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Secondary flows and bubbly drag reduction on heterogeneously rough surfaces in Taylor--Couette turbulence

ORAL

Abstract

We investigate turbulent flow at Reynolds numbers (Re) ranging from $0.5 \times 10^{6}$ till $1.8 \times 10^{6}$ over surfaces that are composed of rough and smooth patches. Our main interest is in how the structure of the flow is influenced by this alternating rough and smooth surface, and how this changes the position of air bubbles in the flow. For this we use the Taylor--Couette geometry, which allows for accurate drag and flow measurements, as well as flow visualisations through its transparant outer cylinder. The inner cylinder wall is covered with sandpaper, leaving room between bands to form a constant pattern in axial direction. This results in a strong secondary flow pattern of radially outward flow on the rough patches and radially inward flow on the smooth patches. Surprisingly, air bubbles do not follow this secondary flow, but rather accumulate on top of the rough wall sections in the flow. Here, locally, the drag is largest and so the drag reducing effect of the bubbles is felt strongest. Therefore, a larger maximum value of bubbly drag reduction is found for the alternating rough and smooth inner cylinder walls compared to the completely rough and completely smooth inner cylinder walls.

Authors

  • Pim Bullee

    Twente University

  • Dennis Bakhuis

    Twente University

  • Rodrigo Ezeta

    Twente University

  • Sander Huisman

    Twente University

  • Chao Sun

    Tsinghua University, Tsinghua University, 100084 Beijing, China

  • Rob Lammertink

    University of Twente, Twente University

  • Detlef Lohse

    Physics of Fluids Group and Max Planck Center Twente, MESA+ Institute and J. M. Burgers Centre for Fluid Dynamics, University of Twente, P.O. Box 217,, Physics of Fluids group, University of Twente, Physics of Fluids Group, University of Twente, Univ of Twente, PoF - University of Twente, The Netherlands, Twente University, Physics of Fluids Group, University of Twente; Max Planck Institute for Dynamics and Self-Organization, University of Twente