3.8 Proceedings Paper

The Dynamics of Turbulent Scalar Mixing near the Edge of a Shear Layer

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IOP PUBLISHING LTD
DOI: 10.1088/1742-6596/318/5/052049

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In free shear flows a sharp and convoluted turbulent/nonturbulent (T/NT) interface separates the outer fluid region, where the flow is essentially irrotational, from the shear layer turbulent region. It was found recently that the entrainment mechanism is mainly caused by small scale ( nibbling) motions (Westerweel et al. (2005)). The dynamics of this interface is crucial to understand important exchanges of enstrophy and scalars that can be conceived as a three-stage process of entrainment, dispersion and diffusion (Dimotakis (2005)). A thorough understanding of scalar mixing and transport is of indisputable relevance to control turbulent combustion, propulsion and contaminant dispersion (Stanley et al. (2002)). The present work uses several DNS of turbulent jets at Reynolds number ranging from Re-lambda = 120 to Re-lambda = 160 (da Silva & Taveira (2010)) and a Schmidt number Sc - 0.7 to analyze the scalar interface and turbulent mixing of a passive scalar. Specifically, we employ conditional statistics, denoted by <>(I), in order to eliminate the intermittency that affects statistics close to the jet edge. The physical mechanisms behind scalar mixing near the T/NT interfaces, their scales and topology are investigated detail. Analysis of the instantaneous fields showed intense scalar gradient sheet-like structures along regions of persistent strain, in particular at the T/NT interface. The scalar gradient transport equation, at the jet edge, showed that almost all mixing mechanisms are taking place in a confined region, beyond which they become reduced to an almost in perfect balance between production and dissipation of scalar variance. At the T/NT interface transport mechanisms are the ones responsible for the growth in the scalar fluctuations to the entrained fluid, where convection plays a dominant role, smoothing scalar gradients inside the interface (0.1 yI/lambda to 1 yI/lambda) and boosting them as far as -2.5 yI/eta(C)(0).

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