High–Reynolds Number Taylor-Couette Turbulence

Author:

Grossmann Siegfried1,Lohse Detlef23,Sun Chao24

Affiliation:

1. Fachbereich Physik, University of Marburg, D-35032 Marburg, Germany

2. Physics of Fluids Group, Faculty of Science and Technology, J.M. Burgers Center for Fluid Dynamics, and MESA+ Institute, University of Twente, 7500 AE Enschede, Netherlands;,

3. Max Planck Institute for Dynamics and Self-Organization, 37077 Göttingen, Germany

4. Center for Combustion Energy and Department of Thermal Engineering, Tsinghua University, 100084 Beijing, China

Abstract

Taylor-Couette flow, the flow between two coaxial co- or counter-rotating cylinders, is one of the paradigmatic systems in the physics of fluids. The (dimensionless) control parameters are the Reynolds numbers of the inner and outer cylinders, the ratio of the cylinder radii, and the aspect ratio. One key response of the system is the torque required to retain constant angular velocities, which can be connected to the angular velocity transport through the gap. Whereas the low–Reynolds number regime was well explored in the 1980s and 1990s of the past century, in the fully turbulent regime major research activity developed only in the past decade. In this article, we review this recent progress in our understanding of fully developed Taylor-Couette turbulence from the experimental, numerical, and theoretical points of view. We focus on the parameter dependence of the global torque and on the local flow organization, including velocity profiles and boundary layers. Next, we discuss transitions between different (turbulent) flow states. We also elaborate on the relevance of this system for astrophysical disks (quasi-Keplerian flows). The review ends with a list of challenges for future research on turbulent Taylor-Couette flow.

Publisher

Annual Reviews

Subject

Condensed Matter Physics

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