Changed species' diffusivity to alphaEff
All multi-specie solvers function on the assumption that the mass-diffusivities of the different species are the same. A consequence of this is that the diffusivities of energy and mass must be the same, otherwise mass diffusivity results in unphysical temperature fluctuations. This change enforces this requirement across all multi-species solvers. For the same reason, the turbulent Schmidt number has been removed from the multi-component phase model in reactingEulerFoam. In order to obey physical constraints this Schmidt number had to be exactly the same as the Prandtl number. This condition is now enforced by the solver, rather than relying on the input being correct.
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@ -28,7 +28,6 @@ gas
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d0 3e-3;
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p0 1e5;
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}
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Sct 0.7;
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residualAlpha 1e-6;
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}
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@ -28,7 +28,6 @@ gas
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d0 3e-3;
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p0 1e5;
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}
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Sct 0.7;
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residualAlpha 1e-6;
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}
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@ -28,7 +28,6 @@ gas
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d0 3e-3;
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p0 1e5;
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}
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Sct 0.7;
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residualAlpha 1e-6;
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}
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@ -41,7 +40,6 @@ liquid
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{
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d 1e-4;
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}
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Sct 0.7;
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residualAlpha 1e-6;
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}
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@ -30,7 +30,6 @@ steam
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d0 3e-3;
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p0 1e5;
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}
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Sct 0.7;
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residualAlpha 1e-3;
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}
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@ -43,7 +42,6 @@ water
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{
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d 1e-4;
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}
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Sct 0.7;
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residualAlpha 1e-3;
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}
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@ -80,8 +80,6 @@ particles
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);
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}
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Sct 1.0;
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residualAlpha 1e-15;
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}
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@ -95,8 +93,6 @@ vapor
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d 1;
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}
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Sct 1.0;
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residualAlpha 1e-5;
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}
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