CNRS, ONERA, Centrale Lille, Univ. Lille, Arts et Metiers ParisTech, FRE2017, Laboratoire de Mécanique des Fluides de Lille-Kampé de Fériet (LMFL), 59000 Lille, France.
Department of Aeronautics, Imperial College London, London SW7 2AZ, United Kingdom.
Phys Rev E. 2018 May;97(5-1):053103. doi: 10.1103/PhysRevE.97.053103.
On the basis of (i) particle image velocimetry data of a turbulent boundary layer with large field of view and good spatial resolution and (ii) a mathematical relation between the energy spectrum and specifically modeled flow structures, we show that the scalings of the streamwise energy spectrum E_{11}(k_{x}) in a wave-number range directly affected by the wall are determined by wall-attached eddies but are not given by the Townsend-Perry attached eddy model's prediction of these spectra, at least at the Reynolds numbers Re_{τ} considered here which are between 10^{3} and 10^{4}. Instead, we find E_{11}(k_{x})∼k_{x}^{-1-p} where p varies smoothly with distance to the wall from negative values in the buffer layer to positive values in the inertial layer. The exponent p characterizes the turbulence levels inside wall-attached streaky structures conditional on the length of these structures. A particular consequence is that the skin friction velocity is not sufficient to scale E_{11}(k_{x}) for wave numbers directly affected by the wall.
基于(i)具有大视场和良好空间分辨率的湍流边界层的粒子图像测速数据,以及(ii)能量谱与特定建模流结构之间的数学关系,我们表明,在受壁面直接影响的波数范围内,流向能量谱 E_{11}(k_{x})的标度由壁面附着涡旋决定,但不受 Townsend-Perry 附着涡旋模型对这些谱的预测,至少在本文考虑的雷诺数 Re_{τ}范围内如此,该雷诺数范围在 10^{3}到 10^{4}之间。相反,我们发现 E_{11}(k_{x})∼k_{x}^{-1-p},其中 p 值随着距壁面的距离从缓冲层中的负值平滑变化到惯性层中的正值。指数 p 描述了壁面附着条纹结构内部的湍流水平,条件是这些结构的长度。一个特别的结果是,对于受壁面直接影响的波数,摩擦速度不足以对 E_{11}(k_{x})进行标度。