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弱惯性波湍流的定量实验观测

Quantitative Experimental Observation of Weak Inertial-Wave Turbulence.

作者信息

Monsalve Eduardo, Brunet Maxime, Gallet Basile, Cortet Pierre-Philippe

机构信息

Université Paris-Saclay, CNRS, FAST, 91405 Orsay, France.

Université Paris-Saclay, CNRS, CEA, Service de Physique de l'État Condensé, 91191 Gif-sur-Yvette, France.

出版信息

Phys Rev Lett. 2020 Dec 18;125(25):254502. doi: 10.1103/PhysRevLett.125.254502.

DOI:10.1103/PhysRevLett.125.254502
PMID:33416336
Abstract

We report the quantitative experimental observation of the weak inertial-wave turbulence regime of rotating turbulence. We produce a statistically steady homogeneous turbulent flow that consists of nonlinearly interacting inertial waves, using rough top and bottom boundaries to prevent the emergence of a geostrophic flow. As the forcing amplitude increases, the temporal spectrum evolves from a discrete set of peaks to a continuous spectrum. Maps of the bicoherence of the velocity field confirm such a gradual transition between discrete wave interactions at weak forcing amplitude and the regime described by weak turbulence theory (WTT) for stronger forcing. In the former regime, the bicoherence maps display a near-zero background level, together with sharp localized peaks associated with discrete resonances. By contrast, in the latter regime, the bicoherence is a smooth function that takes values of the order of the Rossby number in line with the infinite-domain and random-phase assumptions of WTT. The spatial spectra then display a power-law behavior, both the spectral exponent and the spectral level being accurately predicted by WTT at high Reynolds number and low Rossby number.

摘要

我们报告了旋转湍流弱惯性波湍流状态的定量实验观测结果。我们利用粗糙的顶部和底部边界来防止地转流的出现,产生了一种由非线性相互作用的惯性波组成的统计稳定均匀湍流。随着强迫振幅的增加,时间谱从一组离散的峰值演变为连续谱。速度场的双相干图证实了在弱强迫振幅下离散波相互作用与强强迫下弱湍流理论(WTT)所描述的状态之间的这种逐渐转变。在前一种状态下,双相干图显示出接近零的背景水平,以及与离散共振相关的尖锐局部峰值。相比之下,在后一种状态下,双相干是一个平滑函数,其取值与罗斯比数的量级一致,这与WTT的无限域和随机相位假设相符。然后空间谱呈现出幂律行为,在高雷诺数和低罗斯比数下,谱指数和谱水平均由WTT准确预测。

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