Differences

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--- gtspring:spieker_blog:try_2proc [2009/04/07 15:21]
dspieker
+++ gtspring:spieker_blog:try_2proc [2010/02/02 07:55] (current)
@@ Line 28: / Line 28: @@
   for i in eq2_*.ff ; do tag=${i#eq2_} ; couette -T0 0 -T1 400 -o data-${tag%.ff} $i ; done
-I then created a parameter dependent flow field, that mixed the two least contracting directions, or equivalently, john's e_theta.
+I then created a parameter dependent flow field, that mixed two fields, or equivalently, john's e_theta.
-\\latex\\ e_theta = sin(\theta)u_0 + cos(\theta)u_1 \\latex\\
+<latex>
+e_{\theta} = sin(\theta)\vec{u}_0 + cos(\theta)\vec{u}_1
+</latex>
-I set theta to be pi/4, to get the strongest possible contribution from both fields.
+I set theta to be pi/4, to get the strongest possible contribution from both fields.  I then used poincare.cpp to calculate the intersections of each of the trajectories calculated in the script and saved them to disk.  I then plotted them, and what resulted is what is in my blog.

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