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Vorticity generation by shock propagation through bubbles in a gas

Published online by Cambridge University Press:  21 April 2006

J. M. Picone
Affiliation:
Laboratory for Computational Physics, US Naval Research Laboratory, Washington, DC 20375, USA
J. P. Boris
Affiliation:
Laboratory for Computational Physics, US Naval Research Laboratory, Washington, DC 20375, USA

Abstract

We present a new theoretical model of ‘late-time’ phenomena related to the interaction of a planar shock with a local, discrete inhomogeneity in an ambient gas. The term ‘late-time’ applies to the evolution of the inhomogeneity and the flow field after interaction with the incident shock has ceased. Observations of a shock propagating through a bubble or a spherical flame have exhibited or implied the formation of vortex structures and have showed continual distortion of the bubble or flame. Our theory shows that this is due to the generation of long-lived vorticity at the edge of the discrete inhomogeneity. The vorticity interacts with itself through the medium of the fluid, and, depending on the geometry of the discrete inhomogeneity, can roll up into vortex filaments or vortex rings. To verify and amplify this theoretical description, we use numerical solutions of the fluid equations for conservation of mass, momentum, and energy to study the interaction of a weak shock with a cylindrical or spherical bubble. The simulated bubble has either a higher or lower density than the ambient gas. In this way, the calculations provide insights into the effects of both geometry and distortion of the local sound speed. The Mach number of the shock is 1.2, the ambient gas is air, and the pressure is 1 atmosphere. Because of the simple geometry of each bubble, the vorticity generated at the boundary rolls up into a vortex filament pair (cylindrical bubble) or a vortex ring (spherical bubble). The structural features and timescales of the phenomena observed in the calculations agree closely with recent experiments of Haas & Sturtevant, in which helium and Freon bubbles were used to provide the local departures from ambient density. The discussion of results includes a survey of alternative numerical methods, sources of uncertainty in velocities of interfaces or structures, as derived from the laboratory and numerical experiments, and the relationship of our analysis to other theories.

Type
Research Article
Copyright
© 1988 Cambridge University Press

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References

Batchelor, G. K. 1967 An Introduction to Fluid Dynamics. Cambridge University Press.
Book, D. L., Boris, J. P., Kuhl, A. L., Oran, E. S., Picone, J. M. & Zalesak, S. T. 1981 Simulaion of complex shock reflections from wedges in inert and reactive gas mixtures. In Proc. Seventh Int Conf. on Numerical Methods in Fluid Dynamics, pp. 8490.
Boris, J. P. 1976 Flux-corrected modules for solving generalized continuity equations. Naval Research Laboratory Memo. Rep. 3237.
Boris, J. P. & Book, D. L. 1976 Solution of continuity equations by the method of flux-corrected transport. Methods in Computational Physics, vol. 16, pp. 85129. Academic.
Chern, I-L., Glimm, J., McBryan, O., Plohr, B. & Yaniv, S. 1986 Front tracking for gas dynamics. J. Comp. Phys. 62, 83110.Google Scholar
Colella, P. & Woodward, P. R. 1984 The piecewise parabolic method (PPM) for gasdynamical simulations. J. Comp. Phys. 54, 174201.Google Scholar
Didden, N. 1979 On the formation of vortex rings: rolling-up and production of circulation. Z. Angew. Math. Phys. 30, 101116.Google Scholar
Emery, M. H., Gardner, J. H., Boris, J. P. & Cooper, A. L. 1984 Vortex shedding due to laser ablation. Phys. Fluids 27, 13381340.Google Scholar
Fritts, M. J. & Boris, J. P. 1979 The Lagrangian solution of transient problems in hydrodynamics using a triagular mesh. J. Comp. Phys. 31, 173215.Google Scholar
Fyfe, D. E., Gardner, J. H., Picone, J. M. & Fry, M. A. 1985 Fast three-dimensional flux-corrected transport code for highly resolved compressible flow calculations. In Proc. Ninth Intl Conf. on Numerical Methods in Fluid Dynamics. (ed. Soubbaramayer & J. P. Boujot), pp. 230234. Springer.
Fyfe, D. E., Oran, E. S. & Fritts, M. J. 1989 Surface tension and viscosity with Lagrangian hydrodynamics on a triangular mesh. J. Comp. Phys. (to be published).Google Scholar
Gottlieb, D. 1985 Spectral methods for compressible flow problems. In Proc. Ninth Intl Conf. on Numerical Methods in Fluid Dynamics (ed. Soubbaramayer & J. P. Boujot), pp. 4861. Springer.
Grinstein, F. F., Oran, E. S. & Boris, J. P. 1986 Numerical simulations of asymmetric mixing in planar shear flows. J. Fluid Mech. 165, 201220.Google Scholar
Haas, J.-F. L. 1983 Wave propagation and Rayleigh-Taylor instability in non-uniform gases. Bull. Am. Phys. Soc. 28, 1359.Google Scholar
Hass, J.-F. L. 1984 Interaction of weak shock waves and discrete gas inhomogeneities. Ph.D. thesis, California Institute of Technology.
Haas, J.-F. L. & Sturtevant, B. 1987 Interaction of weak shock waves with cylindrical and spherical gas inhomogeneities. J. Fluid Mech. 181, 4176.Google Scholar
Harten, A. 1983 High resolution schemes for hyperbolic conservation laws. J. Comp. Phys. 49, 357393.Google Scholar
Lamb, H. 1945 Hydrodynamics, p. 202. Dover.
Landau, L. D. & Lifshitz, E. M. 1959 Fluid Mechanics, pp. 360365. Pergamon.
Leonard, A. 1980 Vortex methods for flow simulation. J. Comp. Phys. 37, 289335.Google Scholar
Löhner, R. 1987 The efficient simulation of strongly unsteady flows by the finite element method. AIAA-87-055.
Löhner, R., Morgan, K., Peraire, J. & Vahdati, M. 1987 Finite element flux-corrected transport (FEM-FCT) for the Euler and Navier-Stokes equations. Intl. J. Num. Meth. Fluids 7, 10931109.Google Scholar
Löhner, R., Picone, M. & Boris, J. P. 1988 Wave structure produced by shock propagation through single and multiple gas inhomogeneities. In Proc. Sixteenth Intl Symp. on Shock Tubes and Waves. VCH Verlagsgesellschaft (to be published).
Markstein, G. H. 1957a A shock tube study of flame front-pressure wave interactions. In Sixth Symp. (Intl) on Combustion, pp. 387398. Reinhold.
Markstein, G. H. 1957b Flow disturbances induced near a slightly wavy contact surface, or flame front, traversed by a shock wave. J. Aero. Sci. 24, 238.Google Scholar
Maxworthy, T. 1977 Some experimental studies of vortex rings. J. Fluid Mech. 81, 465495.Google Scholar
Meshkov, Y. Y. 1970 Instability of a shock wave accelerated interface between two gases. NASA TT F-13, 074.
Oran, E. S., Young, T. R., Boris, J. P., Picone, J. M. & Edwards, D. H. 1983 A study of detonation structure: the formation of unreacted gas pockets. In Nineteenth Symp. (Intl) on Combustion, pp. 573582. The Combustion Institute.
Picone, J. M. & Boris, J. P. 1983 Vorticity generation by asymmetric energy deposition in a gaseous medium. Phys. Fluids 26, 365382.Google Scholar
Picone, J. M., Boris, J. P., Greig, J. R., Raleigh, M. & Fernsler, R. F. 1981 Convective cooling of lightning channels. J. Atmos. Sci. 38, 20562062.Google Scholar
Picone, J. M., Oran, E. S., Boris, J. P. & Young, T. R. 1985 Theory of vorticity generation by shock wave and flame interactions. In Dynamics of Shock Waves, Explosions, and Detonations, pp. 429448. American Institute of Aeronautics and Astronautics.
Richtmyer, R. D. 1960 Taylor instability in shock acceleration of compressible fluids. Commun. Pure Appl. Maths 23, 297319.Google Scholar
Richtmyer, R. D. & Morton, K. W. 1967 Difference Methods for Initial-Value Problems, pp. 288383. Wiley-Interscience.
Rudinger, G. 1958 Shock wave and flame interactions. In Combustion and Propulsion: Third AGARD Colloquium, pp. 153182. Pergamon.
Rudinger, G. & Somers, L. 1960 Behaviour of small regions of different gases carried in accelerated gas flows. J. Fluid Mech. 7, 161176.Google Scholar
Taylor, G. I. 1953 Formation of a vortex ring by giving an impulse to a circular disk and then dissolving it away. J. Appl. Phys. 24, 104.Google Scholar
Woodward, P. & Colella, P. 1984 The numerical simulation of two-dimensional fluid flow with strong shocks. J. Comp. Phys. 54, 115173.Google Scholar
Yee, H. C. 1987 Construction of explicit and implicit symmetric TVD schemes and their applications. J. Comp. Phys. 68, 151179.Google Scholar
Zalesak, S. T. 1979 Fully multidimensional flux-corrected transport algorithms for fluids. J. Comp. Phys. 31, 335362.Google Scholar