Hostname: page-component-78c5997874-m6dg7 Total loading time: 0 Render date: 2024-11-04T22:00:02.238Z Has data issue: false hasContentIssue false

Stepwise transitions in spin-up of rotating Rayleigh–Bénard convection

Published online by Cambridge University Press:  01 February 2021

D. Noto*
Affiliation:
Laboratory for Flow Control, Faculty of Engineering, Hokkaido University, Sapporo060-8628, Japan
Y. Tasaka
Affiliation:
Laboratory for Flow Control, Faculty of Engineering, Hokkaido University, Sapporo060-8628, Japan
T. Yanagisawa
Affiliation:
Laboratory for Flow Control, Faculty of Engineering, Hokkaido University, Sapporo060-8628, Japan Japan Agency for Marine-Earth Science and Technology (JAMSTEC), Yokosuka, Kanagawa 237-0061, Japan
T. Miyagoshi
Affiliation:
Japan Agency for Marine-Earth Science and Technology (JAMSTEC), Yokosuka, Kanagawa 237-0061, Japan
*
Email address for correspondence: [email protected]

Abstract

Transient behaviours during spin-up in rotating Rayleigh–Bénard convection (RBC) with imposed rotation were quantitatively investigated in laboratory experiments. Horizontal and vertical velocity fields were measured by particle image velocimetry with water as the test fluid. Varying the aspect ratio, Rayleigh number and Taylor number, a total of twenty parameters were systematically explored. Toroidal and spiral rolls were formed when the flow reached the rigid-body rotation state, and creation of these structures propagated from the rim towards the internal regions together with the development of the spin-up. Alternate alignments of rolls with opposite meridional circulation transported azimuthal momentum in the rigid-body rotation, and a meandering velocity profile in the radial direction, induced Kelvin–Helmholtz (KH) instability generating azimuthally aligned vortices. The vortices progressively decreased in horizontal dimensions with the wall-to-centre propagation of the vortex formation, but the vortical structures remain larger than the columnar vortices formed in the equilibrium state of a rotating RBC. At the intermediate radius of the fluid layer, the wall-to-centre propagation of the roll formation was overtaken by that of the KH vortex formation. Farther into the interior region, thermal plumes forming columnar vortices were generated as separations of the thermal boundary layers, and the system reached an equilibrium state of rotating RBC dominated by columnar vortices. Use of a fluid vessel with a moderate aspect ratio clarified these transitions to occur in a stepwise fashion, and a spin-up time scale unique in the rotating RBC was found to be from a few to 10 times the Ekman time scale.

Type
JFM Papers
Copyright
© The Author(s), 2021. Published by Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

Akonur, A. & Lueptow, R.M. 2003 Three-dimensional velocity field for wavy Taylor–Couette flow. Phys. Fluids 15 (4), 947960.CrossRefGoogle Scholar
Benton, E.R. & Clark, A. Jr. 1974 Spin-up. Annu. Rev. Fluid Mech. 6 (1), 257280.CrossRefGoogle Scholar
Boubnov, B.M. & Golitsyn, G.S. 1986 Experimental study of convective structures in rotating fluids. J. Fluid Mech. 167, 503531.CrossRefGoogle Scholar
Cheng, J.S., Aurnou, J.M., Julien, K. & Kunnen, R.P.J. 2018 A heuristic framework for next-generation models of geostrophic convective turbulence. Geophys. Astrophys. Fluid Dyn. 112 (4), 277300.CrossRefGoogle Scholar
Clever, R.M. & Busse, F.H. 1987 Nonlinear oscillatory convection. J. Fluid Mech. 176, 403417.CrossRefGoogle Scholar
Davey, A., Di Prima, R.C. & Stuart, J.T. 1968 On the instability of Taylor vortices. J. Fluid Mech. 31 (1), 1752.CrossRefGoogle Scholar
Drazin, P.G. & Reid, W.H. 2004 Hydrodynamic Stability. Cambridge University Press.CrossRefGoogle Scholar
Fujita, K., Tasaka, Y., Yanagisawa, T., Noto, D. & Murai, Y. 2020 Three-dimensional visualization of columnar vortices in rotating Rayleigh–Bénard convection. J. Vis. 23 (4), 635647.Google Scholar
Grannan, A.M., Favier, B., Le Bars, M. & Aurnou, J.M. 2016 Tidally forced turbulence in planetary interiors. Geophys. J. Intl 208 (3), 16901703.Google Scholar
Gray, D.D. & Giorgini, A. 1976 The validity of the Boussinesq approximation for liquids and gases. Intl J. Heat Mass Transfer 19 (5), 545551.CrossRefGoogle Scholar
Greenspan, H.P. 1968 The Theory of Rotating Fluids. Cambridge University Press.Google Scholar
Greenspan, H.P. & Howard, L.N. 1963 On a time-dependent motion of a rotating fluid. J. Fluid Mech. 17 (3), 385404.CrossRefGoogle Scholar
Horn, S. & Shishkina, O. 2014 Rotating non-Oberbeck–Boussinesq Rayleigh–Bénard convection in water. Phys. Fluids 26 (5), 055111.CrossRefGoogle Scholar
Jones, C.A. 1985 The transition to wavy Taylor vortices. J. Fluid Mech. 157, 135162.CrossRefGoogle Scholar
Jones, C.A. 2011 Planetary magnetic fields and fluid dynamos. Annu. Rev. Fluid Mech. 43, 583614.CrossRefGoogle Scholar
Julien, K., Rubio, A.M., Grooms, I. & Knobloch, E. 2012 Statistical and physical balances in low Rossby number Rayleigh–Bénard convection. Geophys. Astrophys. Fluid Dyn. 106, 392428.CrossRefGoogle Scholar
King, E.M., Stellmach, S. & Aurnou, J.M. 2012 Heat transfer by rapidly rotating Rayleigh–Bénard convection. J. Fluid Mech. 691, 568582.CrossRefGoogle Scholar
Koschmieder, E.L. 1968 Convection on a non-uniformly heated, rotating plane. J. Fluid Mech. 33 (3), 515527.CrossRefGoogle Scholar
Krishnamurti, R. 1973 Some further studies on the transition to turbulent convection. J. Fluid Mech. 60 (2), 285303.CrossRefGoogle Scholar
Liu, Y. & Ecke, R.E. 2009 Heat transport measurements in turbulent rotating Rayleigh–Bénard convection. Phys. Rev. E 80, 036314.CrossRefGoogle ScholarPubMed
Martinand, D., Serre, E. & Lueptow, R.M. 2014 Mechanisms for the transition to waviness for Taylor vortices. Phys. Fluids 26 (9), 094102.CrossRefGoogle Scholar
Noto, D., Tasaka, Y., Yanagisawa, T. & Murai, Y. 2019 Horizontal diffusive motion of columnar vortices in rotating Rayleigh–Bénard convection. J. Fluid Mech. 871, 401426.CrossRefGoogle Scholar
Noto, D., Tasaka, Y., Yanagisawa, T., Park, H.J. & Murai, Y. 2018 Vortex tracking on visualized temperature fields in a rotating Rayleigh–Bénard convection. J. Vis. 21 (6), 987998.CrossRefGoogle Scholar
Ravichandran, S. & Wettlaufer, J.S. 2020 Transient convective spin-up dynamics. J. Fluid Mech. 897, A24.CrossRefGoogle Scholar
Sakai, S. 1997 The horizontal scale of rotating convection in the geostrophic regime. J. Fluid Mech. 333, 8595.CrossRefGoogle Scholar
Stevens, R.J.A.M., Clercx, H.J.H. & Lohse, D. 2013 Heat transport and flow structure in rotating Rayleigh-Bénard convection. Eur. J. Mech. (B/Fluids) 40, 4149.CrossRefGoogle Scholar
Vorobieff, P. & Ecke, R.E. 1998 Transient states during spin-up of a Rayleigh–Bénard cell. Phys. Fluids 10 (10), 25252538.CrossRefGoogle Scholar
Wedemeyer, E.H. 1964 The unsteady flow within a spinning cylinder. J. Fluid Mech. 20 (3), 383399.CrossRefGoogle Scholar
Weidman, P.D. 1976 On the spin-up and spin-down of a rotating fluid. Part 1. Extending the Wedemeyer model. J. Fluid Mech. 77 (4), 685708.CrossRefGoogle Scholar
Weiss, S. & Ahlers, G. 2011 Heat transport by turbulent rotating Rayleigh–Bénard convection and its dependence on the aspect ratio. J. Fluid Mech. 309, 120.Google Scholar
Zhong, J.-Q., Patterson, M.D. & Wettlaufer, J.S. 2010 Streaks to rings to vortex grids: generic patterns in transient convective spin up of an evaporating fluid. Phys. Rev. Lett. 105 (4), 044504.CrossRefGoogle ScholarPubMed

Noto et al. supplementary movie 1

See word file for movie caption

Download Noto et al. supplementary movie 1(Video)
Video 3.3 MB

Noto et al. supplementary movie 2

See word file for movie caption

Download Noto et al. supplementary movie 2(Video)
Video 6.5 MB
Supplementary material: File

Noto et al. supplementary material

Captions for movies 1-2

Download Noto et al. supplementary material(File)
File 12.4 KB