4.7 Article

Scalar mixing in a Kelvin-Helmholtz shear layer and implications for Reynolds-averaged Navier-Stokes modeling of mixing layers

Journal

PHYSICAL REVIEW E
Volume 103, Issue 5, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevE.103.053108

Keywords

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Funding

  1. US Department of Energy by Lawrence Livermore National Laboratory [DE-AC52-07NA27344]

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This study involves large-eddy simulations of a Kelvin-Helmholtz mixing layer, showing similarities in scalar variance integral behavior with a Rayleigh-Taylor mixing layer and a tendency towards mixedness of about 0.8 in the simulated KH shear layer. It is found that using a Reynolds-averaged Navier-Stokes model calibrated for an RT layer to simulate a KH layer results in significant overprediction of scalar variance, suggesting the addition of a buoyancy production term to match mixedness in simulations of both RT and KH layers with a single model calibration.
Large-eddy simulation of a temporally evolving Kelvin-Helmholtz (KH) mixing layer is performed with the tenth-order compact difference code MIRANDA to examine the steady-state behavior of a passive scalar in a shear-driven mixing layer. It is shown that the integral behavior of scalar variance in a KH mixing layer behaves similarly to the integral behavior of scalar variance in a Rayleigh-Taylor (RT) mixing layer, and mixedness of the simulated KH shear layer tends towards a value of about 0.8. It is further shown that if the k-L-a-V Reynolds-averaged Navier-Stokes (RANS) model [B. E. Morgan et al., Phys. Rev. E 98, 033111 (2018)], calibrated to reproduce steady-state mixing in an RT layer, is applied to simulate a KH mixing layer, the RANS model will significantly overpredict the magnitude of scalar variance in the KH layer. A straightforward addition to the k-L-a-V model is then suggested, and self-similarity analysis is applied to determine constraints on model coefficients. It is shown that with the addition of a buoyancy production term in the model equation for scalar variance, it becomes possible to eliminate the model deficiency and match steady-state mixedness in simulations of both RT and KH mixing layers with a single model calibration.

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