From: guido
Date: Tue, 20 Jul 2004 11:33:57 +0000 (+0000)
Subject: more specific
X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=5c11ae8338f84eda39e3273deeb286ddfcaaff61;p=dealii-svn.git
more specific
git-svn-id: https://svn.dealii.org/trunk@9516 0785d39b-7218-0410-832d-ea1e28bc413d
---
diff --git a/deal.II/doc/tutorial/chapter-2.step-by-step/step-16.data/intro.html b/deal.II/doc/tutorial/chapter-2.step-by-step/step-16.data/intro.html
index 51d1f29dec..b43ec05051 100644
--- a/deal.II/doc/tutorial/chapter-2.step-by-step/step-16.data/intro.html
+++ b/deal.II/doc/tutorial/chapter-2.step-by-step/step-16.data/intro.html
@@ -5,8 +5,8 @@
This example shows the basic usage of the multilevel functions in
deal.II. It solves the Helmholtz equation with Neumann boundary conditions
to avoid additional complications due to Dirichlet boundary conditions (there,
-some library functions are missing). In all other respects, it is similar to
-step 5.
+some library functions are missing). Therefore, the solution is the constant
+function with value unity. In all other respects, it is similar to step 5.
In order to allow sufficient flexibility in conjunction with systems of