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arXiv 2103.06250physics.flu-dyn
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拐角流动分离在双楔形体高超声速绕流非定常动力学中的作用

Role of corner flow separation in unsteady dynamics of hypersonic flow over a double wedge geometry

Gaurav Kumar, Ashoke De

摘要:

本文研究了双楔体高超声速绕流中激波结构自诱导振荡的起源和维持。以前,许多研究人员考虑了不同来流和几何参数(如来流马赫数、楔角和楔长)变化的无粘流的双楔流动构型。近年来,对于具有大第二楔角的双楔构型,很少有文献揭示高超声速粘性流场的非定常流动物理。然而,这种自持流量振荡的原因还不完全清楚。本文研究了不同后楔角和楔长比的低焓高超声速流动中这种振荡的起源,考虑了马赫数为7、前楔角为30°的双楔粘性流动。利用OpenFOAM中rhoCentralFoam求解器的改进版本,对分离区和激波-激波干扰区不同网格分辨率下的双楔流场进行了数值模拟。这项研究证实了从以前的文献中观察到的改进的参数范围内的结果在一个自我维持的周期性振荡。本研究还表明,当入射激波位于后楔扩张角附近时,由于不同的楔长比(L1/L2)或后楔角(θ2),非定常是可能的。如果入射激波远超前于后楔形扩张角,则在大后楔形角时,流动仍然是稳定的。

英文摘要:

This study investigates the origin and sustenance of self induced oscillations of shock structures in a hypersonic flow over a double wedge configuration. Previously, various researchers have considered the double wedge flow configuration for inviscid flow with variations of different inflows as well as geometric parameters such as inflow Mach number , wedge angles, and wedge lengths. Few recently published articles reveal an unsteady flow physics involved with the hypersonic viscous flow for double wedge configuration with large second wedge angles. However, the reason for such self sustained flow oscillations is not completely clear. The present work seeks out to investigate the origin of such oscillations in a low enthalpy hypersonic flow with different aft wedge angles and wedge length ratios.In the current study, viscous flow over a double wedge at Mach 7 and fore wedge angle of 30° is considered. An improved version of rhoCentralFoam solver in OpenFOAM is used to investigate the double wedge flow over different grid resolutions in the separation region and shock shock interaction region. This study corroborates the observation from the previous literature with an improvement in the range of parameters which results in a self sustained periodic oscillation. The present study also suggests that the unsteadiness becomes possible when the incidence shock is in the proximity of the aft wedge expansion corner as a consequence of different wedge length ratios(L1/L2) or aft wedge angles (θ2). Flow can still be steady at a large aft wedge angle if the incidence shock is far ahead of the aft wedge expansion corner.

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