[cig-commits] r8103 - doc/CitcomS/manual

[tan2 at geodynamics.org]

Author: tan2
Date: 2007-10-10 17:05:16 -0700 (Wed, 10 Oct 2007)
New Revision: 8103

Modified:
   doc/CitcomS/manual/citcoms.lyx
Log:
Minor fix

Modified: doc/CitcomS/manual/citcoms.lyx
===================================================================
--- doc/CitcomS/manual/citcoms.lyx	2007-10-11 00:03:40 UTC (rev 8102)
+++ doc/CitcomS/manual/citcoms.lyx	2007-10-11 00:05:16 UTC (rev 8103)
@@ -630,9 +630,9 @@
 n dependent viscosity and heat generation by Thorsten Becker; (7) compressed
  ASCII output by Thorsten Becker; (8) an easier way for mesh refinement
  for the radial coordinate by Thorsten Becker; (9) an exchanger package
- for solver coupling; (10) removing the rigid rotation component from the
- velocity by Shijie Zhong; and (11) an option to disable monitoring of maximum
- temperature.
+ for solver coupling; (10) removing the rigid body rotation component from
+ the velocity by Shijie Zhong; and (11) an option to disable monitoring
+ of maximum temperature.
  Additional backward incompatible changes include: (1) the viscosity field
  at element level is not smoothed (this might slow down the convergence
  but will represent the viscosity field more accurately); (2) the Lenardic
@@ -9875,8 +9875,8 @@
  The numerical solution of the velocity and stress fields can be compared
  with semi-analytical solutions.
  The Stokes solver is benchmarked and validated.
- However, no analytical solution exits for the benchmark on the energy equation
- solver, which is nonlinear.
+ However, no analytical solution exists for the benchmark on the energy
+ equation solver, which is nonlinear.
  The steady-state solution is usually used for the comparison with other
  numerical solutions.
  
@@ -16654,6 +16654,9 @@
 \begin_inset Text
 
 \begin_layout Standard
+
+\family typewriter
+\size small
 uzawa=cg
 \end_layout