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Stabilization of the Rayleigh--Taylor instability by convection in smooth density gradient: Wentzel--Kramers--Brillouin analysis

Journal Article · · Physics of Fluids B; (United States)
DOI:https://doi.org/10.1063/1.860357· OSTI ID:6995978
;  [1]
  1. Department of Technology, Uppsala University, Box 534, S-75 121, Uppsala (Sweden)
A self-consistent analytical model based on the Wentzel--Kramers--Brillouin (WKB) approximation is developed to investigate the suppression of the Rayleigh--Taylor (RT) instability by the combined effect of the convective mass flow and structured profiles both, in subsonic and supersonic flow regimes. The eigenvalue problem for the instability growth rates {sigma} is reduced to the problem of solving the system of algebraic equations. In static stratified plasma the eigenvalues spectrum {sigma}{sub {ital n}}({ital k}) ({ital n}=0,1,2,...) is found for any density profile. In the presence of steady-state mass flow the growth rate is obtained as an implicit function of the transverse wave number and as a functional of the unperturbed profiles. The cutoff wave number is expressed explicitly as the function of the unperturbed variables. Applicability of the WKB approach implies Fr={ital v}{sup 2}/{ital gL}{much lt}1 (Fr is the local Froude number, {ital L} is the stratification length scale), still it yields satisfactory agreement with numerical solutions of the boundary value problem for the RT growth rates in the ablatively accelerated plasma of larger targets with sharp density gradient (Fr{similar to}1).
OSTI ID:
6995978
Journal Information:
Physics of Fluids B; (United States), Journal Name: Physics of Fluids B; (United States) Vol. 4:11; ISSN 0899-8221; ISSN PFBPE
Country of Publication:
United States
Language:
English