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arXiv 0812.3891nlin.CDphysics.flu-dyn
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turbulence中速度梯度张量动力学的最近流体变形闭合:时间尺度效应和展开

Recent Fluid Deformation closure for velocity gradient tensor dynamics in turbulence: time-scale effects and expansions

Marco Martins Afonso, Charles Meneveau

摘要:

为了模拟湍流中速度梯度张量的拉格朗日动力学方程中的压力和粘性项,Chevillard & Meneveau(Phys.Rev.Lett. 97,174501,2006)引入了Recent Fluid Deformation闭包。使用矩阵指数,封闭允许克服非物理的有限时间爆破著名的限制欧拉模型。然而,它也需要指定的解相关的时间尺度的速度梯度沿拉格朗日演化,当后者被选择太短(或者,等效地,雷诺数太高),该模型导致非物理统计。在本文中,我们通过数值实验和分析考虑来探讨这种封闭的局限性。我们还研究了使用时间相关的随机强迫,而不是以前采用的白噪声强迫的可能影响。数值实验表明,减少相关的时间尺度中指定的封闭和强迫不会导致相应的减少自相关的时间尺度的预测演变的速度梯度张量。这种观察到的不一致性可以解释不切实际的预测在不断增加的Reynoldsnumbers.We执行一系列的矩阵指数展开的权力的去相关时间尺度,我们比较完整的原始模型与线性化版本。后者是不能够扩展前者的适用性的限制,但允许该模型被铸造的阻尼项,其符号给出了额外的信息,作为第二个不变的速度梯度张量的函数的模型的稳定性。

英文摘要:

In order to model pressure and viscous terms in the equation for the Lagrangian dynamics of the velocity gradient tensor in turbulent flows, Chevillard & Meneveau (Phys. Rev. Lett. 97, 174501, 2006) introduced the Recent Fluid Deformation closure. Using matrix exponentials, the closure allows to overcome the unphysical finite-time blow-up of the well-known Restricted Euler model. However, it also requires the specification of a decorrelation time scale of the velocity gradient along the Lagrangian evolution, and when the latter is chosen too short (or, equivalently, the Reynolds number is too high), the model leads to unphysical statistics. In the present paper, we explore the limitations of this closure by means of numerical experiments and analytical considerations. We also study the possible effects of using time-correlated stochastic forcing instead of the previously employed white-noise forcing. Numerical experiments show that reducing the correlation time scale specified in the closure and in the forcing does not lead to a commensurate reduction of the autocorrelation time scale of the predicted evolution of the velocity gradient tensor. This observed inconsistency could explain the unrealistic predictions at increasing Reynolds numbers.We perform a series expansion of the matrix exponentials in powers of the decorrelation time scale, and we compare the full original model with a linearized version. The latter is not able to extend the limits of applicability of the former but allows the model to be cast in terms of a damping term whose sign gives additional information about the stability of the model as function of the second invariant of the velocity gradient tensor.

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