From 0605357f3e93533b83405ccff72bf40cef1bdceb Mon Sep 17 00:00:00 2001
From: Thomas Fischer <thomas.fischer@ufz.de>
Date: Thu, 10 Oct 2019 10:43:26 +0200
Subject: [PATCH] [web] HeatConduction: coefficient k -> lambda.
---
.../heatconduction/heatconduction-dirichlet.pandoc | 6 +++---
1 file changed, 3 insertions(+), 3 deletions(-)
diff --git a/web/content/docs/benchmarks/heatconduction/heatconduction-dirichlet.pandoc b/web/content/docs/benchmarks/heatconduction/heatconduction-dirichlet.pandoc
index ef514b8eaff..8617c578fb3 100644
--- a/web/content/docs/benchmarks/heatconduction/heatconduction-dirichlet.pandoc
+++ b/web/content/docs/benchmarks/heatconduction/heatconduction-dirichlet.pandoc
@@ -24,19 +24,19 @@ w.r.t boundary conditions
$$
\eqalign{
T(x) = g_D(x) &\quad \text{on }\Gamma_D,\cr
-k{\partial T(x) \over \partial n} = g_N(x) &\quad \text{on }\Gamma_N,
+\lambda {\partial T(x) \over \partial n} = g_N(x) &\quad \text{on }\Gamma_N,
}
$$
where $T$ could be temperature, the subscripts $D$ and $N$ denote the Dirichlet- and Neumann-type boundary conditions, $n$ is the normal vector pointing outside of $\Omega$, and $\Gamma = \Gamma_D \cup \Gamma_N$ and $\Gamma_D \cap \Gamma_N = \emptyset$.
## Problem specification and analytical solution
-We solve the Parabolic equation on a line domain $[60\times 1]$ with $k = 3.2$ and $\rho C_\textrm{p} = 2.5e10^6$ w.r.t. the specific boundary conditions:
+We solve the Parabolic equation on a line domain $[60\times 1]$ with $\lambda = 3.2$ and $\rho C_\textrm{p} = 2.5e10^6$ w.r.t. the specific boundary conditions:
$$
\eqalign{
T(x) = 274.15 &\quad \text{on } (x=0) \subset \Gamma_D,\cr
-k {\partial T(x) \over \partial n} = 0 &\quad \text{on } (x=60) \subset \Gamma_N.
+\lambda {\partial T(x) \over \partial n} = 0 &\quad \text{on } (x=60) \subset \Gamma_N.
}
$$
--
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