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Baltrusaitis, R. M.; Gittings, M. L.; Weaver, R. P.; Benjamin, R. F.; Budzinski, J. M.

Simulation of shock-generated instabilities. (English) Zbl 1027.76563

Phys. Fluids 8, No. 9, 2471-2483 (1996).

Cited in 12 Documents

MSC:

76E17 Interfacial stability and instability in hydrodynamic stability
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[1] Recent examples can be found in A. Burrows, J. Hayes, and B. A. Fryxell, ”On the nature of core-collapse supernova explosions,” Astrophys. J. 450, 830 (1995); ASJOAB0004-637X
[2] J. M. Stone, J. Xu, and L. G. Mundy, ”Formation of ’bullets’ by hydrodynamical instabilities in stellar outflows,” Nature (London) 377, 315 (1995).NATUAS0028-0836
[3] Early work in the importance of Raleigh–Taylor instabilities in ICF implosions: R. E. Kidder, ”Laser-driven compression of hollow shells: Power requirements and stability limitations,” Nucl. Fusion 16, 3 (1976).NUFUAU0029-5515
[4] G. I. Taylor, ”The instability of liquid surfaces when accelerated in a direction perpendicular to their planes. I,” Proc. Soc. London 201, 192 (1950). · Zbl 0038.12201 · doi:10.1098/rspa.1950.0052
[5] R. D. Richtmyer, ”Taylor instability in shock acceleration of compressible fluids,” Commun. Pre Appl. Math. 13, 297 (1960).CPMAMV0010-3640
[6] E. E. Meshkov, ”Instability of the interface of two gases accelerated by a shock wave,” Fluid Dyn. 4, 101 (1969).FLDYAH0015-4628
[7] Recent studies of these instabilities are documented in these workshop proceedings and others in the same series: P. F. Linden, D. L. Youngs, and S. B. Dalziel (editors), ”Proceedings of the 4th International Workshop on the Physics of Compressible Turbulent Mixing,” Cambridge, England (29 March–1 April 1993).
[8] J. W. Shaner, ”Pattern formation by shock processes,” Physica D 12, 154 (1984).PDNPDT0167-2789
[9] J. M. Budzinski, R. F. Benjamin, and J. W. Jacobs, ”Influence of initial conditions on the flow patterns of a shock-accelerated thin fluid layer,” Phys. Fluids 6, 3510 (1994).PHFLE61070-6631
[10] J. W. Jacobs, D. L. Klein, D. G. Jenkins, and R. F. Benjamin, ”Instability growth patterns of a shock-accelerated thin fluid layer,” Phys. Rev. Lett. 70, 583 (1993).PRLTAO0031-9007
[11] J. W. Jacobs, D. G. Jenkins, D. L. Klein, and R. F. Benjamin, ”Nonlinear growth of the shock-accelerated instability of a thin fluid layer,” J. Fluid Mech. 295, 23 (1995).JFLSA70022-1120
[12] K. A. Meyer and P. J. Blewett, ”Numerical investigation of the stability of a shock accelerated interface between two fluids,” Phys. Fluids 15, 753 (1972).PFLDAS0031-9171
[13] R. F. Benjamin, D. Besnard, and J. Haas, ”Shock and reshock of an unstable interface,” LANL Report LA-UR 92–1185, Los Alamos National Laboratory (1993).
[14] J. W. Grove, R. Holmes, D. H. Sharp, Y. Yang, and Q. Zhang, ”Quantitative theory of Richtmyer-Meshkov instability,” Phys. Rev. Lett. 71, 3473 (1993).PRLTAO0031-9007
[15] R. L. Holmes, J. W. Grove, and D. H. Sharp, ”Numerical investigation of Richtmyer–Meshkov instability using front tracking,” J. Fluid Mech. 301, 51 (1995).JFLSA70022-1120
[16] K. O. Mikaelian, ”Rayleigh-Taylor and Richtmyer-Meshkov instabilities in finite-thickness fluid layers,” Phys. Fluids 7, 888 (1995).PHFLE61070-6631
[17] M. L. Gittings, ”SAIC’s Adaptive grid Eulerian Hydrocode,” Defense Nuclear Agency Numerical Methods Symposium, 28–30 April 1992.
[18] N. Byrne, T. Betlach, and M. L. Gittings, ”RAGE: A 2D Adaptive Grid Eulerian Nonequilibrium Radiation Code,” Defense Nuclear Agency Numerical Methods Symposium, 28–30 April 1992.
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