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首页> 外文期刊>Journal of Fluid Mechanics >Wake-induced transition in the low-Reynolds-number flow over a multi-element airfoil
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Wake-induced transition in the low-Reynolds-number flow over a multi-element airfoil

机译:在多元素翼型上的低雷诺数流动中的唤醒诱导的过渡

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摘要

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.
机译:利用时间分辨粒子图像测速技术和氢气泡可视化技术,研究了在1.38×10(4)到3.05×10(4)的收起弦雷诺数范围内,30P30N多段翼型在4度固定攻角下的尾流诱导转捩。在30P30N翼型的汇合边界层中观察到一种特殊的过渡程序,它强烈地受到缝翼尾流的影响。特别是,详细研究了缝翼尾流触发的双次级涡对整个转捩过程的影响。在初始过渡阶段,强烈的缝翼尾流扰动穿透主元件的边界层,然后通过双指数增长放大,产生双次级涡。与简化几何体的情况相比(He等人,《流体力学》第718卷,2013年,第116-130页;He&Wang,《流体物理》第27卷,2015年,第024106页),双指数增长为过渡提供了更强的波动。在中间过渡阶段,尾流扰动通过直接注入或间接诱导触发这些二次涡的三维失稳,从而产生一个涡。由此产生的A涡的展向波长因此被尾迹扰动锁定。在过渡后期,A涡演化为发夹涡包,最终在主元上方形成附加的湍流边界层。在整个过渡过程中,主元件上方的平均流没有出现明显的分离,显示出潜在的空气动力优势。

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