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Effect of roll number on the statistics of turbulent Taylor-Couette flow

Rodolfo Ostilla-Mónico1,2,*, Detlef Lohse1, and Roberto Verzicco3,1

  • 1Physics of Fluids Group, Faculty of Science and Technology, MESA+ Research Institute, and J. M. Burgers Centre for Fluid Dynamics, University of Twente, PO Box 217, 7500 AE Enschede, The Netherlands
  • 2School of Engineering and Applied Sciences, Harvard University, Cambridge, Massachusetts, USA
  • 3Dipartimento di Ingegneria Industriale, University of Rome “Tor Vergata,” Via del Politecnico 1, Rome 00133, Italy

  • *rostillamonico@g.harvard.edu

Phys. Rev. Fluids 1, 054402 – Published 7 September, 2016

DOI: https://doi.org/10.1103/PhysRevFluids.1.054402

Abstract

A series of direct numerical simulations in large computational domains has been performed in order to probe the spatial feature robustness of the Taylor rolls in turbulent Taylor-Couette flow. The latter is the flow between two coaxial independently rotating cylinders of radius ri and ro, respectively. Large axial aspect ratios Γ=78 [with Γ=L/(rori), and L the axial length of the domain] and a simulation with Γ=14 were used in order to allow the system to select the most unstable wave number and to possibly develop multiple states. The radius ratio was taken as η=ri/ro=0.909, the inner cylinder Reynolds number was fixed to Rei=3.4×104, and the outer cylinder was kept stationary, resulting in a frictional Reynolds number of Reτ500, except for the Γ=14 simulation where Rei=1.5×104 and Reτ240. The large-scale rolls were found to remain axially pinned for all simulations. Depending on the initial conditions, stable solutions with different number of rolls nr and roll wavelength λz were found for Γ=7. The effect of λz and nr on the statistics was quantified. The torque and mean flow statistics were found to be independent of both λz and nr, while the velocity fluctuations and energy spectra showed some box-size dependence. Finally, the axial velocity spectra were found to have a very sharp dropoff for wavelengths larger than λz, while for the small wavelengths they collapse.

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