Abstract

A nonlinear spectral model in terms of spherically averaged descriptors is derived for the prediction of homogeneous turbulence dynamics in the presence of arbitrary mean-velocity gradients. The governing equations for the tensor $\hat{\unicode[STIX]{x1D619}}_{ij}(\boldsymbol{k},t)$, the Fourier transform of the two-point second-order correlation tensor, are first closed by an anisotropic eddy-damped quasinormal Markovian procedure. This closure is restricted to turbulent flows where linear effects induced by mean-flow gradients have no essential qualitative effects on the dynamics of triple correlations compared with the induced production effects in the equations for second-order correlations. Truncation at the first relevant order of spectral angular dependence allows us to derive from these equations in vector $\boldsymbol{k}$ our final model equations in terms of the wavenumber modulus $k$ only. Analytical spherical integration results in a significant decrease in computational cost. Besides, the model remains consistent with the decomposition in terms of directional anisotropy and polarization anisotropy, with a spherically averaged anisotropic spectral tensor for each contribution. Restriction of anisotropy to spherically averaged descriptors, however, entails a loss of information, and realizability conditions are considered to quantify the upper boundary of anisotropy that can be investigated with the proposed model. Several flow configurations are considered to assess the validity of the present model. Satisfactory agreement with experiments on grid-generated turbulence subjected to successive plane strains is observed, which confirms the capability of the model to account for production of anisotropy by mean-flow gradients. The nonlinear transfer terms of the model are further tested by considering the return to isotropy (RTI) of different turbulent flows. Different RTI rates for directional anisotropy and polarization anisotropy allow us to correctly predict the apparent delayed RTI shown after axisymmetric expansion. The last test case deals with homogeneous turbulence subjected to a constant pure plane shear. The interplay between linear and nonlinear effects is reproduced, yielding the eventual exponential growth of the turbulent kinetic energy.

Highlights

  • Homogeneous anisotropic turbulence is a very important topic in turbulence theory, since it allows for a detailed analysis of linear and nonlinear effects of the mean-flow gradient on turbulence dynamics

  • The governing equations for the tensor Rij(k, t), the Fourier transform of the two-point second-order correlation tensor, are first closed by an anisotropic eddy-damped quasinormal Markovian procedure. This closure is restricted to turbulent flows where linear effects induced by mean-flow gradients have no essential qualitative effects on the dynamics of triple correlations compared with the induced production effects in the equations for second-order correlations

  • The present model is suited for the study of turbulent flows where the anisotropy is moderate and where linear effects induced by mean-velocity gradients play a negligible role in the dynamics of triple correlations compared with those directly induced in the equations for second-order correlations

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Summary

Introduction

Homogeneous anisotropic turbulence is a very important topic in turbulence theory, since it allows for a detailed analysis of linear and nonlinear effects of the mean-flow gradient on turbulence dynamics. Canuto & Dubovikov (1996a,b,c) These models do not give a detailed insight into anisotropy, since they rely on a strictly isotropic transfer term as in homogeneous isotropic turbulence. This work relies on an exact treatment of the linear operators induced by mean-velocity gradients in the governing equation for the spectral tensor Rij(k, t), which is permitted by the k-space level of description of the proposed model. The latter was used to perform an exhaustive analytical study of homogeneous turbulence subjected to a constant pure plane shear without limitations on time or wavenumber

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