[cig-commits] r4274 - mc/3D/CitcomS/trunk/doc/manual
tan2 at geodynamics.org
tan2 at geodynamics.org
Fri Aug 11 14:36:18 PDT 2006
Author: tan2
Date: 2006-08-11 14:36:18 -0700 (Fri, 11 Aug 2006)
New Revision: 4274
Modified:
mc/3D/CitcomS/trunk/doc/manual/citcoms.lyx
Log:
Fixed the status of CitcomS.py on TeraGrid
Modified: mc/3D/CitcomS/trunk/doc/manual/citcoms.lyx
===================================================================
--- mc/3D/CitcomS/trunk/doc/manual/citcoms.lyx 2006-08-11 20:28:49 UTC (rev 4273)
+++ mc/3D/CitcomS/trunk/doc/manual/citcoms.lyx 2006-08-11 21:36:18 UTC (rev 4274)
@@ -317,7 +317,7 @@
The fundamental basis for the numerical solution of any time-dependent convectio
n problem is the sequential solution of an equation of motion and an energy
equation.
- Convection problems are initially valued (tan2: ?) with boundary conditions,
+ Convection problems are initially valued with boundary conditions,
including all of the problems which are solved with CitComS.py.
The normal sequence of steps for the solution of convection problems starts
with an initial temperature field.
@@ -2972,9 +2972,8 @@
\end_layout
\begin_layout Standard
-CitComS.py has already been installed on several NSF TeraGrid platforms.
- (tan2: this statement may not be true) Accounts for small allocations are
- available directly from CIG.
+CitComS.py has already been tested on several NSF TeraGrid platforms.
+ Accounts for small allocations are available directly from CIG.
\end_layout
\begin_layout Chapter
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