Title | ||
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Lattice-Boltzmann hydrodynamics of single-square-grid generated turbulence - a partial entropic stabilisation approach |
Abstract | ||
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Under-resolved direct numerical simulations of turbulence in the wake of a single-square-grid (SSG) are conducted using the lattice-Boltzmann method (LBM), with varying degrees of partial moment entropic stabilisation. Turbulence statistics along the grid centreline show satisfactory agreement with literature, greatly outperforming a control study employing the single-relaxation-time Smagorinsky LES model with equivalent resolution. The coarse-resolution entropic LBM simulations are able to capture the qualitative behaviour of the anisotropic and non-homogeneous turbulence generated by the SSG, indicating possible extension of the capability of the entropic lattice-Boltzmann method to simulate more exotic forms of turbulence beyond those reported by the majority of current studies. However, in the extreme near field of the single-square-grid, pseudo-compressibility effects, even at a low lattice Mach number, undermine LBM predictions for turbulence which is generated by action of the pressure Hessian — this is found to be an issue for all models studied, and not a numerical artefact of the entropic stabilisation. With regard to the action of the entropic stabiliser, a comparison of models employing differing degrees of stabilisation on higher-order natural moments suggest that the trace of the stress tensor should not be subject to entropic control for better accuracy in turbulence prediction. |
Year | DOI | Venue |
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2020 | 10.1016/j.camwa.2020.06.013 | Computers & Mathematics with Applications |
Keywords | DocType | Volume |
Lattice-Boltzmann method,Partial entropic stabilisation,Large-eddy simulation,Turbulence,Space-filling grid,Single square grid | Journal | 80 |
Issue | ISSN | Citations |
5 | 0898-1221 | 0 |
PageRank | References | Authors |
0.34 | 0 | 3 |
Name | Order | Citations | PageRank |
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Chin Vern Yeoh | 1 | 0 | 0.34 |
E. H. Ooi | 2 | 17 | 10.03 |
Ji Jinn Foo | 3 | 0 | 0.68 |