From 66d656a65f6707cbb06157faa2bfecbbe0feb8a8 Mon Sep 17 00:00:00 2001 From: Wolfgang Bangerth Date: Tue, 22 Feb 2011 18:01:35 +0000 Subject: [PATCH] Minor edits. git-svn-id: https://svn.dealii.org/trunk@23418 0785d39b-7218-0410-832d-ea1e28bc413d --- deal.II/doc/doxygen/headers/vector_valued.h | 5 +++-- 1 file changed, 3 insertions(+), 2 deletions(-) diff --git a/deal.II/doc/doxygen/headers/vector_valued.h b/deal.II/doc/doxygen/headers/vector_valued.h index b1038513b9..662bab6719 100644 --- a/deal.II/doc/doxygen/headers/vector_valued.h +++ b/deal.II/doc/doxygen/headers/vector_valued.h @@ -555,7 +555,7 @@ scalar_product (const Tensor<2,dim> &u, * @endcode * * So if, again, this is not the code we use in step-8, what do - * we do there? The answer rests on the finite element we use. There, we use the + * we do there? The answer rests on the finite element we use. In step-8, we use the * following element: * @code * FESystem finite_element (FE_Q(1), dim); @@ -565,7 +565,8 @@ scalar_product (const Tensor<2,dim> &u, * "primitive" element: an element that may be vector-valued but where each * shape function has exactly one non-zero component. In other words: if the * $x$-component of a displacement shape function is nonzero, then the $y$- - * and $z$-components must be zero and so on. What this means is that also + * and $z$-components must be zero and similarly for the other components. + * What this means is that also * derived quantities based on shape functions inherit this sparsity property. * For example: the divergence * $\mathrm{div}\ \Phi(x,y,z)=\partial_x\varphi_x(x,y,z) + -- 2.39.5