ISSP超高斯科学实验室电磁通量压缩实验的数值模拟

S. F. Garanin, G. G. Ivanova, S. Kuznetsov
{"title":"ISSP超高斯科学实验室电磁通量压缩实验的数值模拟","authors":"S. F. Garanin, G. G. Ivanova, S. Kuznetsov","doi":"10.1109/MEGAGAUSS.2012.6781436","DOIUrl":null,"url":null,"abstract":"The International MegaGauss Science Laboratory at the Institute for Solid State Physics, (ISSP) Japan, conducts experiments on magnetic flux compression by liners [1]. Magnetic fields produced in these experiments currently reach 700 T and break laboratory-scale records. We have conducted 1D numerical simulations of magnetic flux compression under these experimental conditions to determine distributions of parameters across the liner and correlations between resulting magnetic fields and parameters of the liner (thickness and velocity) and seed magnetic field, and to calculate characteristics of plasma, which is predicted [2, 3] to form in such megagauss fields. Our simulation results verify generation of 6-7 MG range magnetic fields in the experiments by Takeyama [1]. In the 1D simulations, as distinct from the experiments, the resulting magnetic fields grow with decrease in the seed magnetic field, which in the simulations is attributed to the fact that the level of magnetic energy produced is controlled by the kinetic energy of the liner and is a weak function of the seed field. Consequently, with decrease in the seed magnetic field, the minimum radius of the liner decreases, and the maximum magnetic field increases. In addition, increase in the liner velocity in the simulations (even for a thinner liner with the same kinetic energy) also leads to higher magnetic fields, which is not observed in the experiments, either. One can suppose that these contradictions between simulation and experiment are related to the development of magnetohydrodynamic instabilities, which produce a compression picture different from 1D. The simulations have also demonstrated that plasma, the temperature of which turns out to be on the order of 20 eV at maximum compression, forms on the inside liner surface (magnetic field/matter interface) starting from a ~360 T magnetic field.","PeriodicalId":299352,"journal":{"name":"2012 14th International Conference on Megagauss Magnetic Field Generation and Related Topics (MEGAGAUSS)","volume":"14 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2012-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Numerical simulations of the electromagnetic flux compression experiments at the Megagauss Science Laboratory at ISSP\",\"authors\":\"S. F. Garanin, G. G. Ivanova, S. Kuznetsov\",\"doi\":\"10.1109/MEGAGAUSS.2012.6781436\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The International MegaGauss Science Laboratory at the Institute for Solid State Physics, (ISSP) Japan, conducts experiments on magnetic flux compression by liners [1]. Magnetic fields produced in these experiments currently reach 700 T and break laboratory-scale records. We have conducted 1D numerical simulations of magnetic flux compression under these experimental conditions to determine distributions of parameters across the liner and correlations between resulting magnetic fields and parameters of the liner (thickness and velocity) and seed magnetic field, and to calculate characteristics of plasma, which is predicted [2, 3] to form in such megagauss fields. Our simulation results verify generation of 6-7 MG range magnetic fields in the experiments by Takeyama [1]. In the 1D simulations, as distinct from the experiments, the resulting magnetic fields grow with decrease in the seed magnetic field, which in the simulations is attributed to the fact that the level of magnetic energy produced is controlled by the kinetic energy of the liner and is a weak function of the seed field. Consequently, with decrease in the seed magnetic field, the minimum radius of the liner decreases, and the maximum magnetic field increases. In addition, increase in the liner velocity in the simulations (even for a thinner liner with the same kinetic energy) also leads to higher magnetic fields, which is not observed in the experiments, either. One can suppose that these contradictions between simulation and experiment are related to the development of magnetohydrodynamic instabilities, which produce a compression picture different from 1D. The simulations have also demonstrated that plasma, the temperature of which turns out to be on the order of 20 eV at maximum compression, forms on the inside liner surface (magnetic field/matter interface) starting from a ~360 T magnetic field.\",\"PeriodicalId\":299352,\"journal\":{\"name\":\"2012 14th International Conference on Megagauss Magnetic Field Generation and Related Topics (MEGAGAUSS)\",\"volume\":\"14 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2012-10-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2012 14th International Conference on Megagauss Magnetic Field Generation and Related Topics (MEGAGAUSS)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/MEGAGAUSS.2012.6781436\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2012 14th International Conference on Megagauss Magnetic Field Generation and Related Topics (MEGAGAUSS)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/MEGAGAUSS.2012.6781436","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

摘要

日本固体物理研究所(ISSP)的国际MegaGauss科学实验室进行了衬垫压缩磁通量的实验[1]。这些实验产生的磁场目前达到700 T,打破了实验室规模的记录。我们在这些实验条件下对磁通量压缩进行了一维数值模拟,以确定参数在衬垫上的分布,以及由此产生的磁场与衬垫参数(厚度和速度)和种子磁场之间的相关性,并计算预测在这些兆高斯场中形成的等离子体的特性[2,3]。我们的仿真结果验证了Takeyama[1]实验中产生的6- 7mg范围的磁场。在一维模拟中,与实验不同的是,产生的磁场随着种子磁场的减小而增大,这在模拟中是由于产生的磁能水平是由衬板的动能控制的,是种子场的弱函数。因此,随着种子磁场的减小,衬板的最小半径减小,最大磁场增大。此外,模拟中线材速度的增加(即使是具有相同动能的较薄的线材)也会导致更高的磁场,这在实验中也没有观察到。可以认为,这些模拟与实验之间的矛盾与磁流体动力学不稳定性的发展有关,它产生了与一维不同的压缩图像。模拟还表明,等离子体从~360 T的磁场开始在内层表面(磁场/物质界面)形成,其最大压缩温度约为20 eV。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Numerical simulations of the electromagnetic flux compression experiments at the Megagauss Science Laboratory at ISSP
The International MegaGauss Science Laboratory at the Institute for Solid State Physics, (ISSP) Japan, conducts experiments on magnetic flux compression by liners [1]. Magnetic fields produced in these experiments currently reach 700 T and break laboratory-scale records. We have conducted 1D numerical simulations of magnetic flux compression under these experimental conditions to determine distributions of parameters across the liner and correlations between resulting magnetic fields and parameters of the liner (thickness and velocity) and seed magnetic field, and to calculate characteristics of plasma, which is predicted [2, 3] to form in such megagauss fields. Our simulation results verify generation of 6-7 MG range magnetic fields in the experiments by Takeyama [1]. In the 1D simulations, as distinct from the experiments, the resulting magnetic fields grow with decrease in the seed magnetic field, which in the simulations is attributed to the fact that the level of magnetic energy produced is controlled by the kinetic energy of the liner and is a weak function of the seed field. Consequently, with decrease in the seed magnetic field, the minimum radius of the liner decreases, and the maximum magnetic field increases. In addition, increase in the liner velocity in the simulations (even for a thinner liner with the same kinetic energy) also leads to higher magnetic fields, which is not observed in the experiments, either. One can suppose that these contradictions between simulation and experiment are related to the development of magnetohydrodynamic instabilities, which produce a compression picture different from 1D. The simulations have also demonstrated that plasma, the temperature of which turns out to be on the order of 20 eV at maximum compression, forms on the inside liner surface (magnetic field/matter interface) starting from a ~360 T magnetic field.
求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
自引率
0.00%
发文量
0
×
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:604180095
Book学术官方微信