1995
DOI: 10.1017/s0022112095000711
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A dynamic localization model for large-eddy simulation of turbulent flows

Abstract: In a previous paper, Germano, et al. (1991) proposed a method for computing coefficients of subgrid-scale eddy viscosity models as a function of space and time. This procedure has the distinct advantage of being self-calibrating and requires no a priori specification of model coefficients or the use of wall damping functions. However, the original formulation contained some mathematical inconsistencies that limited the utility of the model. In particular, the applicability of the model was restricted to flows … Show more

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Cited by 663 publications
(363 citation statements)
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References 14 publications
(24 reference statements)
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“…If in a particular application one aims at the prediction of a time-reversed flow without risking an unlimited amount of backscatter, one can use one of the models given by (10) and (11). A more sophisticated, but also more physical, procedure was proposed by Ghosal et al 26 by basing the flux of energy to the small scales on the subgrid scale energy, which was computed using a transport equation for the Reynolds averaged subgrid scales. This procedure implicitly assumes that the net energy flux from the resolved scales to the subgrid scales is determined by the subgrid energy.…”
Section: Results For Reversed Turbulence From Large Eddy Simulationsmentioning
confidence: 99%
“…If in a particular application one aims at the prediction of a time-reversed flow without risking an unlimited amount of backscatter, one can use one of the models given by (10) and (11). A more sophisticated, but also more physical, procedure was proposed by Ghosal et al 26 by basing the flux of energy to the small scales on the subgrid scale energy, which was computed using a transport equation for the Reynolds averaged subgrid scales. This procedure implicitly assumes that the net energy flux from the resolved scales to the subgrid scales is determined by the subgrid energy.…”
Section: Results For Reversed Turbulence From Large Eddy Simulationsmentioning
confidence: 99%
“…where P = p−1/3τ kk denotes the modified pressure, b i the kinematic body force per unit volume, S ij the symmetric part of the deformation rate tensor, t the time, τ ij the SGS stress tensor, and E SG the SGS kinetic energy; the negative trace of τ kk follows from the positive filter kernel (see, Ghosal et al , 1995). In the following we drop use of the hat for convenience unless explicitly required.…”
Section: Governing Equationsmentioning
confidence: 99%
“…3,4 Some mathematical inconsistencies which arise in the dynamical formulation can be resolved by casting the problem in variational form, resulting in the dynamic localization model. 5 In applications, simplified solutions to the difficulties arising in the dynamic procedure are widely used, for example plane averaging in homogeneous directions 3 or approximate localization. 6 A related class of SGS models are the spectral eddyviscosity models.…”
Section: Introductionmentioning
confidence: 99%