矩形圆柱周围的直接和混合气动声学模拟

H. Yokoyama, A. Iida
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引用次数: 1

摘要

气动声学仿真分为混合仿真和直接仿真。在本章中,通过对流场和声场的直接和混合模拟,重点研究了自由流马赫数对均匀流动中二维方形圆柱体周围流场和声场的影响。这些结果表明了混合仿真的有效性和局限性。马赫数M在0.2 ~ 0.6之间变化。在M = 0.6等高马赫数条件下,声波的传播角与以散射声为主并考虑多普勒效应的修正Curle方程预测的传播角有很大差异。这是因为声场受到直接声的影响,而直接声是由原Curle方程中的四极产生的。为了阐明直接声对声场的影响,对散射声和直接声进行了分解。结果表明,当M≥0.4时,直接声强度过大,不容忽视。此外,利用Lighthill的声源进行了声学模拟。
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Direct and Hybrid Aeroacoustic Simulations Around a Rectangular Cylinder
Aeroacoustic simulations are divided into hybrid and direct simulations. In this chapter, the effects of freestream Mach number on flow and acoustic fields around a two-dimensional square cylinder in a uniform flow are focused on using direct and hybrid simulations of flow and acoustic fields are performed. These results indicate the effectiveness and limit of the hybrid simulations. The Mach number M is varied from 0.2 to 0.6. The propagation angle of the acoustic waves for a high Mach number such as M = 0.6 greatly differs from that predicted by modified Curle ’ s equation, which assumes the scattered sound to be dominant and takes the Doppler effects into consideration. This is because the acoustic field is affected by the direct sound, which is generated by quadrupoles in the original Curle ’ s equation. To clarify the effects of the direct sound on the acoustic field, the scattered and direct sounds are decomposed. The results show that the direct sound is too intense to neglect for M ≥ 0.4. Moreover, acoustic simulations are performed using the Lighthill ’ s acoustic sources.
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