Ka波段分布作用速调管降压收集极设计

王柳亚; 丁海兵

doi:10.11884/HPLPB202032.200093

Ka波段分布作用速调管降压收集极设计

doi: 10.11884/HPLPB202032.200093

王柳亚^{1, 2,},
丁海兵^1, ,

1.
中国科学院空天信息创新研究院，高功率微波源与技术重点实验室，北京 100190
2.
中国科学院大学，北京 100190

详细信息

作者简介:
王柳亚（1996—），女，硕士研究生，从事高功率微波源技术研究；wangliuya9604@163.com

通讯作者:
丁海兵（1977—），男，博士，研究员，从事高功率微波真空电子器件及微波能应用系统的研究；dinghb@aircas.ac.cn

中图分类号: TN122
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- 被引次数: 3
出版历程
- 收稿日期: 2020-04-18
- 修回日期: 2020-06-14
- 刊出日期: 2020-08-13

Design of depressed collector for Ka-band extended interaction klystron

Wang Liuya^{1, 2
,},
Ding Haibing^{1
, ,}

1.
Aerospace Information Research Institute, Chinese Academy of Sciences, Beijing 100190, China
2.
University of Chinese Academy of Sciences, Beijing 100190, China

摘要

摘要: 为满足无线传能系统对高效率大功率毫米波功率源的迫切需求，开展大功率连续波速调管高效率技术研究，采用降压收集极技术实现速调管在效率上的有效提升。主要介绍了某Ka波段大功率连续波分布作用速调管（EIK）降压收集极的设计方案，包括注-波互作用后废电子能量分布及行为特性的研究，收集极初始条件、结构及电极电压的设计，给出了单级降压收集极和两级降压收集极的设计和计算结果。三维粒子模拟（PIC）计算结果表明，该Ka波段连续波EIK采用单级降压收集极时回收效率为41.0%，采用两级降压收集极时回收效率为68.8%，EIK总管效率相比于未采用降压收集极技术时的27.5%上升至54.8%，表明通过降压收集极技术可有效提升毫米波大功率速调管工作效率。
- 分布作用速调管 /
- 降压收集极 /
- Ka波段 /
- 效率 /
- 三维仿真
Abstract: To meet the needs of the wireless transfer system for the high-efficiency high-power millimeter wave power source, the high-efficiency technology research of high-power continuous wave klystron was carried out, and the efficiency of the klystron was effectively improved by using the depressed-collector technology. This paper mainly introduces the design scheme of the depressed collector of a Ka-band high-power CW extended interaction klystron (EIK), including the investigation of electron energy distribution and behavior characteristics, the setting of the initial condition, the structure and the setting of the electrode voltage of the collector, and the design and calculation results of a single-stage depressed collector and a two-stage depressed collector for this high-power EIK. The results of PIC show that the recovery efficiency of the EIK with single-stage and two-stage depressed collector are 41% and 68.8% respectively, the net power conversion efficiency of this EIK is raised from a base value of 27.5% to 54.8% by using a two-stage depressed collector, which shows that it is feasible to improve the efficiency of high-power klystron by adopting the depressed collector technology.
- extended interaction klystron /
- depressed collector /
- Ka-band /
- efficiency /
- 3D simulation

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图 1 总效率和电子效率、收集极效率的关系

Figure 1. Relationship between tube efficiency, electronic efficiency and collector efficiency

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图 2 4级降压收集极的回收功率示意图

Figure 2. Recovery power of the four-stage depressed collector

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图 3 废电子电流随时间周期性变化

Figure 3. Waste electron current changes periodically with time

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图 4 一个射频周期内携带不同能量的粒子数目统计图

Figure 4. Number of particles carrying different energy in one RF cycle

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图 5 一个射频周期内等间隔的8个时间点

Figure 5. Eight equal interval points in one RF cycle

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图 6 8等分时间点上携带不同能量的粒子数目统计图

Figure 6. Number of particles carrying different electron energy of point 1～8

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图 7 单级降压收集极的结构示意图

Figure 7. Structure of one-stage depressed collector

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图 8 未对收集极实施电压降时的电子轨迹

Figure 8. Electron beams trajectories in collector without voltage drop

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图 9 单级降压收集极电子轨迹

Figure 9. Electron beams trajectories in one-stage depressed collector

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图 10 初始两级降压收集极的结构示意图

Figure 10. Structure of initial two-stage depressed collector

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图 11 改进后的二级降压收集极的结构示意图

Figure 11. Structure of improved two-stage depressed collector

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图 12 两级降压收集极内的电子轨迹

Figure 12. Electron beams trajectories in two-stage depressed collector

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表 1 EIK的主要设计参数

Table 1. Main design parameters of the Ka-band extended interaction klystron(EIK)

frequency/GHz	beam voltage/kV	beam current/A	output power of CW/kW	efficiency/%	gain/dB
35	10	0.49	1.35	27.5	54

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表 2 部分废电子信息

Table 2. Information of part of waste electrons

x position/m	y position/m	z position/m	${u}_{x}$	${u}_{y}$	${u}_{z}$	mass/kg	charge/C	macro particle charge/C	time/s
−1.23E−04	−2.81E−05	4.10E−02	−1.28E−03	2.68E−03	0.164	9.10E−31	−1.60E−19	−2.22E−16	2.50E−08
−1.12E−04	−5.39E−05	4.10E−02	−1.83E−03	2.25E−03	0.164	9.10E−31	−1.60E−19	−2.17E−16	2.50E−08
−1.18E−04	−3.67E−05	4.10E−02	9.95E−04	−4.13E−03	0.165	9.10E−31	−1.60E−19	−2.66E−16	2.50E−08
−2.46E−05	−2.33E−04	4.10E−02	−7.46E−03	−9.42E−03	0.164	9.10E−31	−1.60E−19	−1.87E−16	2.50E−08
−9.48E−05	−9.30E−05	4.10E−02	3.41E−03	−2.00E−03	0.164	9.10E−31	−1.60E−19	−2.39E−16	2.50E−08
−9.44E−05	−9.35E−05	4.10E−02	3.37E−03	−2.01E−03	0.164	9.10E−31	−1.60E−19	−2.39E−16	2.50E−08

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表 3 单级降压收集极的设计参数

Table 3. Design parameters of the one-stage depressed collector

drift length/mm	drift entrance radius/mm	drift exit radius/mm	collector length/mm	collector entrance radius/mm	collector exit radius/mm
8	0.45	0.6	71.5	0.9	5

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表 4 单级降压收集极的回收效率、回流率与压降的关系

Table 4. Relationship between recovery efficiency, reflux rate and voltage drop of the one-stage depressed collector

voltage/kV	recovery efficiency/%	electron reflux rate/%
−3.0	26	0
−4.0	40	0
−4.1	41	0.02
−4.2	43	1.00
−4.3	44	1.05
−5.0	54	3.20
−6.0	68	4.60

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表 5 初始两级降压收集极的设计参数

Table 5. Design parameters of initial two-stage depressed collector

length/mm			entrance radius/mm			exit radius/mm
drift	one-stage collector	two-stage collector	drift	one-stage collector	two-stage collector	drift	one-stage collector	two-stage collector
8	31	40	0.35	0.9	3	0.6	5	5

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表 6 改进后的两级降压收集极设计参数

Table 6. Design parameters of improved two-stage depressed collector

length/mm			entrance radius/mm			exit radius/mm
drift	one-stage collector	two-stage collector	drift	one-stage collector	two-stage collector	drift	one-stage collector	two-stage collector
8	13.5	27.5	0.35	0.7	6	0.6	5	5

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表 7 优化的各级压降及回收效率

Table 7. Design parameters of improved two-stage depressed collector

voltage of the first stage/kV	voltage of the second stage/kV	recovery efficiency/%
−4.1	−10	68.8
−3.7	−9	49.2
−3.0	−8	53.6
−2.1	−7	38.7
−1.5	−6	43.1
−0.6	−5	37.3
−4.0	−4	40.0

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表 8 不同初始条件下的回收效率和整管效率

Table 8. Recovery efficiency and tube efficiency under different initial conditions

initial condition	recovery efficiency/%	tube efficiency/%
PID 1	72.4	57.8
PID 2	70.9	56.1
PID 3	64.5	51.6
PID 4	68.8	54.8
PID 5	67.9	54.1
PID 6	66.1	52.8
PID 7	71.3	56.9
PID 8	72.8	58.2

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