From 0249119dcd2b9cb0c0f07b612cae46b0b9dc81b1 Mon Sep 17 00:00:00 2001
From: Dmitri Naumov <github@naumov.de>
Date: Tue, 21 Jul 2020 15:59:23 +0200
Subject: [PATCH] [web] Remove empty lines in latex scope.
This results in wrong rendering otherwise.
---
web/content/docs/benchmarks/creepbgra/CreepBRGa.pandoc | 1 -
.../elliptic/elliptic-dirichlet-volumetric-source-term.pandoc | 1 -
web/content/docs/benchmarks/elliptic/poisson_equation.pandoc | 1 -
...rimary-variable-constrain-dirichlet-boundary-condition.pandoc | 1 -
.../python-bc/laplace-equation/python-laplace-eq.pandoc | 1 -
5 files changed, 5 deletions(-)
diff --git a/web/content/docs/benchmarks/creepbgra/CreepBRGa.pandoc b/web/content/docs/benchmarks/creepbgra/CreepBRGa.pandoc
index e4123dad3ed..e37a04734bd 100644
--- a/web/content/docs/benchmarks/creepbgra/CreepBRGa.pandoc
+++ b/web/content/docs/benchmarks/creepbgra/CreepBRGa.pandoc
@@ -101,7 +101,6 @@ Newton-Raphson is applied to .
Let $$\begin{gathered}
\mathbf{r}= { \mathbf \sigma}^{n+1} -
{ \mathbf \sigma}^{n} - \mathbf{C} (\Delta { \mathbf \epsilon} - \alpha_T \Delta T \mathbf I)
-
+ 2bG \Delta t {\left\Vert{\mathbf s}^{n+1}\right\Vert}^{m-1}
{\mathbf s}^{n+1}
\end{gathered}$$
diff --git a/web/content/docs/benchmarks/elliptic/elliptic-dirichlet-volumetric-source-term.pandoc b/web/content/docs/benchmarks/elliptic/elliptic-dirichlet-volumetric-source-term.pandoc
index f9ab0fb2c4f..603b3f69409 100644
--- a/web/content/docs/benchmarks/elliptic/elliptic-dirichlet-volumetric-source-term.pandoc
+++ b/web/content/docs/benchmarks/elliptic/elliptic-dirichlet-volumetric-source-term.pandoc
@@ -18,7 +18,6 @@ weight = 102
We start with Poisson equation:
$$
\begin{equation}
-
- k\; \Delta p = Q \quad \text{in }\Omega
\end{equation}$$
w.r.t boundary conditions
diff --git a/web/content/docs/benchmarks/elliptic/poisson_equation.pandoc b/web/content/docs/benchmarks/elliptic/poisson_equation.pandoc
index e8a509d6621..bac4ee84302 100644
--- a/web/content/docs/benchmarks/elliptic/poisson_equation.pandoc
+++ b/web/content/docs/benchmarks/elliptic/poisson_equation.pandoc
@@ -18,7 +18,6 @@ weight = 102
The Poisson equation is:
$$
\begin{equation}
-
- k\; \Delta p = Q \quad \text{in }\Omega
\end{equation}$$
w.r.t boundary conditions
diff --git a/web/content/docs/benchmarks/liquid-flow/primary-variable-constrain-dirichlet-boundary-condition.pandoc b/web/content/docs/benchmarks/liquid-flow/primary-variable-constrain-dirichlet-boundary-condition.pandoc
index 609eff114c3..995492abbf8 100644
--- a/web/content/docs/benchmarks/liquid-flow/primary-variable-constrain-dirichlet-boundary-condition.pandoc
+++ b/web/content/docs/benchmarks/liquid-flow/primary-variable-constrain-dirichlet-boundary-condition.pandoc
@@ -20,7 +20,6 @@ $$
\left( c \rho_R + \phi \frac{\partial \rho_R}{\partial p}\right) \frac{\partial
p}{\partial t} - \nabla \cdot
\left[ \rho_R \frac{\kappa}{\mu} \left( \nabla p + \rho_R g \right) \right]
-
- Q_p = 0.
$$
where
diff --git a/web/content/docs/benchmarks/python-bc/laplace-equation/python-laplace-eq.pandoc b/web/content/docs/benchmarks/python-bc/laplace-equation/python-laplace-eq.pandoc
index 2d4d0c2fd18..3b9e0705df4 100644
--- a/web/content/docs/benchmarks/python-bc/laplace-equation/python-laplace-eq.pandoc
+++ b/web/content/docs/benchmarks/python-bc/laplace-equation/python-laplace-eq.pandoc
@@ -33,7 +33,6 @@ We solve Laplace's Equation in 2D on a $1 \times 1$ square domain.
Laplace's equation is
$$
\begin{equation}
-
- \mathop{\mathrm{div}} (a \mathop{\mathrm{grad}} u) = 0
\end{equation}
$$
--
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