[cig-commits] r8208 - doc/CitcomS/manual

[sue at geodynamics.org]

Author: sue
Date: 2007-11-06 11:25:59 -0800 (Tue, 06 Nov 2007)
New Revision: 8208

Modified:
   doc/CitcomS/manual/citcoms.lyx
   doc/CitcomS/manual/citcoms.pdf
Log:
new 3.0 history paragraph

Modified: doc/CitcomS/manual/citcoms.lyx
===================================================================
--- doc/CitcomS/manual/citcoms.lyx	2007-11-06 01:04:43 UTC (rev 8207)
+++ doc/CitcomS/manual/citcoms.lyx	2007-11-06 19:25:59 UTC (rev 8208)
@@ -624,18 +624,21 @@
 \end_layout
 
 \begin_layout Standard
-This release of CitcomS (3.0) contains several new features: (1) two implementati
-ons of compressible convection, one by Wei Leng and Shijie Zhong and the
- other by Eh Tan; (2) the ability to resume computation from previous checkpoint
-s; (3) multi-component chemical convection; (4) a fixed non-Newtonian solver;
- (5) a rheology option for pseudo-plasiticity by Thorsten Becker; (6) compositio
-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 body rotation component from
- the velocity by Shijie Zhong; and (11) an option to disable monitoring
- of maximum temperature.
- Additional changes that are not backward compatible include: (1) the viscosity
+This release of CitcomS (3.0) contains many new features, including two implement
+ations of compressible convection, one by Wei Leng and Shijie Zhong and
+ the other by Eh Tan; the ability to resume computation from previous checkpoint
+s; multi-component chemical convection; a fixed non-Newtonian solver; an
+ exchanger package for solver coupling; removing the rigid body rotation
+ component from the velocity by Shijie Zhong; and an option to disable monitorin
+g of maximum temperature.
+ In addition, a rheology option for pseudo-plasiticity, composition dependent
+ viscosity and heat generation, compressed ASCII output, and an easier way
+ for mesh refinement for the radial coordinate were added by Thorsten Becker.
+ 
+\end_layout
+
+\begin_layout Standard
+Additional changes that are not backward compatible 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
  filter on temperature is disabled by default; (3) the rigid body rotation
@@ -1285,7 +1288,9 @@
 \begin_layout Standard
 \align right
 \begin_inset Formula \begin{equation}
-\bar{\rho}c_{P}\left(T_{,t}+u_{i}T_{,i}\right)\left(1+2\Gamma\left(1-\Gamma\right)\frac{\gamma_{ph}^{2}}{d_{ph}}\frac{Rab}{Ra}Di\left(T+T_{0}\right)\right)=\bar{\rho}c_{P}\kappa T_{,ii}+\rho\alpha gu_{r}Di\left(T+T_{0}\right)\left(1+2\Gamma\left(1-\Gamma\right)\frac{\gamma_{ph}}{d_{ph}}\frac{Rab}{Ra}\right)+\frac{Di}{Ra}\Phi+\bar{\rho}H\label{eq:non-dimensional energy eqn}\end{equation}
+\begin{array}{c}
+\bar{\rho}c_{P}\left(T_{,t}+u_{i}T_{,i}\right)\left(1+2\Gamma\left(1-\Gamma\right)\frac{\gamma_{ph}^{2}}{d_{ph}}\frac{Rab}{Ra}Di\left(T+T_{0}\right)\right)=\bar{\rho}c_{P}\kappa T_{,ii}\\
++\rho\alpha gu_{r}Di\left(T+T_{0}\right)\left(1+2\Gamma\left(1-\Gamma\right)\frac{\gamma_{ph}}{d_{ph}}\frac{Rab}{Ra}\right)+\frac{Di}{Ra}\Phi+\bar{\rho}H\end{array}\label{eq:non-dimensional energy eqn}\end{equation}
 
 \end_inset
 

Modified: doc/CitcomS/manual/citcoms.pdf
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