首页> 外文期刊>Plasma Science, IEEE Transactions on >Neutron Emission Characteristics of NX-3 Plasma Focus Device: Speed Factor as the Guiding Rule for Yield Optimization
【24h】

Neutron Emission Characteristics of NX-3 Plasma Focus Device: Speed Factor as the Guiding Rule for Yield Optimization

机译:NX-3等离子聚焦装置的中子发射特性:以速度因子为优化产率的指导原则

获取原文
获取原文并翻译 | 示例

摘要

This paper reports the results of characterization and optimization experiments carried out on a newly developed NX-3 dense plasma focus device (20 kJ at 20 kV, a quarter time period of $sim!!3 muhbox{s}$, and 10 kJ/600 kA at 14 kV) at the Plasma Radiation Source Laboratory, NIE, Nanyang Technological University, Singapore. Initial experiments were conducted with an electrode assembly configuration having anode radius and length of 20 and 160 mm, respectively, for detailed neutron emission characterization of NX-3 device followed by further optimization of neutron yield using various other electrode configurations designed using the Lee Code. At $geq$10-kJ operation, the average neutron yield on the order of $10^{9}$ neutrons/pulse in $4pihbox{sr}$ was obtained for the deuterium filling gas pressure range of 6–8 mbar. The neutron yield of $sim!!4.6 times 10^{9}$ neutrons/pulse at 10 kJ/6 mbar is the highest ever reported for a device with the same stored energy. The neutron anisotropy measurements point to the beam–target mechanism as the dominant neutron production mechanism for NX-3 plasma focus device. Further optimization of neutron yield in NX-3 was achieved with the peak average neutron yield being enhanced from $sim!!(2.38 pm 0.31) times 10^{9}$ neutrons/shot for the initial electrode configuration to about $sim!!(3.40 pm 0.43) times 10^{9}$ neutrons/shot for the electrode configuration with anode radius and length of 26 and 140 mm, respectively. The analysis of neu- ron yield results for various electrode assembly configurations demonstrates the speed factor as a key optimization tool for maximization of neutron yield.
机译:本文报告了在新开发的NX-3密集等离子体聚焦设备(20 kV在20 kV下,四分之一的时间为$ sim !! 3 muhbox {s} $,和10 kJ /新加坡南洋理工大学NIE等离子体辐射源实验室,在14 kV时为600 kA)。为了分别详细描述NX-3装置的中子发射特性,首先使用阳极半径和长度分别为20和160 mm的电极组件配置进行了初始实验,然后使用使用Lee Code设计的各种其他电极配置进一步优化了中子产率。在$ geq $ 10-kJ操作下,氘充气压力范围为6-8 mbar,获得的中子平均产额为$ 10 ^ {9} $中子/脉冲,约为$ 4pihbox {sr} $。在10 kJ / 6 mbar下,$ sim !!的中子产率为4.6乘以10 ^ {9} $中子/脉冲,是有相同存储能量的设备的最高记录。中子各向异性测量结果表明,射束目标机制是NX-3等离子聚焦装置的主要中子产生机制。 NX-3中子产量的进一步优化实现了,将平均中子的峰值平均产量从$ sim !!(2.38 pm 0.31)乘以初始电极配置的10 ^ {9} $中子/发射到约$ sim !!! (3.40 pm 0.43)乘以10 ^ {9} $中子/发射的电极配置,阳极半径和长度分别为26和140 mm。对各种电极组件配置的中子产率结果的分析表明,速度因子是使中子产率最大化的关键优化工具。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号