Optimal Taylor-Couette flow: direct numerical simulations

Abstract

We numerically simulate turbulent Taylor-Couette flow for independently rotating inner and outer cylinders, focusing on the analogy with turbulent Rayleigh-Bénard flow. Reynolds numbers of $R{e}_i=8\cdot 10^3$ and $R{e}_o=\pm 4\cdot 10^3$ of the inner and outer cylinders, respectively, are reached, corresponding to Taylor numbers Ta up to $10^8$. Effective scaling laws for the torque and other system responses are found. Recent experiments with the Twente turbulent Taylor-Couette ($T^{3}C$) setup and with a similar facility in Maryland at very high Reynolds numbers have revealed an optimum transport at a certain non-zero rotation rate ratio $a=-{\omega }_o/{\omega }_i$ of about $a_{opt}=0.33-0.35$. For large enough $Ta$ in the numerically accessible range we also find such an optimum transport at non-zero counter-rotation. The position of this maximum is found to shift with the driving, reaching a maximum of $a_{opt}=0.15$ for $Ta=2.5\cdot 10^7$. An explanation for this shift is elucidated, consistent with the experimental result that $a_{opt}$ becomes approximately independent of the driving strength for large enough Reynolds numbers. We furthermore numerically calculate the angular velocity profiles and visualize the different flow structures for the various regimes. By writing the equations in a frame co-rotating with the outer cylinder a link is found between the local angular velocity profiles and the global transport quantities.

Under consideration for publication in JFM, 31 pages, 25 figures

References in corpus (3)

• Direct Numerical Simulations of Local and Global Torque in Taylor-Couette Flow up to Re=30.000
• Direct Numerical Simulation of turbulent Taylor-Couette flow
• Non-Oberbeck-Boussinesq effects in two-dimensional Rayleigh-Benard convection in glycerol

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