GMX-FREEVOLUME(1)
NAME π
gmx-freevolume β calculate free volume π«§
SYNOPSIS π
gmx freevolume [-f [<.xtc/.trr/...>]] [-s [<.tpr/.gro/...>]]
[-n [<.ndx>]] [-o [<.xvg>]] [-b <time>] [-e <time>]
[-dt <time>] [-tu <enum>] [-fgroup <selection>]
[-xvg <enum>] [-[no]rmpbc] [-sf <file>]
[-selrpos <enum>] [-select <selection>] [-radius <real>]
[-seed <int>] [-ninsert <int>]
DESCRIPTION π¦
okay bestie, so gmx freevolume figures out the free volume in a box as a function of time, and it plots that free volume as a fraction of the total volume. literally that's the whole errand. π
here's the vibe: the program tries to insert a probe with a given radius into the simulation box, and if the distance between the probe and any atom is less than the sums of the van der Waals radii of both atoms, that position is considered occupied β i.e. non-free. no cap. so if you use a probe radius of 0, the true free volume is computed. and if you use a larger radius, e.g. 0.14 nm, which roughly corresponds to a water molecule π, you'll get the free volume for a hypothetical particle with that size. slay.
β οΈ but note though β since atoms are treated as hard-spheres, these numbers are very approximate, and typically only relative changes are meaningful, for instance by doing a series of simulations at different temperature.
The group specified by the selection is considered to delineate non-free volume. The number of insertions per unit of volume is important to get a converged result β about 1000/nm^3 yields an overall standard deviation that is determined by the fluctuations in the trajectory rather than by the fluctuations due to the random numbers. β¨
The results are critically dependent on the van der Waals radii; we recommend to use the values due to Bondi (1964). ic yk.
The Fractional Free Volume (FFV) that some authors like to use is given by 1 - 1.3*(1-Free Volume). This value is printed on the terminal. π»
OPTIONS π
Options to specify input files π₯
-f [<.xtc/.trr/...>](traj.xtc) (Optional) β input trajectory or single configuration:xtc trr cpt gro g96 pdb tng h5md-s [<.tpr/.gro/...>](topol.tpr) (Optional) β input structure:tpr gro g96 pdb brk ent-n [<.ndx>](index.ndx) (Optional) β extra index groups
Options to specify output files π€
-o [<.xvg>](freevolume.xvg) (Optional) β computed free volume
Other options π§
-b <time>(0) β first frame (ps) to read from trajectory-e <time>(0) β last frame (ps) to read from trajectory-dt <time>(0) β only use frame ift MOD dt == first time(ps)-tu <enum>(ps) β unit for time values:fs, ps, ns, us, ms, s-fgroup <selection>β atoms stored in the trajectory file (if not set, assume first N atoms)-xvg <enum>(xmgrace) β plot formatting:xmgrace, xmgr, none-[no]rmpbc(yes) β make molecules whole for each frame-sf <file>β provide selections from files-selrpos <enum>(atom) β selection reference positions:atom, res_com, res_cog, mol_com, mol_cog, whole_res_com, whole_res_cog, whole_mol_com, whole_mol_cog, part_res_com, part_res_cog, part_mol_com, part_mol_cog, dyn_res_com, dyn_res_cog, dyn_mol_com, dyn_mol_cog-select <selection>β atoms that are considered as part of the excluded volume-radius <real>(0) β radius of the probe to be inserted (nm,0yields the true free volume)-seed <int>(0) β seed for random number generator (0means generate).-ninsert <int>(1000) β number of probe insertions per cubic nm to try for each frame in the trajectory.
SEE ALSO π
gmx(1)- More information about GROMACS is available at <http://www.gromacs.org/>.
COPYRIGHT π
2026, GROMACS development team
and that's the whole thing bestie, no notes. this was GROMACS version 2026.4, dated Oct 02, 2026 β go off, have fun inserting probes, and remember: relative changes only, the hard-sphere approximation is doing its best ππ periodt.
π¦ where this page comes from
- nixpkgs unstable: gromacs 2026.4
- ubuntu stonking: gromacs-data 2026.4-1ubuntu1
- π girlified by deepseek-ai/DeepSeek-V4.1-Flash on : a language model's rewrite of the original, under its terms