The Richtmyer-Meshkov mixing layer is initiated by the passing of a shock over an interface between fluid of differing densities. The energy deposited during the shock passage undergoes a relaxation process during which the fluctuational energy in the flow field decays and the spatial gradients of the flow field decrease in time. This late stage of Richtmyer-Meshkov mixing layers is studied from the viewpoint of self-similarity. Analogies with weakly anisotropic turbulence suggest that both the bubble-side and spike-side widths of the mixing layer should evolve as power-laws in time, with the same power-law exponent and virtual time origin for both sides. The analogy also bounds the power-law exponent between and . It is then shown that the assumption of identical power-law exponents for bubbles and spikes yields fits that are in good agreement with experiment at modest density ratios.
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Growth Rate Exponents of Richtmyer-Meshkov Mixing Layers
Timothy T. Clark,
Timothy T. Clark
Los Alamos National Laboratory
, Los Alamos, NM 87545
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Ye Zhou
Ye Zhou
Lawrence Livermore National Laboratory
, Livermore, CA 94551
Search for other works by this author on:
Timothy T. Clark
Los Alamos National Laboratory
, Los Alamos, NM 87545
Ye Zhou
Lawrence Livermore National Laboratory
, Livermore, CA 94551J. Appl. Mech. May 2006, 73(3): 461-468 (8 pages)
Published Online: November 6, 2005
Article history
Received:
July 29, 2004
Revised:
November 6, 2005
Citation
Clark, T. T., and Zhou, Y. (November 6, 2005). "Growth Rate Exponents of Richtmyer-Meshkov Mixing Layers." ASME. J. Appl. Mech. May 2006; 73(3): 461–468. https://doi.org/10.1115/1.2164510
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