Entrainment in variable-density jets

doi:10.1017/jfm.2024.704

2024-09-20

PRE

DOI：10.1017/jfm.2024.704

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摘要

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The entrainment of ambient fluid into a variable-density jet is typically quantified using an entrainment coefficient alpha. Here, we investigate the dependence of alpha on the ratio of the jet's density rho(m) and that of the ambient fluid rho(0). Current parametrisations of alpha rely on a scaling inferred from early laboratory experiments (Ricou & Spalding, J. Fluid Mech., vol. 11, 1961, pp. 21-32). We demonstrate analytically that the experiments preclude definitive conclusions regarding the dependence of alpha on rho(m)/rho(0) and that the underlying physical processes therefore warrant closer attention. To investigate the physics behind the dependence of entrainment on the density ratio we use a Favre-averaged entrainment decomposition. The decomposition is applied to data from large-eddy simulations of jets characterised by density ratios rho(m)/rho(0) spanning over two orders of magnitude that have been verified against experimental data. Changes in the shape of the velocity profile are a significant contributor to entrainment in the near field due to the breakdown of the potential core, and persist over larger streamwise distances in heavy releases than in light releases. Therefore, to focus exclusively on the effects of density ratio, we study the region where the shape changes have become small but the density ratio is still significant. We show that the dimensionless turbulent kinetic energy production and mean kinetic energy flux depend strongly on the density ratio, both for our large-eddy simulation data and for recent experiments. Despite this, the entrainment coefficient is practically constant in this region and has value alpha approximate to 0.07 for all simulations.

Keyword:

turbulent mixing

shear layer turbulence

jets