From ed047c0f07afec2d6704ddde8af2b6f33ff15d34 Mon Sep 17 00:00:00 2001
From: Wenqing Wang <wenqing.wang@ufz.de>
Date: Tue, 2 Jul 2024 14:08:42 +0200
Subject: [PATCH] [web/benchmark] Fixed a formula display in CreepBGRa
---
.../docs/benchmarks/thermo-mechanics/CreepBGRa/index.md | 4 +++-
1 file changed, 3 insertions(+), 1 deletion(-)
diff --git a/web/content/docs/benchmarks/thermo-mechanics/CreepBGRa/index.md b/web/content/docs/benchmarks/thermo-mechanics/CreepBGRa/index.md
index 45175c5f1fe..85a398426f7 100644
--- a/web/content/docs/benchmarks/thermo-mechanics/CreepBGRa/index.md
+++ b/web/content/docs/benchmarks/thermo-mechanics/CreepBGRa/index.md
@@ -125,10 +125,12 @@ We see that $$\begin{aligned}
If the model is used for the thermo-mechanical problems and the problems
are solved by the monolithic scheme, the displacement-temperature block
of the global Jacobian can be derived as
-$$\begin{aligned}
+$$
+\begin{aligned}
-2G\dfrac{Q}{R} {{\int}_{\Omega} \dfrac{b}{T^2} {\left\Vert{\mathbf s}^{n+1}\right\Vert}^{m-1} \mathbf{B}^T {\mathbf s}^{n+1} \mathrm{d} \Omega}
\end{aligned}
+$$
*Note*: The above rate form of stress integration is implemented in OGS.
Alternatively, one can use an absolute stress integration form, which can be found in the attached
--
GitLab