From ed047c0f07afec2d6704ddde8af2b6f33ff15d34 Mon Sep 17 00:00:00 2001 From: Wenqing Wang 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