Large-eddy simulations of Richtmyer–Meshkov instability in a converging geometry
- Creators
- Lombardini, M.
- Deiterding, R.
Abstract
The Richtmyer–Meshkov instability RMI refers to the baroclinic generation of vorticity at a perturbed density interface when impacted by a shock wave. It is often thought of as the impulsive limit of the Rayleigh–Taylor instability. While the RMI has been widely covered in planar geometries see, for example, Ref. 1, the present simulations investigate the mixing of materials resulting from the interaction of an imploding cylindrical shock wave with a concentric interface, perturbed in both axial and azimuthal directions, which separates outside air from SF_6 initially 5 times denser confined in a 90° wedge. Two incident shocks of Mach numbers M_i=1.3 and 2.0 at initial impact are tested. These canonical simulations support recent work on understanding the compressible turbulent mixing in converging geometries relevant to both inertial confinement fusion and core-collapse supernova dynamics.
Additional Information
© 2010 American Institute of Physics. Received 1 September 2010; published online 30 September 2010. This work was supported by the ASC Program under Subcontract No. B341492 of DoE Contract No. W-7405- ENG-48.Attached Files
Published - Lombardini2010p11695Phys_Fluids.pdf
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Additional details
- Eprint ID
- 20634
- Resolver ID
- CaltechAUTHORS:20101102-093531852
- W-7405- ENG-48
- Department of Energy (DOE)
- Created
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2010-11-03Created from EPrint's datestamp field
- Updated
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2021-11-09Created from EPrint's last_modified field