Hostname: page-component-cd9895bd7-gvvz8 Total loading time: 0 Render date: 2024-12-19T02:58:50.200Z Has data issue: false hasContentIssue false

A comparison between buoyant vortex rings and vortex pairs

Published online by Cambridge University Press:  28 March 2006

J. S. Turner
Affiliation:
Mechanics of Fluids Department, University of Manchester

Abstract

In this paper it is shown how earlier results for buoyant vortex rings may be extended to describe the corresponding two-dimensional case, which arises in the theory of bent-over plumes. It is again assumed that in uniform surroundings the circulation remains constant while the buoyancy acts to increase the momentum of the pair. The behaviour in two dimensions is quite different from that in three, however; a buoyant vortex ring spreads linearly with height, whereas a buoyant pair spreads exponentially with height, or linearly with time (and therefore, in a bent-over plume, linearly with distance downwind).

The theory has been extended to describe the rise of buoyant rings and pairs through stably stratified surroundings having a linear density gradient. The behaviour near the maximum height reached is found to depend critically in both cases on the relative rates at which the circulation and the momentum fall to zero. If these reach zero together, the rings or pairs will steadily increase in size and come to rest at a finite height and with a finite radius. If the circulation is non-zero when the momentum vanishes, the radius begins to decrease soon after the buoyancy becomes zero, and the vortices will therefore tend to break up suddenly and mix into their surroundings. There is a considerable increase in the final height which should be attained by vortex rings or bentover plumes if the initial circulation is increased; it is suggested that releasing smoke intermittently, rather than continuously, at high velocity might be a means of increasing the effective height of chimneys in calm conditions. When the circulation reaches zero before the momentum does, the solutions indicate that the radius becomes very large near the level of zero buoyancy.

Type
Research Article
Copyright
© 1960 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

Lambs, H. 1932 Hydrodynamics, 6th ed. Cambridge University Press.
Morton, B. R., Taylor, G. I. & Turner, J. S. 1956 Proc. Roy. Soc. A, 234, 1.
Morton, B. R. 1959 J. Fluid Mech. 5, 151.
Rouse, H., Yih, C. S. & Humphreys, H. W. 1952 Tellus, 4, 201.
Scorer, R. S. 1958 Natural Aerodynamics. London: Pergamon Press.
Turner, J. S. 1957 Proc. Roy. Soc. A, 239, 61.
Woodward, B. 1959 Quart. J. R. Met. Soc. 85, 144.