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Title: Simple model for mixing at accelerated fluid interfaces with shear and compression

Abstract

A simple model was recently described for predicting linear and nonlinear mixing at an unstable planar interface between two fluids of different density subjected to an arbitrary time-dependent variable acceleration history [J. D. Ramshaw, Phys. Rev. E 58, 5834 (1998)]. Here we generalize this model to include the Kelvin-Helmholtz (KH) instability resulting from a tangential velocity discontinuity {delta}u, as well as the effects of a uniform anisotropic compression or expansion of the mixing layer as a whole. The model consists of a second-order nonlinear ordinary differential equation of motion for the half-width h of the mixing layer. This equation is derived by combining the wavelength renormalization hypothesis used in the earlier model with a suitable expression for the rate of change of the kinetic energy of the mixing layer. The resulting generalized model contains no additional free parameters, and reduces to the previous model in the absence of tangential velocities and compression. It also reduces in the linear regime to the correct linearized stability equation for an accelerated shear layer with compression [J. D. Ramshaw, Phys. Rev. E 61, 1486 (2000)]. For a pure incompressible KH instability in the nonlinear regime, the model predicts that h={eta}|{delta}u|t, where {eta}=[{alpha}(2-{theta})/(sq root)({theta}(1-{theta}))]{radical}({rho}{sub 1}{rho}{submore » 2})/({rho}{sub 1}+{rho}{sub 2}), and {alpha} and {theta} are parameters appearing in the nonlinear Rayleigh-Taylor and Richtmyer-Meshkov growth laws. For equal densities and the same parameter values previously used to match variable-acceleration experimental data, we find {eta}=0.10, in close agreement with experimental data for free shear layers. (c) 2000 The American Physical Society.« less

Authors:
 [1]
  1. Lawrence Livermore National Laboratory, University of California, P. O. Box 808, L-097, Livermore, California 94551 (United States)
Publication Date:
OSTI Identifier:
20216391
Resource Type:
Journal Article
Journal Name:
Physical Review. E, Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics
Additional Journal Information:
Journal Volume: 61; Journal Issue: 5; Other Information: PBD: May 2000; Journal ID: ISSN 1063-651X
Country of Publication:
United States
Language:
English
Subject:
71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; MIXING; SHEAR; COMPRESSIBLE FLOW; ACCELERATION; RENORMALIZATION; HELMHOLTZ INSTABILITY; INSTABILITY GROWTH RATES; INTERFACES; THEORETICAL DATA

Citation Formats

Ramshaw, John D. Simple model for mixing at accelerated fluid interfaces with shear and compression. United States: N. p., 2000. Web. doi:10.1103/PhysRevE.61.5339.
Ramshaw, John D. Simple model for mixing at accelerated fluid interfaces with shear and compression. United States. doi:10.1103/PhysRevE.61.5339.
Ramshaw, John D. Mon . "Simple model for mixing at accelerated fluid interfaces with shear and compression". United States. doi:10.1103/PhysRevE.61.5339.
@article{osti_20216391,
title = {Simple model for mixing at accelerated fluid interfaces with shear and compression},
author = {Ramshaw, John D.},
abstractNote = {A simple model was recently described for predicting linear and nonlinear mixing at an unstable planar interface between two fluids of different density subjected to an arbitrary time-dependent variable acceleration history [J. D. Ramshaw, Phys. Rev. E 58, 5834 (1998)]. Here we generalize this model to include the Kelvin-Helmholtz (KH) instability resulting from a tangential velocity discontinuity {delta}u, as well as the effects of a uniform anisotropic compression or expansion of the mixing layer as a whole. The model consists of a second-order nonlinear ordinary differential equation of motion for the half-width h of the mixing layer. This equation is derived by combining the wavelength renormalization hypothesis used in the earlier model with a suitable expression for the rate of change of the kinetic energy of the mixing layer. The resulting generalized model contains no additional free parameters, and reduces to the previous model in the absence of tangential velocities and compression. It also reduces in the linear regime to the correct linearized stability equation for an accelerated shear layer with compression [J. D. Ramshaw, Phys. Rev. E 61, 1486 (2000)]. For a pure incompressible KH instability in the nonlinear regime, the model predicts that h={eta}|{delta}u|t, where {eta}=[{alpha}(2-{theta})/(sq root)({theta}(1-{theta}))]{radical}({rho}{sub 1}{rho}{sub 2})/({rho}{sub 1}+{rho}{sub 2}), and {alpha} and {theta} are parameters appearing in the nonlinear Rayleigh-Taylor and Richtmyer-Meshkov growth laws. For equal densities and the same parameter values previously used to match variable-acceleration experimental data, we find {eta}=0.10, in close agreement with experimental data for free shear layers. (c) 2000 The American Physical Society.},
doi = {10.1103/PhysRevE.61.5339},
journal = {Physical Review. E, Statistical Physics, Plasmas, Fluids, and Related Interdisciplinary Topics},
issn = {1063-651X},
number = 5,
volume = 61,
place = {United States},
year = {2000},
month = {5}
}