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Structural modeling

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Those that use the physical hypothesis of scale similarity
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1. Those that use the physical hypothesis of scale similarity
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Those derived by formal series expansions
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2. Those derived by formal series expansions
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Mixed models, which are based on linear combinations of the eddy-viscosity and structural types
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3. Mixed models, which are based on linear combinations of the eddy-viscosity and structural types
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Dynamic structure models (non-viscosity version)
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4. Dynamic structure models (non-viscosity version)
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\tau_{ij} = 2k_{sgs} \left(\frac{L_{ij}}{L_{kk}}\right)   
\tau_{ij} = 2k_{sgs} \left(\frac{L_{ij}}{L_{kk}}\right)   
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\tau_{ij} = 2k_{sgs} \left(\frac{G_{ij}}{G_{kk}}\right)
\tau_{ij} = 2k_{sgs} \left(\frac{G_{ij}}{G_{kk}}\right)
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== References ==
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*{{reference-paper|author=R. A. Clark and J. H. Ferziger and W. C. Reynolds|year=1979|title=Evaluation of subgrid-scale models using an accurately simulated turbulent flow|rest=J. Fluid Mech.}}

Revision as of 20:03, 25 June 2013

1. Those that use the physical hypothesis of scale similarity


\tau_{ij} = L_{ij} = \widetilde{\bar{u}_i} \widetilde{\bar{u}_j} - \widetilde{\bar{u}_i \bar{u}_j}


2. Those derived by formal series expansions


\tau_{ij} = G_{ij} = \frac{\Delta^2}{12} \frac{\partial \bar{u}_i}{\partial x_{k}} \frac{\partial \bar{u}_j}{\partial x_{k}}

3. Mixed models, which are based on linear combinations of the eddy-viscosity and structural types


\tau_{ij} = G_{ij}-2\nu_{sgs} S_{ij}

or


\tau_{ij} = L_{ij}-2\nu_{sgs} S_{ij}

4. Dynamic structure models (non-viscosity version)


\tau_{ij} = 2k_{sgs} \left(\frac{L_{ij}}{L_{kk}}\right)

or


\tau_{ij} = 2k_{sgs} \left(\frac{G_{ij}}{G_{kk}}\right)

References

  • R. A. Clark and J. H. Ferziger and W. C. Reynolds (1979), "Evaluation of subgrid-scale models using an accurately simulated turbulent flow", J. Fluid Mech..
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