Interaction of a weak shock wave with a discontinuous heavy-gas cylinder

The interaction between a cylindrical inhomogeneity and a weak planar shock wave is investigated experimentally and numerically, and special attention is given to the wave patterns and vortex dynamics in this scenario. A soap-film technique is realized to generate a well-controlled discontinuous cylinder (SF6 surrounded by air) with no supports or wires in the shock-tube experiment. The symmetric evolving interfaces and few disturbance waves are observed in a high-speed schlieren photography. Numerical simulations are also carried out for a detailed analysis. The refracted shock wave inside the cylinder is perturbed by the diffracted shock waves and divided into three branches. When these shock branches collide, the shock focusing occurs. A nonlinear model is then proposed to elucidate effects of the wave patterns on the evolution of the cylinder. A distinct vortex pair is gradually developing during the shock-cylinder interaction. The numerical results show that a low pressure region appears at the vortex core. Subsequently, the ambient fluid is entrained into the vortices which are expanding at the same time. Based on the relation between the vortex motion and the circulation, several theoretical models of circulation in the literature are then checked by the experimental and numerical results. Most of these theoretical circulation models provide a reasonably good prediction of the vortex motion in the present configuration.

[1]  G. Rudinger,et al.  Behaviour of small regions of different gases carried in accelerated gas flows , 1960, Journal of Fluid Mechanics.

[2]  G. Jourdan,et al.  An attempt to reduce the membrane effects in Richtmyer–Meshkov instability shock tube experiments , 2009 .

[3]  M. Brouillette THE RICHTMYER-MESHKOV INSTABILITY , 2002 .

[4]  R. D. Richtmyer Taylor instability in shock acceleration of compressible fluids , 1960 .

[5]  Oleg Schilling,et al.  High-resolution simulations and modeling of reshocked single-mode Richtmyer-Meshkov instability: Comparison to experimental data and to amplitude growth model predictions , 2006 .

[6]  Ravi Samtaney,et al.  Circulation deposition on shock-accelerated planar and curved density-stratified interfaces: models and scaling laws , 1994, Journal of Fluid Mechanics.

[7]  Todd F. Dupont,et al.  Three-dimensional effects in shock-cylinder interactions , 2008 .

[8]  J. Jacobs,et al.  The dynamics of shock accelerated light and heavy gas cylinders , 1993 .

[9]  G. Jourdan,et al.  Investigation of the Richtmyer-Meshkov instability with stereolithographed interfaces. , 2008, Physical review letters.

[10]  Christopher David Tomkins,et al.  Stretching of material lines in shock-accelerated gaseous flows , 2005 .

[11]  Joseph K. Conroy,et al.  Vortex formation in a shock-accelerated gas induced by particle seeding. , 2011, Physical review letters.

[12]  J. P. Boris,et al.  Vorticity generation by shock propagation through bubbles in a gas , 1988, Journal of Fluid Mechanics.

[13]  Oleg Schilling,et al.  Physics of reshock and mixing in single-mode Richtmyer-Meshkov instability. , 2006, Physical review. E, Statistical, nonlinear, and soft matter physics.

[14]  Mark H. Anderson,et al.  A computational parameter study for the three-dimensional shock–bubble interaction , 2007, Journal of Fluid Mechanics.

[15]  S. Balasubramanian,et al.  Turbulent mixing in a Richtmyer–Meshkov fluid layer after reshock: velocity and density statistics , 2012, Journal of Fluid Mechanics.

[16]  Edward E. Zukoski,et al.  Applications of Shock-Induced Mixing to Supersonic Combustion , 1993 .

[17]  Norman J. Zabusky,et al.  Vortex-accelerated secondary baroclinic vorticity deposition and late-intermediate time dynamics of a two-dimensional Richtmyer–Meshkov interface , 2003 .

[18]  Santhosh K. Shankar,et al.  Two-dimensional viscous flow simulation of a shock accelerated heavy gas cylinder , 2011 .

[19]  S. Balasubramanian,et al.  Experimental study of initial condition dependence on Richtmyer-Meshkov instability in the presence of reshock , 2012 .

[20]  Kathy Prestridge,et al.  An experimental investigation of mixing mechanisms in shock-accelerated flow , 2008, Journal of Fluid Mechanics.

[21]  G. Weirs,et al.  Validating the Flash Code: Vortex-Dominated Flows , 2004, astro-ph/0405410.

[22]  T. Si,et al.  Generation of polygonal gas interfaces by soap film for Richtmyer–Meshkov instability study , 2012 .

[23]  T. Si,et al.  On the interaction of a planar shock with a light polygonal interface , 2014, Journal of Fluid Mechanics.

[24]  Norman J. Zabusky,et al.  VORTEX PARADIGM FOR ACCELERATED INHOMOGENEOUS FLOWS: Visiometrics for the Rayleigh-Taylor and Richtmyer-Meshkov Environments , 1999 .

[25]  J. Jacobs,et al.  Shock-induced mixing of a light-gas cylinder , 1992, Journal of Fluid Mechanics.

[26]  J. Jacobs,et al.  PLIF flow visualization and measurements of the Richtmyer–Meshkov instability of an air/SF6 interface , 2002, Journal of Fluid Mechanics.

[27]  David Arnett The Role of Mixing in Astrophysics , 2000 .

[28]  J. Haas,et al.  Interaction of weak shock waves with cylindrical and spherical gas inhomogeneities , 1987, Journal of Fluid Mechanics.

[29]  Ting Si,et al.  On the evolution of spherical gas interfaces accelerated by a planar shock wave , 2011 .

[30]  Kazuyoshi Takayama,et al.  Conservative Smoothing on an Adaptive Quadrilateral Grid , 1999 .

[31]  Edward E. Zukoski,et al.  A model for characterization of a vortex pair formed by shock passage over a light-gas inhomogeneity , 1994, Journal of Fluid Mechanics.

[32]  E. Meshkov Instability of the interface of two gases accelerated by a shock wave , 1969 .

[33]  John Lindl,et al.  Review of the National Ignition Campaign 2009-2012 , 2014 .

[34]  R. Bonazza,et al.  Shock-Bubble Interactions , 2011 .

[35]  James J. Quirk,et al.  On the dynamics of a shock–bubble interaction , 1994, Journal of Fluid Mechanics.