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العنوان
Dynamics of a Pulsed Plasma Gas discharge /
المؤلف
Abdul Fattah, Tarek Ahmed.
الموضوع
Plasma Physics. Mathematics. Physics.
تاريخ النشر
2004.
عدد الصفحات
xii, 131 P. :
الفهرس
Only 14 pages are availabe for public view

from 150

from 150

Abstract

The linear Z pinch discharge occurred in a cylinderical Pyrex glass vessel of 11.0 cm diameter and 25.0 cm long, between the two end aluminum electrodes. The vessel is evacuated using the a rotary pump to a base pressure of 20 mTorr, the working gas is argon and is introduced by a
needle valve to a pressure of 10 mTorr. The electric circuit is composed of
four capacitors of 7. 71 ~F, 1.25 kJ each. They are arranged in a parallel
combination to give a total capacitance of30.84 ~F. We use a power supply of
45 kV to charge the capacitor bank, the discharge occurs through a pressurized
spark gap externally triggered by a high voltage trigger signal of 14 kV. The
plasma is stablized, by an an external return current of six copper cables
distributed along the discharge vessel and are fed with the discharge current.
The total discharge current is 28.5 KA with a periodic time of 28 us. The
electrical parameters of the system is, 91 m n total system resistance and 644
oH total system inductance.
Many diagnostic techniques are used such as; Rogowski coil, capacitive
coupling potential divider, magnetic probe and spectroscopy by using relative
continuum intensity radiation method. A special design of capacitive coupling
potential divider is used which consists of two parallel thin plates with area 41cm2 and are separated by an insulating sheet ofpolysteren of thickness 2mm and it forms a capacitor of 46 pF. One plate is connected to the high voltage electrode, and the other is connected the 160 nF capacitor with shunt resistor 500 n and the output is taken on it. The spectroscopic diagnostic is mainly a photomultiplier which collects light through a colored filter, for perturbation reason the light from the discharge is fed to the photomultiplier through a light
guide .. The electron temperature is calculated from the measurements of the
intensity of continuum radiation at two different wavelengths A1 and A2 .