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 51d1f29dec894ef76c5d6f9b34b1dfa09f309ffb..b43ec050518ff7a57e1d483626b5eccec85f5ba7 100644 (file)
--- 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
 <tt>deal.II</tt>. 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.
 </p>
 
 <p> In order to allow sufficient flexibility in conjunction with systems of