论文标题

在平坦沉积床的不稳定性方面相对于涟漪样图案

On the scaling of the instability of a flat sediment bed with respect to ripple-like patterns

论文作者

Scherer, Markus, Kidanemariam, Aman G., Uhlmann, Markus

论文摘要

我们通过具有完全分辨颗粒的直接数值模拟来研究湍流开口通道流中水下横向床形的形成。本分析的主要目标是解决以下问题,是用颗粒直径的初始图案波长尺度还是平均流体高度。先前的一项研究(Kidanemariam和Uhlmann,J。流体机械,第818卷,2017年,第716-743页)已经观察到在粒子直径的75-100倍的最不稳定图案波长的下限,相当于平均流体高度的3-4倍。在当前的论文中,我们独立地根据粒子直径和平均流体高度来改变流向框的长度,以区分两个可能的缩放关系。对于所选的参数范围,获得的结果清楚地表现出具有颗粒直径的初始图案波长的缩放,并在大约80个粒子直径的流倾向范围内有一个下限。另一方面,在较长的域中,在初始波长的150-180倍范围内观察到了颗粒直径的150-180倍,这与实验测量非常吻合。另一方面,平均流体高度的变化似乎对最不稳定的初始图案波长没有显着影响。此外,对于具有最大相对淹没的情况,我们观察到与进化和叠加的幅度相似的跨度和流向沉积物波,从而导致三维沉积物模式。

We investigate the formation of subaqueous transverse bedforms in turbulent open channel flow by means of direct numerical simulations with fully-resolved particles. The main goal of the present analysis is to address the question whether the initial pattern wavelength scales with the particle diameter or with the mean fluid height. A previous study (Kidanemariam and Uhlmann, J. Fluid Mech., vol. 818, 2017, pp. 716-743) has observed a lower bound for the most unstable pattern wavelength in the range 75-100 times the particle diameter, which was equivalent to 3-4 times the mean fluid height. In the current paper, we vary the streamwise box length in terms of the particle diameter and of the mean fluid height independently in order to distinguish between the two possible scaling relations. For the chosen parameter range, the obtained results clearly exhibit a scaling of the initial pattern wavelength with the particle diameter, with a lower bound around a streamwise extent of approximately 80 particle diameters. In longer domains, on the other hand, patterns are observed at initial wavelengths in the range 150-180 times the particle diameter, which is in good agreement with experimental measurements. Variations of the mean fluid height, on the other hand, seem to have no significant influence on the most unstable initial pattern wavelength. Furthermore, for the cases with the largest relative submergence, we observe spanwise and streamwise sediment waves of similar amplitude to evolve and superimpose, leading to three-dimensional sediment patterns.

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