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1.
设计了一个X波段相对论返波管,通过对器件结构的特殊设计,提高了器件的Q值,同时增大了电子束与慢波结构之间的耦合阻抗,从而实现器件的低磁场运行以便对其进行永磁包装;当引导磁场强度0.46 T、电子束束压750 kV、束流约5.5 kA时,得到频率9.1 GHz、功率1.24 GW的微波输出。根据模拟结果设计加工了一个磁场强度为0.46 T的小型化永磁磁体,该磁体长48 cm,最大外半径15 cm,总重量约116 kg。开展了永磁包装返波管的实验研究,得到以20 Hz的频率运行1 s时功率900 MW、单次运行时功率940 MW的X波段微波输出。  相似文献   

2.
 对基于短电子束脉冲超辐射机理的X波段相对论返波管进行了优化设计和粒子模拟,结果表明:在超辐射机理作用下,该器件能实现高峰值功率和高功率转换效率的微波辐射。在小型Tesla脉冲源基础上设计了阻抗变换段、二极管、磁场系统等装置,建立了一套小型窄脉冲电子加速器,以此为实验平台在低磁场条件下进行了器件的初步实验研究。在磁场0.73 T、束压约380 kV、束流约4.5 kA、脉宽3.1 ns条件下,实验获得的微波脉冲峰值功率约360 MW,脉宽1.10 ns,上升沿800 ps,频率9.15 GHz,功率转换效率为21%。  相似文献   

3.
运用超辐射机理,通过粒子模拟设计了X波段超辐射相对论返波管,并在小型Tesla脉冲源平台上开展了实验研究。通过空间功率积分和直接对辐射微波时域波形的分析得到实验结果:在束压350 kV、束流4.8 kA、脉宽3.1 ns、引导磁场2.2 T条件下,产生的微波辐射功率1.4 GW,中心频率9.36 GHz,脉宽500~700 ps,辐射模式为TE11,能在重复频率100 Hz下稳定运行。功率转换效率超过80%。实验结果与粒子模拟结果比较吻合,成功实现了在短脉冲条件下产生重复频率、亚纳秒脉宽、GW级微波辐射。  相似文献   

4.
Reported in this paper are the results of an experiment to produce high-power microwave radiation from a gas-filled backward wave oscillator (BWO) driven by a relativistic electron beam without external guiding magnetic field. A peak power for background gas pressure at 5.25 mTorr has been observed as argon pressure from 0.75 mTorr to 15 mTorr. Operating frequency of the oscillator has been measured at 9.6 ± 0.4 GHz. The results of PIC simulation are in good agreement with the experimental results. A reasonable explanation is given for experimental results by PIC simulation.  相似文献   

5.
介绍了一种重复频率脉冲磁场作为高功率微波源的导引磁场的设计,该磁场电源具有功耗低、发热量小、结构紧凑等优点,符合高功率微波朝重复频率方向发展的需求。从产生脉冲磁场的电流表达式出发,根据涡流损耗不能太大、品质因数要高和电容储能要小的原则,给出了脉冲磁场产生系统的储能电容和充电电压的优化设计方法。最后将此方法应用于Ka波段返波振荡器导引磁场的设计,确定出产生脉冲磁场电路的电容和充电电压的值,并进行了仿真和实验研究,结果与理论要求吻合较好,在重复频率10 Hz条件下能稳定运行,验证了设计的合理性。  相似文献   

6.
李正红  谢鸿全 《物理学报》2019,68(5):54103-054103
作为一个典型的高功率微波振荡器,过模返波管(backward wave oscillator,BWO)的束波互作用过程复杂,束流负载效应影响明显,但是作为振荡器本身,其本质就是一个正反馈电路,电子从阴极发射后,穿过谐振反射腔和慢波结构(slow-wave structure,SWS),在SWS区电子动能转化为微波能,其中的一部分微波反馈到谐振反射腔,实现对电子束的调制,其他微波通过后面输出端口向外辐射.本文根据这种正反馈机制,建立器件工作模式等效电路和束波互作用的自洽过程,从理论上给出正反馈机制对器件模式控制、起振电流等参数的影响,并模拟研究了这种反馈机制对模式控制的影响,由此设计了一个能够在(1 MV,20 kA)电子束条件下克服模式竞争的过模BWO,其微波输出功率为7.9 GW,频率为8.68 GHz,相应的效率为39.5%.  相似文献   

7.
为提高高功率微波(HPM)辐射天线的功率容量,设计了带均压环的HPM微波辐射天线窗。均压环嵌入介质窗表面后介质窗表面电场分布发生改变,电子运动轨迹也随之发生改变,改变电子运动轨迹能有效抑制二次电子倍增造成的介质窗击穿。当均压环与辐射场电场垂直时,CST模拟表明,均压环的加入基本不影响天线的辐射性能。将其应用于返波管振荡器(BWO)实验中(输出微波为TM01模),结果表明:在束压3 MV、束流10 kA、效率30%时,普通天线窗输出脉宽为45 ns,而加入均压环的天线窗输出脉宽100 ns。  相似文献   

8.
黄华  李士锋  孙利民  谭杰  王朋  刘振帮  向启帆 《强激光与粒子束》2022,34(11):113001-1-113001-7
为了实现高功率微波源低磁场及长时间稳定运行,开展了S波段GW级多注相对论速调管放大器(RKA)的理论模拟设计与实验研究。首先,采用一维大信号非线性理论软件优化设计了S波段4腔多注RKA,找到了器件工作的最佳参数:采用电压550 kV、束流4.7 kA的14注RKA,获得功率1.1 GW、效率43%的输出微波。随后,采用粒子模拟软件对理论设计的束波互作用参数进行了验证,获得了输出功率992 MW,器件效率为37%。最后,根据模拟参数开展了器件重频长时间运行实验研究。采用紧凑同轴Marx功率源驱动S波段四腔多注RKA,在电压530 kV、束流5.4 kA、重频20 Hz、运行时间1 s、引导磁场强度0.39 T、注入微波功率1.7 kW的条件下,获得了功率934 MW、脉宽69 ns的输出微波,束波转换效率33%。在器件重频20 Hz、运行时间10 min条件下,坚实了平均功率889 MW、平均脉宽42 ns的输出微波。该研究结果为S波段RKA的低磁场和长时间运行打下了的技术基础。  相似文献   

9.
For practicability of the high power microwave source,a C-band backward wave oscillator(BWO)which has high conversion efficiency is designed.When the axial guiding magnetic field is 0.83 T,the electron energy and the beam current of the diode are respectively 80 keV and 2.1 kA,a microwave output power of100 MW at 7.4 GHz microwave frequency with 65% conversion efficiency is achieved in simulation.  相似文献   

10.
The experimental results of an overmoded slow-wave high-power microwave generator operated at low magnetic field are presented. The feasibility of low magnetic field operation is investigated both theoretically and experimentally based on the characteristics of the overmoded slow-wave device. The experiments were carried out at the Spark-2 accelerator. Under the condition of guiding magnetic field strength of 0.55 T, diode voltage of 4 74 k V,and beam current of 5.2kA, a microwave was generated with power of 510 MW, mode of TM01, and frequency of 9.54 GHz. The relative half-width of the frequency spectrum is less than 1%, and the beam-to-microwave efficiency is about 21% in our experiments.  相似文献   

11.
The PASOTRONTM is a unique, high-power microwave source that uses a long-pulse (⩽100 μs) plasma-cathode electron-gun and plasma-filled slow-wave structure (SWS) to produce high-energy microwave pulses. The device utilizes no externally-produced magnetic fields; relying on a beam-generated plasma channel in the SWS to transport the beam. Peak powers of up to 5 MW were previously reported in C-band using a rippled-wall waveguide SWS. Scaling experiments indicated that increasing the beam voltage above the 90 kV C-band operation produces significantly higher peak powers. We report results from an L-band PASOTRONTM BWO designed to operate at 200 kV. The plasma-cathode E-gun built for this device generated beams with voltages of up to 225 kV and currents in excess of 1 kA for pulse lengths of up to 200 μs. The L-band PASOTRONTM BWO produced 10-20 MW of peak power in the TM01 mode, which was converted in the output to a TE11 mode with fixed polarization. The PASOTRON TM also directly produced TE-mode radiation in the 5-10 MW power range with a rotating output polarization, the rate of which can be controlled externally. The peak power and poise width was limited by the stability of the plasma channel at high peak powers and excessive plasma generation in the SWS during the long pulse length  相似文献   

12.
ARTI HADAP  K C MITTAL 《Pramana》2013,80(2):277-282
Transport of high current (~kA range with particle energy ~1 MeV) planar electron beams is a topic of increasing interest for applications in high-power (1–10 GW) and high-frequency (10–20 GHz) microwave devices such as backward wave oscillator (BWO), klystrons, gyro-BWOs, etc. In this paper, we give a simulated result for transport of electron beams with velocity $V_{\rm b} = 5.23 \times 10^{8}$  cm s???1, relativistic factor γ?=?1.16, and beam voltage = ~80 kV in notched wiggler magnet array. The calculation includes self-consistent effects of beam-generated fields. Our results show that the notched wiggler configuration with ~6.97 kG magnetic field strength can provide vertical and horizontal confinements for a sheet electron beam with 0.3 cm thickness and 2 cm width. The feasibility calculation addresses to a system expected to drive for 13–20 GHz BWO with rippled waveguide parameters as width w?=?3.0 cm, thickness t?=?1.0 cm, corrugation depth h?=?0.225 cm, and spatial periodicity d?=?1.67 cm.  相似文献   

13.
设计了一个过模太赫兹返波管振荡器,通过对慢波结构的精心设计,使电子束动能得到充分提取,实现器件的大功率及高效率运行。在电子能量和束流分别为280keV和320A的条件下,当引导磁场强度为3T时,采用2.5维Particle in Cell(PIC)程序模拟得到频率为121.8GHz、功率为13MW的太赫兹波输出,器件的束波转换效率约为14.5%。  相似文献   

14.
陈凯柏  高敏  周晓东  岛新煜 《强激光与粒子束》2019,31(11):113003-1-113003-7
针对高功率微波对毫米波引信的前门耦合效应问题,利用电磁仿真软件对某型毫米波调频连续波引信模型进行辐照试验,并与引信前端限幅电路结合进行联合仿真。在此基础上,继续设计正交试验,对信号参数影响水平进行分析。通过仿真试验发现,在高功率微波信号频率和引信工作频率对准的情况下,辐照场强峰值为60 kV/m时,天线末端耦合电压最大可达188 V;当辐照场强峰值为40 kV/m时,改变辐照信号特征参数,发现长脉宽信号更容易导致限幅器的热击穿效应;信号上升时间会影响天线末端耦合电压波形复杂程度,当信号峰值、脉宽一定时,上升时间为5 ns的输入信号导致的尖峰泄漏电压约为5.94 V,而当上升时间为0.1 ns时,尖峰泄漏电压为18.4 V,并且限幅电路更快达到饱和状态;通过正交试验发现,信号上升时间对尖峰泄漏峰值电压的影响最大,信号峰值对其的影响次之。  相似文献   

15.
 为开发回旋超辐射在毫米波和亚毫米波超辐射高功率微波源中的优势,采用3维PIC粒子模拟对回旋超辐射的工作特性进行了分析,并在此基础上优化设计了器件结构及工作参数范围。模拟表明,微波峰值功率与电子束脉宽在一定范围内成平方关系,符合超辐射的典型特征。初步实验在210 kV, 250 A的电子束参数下获得了6 MW的微波峰值功率输出,工作频率37.2 GHz,模式为TE01,与粒子模拟的结果基本一致。  相似文献   

16.
基于低磁场返波管振荡器的工作原理,设计了一个捷变频相对论返波管振荡器,该器件由两段对电子束参数要求基本一致的慢波结构串接而成,通过调节引导磁场强度实现器件频率的调节,使其分别工作于C波段和X波段。在电子能量和束流分别为670keV和8kA的条件下,当引导磁场强度为0.5T时,采用2.5维PIC程序模拟得到频率为6.28GHz、功率为1.0GW的微波输出;而当引导磁场强度为0.8T时,得到频率为9.25GHz、功率为0.75GW的微波输出。  相似文献   

17.
对Ka波段TM02模式低磁场相对论返波管的结构特点、工作原理进行了介绍,详细分析了该器件以TM02模工作的模式选择机制。通过粒子模拟,该器件在1 T引导磁场下获得了功率为493 MW、频率29.3 GHz的微波输出,工作模式及频率与理论设计相一致。随后,基于模拟中的结构参数开展了初步的实验研究,当二极管电压为580 kV、电流为3.56 kA、引导磁场1 T时,获得了功率286 MW、频率29.3 GHz、脉宽约10 ns的微波输出。实验获得的微波频率与数值模拟一致,但是微波功率与数值模拟结果有明显差异,并且微波脉冲后沿有明显的缩短,分析认为在低磁场下后端谐振腔链受到电子轰击是导致该问题的主要原因。  相似文献   

18.
设计了一种基于超辐射机理的X波段相对论返波管结构, 利用全电磁2.5维粒子模拟程序对返波管中的超辐射机理进行了粒子模拟研究. 模拟表明: 在束430kV、束流4kA, 脉宽3.1ns的电子束驱动下,实现了峰值功率1.5GW、频率10GHz、脉宽500ps的亚纳秒微波脉冲输出, 峰值功率转换效率达到87.2%;在超辐射机理作用下, 微波峰值功率与电子束脉宽在一定的范围内成平方关系.  相似文献   

19.
Experimental studies of a plasma-filled X-band backward-wave oscillator (BWO) are presented. Depending on the background gas pressure, microwave frequency upshifts of up to 1 GHz appeared along with an enhancement by a factor of 7 in the total microwave power emission. The bandwidth of the microwave emission increased from ⩽0.5 GHz to 2 GHz when the BWO was working at the RF power enhancement pressure region. The RF power enhancement appeared over a much wider pressure range in a high beam current case (10-100 mT for 3 kA) than in a lower beam case (80-115 mT for 1.6 kA). The plasma-filled BWO has higher power output than the vacuum BWO over a broader region of magnetic guide field strength. Trivelpiece-Gould modes (T-G modes) are observed with frequencies up to the background plasma frequency in a plasma-filled BWO. Mode competition between the T-G modes and the X-band Tm01 mode prevailed when the background plasma density was below 6×1011 cm-3 . At a critical background plasma density of ≃8×1011 cm-3 power enhancement appeared in both X-band and the T-G modes. Power enhancement of the S-band in this mode collaboration region reached up to 8 dB. Electric fields measured by the Stark-effect method were as high as 34 kV/cm while the BWO power level was 80 MW. These electric fields lasted throughout the high-power microwave pulse  相似文献   

20.
 设计了一种带有反射腔的能在X波段实现稳定双频输出的圆柱结构相对论返波管,采用2.5维相对论全电磁PIC粒子模拟软件行粒子模拟研究。仿真结果表明:在输入电压433 kV、引导磁场2.2 T的条件下,实现了9.53,10.09 GHz的双频稳定输出,平均输出功率340 MW,平均功率效率24.1%。  相似文献   

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