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Abstract

This letter presents a kinetic closure of the filtered Boltzmann-BGK equation, paving the way towards an alternative description of turbulence. The closure naturally incorporates the turbulent subfilter stress tensor without the need for explicit modeling, unlike in Navier-Stokes models. In contrast, it accounts for the subfilter turbulent diffusion in the nonconserved moments by generalizing the BGK collision operator. The model requires neither scale separation nor a Smagorinsky-type ansatz for the subfilter stress tensor. The Chapman-Enskog analysis shows that its hydrodynamic limit converges exactly to the filtered Navier-Stokes equations, with velocity gradients isolating subfilter contributions. Validations through lattice Boltzmann simulations of the Taylor-Green vortex and the turbulent mixing layer demonstrate improved stability and reduced dissipation, benchmarked against the Smagorinsky model.