Parente E, Farano M, Robinet J-Ch, De Palma P, Cherubini S
Department of Mechanics, Mathematics and Management, Politecnico di Bari, Via Re David 200, 70125 Bari, Italy.
Laboratoire DynFluid, Arts et Metiers ParisTech, Bd de l'Hopital 75013 Paris, France.
Philos Trans A Math Phys Eng Sci. 2022 Jun 27;380(2226):20210031. doi: 10.1098/rsta.2021.0031. Epub 2022 May 9.
A new mathematical framework is proposed for characterizing the coherent motion of fluctuations around a mean turbulent channel flow. We search for statistically invariant coherent solutions of the unsteady Reynolds-averaged Navier-Stokes equations written in a perturbative form with respect to the turbulent mean flow, using a suitable approximation of the Reynolds stress tensor. This is achieved by setting up a continuation procedure of known solutions of the perturbative Navier-Stokes equations, based on the continuous increase of the turbulent eddy viscosity towards its turbulent value. The recovered solutions, being sustained only in the presence of the Reynolds stress tensor, are representative of the statistically coherent motion of turbulent flows. For small friction Reynolds number and/or domain size, the statistically invariant motion is almost identical to the corresponding invariant solution of the Navier-Stokes equations. Whereas, for sufficiently large friction number and/or domain size, it considerably departs from the starting invariant solution of the Navier-Stokes equations, presenting spatial structures, main wavelengths and scaling very close to those characterizing both large- and small-scale motion of turbulent channel flows. This article is part of the theme issue 'Mathematical problems in physical fluid dynamics (part 2)'.
提出了一种新的数学框架,用于描述平均湍流通道流周围波动的相干运动。我们使用雷诺应力张量的适当近似,寻找以湍流平均流为微扰形式写出的非定常雷诺平均纳维-斯托克斯方程的统计不变相干解。这是通过基于湍流涡粘性朝着其湍流值的连续增加,建立微扰纳维-斯托克斯方程已知解的延拓过程来实现的。恢复的解仅在雷诺应力张量存在的情况下维持,代表了湍流的统计相干运动。对于小摩擦雷诺数和/或域尺寸,统计不变运动几乎与纳维-斯托克斯方程的相应不变解相同。然而,对于足够大的摩擦数和/或域尺寸,它与纳维-斯托克斯方程的起始不变解有很大不同,呈现出与湍流通道流的大尺度和小尺度运动特征非常接近的空间结构、主要波长和标度。本文是主题为“物理流体动力学中的数学问题(第2部分)”的一部分。