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Turbulent convection at very high Rayleigh numbers

Author

Listed:
  • J. J. Niemela

    (University of Oregon)

  • L. Skrbek

    (University of Oregon)

  • K. R. Sreenivasan

    (University of Oregon
    Mason Laboratory, Yale University)

  • R. J. Donnelly

    (University of Oregon)

Abstract

Turbulent convection occurs when the Rayleigh number (Ra)—which quantifies the relative magnitude of thermal driving to dissipative forces in the fluid motion—becomes sufficiently high. Although many theoretical and experimental studies of turbulent convection exist, the basic properties of heat transport remain unclear. One important question concerns the existence of an asymptotic regime that is supposed to occur at very high Ra. Theory predicts that in such a state the Nusselt number (Nu), representing the global heat transport, should scale as Nu ∝ Raβ with β = 1/2. Here we investigate thermal transport over eleven orders of magnitude of the Rayleigh number (106 ≤ Ra ≤ 1017), using cryogenic helium gas as the working fluid. Our data, over the entire range of Ra, can be described to the lowest order by a single power-law with scaling exponent β close to 0.31. In particular, we find no evidence for a transition to the Ra1/2 regime. We also study the variation of internal temperature fluctuations with Ra, and probe velocity statistics indirectly.

Suggested Citation

  • J. J. Niemela & L. Skrbek & K. R. Sreenivasan & R. J. Donnelly, 2000. "Turbulent convection at very high Rayleigh numbers," Nature, Nature, vol. 404(6780), pages 837-840, April.
  • Handle: RePEc:nat:nature:v:404:y:2000:i:6780:d:10.1038_35009036
    DOI: 10.1038/35009036
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    Cited by:

    1. Yadati, Yash & Mears, Nicholas & Chatterjee, Atanu, 2020. "Spatio-temporal characterization of thermal fluctuations in a non-turbulent Rayleigh–Bénard convection at steady state," Physica A: Statistical Mechanics and its Applications, Elsevier, vol. 547(C).

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