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二维弹性湍流的统计特性。

Statistical properties of two-dimensional elastic turbulence.

作者信息

Garg Himani, Calzavarini Enrico, Berti Stefano

机构信息

Université de Lille, ULR 7512-Unité de Mécanique de Lille Joseph Boussinesq (UML), F-59000 Lille, France.

出版信息

Phys Rev E. 2021 Sep;104(3-2):035103. doi: 10.1103/PhysRevE.104.035103.

Abstract

We numerically investigate the spatial and temporal statistical properties of a dilute polymer solution in the elastic turbulence regime, i.e., in the chaotic flow state occurring at vanishing Reynolds and high Weissenberg numbers. We aim at elucidating the relations between measurements of flow properties performed in the spatial domain with the ones taken in the temporal domain, which is a key point for the interpretation of experimental results on elastic turbulence and to discuss the validity of Taylor's hypothesis. To this end, we carry out extensive direct numerical simulations of the two-dimensional Kolmogorov flow of an Oldroyd-B viscoelastic fluid. Static pointlike numerical probes are placed at different locations in the flow, particularly at the extrema of mean flow amplitude. The results in the fully developed elastic turbulence regime reveal large velocity fluctuations, as compared to the mean flow, leading to a partial breakdown of Taylor's frozen-field hypothesis. While second-order statistics, probed by spectra and structure functions, display consistent scaling behaviors in the spatial and temporal domains, the third-order statistics highlight robust differences. In particular the temporal analysis fails to capture the skewness of streamwise longitudinal velocity increments. Finally, we assess both the degree of statistical inhomogeneity and isotropy of the flow turbulent fluctuations as a function of scale. While the system is only weakly nonhomogenous in the cross-stream direction, it is found to be highly anisotropic at all scales.

摘要

我们对处于弹性湍流状态的稀聚合物溶液的空间和时间统计特性进行了数值研究,即在雷诺数为零和魏森贝格数较高时出现的混沌流动状态。我们旨在阐明在空间域中进行的流动特性测量与在时间域中进行的测量之间的关系,这是解释弹性湍流实验结果的关键要点,并讨论泰勒假设的有效性。为此,我们对奥尔德罗伊德 - B 粘弹性流体的二维柯尔莫哥洛夫流进行了广泛的直接数值模拟。静态点状数值探针放置在流动中的不同位置,特别是在平均流幅的极值处。在充分发展的弹性湍流状态下的结果表明,与平均流相比,速度波动很大,导致泰勒冻结场假设部分失效。虽然通过频谱和结构函数探测的二阶统计量在空间和时间域中显示出一致的标度行为,但三阶统计量突出了明显的差异。特别是时间分析未能捕捉到流向纵向速度增量的偏度。最后,我们评估了流动湍流波动的统计不均匀度和各向同性程度与尺度的函数关系。虽然系统在横向方向上只是弱非均匀的,但发现在所有尺度上它都是高度各向异性的。

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