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Kinetic energy of Rayleigh--Taylor and Richtmyer--Meshkov instabilities

Journal Article · · Physics of Fluids A; (United States)
DOI:https://doi.org/10.1063/1.858151· OSTI ID:5232970
 [1]
  1. University of California, Lawrence Livermore National Laboratory, Livermore, California (USA)

General expressions for the kinetic energy associated with Rayleigh--Taylor (RT) and Richtmyer--Meshkov (RM) instabilities in incompressible fluids are derived. The results are valid for small perturbations in continuous as well as discontinuous density profiles. It was found that KE{sup RT} /KE{sup RM}={ital ge}{sup 2{gamma}{tau}} /({Delta}{ital v}{Gamma}){sup 2}=({ital ge}{sup {gamma}{tau}}/{Delta}{ital v}{gamma}){sup 2}, where {tau}=time, {ital g}=acceleration, {Delta}{ital v}=velocity jump, and {gamma} is the exponential growth rate of the RT amplitude. The linear growth rate of the RM amplitude is {Delta}{ital v}{Gamma}{sup 2}={Delta}{ital v}{gamma}{sup 2}/{ital g}, and is found by solving an eigenvalue equation for a given density profile subject to appropriate boundary conditions. In general, KE{sup RT} asymptotes to a constant value at large {ital k} ({ital k}=2{pi}/{lambda}, {lambda}=wavelength), while KE{sup RM} continues to grow with {ital k}. Several analytic examples are illustrated and the {ital k} dependence of the kinetic energies is displayed.

DOE Contract Number:
W-7405-ENG-48
OSTI ID:
5232970
Journal Information:
Physics of Fluids A; (United States), Journal Name: Physics of Fluids A; (United States) Vol. 3:11; ISSN 0899-8213; ISSN PFADE
Country of Publication:
United States
Language:
English