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作 者:王震 王涛[1] 柏劲松[1,2] 肖佳欣 WANG Zhen;WANG Tao;BAI Jingsong;XIAO Jiaxin(Institute of Fluid Physics, China Academy of Engineeing Physics, Mianyang 621999, Sichuan, China;National Key Laboratory of Shock Wave and Detonation Physics, Institute of Fluid Physics,China Academy of Engineeing Physics, Mianyang 621999, Sichuan, China;Science and Technology on Space Physics Laboratory, Beijing 100076, China)
机构地区:[1]中国工程物理研究院流体物理研究所,四川绵阳621999 [2]中国工程物理研究院流体物理研究所冲击波物理与爆轰物理实验室,四川绵阳621999 [3]北京临近空间飞行器系统工程研究所,北京100076
出 处:《爆炸与冲击》2019年第4期59-68,共10页Explosion and Shock Waves
基 金:科学挑战专题(TZ2016001);国家自然科学基金(11702272;11532012);装备预研基金(6142A0302010417)
摘 要:基于Navier-Stokes方程组,采用可压缩多介质黏性流动和湍流大涡模拟程序MVFT (multi-viscousflow and turbulence),模拟了均匀流场与初始密度呈现高斯函数分布的非均匀流场中马赫数为1.25的非平面激波加载初始扰动air/SF6界面的Richtmyer-Meshkov (RM)不稳定性现象。数值模拟结果表明,初始流场非均匀性将会影响非平面激波诱导的RM不稳定性演化过程。反射激波加载前,非平面激波导致的界面扰动振幅随着流场非均匀性增强而增大;反射激波加载后,非均匀流场与均匀流场条件下的界面扰动振幅差异有所减小。进一步,定量分析流场中环量分布及脉动速度统计量揭示了前述规律的原因。此外,还与平面激波诱导的RM不稳定性进行了简单对比,发现由于非平面激波波阵面区域的涡量与激波冲击界面时产生的涡量的共同作用,使得非平面激波与平面激波诱导的界面失稳过程存在差异。Based on the Navier-Stokes equations, the large-eddy simulation code MVFT(multi-viscousflow and turbulence) was applied to numerically study the Richtmyer-Meshkov instability(i.e. RMI) for a perturbed interface, which is driven by a non-planar shock wave with Ma=1.25 in uniform and non-uniform flows with Gaussian distribution of the initial density. The simulation results show that the interface evolution of the RMI induced by non-planar shock wave is affected by the non-uniformity of the initial flows. Before reshock, the growth of the disturbed interface increases with the increasing of the nonuniformity flow field for either φ=0 or φ=π. However, these discrepancies are reduced as the flow enters the turbulent mixing. Further quantitative analysis of the circulations and high-order fluctuating velocity correlation in the flow field reveal the mechanisms for the aforementioned regulations. In addition, it is found that the interface evolution of the RMI induced by non-planar shock wave is different from that driven by planar shock wave. The mechanism for the difference is the influence of the initial vorticity of non-planar shock wave and the vorticity generated by the shock-interface.
关 键 词:RICHTMYER-MESHKOV不稳定性 非均匀流场 非平面激波 大涡模拟
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