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How to use powerLaw rheological model with incompressibleMultiphaseVoF solver |
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September 29, 2024, 09:33 |
How to use powerLaw rheological model with incompressibleMultiphaseVoF solver
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#1 | ||||
New Member
Wesley T.
Join Date: Apr 2009
Posts: 28
Rep Power: 17 |
What is the correct way to setup a powerLaw viscosity model when using the incompressibleMultiphaseVoF solver?
I am using OpenFOAM 12. I have not found a multiphase tutorial with a non-Newtonian fluid, so do not have a template to build from. I do have the powerLaw model working with the incompressibleFluid and the incompressibleVoF solvers. I built the file structure assuming it should be analogous to the file structure for the incompressibleVoF solver, which I do have running and reading the powerLaw fluid model. I believe the issue is in the “constant” directory because the only issue appears to be that I am not correctly defining the rheological model (powerLaw). The simulation is currently using only the viscosities defined in the two physical properties files. My current file structure for the constant directory is (boundary, faces, neighbour, owner, and points are subdirectories in polyMesh, but I can't get the tree to display correctly: Quote:
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Guidance/help on getting the powerLaw rheological model working with the incompressibleMultiphaseVoF solver is greatly appreciated. |
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October 19, 2024, 12:12 |
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#2 |
New Member
Wesley T.
Join Date: Apr 2009
Posts: 28
Rep Power: 17 |
Until I can work out or told how to setup multiphase non-Newtonian models in OpenFOAM 12, I will use OpenFOAM 9, which uses the previous file structure.
For OpenFOAM 9, I have a directory structure of: Code:
├── 0 │ ├── alpha.ExtrudateA │ ├── alpha.ExtrudateB │ ├── alpha.ExtrudateC │ ├── alphas │ ├── p_rgh │ └── U ├── CoEx3FlowPipe.unv ├── constant │ ├── g │ ├── momentumTransport │ ├── polyMesh │ │ ├── boundary │ │ ├── faces │ │ ├── neighbour │ │ ├── owner │ │ └── points │ └── transportProperties ├── system │ ├── controlDict │ ├── fvSchemes │ └── fvSolution Code:
FoamFile { format ascii; class dictionary; location "constant"; object transportProperties; } // * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * // phases ( ExtrudateA { transportModel powerLaw; powerLawCoeffs { k k [0 2 -1 0 0 0 0] 3000; n n [0 0 0 0 0 0 0] 0.4; nuMin nuMin [0 2 -1 0 0 0 0] .1; nuMax nuMax [0 2 -1 0 0 0 0] 1000000; } rho 1250; } ExtrudateB { transportModel powerLaw; powerLawCoeffs { k k [0 2 -1 0 0 0 0] 300; n n [0 0 0 0 0 0 0] 0.4; nuMin nuMin [0 2 -1 0 0 0 0] .1; nuMax nuMax [0 2 -1 0 0 0 0] 1000000; } rho 1250; } ExtrudateC { transportModel powerLaw; powerLawCoeffs { k k [0 2 -1 0 0 0 0] 300; n n [0 0 0 0 0 0 0] 0.4; nuMin nuMin [0 2 -1 0 0 0 0] .1; nuMax nuMax [0 2 -1 0 0 0 0] 1000000; } rho 1250; } ); sigmas ( (ExtrudateA ExtrudateB) 0.07 (ExtrudateA ExtrudateC) 0.07 (ExtrudateB ExtrudateC) 0.07 ); // ************************************************************************* // Wes |
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Tags |
non-newtonian, powerlaw |
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