Dependence of Plasma Focus Argon Soft X-Ray Yield on Storage Energy, Total and Pinch Currents

2011 ◽  
Vol 31 (2) ◽  
pp. 143-150 ◽  
Author(s):  
M. Akel ◽  
S. Lee
Keyword(s):  
X Ray ◽  
Author(s):  
Vichai PURIPUNYAVANICH ◽  
Arlee TAMMAN ◽  
Piyanuch ORPONG ◽  
Roppon PICHA ◽  
Mayuree LIMTIYAYOTHIN ◽  
...  

Thailand Plasma Focus 2 (TPF-2) is operated at 2.16 kJ of storage energy with argon as a filled gas and can emit sharp x-ray pulses to plant cells in nanosecond (10-9 s) duration. The effects of plasma focus x-ray on seed germination and seedling growth of 14 Thai rice varieties treated under 10 conditions; 0 (control), 2, 4, 6, 8, 10, 12, 14, 16, and 18 plasma focus shots, were investigated. The results show that the germination rates and growth reduction rates were significantly different among the rice varieties. The germination rate of 10 varieties (Jek Chuey, KDML105, LPT123, PTT1, RD41, RD47, RD49, RD67, RD79, and SPR2) decreased when treated with a high number of plasma focus shots. LD50 and GR50 values were calculated, except for KTH17, RD1, RD7, and RD31 whose germination only slightly decreased, or remained constant, even after they were treated by 18 plasma focus shots. HIGHLIGHTS Effects of plasma focus irradiation on germination and growth were assessed on 14 Thai rice varieties  Shoot and root lengths of rice seedlings were measured 10 days after of plasma treatment Plasma focus was operated at 12 kV and the number of plasma focus shots was varied from 0 (control) to 18 shots Sensitivity to plasma irradiation was found to differ among rice seeds tested GRAPHICAL ABSTRACT


1999 ◽  
Vol 6 (12) ◽  
pp. 4679-4684 ◽  
Author(s):  
Takeshi Yanagidaira ◽  
Katsuji Shimoda ◽  
Yasushi Ono ◽  
Katsumi Hirano
Keyword(s):  
X Ray ◽  

2005 ◽  
Vol 14 (1) ◽  
pp. 61-69 ◽  
Author(s):  
S Hussain ◽  
M Shafiq ◽  
R Ahmad ◽  
A Waheed ◽  
M Zakaullah
Keyword(s):  

1974 ◽  
Vol 25 (10) ◽  
pp. 547-549 ◽  
Author(s):  
K. H. Schönbach ◽  
L. Michel ◽  
Heinz Fischer

2015 ◽  
Vol 653 ◽  
pp. 012023
Author(s):  
A K Dulatov ◽  
B D Lemeshko ◽  
Yu V Mikhailov ◽  
I A Prokuratov ◽  
A N Selifanov

2000 ◽  
Vol 14 (15) ◽  
pp. 563-570 ◽  
Author(s):  
M. ZAKAULLAH ◽  
IJAZ AKHTAR ◽  
S. F. MEHMOOD ◽  
A. WAHEED ◽  
G. MURTAZA

A time-resolved rugged X-ray detector (XRD) which may be used in intense radiation environment is developed. The detector is used to study the X-ray emission from a low-energy (2.3 kJ) Mather-type plasma focus energized by a 32 μF single capacitor, using hydrogen and argon (3:2) mixture as gas filling. In the detector, the electron emitter is made of nickel and aluminum. The sensitivity of the detector with nickel cathode is found to be very low. No signal could be recorded by masking the detector with even the 2 μm thick Al foil. When Al cathode is used in the XRD, the sensitivity of the detector increases abruptly. To stop the optical/ultraviolet radiation from approaching the active area, it is masked with 6 μm Al filter. It is found that an XRD with nickel cathode is not useful for X-ray detection in a low-energy plasma focus. However, due to its excellent response to vacuum ultraviolet radiation (≤600 Å), it may find application in the study of the axial rundown of current sheath, and its velocity. The X-ray emission from focus plasma is the highest at 0.5 mbar. With increase in pressure, the emission is dropped. At filling pressures of 2.0–2.5 mbar, the X-ray emission increases again. High X-ray emission at 0.5 mbar is due to interaction of energetic electrons in the current sheath with the anode surface, whereas moderately high emission at 2.0–2.5 mbar is caused by an axially moving shockwave.


1998 ◽  
Vol 67 (2) ◽  
pp. 481-486 ◽  
Author(s):  
Hiroyuki Kitaoka ◽  
Toshikazu Yamamoto ◽  
Katsumi Hirano

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