4.7 Article

Wake-induced transition in the low-Reynolds-number flow over a multi-element airfoil

期刊

JOURNAL OF FLUID MECHANICS
卷 915, 期 -, 页码 -

出版社

CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2021.20

关键词

vortex dynamics; vortex interactions; turbulent transition

资金

  1. National Natural Science Foundation of China [91852206, 11721202]

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The study investigates the wake-induced transition of a multi-element airfoil and finds that the double-secondary vortices triggered by the slat wake play a crucial role in the transition process, leading to stronger fluctuations and eventually contributing to an attached turbulent boundary layer.
Time-resolved particle image velocimetry and hydrogen bubble visualization are used to investigate the wake-induced transition of a 30P30N multi-element airfoil at a fixed angle of attack of 4 degrees within the stowed chord Reynolds-number range of 1.38 x 10(4) to 3.05 x 10(4). A special transition routine, strongly affected by the slat wake, is observed in the confluent boundary layer over the 30P30N airfoil. In particular, the effects of slat-wake-triggered double-secondary vortices on the whole transition process are explored in detail. At the initial transition stage, the strong slat-wake disturbances penetrate the boundary layer of the main element and are then amplified by double-exponential growth to generate double-secondary vortices. Compared to the scenarios of simplified geometries (He et al., J. Fluid Mech., vol. 718, 2013, pp. 116-130; He & Wang, Phys. Fluids, vol. 27, 2015, 024106), the double-exponential growth provides stronger fluctuations for the transition. At the intermediate transition stage, the wake disturbances trigger the three-dimensional destabilization of these secondary vortices by direct injection or indirect induction, leading to A vortices. The spanwise wavelength of the consequent A vortices is therefore locked on by the wake disturbances. At the late transition stage, the A vortices evolve into hairpin vortex packets and finally contribute to an attached turbulent boundary layer above the main element. Throughout the transition process, no obvious separation occurs in the mean flow above the main element, revealing potential aerodynamic benefits.

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