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High-resolution simulations and modeling of reshocked single-mode Richtmyer-Meshkov instability: Comparison to experimental data and to amplitude growth model predictions

机译:重构的单模Richtmyer-Meshkov不稳定性的高分辨率仿真和建模:与实验数据和幅度增长模型预测的比较

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摘要

The reshocked single-mode Richtmyer-Meshkov instability is simulated in two spatial dimensions using the fifth- and ninth-order weighted essentially nonoscillatory shock-capturing method with uniform spatial resolution of 256 points per initial perturbation wavelength. The initial conditions and computational domain are modeled after the single-mode, Mach 1.21 air(acetone)/SF6 shock tube experiment of Collins and Jacobs [J. Fluid Mech. 464, 113 (2002)]. The simulation densities are shown to be in very good agreement with the corrected experimental planar laser-induced fluorescence images at selected times before reshock of the evolving interface. Analytical, semianalytical, and phenomenological linear and nonlinear, impulsive, perturbation, and potential flow models for single-mode Richtmyer-Meshkov unstable perturbation growth are summarized. The simulation amplitudes are shown to be in very good agreement with the experimental data and with the predictions of linear amplitude growth models for small times, and with those of nonlinear amplitude growth models at later times up to the time at which the driver-based expansion in the experiment (but not present in the simulations or models) expands the layer before reshock. The qualitative and quantitative differences between the fifth- and ninth-order simulation results are discussed. Using a local and global quantitative metric, the prediction of the Zhang and Sohn [Phys. Fluids 9, 1106 (1997)] nonlinear Padé model is shown to be in best overall agreement with the simulation amplitudes before reshock. The sensitivity of the amplitude growth model predictions to the initial growth rate from linear instability theory, the post-shock Atwood number and amplitude, and the velocity jump due to the passage of the shock through the interface is also investigated numerically.
机译:使用五阶和九阶加权基本非振荡震荡捕获方法在两个空间维度上模拟重新震荡的单模Richtmyer-Meshkov不稳定性,每个初始扰动波长的均匀空间分辨率为256点。初始条件和计算域是在Collins和Jacobs的单模马赫1.21空气(丙酮)/ SF6冲击管实验之后建模的[J.流体机械。 464,113(2002)]。结果表明,在重新演化界面之前的选定时间,模拟密度与校正的实验平面激光诱导的荧光图像非常吻合。总结了单模Richtmyer-Meshkov不稳定扰动增长的解析,半解析和现象学线性和非线性,脉冲,摄动和势流模型。结果表明,模拟幅度与实验数据和线性幅度增长模型的预测在很短时间内非常吻合,非线性幅度增长模型的预测在以后直到基于驾驶员的扩张时,都非常吻合。在实验中(但在模拟或模型中不存在)在重新震荡之前先扩展图层。讨论了五阶和九阶模拟结果之间的定性和定量差异。使用局部和全局定量度量,对Zhang和Sohn的预测[Phys。流体9(1106(1997))]非线性Padé模型显示与重新震荡之前的模拟振幅具有最佳的总体一致性。还数值研究了线性增长理论对振幅增长模型对初始增长率的敏感性,震后阿特伍德数和振幅以及由于冲击通过界面而引起的速度跳跃。

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