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Thermals with background rotation and stratification

Published online by Cambridge University Press:  26 April 2006

Karl R. Helfrich
Affiliation:
Department of Physical Oceanography, Woods Hole Oceanographic Institution, Woods Hole, MA 02543, USA

Abstract

Scaling analysis and experiments are used to study the evolution of thermals in the presence of background rotation. When the ambient environment is homogeneous, the thermal rises and expands until it reaches a critical height where the Rossby number becomes ∼ 1. The thermal then stops expanding and rises in a column. Both the critical height and column radius scale with (F0f-2)1/4. F0 is the initial thermal buoyancy and f is the Coriolis frequency. The thermal vertical velocity is independent of f. When the background is stratified with buoyancy frequency N, the thermal rises to a neutral buoyancy level which scales with (F0N-2)1/4. For N/f [Lt ] 0.6 column formation occurs before the thermal reaches the neutral level. For N/f [Gt ] 0.6 the thermal reaches the neutral level before rotation is important. In both regimes, geostrophic adjustment eventually causes the formation of a baroclinic vortex consisting of an anticyclonic lens of thermal fluid at the neutral level and cyclonic circulation below. The lens has Nh/fl ∼ 1. The lens thickness 2h and the radius l obey relations of the form (F0N-2)1/4 (N/f)m. However, the exponents m are different in the two regimes. The relevance of these results to deep-ocean convection and hydrothermal venting is discussed.

Type
Research Article
Copyright
© 1994 Cambridge University Press

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References

Baker, E. T., Lavelle, J. W., Feely, R. A., Massoth, G. J. & Walker, S. L. 1989 Episodic venting of hydrothermal fluids from the Juan de Fuca Ridge. J. Geophys. Res. 94, 92379250.Google Scholar
Chadwick, W. R., Embley, R. W. & Fox, C. G. 1991 Evidence for volcanic eruption on the southern Juan de Fuca Ridge between 1981 and 1987. Nature 350, 416418.Google Scholar
Elrick, J. R. 1979 Interaction between a discrete downdraft and a rotating environment. J. Atmos. Sci. 36, 306312.Google Scholar
Fernando, H. J. S., Chen, R.-R. & Boyer, D. L. 1991 Effects of rotation on convective turbulence. J. Fluid Mech. 228, 513547.Google Scholar
Gascard, J.-C. 1978 Mediterranean deep water formation – baroclinic instability and oceanic eddies. Oceanol. Acta 1, 315330.Google Scholar
Gill, A. E. 1981 Homogeneous intrusions in a rotating stratified fluid. J. Fluid Mech. 103, 275296.Google Scholar
Griffiths, R. W. & Linden, P. F. 1981 The stability of vortices in a rotating, stratified fluid. J. Fluid Mech. 105, 283316.Google Scholar
Helfrich, K. R. & Battisti, T. M. 1991 Experiments on baroclinic vortex shedding from hydrothermal plumes. J. Geophys. Res. 96, 1251112518.Google Scholar
Helfrich, K. R. & Send, U. 1988 Finite-amplitude evolution of two-layer geostrophic vortices. J. Fluid Mech. 197, 331348.Google Scholar
Jones, H. & Marshall, J. 1993 Convection with rotation in a neutral ocean; a study of open-ocean deep convection. J. Phys. Oceanogr. 23, 10091039.Google Scholar
Maxworthy, T. & Narimousa, S. 1993 Unsteady deep convection in a homogeneous rotating fluid. J. Phys. Oceanogr. in press.Google Scholar
Morton, B. R., Taylor, G. J. & Turner, J. S. 1956 Turbulent gravitational convection from maintained and instantaneous sources. Proc. R. Soc. Lond. A 234, 123.Google Scholar
Sanchez, O., Raymond, D. J., Libersky, L. & Petschek, A. G. 1989 The development of thermals from rest. J. Atmos. Sci. 46, 22802292.Google Scholar
Schott, F. & Leaman, K. D. 1991 Observations with moored acoustic doppler current profilers in the convection regime in the Gulf du Lion. J. Phys. Oceanogr. 21, 558574.Google Scholar
Scorer, R. S. 1957 Experiments on convection of isolated masses of buoyant fluid. J. Fluid Mech. 2, 583594.Google Scholar
Speer, K. G. 1989 A forced baroclinic vortex around a hydrothermal plume. Geophys. Res. Lett. 16, 461464.Google Scholar
Stommel, H., Voorhis, A. & Webb, D. 1971 Submarine clouds in the deep ocean. Am. Scientist 59, 717723.Google Scholar
Turner, J. S. 1973 Buoyancy Effects in Fluids. Cambridge University Press.
Turner, J. S. 1986 Turbulent entrainment: the development of the entrainment assumption, and its application to geophysical flows. J. Fluid Mech. 173, 431472.Google Scholar
Wilkins, E. M., Sasaki, Y. K., Friday, E. W., McCarthy, J. & McIntyre, J. R. 1969 Properties of simulated thermals in a rotating fluid. J. Geophys. Res. 74, 44724486.Google Scholar