设计了用于Z箍缩丝阵实验的重频LTD 驱动器,含6路并联模组,每组由8个0.8 MA 原型模块串联组成,全真空结构.原型模块采用全新的单路触发和电感隔离技术,触发难度和重频运行可靠性得到显著优化.利用电路模拟程序对驱动器进行了仿真计算,...设计了用于Z箍缩丝阵实验的重频LTD 驱动器,含6路并联模组,每组由8个0.8 MA 原型模块串联组成,全真空结构.原型模块采用全新的单路触发和电感隔离技术,触发难度和重频运行可靠性得到显著优化.利用电路模拟程序对驱动器进行了仿真计算,结果表明:在初始半径1.2cm、线质量1mg/cm 的Z箍缩负载上,驱动器的输出电流峰值可到5.2 MA,前沿91ns;负载内爆最大动能78kJ,从电容储能至负载动能的转化效率为11.7%.该驱动器预期将获得高达20%~30%的辐射能量效率,可为Z箍缩物理研究提供高效的实验平台.展开更多
介绍了一种用于丝阵Z箍缩(Z-pinch)内爆实验研究的脉冲放电模块的设计。模块基于直线型变压器驱动器(LTD)技术,包含34个放电支路,通过4个铁基非晶磁芯耦合。每支路由2个40nF电容器和1只4间隙串联气体开关组成,回路电感为220nH。设计了...介绍了一种用于丝阵Z箍缩(Z-pinch)内爆实验研究的脉冲放电模块的设计。模块基于直线型变压器驱动器(LTD)技术,包含34个放电支路,通过4个铁基非晶磁芯耦合。每支路由2个40nF电容器和1只4间隙串联气体开关组成,回路电感为220nH。设计了水电阻负载检验模块输出性能,在匹配状态下,负载上的输出电流峰值916 k A,上升时间99.8 ns。设计了磁绝缘传输线将输出脉冲传输至Z-pinch丝阵负载,并利用"零维模型"对LTD模块和负载的耦合放电进行了模拟计算。结果显示,丝阵负载上的放电电流峰值可达960 k A,上升时间为114 ns。展开更多
采用复合金属收集极设计的真空康普顿探测器,使伽马探测灵敏度有效提高。为表征探测器测量信号的质量和可靠性,需要对探测器的γ/n鉴别本领进行评估。应用强钴源(能量1.25 Me V)伽马和DT(能量14 Me V)中子源对这种探测效率增强的新型真...采用复合金属收集极设计的真空康普顿探测器,使伽马探测灵敏度有效提高。为表征探测器测量信号的质量和可靠性,需要对探测器的γ/n鉴别本领进行评估。应用强钴源(能量1.25 Me V)伽马和DT(能量14 Me V)中子源对这种探测效率增强的新型真空探测器灵敏度进行实验测量,采用蒙特卡罗模拟法(MC)模拟统计收集极输出净电子数的方法,对其在裂变能量区几个特征能量点的伽马、中子灵敏度进行模拟计算。结果表明:对于中子、伽马能量为1.25 Me V的情况,这种新型真空康普顿探测器的γ/n鉴别本领,理论模拟计算值为40.94,综合理论计算和实验测量结果的实验推算评估值为28.31;属于适合中子、伽马混合场中测量伽马的可选探测器。展开更多
The fission electron-collection neutron detector (FECND) is a current-type neutron detector. Based on the analysis of the generation process of the gamma signals of the FECND, a mechanism utilizing symmetrical struc...The fission electron-collection neutron detector (FECND) is a current-type neutron detector. Based on the analysis of the generation process of the gamma signals of the FECND, a mechanism utilizing symmetrical structure is proposed and discussed to suppress the gamma signals. According to this mechanism, tile electrons generated from the gamma rays can be well compensated for by the adjustment of the electrodes' thickness and distance. In this study, based on the Monte-Carlo simulation of the gamma signals of the FECND, the varying patterns are obtained between the gamma signals and the detector parameter settings. As indicated by the simulation results, the gamma electrons can be compensated for completely by simply adjusting the coated electrode substrate thickness and distance. Moreover, with a proposed optimal parameter setting, the gamma sensitivity can be as low as 3.39×10-23 C.cm2, while the signal-to-noise ratio can be higher than 200:1. The compensation results of the γ-rays in the FECND will be slightly affected by the manufacturing error or the assembly error.展开更多
文摘介绍了一种用于丝阵Z箍缩(Z-pinch)内爆实验研究的脉冲放电模块的设计。模块基于直线型变压器驱动器(LTD)技术,包含34个放电支路,通过4个铁基非晶磁芯耦合。每支路由2个40nF电容器和1只4间隙串联气体开关组成,回路电感为220nH。设计了水电阻负载检验模块输出性能,在匹配状态下,负载上的输出电流峰值916 k A,上升时间99.8 ns。设计了磁绝缘传输线将输出脉冲传输至Z-pinch丝阵负载,并利用"零维模型"对LTD模块和负载的耦合放电进行了模拟计算。结果显示,丝阵负载上的放电电流峰值可达960 k A,上升时间为114 ns。
文摘采用复合金属收集极设计的真空康普顿探测器,使伽马探测灵敏度有效提高。为表征探测器测量信号的质量和可靠性,需要对探测器的γ/n鉴别本领进行评估。应用强钴源(能量1.25 Me V)伽马和DT(能量14 Me V)中子源对这种探测效率增强的新型真空探测器灵敏度进行实验测量,采用蒙特卡罗模拟法(MC)模拟统计收集极输出净电子数的方法,对其在裂变能量区几个特征能量点的伽马、中子灵敏度进行模拟计算。结果表明:对于中子、伽马能量为1.25 Me V的情况,这种新型真空康普顿探测器的γ/n鉴别本领,理论模拟计算值为40.94,综合理论计算和实验测量结果的实验推算评估值为28.31;属于适合中子、伽马混合场中测量伽马的可选探测器。
基金Supported by the National Natural Science Foundation of China under Grant No 11205141the Science and Technology Foundation of China Academy of Engineering Physics under Grant No 2012B0103003
文摘The fission electron-collection neutron detector (FECND) is a current-type neutron detector. Based on the analysis of the generation process of the gamma signals of the FECND, a mechanism utilizing symmetrical structure is proposed and discussed to suppress the gamma signals. According to this mechanism, tile electrons generated from the gamma rays can be well compensated for by the adjustment of the electrodes' thickness and distance. In this study, based on the Monte-Carlo simulation of the gamma signals of the FECND, the varying patterns are obtained between the gamma signals and the detector parameter settings. As indicated by the simulation results, the gamma electrons can be compensated for completely by simply adjusting the coated electrode substrate thickness and distance. Moreover, with a proposed optimal parameter setting, the gamma sensitivity can be as low as 3.39×10-23 C.cm2, while the signal-to-noise ratio can be higher than 200:1. The compensation results of the γ-rays in the FECND will be slightly affected by the manufacturing error or the assembly error.