Investigation of a spherical plasma focus concept as a neutron and bremsstrahlung radiation source

Author(s):  
Yasar Ay ◽  
Mohamed A. Abd Al-Halim ◽  
Mohamed Bourham
2020 ◽  
Vol 46 (10) ◽  
pp. 978-991
Author(s):  
S. F. Garanin ◽  
V. Yu. Dolinskii ◽  
N. G. Makeev ◽  
V. I. Mamyshev ◽  
V. V. Maslov

2015 ◽  
Vol 69 (9) ◽  
Author(s):  
Yasar Ay ◽  
Mohamed A. Abd Al-Halim ◽  
Mohamed A. Bourham

2019 ◽  
Vol 28 (11) ◽  
pp. 1950097 ◽  
Author(s):  
Yasar Ay

The developed spherical plasma focus model is used in this study to investigate the optimum neutron yield in terms of the gas pressure, cathode radius and external inductance. The optimum values for these parameters are found separately. Then, the charging voltage is varied from 25[Formula: see text]kV to 35[Formula: see text]kV with 1[Formula: see text]kV increment by using these separately found optimum values to see the rate of increase in neutron yield. While the used gas pressure range is 1–40[Formula: see text]Torr with 1[Formula: see text]Torr increment, cathode radius range is 11.5–17[Formula: see text]cm with 0.5[Formula: see text]cm increment. External inductance is varied from 10[Formula: see text]nH to 150[Formula: see text]nH with 5[Formula: see text]nH increment. The optimum values for gas pressure, cathode radius and external inductance are found to be 26[Formula: see text]Torr, 15[Formula: see text]cm and 75[Formula: see text]nH, respectively. Even though combining these separately found optimum values of pressure, cathode radius and external inductance does not necessarily form an optimized set of operational conditions for the SPF, they lead to a higher neutron yield in that while neutron yield with these separately found optimum values at 25[Formula: see text]kV charging voltage is [Formula: see text] (higher than the measured neutron yield of [Formula: see text] at 25[Formula: see text]kV), it increases to [Formula: see text], when charging voltage is increased to 35[Formula: see text]kV. Using these values shows that spherical plasma focus device can be used as a neutron source with high neutron yield (on the order of [Formula: see text]).


2015 ◽  
Vol 35 (2) ◽  
pp. 407-414 ◽  
Author(s):  
Yasar Ay ◽  
Mohamed A. Abd Al-Halim ◽  
Mohamed A. Bourham

1995 ◽  
Vol 2 (1) ◽  
pp. 325-331 ◽  
Author(s):  
W. Jiang ◽  
T. Sakagami ◽  
K. Masugata ◽  
K. Yatsui

1998 ◽  
Vol 16 (1) ◽  
pp. 177-183
Author(s):  
Kazuo Imanari ◽  
Takeru Bingo ◽  
Kozue Sasaki ◽  
Weihua Jiang ◽  
Katsumi Masugata ◽  
...  

Experiments and the associated simulations for the evaluation of the focusibility of spherical Plasma focus diode (SPFD) were carried out. To evaluate the ion beam focusibility, two types of time-integrated Rutherford scattering pinhole camera were used: angle-integrated and angle-resolved type. From the former method, the ion beam has been found to focus in a cylindrical area with 4.5mmφ × 6.0 mm. The ion density profile shows a peak at 2.5 mm downstream from the geometric focusing point. From the latter method, it is found that a large fraction of the ion beam is produced from the downstream region of the diode. In simulations, the influence of an initial ion thermal energy was evaluated on the ion beam focusibility. When the initial energy is 20 eV, the ion beam focused in a cylindrical area of 0.4 mmφ × 2.4 mm. The experimental focusing parameters seem to be much worse than those evaluated numerically presumably due to the aiming error of ion beam.


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