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Initial growth of the Rayleigh-Taylor instability via molecular dynamics

机译:瑞利泰勒不稳定性通过分子动力学的初始增长

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At small length scales, the fluctuations that are neglected in most continuum descriptions of fluids become important. In this work, we explore the emergence of the Navier-Stokes equations as the ensemble mean of these fluctuations, which are inherent in the fundamental molecular processes underlying a fluid. This is accomplished by examining the initial growth of the Rayleigh-Taylor instability via hundreds of large-scale molecular dynamics simulations. A comparison of the mean growth rate spectra with the corresponding continuum predictions yields good agreement over a range of length scales from similar to 1 mu m to as small as similar to 10 nm. However, individual simulations exhibit significant variations from the continuum prediction. This work helps pave the way to a more fundamental understanding of fluid dynamics on small scales, and the mechanisms by which macroscopic, continuum models emerge. Such an understanding is essential, for example, in the rapidly growing field of nanotechnology.
机译:在小尺度上,在大多数连续流体描述中忽略的波动变得很重要。在这项工作中,我们探索了Navier-Stokes方程的出现,作为这些波动的整体平均值,这些波动是流体基础的基本分子过程所固有的。这是通过数百次大规模分子动力学模拟检查瑞利-泰勒不稳定性的初始增长来实现的。将平均生长速率光谱与相应的连续谱预测值进行比较,可以在从大约1微米到最小至10纳米的长度范围内达成良好的一致性。但是,单独的模拟与连续谱预测相比有很大的不同。这项工作有助于为对小规模流体动力学以及宏观连续模型出现的机理更基本的了解铺平道路。例如,在迅速发展的纳米技术领域,这种理解至关重要。

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