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arXiv 2107.09112physics.flu-dyn
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不稳定性是否影响静止各向同性turbulence中的惯性传递率?

Does intermittency affect the inertial transfer rate in stationary isotropic turbulence?

S. R. Yoffe, W. D. McComb

摘要:

对受迫纳维-斯托克斯方程进行了直接数值模拟,其中每个壳平均量从适合于初始高斯状态的值演变为围绕平均值波动。一旦瞬态已经通过,平均值(及其相关的统计数据)通过采样的演变时间序列的时间间隔的顺序的涡流周转时间。在泰勒-雷诺数从10.6到335.2的范围内重复这一过程。随着雷诺数的增加,能量谱、传递谱和惯性通量的计算结果支持了Kolmogorov-Obukhov湍流能量传递模型。特别是,我们观察到的惯性通量的标度不变性的开始,伴随着在相应的惯性波数范围内的能量谱中的-5/3幂律的开始。详细的比较表明,我们的结果与许多其他调查中发现的一致。采用流动显示方法研究了内流率。这种现象在单个实现中可以看到,但发现在整体平均下随着实现数量的增加而平均化。在对关于非线性效应与有限雷诺数修正的争论的文献进行批判性审查之后,得出的结论是,对于静止各向同性湍流的情况,内部非线性不能影响Kolmogorov-Obukhov图像,因为这完全是根据整体平均平均量构建的。

英文摘要:

Direct numerical simulations of the forced Navier-Stokes equations were performed, in which each shell-averaged quantity evolved from a value appropriate to an initial Gaussian state, to fluctuate about a mean value. Once the transient had passed, mean values (and their associated statistics) were obtained by sampling the evolved time-series at intervals of the order of an eddy-turnover time. This was repeated for a range of Taylor-Reynolds numbers from 10.6 to 335.2. With increasing Reynolds number, our results for energy spectra, transfer spectra and inertial flux supported the Kolmogorov-Obukhov picture of turbulent energy transfer. In particular, we observed the onset of scale-invariance of the inertial flux, accompanied by the onset of the -5/3 power law in the energy spectrum for the corresponding inertial range of wavenumbers. Detailed comparisons showed that our results were in agreement with those found in many other investigations. Flow visualization methods were used to study the internal intermittency. This phenomenon is seen in single realisations but was found to average out with increasing number of realisations under ensemble-averaging. Following a critical review of the literature relating to the controversy about intermittency effects versus finite-Reynolds number corrections, it was concluded that, for the case of stationary isotropic turbulence, internal intermittency cannot affect the Kolmogorov-Obukhov picture, as this is constructed entirely in terms of ensemble-averaged mean quantities.

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