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Experimental Investigation of Unsteady Vehicle Aerodynamics under Time-Dependent Flow Conditions - Part2

机译:时变流动条件下车辆非定常空气动力学的实验研究-第2部分

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Unsteady aerodynamic flow phenomena are investigated in a wind tunnel by oscillating a realistic 50% scale model around the vertical axis. Thus the model is exposed to time-dependent flow conditions at realistic Reynolds and Strouhal numbers. Using this setup unsteady aerodynamic loads are observed to differ significantly from quasi steady loads. In particular, the unsteady yaw moment exceeds the quasi steady approximation significantly. On the other hand, side force and roll moment are over predicted by quasi steady approximation but exhibit a significant time delay. Part 2 of this study proves that a delayed and enhanced response of the surface pressures at the rear side of the vehicle is responsible for the differences between unsteady and quasi steady loads. The pressure changes at the vehicle front, however, are shown to have similar amplitudes and almost no phase shift compared to quasi steady flow conditions. The difference between unsteady and quasi steady yaw moment proves to be independent of oscillation amplitudes between 2deg and 4deg. It is assumed that the intensity of the unsteady flow phenomena is determined by the interaction of the time scale of the model rotation and the time scale of the delayed wake flow, described by the Strouhal number. The largest magnification factors for the yaw moment are found at 140kph and 2Hz for the notchback geometry, which results in a Strouhal number of Sr=0.12. It is finally shown that the yaw moment overshoot is less pronounced for a fastback and especially for a fullback geometry, which is explained by smaller unsteady pressure variations at the rear side of the fullback.
机译:通过绕垂直轴振荡现实的50%比例模型,研究风洞中的非稳态空气流动现象。因此,该模型在真实的雷诺数和斯特劳哈尔数下处于与时间相关的流动条件下。使用这种设置,观察到非稳态气动载荷与准稳态载荷显着不同。特别是,非稳态偏航力矩明显超过了准稳态近似值。另一方面,侧向力和侧倾力矩通过准稳态逼近法得到了过度预测,但显示出显着的时间延迟。本研究的第二部分证明,车辆后部表面压力的延迟和增强响应是造成非稳态载荷和准稳态载荷之间差异的原因。然而,与准稳态流动条件相比,车辆前部的压力变化具有相似的幅度且几乎没有相移。非稳态和准稳态偏航力矩之间的差异被证明与2deg和4deg之间的振荡幅度无关。假定非稳态流动现象的强度由模型旋转的时间尺度和延迟的尾流的时间尺度的相互作用决定,该相互作用由斯特劳哈尔数描述。对于后退几何,偏航力矩的最大放大系数为140kph和2Hz,这导致Strouhal数Sr = 0.12。最终表明,偏航力矩的超调对于快背,尤其是后卫的几何形状不太明显,这可以通过后卫的后侧较小的非定常压力变化来解释。

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