From: bangerth Date: Mon, 30 Oct 2006 16:10:34 +0000 (+0000) Subject: One more crosslink X-Git-Url: https://gitweb.dealii.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=c69d64fe7cebd94cf0a5f0472e93d78769cf9b5c;p=dealii-svn.git One more crosslink git-svn-id: https://svn.dealii.org/trunk@14127 0785d39b-7218-0410-832d-ea1e28bc413d --- diff --git a/deal.II/examples/step-21/doc/intro.dox b/deal.II/examples/step-21/doc/intro.dox index f165ed298f..66761658ac 100644 --- a/deal.II/examples/step-21/doc/intro.dox +++ b/deal.II/examples/step-21/doc/intro.dox @@ -128,7 +128,8 @@ as well as the time dependent Maxwell equations (here, the algebraic constraint is that the divergence of the electric displacement field equals the charge density, $\textrm{div}\ \mathbf D = \rho$ and that the divergence of the magnetic flux density is zero: $\textrm{div}\ \mathbf -B = 0$). We will see that the different character of the two equations +B = 0$); even the quasistatic model of @ref step_18 "step-18" falls into this +category. We will see that the different character of the two equations will inform our discretization strategy for the two equations.