网格湍流衰减控制尺度识别的数据同化研究

V. Mons, J. Chassaing, T. Gomez, P. Sagaut
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引用次数: 0

摘要

不可压缩均匀各向同性湍流(HIT)的衰减可以通过网格湍流实验来研究,这是湍流理论中最重要的问题之一,因为各向同性湍流是对湍流非线性特征进行最深入研究的框架。尽管一个世纪以来对HIT进行了大量的研究,但仍有许多问题有待解决。其中,控制HIT衰变的尺度的确定还有待进一步研究。虽然人们一致认为,湍流动能K在经过一个可能的瞬态松弛阶段后,遵循一个代数定律,即K(t)∝tnK,但指数nK与初始条件的某些特定特征的依赖性问题引起了一些争议。然而,最近的研究表明,没有一个普遍的机制,衰变速率肯定是由初始条件的细节决定的。实际上,文献中一般认为,指数nK与纵向速度相关函数f (r, t = 0)在物理空间中的渐近大尺度行为有关,或者等价地与谱空间中的磁能谱me (k, t = 0)的渐近行为有关。但值得记住的是,由于技术限制,在比积分尺度大得多的尺度上,速度相关函数或能谱的确切行为目前逃避了实验和数值研究。此外,大尺度渐近行为的概念很难与现实生活中的湍流相一致,这些湍流在空间上是有界的,只能在有限时间内观察到。值得注意的是,孔德-贝洛-柯尔辛理论(Comte-Bellot corsin theory)在预测指数nk值方面被证明是有效的,它依赖于一个单一的长度尺度,即积分尺度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A DATA ASSIMILATION STUDY FOR THE IDENTIFICATION OF SCALES GOVERNING GRID TURBULENCE DECAY
The decay of incompressible homogeneous isotropic turbulence (HIT), which can be studied via grid turbulence experiments, is among the most important issue in turbulence theory, since isotropic turbulence is the framework in which the deepest investigations of nonlinear features o f turbulence can be performed. Even though numerous studies have been devoted to HIT since about one century, many questions remain open. Among them, the identification of scales which govern the decay of HIT still deserves further investigations. Although there is consensus that the turbu lent kinetic energyK, after a possible transient relaxation phase, follows an algebraic law, i.e. K(t) ∝ tnK , the question of the dependence of the exponent nK to some specific features of the initial condition has raised some controver sies. However, the most recent works indicate that there is no universal regime and that the decay rate is definitely governed by the details of the initial condition. Indeed, it is generally stated in the literature that the exponent nK is related to the asymptotic large-scale behavior of the longi tudinal velocity correlation functionf (r, t = 0) in physical space, or equivalently, to the asymptotic behavior of the ki netic energy spectrumE(k, t = 0) in spectral space. But it is worth keeping in mind that, due to technological limitations, the exact behavior of the velocity correlation function, or that of the energy spectrum, at scales much larger than the integral scale escapes both experimental and numerical investigation at the present time. Besides, the con cept of large-scale asymptotic behavior is hard to reconcil e with real-life turbulent flows, which are bounded in space and can be observed over finite times only. It is also interesting to note that the Comte-Bellot Corrsin theory, which proves to be effective in predicting the value of the exponentnK , relies on a single length scale which is the integral scale.
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