A proper velocity scale for modeling subgrid-scale eddy viscosities in large eddy simulation
- 1 January 1993
- journal article
- research article
- Published by AIP Publishing in Physics of Fluids A: Fluid Dynamics
- Vol. 5 (1) , 146-157
- https://doi.org/10.1063/1.858800
Abstract
The limitations of the commonly used Smagorinsky subgrid‐scale (SGS) eddy viscosity model in large eddy simulation (LES) of turbulent flows are that the model’s eddy viscosity constant must be optimized in different flows, and also that a damping function must be used to account for near‐wall effects. A new SGS model which mitigates these drawbacks is proposed, i.e., a more proper eddy viscosity velocity scale was determined by utilizing the third‐order terms in an anisotropic representation model of the Reynolds stresses [K. Horiuti, Phys. Fluids A 2, 1708 (1990)]. This method utilizes the direct numerical simulation (DNS) database for fully developed turbulent channel flow to show these drawbacks to be inherent in the use of an improper velocity scale, i.e., the total SGS energy component adopted in the Smagorinsky model. As a result, the SGS normal shear stress was alternatively employed as the velocity scale, thereby significantly improving the correlation with DNS data. Methods to correlate the SGS normal shear stress to the grid scale quantities are proposed and compared, and the resultant high accuracy of the scale‐similarity model to represent the SGS turbulence fluctuations is shown. The proposed SGS model was also tested in actual LES computations of turbulent channel flow, where it was found that the SGS eddy viscosity in the near‐wall region similarly acted as the conventionally used Van Driest damping function. This result is consistent with previous reports which assert that in the Reynolds averaged models, the rapid reduction of the Reynolds shear stress as the wall is approached is due to the preferential damping of the normal shear stress. It is shown that three eddy viscosity parameters contained in the proposed SGS model can be practically reduced to a single parameter, which is subsequently shown to be more universal and independent of the flow field than the Smagorinsky model constant. A qualitative interpretation for the variance of the Smagorinsky model constant in different flows is also provided via a correlation with the anisotropy of SGS turbulence intensities.Keywords
This publication has 35 references indexed in Scilit:
- Assessment of two-equation models of turbulent passive-scalar diffusion in channel flowJournal of Fluid Mechanics, 1992
- Subgrid-scale backscatter in turbulent and transitional flowsPhysics of Fluids A: Fluid Dynamics, 1991
- Renormalization group formulation of large-eddy simulationsJournal of Scientific Computing, 1989
- The role of the Bardina model in large eddy simulation of turbulent channel flowPhysics of Fluids A: Fluid Dynamics, 1989
- Reynolds-stress and dissipation-rate budgets in a turbulent channel flowJournal of Fluid Mechanics, 1988
- Turbulent channel and Couette flows using an anisotropic k-epsilon modelAIAA Journal, 1987
- On the magnitude of the subgrid-scale eddy coefficient in large-eddy simulations of turbulent channel flowJournal of Fluid Mechanics, 1986
- Subgrid scale stress models for the large-eddy simulation of rotating turbulent flowsGeophysical & Astrophysical Fluid Dynamics, 1985
- Galilean invariance of subgrid-scale stress models in the large-eddy simulation of turbulenceJournal of Fluid Mechanics, 1985
- Numerical Simulation of Turbulent FlowsAnnual Review of Fluid Mechanics, 1984