mirror of https://github.com/lammps/lammps.git
Added FixMSST in package shock
git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@4276 f3b2605a-c512-4ea7-a41b-209d697bcdaa
This commit is contained in:
parent
73b32571d9
commit
0166234a3c
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@ -367,6 +367,7 @@ package".
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<TR><TD >poems </TD><TD > coupled rigid body motion</TD></TR>
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<TR><TD >prd </TD><TD > parallel replica dynamics</TD></TR>
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<TR><TD >reax </TD><TD > ReaxFF potential</TD></TR>
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<TR><TD >shock </TD><TD > methods for MD simulations of shock loading</TD></TR>
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<TR><TD >xtc </TD><TD > dump atom snapshots in XTC format
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</TD></TR></TABLE></DIV>
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@ -361,6 +361,7 @@ peri : Peridynamics model and potential
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poems : coupled rigid body motion
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prd : parallel replica dynamics
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reax : ReaxFF potential
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shock : methods for MD simulations of shock loading
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xtc : dump atom snapshots in XTC format :tb(s=:)
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There are also user-contributed packages which may be as simple as a
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@ -0,0 +1,168 @@
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<HTML>
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<CENTER><A HREF = "http://lammps.sandia.gov">LAMMPS WWW Site</A> - <A HREF = "Manual.html">LAMMPS Documentation</A> - <A HREF = "Section_commands.html#comm">LAMMPS Commands</A>
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</CENTER>
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<HR>
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<H3> fix msst command
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</H3>
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<P><B>Syntax:</B>
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</P>
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<PRE>fix ID group-ID msst dir shockvel keyword value ...
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</PRE>
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<UL><LI>ID, group-ID are documented in <A HREF = "fix.html">fix</A> command
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<LI>msst = style name of this fix
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<LI>dir = <I>x</I> or <I>y</I> or <I>z</I>
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<LI>shockvel = shock velocity (strictly positive, distance/time units)
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<LI>zero or more keyword value pairs may be appended
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<LI>keyword = <I>q</I> or <I>mu</I> or <I>p0</I> or <I>v0</I> or <I>e0</I> or <I>tscale</I>
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<PRE> <I>q</I> value = cell mass-like parameter (mass^2/distance^4 units)
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<I>mu</I> value = artificial viscosity (mass/length/time units)
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<I>p0</I> value = initial pressure in the shock equations (pressure units)
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<I>v0</I> value = initial simulation cell volume in the shock equations (distance^3 units)
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<I>e0</I> value = initial total energy (energy units)
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<I>tscale</I> value = reduction in initial temperature (unitless fraction between 0.0 and 1.0)
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</PRE>
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</UL>
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<P><B>Examples:</B>
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</P>
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<PRE>fix 1 all msst y 100.0 q 1.0e5 mu 1.0e5
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fix 2 all msst z 50.0 q 1.0e4 mu 1.0e4 v0 4.3419e+03 p0 3.7797e+03 e0 -9.72360e+02 tscale 0.01
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</PRE>
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<P><B>Description:</B>
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</P>
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<P>This command performs the Multi-Scale Shock Technique (MSST) integration
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to update positions and velocities each timestep to mimic a compressive shock
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wave passing over the system. See <A HREF = "#Reed">(Reed)</A> for a detailed description of this method.
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The MSST varies the cell volume and temperature in such a
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way as to restrain the system to the shock Hugoniot and the Rayleigh
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line. These restraints correspond to the macroscopic conservation laws
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dictated by a shock front. <I>shockvel</I> determines the steady shock
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velocity that will be simulated.
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</P>
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<P>To perform a simulation, choose a value of <I>q</I> that provides volume compression
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on the timescale of 100 fs to 1 ps. If the volume is not compressing, either
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the shock speed is chosen to be below the material sound speed or <I>p0</I> has been
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chosen inaccurately. Volume compression at the start can
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be sped up by using a non-zero value of <I>tscale</I>. Use the smallest value of
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<I>tscale</I> that results in compression.
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</P>
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<P>Under some special high-symmetry conditions, the pressure (volume) and/or temperature
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of the system may oscillate for many cycles even with an appropriate
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choice of mass-like parameter <I>q</I>. Such oscillations have physical
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significance in some cases. The optional <I>mu</I> keyword adds an artificial
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viscosity that helps break the system symmetry
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to equilibrate to the shock Hugoniot and Rayleigh line more rapidly in such cases.
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</P>
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<P><I>tscale</I> is a factor between 0 and 1 that determines
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what fraction of thermal kinetic energy is converted to compressive strain
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kinetic energy at the start of the simulation. Setting this parameter to a
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non-zero value may assist in compression at the start of simulations where it
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is slow to occur.
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</P>
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<P>If keywords <I>e0</I>, <I>p0</I>,or <I>v0</I> are not supplied, these quantities will be calculated
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on the first step, after the energy specified by <I>tscale</I> is removed.
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The value of <I>e0</I> is not used in the dynamical equations,
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but is used in calculating the deviation from the Hugoniot.
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</P>
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<P>Values of shockvel less than a critical value determined by the material
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response will not have compressive solutions. This will be reflected in
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lack of significant change of the volume in the MSST.
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</P>
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<P>For all pressure styles, the simulation box stays orthogonal in shape.
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Parrinello-Rahman boundary conditions (tilted box) are supported by LAMMPS,
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but are not implemented for MSST.
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</P>
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<P>This fix computes a temperature and pressure each timestep. To do this,
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the fix creates its own computes of style "temp" and "pressure", as if
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these commands had been issued:
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</P>
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<PRE>compute fix-ID_temp group-ID temp
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compute fix-ID_press group-ID pressure fix-ID_temp
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</PRE>
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<P>See the <A HREF = "compute_temp.html">compute temp</A> and <A HREF = "compute_pressure.html">compute
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pressure</A> commands for details. Note that the
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IDs of the new computes are the fix-ID + underscore + "temp" or fix_ID
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+ underscore + "press". The group for
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the new computes is "all".
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</P>
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<P><B>Restart, fix_modify, output, run start/stop, minimize info:</B>
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</P>
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<P>This fix writes the state of all internal
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variables to <A HREF = "restart.html">binary restart files</A>. See the
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<A HREF = "read_restart.html">read_restart</A> command for info on how to re-specify
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a fix in an input script that reads a restart file, so that the
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operation of the fix continues in an uninterrupted fashion.
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</P>
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<P>The progress of the MSST can be monitored by printing the global scalar and
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global vector quantities computed by the fix.
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</P>
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<P>The scalar is the cumulative energy change due to the fix. This is also the energy
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added to the potential energy by the <A HREF = "fix_modify.html">fix_modify</A> <I>energy</I> command.
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With this command, the thermo keyword
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<I>etotal</I> prints the conserved quantity of the MSST dynamic equations. This can be
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used to test if the MD timestep is sufficiently small for accurate integration
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of the dynamic equations. See also <A HREF = "thermo_style.html">thermo_style</A> command.
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</P>
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<P>The global vector contains four values in this order:
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</P>
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<P>[<I>dhugoniot</I>, <I>drayleigh</I>, <I>lagrangian_speed</I>, <I>lagrangian_position</I>]
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</P>
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<OL><LI><I>dhugoniot</I> is the departure from the Hugoniot (temperature units).
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<LI><I>drayleigh</I> is the departure from the Rayleigh line (pressure units).
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<LI><I>lagrangian_speed</I> is the laboratory-frame Lagrangian speed (particle velocity) of the computational cell (velocity units).
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<LI><I>lagrangian_position</I> is the computational cell position in the reference frame moving at the shock speed. This is usually a good estimate of distance of the computational cell behind the shock front.
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</OL>
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<P>To print these quantities to the log file with descriptive column headers, the
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following LAMMPS commands are suggested:
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</P>
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<PRE>fix msst all msst z
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fix_modify msst energy yes
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variable dhug equal f_msst[1]
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variable dray equal f_msst[2]
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variable lgr_vel equal f_msst[3]
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variable lgr_pos equal f_msst[4]
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thermo_style custom step temp ke pe lz pzz etotal v_dhug v_dray v_lgr_vel v_lgr_pos f_msst
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</PRE>
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<P>These fixes compute a global scalar and a global vector of 4 quantities,
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which can be accessed by various <A HREF = "Section_howto.html#4_15">output commands</A>.
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The scalar values calculated by
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this fix are "extensive"; the vector values are "intensive".
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</P>
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<P><B>Restrictions:</B>
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</P>
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<P>This fix style is part of the "shock" package. It is only enabled if
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LAMMPS was built with that package. See the <A HREF = "Section_start.html#2_3">Making
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LAMMPS</A> section for more info.
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</P>
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<P>All cell dimensions must be periodic. This fix can not be used with a triclinic cell.
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The MSST fix has been tested only for the group-ID all.
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</P>
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<P><B>Related commands:</B>
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</P>
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<P><A HREF = "fix_deform.html">fix deform</A>
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</P>
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<P><B>Default:</B>
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</P>
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<P>The keyword defaults are q = 10, mu = 0, tscale = 0.01. p0, v0, and e0
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are calculated on the first step.
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</P>
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<HR>
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<A NAME = "Reed"></A>
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<P><B>(Reed)</B> Reed, Fried, and Joannopoulos, Phys. Rev. Lett., 90, 235503 (2003).
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</P>
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</HTML>
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@ -0,0 +1,155 @@
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"LAMMPS WWW Site"_lws - "LAMMPS Documentation"_ld - "LAMMPS Commands"_lc :c
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:link(lws,http://lammps.sandia.gov)
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:link(ld,Manual.html)
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:link(lc,Section_commands.html#comm)
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:line
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fix msst command :h3
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[Syntax:]
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fix ID group-ID msst dir shockvel keyword value ... :pre
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ID, group-ID are documented in "fix"_fix.html command :ulb,l
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msst = style name of this fix :l
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dir = {x} or {y} or {z} :l
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shockvel = shock velocity (strictly positive, distance/time units) :l
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zero or more keyword value pairs may be appended :l
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keyword = {q} or {mu} or {p0} or {v0} or {e0} or {tscale} :l
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{q} value = cell mass-like parameter (mass^2/distance^4 units)
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{mu} value = artificial viscosity (mass/length/time units)
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{p0} value = initial pressure in the shock equations (pressure units)
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{v0} value = initial simulation cell volume in the shock equations (distance^3 units)
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{e0} value = initial total energy (energy units)
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{tscale} value = reduction in initial temperature (unitless fraction between 0.0 and 1.0) :pre
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:ule
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[Examples:]
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fix 1 all msst y 100.0 q 1.0e5 mu 1.0e5
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fix 2 all msst z 50.0 q 1.0e4 mu 1.0e4 v0 4.3419e+03 p0 3.7797e+03 e0 -9.72360e+02 tscale 0.01 :pre
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[Description:]
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This command performs the Multi-Scale Shock Technique (MSST) integration
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to update positions and velocities each timestep to mimic a compressive shock
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wave passing over the system. See "(Reed)"_#Reed for a detailed description of this method.
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The MSST varies the cell volume and temperature in such a
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way as to restrain the system to the shock Hugoniot and the Rayleigh
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line. These restraints correspond to the macroscopic conservation laws
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dictated by a shock front. {shockvel} determines the steady shock
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velocity that will be simulated.
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To perform a simulation, choose a value of {q} that provides volume compression
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on the timescale of 100 fs to 1 ps. If the volume is not compressing, either
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the shock speed is chosen to be below the material sound speed or {p0} has been
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chosen inaccurately. Volume compression at the start can
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be sped up by using a non-zero value of {tscale}. Use the smallest value of
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{tscale} that results in compression.
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Under some special high-symmetry conditions, the pressure (volume) and/or temperature
|
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of the system may oscillate for many cycles even with an appropriate
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choice of mass-like parameter {q}. Such oscillations have physical
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significance in some cases. The optional {mu} keyword adds an artificial
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viscosity that helps break the system symmetry
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to equilibrate to the shock Hugoniot and Rayleigh line more rapidly in such cases.
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{tscale} is a factor between 0 and 1 that determines
|
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what fraction of thermal kinetic energy is converted to compressive strain
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kinetic energy at the start of the simulation. Setting this parameter to a
|
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non-zero value may assist in compression at the start of simulations where it
|
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is slow to occur.
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If keywords {e0}, {p0},or {v0} are not supplied, these quantities will be calculated
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on the first step, after the energy specified by {tscale} is removed.
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The value of {e0} is not used in the dynamical equations,
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but is used in calculating the deviation from the Hugoniot.
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Values of shockvel less than a critical value determined by the material
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response will not have compressive solutions. This will be reflected in
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lack of significant change of the volume in the MSST.
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For all pressure styles, the simulation box stays orthogonal in shape.
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Parrinello-Rahman boundary conditions (tilted box) are supported by LAMMPS,
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but are not implemented for MSST.
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This fix computes a temperature and pressure each timestep. To do this,
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the fix creates its own computes of style "temp" and "pressure", as if
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these commands had been issued:
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compute fix-ID_temp group-ID temp
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compute fix-ID_press group-ID pressure fix-ID_temp :pre
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See the "compute temp"_compute_temp.html and "compute
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pressure"_compute_pressure.html commands for details. Note that the
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IDs of the new computes are the fix-ID + underscore + "temp" or fix_ID
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+ underscore + "press". The group for
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the new computes is "all".
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[Restart, fix_modify, output, run start/stop, minimize info:]
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This fix writes the state of all internal
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variables to "binary restart files"_restart.html. See the
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"read_restart"_read_restart.html command for info on how to re-specify
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a fix in an input script that reads a restart file, so that the
|
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operation of the fix continues in an uninterrupted fashion.
|
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The progress of the MSST can be monitored by printing the global scalar and
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global vector quantities computed by the fix.
|
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The scalar is the cumulative energy change due to the fix. This is also the energy
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added to the potential energy by the "fix_modify"_fix_modify.html {energy} command.
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With this command, the thermo keyword
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{etotal} prints the conserved quantity of the MSST dynamic equations. This can be
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used to test if the MD timestep is sufficiently small for accurate integration
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of the dynamic equations. See also "thermo_style"_thermo_style.html command.
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The global vector contains four values in this order:
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\[{dhugoniot}, {drayleigh}, {lagrangian_speed}, {lagrangian_position}\]
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{dhugoniot} is the departure from the Hugoniot (temperature units).
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{drayleigh} is the departure from the Rayleigh line (pressure units).
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{lagrangian_speed} is the laboratory-frame Lagrangian speed (particle velocity) of the computational cell (velocity units).
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{lagrangian_position} is the computational cell position in the reference frame moving at the shock speed. This is usually a good estimate of distance of the computational cell behind the shock front. :ol
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To print these quantities to the log file with descriptive column headers, the
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following LAMMPS commands are suggested:
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fix msst all msst z
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fix_modify msst energy yes
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variable dhug equal f_msst\[1\]
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variable dray equal f_msst\[2\]
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variable lgr_vel equal f_msst\[3\]
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variable lgr_pos equal f_msst\[4\]
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thermo_style custom step temp ke pe lz pzz etotal v_dhug v_dray v_lgr_vel v_lgr_pos f_msst :pre
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These fixes compute a global scalar and a global vector of 4 quantities,
|
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which can be accessed by various "output commands"_Section_howto.html#4_15.
|
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The scalar values calculated by
|
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this fix are "extensive"; the vector values are "intensive".
|
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|
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[Restrictions:]
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|
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This fix style is part of the "shock" package. It is only enabled if
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LAMMPS was built with that package. See the "Making
|
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LAMMPS"_Section_start.html#2_3 section for more info.
|
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|
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All cell dimensions must be periodic. This fix can not be used with a triclinic cell.
|
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The MSST fix has been tested only for the group-ID all.
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[Related commands:]
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"fix deform"_fix_deform.html
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[Default:]
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The keyword defaults are q = 10, mu = 0, tscale = 0.01. p0, v0, and e0
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are calculated on the first step.
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:line
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:link(Reed)
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[(Reed)] Reed, Fried, and Joannopoulos, Phys. Rev. Lett., 90, 235503 (2003).
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@ -223,7 +223,7 @@ barostat variables.
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The {mtk} keyword controls whether or not the correction terms due to
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Martyna, Tuckerman, and Klein are included in the equations of motion
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"(Martyna1994)"_#Martyna1994. Specifying {no} reproduces the original
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"(Martyna)"_#Martyna. Specifying {no} reproduces the original
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Hoover barostat, whose volume probability distribution function
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differs from the true NPT and NPH ensembles by a factor of 1/V. Hence
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using {yes} is more correct, but in many cases the difference is
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