scholarly journals Self-Generated Plasma Rotation in a Z-Pinch Implosion with Preembedded Axial Magnetic Field

2022 ◽  
Vol 128 (1) ◽  
Author(s):  
M. Cvejić ◽  
D. Mikitchuk ◽  
E. Kroupp ◽  
R. Doron ◽  
P. Sharma ◽  
...  
2006 ◽  
Vol 99 (1) ◽  
pp. 013305 ◽  
Author(s):  
Sunao Katsuki ◽  
Akihiro Kimura ◽  
Yoshihiro Kondo ◽  
Hiroyuki Horita ◽  
Takao Namihira ◽  
...  

2003 ◽  
Vol 21 (2) ◽  
pp. 255-264 ◽  
Author(s):  
S.A. CHAIKOVSKY ◽  
A.Yu. LABETSKY ◽  
V.I. ORESHKIN ◽  
A.V. SHISHLOV ◽  
R.B. BAKSHT ◽  
...  

A double shell z-pinch with an axial magnetic field is considered as a K-shell plasma radiation source. One-dimensional radiation-hydrodynamics calculations performed suggest that this scheme holds promise for the production of the K-shell radiation of krypton (hν ≈ 12–17 keV). As a first step in verifying the advantages of this scheme, experiments have been performed to optimize a neon double-shell gas puff with an axial magnetic yield for the K-shell yield and power. The experiments show that the application of an axial magnetic field makes it possible to increase the K-shell radiation power and reduce the shot-to-shot spread in the K-shell yield. Comparisons between the experiments and modeling are made and show good agreement.


1994 ◽  
Vol 52 (3) ◽  
pp. 365-371 ◽  
Author(s):  
Arshad M. Mirza ◽  
N. A. D. Khattak ◽  
M. Iqbal ◽  
G. Murtaza

We investigate the implosion of a dense τ-pinch plasma driven by an annular finite-thickness gas-puff Z-pinch. The imploding Z-pinch traps an axial magnetic field Bz, compressing it to large values in an extremely short time. The temporal variation of Bz then induces an azimuthal τ current on the surface of a fibre placed on the axis, with a rise time an order of magnitude shorter than the rise time of the Z-pinch current. Our numerical results demonstrate that, for a thick gas-puff layer, maximum compression occurs before the current peaks.We also find that at peak compression, fuel densities of the order of 1025 cm-3 and temperatures above 10 keV can be achieved on a time scale of the order of 0.1 ns. Thus a Lawson parameter nτ ≈ 1014 s cm-3 for a DT fibre becomes achievable. The snowplough effect in the Z-pinch exercises a stabilization effect on the growth of sausage and Rayleigh—Taylor instabilities. In the limit of a very thin gas-puff layer, previous results are fully recovered.


2014 ◽  
Vol 21 (5) ◽  
pp. 056303 ◽  
Author(s):  
T. J. Awe ◽  
C. A. Jennings ◽  
R. D. McBride ◽  
M. E. Cuneo ◽  
D. C. Lamppa ◽  
...  

2017 ◽  
Vol 24 (6) ◽  
pp. 063519 ◽  
Author(s):  
A. G. Rousskikh ◽  
A. S. Zhigalin ◽  
V. I. Oreshkin ◽  
R. B. Baksht

2014 ◽  
Vol 42 (10) ◽  
pp. 2524-2525 ◽  
Author(s):  
Dimitry Mikitchuk ◽  
Christine Stollberg ◽  
Ramy Doron ◽  
Eyal Kroupp ◽  
Yitzhak Maron ◽  
...  

2019 ◽  
Vol 122 (4) ◽  
Author(s):  
D. Mikitchuk ◽  
M. Cvejić ◽  
R. Doron ◽  
E. Kroupp ◽  
C. Stollberg ◽  
...  

Author(s):  
Rina B. Baksht ◽  
Alexander G. Rousskikh ◽  
Alexander S. Zhigalin ◽  
Nataly A. Labetskaya ◽  
Stanislav A. Chaikovaskii ◽  
...  

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