From: Wolfgang Bangerth <bangerth@math.tamu.edu>
Date: Thu, 30 Jul 2009 13:01:51 +0000 (+0000)
Subject: Minor text edit.
X-Git-Tag: v8.0.0~7430
X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=d046e13265dd9864e5a00089e88e7aaa80394210;p=dealii.git

Minor text edit.


git-svn-id: https://svn.dealii.org/trunk@19135 0785d39b-7218-0410-832d-ea1e28bc413d
---

diff --git a/deal.II/examples/step-36/doc/intro.dox b/deal.II/examples/step-36/doc/intro.dox
index 1df6e81ec8..32fb3ea090 100644
--- a/deal.II/examples/step-36/doc/intro.dox
+++ b/deal.II/examples/step-36/doc/intro.dox
@@ -52,9 +52,9 @@ for linear algebra contents.
 
 The basic equation of stationary quantum mechanics is the
 Schr&ouml;dinger equation which models the motion of particles in an
-external potential $V(\mathbf x)$ as if it were governed a wave
+external potential $V(\mathbf x)$. The particle is described by a wave
 function $\Psi(\mathbf x)$ that satisfies a relation of the
-(non-dimensionalized   ) form 
+(non-dimensionalized) form 
 @f{align*} [-\Delta + V(\mathbf x)]
 \Psi(\mathbf x) &= \varepsilon \Psi(\mathbf x) \qquad &&\text{in}\
 \Omega\quad, \\ \Psi &= 0 &&\text{on}\ \partial\Omega\quad.