scholarly journals Effect of the gas blanket on the stability of the dense z-pinch

1979 ◽  
Author(s):  
B.R. Suydam
Keyword(s):  
1984 ◽  
Vol 27 (12) ◽  
pp. 2886 ◽  
Author(s):  
M. Coppins ◽  
D. J. Bond ◽  
M. G. Haines
Keyword(s):  

Author(s):  
S.T. Zalesak ◽  
A.L. Velikovich ◽  
J.L. Giuliani ◽  
Andrey Beresnyak
Keyword(s):  

1989 ◽  
Author(s):  
A. H. Glasser ◽  
R. A. Nebel
Keyword(s):  

1987 ◽  
Vol 38 (3) ◽  
pp. 495-499 ◽  
Author(s):  
M. Faghihi ◽  
J. Scheffel

The double adiabatic equations are used to study the stability of a cylindrical Z-pinch with respect to small axial wavelength, internal kink (m ≥ 1) modes. It is found that marginally (ideally) unstable, isotropic equilibria are stabilized. Also, constant-current-density equilibria can be stabilized for P⊥ > P∥ and large β⊥


1983 ◽  
Vol 30 (1) ◽  
pp. 169-178 ◽  
Author(s):  
Ulrich Schaper

A dispersion relation is derived for axisymmetric perturbations of an infinitely extended circular incompressible Z pinch with a step-like volume current profile. This profile is characterized by constant but different volume currents in different regions of the plasma and at the step surface there is a sheet current. The stability boundaries are shifted compared with stability limits in ideal MHD theory. For equilibria with no current reversal there is a new stable range whereas for equilibria with current reversal there is a new unstable range. The number of solutions of the dispersion relation depends on the equilibrium. The behaviour of the eigenvalues near the stability boundaries is treated in accordance with bifurcation theory.


2006 ◽  
Vol 55 (5) ◽  
pp. 2333
Author(s):  
Zhang Yang ◽  
Ding Ning
Keyword(s):  

2014 ◽  
Vol 21 (5) ◽  
pp. 052701 ◽  
Author(s):  
A. G. Rousskikh ◽  
A. S. Zhigalin ◽  
V. I. Oreshkin ◽  
N. A. Labetskaya ◽  
S. A. Chaikovsky ◽  
...  

2018 ◽  
Vol 84 (2) ◽  
Author(s):  
Alexey Mishchenko ◽  
Gabriel G. Plunk ◽  
Per Helander

The electrostatic stability of electron–positron plasmas is investigated in the point-dipole and Z-pinch limits of dipole geometry. The kinetic dispersion relation for sub-bounce-frequency instabilities is derived and solved. For the zero-Debye-length case, the stability diagram is found to exhibit singular behaviour. However, when the Debye length is non-zero, a fluid mode appears, which resolves the observed singularity, and also demonstrates that both the temperature and density gradients can drive instability. It is concluded that a finite Debye length is necessary to determine the stability boundaries in parameter space. Landau damping is investigated at scales sufficiently smaller than the Debye length, where instability is absent.


1982 ◽  
Vol 99 ◽  
pp. 605-613
Author(s):  
P. S. Conti

Conti: One of the main conclusions of the Wolf-Rayet symposium in Buenos Aires was that Wolf-Rayet stars are evolutionary products of massive objects. Some questions:–Do hot helium-rich stars, that are not Wolf-Rayet stars, exist?–What about the stability of helium rich stars of large mass? We know a helium rich star of ∼40 MO. Has the stability something to do with the wind?–Ring nebulae and bubbles : this seems to be a much more common phenomenon than we thought of some years age.–What is the origin of the subtypes? This is important to find a possible matching of scenarios to subtypes.


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