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Time-resolved particle image velocimetry measurements of the turbulent Richtmyer-Meshkov instability

机译:湍流Richtmyer-Meshkov稳定性的时间分辨粒子图像速度测量

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摘要

Experiments are presented on the Richtmyer-Meshkov instability (RMI) with a three-dimensional, multi-mode initial perturbation. The experiments use a vertical shock tube, where a stably stratified interface is formed between air and sulphur hexafluoride (SF) via counterflow. A perturbation is imposed at the interface by vertical oscillation of the gas column, forming Faraday waves. The interface is accelerated by a Mach 1.17 (in air) shock wave, and the development of the mixing region between the gases is investigated using particle image velocimetry. Following shock acceleration, a reflected shock wave from the bottom of the shock tube interacts with the mixing layer a second time (reshock). The experiment is initialized with both high and low amplitude perturbations to examine the effect of the perturbation amplitude on measured quantities. The instability growth exponent () is determined from the kinetic energy field using the width of the mixing layer and the decay of kinetic energy, which are found to be in agreement when the flow is most strongly excited. A growth exponent of is found for all cases except the high-amplitude reshocked regime (where ). High-amplitude experiments exhibit the transitional outer Reynolds number required for mixing transition following the incident shock, and both experiments are elevated well above this threshold following reshock. However, neither set of experiments meet the more stringent requirements proposed by Zhou et al. (Phys. Rev.E, vol. 67, issue 5, 2003) which include the time dependent aspect of the RMI, an observation which is also made when examining the spectra.
机译:对具有三维多模初始扰动的Richtmyer-Meshkov不稳定性(RMI)进行了实验研究。实验使用垂直激波管,空气和六氟化硫(SF)之间通过逆流形成稳定的分层界面。气柱的垂直振动在界面处施加扰动,形成法拉第波。用马赫数为1.17(空气中)的冲击波加速界面,并用粒子图像测速仪研究气体间混合区的发展。激波加速后,激波管底部的反射激波再次与混合层相互作用(再冲击)。用高振幅和低振幅扰动对实验进行初始化,以检查扰动振幅对测量量的影响。不稳定性增长指数()由动能场确定,使用混合层的宽度和动能的衰减,当气流受到最强烈的激发时,发现两者是一致的。除高振幅再冲击区(其中)外,所有情况下的增长指数均为。高振幅实验显示了入射激波后混合转变所需的过渡外雷诺数,两个实验在再激波后都大大高于该阈值。然而,这两组实验都不符合Zhou等人(Phys.Rev.E,第67卷,2003年第5期)提出的更严格的要求,其中包括RMI的时间依赖性,在检查光谱时也进行了观察。

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