2002
DOI: 10.1142/s0218202502002057
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Mathematical Analysis for the Rational Large Eddy Simulation Model

Abstract: In this paper we consider the Rational Large Eddy Simulation model recently introduced by Galdi and Layton. We briefly present this model, which (in principle) is similar to others commonly used, and we prove the existence and uniqueness of a class of strong solutions. Contrary to the gradient model, the main feature of this model is that it allows a better control of the kinetic energy. Consequently, to prove existence of strong solutions, we do not need subgrid-scale regularization operators, as proposed by … Show more

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Cited by 27 publications
(20 citation statements)
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“…Results in [4,1] show that the term ∇ · (I − α 2 2 ∆) −1 α 2 ∇w∇w T plays the same role (in terms of Sobolev spaces inequalities) of the convective term. This prevents from proving global-in-time estimates.…”
Section: Some Properties Of the Horizontal Rational/clark Modelmentioning
confidence: 98%
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“…Results in [4,1] show that the term ∇ · (I − α 2 2 ∆) −1 α 2 ∇w∇w T plays the same role (in terms of Sobolev spaces inequalities) of the convective term. This prevents from proving global-in-time estimates.…”
Section: Some Properties Of the Horizontal Rational/clark Modelmentioning
confidence: 98%
“…It is well-known that instabilities occur in the numerical implementation and that some kind of smoothing must be added in order to have effective simulations, see [17]. In particular, a filtered version of the Gradient method is called Rational or 4 Clark-α method, and the stress-tensor reads as…”
Section: An Anisotropic Large Eddy Simulation Modelmentioning
confidence: 99%
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“…35 The mathematical analysis associated with the RLES model ͑12͒ was presented in Ref. 36. The first steps in the numerical analysis and validation of the RLES model ͑12͒ were made in Refs.…”
Section: ͑12͒mentioning
confidence: 99%