From f4b57f9828a4abcc5db2f6e6b3bd58c677ceb0ae Mon Sep 17 00:00:00 2001 From: bangerth Date: Wed, 23 Sep 2009 18:15:28 +0000 Subject: [PATCH] Escape 'identity'. git-svn-id: https://svn.dealii.org/trunk@19511 0785d39b-7218-0410-832d-ea1e28bc413d --- deal.II/examples/step-34/doc/intro.dox | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/deal.II/examples/step-34/doc/intro.dox b/deal.II/examples/step-34/doc/intro.dox index a8a93064d5..d09e079ec3 100644 --- a/deal.II/examples/step-34/doc/intro.dox +++ b/deal.II/examples/step-34/doc/intro.dox @@ -142,7 +142,7 @@ satisfy in a distributional sense the equation: where the derivative is done in the variable $\mathbf{y}$. By using the usual Green identities, our problem can be written on the boundary $\partial\Omega = \Gamma$ only. We recall the general definition of -the second Green identity: +the second Green %identity: \f[\label{green} \int_{\omega} @@ -168,7 +168,7 @@ $\Omega$, that is, they are in fact inner to the integration domain, and some care is required in defining the various integrals with the correct signs for the normals. -If we substitute $u$ and $v$ in the Green identity with the solution +If we substitute $u$ and $v$ in the Green %identity with the solution $\phi$ and with the fundamental solution of the Laplace equation respectively, as long as $\mathbf{x}$ is chosen in the region $\mathbb{R}^n\backslash\Omega$, we obtain: -- 2.39.5