From: bangerth <bangerth@0785d39b-7218-0410-832d-ea1e28bc413d>
Date: Mon, 14 Oct 2013 20:56:11 +0000 (+0000)
Subject: Fix typo.
X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=8aa74b07a33fe8cf867d3f199afc981c15dd2a86;p=dealii-svn.git

Fix typo.


git-svn-id: https://svn.dealii.org/trunk@31231 0785d39b-7218-0410-832d-ea1e28bc413d
---

diff --git a/deal.II/examples/step-20/doc/intro.dox b/deal.II/examples/step-20/doc/intro.dox
index dd4c3829ca..13476bc201 100644
--- a/deal.II/examples/step-20/doc/intro.dox
+++ b/deal.II/examples/step-20/doc/intro.dox
@@ -400,10 +400,10 @@ also a full matrix. On the other hand, the CG algorithm doesn't require
 us to actually have a representation of $S$, it is sufficient to form
 matrix-vector products with it. We can do so in steps: to compute $Sv=B^TM^{-1}Bv=B^T(M^{-1}(Bv))$, we
 <ol>
- <li> form $w = T v$;
+ <li> form $w = B v$;
  <li> solve $My = w$ for $y=M^{-1}w$, using the CG method applied to the
   positive definite and symmetric mass matrix $M$;
- <li> form $z=B^Ty$ to obtain $Sv=z$.
+ <li> form $z=B^Ty$ to obtain $z=Sv$.
 </ol>
 Note how we evaluate the expression $B^TM^{-1}Bv$ right to left to
 avoid matrix-matrix products; this way, all we have to do is evaluate