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Analytical nonlinear theory of unstable fluid mixing driven by a shock wave.

机译:激波驱动的不稳定流体混合的解析非线性理论。

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摘要

e present a nonlinear theory of the growth of fingers at interface between two fluids of different densities driven by a shock wave. This interfacial instability is known as the Richtmyer-Meshkov (RM) instability. Previous theoretical work focused on linear regime and failed to give a quantitatively correct prediction for the growth rate of Richtmyer-Meshkov unstable interface in the nonlinear regime. Spikes and bubbles are formed at the unstable interface. A spike (bubble) is a portion of heavy (light) fluid penetrating into light (heavy) fluid. The theory presented in this dissertation provides analytical, explicit expressions for quantitative predictions of the overall growth rate as well as the growth rate of the spike and bubble of the unstable interface between fluids of arbitrary density ratios in two and three dimensions.;The mathematical techniques which we used in our theoretical formulation are a systematic nonlinear perturbation expansions, Pade approximation and the asymptotic matching. Our validation study shows that these techniques have been successfully applied to predict the growth rates of the unstable interface.;Our theory contains no adjustable parameters. The theoretical predictions of our nonlinear theory are are in excellent agreements with results of full nonlinear numerical simulations and the experimental data in two dimensions from the linear (small amplitude) to the nonlinear regimes. The predictions of linear theories are qualitatively incorrect at late times. Our theory has identified that the RM unstable system goes through a transition from a compressible and linear one at early times to a nonlinear and incompressible one at later times.;The nonlinear theory has been extended to fluids in three dimensions. Our results show that the growth rates for different orientation angle
机译:e提出了一种非线性理论,即在冲击波驱动的两种不同密度的流体之间的界面处,指状物的生长。这种界面不稳定性称为Richtmyer-Meshkov(RM)不稳定性。先前的理论工作集中在线性状态,未能对非线性状态下Richtmyer-Meshkov不稳定界面的增长率给出定量正确的预测。在不稳定的界面处会形成尖峰和气泡。尖峰(气泡)是重(轻)流体渗入轻(重)流体的一部分。本文提出的理论为定量预测整体增长率以及二维和三维任意密度比的流体之间的不稳定界面之间的尖峰和气泡的增长速度提供了解析,明确的表达式。我们在理论公式中使用的是系统非线性摄动展开,Pade逼近和渐近匹配。我们的验证研究表明,这些技术已成功应用于预测不稳定界面的增长率。我们的非线性理论的理论预测与完全非线性数值模拟的结果以及从线性(小振幅)到非线性状态的二维实验数据非常吻合。在后期,线性理论的预测在质量上是不正确的。我们的理论已经确定,RM不稳定系统经历了从早期的可压缩线性模型到后期的非线性和不可压缩模型的过渡。非线性理论已经扩展到三维流体。我们的结果表明,不同取向角的增长率

著录项

  • 作者

    Son, Sungik.;

  • 作者单位

    State University of New York at Stony Brook.;

  • 授予单位 State University of New York at Stony Brook.;
  • 学科 Applied Mechanics.;Mathematics.;Physics Fluid and Plasma.
  • 学位 Ph.D.
  • 年度 1996
  • 页码 102 p.
  • 总页数 102
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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