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arXiv 2511.03462physics.flu-dyn
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利用扩散波光谱测量湍流边界处耗散率的时空统计

Spatiotemporal statistics of the dissipation rate at the boundary of a turbulent flow using Diffusing-Wave Spectroscopy

Enzo Francisco, Julien Lambret, Sébastien Aumaître

AI总结:

本文首次利用扩散波光谱对湍流边界耗散率进行时空分辨测量,验证了 ε∝Re³ 标度律并发现其涨落呈对数正态分布,但功率密度谱与均匀各向同性湍流预期不符。

摘要:

我们使用扩散波光谱(DWS)首次对湍流边界处的耗散率 ε 进行了直接的空间和时间分辨测量。我们在先前发表的文章中已经证明,该技术能够提供牛顿流体耗散率的空间分布图。本文中,我们将该技术应用于由叶轮在方形箱体内搅拌流体所产生的湍流边界处。尽管测量仅在边界附近的小区域内进行,我们仍表明耗散率与注入功率保持正比,并遵循湍流标度律 ε∝Re³,其中雷诺数 Re 的范围为 1.5×10⁴ 至 6×10⁵。对于该流动,无需对数修正即可重现平坦边界附近的耗散行为。此外,我们的实验装置还允许测量边界附近耗散率的时空涨落。这些涨落相当大(相对涨落约为 50%),并且很好地符合对数正态分布,这与均匀各向同性湍流(HIT)体相中耗散率的预期一致,但功率密度谱(PDS)并不符合 HIT 所预期的谱形。

英文摘要:

We use Diffusing Wave Spectroscopy (DWS) to perform the first direct space- and time-resolved measurement of the dissipation rate~$ε$ at the boundary of a turbulent flow. We have shown in a previous publication that this technique provides maps of the dissipation rate of Newtonian fluids~\cite{Francisco}. Here, we apply the technique at the boundary of a turbulent flow generated in a square box by an impeller stirring the fluids. Although the measurement is made on a small region near the boundary, we show that the dissipation remains proportional to the injected power and follows the turbulent scaling $ε\propto \mathrm{Re}^3$, with Re being the Reynolds number ranging from $1.5 \times 10^4$ to $6 \times 10^5$. With this flow, there is no need for logarithmic corrections to reproduce the dissipation near the flat boundary. In addition, our setup allows us to measure the spatio-temporal fluctuations of the dissipation near the boundary. These fluctuations are quite large (the relative fluctuations are about 50\%) and are well described by a log-normal distribution, as expected for the dissipation rate in the bulk of homogeneous and isotropic turbulence (HIT) but Power Density Spectra (PDS) do not correspond to those expected for HIT \cite{Li07,Graham16,K62}

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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