Plasma formation in the wire array Z-pinch

Author(s):  
S.V. Lebedev ◽  
R. Aliaga-Rossel ◽  
I.H. Mitchell ◽  
J.P. Chittenden ◽  
A.E. Danger ◽  
...  
Keyword(s):  
The Wire ◽  
2001 ◽  
Author(s):  
P. Kubes ◽  
J. Kravarik ◽  
D. Klir ◽  
Yu. L. Bakshaev ◽  
P. I. Blinov ◽  
...  

2011 ◽  
Vol 29 (2) ◽  
pp. 155-160 ◽  
Author(s):  
J. Wu ◽  
L. Wang ◽  
A. Qiu ◽  
J. Han ◽  
M. Li ◽  
...  

AbstractExperiments of the return current post installed X-pinches were carried out on the 1-MA “QiangGuang-1” facility with the purpose of understanding X-pinch characteristics under this setup and establishing X-pinch backlighting diagnostics for the wire-array Z-pinches. Different wire-array loads along with the two-wire 30 µm Mo X-pinch backlighter were tested. The X-pinches emit the X-ray radiation with the burst time variation of ± 4 ns and the bright spot size of  ~30 µm. X-ray backlighting shadowgraphy images of the over-mass and radiation-suppressed Z-pinch wire array were obtained.


2008 ◽  
Vol 15 (5) ◽  
pp. 056301 ◽  
Author(s):  
Edmund P. Yu ◽  
M. E. Cuneo ◽  
M. P. Desjarlais ◽  
R. W. Lemke ◽  
D. B. Sinars ◽  
...  

1998 ◽  
Vol 26 (4) ◽  
pp. 1275-1281 ◽  
Author(s):  
M.G. Haines
Keyword(s):  
The Wire ◽  

1993 ◽  
Vol 11 (3) ◽  
pp. 587-593 ◽  
Author(s):  
R.B. Baksht ◽  
S.P. Bugaev ◽  
I.M. Datsko ◽  
A.A. Kim ◽  
B.M. Koval'chuk ◽  
...  

We report experiments that were carried out at the inductive storage machine GIT-4 with wire arrays. The tungsten wire array parameters were the following: the mass per centimeter was equal to 370 μg/cm, the length was 4 cm, and the initial radius was 0.2 cm. When the wire array current was 1.5 MA, the rise time was 100 ns and the total radiation energy was 50 kJ at the 80–100–kJ energy transferred to the wire array.


2001 ◽  
Vol 19 (3) ◽  
pp. 355-376 ◽  
Author(s):  
S.V. LEBEDEV ◽  
F.N. BEG ◽  
S.N. BLAND ◽  
J.P. CHITTENDEN ◽  
A.E. DANGOR ◽  
...  
Keyword(s):  

2007 ◽  
Vol 14 (2) ◽  
pp. 022705 ◽  
Author(s):  
Edmund P. Yu ◽  
B. V. Oliver ◽  
D. B. Sinars ◽  
T. A. Mehlhorn ◽  
M. E. Cuneo ◽  
...  

2014 ◽  
Vol 32 (3) ◽  
pp. 437-442 ◽  
Author(s):  
Shen Zhao ◽  
Xinlei Zhu ◽  
Ran Zhang ◽  
Haiyun Luo ◽  
Xiaobing Zou ◽  
...  

AbstractIn order to use two paralleled X-pinches as X-ray sources for the time-resolved backlighting of wire-array Z-pinch plasma, it is necessary to make these two X-pinches emit X-rays at different but roughly preset time instants. The timing of the X-ray burst from an X-pinch independence of the current, and the wire mass of the X-pinch was investigated. The currents flowing through two paralleled X-pinches were measured and it was found that the total current is almost equally divided between these two X-pinches no matter how different the wires for these two X-pinches are. The reason for the equal current division between two paralleled X-pinches was given based on the inductance calculation of the X-pinch circuit.


Sign in / Sign up

Export Citation Format

Share Document