The transport equation of subgrid scale (SGS) kinetic energy, , is used for the large-eddy simulation (LES), considering its consistency with dynamic procedure. The dynamically determined parameter is suitable for describing the energy transfer from resolved turbulence to SGS portion. Thus the procedure is applied to the production term in the transport equation of , while the eddy viscosity in the filtered equation of motion is determined indirectly through . The statistically derived model for equation is adopted for the basis of our improvement. Computational examination has been conducted for fully developed turbulent flow in a plane channel. Agreement with DNS database was satisfactory. Moreover, in a channel on solid body rotation, our model reasonably reproduced the decay of SGS turbulence in the vicinity of the suction side.
Issue Section:
Technical Papers
1.
Smagorinsky
, J.
, 1963, “General Circulation Experiments With the Primitive Equations
,” Mon. Weather Rev.
0027-0644, 91
, pp. 99
–164
.2.
Germano
, M.
, Piomelli
, U.
, Moin
, P.
, and Cabot
, W. H.
, 1991, “A Dynamic Subgrid-Scale Eddy Viscosity Model
,” Phys. Fluids A
0899-8213, 3
(7
), pp. 1760
–64
.3.
Lilly
, D. K.
, 1992, “A Proposed Modification of the Germano Subgrid Scale Closure Method
,” Phys. Fluids A
0899-8213, 4
(3
), pp. 633
–635
.4.
Yoshizawa
, A.
, and Horiuti
, K.
, 1985, “A Statistically-Derived Subgrid-Scale Kinetic Energy Model for the Large-Eddy Simulation of Turbulent Flows
,” J. Phys. Soc. Jpn.
0031-9015, 54
(8
), pp. 2834
–2839
.5.
Horiuti
, K.
, 1985, “Large Eddy Simulation of Turbulent Channel Flow by One-Equation Modeling
,” J. Phys. Soc. Jpn.
0031-9015, 54
(8
), pp. 2855
–2866
.6.
Okamoto
, M.
, and Shima
, N.
, 1999, “Investigation for the One-Equation-Type Subgrid Model With Eddy-Viscosity Expression Including the Shear-Dumping Effect
,” JSME Int. J., Ser. B
1340-8054, 42
(2
), pp. 154
–161
.7.
Ghosal
, S.
, Lund
, T. S.
, Moin
, P.
, and Akselvoll
, K.
, 1995, “A Dynamic Localization Model for Large-Eddy Simulation of Turbulent Flows
,” J. Fluid Mech.
0022-1120, 286
, pp. 229
–255
.8.
Davidson
, L.
, 1997, “Large Eddy Simulation: A Dynamic One-Equation Subgrid Model for Three-Dimensional Recirculating Flow
,” 11th International Symposium on Turbulent Shear Flow
, Vol. 3
, pp. 26.1
–26.6
.9.
Sohankar
, A.
, Davidson
, L.
, and Norberg
, C.
, 2000, “Large Eddy Simulation of Flow Past a Square Cylinder: Comparison of Different Subgrid Scale Models
,” ASME J. Fluids Eng.
0098-2202, 122
, pp. 39
–47
.10.
Moser
, R. D.
, Kim
, J.
, and Mansour
, N. N.
, 1999, “Direct Numerical Simulation of Turbulent Channel Flow up to Reτ=590
,” Phys. Fluids
1070-6631, 11
(4
), pp. 943
–945
.11.
Horiuti
, K.
, 1990, “Higher-Order Terms in the Anisotropic Representation of Reynolds Stresses
,” Phys. Fluids A
0899-8213, 2
(10
), pp. 1708
–1710
.12.
Horiuti
, K.
, 1993, “A Proper Velocity Scale for Modeling Subgrid-Scale Eddy Viscosities in Large Eddy Simulation
,” Phys. Fluids A
0899-8213, 5
(1
), pp. 146
–157
.13.
Jones
, W. P.
, and Launder
, B. E.
, 1972, “The Prediction of Laminarization With a Two-Equation Model of Turbulence
,” Int. J. Heat Mass Transfer
0017-9310, 15
, pp. 301
–314
.14.
Kajishima
, T.
, Ohta
, T.
, Okazaki
, K.
, and Miyake
, Y.
, 1998, “High-Order Finite-Difference Method for Incompressible Flows Using Collocated Grid System
,” JSME Int. J., Ser. B
1340-8054, 41
(4
), pp. 830
–839
.15.
Leonard
, A.
, 1974, “On the Energy Cascade in Large-Eddy Simulation of Turbulent Fluid Flows
,” Adv. Geophys.
0065-2687, 18A
, pp. 237
–248
.16.
Morinishi
, Y.
, and Vasilyev
, O. V.
, 2001, “A Recommended Modification to the Dynamic Two-Parameter Mixed Subgrid Scale Model for Large Eddy Simulation of Wall Bounded Turbulent Flow
,” Phys. Fluids
1070-6631, 13
(11
), pp. 3400
–3411
.17.
Miyake
, Y.
, and Kajishima
, T.
, 1986a, “Numerical Simulation of the Effects of Coriolis Force on the Structure of Turbulence: 1st Report, Global Effects
,” Bull. JSME
0021-3764, 29
(256
), pp. 3341
–3346
.18.
Miyake
, Y.
, and Kajishima
, T.
, 1986b, “Numerical Simulation of the Effects of Coriolis Force on the Structure of Turbulence: 2nd Report, Structure of Turbulence
,” Bull. JSME
0021-3764, 29
(256
), pp. 3347
–3351
.19.
Kristoffersen
, R.
, and Andersson
, H.
, 1993, “Direct Simulations of Low-Reynolds-Number Turbulent Flow in a Rotationg Channel
,” J. Fluid Mech.
0022-1120, 256
, pp. 163
–197
.Copyright © 2006
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