This benchmark is based on the benchmark presented in {cite:t}gerya:2010
and
extended in {cite:t}thieulot:2011
. It consists of a two-dimensional
\text{ Pa s}$. A square block of size
$128\text{ km}\times 128~\text{ km}$ is placed in the domain and is centered at
location
In a geodynamical context, the block could be interpreted as a detached slab
or a plume head. As such its viscosity and density can vary (a cold slab has a
higher effective viscosity than the surrounding mantle while it is the other
way around for a plume head). The block densities can then vary from a few
units to several hundreds of \text{ Pa s}$ and
$\delta\rho=32\text{ kg m}^{-3}$ is shown in {numref}fig:sinking_block1
.
As shown in {cite:t}thieulot:2011
one can independently vary \text{ Pa s}$ and
$\delta\rho=8,32,128\text{ kg m}^{-3}$. Results are shown in
{numref}fig:sinking_block2
and we indeed recover the expected trend with all data
points forming a single smooth line.
Description of benchmark files
<img src="dens_vel.png" style="width:60.0%" />
Density field with velocity arrows for $\eta_2=10^{27}~\text{ Pa s}$ and $\delta\rho=32~\text{ kg m}^{-3}$
<img src="plot.svg" style="width:80.0%" />
Scaled velocity measurements as a function of the viscosity contrast between surrounding medium and block for all experiments.
:::{toctree} ../README.md :::