From fb4cc15d79d09bbe6ac5b808d30d8f62c059874e Mon Sep 17 00:00:00 2001
From: sjplimp
Date: Thu, 15 Nov 2007 15:29:14 +0000
Subject: [PATCH] git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@1170
f3b2605a-c512-4ea7-a41b-209d697bcdaa
---
doc/fix_langevin.html | 8 +++++++-
doc/fix_langevin.txt | 7 ++++++-
doc/fix_nph.html | 20 ++++++++++++++++----
doc/fix_nph.txt | 18 ++++++++++++++----
doc/fix_npt.html | 23 ++++++++++++++++++++---
doc/fix_npt.txt | 20 +++++++++++++++++---
doc/fix_nvt.html | 10 ++++++++--
doc/fix_nvt.txt | 9 +++++++--
8 files changed, 95 insertions(+), 20 deletions(-)
diff --git a/doc/fix_langevin.html b/doc/fix_langevin.html
index c6e54a7734..4498d1b134 100644
--- a/doc/fix_langevin.html
+++ b/doc/fix_langevin.html
@@ -68,7 +68,9 @@ into the particle. As derived from the fluctuation/dissipation
theorum, its magnitude is proportional to sqrt(T m / dt damp), where T
is the desired temperature, m is the mass of the particle, dt is the
timestep size, and damp is the damping factor. Random numbers are
-used to randomize the direction and magnitude of this force.
+used to randomize the direction and magnitude of this force as
+described in (Dunweg), where a uniform random number is used
+(instead of a Gaussian random number) for speed.
The desired temperature at each timestep is a ramped value during the
run from Tstart to Tstop.
@@ -146,4 +148,8 @@ viscous
Default: none
+
+
+(Dunweg) Dunweg and Paul, Int J of Modern Physics C, 2, 817-27 (1991).
+