期刊文献+

回旋速调管双阳极磁控注入电子枪的设计与优化 被引量:6

Design of a double anode magnetron injection gun for gyroklystron amplifier
下载PDF
导出
摘要 根据8 mm回旋速调管放大器对双阳极磁控注入电子枪的要求,分析了电极形状、阳极电压、磁场、注电流对电子注横纵速度比和速度零散的影响,并进行了粒子模拟。分析表明:这些因素可归根为电场和磁场的作用,阴极附近高的电场有助于提高横纵速度比和降低速度零散;而高的磁场及低的磁压缩比将降低横纵速度比,但对速度零散影响无明显规律。在此基础上通过优化电极形状、磁场分布、电流、第一阳极电压和第二阳极电压,模拟并试制出工作电压65 kV、电流12 A、磁场1.4 T的双阳极电子枪,得到的横纵速度比值为1.4,横向速度零散为4.5%,为8 mm回旋速调管提供了稳定高质量的电子注。 According to demand of the double anode magnetron injection gun for gyroklystron amplifier, many factors influencing electron gun performance, such as electrode shape, magnetic distribution, beam current, first anode voltage, second anode voltage, were discussed, The results show that the transverse to longitudinal velocity ratio of beam increases and the trans-velocity spread decreases when the first anode voltage increases or magnetic induction at the cathode decreases, when the first anode obliquity reduces and cathode obliquity increases, the transverse to longitudinal velocity ratio of beam increases and the transvelocity spread will decrease. Quality of electron beam is improved by adjusting the distance between the cathode and the first anode and the first anode voltage properly. An electron gun with the transverse to longitudinal velocity ratio of beam 1.4 and the trans-velocity spread 4.5% was abtained by a great deal of simulation using Egun program when the working voltage was 65 kV and the working electric current was 12 A.
作者 蒲友雷 罗勇
出处 《强激光与粒子束》 EI CAS CSCD 北大核心 2007年第6期951-955,共5页 High Power Laser and Particle Beams
基金 国家863计划项目资助课题
关键词 高功率微波 回旋速调管放大器 磁控注入电子枪 横纵速度比 速度零散 High power microwave Gyroklystron amplifier Magnetron injection gun Transverse to longitudinal velocity ratio Velocity spread
  • 相关文献

参考文献6

二级参考文献54

  • 1王华军.回旋管磁控注入枪CAD:硕士论文[M].成都:电子科技大学,1996..
  • 2李家胤 王华军 等.三次谐波回旋管电子枪的设计[J].电子科技大学学报,1994,25(7):72-75.
  • 3Calame J P, Garven M, Choi J J, et al. Experimental studies of bandwidth and power production in a three-cavity, 35GHz gyroklystron amplifier[J]. Phys Plasma, 1999, 6(1) : 285-297.
  • 4Antokov I I, Zasypkin E V, Sokolov E V. 35GHz radar gyroklystron[A]. Proc of 18th Int Conf IR&MM Waves[C]. Colchester, UK,1993, 2104:338-339.
  • 5Blank M, Danly B G, Levush B, et al. Experiment investigation of W-band(93 GHz)gyroklystron amplifiers[J]. IEEE Trans Plasma Sci, 1998, 26(3): 409 415.
  • 6Gachev I G, Antakov I I, Lygin V K, et al. A Ka-band second-harmonic gyroklystron with permanent magnet[A]. Fifth International Workshop Strong Microwaves in Plasmas[C]. Russia, 2002.
  • 7Choi J J, McCurdy A H, Wood F N, et al. Experimental Investigation of a high power, two-cavity, 35GHz gyroklystron amplifier[J]. IEEE Trans Plasma Science, 1998, 26(3) : 416-425.
  • 8Garven M, Manheimer W M, Blank M. Simple theory of input couplers for gyroklystron amplifiers[J]. IEEETrans Plasma Sci , 1998, 26(3): 433 - 443.
  • 9McDonald N A. Electric and magnetic coupling through small apertures in shield walls of any thickness[J]. IEEE Trans Microwave Theoryand Techniques, 1972, 20(10) : 689 -695.
  • 10McCurdy A H, Choi J J. Design and analysis of a coaxial coupler for a 35 GHz gyroklystron amplifier[J]. IEEETrans Plasma Sci, 1999,47(2) : 164-175.

共引文献53

同被引文献51

引证文献6

二级引证文献15

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部