A proper velocity scale for modeling subgrid-scale eddy viscosities in large eddy simulation

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 n...

[1]  K. Horiuti,et al.  Assessment of two-equation models of turbulent passive-scalar diffusion in channel flow , 1992, Journal of Fluid Mechanics.

[2]  J. Deardorff A numerical study of three-dimensional turbulent channel flow at large Reynolds numbers , 1970, Journal of Fluid Mechanics.

[3]  D. C. Leslie,et al.  Analysis of a strongly sheared, nearly homogeneous turbulent shear flow , 1980, Journal of Fluid Mechanics.

[4]  K. Horiuti,et al.  Higher‐order terms in the anisotropic representation of Reynolds stresses , 1990 .

[5]  T. Gatski,et al.  Modelling the pressure–strain correlation of turbulence: an invariant dynamical systems approach , 1991, Journal of Fluid Mechanics.

[6]  U. Schumann Subgrid Scale Model for Finite Difference Simulations of Turbulent Flows in Plane Channels and Annuli , 1975 .

[7]  Kiyosi Horiuti The role of the Bardina model in large eddy simulation of turbulent channel flow , 1989 .

[8]  P. Moin,et al.  A dynamic subgrid‐scale eddy viscosity model , 1990 .

[9]  C. G. Speziale Subgrid scale stress models for the large-eddy simulation of rotating turbulent flows , 1985 .

[10]  B. Launder,et al.  Contribution to the second-moment modeling of sublayer turbulent transport , 1990 .

[11]  Akira Yoshizawa,et al.  Statistical analysis of the deviation of the Reynolds stress from its eddy‐viscosity representation , 1984 .

[12]  J. Smagorinsky,et al.  GENERAL CIRCULATION EXPERIMENTS WITH THE PRIMITIVE EQUATIONS , 1963 .

[13]  S. Orszag,et al.  Renormalization group analysis of turbulence. I. Basic theory , 1986 .

[14]  William C. Reynolds,et al.  Measurements in fully developed turbulent channel flow , 1975 .

[15]  B. Launder,et al.  Progress in the development of a Reynolds-stress turbulence closure , 1975, Journal of Fluid Mechanics.

[16]  W. Rodi A new algebraic relation for calculating the Reynolds stresses , 1976 .

[17]  Robert Rubinstein,et al.  Nonlinear Reynolds stress models and the renormalization group , 1990 .

[18]  P. Moin,et al.  Subgrid-scale backscatter in turbulent and transitional flows , 1991 .

[19]  C. G. Speziale On nonlinear K-l and K-ε models of turbulence , 1987, Journal of Fluid Mechanics.

[20]  B. Launder An introduction to single-point closure methodology , 1991 .

[21]  P. Moin,et al.  Turbulence statistics in fully developed channel flow at low Reynolds number , 1987, Journal of Fluid Mechanics.

[22]  P. Moin,et al.  Reynolds-stress and dissipation-rate budgets in a turbulent channel flow , 1987, Journal of Fluid Mechanics.

[23]  S. Orszag,et al.  Renormalization group analysis of turbulence. I. Basic theory , 1986, Physical review letters.

[24]  John L. Lumley,et al.  Computational Modeling of Turbulent Flows , 1978 .

[25]  C. G. Speziale Galilean invariance of subgrid-scale stress models in the large-eddy simulation of turbulence , 1985, Journal of Fluid Mechanics.

[26]  A. Yakhot,et al.  Renormalization group formulation of large-eddy simulations , 1989 .

[27]  D. Lilly,et al.  A proposed modification of the Germano subgrid‐scale closure method , 1992 .

[28]  M. Antonopoulos-Domis,et al.  Large-eddy simulation of a passive scalar in isotropic turbulence , 1981, Journal of Fluid Mechanics.

[29]  V. Wong,et al.  A proposed statistical‐dynamic closure method for the linear or nonlinear subgrid‐scale stresses , 1992 .

[30]  P. Moin,et al.  Model consistency in large eddy simulation of turbulent channel flows , 1988 .

[31]  E. R. V. Driest On Turbulent Flow Near a Wall , 1956 .

[32]  Akira Yoshizawa,et al.  Turbulent channel and Couette flows using an anisotropic k-epsilon model , 1987 .

[33]  J. Ferziger,et al.  Evaluation of subgrid-scale models using an accurately simulated turbulent flow , 1979, Journal of Fluid Mechanics.

[34]  K. Horiuti,et al.  Comparison of conservative and rotational forms in large Eddy simulation of turbulent channel flow , 1987 .

[35]  P. Moin,et al.  Numerical Simulation of Turbulent Flows , 1984 .

[36]  C. Leith,et al.  Developments in the theory of turbulence , 1973 .

[37]  P. Durbin Near-wall turbulence closure modeling without “damping functions” , 1991, Theoretical and Computational Fluid Dynamics.

[38]  P. J. Mason,et al.  On the magnitude of the subgrid-scale eddy coefficient in large-eddy simulations of turbulent channel flow , 1986, Journal of Fluid Mechanics.

[39]  P. Moin,et al.  Numerical investigation of turbulent channel flow , 1981, Journal of Fluid Mechanics.

[40]  K. Lilly On the application of the eddy viscosity concept in the Inertial sub-range of turbulence , 1966 .

[41]  Hans Edelmann,et al.  Vier Woodbury-Formeln hergeleitet aus dem Variablentausch einer speziellen Matrix , 1976 .