Fix some miscellaneous typos.

diff --git a/examples/step-12/step-12.cc b/examples/step-12/step-12.cc
index 59280b5feb3f4e4d3dd69730687bcc2d28eab25d..ba56c488a02a87e073020b77028cba49eea844db 100644 (file)
--- a/examples/step-12/step-12.cc
+++ b/examples/step-12/step-12.cc
@@ -134,7 +134,7 @@ namespace Step12
   //
   // The following objects are the scratch and copy objects we use in the call
   // to MeshWorker::mesh_loop(). The new object is the FEInterfaceValues object,
-  // that works similar to FEValues or FEFacesValues, except that it acts on
+  // that works similar to FEValues or FEFaceValues, except that it acts on
   // an interface between two cells and allows us to assemble the interface
   // terms in our weak form.
 

diff --git a/include/deal.II/fe/fe_simplex_p_bubbles.h b/include/deal.II/fe/fe_simplex_p_bubbles.h
index 556fa53e8a379b830d816dbe562e6e38e84ff5ae..8b556fcfc2cc6f2ed98b6206dfe9ef481d66eb0b 100644 (file)
--- a/include/deal.II/fe/fe_simplex_p_bubbles.h
+++ b/include/deal.II/fe/fe_simplex_p_bubbles.h
@@ -25,7 +25,8 @@
 DEAL_II_NAMESPACE_OPEN
 
 /**
- * @brief Enriched version of FE_P that can be used with nodal quadrature.
+ * @brief Enriched version of FE_SimplexP that can be used with nodal
+ * quadrature.
  *
  * Many explicit time integration schemes require solving a mass matrix at
  * each time step. There are various ways around this requirement - for
@@ -40,18 +41,18 @@ DEAL_II_NAMESPACE_OPEN
  * cannot be used with nodal quadrature since some of the quadrature weights
  * end up being either zero or negative, resulting in either an unsolvable or
  * unstable approximation to the mass matrix. For example: the shape functions
- * of FE_P<2>(2) with support points at vertices have mean values of zero so
- * that element cannot be used with mass lumping.
+ * of FE_SimplexP<2>(2) with support points at vertices have mean values of
+ * zero so that element cannot be used with mass lumping.
 
- * This element avoids this issue by replacing the shape functions of FE_P
- * with an augmented space amendable to the construction of nodal quadrature
- * rules. For example, on the triangle a single basis function is added
- * corresponding to interpolation at the centroid (and all other basis
+ * This element avoids this issue by replacing the shape functions of
+ * FE_SimplexP with an augmented space amenable to the construction of nodal
+ * quadrature rules. For example, on the triangle a single basis function is
+ * added corresponding to interpolation at the centroid (and all other basis
  * functions are updated to preserve the partition of unity property). This
  * results in shape functions with positive means (i.e., a valid nodal
- * quadrature formula). Similarly, in 3D, the polynomial space of FE_P<3>(2)
- * is enriched with five additional degrees of freedom (where four have
- * support points at face centroids and one has a support point at the
+ * quadrature formula). Similarly, in 3D, the polynomial space of
+ * FE_SimplexP<3>(2) is enriched with five additional degrees of freedom (where
+ * four have support points at face centroids and one has a support point at the
  * centroid) to enable construction of valid nodal quadrature rule.
  *
  * Since this FE space includes bubbles (i.e., extra functions which are