Azimuthal diffusion of the large-scale-circulation plane, and absence of significant non-Boussinesq effects, in turbulent convection near the ultimate-state transition

Abstract

We present measurements of the orientation ${\theta }_0$ and temperature amplitude $\delta$ of the large-scale circulation in a cylindrical sample of turbulent Rayleigh-Benard convection (RBC) with aspect ratio $\Gamma \equiv D/L=1.00$ ($D$ and $L$ are the diameter and height respectively) and for the Prandtl number $Pr\simeq 0.8$. Results for ${\theta }_0$ revealed a preferred orientation with upflow in the West, consistent with a broken azimuthal invariance due to Earth's Coriolis force [see \cite{BA06b}]. They yielded the azimuthal diffusivity $D_{\theta }$ and a corresponding Reynolds number $R{e}_{\theta }$ for Rayleigh numbers over the range $2\times 10^{12}<Ra<1.5\times 10^{14}$. In the classical state ($Ra<2\times 10^{13}$) the results were consistent with the measurements by \cite{BA06a} for $Ra<10^{11}$ and $Pr=4.38$ which gave $R{e}_{\theta }\propto R{a}^{0.28}$, and with the Prandtl-number dependence $R{e}_{\theta }\propto P{r}^{-1.2}$ as found previously also for the velocity-fluctuation Reynolds number $R{e}_V$ \cite[]{HGBA15b}. At larger $Ra$ the data for $R{e}_{\theta }(Ra)$ revealed a transition to a new state, known as the "ultimate" state, which was first seen in the Nusselt number $Nu(Ra)$ and in $R{e}_V(Ra)$ at $R{a}_1^{\ast }\simeq 2\times 10^{13}$ and $R{a}_2^{\ast }\simeq 8\times 10^{13}$. In the ultimate state we found $R{e}_{\theta }\propto R{a}^{0.40\pm 0.03}$. Recently \cite{SU15} claimed that non-Oberbeck-Boussinesq effects on the Nusselt and Reynolds numbers of turbulent RBC may have been interpreted erroneously as a transition to a new state. We demonstrate that their reasoning is incorrect and that the transition observed in the Göttingen experiments and discussed in the present paper is indeed to a new state of RBC referred to as "ultimate".

12 pages, 4 figures, to be pub. in JFMR

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• Thermal Convection over Fractal Surfaces