Hostname: page-component-cd9895bd7-jn8rn Total loading time: 0 Render date: 2024-12-19T08:54:26.971Z Has data issue: false hasContentIssue false

The motion of the front of a gravity current travelling down an incline

Published online by Cambridge University Press:  19 April 2006

R. E. Britter
Affiliation:
Department of Applied Mathematics and Theoretical Physics, Silver Street, Cambridge CB3 9EW
P. F. Linden
Affiliation:
Department of Applied Mathematics and Theoretical Physics, Silver Street, Cambridge CB3 9EW

Abstract

The motion of the head of a gravity current travelling down a slope of angle θ to the horizontal is investigated in the laboratory. The head is produced by suddenly initiating a buoyancy flux from a line source at the top of the slope. It is found that for very small slopes (θ [les ] 0.5°) the head decelerates with distance from the source, but at greater slopes the buoyancy force is large enough to overcome frictional effects and a steady head velocity results. Over a wide range of slope angles the front velocity Uf, non-dimensionalized by the cube root of the buoyancy flux (g0Q)1/3, is almost independent of the slope angle and Uf/(g0Q)1/3 = 1.5 ± 0.2 for 5° [les ] θ [les ] 90°. This result is shown to follow from some simple analysis which relates the velocity of the front to the following flow. For a Boussinesq plume the front velocity is found to be approximately 60% of the mean velocity of the following flow. This means that the head increases in size as it travels down the slope, both by direct entrainment into the head itself and by addition of fluid from the following flow. We find that direct entrainment increases with increasing slope and accounts for one-tenth of the growth of the head at 10° and about two-thirds at 90°.

Type
Research Article
Copyright
© 1980 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

Britter, R. E. & Simpson, J. E. 1978 Experiments on the dynamics of a gravity current head. J. Fluid Mech. 88, 223240.Google Scholar
Ellison, T. H. & Turner, J. S. 1959 Turbulent entrainment in stratified flows. J. Fluid Mech. 6, 423448.Google Scholar
Georgeson, E. H. M. 1942 The free streaming of gases in sloping galleries. Proc. Roy. Soc. A 180, 484493.Google Scholar
Hopfinger, E. J. & Tochon-Dangay, J. C. 1977 A model study of powder-snow avalanches. Glaciology 19 (81), 343356.Google Scholar
Middleton, G. V. 1966 Experiments on density and turbidity currents. 1. Motion of the head. Can. J. Earth Sci. 3, 523546.Google Scholar
Prandtl, L. 1952 Essentials of Fluid Dynamics. London: Blackie.
Simpson, J. E. & Britter, R. E. 1979 The dynamics of the head of a gravity current advancing over a horizontal surface. J. Fluid Mech. 94, 477495.Google Scholar
Tochon-Dangay, J. C. 1977 Étude des courants de gravité sur forte pente avec application aux avalanches poudreuses. Thèse, L'Université Scientifique et Médicale de Grenoble.
Tsang, G. & Wood, I. R. 1968 Motion of two-dimensional starting plume. J. Engng Mech. Div. A.S.C.E. EM6, 15471561.Google Scholar
Turner, J. S. 1962 The ‘starting plume’ in neutral surroundings. J. Fluid Mech. 13, 356368.Google Scholar
Turner, J. S. 1973 Buoyancy Effects in Fluids. Cambridge University Press.
Wood, I. R. 1965 Studies in unsteady self preserving turbulent flows. Univ. of N.S.W., Aust., Water Res. Lab. Rep. no. 81.Google Scholar