Hostname: page-component-cd9895bd7-lnqnp Total loading time: 0 Render date: 2024-12-19T13:05:57.615Z Has data issue: false hasContentIssue false

The Rayleigh–Taylor instability of a viscous liquid layer resting on a plane wall

Published online by Cambridge University Press:  26 April 2006

Lori A. Newhouse
Affiliation:
Department of Applied Mechanics and Engineering Sciences, R-011, University of California, San Diego, La Jolla, CA 92093, USA
C. Pozrikidis
Affiliation:
Department of Applied Mechanics and Engineering Sciences, R-011, University of California, San Diego, La Jolla, CA 92093, USA

Abstract

The nonlinear Rayleigh–Taylor instability of a liquid layer resting on a plane wall below a second liquid of higher density is considered. Under the assumption of creeping flow, the motion is studied as a function of surface tension and the ratio of the viscosities of the two fluids. The flow induced by the deformation of the layer is represented by an interfacial distribution of Green's functions. A Fredholm integral equation of the second kind is derived for the density of the distribution, and is solved by successive iteration. The results show that for small and moderate surface tension, the instability of the layer leads to the formation of a periodic array of viscous plumes which penetrate into the overlying fluid. The morphology of these plumes strongly depends upon the viscosity ratio and surface tension. When the viscosity of the overlying fluid is comparable with or larger than that of the layer, the plumes are composed of a well-defined leading drop on top of a narrow stem. When the viscosity of the overlying fluid is smaller than that of the layer, the plumes take the form of a compact column of rising fluid. The size of the drop leading a plume is roughly proportional to the initial thickness of the layer. When surface tension is sufficiently small, ambient fluid is entrained into the leading drop and circulates in a spiral pattern. Convection currents generated by the rising plumes are visualized with streamline patterns, and the rate of thinning of the remnant layer, as well as the speed of the rising drop or plumes, are discussed.

Type
Research Article
Copyright
© 1990 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

Babchin, A. J., Frenkel, A. L., Levich, B. G. & Sivashinsky, G. I. 1983 Nonlinear saturation of Rayleigh—Taylor instability in thin films. Phys. Fluids 26, 31593161.Google Scholar
Baker, G. R., McCrory, R. L., Verdon, C. P. & Orsag, S. A. 1987 Rayleigh—Taylor instability of fluid layers. J. Fluid Mech. 178, 161175.Google Scholar
Blake, J. R. 1971 A note on the image system for a stokeslet in a no-slip boundary. Proc. Camb. Phil. Soc. 70, 303310.Google Scholar
Chandrasekhar, S. 1961 Hydrodynamic and Hydromagnetic Stability. Dover.
Gardner, C. L., Glimm, J., McBryan, O., Menikoff, R., Sharp, D. H. & Zhang, Q. 1988 The dynamics of bubble growth for Rayleigh—Taylor unstable interfaces. Phys. Fluids 31, 447465.Google Scholar
Hooper, A. P. & Boyd, W. G. 1983 Shear-flow instability at the interface between two viscous fluids. J. Fluid Mech. 128, 507528.Google Scholar
Jacobs, J. W. & Catton, I. 1988a Three-dimensional Rayleigh—Taylor instability. Part 1. Weakly nonlinear theory. J. Fluid Mech. 187, 329352.Google Scholar
Jacobs, J. W. & Catton, I. 1988b Three-dimensional Rayleigh—Taylor instability. Part 2. Experiment. J. Fluid Mech. 187, 353371.Google Scholar
Jain, R. K. & Ruckenstein, E. 1976 Stability of stagnant films on a solid surface. J. Colloid Interface Sci. 54, 108116.Google Scholar
Kerr, R. 1988 Simulation of Rayleigh—Taylor flows using vortex blobs. J. Comput. Phys. 76, 4884.Google Scholar
Keunings, R. & Bousfield, D. W. 1987 Analysis of surface tension driven leveling in viscoelastic films. J. Non-Newtonian Fluid Mech. 22, 219233.Google Scholar
Ladyzhenskaya, O. A. 1969 The Mathematical Theory of Viscous Incompressible Flow. Gordon & Breach.
Lamb, H. 1932 Hydrodynamics, 6th edn. Cambridge University Press.
Menikoff, R., Mjolsness, R. C., Sharp, D. H. & Zemach, C. 1977 Unstable normal mode for Rayleigh—Taylor instability in viscous fluids. Phys. Fluids 20, 20002004.Google Scholar
Menikoff, R., Mjolsness, R. C., Sharp, D. H. & Zemach, C. 1978 Initial value problem for Rayleigh—Taylor instability of viscous fluids. Phys. Fluids 21, 16741687.Google Scholar
Olson, P. & Singer, H. 1985 Creeping plumes. J. Fluid Mech. 158, 511531.Google Scholar
Orchard, S. E. 1963 On surface levelling in viscous liquids and gels. Appl. Sci. Res. A11, 451.Google Scholar
Pozrikidis, C. 1987 Stokes flow in two-dimensional channels. J. Fluid Mech. 180, 495514.Google Scholar
Pozrikidis, C. 1990a The instability of a moving viscous drop. J. Fluid Mech. 210, 121.Google Scholar
Pozrikidis, C. 1990b The deformation of a viscous drop moving normal to a plane wall. J. Fluid Mech. 215, 331363.Google Scholar
Rayleigh, Lord 1900 Scientific Papers, vol. II. Cambridge University Press.
Sharp, D. H. 1984 An overview of Rayleigh—Taylor instability. Physica 12D, 318.Google Scholar
Tryggvason, G. 1988 Numerical simulations of the Rayleigh—Taylor instability. J. Comput. Phys. 75, 253282.Google Scholar
Verdon, C. P., McCrory, R. L., Morse, R. L., Baker, G. R., Meiron, D. I. & Orszag, S. A. 1982 Nonlinear effects of multifrequency hydrodynamic instabilities on ablatively accelerated thin cells. Phys. Fluids 25, 16531674.Google Scholar
Whitehead, J. A. 1988 Fluid models of geological hotspots. Ann. Rev. Fluid Mech. 20, 6187.Google Scholar
Yiantsios, S. G. & Higgins, B. G. 1989 Rayleigh—Taylor instability in thin viscous films. Phys. Fluids A 1, 14841501.Google Scholar
Zufiria, J. A. 1988 Bubble competition in Rayleigh—Taylor instability. Phys. Fluids. 31, 440446.Google Scholar