From 33e2d4a69e82846e21d2aeeff68564ef56b68045 Mon Sep 17 00:00:00 2001
From: bangerth <bangerth@0785d39b-7218-0410-832d-ea1e28bc413d>
Date: Tue, 3 Mar 2009 18:22:08 +0000
Subject: [PATCH] Unify upper/lower case in headings.

git-svn-id: https://svn.dealii.org/trunk@18445 0785d39b-7218-0410-832d-ea1e28bc413d
---
 deal.II/examples/step-34/doc/intro.dox | 4 ++--
 1 file changed, 2 insertions(+), 2 deletions(-)

diff --git a/deal.II/examples/step-34/doc/intro.dox b/deal.II/examples/step-34/doc/intro.dox
index 9eddab7663..f251658708 100644
--- a/deal.II/examples/step-34/doc/intro.dox
+++ b/deal.II/examples/step-34/doc/intro.dox
@@ -2,7 +2,7 @@
 
 <h1>Introduction</h1>
 
-<h3> Irrotational Flow </h3>
+<h3> Irrotational flow </h3>
 The motion of an inviscid fluid past a body (for example air past an
 airplane wing, or air or water past a propeller) is usually modeled by
 the Euler equations of fluid dynamics:
@@ -262,7 +262,7 @@ element $\hat K := [0,1]^n$, and we perform the integrations after a
 change of variables from the real element $K_i$ to the reference
 element $\hat K$.
 
-<h3> Singular Integrals in two dimension. </h3>
+<h3> Singular integrals in two dimension. </h3>
 
 In two dimensions it is not necessary to compute the diagonal elements
 $\mathbf{A}_{ii}$ of the system matrix, since, even if the denominator
-- 
2.39.5