forked from lijiext/lammps
135 lines
5.5 KiB
Plaintext
135 lines
5.5 KiB
Plaintext
"LAMMPS WWW Site"_lws - "LAMMPS Documentation"_ld - "LAMMPS Commands"_lc :c
|
|
|
|
:link(lws,http://lammps.sandia.gov)
|
|
:link(ld,Manual.html)
|
|
:link(lc,Section_commands.html#comm)
|
|
|
|
:line
|
|
|
|
compute temp/profile command :h3
|
|
|
|
[Syntax:]
|
|
|
|
compute ID group-ID temp/profile xflag yflag zflag binstyle args :pre
|
|
|
|
ID, group-ID are documented in "compute"_compute.html command :ulb,l
|
|
temp/profile = style name of this compute command :l
|
|
xflag,yflag,zflag = 0/1 for whether to exclude/include this dimension :l
|
|
binstyle = {x} or {y} or {z} or {xy} or {yz} or {xz} or {xyz} :l
|
|
{x} arg = Nx
|
|
{y} arg = Ny
|
|
{z} arg = Nz
|
|
{xy} args = Nx Ny
|
|
{yz} args = Ny Nz
|
|
{xz} args = Nx Nz
|
|
{xyz} args = Nx Ny Nz
|
|
Nx,Ny,Nz = number of velocity bins in x,y,z dimensions :pre
|
|
:ule
|
|
|
|
[Examples:]
|
|
|
|
compute myTemp flow temp/profile 1 1 1 x 10
|
|
compute myTemp flow temp/profile 0 1 1 xyz 20 20 20 :pre
|
|
|
|
[Description:]
|
|
|
|
Define a computation that calculates the temperature of a group of
|
|
atoms, after subtracting out a spatially-averaged velocity field,
|
|
before computing the kinetic energy. This can be useful for
|
|
thermostatting a collection of atoms undergoing a complex flow,
|
|
e.g. via a profile-unbiased thermostat (PUT) as described in
|
|
"(Evans)"_#Evans. A compute of this style can be used by any command
|
|
that computes a temperature, e.g. "thermo_modify"_thermo_modify.html,
|
|
"fix temp/rescale"_fix_temp_rescale.html, "fix npt"_fix_npt.html, etc.
|
|
|
|
The {xflag}, {yflag}, {zflag} settings determine which components of
|
|
average velocity are subtracted out.
|
|
|
|
The {binstyle} setting and its {Nx}, {Ny}, {Nz} arguments determine
|
|
how bins are setup to perform spatial averaging. "Bins" can be 1d
|
|
slabs, 2d pencils, or 3d bricks depending on which {binstyle} is used.
|
|
The simulation box is partitioned conceptually into {Nx} by {Ny} by
|
|
{Nz} bins. Depending on the {binstyle}, you may only specify one or
|
|
two of these values; the others are effectively set to 1 (no binning
|
|
in that dimension). For non-orthogonal (triclinic) simulation boxes,
|
|
the bins are "tilted" slabs or pencils or bricks that are parallel to
|
|
the tilted faces of the box. See the "region prism"_region.html
|
|
command for a discussion of the geometry of tilted boxes in LAMMPS.
|
|
|
|
When a temperature is computed, the velocity for the set of atoms that
|
|
are both in the compute group and in the same spatial bin is summed to
|
|
compute an average velocity for the bin. This bias velocity is then
|
|
subtracted from the velocities of individual atoms in the bin to yield
|
|
a thermal velocity for each atom. Note that if there is only one
|
|
atom in the bin, it's thermal velocity will thus be 0.0.
|
|
|
|
After the spatially-averaged velocity field has been subtracted from
|
|
each atom, the temperature is calculated by the formula KE = dim/2 N k
|
|
T, where KE = total kinetic energy of the group of atoms (sum of 1/2 m
|
|
v^2), dim = 2 or 3 = dimensionality of the simulation, N = number of
|
|
atoms in the group, k = Boltzmann constant, and T = temperature.
|
|
|
|
A 6-component kinetic energy tensor is also calculated by this compute
|
|
for use in the calculation of a pressure tensor. The formula for the
|
|
components of the tensor is the same as the above formula, except that
|
|
v^2 is replaced by vx * vy for the xy component, etc.
|
|
|
|
The number of atoms contributing to the temperature is assumed to be
|
|
constant for the duration of the run; use the {dynamic} option of the
|
|
"compute_modify"_compute_modify.html command if this is not the case.
|
|
|
|
The removal of the spatially-averaged velocity field by this fix is
|
|
essentially computing the temperature after a "bias" has been removed
|
|
from the velocity of the atoms. If this compute is used with a fix
|
|
command that performs thermostatting then this bias will be subtracted
|
|
from each atom, thermostatting of the remaining thermal velocity will
|
|
be performed, and the bias will be added back in. Thermostatting
|
|
fixes that work in this way include "fix nvt"_fix_nvt.html, "fix
|
|
temp/rescale"_fix_temp_rescale.html, "fix
|
|
temp/berendsen"_fix_temp_berendsen, and "fix
|
|
langevin"_fix_langevin.html.
|
|
|
|
This compute subtracts out degrees-of-freedom due to fixes that
|
|
constrain molecular motion, such as "fix shake"_fix_shake.html and
|
|
"fix rigid"_fix_rigid.html. This means the temperature of groups of
|
|
atoms that include these constraints will be computed correctly. If
|
|
needed, the subtracted degrees-of-freedom can be altered using the
|
|
{extra} option of the "compute_modify"_compute_modify.html command.
|
|
|
|
See "this howto section"_Section_howto.html#4_16 of the manual for a
|
|
discussion of different ways to compute temperature and perform
|
|
thermostatting. Using this compute in conjunction with a
|
|
thermostatting fix, as explained there, will effectively implement a
|
|
profile-unbiased thermostat (PUT), as described in "(Evans)"_#Evans.
|
|
|
|
[Output info:]
|
|
|
|
The scalar value calculated by this compute is "intensive", meaning it
|
|
is independent of the number of atoms in the simulation. The vector
|
|
values are "extensive", meaning they scale with the number of atoms in
|
|
the simulation.
|
|
|
|
[Restrictions:]
|
|
|
|
You should not use too large a velocity-binning grid, especially in
|
|
3d. In the current implementation, the binned velocity averages are
|
|
summed across all processors, so this will be inefficient if the grid
|
|
is too large, and the operation is performed every timestep, as it
|
|
will be for most thermostats.
|
|
|
|
[Related commands:]
|
|
|
|
"compute temp"_compute_temp.html, "compute
|
|
temp/ramp"_compute_temp_ramp.html, "compute
|
|
temp/deform"_compute_temp_deform.html, "compute
|
|
pressure"_compute_pressure.html
|
|
|
|
[Default:]
|
|
|
|
The option default is units = lattice.
|
|
|
|
:line
|
|
|
|
:link(Evans)
|
|
[(Evans)] Evans and Morriss, Phys Rev Lett, 56, 2172-2175 (1986).
|