Numerical Modeling of Plasma Dynamics and Neutron Generation in Z-pinch at the ANGARA-5-1 Facility

IF 0.9 4区 物理与天体物理 Q4 PHYSICS, FLUIDS & PLASMAS
S. F. Garanin, V. Yu. Dolinskii
{"title":"Numerical Modeling of Plasma Dynamics and Neutron Generation in Z-pinch at the ANGARA-5-1 Facility","authors":"S. F. Garanin,&nbsp;V. Yu. Dolinskii","doi":"10.1134/S1063780X24601007","DOIUrl":null,"url":null,"abstract":"<p>Deuterium Z-pinch experimental studies [1] were carried out at the Angara-5-1 facility at a current of 2–2.5 MA with 100 ns rise time. Neutron yield in experiments ranged from 5 × 10<sup>10</sup> to 8 × 10<sup>11</sup> neutrons per pulse. In order to explain experimental results, the two-dimensional MHD calculations were performed taking into account the generation of DD-neutrons using thermonuclear and beam-target mechanisms. MHD calculations of pinch dynamics, carried out taking into account the deuterium density distribution in the gas puff, satisfactory agree with voltage measurements. The neutron yield in the calculations ranges from 4 × 10<sup>10</sup> to 1.5 × 10<sup>11</sup> depending on the deuterium density and the time delay between the start of gas puff and the moment of generator start-up. The energy of accelerated deuterons, which lead to neutron generation in the beam-target mechanism, is calculated to be from 55 to 900 keV, which is in satisfactory agreement with the estimates obtained [1]. An important difference between neutron generation in a fast gas Z-pinch and neutron generation in a dense plasma focus is that the contributions of thermonuclear and beam-target mechanisms to neutron generation in a fast gas Z-pinch are comparable, whereas in a dense plasma focus the main neutron generation mechanism is the beam-target mechanism.</p>","PeriodicalId":735,"journal":{"name":"Plasma Physics Reports","volume":"50 8","pages":"948 - 963"},"PeriodicalIF":0.9000,"publicationDate":"2024-09-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Plasma Physics Reports","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1134/S1063780X24601007","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"PHYSICS, FLUIDS & PLASMAS","Score":null,"Total":0}
引用次数: 0

Abstract

Deuterium Z-pinch experimental studies [1] were carried out at the Angara-5-1 facility at a current of 2–2.5 MA with 100 ns rise time. Neutron yield in experiments ranged from 5 × 1010 to 8 × 1011 neutrons per pulse. In order to explain experimental results, the two-dimensional MHD calculations were performed taking into account the generation of DD-neutrons using thermonuclear and beam-target mechanisms. MHD calculations of pinch dynamics, carried out taking into account the deuterium density distribution in the gas puff, satisfactory agree with voltage measurements. The neutron yield in the calculations ranges from 4 × 1010 to 1.5 × 1011 depending on the deuterium density and the time delay between the start of gas puff and the moment of generator start-up. The energy of accelerated deuterons, which lead to neutron generation in the beam-target mechanism, is calculated to be from 55 to 900 keV, which is in satisfactory agreement with the estimates obtained [1]. An important difference between neutron generation in a fast gas Z-pinch and neutron generation in a dense plasma focus is that the contributions of thermonuclear and beam-target mechanisms to neutron generation in a fast gas Z-pinch are comparable, whereas in a dense plasma focus the main neutron generation mechanism is the beam-target mechanism.

Abstract Image

ANGARA-5-1 设施 Z-pinch 中等离子体动力学和中子生成的数值建模
氘 Z-pinch 实验研究[1] 是在安加拉-5-1 设备上进行的,电流为 2-2.5 MA,上升时间为 100 ns。实验中的中子产率为每个脉冲 5 × 1010 到 8 × 1011 个中子。为了解释实验结果,进行了二维 MHD 计算,其中考虑到了利用热核机制和束靶机制产生的 DD 中子。考虑到气泡中的氘密度分布而进行的挤压动力学 MHD 计算与电压测量结果完全吻合。计算得出的中子产率从 4 × 1010 到 1.5 × 1011 不等,这取决于氘密度以及气浮开始到发电机启动之间的时间延迟。根据计算,在束-靶机制中导致中子产生的加速氘核的能量为 55 至 900 千伏,这与所获得的估计值[1]完全一致。快速气体 Z 型夹中子生成与稠密等离子体焦点中子生成的一个重要区别是,在快速气体 Z 型夹中,热核机制和束靶机制对中子生成的贡献相当,而在稠密等离子体焦点中,主要的中子生成机制是束靶机制。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
来源期刊
Plasma Physics Reports
Plasma Physics Reports 物理-物理:流体与等离子体
CiteScore
1.90
自引率
36.40%
发文量
104
审稿时长
4-8 weeks
期刊介绍: Plasma Physics Reports is a peer reviewed journal devoted to plasma physics. The journal covers the following topics: high-temperature plasma physics related to the problem of controlled nuclear fusion based on magnetic and inertial confinement; physics of cosmic plasma, including magnetosphere plasma, sun and stellar plasma, etc.; gas discharge plasma and plasma generated by laser and particle beams. The journal also publishes papers on such related topics as plasma electronics, generation of radiation in plasma, and plasma diagnostics. As well as other original communications, the journal publishes topical reviews and conference proceedings.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信