Chessboard pattern in pore pressure #31175
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jmeier
asked this question in
Q&A Modules: Porous Flow
Replies: 1 comment 17 replies
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Hello Given that hex20 looks weird too and tet14 segfaults (oob in the material properties), I think this is a problem with porous flow and higher order variables. Maybe the nodal mass lumping @jmeier can we simplify this further? Maybe using less material properties, using standard BCs and kernels. I remember @lindsayad was interested in tet10 oscillations with constraints so here's a ping. |
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Dear Moose Community,
To get a little more insight what is going on in #30828, I did some tinkering with one of the porous flow tests: modules/porous_flow/test/tests/sinks/s06.i. Up to my understanding this is a pure porous-flow test with no solid mechanics involved.
My context is: I have to build a hydro-mechanical coupled Moose model using TET10 elements.
Originally, this test consists of one HEX8 element (
nx=ny=nz=1). I modified to havenx=ny=nz=5and second order elements (HEX27 or TET10). Furthermore, I modified some of the material constants (to get more physical values), scaleddt(andend_time) and reduced tolerances a bit. But nothing what should change the overall behavior. Please find the resulting input file below.Switching between HEX27 and TET10 leads to some differences starting from time step 1. Please see the image below. The result for the HEX27 seem to be plausible. But it looks as if for TET10 the porous flow sink is not applied to the nodes at the corners of the elements but to the nodes at the midpoints:
input file
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