Qing-Gang Zhou, Yanjie Zhang, C. Sang, Jiaxian Li, Guoyao Zheng, Yilin Wang, Yihan Wu, Dezhen Wang
{"title":"Simulation of tungsten impurity transport by DIVIMP under different divertor magnetic configurations on HL-3","authors":"Qing-Gang Zhou, Yanjie Zhang, C. Sang, Jiaxian Li, Guoyao Zheng, Yilin Wang, Yihan Wu, Dezhen Wang","doi":"10.1088/2058-6272/ad6817","DOIUrl":null,"url":null,"abstract":"\n Tungsten (W) accumulation in the core, depending on W generation and transport in the edge region, is a severe issue in fusion reactor. The divertor plasma parameters, such as heat flux to the target, can be effectively suppressed by changing the divertor magnetic configuration. Nevertheless, its impact on W core accumulation remains unclear. The HL-3 tokamak has advantage of operating with flexible divertor configurations, e.g. standard divertor (SD) and snowflake divertors (SFD). In this study, DIVIMP combined with SOLPS-ITER is applied to investigate the effects of divertor magnetic configurations (SD vs SFD) on W accumulation during neon injection in HL-3. It is found that W concentration in the core of SFD is significantly higher than that of SD with similar total W erosion flux. The reasons are: (1) W impurities in the core of SFD mainly originate from inner divertor, which has short leg, and the source is close to the divertor entrance and upstream separatrix. Furthermore, the SW0 is much stronger, especially near divertor entrance. (2) the region overlap of SW0 and F_(W,TOT) pointing to upstream promote W accumulation in the core. Moreover, influence of W source locations at inner target on W transport in the SFD is investigated. Tungsten impurity in the core is mainly contributed by target erosion at common flux region (CFR) away from strike point. This is attributed to that W source at this location enhances ionization source above the W ion stagnation point, which sequentially increases W penetration. Therefore, the suppression of far SOL inner target erosion can effectively prevent W impurities from accumulating in the core.","PeriodicalId":506986,"journal":{"name":"Plasma Science and Technology","volume":"46 16","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Plasma Science and Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/2058-6272/ad6817","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Tungsten (W) accumulation in the core, depending on W generation and transport in the edge region, is a severe issue in fusion reactor. The divertor plasma parameters, such as heat flux to the target, can be effectively suppressed by changing the divertor magnetic configuration. Nevertheless, its impact on W core accumulation remains unclear. The HL-3 tokamak has advantage of operating with flexible divertor configurations, e.g. standard divertor (SD) and snowflake divertors (SFD). In this study, DIVIMP combined with SOLPS-ITER is applied to investigate the effects of divertor magnetic configurations (SD vs SFD) on W accumulation during neon injection in HL-3. It is found that W concentration in the core of SFD is significantly higher than that of SD with similar total W erosion flux. The reasons are: (1) W impurities in the core of SFD mainly originate from inner divertor, which has short leg, and the source is close to the divertor entrance and upstream separatrix. Furthermore, the SW0 is much stronger, especially near divertor entrance. (2) the region overlap of SW0 and F_(W,TOT) pointing to upstream promote W accumulation in the core. Moreover, influence of W source locations at inner target on W transport in the SFD is investigated. Tungsten impurity in the core is mainly contributed by target erosion at common flux region (CFR) away from strike point. This is attributed to that W source at this location enhances ionization source above the W ion stagnation point, which sequentially increases W penetration. Therefore, the suppression of far SOL inner target erosion can effectively prevent W impurities from accumulating in the core.
钨(W)在堆芯中的积累取决于 W 在边缘区域的生成和传输,这是聚变反应堆中的一个严重问题。通过改变岔流器的磁场配置,可以有效地抑制岔流器等离子体参数,如到达目标的热通量。尽管如此,它对 W 核积累的影响仍不明确。HL-3 托卡马克具有使用灵活的岔流器配置(如标准岔流器(SD)和雪花岔流器(SFD))的优势。在本研究中,DIVIMP 与 SOLPS-ITER 结合使用,研究了 HL-3 中子注入过程中分流器磁配置(SD 与 SFD)对 W 累积的影响。研究发现,在 W 总侵蚀通量相近的情况下,SFD 内核中的 W 浓度明显高于 SD 内核中的 W 浓度。原因如下(1) SFD 内核中的 W 杂质主要来源于内岔道,而内岔道支腿较短,且来源靠近岔道入口和上游分离矩阵。此外,SW0 的强度更大,尤其是在分流器入口附近。(2) SW0 和 F_(W,TOT)指向上游的重叠区域促进了 W 在堆芯中的积累。此外,还研究了内靶的 W 源位置对 W 在 SFD 中传输的影响。堆芯中的钨杂质主要是由远离打击点的共同通量区(CFR)的靶材侵蚀造成的。这是因为该位置的 W 源增强了 W 离子停滞点上方的电离源,从而增加了 W 的穿透力。因此,抑制远 SOL 内靶侵蚀可有效防止 W 杂质在堆芯中积累。