[cig-commits] r12886 - mc/2D/ConMan/trunk/doc
sue at geodynamics.org
sue at geodynamics.org
Mon Sep 15 14:16:04 PDT 2008
Author: sue
Date: 2008-09-15 14:16:04 -0700 (Mon, 15 Sep 2008)
New Revision: 12886
Modified:
mc/2D/ConMan/trunk/doc/conman.lyx
Log:
removed TODOs that are done
Modified: mc/2D/ConMan/trunk/doc/conman.lyx
===================================================================
--- mc/2D/ConMan/trunk/doc/conman.lyx 2008-09-15 21:09:38 UTC (rev 12885)
+++ mc/2D/ConMan/trunk/doc/conman.lyx 2008-09-15 21:16:04 UTC (rev 12886)
@@ -3397,13 +3397,13 @@
\begin_layout Standard
The second major change is that we have implemented a Picard iteration algorithm
- for steady-state problems (c.f.
- van Keken - thesis
-\series bold
-[TODO: This sounds different from the van Keken bib entry we have now.
- What thesis?]
-\series default
-).
+ for steady-state problems
+\begin_inset LatexCommand cite
+key "van Keken 1993"
+
+\end_inset
+
+.
Currently, this is implemented by changing compiler flags in the Makefile.
Picard iteration is an implicit solution to the energy equation (as opposed
to the predictor-corrector method described above); hence, non-symmetric
@@ -16373,11 +16373,12 @@
\end_layout
\begin_layout Standard
-Here we reproduce the results from Blankenbach et al.
- (1989)
-\series bold
-[TODO need reference for bibliography]
-\series default
+Here we reproduce the results from Blankenbach
+\begin_inset LatexCommand cite
+key "Blankenbach et al, 1989"
+
+\end_inset
+
for constant viscosity in a unit-aspect ratio domain, with free-slip boundary
conditions, heated from below and cooled from above.
The user should note that to run this problem, you will need to modify
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