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Vorticity-dependent and symmetry-preserving LES models

Oscar Cosserat, Dina Razafindralandy, Can Selçuk

TL;DR

The paper develops a Lie-group–based framework to construct symmetry-preserving SGS models for the incompressible NS equations, with closures that depend on the filtered strain-rate $S$ and vorticity $Omega$. It-derived invariant tensor forms under $G_t$, $Gal$, $SO(3)$, $G_p$, and $G_s$, and shows how $ au^d$ can be expressed as a potential-driven closure using a scalar function $g$ of invariants, guaranteeing positive total dissipation under convexity conditions. A central result links the SGS tensor to a potential $ ewphi$, yielding explicit forms in terms of a generating function $g(v_1,v_3,v_4)$ and establishing a convexity-based criterion for stability. The work positions these symmetry-preserving models alongside established SGS approaches, outlining pathways for numerical validation and extensions to multiphase and wall-boundary contexts.

Abstract

Within the Large Eddy Simulation framework, we propose a methodology based on the Lie theory to derive symmetry-preserving turbulence models. We apply this methodology to the incompressible Navier-Stokes equations.} These models explicitly depend on both the filtered strain-rate tensor and the filtered vorticity tensor. Particular emphasis is placed on models that additionally ensure stability.

Vorticity-dependent and symmetry-preserving LES models

TL;DR

The paper develops a Lie-group–based framework to construct symmetry-preserving SGS models for the incompressible NS equations, with closures that depend on the filtered strain-rate and vorticity . It-derived invariant tensor forms under , , , , and , and shows how can be expressed as a potential-driven closure using a scalar function of invariants, guaranteeing positive total dissipation under convexity conditions. A central result links the SGS tensor to a potential , yielding explicit forms in terms of a generating function and establishing a convexity-based criterion for stability. The work positions these symmetry-preserving models alongside established SGS approaches, outlining pathways for numerical validation and extensions to multiphase and wall-boundary contexts.

Abstract

Within the Large Eddy Simulation framework, we propose a methodology based on the Lie theory to derive symmetry-preserving turbulence models. We apply this methodology to the incompressible Navier-Stokes equations.} These models explicitly depend on both the filtered strain-rate tensor and the filtered vorticity tensor. Particular emphasis is placed on models that additionally ensure stability.

Paper Structure

This paper contains 11 sections, 4 theorems, 59 equations.

Key Result

Theorem 1

Let ${ \mathsfbi{\tau} }$ be the subgrid tensor with deviatoric part where $\alpha_1, ..., \alpha_7$ are abitrary scalar functions of the variables $\left(I_1,I_2,B_1,B_2,B_3,B_4 \right)$ defined by Then ${ \mathsfbi{\tau} }$ is invariant under the symmetry groups $G_t$, $Gal$, $SO(3)$ and $G_p$. Moreover, the representation (eq_tau_zheng) is minimal.

Theorems & Definitions (11)

  • Theorem 1
  • proof
  • Remark 1
  • Theorem 2
  • proof
  • Remark 2
  • Theorem 3
  • proof
  • Remark 3
  • Theorem 4
  • ...and 1 more