GMX-VANHOVE(1) | GROMACS | GMX-VANHOVE(1) |
gmx-vanhove - Compute Van Hove displacement and correlation functions
gmx vanhove [-f [<.xtc/.trr/...>]] [-s [<.tpr/.gro/...>]] [-n [<.ndx>]]
[-om [<.xpm>]] [-or [<.xvg>]] [-ot [<.xvg>]] [-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>]
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 periodic 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 spacing between the times. The binwidth is set with option -rbin. The number 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 to specify input files:
Options to specify output files:
Other options:
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2021, GROMACS development team
March 29, 2021 | 2020.6-Debian-2020.6-2 |