Hostname: page-component-8448b6f56d-tj2md Total loading time: 0 Render date: 2024-04-24T02:01:06.484Z Has data issue: false hasContentIssue false

Bubble growth in porous media and Hele–Shaw cells

Published online by Cambridge University Press:  14 November 2011

S. D. Howison
Affiliation:
Department of Mathematical Sciences, Rensselaer Polytechnic Institute, Troy N.Y. 12181, U.S.A.

Synopsis

We consider the characterisation of a class of free boundary problems arising in the flow of a viscous liquid in a porous medium (or, in two dimensions, a Hele–Shaw cell). Injected air forms a bubble which grows as time increases; it is shown that three kinds of behaviour can occur. Firstly, the solution may cease to exist in finite time; secondly, the solution may exist for all time and the free boundary may have one or more limit points as t tends to infinity; and thirdly, the bubble may exist for all time and fill the whole space as t tends to infinity. Two-dimensional explicit examples arc given of all three types of behaviour, and it is proved that the only solutions of the third kind are those in which the bubble is always elliptical; the proof uses the theory of null quadrature domains. It is shown that solutions for ellipsoidal bubbles exist in three dimensions and it is conjectured that the only three-dimensional null quadrature domains with finite complement are those whose complement is an ellipsoid.

Type
Research Article
Copyright
Copyright © Royal Society of Edinburgh 1986

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

1Aitchison, J. and Howison, S. D.. Computation of Hele-Shaw flows with free boundaries. To appear in J. Comput. Phys. (1985).CrossRefGoogle Scholar
2DiBenedetto, E. and Friedman, A.. The ill-posed Hele-Shaw model and the Stefan problem for supercooled water. Trans. Amer. Math. Soc. 282 (1984), 183204.CrossRefGoogle Scholar
3Elliott, C. M. and Janovsky, V.. A variational inequality approach to the Hele-Shaw flow with a moving boundary. Proc. Roy. Soc. Edinburgh Sect. A 88 (1981), 93107.CrossRefGoogle Scholar
4Elliott, C. M. and Ockendon, J. R.. Weak and variational methods for moving boundary problems (London: Pitman, 1982).Google Scholar
5Galin, L. A.. Unsteady seepage with a free surface. Dokl. Akad. Nauk 47 (1945), 246249.Google Scholar
6Howison, S. D.. Cusp development in Hele-Shaw flow with a free surface. To appear in SIAM J. Appl. Math. (1986).CrossRefGoogle Scholar
7Jacquard, P. and Séguier, P.. Mouvement de deux fluides en contact dans un milieu poreux. J. de Mécanique 1 (1962), 367394.Google Scholar
8Lacey, A. A.. Moving boundary problems in the flow of liquid through porous media. J. Austral. Math. Soc. Ser. B 24 (1982), 171193.CrossRefGoogle Scholar
9Langer, J. S.. Instabilities and pattern formation in crystal growth. Rev. Modern Phys. 52 (1980), 128.CrossRefGoogle Scholar
10Meyer, G. H.. Hele-Shaw flow with a cusping free boundary. J. Comput. Phys. 44 (1981) 262276.CrossRefGoogle Scholar
11Paterson, L.. Radial fingering in a Hele-Shaw cell. J. Fluid Mech. 113 (1981), 513529.CrossRefGoogle Scholar
12Richardson, S.. Hele-Shaw flows with a free boundary produced by the injection of fluid into a narrow channel. J. Fluid Mech. 56 (1972), 609618.CrossRefGoogle Scholar
13Sakai, M.. Null quadrature domains. J. Analyse Math. 40 (1981), 144154.CrossRefGoogle Scholar
14Saffman, P. G.. Exact solutions for the growth of fingers from a fiat interface between two fluids in a porous medium or Hele-Shaw cell, Quart. J. Mech. Appl. Math. 12 (1959), 146150.CrossRefGoogle Scholar
15Saffman, P. G. and Taylor, G. I.. The penetration of a fluid into a porous medium or Hele-Shaw cell containing a more viscous liquid. Proc. Roy. Soc. London Ser. A 245 (1958), 743775.Google Scholar