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Experiments on the Richtmyer-Meshkov instability of incompressible fluids

机译:不可压缩流体的Richtmyer-Meshkov不稳定性实验

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摘要

Richtmyer-Meshkov (R-M) instability occurs when two different density fluids are impulsively accelerated in the direction normal to their nearly planar interface. The instability causes perturbations on the interface to grow and to possibly become turbulent. R-M instability is a fundamental fluid instability that is important to fields ranging from astrophysics to high-speed combustion. For example, R-M instability is currently one of the limiting factors in achieving a positive net yield in laser driven inertial confinement fusion experiments. This experimental study investigates the instability of an interface between incompressible, miscible liquids with an initial sinusoidal perturbation. After undergoing a nearly impulsive acceleration, the initial perturbation quickly inverts and then grows in amplitude. The vorticity on the interface eventually coalesces into a series of alternating signed vortices. Disturbance amplitudes are measured and compared to theoretical predictions. Linear stability theory gives excellent agreement with the measured initial perturbation growth rates, while the predicted amplitudes differ by less than 10% from experimental measurements up to a nondimensional time kȧ₀t = 0.7. Fourth order, single-mode perturbation theory extends the 1.0% amplitude agreement up to a nondimensional time kȧ₀t = 1.3. A discrete vortex model and a combined model equation are within 10% of the experimental amplitude measurements up to the maximum experimental nondimensional time kȧ₀t = 30. The effects of Reynolds number (based on circulation) on the vortex core evolution and overall growth rate of the interface are also investigated. In addition, an instability in the vortex cores is observed for the first time and criteria established for its occurrence.
机译:Richtmyer-Meshkov(R-M)不稳定发生在两种不同密度的流体沿垂直于其几乎平面界面的方向被脉冲加速时。不稳定性导致界面上的扰动增大,并可能变得湍流。 R-M不稳定性是一种基本的流体不稳定性,对于从天体物理学到高速燃烧的各个领域都很重要。例如,R-M不稳定性目前是在激光驱动惯性约束聚变实验中获得正净产量的限制因素之一。这项实验研究调查了具有初始正弦波扰动的不可压缩混溶液体之间界面的不稳定性。在经历了近乎脉冲的加速度之后,初始扰动迅速反转,然后振幅增大。界面上的涡流最终合并为一系列交替的带符号涡流。测量干扰幅度,并将其与理论预测值进行比较。线性稳定性理论与测得的初始扰动增长率极佳地吻合,而在无量纲时间kȧ₀t= 0.7时,预测幅度与实验测量值相差不到10%。四阶单模摄动理论将1.0%幅度一致扩展到无量纲时间kȧ₀t= 1.3。直到最大实验无量纲时间kȧ₀t= 30,离散涡旋模型和组合模型方程均在实验幅度测量的10%以内。雷诺数(基于循环)对涡旋核心演化和整体涡旋速度的影响界面也进行了调查。此外,首次观察到涡流核的不稳定性,并确定了其发生的标准。

著录项

  • 作者

    Niederhaus Charles Edward;

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  • 年度 2000
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  • 原文格式 PDF
  • 正文语种 en_US
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