[cig-commits] r5747 - geodyn/3D/MAG/trunk/doc

[wei at geodynamics.org]

Author: wei
Date: 2007-01-09 17:21:19 -0800 (Tue, 09 Jan 2007)
New Revision: 5747

Modified:
   geodyn/3D/MAG/trunk/doc/mag_book.lyx
Log:
more editing on Chapt.5

Modified: geodyn/3D/MAG/trunk/doc/mag_book.lyx
===================================================================
--- geodyn/3D/MAG/trunk/doc/mag_book.lyx	2007-01-10 00:45:35 UTC (rev 5746)
+++ geodyn/3D/MAG/trunk/doc/mag_book.lyx	2007-01-10 01:21:19 UTC (rev 5747)
@@ -1,4 +1,4 @@
-#LyX 1.4.3 created this file. For more info see http://www.lyx.org/
+#LyX 1.4.2 created this file. For more info see http://www.lyx.org/
 \lyxformat 245
 \begin_document
 \begin_header
@@ -1392,33 +1392,30 @@
 \end_layout
 
 \begin_layout Chapter
-Cookbook
+Examples
 \end_layout
 
 \begin_layout Standard
-Included in the cookbook are two benchmarkcases and a reversal dynamo case.
+Included in this chapter are two benchmark cases and a reversal dynamo case.
  We will present the cases with their input parameters and typical run of
  the case with output data analysis.
 \end_layout
 
 \begin_layout Section
-Benchmark Case 0
+Benchmark Cases 
 \end_layout
 
 \begin_layout Standard
-Historically this is the case defined in the benchmark study publish in
- 2001 paper by Gary Glazmeier et.
- al.
- It is a case of rotating non-magnetice converction.
- 
-\end_layout
+Historically, these are the cases defined in the benchmark study publish
+ in 2001 paper by Gary Glazmeier et.
+ al 
+\begin_inset LatexCommand \cite{benchmark cases}
 
-\begin_layout Section
-Benchmark Case 1
-\end_layout
+\end_inset
 
-\begin_layout Standard
-In this case, we have an insulation inner core co-rotating with the outer
+.
+ Case 0 is a benchmark of rotating non-magnetice converction.
+ Case 1 is a dynamo with an insulation inner core co-rotating with the outer
  boundary.
  The regions outside the fluid shelll are electrical insulators and the
  magnetic field on the boundaries matches with appropriate potential fields
@@ -1426,6 +1423,37 @@
  
 \end_layout
 
+\begin_layout Standard
+In both cases the Ekman number is 
+\begin_inset Formula $E$
+\end_inset
+
+ = 10
+\begin_inset Formula $^{-3}$
+\end_inset
+
+ and the Prandtl numver is 
+\begin_inset Formula $Pr$
+\end_inset
+
+ = 1.
+ The Rayleigh number is set to 
+\begin_inset Formula $Ra$
+\end_inset
+
+ = 100.
+ The magnetic Prandtl number is zero in the non-magnetic converction case
+ 0, and is 
+\begin_inset Formula $Pm$
+\end_inset
+
+ = 5 in case 1.
+\begin_inset Formula $$
+\end_inset
+
+
+\end_layout
+
 \begin_layout Section
 Reversal Dynamo Case
 \end_layout