Calculation and optimization of topology of a radial insulating magnetic field in an acceleration gap of a high-power ion diode with an induction plasma source; Laser and Particle Beams; Vol. 34, № 2

書目詳細資料
Parent link:Laser and Particle Beams
Vol. 34, № 2.— 2016.— [P. 352-355]
企業作者: Национальный исследовательский Томский политехнический университет Институт физики высоких технологий Лаборатория № 1
其他作者: Petrov A. V. Anatoly Viktorovich, Remnev (Remnyov) G. E. Gennady Efimovich, Pavlov S. K. Sergey Konstantinovich, Rumyantsev I. D. Iljya Dmitrievich
總結:Title screen
The paper presents the results of calculation and optimization of a structure of a radial insulating magnetic field in an acceleration gap of a high-power ion diode. A diode configuration with an induction plasma source and an anode configuration with azimuthally symmetrical slots and a pair of cathode coils of a magnetic diode system have been studied. When the size of the slots is ≤5 mm and codirectional magnetic fields of a diode and shock induction coil, the perturbation of the B-field does not exceed ≤20% and is located in the region near the anode. In this condition, the topology of the magnetic field В = f(1/r) is maintained in the acceleration gap. It was shown that the required radial distribution of the B-field can be optimized by varying the anode profile in the region opposite to two cathode coils of the diode magnetic system.
Режим доступа: по договору с организацией-держателем ресурса
語言:英语
出版: 2016
主題:
在線閱讀:http://dx.doi.org/10.1017/S0263034616000148
格式: 電子 Book Chapter
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=649379

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330 |a The paper presents the results of calculation and optimization of a structure of a radial insulating magnetic field in an acceleration gap of a high-power ion diode. A diode configuration with an induction plasma source and an anode configuration with azimuthally symmetrical slots and a pair of cathode coils of a magnetic diode system have been studied. When the size of the slots is ≤5 mm and codirectional magnetic fields of a diode and shock induction coil, the perturbation of the B-field does not exceed ≤20% and is located in the region near the anode. In this condition, the topology of the magnetic field В = f(1/r) is maintained in the acceleration gap. It was shown that the required radial distribution of the B-field can be optimized by varying the anode profile in the region opposite to two cathode coils of the diode magnetic system. 
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