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所有波数下烧蚀瑞利-泰勒不稳定性的非线性激发。

Nonlinear excitation of the ablative Rayleigh-Taylor instability for all wave numbers.

机构信息

Department of Mechanical Engineering and Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA.

Department of Modern Mechanics, University of Science and Technology of China, Hefei 230026, China.

出版信息

Phys Rev E. 2018 Jan;97(1-1):011203. doi: 10.1103/PhysRevE.97.011203.

Abstract

Small-scale perturbations in the ablative Rayleigh-Taylor instability (ARTI) are often neglected because they are linearly stable when their wavelength is shorter than a linear cutoff. Using two-dimensional (2D) and three-dimensional (3D) numerical simulations, it is shown that linearly stable modes of any wavelength can be destabilized. This instability regime requires finite amplitude initial perturbations and linearly stable ARTI modes to be more easily destabilized in 3D than in 2D. It is shown that for conditions found in laser fusion targets, short wavelength ARTI modes are more efficient at driving mixing of ablated material throughout the target since the nonlinear bubble density increases with the wave number and small-scale bubbles carry a larger mass flux of mixed material.

摘要

烧蚀瑞利-泰勒不稳定性(ARTI)的小尺度涨落通常被忽略,因为当它们的波长短于线性截止波长时,它们是线性稳定的。通过二维(2D)和三维(3D)数值模拟,表明任何波长的线性稳定模式都可以失稳。这种不稳定性模式需要有限振幅的初始涨落,并且在 3D 中比在 2D 中更容易失稳的线性稳定的 ARTI 模式。结果表明,对于在激光聚变靶中发现的条件,短波长的 ARTI 模式在驱动整个目标中烧蚀材料的混合方面更为有效,因为非线性气泡密度随波数增加,小尺度气泡携带更大的混合材料的质量通量。

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