Plasma performance enhancement and impurity control using a novel technique of argon–hydrogen mixture fueled glow discharge wall conditioning in the ADITYA-U tokamak

IF 3.5 1区 物理与天体物理 Q1 PHYSICS, FLUIDS & PLASMAS
K.A. Jadeja, J. Ghosh, K.M. Patel, A.B. Patel, R.L. Tanna, Kiran Patel, B.G. Arambhadiya, K.D. Galodiya, Rohit Kumar, S. Aich, Harshita Raj, L. Pradhan, M.B. Chowdhuri, R. Manchanda, N. Ramaiya, Nandini Yadava, Sharvil Patel, Kajal Shah, Dipexa Modi, A. Gauttam, K. Singh, S. Dolui, Ankit Kumar, B. Hegde, A. Kumawat, Minsha Shah, R. Rajpal, U. Nagora, P.K. Atrey, S.K. Pathak, Shishir Purohit, A. Adhiya, Manoj Kumar, Kumudni Assudani, D. Kumavat, S.K. Jha, K.S. Shah, M.N. Makwana, Shivam Gupta, Supriya Nair, Kishore Mishra, D. Raju, P.K. Chattopadhyay, B.R. Kataria
{"title":"Plasma performance enhancement and impurity control using a novel technique of argon–hydrogen mixture fueled glow discharge wall conditioning in the ADITYA-U tokamak","authors":"K.A. Jadeja, J. Ghosh, K.M. Patel, A.B. Patel, R.L. Tanna, Kiran Patel, B.G. Arambhadiya, K.D. Galodiya, Rohit Kumar, S. Aich, Harshita Raj, L. Pradhan, M.B. Chowdhuri, R. Manchanda, N. Ramaiya, Nandini Yadava, Sharvil Patel, Kajal Shah, Dipexa Modi, A. Gauttam, K. Singh, S. Dolui, Ankit Kumar, B. Hegde, A. Kumawat, Minsha Shah, R. Rajpal, U. Nagora, P.K. Atrey, S.K. Pathak, Shishir Purohit, A. Adhiya, Manoj Kumar, Kumudni Assudani, D. Kumavat, S.K. Jha, K.S. Shah, M.N. Makwana, Shivam Gupta, Supriya Nair, Kishore Mishra, D. Raju, P.K. Chattopadhyay, B.R. Kataria","doi":"10.1088/1741-4326/ad6a6e","DOIUrl":null,"url":null,"abstract":"Effective control of impurities and precise regulation of the fueling gas are supreme prerequisites for optimal operation in any fusion device. Conventional wall-conditioning methods fall short of achieving optimal wall conditioning. Conventional wall-conditioning methods, such as vessel baking and H<sub>2</sub>/(D<sub>2</sub>)-fueled glow discharge cleaning (GDC), are generally required to remove wall-absorbed impurities in bulk after vessel venting. The excess amount of hydrogen, injected during H<sub>2</sub> GDC, can be reduced by helium (He)-fueled GDC. However, He removal from the vessel is more challenging due to its low molecular mass, very low condensation temperature, and inert characteristics. In ADITYA-U, optimal wall conditioning cannot be achieved using H<sub>2</sub> followed by He-fueled GDC when applied for extended periods spanning hours or days. A GDC with a mixture of argon and hydrogen (Ar–H<sub>2</sub>) is introduced in the ADITYA-U tokamak to obtain better wall conditioning than H<sub>2</sub> followed by He GDC. In Ar–H<sub>2</sub> GDC, long-lived ArH<sup>+</sup> ions are formed in sufficient numbers and accelerated toward the vessel wall with high momentum. This results in the breaking of high energy bonds of impurities with the wall/plasma facing components, which is not possible by H<sup>+</sup>, H<sub>2</sub><sup>+,</sup> H<sub>3</sub><sup>+</sup> ions in H<sub>2</sub> GDC due to their lower momentum. An optimal blend ratio of Ar to H<sub>2</sub> is established at 15%–20% for the mixture. This composition ensures that the introduction of high-<italic toggle=\"yes\">Z</italic> Ar does not adversely affect tokamak plasma operations. The C- and O-containing impurities are reduced beyond the limit of the prolonged operation of H<sub>2</sub> GDC. Relative low pressures of dominant impurities such as CO, CH<sub>4</sub>, and H<sub>2</sub>O are obtained due to the Ar–H<sub>2</sub> GDC compared to routinely operated H<sub>2</sub> GDC. A comparison study of H<sub>2</sub> GDC and the developed Ar–H<sub>2</sub> GDC is performed in terms of wall conditioning and tokamak plasma operation. The encouraging results of the Ar–H<sub>2</sub> GDC are obtained in both wall cleaning and tokamak operation scenarios in the midsize tokamak ADITYA-U. This development and application of Ar–H<sub>2</sub> GDC are beneficial for large-sized fusion devices, leading to improved impurity reduction, reduced operational fuel consumption (H<sub>2</sub>/D<sub>2</sub>/He), and enhanced control over fuel recycling/extraction.","PeriodicalId":19379,"journal":{"name":"Nuclear Fusion","volume":"12 1","pages":""},"PeriodicalIF":3.5000,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Fusion","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1741-4326/ad6a6e","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, FLUIDS & PLASMAS","Score":null,"Total":0}
引用次数: 0

Abstract

Effective control of impurities and precise regulation of the fueling gas are supreme prerequisites for optimal operation in any fusion device. Conventional wall-conditioning methods fall short of achieving optimal wall conditioning. Conventional wall-conditioning methods, such as vessel baking and H2/(D2)-fueled glow discharge cleaning (GDC), are generally required to remove wall-absorbed impurities in bulk after vessel venting. The excess amount of hydrogen, injected during H2 GDC, can be reduced by helium (He)-fueled GDC. However, He removal from the vessel is more challenging due to its low molecular mass, very low condensation temperature, and inert characteristics. In ADITYA-U, optimal wall conditioning cannot be achieved using H2 followed by He-fueled GDC when applied for extended periods spanning hours or days. A GDC with a mixture of argon and hydrogen (Ar–H2) is introduced in the ADITYA-U tokamak to obtain better wall conditioning than H2 followed by He GDC. In Ar–H2 GDC, long-lived ArH+ ions are formed in sufficient numbers and accelerated toward the vessel wall with high momentum. This results in the breaking of high energy bonds of impurities with the wall/plasma facing components, which is not possible by H+, H2+, H3+ ions in H2 GDC due to their lower momentum. An optimal blend ratio of Ar to H2 is established at 15%–20% for the mixture. This composition ensures that the introduction of high-Z Ar does not adversely affect tokamak plasma operations. The C- and O-containing impurities are reduced beyond the limit of the prolonged operation of H2 GDC. Relative low pressures of dominant impurities such as CO, CH4, and H2O are obtained due to the Ar–H2 GDC compared to routinely operated H2 GDC. A comparison study of H2 GDC and the developed Ar–H2 GDC is performed in terms of wall conditioning and tokamak plasma operation. The encouraging results of the Ar–H2 GDC are obtained in both wall cleaning and tokamak operation scenarios in the midsize tokamak ADITYA-U. This development and application of Ar–H2 GDC are beneficial for large-sized fusion devices, leading to improved impurity reduction, reduced operational fuel consumption (H2/D2/He), and enhanced control over fuel recycling/extraction.
在 ADITYA-U 托卡马克中使用新型氩氢混合燃料辉光放电壁调节技术提高等离子体性能并控制杂质
有效控制杂质和精确调节燃料气体是任何聚变装置实现最佳运行的最高前提。传统的壁调节方法无法实现最佳的壁调节效果。传统的壁处理方法,如容器烘烤和以 H2/(D2)为燃料的辉光放电清洗 (GDC),通常需要在容器排气后大量清除壁吸收的杂质。以氦(He)为燃料的 GDC 可以减少 H2 GDC 过程中注入的过量氢气。然而,由于氦气的分子质量低、冷凝温度极低,且具有惰性,因此从容器中去除氦气更具挑战性。在 ADITYA-U 中,使用 H2 后再使用以 He 为燃料的 GDC 时,如果使用时间长达数小时或数天,则无法达到最佳的壁调节效果。在 ADITYA-U 托卡马克中引入了氩氢混合物(Ar-H2)的 GDC,以获得比 H2 和 He GDC 更佳的壁调节效果。在 Ar-H2 GDC 中,会形成足够数量的长寿命 ArH+ 离子,并以高动量加速冲向容器壁。这将导致杂质与器壁/等离子面对的成分之间的高能键断裂,而 H2 GDC 中的 H+、H2+、H3+ 离子由于动量较小,无法实现这一点。混合物中 Ar 与 H2 的最佳混合比例为 15%-20%。这种成分可确保高 Z Ar 的引入不会对托卡马克等离子体的运行产生不利影响。含 C 和 O 的杂质减少到超过 H2 GDC 长期运行的极限。与常规运行的 H2 GDC 相比,Ar-H2 GDC 获得了 CO、CH4 和 H2O 等主要杂质的相对低压。在壁调节和托卡马克等离子体运行方面,对 H2 GDC 和开发的 Ar-H2 GDC 进行了比较研究。在中型托卡马克 ADITYA-U 中,Ar-H2 GDC 在壁清洁和托卡马克运行情况下都取得了令人鼓舞的结果。Ar-H2 GDC 的开发和应用有利于大型核聚变装置,从而减少杂质,降低运行燃料消耗(H2/D2/He),并加强对燃料回收/提取的控制。
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
Nuclear Fusion
Nuclear Fusion 物理-物理:核物理
CiteScore
6.30
自引率
39.40%
发文量
411
审稿时长
2.6 months
期刊介绍: Nuclear Fusion publishes articles making significant advances to the field of controlled thermonuclear fusion. The journal scope includes: -the production, heating and confinement of high temperature plasmas; -the physical properties of such plasmas; -the experimental or theoretical methods of exploring or explaining them; -fusion reactor physics; -reactor concepts; and -fusion technologies. The journal has a dedicated Associate Editor for inertial confinement fusion.
×
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