An experimental study of off-centred rotating thermal convection: a laboratory model for the tidal effects

• Published in: Journal of fluid mechanics 2023-06, Vol.966, Article A21
• Main Authors: Hu, Yun-Bing, Xia, Ke-Qing
• Format: Article
• Language: English
• Subjects: Cellular convection; Centrifugal force; Cold; Convection; Convection cells; Earth; Fluid flow; Fluid mechanics; Free convection; Froude number; Gravity; Heat transport; Investigations; JFM Papers; Jupiter; Laboratories; Particle image velocimetry; Rayleigh-Benard convection; Rotation; Scale models; Solar system; Temperature measurement; Tidal effects; Volcanoes
• ISSN: 0022-1120; 1469-7645
• DOI: 10.1017/jfm.2023.432

A novel experiment was performed in rotating Rayleigh–Bénard convection (RRBC), wherein the convection cell with radius $R$ was shifted away from the rotation axis by a distance $d$. In this case, the centrifugal force felt by a fluid parcel (characterized by the Froude number $Fr$) can be decomposed into an axisymmetrical part $Fr_R$ and a directed one $Fr_d$. It has been reported that the global heat transport enhances at $Fr_{d,c}$ and then reaches an optimal state at $Fr_{d,max}$ (Hu et al., Phys. Rev. Lett., vol. 127, 2021, 244501). In this paper, the local properties after the offset effects set in are investigated further, which show different features before and after $Fr_{d,max}$. The local temperature measurements at the cell centre reveal that the bulk flow turns from a turbulent state into a laminar state at $Fr_{d,max}$, which is consistent with the particle image velocimetry results. This transition can be qualitatively understood by an equivalent tilted RRBC system. As for the hot and cold coherent structures near the sidewall, their vertical temperature variations reach a minimum at $Fr_{d,max}$, implying that these structures are mostly uniform in the vertical direction at $Fr_{d,max}$. Their temperature contrasts show a linear dependence on $Fr_d$ and start to deviate from this linear behaviour when $Fr_d>Fr_{d,max}$. Besides the dominant effects of $Fr_d$, the secondary effects of $Fr_R$ are also investigated. Due to the positive effect of $+Fr_R$ on the cold structure and the negative effect of $-Fr_R$ on the hot one, the cold structure is more coherent than the hot one, but its size is smaller. The shift of the cold cluster centre from the farthest point is also larger than the shift of the hot one from the nearest point.