An eddy-viscosity model is proposed and applied in large-eddy simulation of turbulent shear flows with quite satisfactory results. The model is essentially not more complicated than the Smagorinsky model, but is constructed in such a way that its dissipation is relatively small in transitional and near-wall regions. The model is expressed in first-order derivatives, does not involve explicit filtering, averaging, or clipping procedures, and is rotationally invariant for isotropic filter widths. Because of these highly desirable properties the model seems to be well suited for engineering applications. In order to provide a foundation of the model, an algebraic framework for general three-dimensional flows is introduced. Within this framework several types of flows are proven to have zero energy transfer to subgrid scales. The eddy viscosity is zero in the same cases; the theoretical subgrid dissipation and the eddy viscosity have the same algebraic structure. In addition, the model is based on a fundamental realizability inequality for the theoretical subgrid dissipation. Results are shown for a transitional and turbulent mixing layer at high Reynolds number and a turbulent channel flow. In both cases the present model is found to be more accurate than the Smagorinsky model and as good as the standard dynamic model. Unlike the Smagorinsky model, the present model is able to adequately handle not only turbulent but also transitional flow.

1.
C.
Meneveau
and
J.
Katz
, “
Scale-invariance and turbulence models for large-eddy simulation
,”
Annu. Rev. Fluid Mech.
32
,
1
(
2000
).
2.
S.B.
Pope
, Turbulent Flows (Cambridge University Press, Cambridge,
2000
).
3.
J.
Smagorinsky
, “
General circulation experiments with the primitive equations
,”
Mon. Weather Rev.
91
,
99
(
1963
).
4.
M.
Germano
,
U.
Piomelli
,
P.
Moin
, and
W. H.
Cabot
, “
A dynamic subgrid-scale eddy-viscosity model
,”
Phys. Fluids A
3
,
1760
(
1991
).
5.
A.
Leonard
, “
Energy cascade in large-eddy simulations of turbulent fluid flows
,”
Adv. Geophys.
18
,
237
(
1974
).
6.
R. A.
Clark
,
J. H.
Ferziger
, and
W. C.
Reynolds
, “
Evaluation of subgrid-scale models using an accurately simulated turbulent flow
,”
J. Fluid Mech.
91
,
1
(
1979
).
7.
B.
Vreman
,
B.
Geurts
, and
H.
Kuerten
, “
Large-eddy simulation of the temporal mixing layer using the Clark model
,”
Theor. Comput. Fluid Dyn.
8
,
309
(
1996
).
8.
B.
Vreman
,
B.
Geurts
, and
H.
Kuerten
, “
Realizability conditions for the turbulent stress tensor in large eddy simulation
,”
J. Fluid Mech.
278
,
351
(
1994
).
9.
A. W.
Vreman
, “
The adjoint filter operator in large-eddy simulation of turbulent flow
,”
Phys. Fluids
16
,
2012
(
2004
).
10.
C. D.
Pruett
and
N. A.
Adams
, “
A priori analyses of three subgrid-scale models for one-parameter families of filters
,”
Phys. Fluids
12
,
1133
(
2000
).
11.
A.W.
Vreman
,
B.J.
Geurts
,
N.G.
Deen
, and
J.A. M.
Kuipers
, “
Large-eddy simulation of a particle-laden turbulent channel flow
,” in Direct and Large-Eddy Simulation V, edited by
R.
Friedrich
,
B. J.
Geurts
, and
O.
Metais
(Kluwer, Dordrecht,
2004
), pp.
271
278
.
12.
U.
Schumann
, “
Subgrid scale model for finite difference simulations of turbulent flows in plane channels and annuli
,”
J. Comput. Phys.
18
,
376
(
1975
).
13.
D.K.
Lilly
, “
The representation of small-scale turbulence in numerical simulation experiments
,” in Proceedings of IBM Scientific Computing Symposium on Environmental Sciences, edited by H. H. Goldstine (Yorktown Heights, New York,
1967
), pp.
195
210
.
14.
W. D.
Urban
and
M. G.
Mungal
, “
Planar velocity measurements in compressible mixing layers
,”
J. Fluid Mech.
431
,
189
(
2001
).
15.
B.
Vreman
,
B.
Geurts
, and
H.
Kuerten
, “
Comparison of numerical schemes in large-eddy simulation of the temporal mixing layer
,”
Int. J. Numer. Methods Fluids
22
,
297
(
1996
).
16.
B.
Vreman
,
B.
Geurts
, and
H.
Kuerten
, “
Large-eddy simulation of the turbulent mixing layer
,”
J. Fluid Mech.
339
,
357
(
1997
).
17.
J. W.
Deardorff
, “
A numerical study of three-dimensional turbulent channel flow at large Reynolds numbers
,”
J. Fluid Mech.
41
,
453
(
1970
).
18.
Z.W.
Hu
and
N.D.
Sandham
, “
DNS databases for turbulent Couette and Poiseuille flow
,” University of Southampton, Report No. AFM-01/04,
2001
(unpublished).
19.
R. D.
Moser
,
J.
Kim
, and
N. N.
Mansour
, “
Direct numerical simulation of turbulent channel flow up to Reτ=590
,”
Phys. Fluids
11
,
943
(
1999
).
20.
S.
Stolz
,
N. A.
Adams
, and
L.
Kleiser
, “
An approximate deconvolution model for large-eddy simulation with application to incompressible wall-bounded flows
,”
Phys. Fluids
13
,
997
(
2001
).
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