]> https://gitweb.dealii.org/ - dealii.git/commitdiff
Fix a typo in the step-20 introduction.
authorDavid Wells <wellsd2@rpi.edu>
Sat, 20 Feb 2016 22:15:12 +0000 (17:15 -0500)
committerDavid Wells <wellsd2@rpi.edu>
Sat, 20 Feb 2016 22:15:12 +0000 (17:15 -0500)
examples/step-20/doc/intro.dox
examples/step-20/step-20.cc

index 5033c9b00e9a4fe06e952d0c74926633898236ed..bc1d59228f8dc9dc53f7b78df64f4530f363c3bb 100644 (file)
@@ -37,7 +37,7 @@ for fluid flow in porous media. In particular, if flow is so slow that all
 dynamic effects such as the acceleration terms in the Navier-Stokes equation
 become irrelevant, and if the flow pattern is stationary, then the
 Laplace
-equation models the pressure that drives the flow reasonable well. (Because the
+equation models the pressure that drives the flow reasonably well. (Because the
 solution variable is a pressure, we here use the name $p$ instead of the
 name $u$ more commonly used for the solution of partial differential equations.)
 
index d754d3549799f25928f9db5c554eb7c0c5c1d068..40260643a8cd2b722435fd9f502fa3f5401b287b 100644 (file)
 #include <deal.II/lac/block_sparse_matrix.h>
 #include <deal.II/lac/solver_cg.h>
 #include <deal.II/lac/precondition.h>
-// For our Schur complement solver, we need two new objects. One is a matrix
-// object which acts as the inverse of a matrix by calling an iterative
-// solver.
-#include <deal.II/lac/iterative_inverse.h>
 
 #include <deal.II/grid/tria.h>
 #include <deal.II/grid/grid_generator.h>

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