Numerical investigation on the stabilization of the deceleration phase Rayleigh-Taylor instability due to alpha particle heating in ignition target

2012 ◽  
Vol 99 (6) ◽  
pp. 65003 ◽  
Author(s):  
Zhengfeng Fan ◽  
Shaoping Zhu ◽  
Wenbing Pei ◽  
Wenhua Ye ◽  
Meng Li ◽  
...  
1994 ◽  
Vol 12 (2) ◽  
pp. 163-183 ◽  
Author(s):  
R.P.J. Town ◽  
B.J. Jones ◽  
J.D. Findlay ◽  
A.R. Bell

The growth of the Rayleigh-Taylor instability in three dimensions is ex amined during the deceleration phase of an inertial confinement fusion implosion. A detailed discussion of the three-dimensional hydrocode, PLATO, is presented. A review of previous calculations is given, concentrating on theshape of the R-T instability in three dimensions. Results of the growth rate during the linear phase, the saturation amplitude, and the nonlinear evolution are presented.


2015 ◽  
Vol 22 (7) ◽  
pp. 072702 ◽  
Author(s):  
A. Bose ◽  
K. M. Woo ◽  
R. Nora ◽  
R. Betti

2020 ◽  
Vol 142 (12) ◽  
Author(s):  
Denis Aslangil ◽  
Zachary Farley ◽  
Andrew G. W. Lawrie ◽  
Arindam Banerjee

Abstract We present our findings from a numerical investigation of the acceleration-driven Rayleigh–Taylor Instability, modulated by varying periods without an applied acceleration field. It is well known from studies on shock-driven Richtmyer–Meshkov instability that mixing without external forcing grows with a scaling exponent as ≈t0.20−0.28. When the Rayleigh–Taylor Instability is subjected to varying periods of “zero” acceleration, the structural changes to the mixing layer remain remarkably small. After the acceleration is re-applied, the mixing layer quickly resumes the profile of development it would have had if there had been no intermission. This behavior contrasts in particular with the strong sensitivity that is found to other variable acceleration profiles examined previously in the literature.


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