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| 1 | 反射激波诱导界面不稳定性研究进展显示文摘运动激波与流体界面相互作用能够引起复杂的流动现象,包括激波反射折射、界面失稳以及湍流混合等,在自然界和工程实际中具有重要的应用价值和研究意义.入射激波冲击之后,初始界面上的扰动在斜压涡量和压力扰动等机制下经历线性和非线性增长,界面形态不断发生变化;当反射激波再次冲击变形的界面时,涡量的产生及输运将改变界面不稳定性的演化过程,产生不同的物理现象和规律.由于反射激波的生成及控制比单次激波要更加复杂,开展与之相关的界面不稳定性研究工作具有极大的挑战性.本文回顾了近年来学者们在反射激波诱导界面失稳和湍流混合方面取得的实验、数值和理论研究进展,重点从平面和汇聚两种典型的初始激波形状出发,讨论了界面形状、激波强度、反射距离等初始条件对反射激波再次作用下界面不稳定性的影响规律,并进一步展望今后的研究重点和方向. | 丛洲洋 郭旭 司廷 | 2020 | 中国科学:物理学、力学、天文学2020，50，10： | 5 |
| 2 | 圆柱形汇聚激波诱导Richtmyer-Meshkov不稳定的SPH模拟显示文摘汇聚激波诱导不同物质界面的Richtmyer-Meshkov(RM)不稳定现象在惯性约束核聚变领域有重要的学术意义和工程背景.基于网格离散的宏观流体力学方法由于数值扩散问题往往需要高阶精度算法才能准确追踪界面演化,且对大变形和破碎合并等复杂界面追踪也极为困难.光滑粒子流体动力学(smoothed particlehydrodynamics,SPH)方法采用纯拉格朗日算法,可以有效克服上述难点.但经典SPH算法需采用人工黏性处理强间断,在激波间断处往往会出现严重的非物理振荡,对于涉及强冲击不稳定性问题,很难达到理想的模拟效果.本文采用基于HLL黎曼求解器的SPH算法,实现了对强激波和大密度比物质界面的有效分辨和追踪.一维数值校核证明了代码的可靠性、健壮性,并进一步模拟了二维圆柱形汇聚冲击波冲击四边形轻/重气界面诱导的RM不稳定性问题,与已有实验结果进行了对比,发现模拟结果与实验结果吻合.通过分析界面演化过程中的密度及压力变化,发现本文所采用的方法可准确地追踪激波与界面作用的复杂界面和波系演化规律.研究结果为进一步理解和解释汇聚冲击条件下的RM不稳定性机理奠定了基础. | 徐建于 黄生洪 | 2019 | 力学学报2019，51，4： | 4 |
| 3 | 激波诱导异质气体界面失稳的数值模拟显示文摘基于二维N-S方程,利用有限差分数值离散方法,对激波诱导异质气体界面失稳的现象进行了数值模拟,与文献中实验结果和计算结果进行了定性比较,并进一步分析了整个流动的非定常动态变化特性和非线性特征。研究表明,本文数值模拟的非定常流场图谱与文献中的实验结果和数值结果吻合较好;数值结果捕捉到了六氟化硫界面的演变过程及流场中复杂的波系结构。 | 周松柏 刘君 郭正 刘瑜 | 2009 | 国防科技大学学报2009，31，1： | 2 |
| 4 | Mode coupling in converging Richtmyer-Meshkov instability of dual-mode interface显示文摘The converging Richtmyer-Meshkov(RM)instability on single-and dual-mode N2/SF6 interfaces is studied by an upwind conservation element and solution element solver.An unperturbed case is first considered,and it is found that the shocked interface undergoes a long-term deceleration after a period of uniform motion.The evolution of single-mode interface at the early stage exhibits an evident nonlinearity,which can be reasonably predicted by the nonlinear model of Wang et al.(Phys Plasmas 22:082702,2015).During the deceleration stage,the perturbation amplitude drops quickly and even becomes a negative(phase inversion)before the reshock due to the Rayleigh-Taylor(RT)stabilization.After the reshock,the interface experiences a phase inversion again or does not,depending on the reshock time.The growth of the second-order harmonic in the deceleration stage clearly reveals the competition between the RT effect and the nonlinearity.For dual-mode interfaces,the growth of the first mode(wavenumber k1)relies heavily on the second mode(wavenumber k2)due to the mode coupling effect.Specifically,for cases where k2 is an even or odd multiple of k1,the growth of the first mode is inhibited or promoted depending on its initial amplitude sign and the phase difference between two basic waves,while for cases where k2 is a non-integer multiple of k1,the second mode has negligible influence on the first mode.Through a systematic study,signs of perturbation amplitudes of the generated k2−k1 and k2+k1 waves are obtained for all possible dual-mode configurations,which are reasonably predicted by a modified Haan model(Phys Fluids B 3:2349-2355,1991). | Zhangbo Zhou Juchun Ding Zhigang Zhai Wan Cheng Xisheng Luo | 2020 | Acta Mechanica Sinica2020，36，2： | 1 |
| 5 | Numerical study on the laser ablative Rayleigh-Taylor instability显示文摘The laser ablative Rayleigh-Taylor instability plays an important role in the ignition of inertial refinement fusion.An accurate simulation of this process is important to control the growth of flow instability during the implosion.In this paper,taking the simulations of the hydrodynamics,the laser energy deposition and the electronic thermal conductivity into consideration,a massively parallel laser ablative Rayleigh-Taylor instability code based on Euler method is developed.Some open source codes are used to improve the code development efficiency.The accuracy of the hydrodynamics simulation is tested by an analytical theory about the weakly nonlinear Rayleigh-Taylor instability with double interfaces.The benchmark of an one dimensional heat conductivity is used to test the accuracy of the thermal conductivity simulation.The laser ablative plane target and the laser ablative Rayleigh-Taylor instability are used to test the reliability of the code on the simulation of the whole laser ablative process.It is shown that the confidence of our numerical simulation code is high and the code framework we designed is effective.It can be a basis on studying the problems about the laser ablative instability in inertial refinement fusion. | Zhiyuan Li Lifeng Wang Junfeng Wu Wenhua Ye | 2020 | Acta Mechanica Sinica2020，36，4： | 1 |
| 6 | Effect of Atwood number on convergent Richtmyer-Meshkov instability显示文摘Developments of two-dimensional single-mode light/heavy interfaces driven by convergent shock waves are numerically investigated,focusing on the effect of the Atwood number on the Rayleigh-Taylor stabilization,the compressibility and the nonlinearity.Five different test gases,including C〇2,Kr,R22,R12 and SF6,are considered with air as the ambient gas.It is clarified for the first time that the unperturbed interface begins to decelerate when the shock focuses at the convergence center,and the acceleration during the deceleration phase is proportional to the Atwood number.During the first reshock,the interface moves outwards with a deceleration until it starts moving inwards.When the initial interface is weakly disturbed,a more obvious amplitude reduction is observed for the case with a larger Atwood number before the reshock,which means that the Rayleigh-Taylor stabilization is stronger.To assess the effect of the Atwood number on the compressibility and the nonlinearity,three models,including a linear incompressible model,a nonlinear incompressible model and a linear compressible model,are adopted to predict the amplitude growth before the reshock.The results show that the nonlinearity is weak,and is almost not influenced by the Atwood number before the reshock.The compressibility,however,greatly changes the amplitude growth.As the Atwood number increases,the compressibility plays a less significant role in the amplitude growth because a heavier gas is harder to be compressed.Although a gas with a larger specific heat ratio is also difficult to be compressed,the specific heat ratio plays a minor role to the compressibility relative to the Atwood number.During the reshock,the amplitude grows linearly until the nonlinearity in the cases with large Atwood numbers is strong enough to reduce the amplitude growth rate. | Jinggang Tang Fu Zhang Xisheng Luo Zhigang Zhai | 2021 | Acta Mechanica Sinica2021，37，3： | 0 |
| 7 | 扩散型气柱界面R-M失稳中混合率的实验研究显示文摘Richtmyer-Meshkov(R-M)不稳定性普遍存在于众多工程问题中,激波管实验是研究R-M失稳问题的主要手段.高精度的平面激光诱导荧光(planar laser-induced fluorescence,PLIF)技术具有分子量级的示踪能力,可获得界面气体浓度(摩尔分数)分布,为研究界面失稳混合问题提供了有力工具.在弱激波(Ma=1.25)冲击扩散型气柱界面实验中,采用PLIF技术对R-M失稳引起的SF6-Air界面混合问题进行了研究.通过改变椭圆形初始界面的长短轴比,得到了3种扩散型初始界面失稳演化过程中气体摩尔分数,观察到了斜压机制下界面的简单拉伸、二次不稳定性、挤压射流等现象.利用浓度分布进一步得到了界面的瞬时混合率,通过瞬时混合率、界面整体平均混合率以及混合率的概率密度分布,分析了界面在不同演化阶段的界面混合特征,初步讨论了界面失稳混合的机制.演化初期,界面在斜压涡的作用下发生拉伸卷曲,通过增大浓度梯度来促进界面的混合.当演化进一步发展,二次不稳定性出现后,界面通过小尺度对流的方式达到湍流混合状态,而浓度梯度驱使的分子间混合逐渐减弱.由浓度梯度引起的扩散与由二次不稳定性引起的对流存在着'竞争'关系,二者共同主导了界面的混合. | 黄熙龙 廖深飞 邹立勇 刘金宏 曹仁义 | 2016 | 力学学报2016，48，5： | 0 |
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