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gmx-density(1)			GROMACS Manual			gmx-density(1)

NAME
       gmx-density - Calculate the density of the system

SYNOPSIS
       gmx density [-f [<.xtc/.trr/...>]] [-n [<.ndx>]]
		   [-s [<.tpr/.tpb/...>]] [-ei [<.dat>]] [-o [<.xvg>]]
		   [-nice <int>] [-b <time>] [-e <time>] [-dt <time>]
		   [-[no]w] [-xvg <enum>] [-d <string>] [-sl <int>]
		   [-dens <enum>] [-ng <int>] [-[no]center] [-[no]symm]
		   [-[no]relative]

DESCRIPTION
       gmx  density  computes partial densities across the box, using an index
       file.

       For the total density of NPT simulations, use gmx energy instead.

       Option -center performs the histogram binning relative to the center of
       an arbitrary group, in absolute box coordinates. If you are calculating
       profiles along the Z axis box dimension bZ, output would be from	 -bZ/2
       to bZ/2 if you center based on the entire system. Note that this behav‐
       iour has changed in Gromacs 5.0; earlier versions  merely  performed  a
       static  binning	in  (0,bZ)  and shifted the output. Now we compute the
       center for each frame and bin in (-bZ/2,bZ/2).

       Option -symm symmetrizes the output around the center. This will	 auto‐
       matically turn on -center too. Option -relative performs the binning in
       relative instead of absolute box coordinates, and scales the final out‐
       put  with  the average box dimension along the output axis. This can be
       used in combination with -center.

       Densities are in kg/m3, and number densities or electron densities  can
       also  be calculated. For electron densities, a file describing the num‐
       ber of electrons for each type of atom should be provided using -ei. It
       should  look  like: 2 atomname = nrelectrons atomname = nrelectrons The
       first line contains the number of lines to read from  the  file.	 There
       should be one line for each unique atom name in your system. The number
       of electrons for each atom is modified by its atomic partial charge.

       IMPORTANT CONSIDERATIONS FOR BILAYERS

       One of the most common usage scenarios is to calculate the  density  of
       various	groups across a lipid bilayer, typically with the z axis being
       the normal direction. For short simulations, small systems,  and	 fixed
       box  sizes  this	 will  work  fine, but for the more general case lipid
       bilayers can be complicated. The first problem that while both proteins
       and lipids have low volume compressibility, lipids have quite high area
       compressiblity.	This  means  the  shape	 of  the  box  (thickness  and
       area/lipid)  will fluctuate substantially even for a fully relaxed sys‐
       tem. Since Gromacs places the box between the origin and positive coor‐
       dinates,	 this  in  turn	 means that a bilayer centered in the box will
       move a bit up/down due to these fluctuations, and smear out  your  pro‐
       file. The easiest way to fix this (if you want pressure coupling) is to
       use the -center option that calculates the density profile with respect
       to the center of the box. Note that you can still center on the bilayer
       part even if you have a complex non-symmetric  system  with  a  bilayer
       and,  say,  membrane  proteins  - then our output will simply have more
       values on one side of the (center) origin reference.

       Even the centered calculation will lead to some smearing out the output
       profiles,  as  lipids  themselves  are compressed and expanded. In most
       cases you probably want	this  (since  it  corresponds  to  macroscopic
       experiments),  but if you want to look at molecular details you can use
       the -relative option to attempt to remove even more of the  effects  of
       volume fluctuations.

       Finally,	 large bilayers that are not subject to a surface tension will
       exhibit undulatory fluctuations, where there are 'waves' forming in the
       system. This is a fundamental property of the biological system, and if
       you are comparing against experiments you likely want  to  include  the
       undulation smearing effect.

OPTIONS
       Options to specify input and output files:

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

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

       -s [<.tpr/.tpb/...>] (topol.tpr) (Input)
	   Run input file: tpr tpb tpa

       -ei [<.dat>] (electrons.dat) (Input, Optional)
	   Generic data file

       -o [<.xvg>] (density.xvg) (Output)
	   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

       -d <string> (Z)
	   Take the normal on the membrane in direction X, Y or Z.

       -sl <int> (50)
	   Divide the box in this number of slices.

       -dens <enum> (mass)
	   Density: mass, number, charge, electron

       -ng <int> (1)
	   Number of groups of which to compute densities.

       -[no]center  (no)
	   Perform  the	 binning relative to the center of the (changing) box.
       Useful for bilayers.

       -[no]symm  (no)
	   Symmetrize the density along the axis, with respect to the  center.
       Useful for bilayers.

       -[no]relative  (no)
	   Use	relative  coordinates  for  changing boxes and scale output by
       average dimensions.

KNOWN ISSUES
       - When calculating electron densities, atomnames are  used  instead  of
       types. This is bad.

SEE ALSO
       gromacs(7)

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

VERSION 5.0.6							gmx-density(1)
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