4.7 Article

Spatial evolution of the turbulent/turbulent interface geometry in a cylinder wake

Journal

JOURNAL OF FLUID MECHANICS
Volume 969, Issue -, Pages -

Publisher

CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2023.547

Keywords

turbulent mixing; intermittency; wakes

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This study examines the spatial evolution of the geometrical features of the turbulent/turbulent interface (TTI) in a cylinder wake. Comparisons are made to a turbulent/non-turbulent interface (TNTI) by exposing the wake to various turbulent backgrounds. It is found that the TTI spreads faster towards the ambient flow than the TNTI, and a transition region of the interfaces' spreading is observed. Moreover, the positions of both the TNTI and TTI exhibit non-Gaussian probability density functions (PDFs) in the near wake due to the influence of large-scale coherent motions.
This study aims to examine the spatial evolution of the geometrical features of the turbulent/turbulent interface (TTI) in a cylinder wake. The wake is exposed to various turbulent backgrounds in which the turbulence intensity and the integral length scale are varied independently, and comparisons to a turbulent/non-turbulent interface (TNTI) are drawn. The turbulent wake was marked with a high Schmidt number (Sc) scalar, and a planar laser induced fluorescence experiment was carried out to capture the interface between the wake and the ambient flow from x/d = 5 to 40, where x is the streamwise coordinate from the centre of the cylinder, and d is the cylinder's diameter. It is found that the TTI generally spreads faster towards the ambient flow than the TNTI. A transition region of the interfaces' spreading is found at x/d approximate to 15, after which the interfaces propagate at a slower rate than previously (upstream), and the mean interface positions of both the TNTI and TTI scale with the local wake half-width. The locations of both the TNTI and TTI have non-Gaussian probability density functions (PDFs) in the near wake because of the influence of the large-scale coherent motions present within the flow. Further downstream, after the large-scale coherent motions have dissipated, the TNTI position PDF does become Gaussian. For the first time, we explore the spatial variation of the `roughness' of the TTI, quantified via the fractal dimension, from near field to far field. The length scale in the background flow has a profound effect on the TTI fractal dimension in the near wake, whilst the turbulence intensity becomes important only for the fractal dimension farther downstream.

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