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BUG: fix kkLOmega model - omegaWallFunction inconsistency (#1484)
- `Pkt` was directed to `GName` to allow wall functions
are usable by kkLOmega model
- `Pkt` was changed to a non-const object, so that omegaWallFunc
can modify `Pkt` at the wall, if need be.
- Elementwise backward compatibility was checked by
pimpleFoam/RAS/ellipsekkLOmega
- New implementation was checked by changing omega:hole boundary
in pimpleFoam/RAS/ellipsekkLOmega to omegaWallFunction
This commit is contained in:
@ -636,7 +636,7 @@ void kkLOmega::correct()
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*fINT()
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*Cmu(sqrt(S2))*sqrt(ktS)*lambdaEff
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);
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const volScalarField Pkt(nuts*S2);
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volScalarField Pkt(this->GName(), nuts*S2);
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const volScalarField ktL(kt_ - ktS);
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const volScalarField ReOmega(sqr(y_)*Omega/nu());
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@ -34,25 +34,22 @@ Description
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Low Reynolds-number k-kl-omega turbulence model for
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incompressible flows.
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This turbulence model is described in:
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Reference:
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\verbatim
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Walters, D. K., & Cokljat, D. (2008).
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A three-equation eddy-viscosity model for Reynolds-averaged
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Navier–Stokes simulations of transitional flow.
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Journal of Fluids Engineering, 130(12), 121401.
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Standard model:
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Walters, D. K., & Cokljat, D. (2008).
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A three-equation eddy-viscosity model for Reynolds-averaged
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Navier–Stokes simulations of transitional flow.
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Journal of Fluids Engineering, 130(12), 121401.
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DOI:10.1115/1.2979230
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Typo corrections:
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Furst, J. (2013).
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Numerical simulation of transitional flows
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with laminar kinetic energy.
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Engineering MECHANICS, 20(5), 379-388.
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\endverbatim
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however the paper contains several errors which must be corrected for the
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model to operation correctly as explained in
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\verbatim
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Furst, J. (2013).
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Numerical simulation of transitional flows with laminar kinetic energy.
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Engineering MECHANICS, 20(5), 379-388.
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\endverbatim
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All these corrections and updates are included in this implementation.
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The default model coefficients are
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\verbatim
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kkLOmegaCoeffs
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