4.2 Article

The effect of subgrid-scale models on the entrainment of a passive scalar in a turbulent planar jet

Journal

JOURNAL OF TURBULENCE
Volume 16, Issue 4, Pages 342-366

Publisher

TAYLOR & FRANCIS LTD
DOI: 10.1080/14685248.2014.986329

Keywords

turbulent entrainment; large-eddy simulation (LES); jet; turbulent; non-turbulent interface (TNTI); passive scalar

Funding

  1. Portuguese Foundation for Science and Technology (FCT) [SFRH/BD/46036/2008]
  2. Fundação para a Ciência e a Tecnologia [SFRH/BD/46036/2008] Funding Source: FCT

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Classical large-eddy simulation (LES) modelling assumes that the passive subgrid-scale (SGS) models do not influence large-scale quantities, even though there is now ample evidence of this in many flows. In this work, direct numerical simulation (DNS) and large-eddy simulations of turbulent planar jets at Reynolds number Re-H = 6000 including a passive scalar with Schmidt number Sc = 0.7 are used to study the effect of several SGS models on the flow integral quantities e.g. velocity and scalar jet spreading rates. The models analysed are theSmagorinsky, dynamic Smagorinsky, shear-improved Smagorinsky and the Vreman. Detailed analysis of the thin layer bounding the turbulent and non-turbulent regions - the so-called turbulent/non-turbulent interface (TNTI) - shows that this region raises new challenges for classical SGS models. The small scales are far from equilibrium and contain a high fraction of the total kinetic energy and scalar variance, but the situation is worse for the scalar than for the velocity field. Both a-priori and a-posteriori (LES) tests show that the dynamic Smagorinsky and shear-improved models give the best results because they are able to accurately capture the correct statistics of the velocity and passive scalar fluctuations near the TNTI. The results also suggest the existence of a critical resolution (x), of the order of the Taylor scale , which is needed for the scalar field. Coarser passive scalar LES i.e. (x) results in dramatic changes in the integral quantities. This fact is explained by the dynamics of the small scales near the jet interface.

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