P. Ramaprabhu, G. Dimonte, P. Woodward, Chris L. Fryer, G. Rockefeller, K. Muthuraman, Pei-Hung Lin, J. Jayaraj
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引用次数: 80
Abstract
We report on numerical simulations of the detailed evolution of the single mode Rayleigh-Taylor [Lord Rayleigh, Scientific Papers II (Cambridge University Press, Cambridge, 1900), p. 200; G. I. Taylor, “The instability of liquid surfaces when accelerated in a direction perpendicular to their plane,” Proc. R. Soc. London, Ser. A 201, 192 (1950)10.1098/rspa.1950.0052; S. Chandrasekhar, Hydrodynamic and Hydromagnetic Stability (Oxford University Press, Oxford, 1961)] instability to late times and high aspect ratios. In contrast to established potential flow models that predict a terminal velocity and a constant Froude number at low Atwood numbers, we observe a complex sequence of events that can be summarized in four stages: I. Exponential growth of imposed perturbations, II. Saturation to terminal velocity, III. Reacceleration to a higher Froude number, and IV. Chaotic mixing. The observed reacceleration away from the Froude number predicted by potential flow theory is attributed to the appearance of second...
我们报告了单模瑞利-泰勒的详细演化的数值模拟[瑞利勋爵,科学论文II(剑桥大学出版社,剑桥,1900),第200页;G. I. Taylor,“液体表面在垂直于其平面方向加速时的不稳定性,”Proc. R. Soc。伦敦,爵士。[j] .中国农业科学,2012,32 (5):1055 - 1055;S.钱德拉塞卡,《水动力和磁稳定性》(牛津大学出版社,牛津,1961)]晚期和高纵横比的不稳定性。与已建立的预测终端速度和低阿特伍德数时恒定弗劳德数的势流模型相反,我们观察到一系列复杂的事件,可以概括为四个阶段:1 .施加扰动的指数增长;饱和到终端速度,III。再加速到更高的弗劳德数,和IV.混沌混合。观测到的偏离势流理论预测的弗劳德数的再加速度归因于秒…
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