Hostname: page-component-7479d7b7d-c9gpj Total loading time: 0 Render date: 2024-07-09T05:51:46.916Z Has data issue: false hasContentIssue false

Convection in a saturated porous medium at large Rayleigh number or Peclet number

Published online by Cambridge University Press:  28 March 2006

R. A. Wooding
Affiliation:
Applied Mathematics Laboratory, D.S.I.R., Wellington, New Zealand

Abstract

When the dimensions of a convective system in a saturated porous medium are sufficiently great, diffusion effects can be neglected except in regions where the gradients of fluid properties are very large. A boundary-layer theory is developed for vertical plane flows in such regions. In special cases, the theory is equivalent to that for laminar incompressible flow in a two-dimensional half-jet, or in a plane jet or round jet, for which similarity solutions are well known.

A number of experiments have been performed using a Hele-Shaw cell immersed in water, with a source of potassium permanganate solution located between the plates. At very small values of the source strength, a flow analogous to that of a plane jet from a slit is obtained. The distance advanced by the jet front, or cap, is measured as a function of time, and the velocity is found to be nearly proportional to the velocity of the fluid on the axis of the steady jet behind the cap, as given by the similarity law of Schlichting and Bickley. At large values of the source strength, a two-dimensional ‘broad jet’ of homogeneous solution descending under gravity is produced; the shape of the flow region can be calculated with little error from potential theory, neglecting the effect of the mixing layers.

A possible example of a mixing layer observed in a geothermal region is examined. The theoretical form of the temperature distribution is calculated numerically, taking into account the large viscosity variation with temperature and also the possibility of a large permeability variation. These effects are found to have less influence upon the solution than might have been expected. Quantitative values obtained for the physical parameters are consistent with other geophysical observations.

Type
Research Article
Copyright
© 1963 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

Banwell, C. J. 1957 Proc. ASME, 79, 255.
Bickley, W. G. 1937 Phil. Mag. (7), 23, 727.
Fürth, R. & Ullman, E. 1926 Kolloidschr. 41, 307.
Görtler, H. 1942 Z. angew. Math. Mech. 22, 244.
Jeffreys, Sir Harold 1959 The Earth, 4th ed. Cambridge University Press.
Lamb, H. 1932 Hydrodynamics. Cambridge University Press.
Mises, R. von 1927 Z. angew. Math. Mech. 7, 425.
Pai, S. I. 1954 Fluid Dynamics of Jets. New York: Van Nostrand.
Saffman, P. G. 1960 J. Fluid Mech. 7, 194.
Schlichting, H. 1933 Z. angew. Math. Mech. 13, 260.
Schlichting, H. 1960 Boundary Layer Theory, 4th ed. New York: McGraw-Hill.
Segedin, C. M. & Miller, J. B. 1962 N. Z. J. Sci. 5, 43.
Studt, F. E. & Modriniak, N. 1959 N. Z. J. Geol. Geophys. 2, 654.
Taylor, Sir Geoffrey & Saffman, P. G. 1959 Quart. J. Mech. Appl. Math. 12, 265.
Thompson, G. E. K., Banwell, C. J., Dawson, G. B. & Dickinson, D. J. 1961 U. N. Conference on New Sources of Energy, Paper no. E/CONF. 35/G/54.
Turner, J. S. 1962 J. Fluid Mech. 13, 356.
Wooding, R. A. 1957 J. Fluid Mech. 2, 273.
Wooding, R. A. 1960 J. Fluid Mech. 7, 501.
Yih, C.-S. 1961 J. Fluid Mech. 10, 133.