Synergistic mitigation of the Rayleigh–Taylor instability in Z-pinch implosions by sheared axial flow and finite Larmor radius effect

2003 ◽  
Vol 10 (7) ◽  
pp. 2956-2961 ◽  
Author(s):  
X. M. Qiu ◽  
L. Huang ◽  
G. D. Jian
Keyword(s):  
Axial Flow ◽  
Taylor Instability ◽  
Larmor Radius ◽  
Finite Larmor Radius ◽  
Rayleigh Taylor Instability ◽  
Z Pinch

Effects of compressibility on the finite Larmor radius stabilized Rayleigh–Taylor instability in Z-pinch implosions

2008 ◽  
Vol 15 (2) ◽  
pp. 022103 ◽  
Author(s):  
L. Huang ◽  
G. D. Jian ◽  
X. M. Qiu ◽  
X. D. Peng ◽  
S. Q. Wang
Keyword(s):  
Taylor Instability ◽  
Larmor Radius ◽  
Finite Larmor Radius ◽  
Rayleigh Taylor Instability ◽  
Z Pinch

Rayleigh-Taylor Instability of a Stratified Plasma

1974 ◽  
Vol 29 (3) ◽  
pp. 518-523 ◽  
Author(s):  
K. M. Srivastava
Keyword(s):  
Magnetic Field ◽  
Boussinesq Approximation ◽  
Short Wave ◽  
Taylor Instability ◽  
Larmor Radius ◽  
Finite Larmor Radius ◽  
Wave Disturbances ◽  
Magnetic Field Gradients ◽  
Rayleigh Taylor Instability ◽  
The Magnetic Field

We have investigated the effect of finite Larmor radius on the Rayleigh-Taylor instability of a semi-infinite, compressible, stratified and infinitely conducting plasma. The plasma is assumed to have a one dimensional density and magnetic field gradients. The eigenvalue problem has been solved under Boussinesq approximation for disturbances parallel to the magnetic field. It has been established that for perturbation parallel to the magnetic field, the system is stable for both stable and unstable stratification. For perturbation perpendicular to the magnetic field, the problem has been solved without Boussinesq approximation. The dispersion relation has been discussed in the two limiting cases, the short and long wave disturbances. It has been observed that the gyroviscosity has a destabilizing influence from k = 0 to k = 4.5 for ß* = 0.1 and for ß* = 0.1 up to k* = 2.85 and then onwards it acts as a stabilizing agent. It has a damping effect on the short wave disturbances. For some parameters, the largets imaginary part has been shown in Figs. 1 and 2

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