX, NFILE, fnm), 1, &nidx, &index, &grpnm);
printf("Select group to output coords (e.g. solute):\n");
get_index(atoms, ftp2fn_null(efNDX, NFILE, fnm), 1, &nidxp, &indexp, &grpnmp);
/* The first time we read data is a little special */
natoms = read_first_frame(oenv, &status, ftp2fn(efTRX, NFILE, fnm), &fr, flags);
/* Memory Allocation */
MINBIN[XX] = MAXBIN[XX] = fr.x[0][XX];
MINBIN[YY] = MAXBIN[YY] = fr.x[0][YY];
MINBIN[ZZ] = MAXBIN[ZZ] = fr.x[0][ZZ];
for (i = 1; i < top.atoms.nr; ++i)
{
if (fr.x[i][XX] < MINBIN[XX])
{
MINBIN[XX] = fr.x[i][XX];
}
if (fr.x[i][XX] > MAXBIN[XX])
{
MAXBIN[XX] = fr.x[i][XX];
}
if (fr.x[i][YY] < MINBIN[YY])
开发者ID:pjohansson,项目名称:gromacs,代码行数:67,代码来源:gmx_spatial.cpp
示例3: gmx_pme_error
int gmx_pme_error(int argc,char *argv[])
{
const char *desc[] = {
"g_pme_error estimates the error of the electrostatic forces",
"if using the SPME algorithm. The flag [TT]-tune[tt] will determine",
"the splitting parameter such that the error is equally",
"distributed over the real and reciprocal space part.",
"As a part of the error stems from self interaction of the particles "
"and is computationally very demanding a good a approximation is possible",
"if just a fraction of the particles is used to calculate the average",
"of this error by using the flag [TT]-self[tt].[PAR]",
};
int repeats=2;
real fs=0.0; /* 0 indicates: not set by the user */
real user_beta=-1.0;
real fracself=-1.0;
t_perf **perfdata;
t_inputinfo info;
t_state state; /* The state from the tpr input file */
gmx_mtop_t mtop; /* The topology from the tpr input file */
t_inputrec *ir=NULL; /* The inputrec from the tpr file */
FILE *fp=NULL;
t_commrec *cr;
unsigned long PCA_Flags;
gmx_bool bTUNE=FALSE;
static t_filenm fnm[] = {
/* g_tune_pme */
{ efTPX, "-s", NULL, ffREAD },
{ efOUT, "-o", "error", ffWRITE },
{ efTPX, "-so", "tuned", ffOPTWR }
};
output_env_t oenv=NULL;
t_pargs pa[] = {
/***********************/
/* g_tune_pme options: */
/***********************/
{ "-beta", FALSE, etREAL, {&user_beta},
"If positive, overwrite ewald_beta from tpr file with this value" },
{ "-tune", FALSE, etBOOL, {&bTUNE},
"If flag is set the splitting parameter will be tuned to distribute the error equally in real and rec. space" },
{ "-self", FALSE, etREAL, {&fracself},
"If positive, determine selfinteraction error just over this fraction (default=1.0)" }
};
#define NFILE asize(fnm)
cr = init_par(&argc,&argv);
if (MASTER(cr))
CopyRight(stderr,argv[0]);
PCA_Flags = PCA_NOEXIT_ON_ARGS;
PCA_Flags |= (MASTER(cr) ? 0 : PCA_QUIET);
parse_common_args(&argc,argv,PCA_Flags,
NFILE,fnm,asize(pa),pa,asize(desc),desc,
0,NULL,&oenv);
if (!bTUNE)
bTUNE = opt2bSet("-so",NFILE,fnm);
info.n_entries = 1;
/* Allocate memory for the inputinfo struct: */
create_info(&info);
info.fourier_sp[0] = fs;
/* Read in the tpr file and open logfile for reading */
if (MASTER(cr))
{
snew(ir,1);
read_tpr_file(opt2fn("-s",NFILE,fnm), &info, &state, &mtop, ir, user_beta,fracself);
fp=fopen(opt2fn("-o",NFILE,fnm),"w");
}
/* Check consistency if the user provided fourierspacing */
if (fs > 0 && MASTER(cr))
{
/* Recalculate the grid dimensions using fourierspacing from user input */
info.nkx[0] = 0;
info.nky[0] = 0;
info.nkz[0] = 0;
calc_grid(stdout,state.box,info.fourier_sp[0],&(info.nkx[0]),&(info.nky[0]),&(info.nkz[0]));
if ( (ir->nkx != info.nkx[0]) || (ir->nky != info.nky[0]) || (ir->nkz != info.nkz[0]) )
gmx_fatal(FARGS, "Wrong fourierspacing %f nm, input file grid = %d x %d x %d, computed grid = %d x %d x %d",
fs,ir->nkx,ir->nky,ir->nkz,info.nkx[0],info.nky[0],info.nkz[0]);
}
/* Estimate (S)PME force error */
//.........这里部分代码省略.........
开发者ID:andersx,项目名称:gmx-debug,代码行数:101,代码来源:gmx_pme_error.c
示例4: gmx_sorient
int gmx_sorient(int argc, char *argv[])
{
t_topology top;
int ePBC = -1;
t_trxstatus *status;
int natoms;
real t;
rvec *xtop, *x;
matrix box;
FILE *fp;
int i, p, sa0, sa1, sa2, n, ntot, nf, m, *hist1, *hist2, *histn, nbin1, nbin2, nrbin;
real *histi1, *histi2, invbw, invrbw;
double sum1, sum2;
int *isize, nrefgrp, nrefat;
int **index;
char **grpname;
real inp, outp, nav, normfac, rmin2, rmax2, rcut, rcut2, r2, r;
real c1, c2;
char str[STRLEN];
gmx_bool bTPS;
rvec xref, dx, dxh1, dxh2, outer;
gmx_rmpbc_t gpbc = NULL;
t_pbc pbc;
const char *legr[] = {
"<cos(\\8q\\4\\s1\\N)>",
"<3cos\\S2\\N(\\8q\\4\\s2\\N)-1>"
};
const char *legc[] = {
"cos(\\8q\\4\\s1\\N)",
"3cos\\S2\\N(\\8q\\4\\s2\\N)-1"
};
const char *desc[] = {
"[THISMODULE] analyzes solvent orientation around solutes.",
"It calculates two angles between the vector from one or more",
"reference positions to the first atom of each solvent molecule:",
"",
" * [GRK]theta[grk][SUB]1[sub]: the angle with the vector from the first atom of the solvent",
" molecule to the midpoint between atoms 2 and 3.",
" * [GRK]theta[grk][SUB]2[sub]: the angle with the normal of the solvent plane, defined by the",
" same three atoms, or, when the option [TT]-v23[tt] is set, ",
" the angle with the vector between atoms 2 and 3.",
"",
"The reference can be a set of atoms or",
"the center of mass of a set of atoms. The group of solvent atoms should",
"consist of 3 atoms per solvent molecule.",
"Only solvent molecules between [TT]-rmin[tt] and [TT]-rmax[tt] are",
"considered for [TT]-o[tt] and [TT]-no[tt] each frame.[PAR]",
"[TT]-o[tt]: distribtion of [MATH][COS][GRK]theta[grk][SUB]1[sub][cos][math] for rmin<=r<=rmax.[PAR]",
"[TT]-no[tt]: distribution of [MATH][COS][GRK]theta[grk][SUB]2[sub][cos][math] for rmin<=r<=rmax.[PAR]",
"[TT]-ro[tt]: [MATH][CHEVRON][COS][GRK]theta[grk][SUB]1[sub][cos][chevron][math] and [MATH][CHEVRON]3[COS]^2[GRK]theta[grk][SUB]2[sub][cos]-1[chevron][math] as a function of the",
"distance.[PAR]",
"[TT]-co[tt]: the sum over all solvent molecules within distance r",
"of [MATH][COS][GRK]theta[grk][SUB]1[sub][cos][math] and [MATH]3[COS]^2([GRK]theta[grk][SUB]2[sub])-1[cos][math] as a function of r.[PAR]",
"[TT]-rc[tt]: the distribution of the solvent molecules as a function of r"
};
gmx_output_env_t *oenv;
static gmx_bool bCom = FALSE, bVec23 = FALSE, bPBC = FALSE;
static real rmin = 0.0, rmax = 0.5, binwidth = 0.02, rbinw = 0.02;
t_pargs pa[] = {
{ "-com", FALSE, etBOOL, {&bCom},
"Use the center of mass as the reference postion"
},
{ "-v23", FALSE, etBOOL, {&bVec23},
"Use the vector between atoms 2 and 3"
},
{ "-rmin", FALSE, etREAL, {&rmin}, "Minimum distance (nm)" },
{ "-rmax", FALSE, etREAL, {&rmax}, "Maximum distance (nm)" },
{ "-cbin", FALSE, etREAL, {&binwidth}, "Binwidth for the cosine" },
{ "-rbin", FALSE, etREAL, {&rbinw}, "Binwidth for r (nm)" },
{ "-pbc", FALSE, etBOOL, {&bPBC}, "Check PBC for the center of mass calculation. Only necessary when your reference group consists of several molecules." }
};
t_filenm fnm[] = {
{ efTRX, NULL, NULL, ffREAD },
{ efTPS, NULL, NULL, ffREAD },
{ efNDX, NULL, NULL, ffOPTRD },
{ efXVG, NULL, "sori", ffWRITE },
{ efXVG, "-no", "snor", ffWRITE },
{ efXVG, "-ro", "sord", ffWRITE },
{ efXVG, "-co", "scum", ffWRITE },
{ efXVG, "-rc", "scount", ffWRITE }
};
#define NFILE asize(fnm)
if (!parse_common_args(&argc, argv, PCA_CAN_TIME | PCA_CAN_VIEW,
NFILE, fnm, asize(pa), pa, asize(desc), desc, 0, NULL, &oenv))
{
return 0;
}
bTPS = (opt2bSet("-s", NFILE, fnm) || !opt2bSet("-n", NFILE, fnm) || bCom);
if (bTPS)
{
read_tps_conf(ftp2fn(efTPS, NFILE, fnm), &top, &ePBC, &xtop, NULL, box,
bCom);
}
//.........这里部分代码省略.........
开发者ID:pjohansson,项目名称:gromacs,代码行数:101,代码来源:gmx_sorient.cpp
示例5: gmx_dielectric
int gmx_dielectric(int argc, char *argv[])
{
const char *desc[] = {
"[THISMODULE] calculates frequency dependent dielectric constants",
"from the autocorrelation function of the total dipole moment in",
"your simulation. This ACF can be generated by [gmx-dipoles].",
"The functional forms of the available functions are:[PAR]",
"One parameter: y = [EXP]-a[SUB]1[sub] x[exp],[BR]",
"Two parameters: y = a[SUB]2[sub] [EXP]-a[SUB]1[sub] x[exp],[BR]",
"Three parameters: y = a[SUB]2[sub] [EXP]-a[SUB]1[sub] x[exp] + (1 - a[SUB]2[sub]) [EXP]-a[SUB]3[sub] x[exp].[BR]",
"Start values for the fit procedure can be given on the command line.",
"It is also possible to fix parameters at their start value, use [TT]-fix[tt]",
"with the number of the parameter you want to fix.",
"[PAR]",
"Three output files are generated, the first contains the ACF,",
"an exponential fit to it with 1, 2 or 3 parameters, and the",
"numerical derivative of the combination data/fit.",
"The second file contains the real and imaginary parts of the",
"frequency-dependent dielectric constant, the last gives a plot",
"known as the Cole-Cole plot, in which the imaginary",
"component is plotted as a function of the real component.",
"For a pure exponential relaxation (Debye relaxation) the latter",
"plot should be one half of a circle."
};
t_filenm fnm[] = {
{ efXVG, "-f", "dipcorr", ffREAD },
{ efXVG, "-d", "deriv", ffWRITE },
{ efXVG, "-o", "epsw", ffWRITE },
{ efXVG, "-c", "cole", ffWRITE }
};
#define NFILE asize(fnm)
output_env_t oenv;
int i, j, nx, ny, nxtail, eFitFn, nfitparm;
real dt, integral, fitintegral, fac, rffac;
double *fitparms;
double **yd;
real **y;
const char *legend[] = { "Correlation", "Std. Dev.", "Fit", "Combined", "Derivative" };
static int fix = 0, bX = 1, nsmooth = 3;
static real tendInt = 5.0, tbegin = 5.0, tend = 500.0;
static real A = 0.5, tau1 = 10.0, tau2 = 1.0, eps0 = 80, epsRF = 78.5, tail = 500.0;
real lambda;
t_pargs pa[] = {
{ "-x1", FALSE, etBOOL, {&bX},
"use first column as [IT]x[it]-axis rather than first data set" },
{ "-eint", FALSE, etREAL, {&tendInt},
"Time to end the integration of the data and start to use the fit"},
{ "-bfit", FALSE, etREAL, {&tbegin},
"Begin time of fit" },
{ "-efit", FALSE, etREAL, {&tend},
"End time of fit" },
{ "-tail", FALSE, etREAL, {&tail},
"Length of function including data and tail from fit" },
{ "-A", FALSE, etREAL, {&A},
"Start value for fit parameter A" },
{ "-tau1", FALSE, etREAL, {&tau1},
"Start value for fit parameter [GRK]tau[grk]1" },
{ "-tau2", FALSE, etREAL, {&tau2},
"Start value for fit parameter [GRK]tau[grk]2" },
{ "-eps0", FALSE, etREAL, {&eps0},
"[GRK]epsilon[grk]0 of your liquid" },
{ "-epsRF", FALSE, etREAL, {&epsRF},
"[GRK]epsilon[grk] of the reaction field used in your simulation. A value of 0 means infinity." },
{ "-fix", FALSE, etINT, {&fix},
"Fix parameters at their start values, A (2), tau1 (1), or tau2 (4)" },
{ "-ffn", FALSE, etENUM, {s_ffn},
"Fit function" },
{ "-nsmooth", FALSE, etINT, {&nsmooth},
"Number of points for smoothing" }
};
if (!parse_common_args(&argc, argv, PCA_CAN_TIME | PCA_CAN_VIEW,
NFILE, fnm, asize(pa), pa, asize(desc), desc, 0, NULL, &oenv))
{
return 0;
}
please_cite(stdout, "Spoel98a");
printf("WARNING: non-polarizable models can never yield an infinite\n"
"dielectric constant that is different from 1. This is incorrect\n"
"in the reference given above (Spoel98a).\n\n");
nx = read_xvg(opt2fn("-f", NFILE, fnm), &yd, &ny);
dt = yd[0][1] - yd[0][0];
nxtail = min(tail/dt, nx);
printf("Read data set containing %d colums and %d rows\n", ny, nx);
printf("Assuming (from data) that timestep is %g, nxtail = %d\n",
dt, nxtail);
snew(y, 6);
for (i = 0; (i < ny); i++)
{
snew(y[i], max(nx, nxtail));
}
for (i = 0; (i < nx); i++)
{
y[0][i] = yd[0][i];
for (j = 1; (j < ny); j++)
{
y[j][i] = yd[j][i];
//.........这里部分代码省略.........
开发者ID:schlaicha,项目名称:gromacs,代码行数:101,代码来源:gmx_dielectric.c
示例6: gmx_mindist
int gmx_mindist(int argc, char *argv[])
{
const char *desc[] = {
"[THISMODULE] computes the distance between one group and a number of",
"other groups. Both the minimum distance",
"(between any pair of atoms from the respective groups)",
"and the number of contacts within a given",
"distance are written to two separate output files.",
"With the [TT]-group[tt] option a contact of an atom in another group",
"with multiple atoms in the first group is counted as one contact",
"instead of as multiple contacts.",
"With [TT]-or[tt], minimum distances to each residue in the first",
"group are determined and plotted as a function of residue number.[PAR]",
"With option [TT]-pi[tt] the minimum distance of a group to its",
"periodic image is plotted. This is useful for checking if a protein",
"has seen its periodic image during a simulation. Only one shift in",
"each direction is considered, giving a total of 26 shifts.",
"It also plots the maximum distance within the group and the lengths",
"of the three box vectors.[PAR]",
"Also [gmx-distance] calculates distances."
};
const char *bugs[] = {
"The [TT]-pi[tt] option is very slow."
};
static gmx_bool bMat = FALSE, bPI = FALSE, bSplit = FALSE, bMax = FALSE, bPBC = TRUE;
static gmx_bool bGroup = FALSE;
static real rcutoff = 0.6;
static int ng = 1;
static gmx_bool bEachResEachTime = FALSE, bPrintResName = FALSE;
t_pargs pa[] = {
{ "-matrix", FALSE, etBOOL, {&bMat},
"Calculate half a matrix of group-group distances" },
{ "-max", FALSE, etBOOL, {&bMax},
"Calculate *maximum* distance instead of minimum" },
{ "-d", FALSE, etREAL, {&rcutoff},
"Distance for contacts" },
{ "-group", FALSE, etBOOL, {&bGroup},
"Count contacts with multiple atoms in the first group as one" },
{ "-pi", FALSE, etBOOL, {&bPI},
"Calculate minimum distance with periodic images" },
{ "-split", FALSE, etBOOL, {&bSplit},
"Split graph where time is zero" },
{ "-ng", FALSE, etINT, {&ng},
"Number of secondary groups to compute distance to a central group" },
{ "-pbc", FALSE, etBOOL, {&bPBC},
"Take periodic boundary conditions into account" },
{ "-respertime", FALSE, etBOOL, {&bEachResEachTime},
"When writing per-residue distances, write distance for each time point" },
{ "-printresname", FALSE, etBOOL, {&bPrintResName},
"Write residue names" }
};
output_env_t oenv;
t_topology *top = NULL;
int ePBC = -1;
char title[256];
real t;
rvec *x;
matrix box;
gmx_bool bTop = FALSE;
FILE *atm;
int i, j, nres = 0;
const char *trxfnm, *tpsfnm, *ndxfnm, *distfnm, *numfnm, *atmfnm, *oxfnm, *resfnm;
char **grpname;
int *gnx;
atom_id **index, *residues = NULL;
t_filenm fnm[] = {
{ efTRX, "-f", NULL, ffREAD },
{ efTPS, NULL, NULL, ffOPTRD },
{ efNDX, NULL, NULL, ffOPTRD },
{ efXVG, "-od", "mindist", ffWRITE },
{ efXVG, "-on", "numcont", ffOPTWR },
{ efOUT, "-o", "atm-pair", ffOPTWR },
{ efTRO, "-ox", "mindist", ffOPTWR },
{ efXVG, "-or", "mindistres", ffOPTWR }
};
#define NFILE asize(fnm)
if (!parse_common_args(&argc, argv,
PCA_CAN_VIEW | PCA_CAN_TIME | PCA_TIME_UNIT | PCA_BE_NICE,
NFILE, fnm, asize(pa), pa, asize(desc), desc, 0, NULL, &oenv))
{
return 0;
}
trxfnm = ftp2fn(efTRX, NFILE, fnm);
ndxfnm = ftp2fn_null(efNDX, NFILE, fnm);
distfnm = opt2fn("-od", NFILE, fnm);
numfnm = opt2fn_null("-on", NFILE, fnm);
atmfnm = ftp2fn_null(efOUT, NFILE, fnm);
oxfnm = opt2fn_null("-ox", NFILE, fnm);
resfnm = opt2fn_null("-or", NFILE, fnm);
if (bPI || resfnm != NULL)
{
/* We need a tps file */
tpsfnm = ftp2fn(efTPS, NFILE, fnm);
}
else
{
//.........这里部分代码省略.........
开发者ID:exianshine,项目名称:gromacs,代码行数:101,代码来源:gmx_mindist.c
示例7: gmx_spol
int gmx_spol(int argc, char *argv[])
{
t_topology *top;
t_inputrec *ir;
t_atom *atom;
char title[STRLEN];
t_trxstatus *status;
int nrefat, natoms, nf, ntot;
real t;
rvec *xtop, *x, xref, trial, dx = {0}, dip, dir;
matrix box;
FILE *fp;
int *isize, nrefgrp;
atom_id **index, *molindex;
char **grpname;
real rmin2, rmax2, rcut, rcut2, rdx2 = 0, rtry2, qav, q, dip2, invbw;
int nbin, i, m, mol, a0, a1, a, d;
double sdip, sdip2, sinp, sdinp, nmol;
int *hist;
t_pbc pbc;
gmx_rmpbc_t gpbc = NULL;
const char *desc[] = {
"[THISMODULE] analyzes dipoles around a solute; it is especially useful",
"for polarizable water. A group of reference atoms, or a center",
"of mass reference (option [TT]-com[tt]) and a group of solvent",
"atoms is required. The program splits the group of solvent atoms",
"into molecules. For each solvent molecule the distance to the",
"closest atom in reference group or to the COM is determined.",
"A cumulative distribution of these distances is plotted.",
"For each distance between [TT]-rmin[tt] and [TT]-rmax[tt]",
"the inner product of the distance vector",
"and the dipole of the solvent molecule is determined.",
"For solvent molecules with net charge (ions), the net charge of the ion",
"is subtracted evenly from all atoms in the selection of each ion.",
"The average of these dipole components is printed.",
"The same is done for the polarization, where the average dipole is",
"subtracted from the instantaneous dipole. The magnitude of the average",
"dipole is set with the option [TT]-dip[tt], the direction is defined",
"by the vector from the first atom in the selected solvent group",
"to the midpoint between the second and the third atom."
};
output_env_t oenv;
static gmx_bool bCom = FALSE, bPBC = FALSE;
static int srefat = 1;
static real rmin = 0.0, rmax = 0.32, refdip = 0, bw = 0.01;
t_pargs pa[] = {
{ "-com", FALSE, etBOOL, {&bCom},
"Use the center of mass as the reference postion" },
{ "-refat", FALSE, etINT, {&srefat},
"The reference atom of the solvent molecule" },
{ "-rmin", FALSE, etREAL, {&rmin}, "Maximum distance (nm)" },
{ "-rmax", FALSE, etREAL, {&rmax}, "Maximum distance (nm)" },
{ "-dip", FALSE, etREAL, {&refdip}, "The average dipole (D)" },
{ "-bw", FALSE, etREAL, {&bw}, "The bin width" }
};
t_filenm fnm[] = {
{ efTRX, NULL, NULL, ffREAD },
{ efTPR, NULL, NULL, ffREAD },
{ efNDX, NULL, NULL, ffOPTRD },
{ efXVG, NULL, "scdist", ffWRITE }
};
#define NFILE asize(fnm)
if (!parse_common_args(&argc, argv, PCA_CAN_TIME | PCA_CAN_VIEW,
NFILE, fnm, asize(pa), pa, asize(desc), desc, 0, NULL, &oenv))
{
return 0;
}
snew(top, 1);
snew(ir, 1);
read_tpx_top(ftp2fn(efTPR, NFILE, fnm),
ir, box, &natoms, NULL, NULL, NULL, top);
/* get index groups */
printf("Select a group of reference particles and a solvent group:\n");
snew(grpname, 2);
snew(index, 2);
snew(isize, 2);
get_index(&top->atoms, ftp2fn_null(efNDX, NFILE, fnm), 2, isize, index, grpname);
if (bCom)
{
nrefgrp = 1;
nrefat = isize[0];
}
else
{
nrefgrp = isize[0];
nrefat = 1;
}
spol_atom2molindex(&(isize[1]), index[1], &(top->mols));
srefat--;
//.........这里部分代码省略.........
开发者ID:FoldingAtHome,项目名称:gromacs,代码行数:101,代码来源:gmx_spol.c
示例8: gmx_trjorder
int gmx_trjorder(int argc, char *argv[])
{
const char *desc[] = {
"[THISMODULE] orders molecules according to the smallest distance",
"to atoms in a reference group",
"or on z-coordinate (with option [TT]-z[tt]).",
"With distance ordering, it will ask for a group of reference",
"atoms and a group of molecules. For each frame of the trajectory",
"the selected molecules will be reordered according to the shortest",
"distance between atom number [TT]-da[tt] in the molecule and all the",
"atoms in the reference group. The center of mass of the molecules can",
"be used instead of a reference atom by setting [TT]-da[tt] to 0.",
"All atoms in the trajectory are written",
"to the output trajectory.[PAR]",
"[THISMODULE] can be useful for e.g. analyzing the n waters closest to a",
"protein.",
"In that case the reference group would be the protein and the group",
"of molecules would consist of all the water atoms. When an index group",
"of the first n waters is made, the ordered trajectory can be used",
"with any GROMACS program to analyze the n closest waters.",
"[PAR]",
"If the output file is a [REF].pdb[ref] file, the distance to the reference target",
"will be stored in the B-factor field in order to color with e.g. Rasmol.",
"[PAR]",
"With option [TT]-nshell[tt] the number of molecules within a shell",
"of radius [TT]-r[tt] around the reference group are printed."
};
static int na = 3, ref_a = 1;
static real rcut = 0;
static gmx_bool bCOM = FALSE, bZ = FALSE;
t_pargs pa[] = {
{ "-na", FALSE, etINT, {&na},
"Number of atoms in a molecule" },
{ "-da", FALSE, etINT, {&ref_a},
"Atom used for the distance calculation, 0 is COM" },
{ "-com", FALSE, etBOOL, {&bCOM},
"Use the distance to the center of mass of the reference group" },
{ "-r", FALSE, etREAL, {&rcut},
"Cutoff used for the distance calculation when computing the number of molecules in a shell around e.g. a protein" },
{ "-z", FALSE, etBOOL, {&bZ},
"Order molecules on z-coordinate" }
};
FILE *fp;
t_trxstatus *out;
t_trxstatus *status;
gmx_bool bNShell, bPDBout;
t_topology top;
int ePBC;
rvec *x, *xsol, xcom, dx;
matrix box;
t_pbc pbc;
gmx_rmpbc_t gpbc;
real t, totmass, mass, rcut2 = 0, n2;
int natoms, nwat, ncut;
char **grpname;
int i, j, d, *isize, isize_ref = 0, isize_sol;
int sa, sr, *swi, **index, *ind_ref = NULL, *ind_sol;
gmx_output_env_t *oenv;
t_filenm fnm[] = {
{ efTRX, "-f", NULL, ffREAD },
{ efTPS, NULL, NULL, ffREAD },
{ efNDX, NULL, NULL, ffOPTRD },
{ efTRO, "-o", "ordered", ffOPTWR },
{ efXVG, "-nshell", "nshell", ffOPTWR }
};
#define NFILE asize(fnm)
if (!parse_common_args(&argc, argv, PCA_CAN_TIME,
NFILE, fnm, asize(pa), pa, asize(desc), desc, 0, NULL, &oenv))
{
return 0;
}
read_tps_conf(ftp2fn(efTPS, NFILE, fnm), &top, &ePBC, &x, NULL, box, TRUE);
sfree(x);
/* get index groups */
printf("Select %sa group of molecules to be ordered:\n",
bZ ? "" : "a group of reference atoms and ");
snew(grpname, 2);
snew(index, 2);
snew(isize, 2);
get_index(&top.atoms, ftp2fn_null(efNDX, NFILE, fnm), bZ ? 1 : 2,
isize, index, grpname);
if (!bZ)
{
isize_ref = isize[0];
isize_sol = isize[1];
ind_ref = index[0];
ind_sol = index[1];
}
else
{
isize_sol = isize[0];
ind_sol = index[0];
}
natoms = read_first_x(oenv, &status, ftp2fn(efTRX, NFILE, fnm), &t, &x, box);
if (natoms > top.atoms.nr)
//.........这里部分代码省略.........
开发者ID:pjohansson,项目名称:gromacs,代码行数:101,代码来源:gmx_trjorder.cpp
示例9: gmx_velacc
int gmx_velacc(int argc,char *argv[])
{
const char *desc[] = {
"[TT]g_velacc[tt] computes the velocity autocorrelation function.",
"When the [TT]-m[tt] option is used, the momentum autocorrelation",
"function is calculated.[PAR]",
"With option [TT]-mol[tt] the velocity autocorrelation function of",
"molecules is calculated. In this case the index group should consist",
"of molecule numbers instead of atom numbers.[PAR]",
"Be sure that your trajectory contains frames with velocity information",
"(i.e. [TT]nstvout[tt] was set in your original [TT].mdp[tt] file),",
"and that the time interval between data collection points is",
"much shorter than the time scale of the autocorrelation."
};
static gmx_bool bMass=FALSE,bMol=FALSE,bRecip=TRUE;
t_pargs pa[] = {
{ "-m", FALSE, etBOOL, {&bMass},
"Calculate the momentum autocorrelation function" },
{ "-recip", FALSE, etBOOL, {&bRecip},
"Use cm^-1 on X-axis instead of 1/ps for spectra." },
{ "-mol", FALSE, etBOOL, {&bMol},
"Calculate the velocity acf of molecules" }
};
t_topology top;
int ePBC=-1;
t_trxframe fr;
matrix box;
gmx_bool bTPS=FALSE,bTop=FALSE;
int gnx;
atom_id *index;
char *grpname;
char title[256];
/* t0, t1 are the beginning and end time respectively.
* dt is the time step, mass is temp variable for atomic mass.
*/
real t0,t1,dt,mass;
t_trxstatus *status;
int counter,n_alloc,i,j,counter_dim,k,l;
rvec mv_mol;
/* Array for the correlation function */
real **c1;
real *normm=NULL;
output_env_t oenv;
#define NHISTO 360
t_filenm fnm[] = {
{ efTRN, "-f", NULL, ffREAD },
{ efTPS, NULL, NULL, ffOPTRD },
{ efNDX, NULL, NULL, ffOPTRD },
{ efXVG, "-o", "vac", ffWRITE },
{ efXVG, "-os", "spectrum", ffOPTWR }
};
#define NFILE asize(fnm)
int npargs;
t_pargs *ppa;
npargs = asize(pa);
ppa = add_acf_pargs(&npargs,pa);
parse_common_args(&argc,argv,PCA_CAN_VIEW | PCA_CAN_TIME | PCA_BE_NICE,
NFILE,fnm,npargs,ppa,asize(desc),desc,0,NULL,&oenv);
if (bMol || bMass) {
bTPS = ftp2bSet(efTPS,NFILE,fnm) || !ftp2bSet(efNDX,NFILE,fnm);
}
if (bTPS) {
bTop=read_tps_conf(ftp2fn(efTPS,NFILE,fnm),title,&top,&ePBC,NULL,NULL,box,
TRUE);
get_index(&top.atoms,ftp2fn_null(efNDX,NFILE,fnm),1,&gnx,&index,&grpname);
} else
rd_index(ftp2fn(efNDX,NFILE,fnm),1,&gnx,&index,&grpname);
if (bMol) {
if (!bTop)
gmx_fatal(FARGS,"Need a topology to determine the molecules");
snew(normm,top.atoms.nr);
precalc(top,normm);
index_atom2mol(&gnx,index,&top.mols);
}
/* Correlation stuff */
snew(c1,gnx);
for(i=0; (i<gnx); i++)
c1[i]=NULL;
read_first_frame(oenv,&status,ftp2fn(efTRN,NFILE,fnm),&fr,TRX_NEED_V);
t0=fr.time;
n_alloc=0;
counter=0;
do {
if (counter >= n_alloc) {
n_alloc+=100;
for(i=0; i<gnx; i++)
srenew(c1[i],DIM*n_alloc);
}
counter_dim=DIM*counter;
//.........这里部分代码省略.........
开发者ID:martinhoefling,项目名称:gromacs,代码行数:101,代码来源:gmx_velacc.c
示例10: gmx_dih
int gmx_dih(int argc,char *argv[])
{
const char *desc[] = {
"g_dih can do two things. The default is to analyze dihedral transitions",
"by merely computing all the dihedral angles defined in your topology",
"for the whole trajectory. When a dihedral flips over to another minimum",
"an angle/time plot is made.[PAR]",
"The opther option is to discretize the dihedral space into a number of",
"bins, and group each conformation in dihedral space in the",
"appropriate bin. The output is then given as a number of dihedral",
"conformations sorted according to occupancy."
};
static int mult = -1;
static gmx_bool bSA = FALSE;
t_pargs pa[] = {
{ "-sa", FALSE, etBOOL, {&bSA},
"Perform cluster analysis in dihedral space instead of analysing dihedral transitions." },
{ "-mult", FALSE, etINT, {&mult},
"mulitiplicity for dihedral angles (by default read from topology)" }
};
FILE *out;
t_xrama *xr;
t_topology *top;
real **dih,*time;
real dd;
int i,nframes,maxframes=1000;
output_env_t oenv;
t_filenm fnm[] = {
{ efTRX, "-f", NULL, ffREAD },
{ efTPX, NULL, NULL, ffREAD },
{ efOUT, NULL, NULL, ffWRITE }
};
#define NFILE asize(fnm)
CopyRight(stderr,argv[0]);
parse_common_args(&argc,argv,PCA_CAN_VIEW | PCA_CAN_TIME | PCA_BE_NICE,
NFILE,fnm,asize(pa),pa,asize(desc),desc,0,NULL,&oenv);
if (mult != -1)
fprintf(stderr,"Using %d for dihedral multiplicity rather than topology values\n",mult);
snew(xr,1);
init_rama(oenv,ftp2fn(efTRX,NFILE,fnm),
ftp2fn(efTPX,NFILE,fnm),xr,3);
top=read_top(ftp2fn(efTPX,NFILE,fnm),NULL);
/* Brute force malloc, may be too big... */
snew(dih,xr->ndih);
for(i=0; (i<xr->ndih); i++)
snew(dih[i],maxframes);
snew(time,maxframes);
fprintf(stderr,"\n");
nframes = 0;
while (new_data(xr)) {
for(i=0; (i<xr->ndih); i++) {
dd=xr->dih[i].ang*RAD2DEG;
while (dd < 0)
dd+=360;
while (dd > 360)
dd-=360;
dih[i][nframes]=dd;
}
time[nframes]=xr->t;
nframes++;
if (nframes > maxframes) {
maxframes += 1000;
for(i=0; (i<xr->ndih); i++)
srenew(dih[i],maxframes);
srenew(time,maxframes);
}
}
fprintf(stderr,"\nCalculated all dihedrals, now analysing...\n");
out=ftp2FILE(efOUT,NFILE,fnm,"w");
if (bSA) {
/* Cluster and structure analysis */
ana_cluster(out,xr,dih,time,top,nframes,mult);
}
else {
/* Analyse transitions... */
ana_trans(out,xr,dih,time,top,nframes,oenv);
}
ffclose(out);
thanx(stderr);
return 0;
}
开发者ID:andersx,项目名称:gmx-debug,代码行数:91,代码来源:gmx_dih.c
示例11: gmx_xpm2ps
//.........这里部分代码省略.........
{ "-yonce", FALSE, etBOOL, {&bYonce}, "Show y-label only once" },
{ "-legend", FALSE, etENUM, {legend}, "Show legend" },
{ "-diag", FALSE, etENUM, {diag}, "Diagonal" },
{ "-size", FALSE, etREAL, {&size},
"Horizontal size of the matrix in ps units" },
{ "-bx", FALSE, etREAL, {&boxx},
"Element x-size, overrides [TT]-size[tt] (also y-size when [TT]-by[tt] is not set)" },
{ "-by", FALSE, etREAL, {&boxy}, "Element y-size" },
{ "-rainbow", FALSE, etENUM, {rainbow},
"Rainbow colors, convert white to" },
{ "-gradient", FALSE, etRVEC, {grad},
"Re-scale colormap to a smooth gradient from white {1,1,1} to {r,g,b}" },
{ "-skip", FALSE, etINT, {&skip},
"only write out every nr-th row and column" },
{ "-zeroline", FALSE, etBOOL, {&bZeroLine},
"insert line in [TT].xpm[tt] matrix where axis label is zero"},
{ "-legoffset", FALSE, etINT, {&mapoffset},
"Skip first N colors from [TT].xpm[tt] file for the legend" },
{ "-combine", FALSE, etENUM, {combine}, "Combine two matrices" },
{ "-cmin", FALSE, etREAL, {&cmin}, "Minimum for combination output" },
{ "-cmax", FALSE, etREAL, {&cmax}, "Maximum for combination output" }
};
#define NPA asize(pa)
t_filenm fnm[] = {
{ efXPM, "-f", NULL, ffREAD },
{ efXPM, "-f2", "root2", ffOPTRD },
{ efM2P, "-di", NULL, ffLIBOPTRD },
{ efM2P, "-do", "out", ffOPTWR },
{ efEPS, "-o", NULL, ffOPTWR },
{ efXPM, "-xpm", NULL, ffOPTWR }
};
#define NFILE asize(fnm)
if (!parse_common_args(&argc, argv, PCA_CAN_VIEW,
NFILE, fnm, NPA, pa,
asize(desc), desc, 0, NULL, &oenv))
{
return 0;
}
etitle = nenum(title);
elegend = nenum(legend);
ediag = nenum(diag);
erainbow = nenum(rainbow);
ecombine = nenum(combine);
bGrad = opt2parg_bSet("-gradient", NPA, pa);
for (i = 0; i < DIM; i++)
{
if (grad[i] < 0 || grad[i] > 1)
{
gmx_fatal(FARGS, "RGB value %g out of range (0.0-1.0)", grad[i]);
}
}
if (!bFrame)
{
etitle = etNone;
elegend = elNone;
}
epsfile = ftp2fn_null(efEPS, NFILE, fnm);
xpmfile = opt2fn_null("-xpm", NFILE, fnm);
if (epsfile == NULL && xpmfile == NULL)
{
if (ecombine != ecHalves)
{
xpmfile = opt2fn("-xpm", NFILE, fnm);
开发者ID:exianshine,项目名称:gromacs,代码行数:67,代码来源:gmx_xpm2ps.c
示例12: main
int main(int argc, char *argv[]) {
const char *desc[] = {
"g_ensemble_comp evaluates the difference between two conformational ensembles, R and R'.",
"Quanitification is in terms of a true metric that satisfies the conditions set forth by the zeroth law of thermodynamics.",
"The quantification metric eta=1-|Overlap|=|R'|-|Overlap|=DeltaR is normalized, that is, 0<=eta<1,",
"and takes up a value closer to unity as the difference between the ensembles increases.",
"For two Gaussian distributions with identical standard deviations of 0.5 A,",
"eta=0.68 represents a geometric center deviation of 1 A.\n",
"The two ensembles are provided as two trajectory files specified by the -f1 and -f2 options (supported formats=xtc,trr,pdb).",
"We recommend that frames numbers in the trajectory files are in the range 2500-5000.",
"While the speed of the algorithm decreases with increase in ensemble size,",
"the numerical accuracy of the calculation reduces with decrease in ensemble size,",
"and a small number of frames may not provide a good representation of the ensemble.",
"Note that if you are not interested in eta to reflect changes in whole molecule translation/rotation,",
"then these degress of freedom need to be removed prior to ensemble comparison.",
"For most cases, this can be accomplished by fitting all conformations",
"in the two ensembles on to one single representative structure, such as the x-ray structure",
"For this, we recommend the use of trjconv with the -fit rot+trans option.\n"
"By default, differences (eta) are estimated for all atoms, but comparisons can be done for a smaller specific group of atoms,",
"which can be selected from index files -n1 and -n2. ",
"The average eta can also be calculated for each residue specified in a structure file given by -res (.pdb and .gro are supported).\n",
"Overlaps are estimated by training a support vector machine in a pre-defined Hilbert space specified by",
"the width of the RDF Kernel (gamma=0.4) and",
"the maximum value that can be taken up by the Lagrange multiplier (C=100.0).",
"The values of C and gamma can be changed with -c and -g,",
"but such changes may increase mean absolute error (MAE=3.26%) of the method.\n",
"If g_ensemble_comp was built with OPENMP, you can set the number of threads to use with -nthreads X,\n",
"where X is the number of threads to use. The default behavior is to use the maximum number of
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