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gmx-vanhove(1)			GROMACS Manual			gmx-vanhove(1)

NAME
       gmx-vanhove - Compute Van Hove displacement and correlation functions

SYNOPSIS
       gmx vanhove [-f [<.xtc/.trr/...>]] [-s [<.tpr/.tpb/...>]]
		   [-n [<.ndx>]] [-om [<.xpm>]] [-or [<.xvg>]]
		   [-ot [<.xvg>]] [-nice <int>] [-b <time>] [-e <time>]
		   [-dt <time>] [-[no]w] [-xvg <enum>] [-sqrt <real>]
		   [-fm <int>] [-rmax <real>] [-rbin <real>] [-mmax <real>]
		   [-nlevels <int>] [-nr <int>] [-fr <int>] [-rt <real>]
		   [-ft <int>]

DESCRIPTION
       gmx  vanhove  computes  the Van Hove correlation function. The Van Hove
       G(r,t) is the probability that a particle that is at r_0 at  time  zero
       can  be found at position r_0+r at time t. gmx vanhove determines G not
       for a vector r, but for the length of r. Thus it gives the  probability
       that a particle moves a distance of r in time t. Jumps across the peri‐
       odic boundaries are removed. Corrections are made for  scaling  due  to
       isotropic or anisotropic pressure coupling.

       With  option -om the whole matrix can be written as a function of t and
       r or as a function of sqrt(t) and r (option -sqrt).

       With option -or the Van Hove function is plotted for one or more values
       of  t. Option -nr sets the number of times, option -fr the number spac‐
       ing between the times. The binwidth is set with option -rbin. The  num‐
       ber of bins is determined automatically.

       With  option  -ot the integral up to a certain distance (option -rt) is
       plotted as a function of time.

       For all frames that are read the coordinates of the selected  particles
       are  stored  in	memory. Therefore the program may use a lot of memory.
       For options -om and -ot the program may be slow. This  is  because  the
       calculation  scales as the number of frames times -fm or -ft. Note that
       with the -dt option the	memory	usage  and  calculation	 time  can  be
       reduced.

OPTIONS
       Options to specify input and output files:

       -f [<.xtc/.trr/...>] (traj.xtc) (Input)
	   Trajectory: xtc trr cpt trj gro g96 pdb tng

       -s [<.tpr/.tpb/...>] (topol.tpr) (Input)
	   Structure+mass(db): tpr tpb tpa gro g96 pdb brk ent

       -n [<.ndx>] (index.ndx) (Input, Optional)
	   Index file

       -om [<.xpm>] (vanhove.xpm) (Output, Optional)
	   X PixMap compatible matrix file

       -or [<.xvg>] (vanhove_r.xvg) (Output, Optional)
	   xvgr/xmgr file

       -ot [<.xvg>] (vanhove_t.xvg) (Output, Optional)
	   xvgr/xmgr file

       Other options:

       -nice <int> (19)
	   Set the nicelevel

       -b <time> (0)
	   First frame (ps) to read from trajectory

       -e <time> (0)
	   Last frame (ps) to read from trajectory

       -dt <time> (0)
	   Only use frame when t MOD dt = first time (ps)

       -[no]w  (no)
	   View output .xvg, .xpm, .eps and .pdb files

       -xvg <enum> (xmgrace)
	   xvg plot formatting: xmgrace, xmgr, none

       -sqrt <real> (0)
	   Use sqrt(t) on the matrix axis which binspacing  in sqrt(ps)

       -fm <int> (0)
	   Number of frames in the matrix, 0 is plot all

       -rmax <real> (2)
	   Maximum r in the matrix (nm)

       -rbin <real> (0.01)
	   Binwidth in the matrix and for -or (nm)

       -mmax <real> (0)
	   Maximum density in the matrix, 0 is calculate (1/nm)

       -nlevels <int> (81)
	   Number of levels in the matrix

       -nr <int> (1)
	   Number of curves for the -or output

       -fr <int> (0)
	   Frame spacing for the -or output

       -rt <real> (0)
	   Integration limit for the -ot output (nm)

       -ft <int> (0)
	   Number of frames in the -ot output, 0 is plot all

SEE ALSO
       gromacs(7)

       More   information  about  GROMACS  is  available  at  <http://www.gro‐
       macs.org/>.

VERSION 5.0.6							gmx-vanhove(1)
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