Effects of a trailing-edge flap on stall cell characteristics of a NACA0012 wing

IF 2.8 Q2 MECHANICS Flow (Cambridge, England) Pub Date : 2022-07-01 DOI:10.1017/flo.2022.11
Francis De Voogt, B. Ganapathisubramani
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Abstract

Abstract In this case study, we examine the effect of airfoil shape/camber on the formation and existence of stall cells. A series of experiments using a NACA0012 wing with a trailing-edge flap has been carried out over a range of angles of attack ($11.5^\circ$–$21^\circ$), flap angles ($0^\circ$, $5^\circ$, $10^\circ$) and chord-length-based Reynolds numbers (100 000–500 000). The influence of these parameters on stall cell formation has been explored. Tufts have been used to identify the flow behaviour near the surface, while forces have been measured to relate the surface flow behaviour and wing performance. The results from the tuft analysis on the wing indicated that two different Reynolds-number regimes exist with respect to stall cell formation criteria. A preliminary estimate of the airfoil shape influence on stall cell formation is presented. A data-driven approach is used to relate the aerodynamic parameters (lift coefficient and lift-curve slope) to the formation criteria of stall cells for the wing (and flap angles). The lift coefficient can be used to implicitly take into account the change in airfoil shape in addition to the angle of attack and the Reynolds number. It is hoped that the results presented in this case study could be extended to various other airfoil shapes and that the stall cell formation angle of attack can be deduced from just the mean lift behaviour.
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后缘襟翼对NACA0012机翼失速单元特性的影响
摘要在本案例研究中,我们考察了翼型/弯度对失速单元形成和存在的影响。使用带后缘襟翼的NACA0012机翼进行了一系列实验,攻角范围为(11.5美元-21美元)、襟翼角度(0美元、5美元、10美元)和基于弦长的雷诺数(10万-50万)。研究了这些参数对失速细胞形成的影响。塔夫茨已被用于识别表面附近的流动行为,而力已被测量以将表面流动行为与机翼性能联系起来。机翼上的簇分析结果表明,在失速单元形成标准方面存在两种不同的雷诺数状态。对翼型对失速单元形成的影响进行了初步估计。数据驱动方法用于将空气动力学参数(升力系数和升力曲线斜率)与机翼失速单元的形成标准(和襟翼角度)联系起来。升力系数可以用来隐含地考虑机翼形状的变化以及攻角和雷诺数。希望本案例研究中的结果可以扩展到各种其他翼型,并且失速单元形成攻角可以仅从平均升力行为中推导出来。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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2.40
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