Please wait a minute...
Chin. Phys. B, 2024, Vol. 33(11): 115201    DOI: 10.1088/1674-1056/ad711e
PHYSICS OF GASES, PLASMAS, AND ELECTRIC DISCHARGES Prev   Next  

Comparative study of boron and neon injections on divertor heat fluxes using SOLPS-ITER simulations

Lei Peng(彭磊)1, Zhen Sun(孙震)2, Ji-Zhong Sun(孙继忠)1,†, Rajesh Maingi2, Fang Gao(高放)3, Xavier Bonnin4, Hua-Yi Chang(常华溢)1, Wei-Kang Wang(汪炜康)1, and Jin-Yuan Liu(刘金远)1
1 Key Laboratory of Materials Modification by Laser, Ion, and Electron Beams (Ministry of Education), Dalian University of Technology, Dalian 116024, China;
2 Princeton Plasma Physics Laboratory, Princeton, NJ 08543, United States of America;
3 School of Computer and Communication Engineering, Dalian Jiaotong University, Dalian 116028, China;
4 ITER Organization, Route de Vinon-sur-Verdon, CS 90 046, 13067 St-Paul-lez-Durance, France
Abstract  Based on the EAST equilibrium, the effects of boron (B) and neon (Ne) injected at different locations on the target heat load, and the distributions of B and Ne particles were investigated by transport code SOLPS-ITER. It was found that the B injection was more sensitive to the injection location for heat flux control than impurity Ne. The high electron and ion densities near the inner target in the discharge with impurity B injected from over $X$-point ($R_{1}$) led to plasma detachment only at the inner target, and the localized B ions in the cases with injection from outer target location ($R_{2}$) and upstream location ($R_{3}$) led to far-SOL detachment at the outer target, but not at the inner target. In contrast, for Ne, the spatial distributions of Ne ions and electrons were found to be similar in all the cases at the three injection locations, and the detached plasma was achieved at the inner target and the electron temperature was reduced at the outer target. For locations $R_{2}$ and $R_{3}$, impurity B showed a more pronounced effect on the heat flux at the far-SOL of the outer target. Further analysis indicated that Ne atoms came mainly from the recycling sources, whereas B atoms came mainly from injection, and that their distinct atomic distributions resulted from the difference in the ionization threshold and ionization mean free path. In addition, the radiation proportion of B in the divertor region was larger than that of Ne when the total radiation power was similar, which suggests that B has less influence on the core region.
Keywords:  boron      neon      injection location      heat flux  
Received:  29 June 2024      Revised:  13 August 2024      Accepted manuscript online:  20 August 2024
PACS:  52.25.Vy (Impurities in plasmas)  
  52.55.Fa (Tokamaks, spherical tokamaks)  
  52.55.Rk (Power exhaust; divertors)  
  52.65.-y (Plasma simulation)  
Fund: Project supported by the National Key R&D Program of China (Grant No. 2019YFE03030004), the National Natural Science Foundation of China (Grant No. 12275040), and the Users with Excellence Program of Hefei Science Center CAS (Grant No. 2020HSC-UE010). This research is also sponsored in part by the U.S. Department of Energy under contract DEAC02-09CH11466.
Corresponding Authors:  Ji-Zhong Sun     E-mail:  jsun@dlut.edu.cn

Cite this article: 

Lei Peng(彭磊), Zhen Sun(孙震), Ji-Zhong Sun(孙继忠), Rajesh Maingi, Fang Gao(高放), Xavier Bonnin, Hua-Yi Chang(常华溢), Wei-Kang Wang(汪炜康), and Jin-Yuan Liu(刘金远) Comparative study of boron and neon injections on divertor heat fluxes using SOLPS-ITER simulations 2024 Chin. Phys. B 33 115201

[1] Xiao W W, Diamond P H, Zou X L, et al. 2012 Nuclear Fusion 52 114027
[2] Lunsford R, Hu J S, Sun Z, et al. 2018 Nuclear Fusion 58 126021
[3] Lang P T, Maingi R, Mansfield D K, et al. 2017 Nuclear Fusion 57 016030
[4] Reimold F, Wischmeier M, Bernert M, et al. 2015 Nuclear Fusion 55 033004
[5] Kallenbach A, Dux R, Fuchs J C, et al. 2010 Plasma Physics and Controlled Fusion 52 055002
[6] Nakano T 2015 Journal of Nuclear Materials 463 555
[7] Bernert M, Wischmeier M, Huber A, et al. 2017 Nuclear Materials and Energy 12 111
[8] Pitts R A, Bonnin X, Escourbiac F, et al. 2019 Nuclear Materials and Energy 20 100696
[9] Li L, Zhang D H, Meng X C, et al. 2021 Nuclear Materials and Energy 28 101049
[10] Li K, Lin X, Yang Z, et al. 2023 Nuclear Fusion 63 026025
[11] Lunsford R, Rohde V, Bortolon A, et al. 2019 Nuclear Fusion 59 126034
[12] Kawate T, Ashikawa N, Goto M, et al. 2022 Nuclear Fusion 62 126052
[13] Gilson E P, Lee H H, Bortolon A, et al. 2021 Nuclear Materials and Energy 28 101043
[14] Bodner G, Gallo A, Diallo A, et al. 2022 Nuclear Fusion 62 086020
[15] Effenberg F, Bortolon A, Casali L, et al. 2022 Nuclear Fusion 62 106015
[16] Sun Z, Diallo A, Maingi R, et al. 2021 Nuclear Fusion 61 014002
[17] Maingi R, Hu J S, Sun Z, et al. 2020 Journal of Fusion Energy 39 429
[18] Stangeby P C 2000 The Plasma Boundary of Magnetic Fusion Devices (Boca Raton)
[19] Schneider R, Bonnin X, Borrass K, et al. 2006 Contributions to Plasma Physics 46 3
[20] Chankin A V, Coster D P, Dux R, et al. 2006 Plasma Physics and Controlled Fusion 48 839
[21] Bonnin X, Dekeyser W, Pitts R, et al. 2016 Plasma and Fusion Research 11 1403102
[22] Xu W, Hu J S, Sun Z, et al. 2021 Physica Scripta 96 124034
[23] Wang R, Yang Z, Li K, et al. 2022 Physics of Plasmas 29 112502
[24] Sun Z, Maingi R, Hu J S, et al. 2019 Nuclear Materials and Energy 19 124
[25] Jia G, Wang H, Xu G, et al. 2022 Nuclear Fusion 62 056005
[26] Ma X, Wang H Q, Guo H Y, et al. 2021 Nuclear Fusion 61 054002
[27] Xu J C, Wang L, Wang H Q, et al. 2021 Nuclear Fusion 61 096004
[28] Paradela Pérez I, Groth M, Wischmeier M, et al. 2019 Nuclear Materials and Energy 19 531
[29] Park J S, Bonnin X, Pitts R, et al. 2024 Nuclear Fusion 64 036002
[30] Tokar M Z 2008 Fusion Science and Technology 53 243
[31] OPEN-ADAS, https://open.adas.ac.uk/
[32] Xu G S, Yuan Q P, Li K D, et al. 2020 Nuclear Fusion 60 086001
[33] Groth M, Andrew P, Fundamenski W, et al. 2002 Nuclear Fusion 42 591
[34] Chrobak C P, Stangeby P C, Hollmann E, et al. 2018 Nuclear Fusion 58 106019
[1] Quasi-plastic deformation mechanisms and inverse Hall-Petch relationship in nanocrystalline boron carbide under compression
Zhen Yue(岳珍), Jun Li(李君), Lisheng Liu(刘立胜), and Hai Mei(梅海). Chin. Phys. B, 2024, 33(8): 086105.
[2] Stability and melting behavior of boron phosphide under high pressure
Wenjia Liang(梁文嘉), Xiaojun Xiang(向晓君), Qian Li(李倩), Hao Liang(梁浩), and Fang Peng(彭放). Chin. Phys. B, 2024, 33(4): 046201.
[3] Numerical studies for plasmas of a linear plasma device HIT-PSI with geometry modified SOLPS-ITER
Min Wang(王敏), Qiuyue Nie(聂秋月), Tao Huang(黄韬), Xiaogang Wang(王晓钢), and Yanjie Zhang(张彦杰). Chin. Phys. B, 2024, 33(3): 035204.
[4] Quantum-mechanical understanding on structure dependence of image potentials of single-walled boron nitride nanotubes
Yu Zhang(张煜), Zhiman Zhang(张芷蔓), Weiliang Wang(王伟良), Shaolin Zhang(张绍林), and Haiming Huang(黄海鸣). Chin. Phys. B, 2024, 33(12): 128501.
[5] Recension of boron nitride phase diagram based on high-pressure and high-temperature experiments
Ruike Zhang(张瑞柯), Ruiang Guo(郭睿昂), Qian Li(李倩), Shuaiqi Li(李帅琦), Haidong Long(龙海东), and Duanwei He(贺端威). Chin. Phys. B, 2024, 33(10): 108103.
[6] Unveiling phonon frequency-dependent mechanism of heat transport across stacking fault in silicon carbide
Fu Wang(王甫), Yandong Sun(孙彦东), Yu Zou(邹宇), Ben Xu(徐贲), and Baoqin Fu(付宝勤). Chin. Phys. B, 2023, 32(9): 096301.
[7] Diamond/c-BN van der Waals heterostructure with modulated electronic structures
Su-Na Jia(贾素娜), Gao-Xian Li(李高贤), Nan Gao(高楠), Shao-Heng Cheng(成绍恒), and Hong-Dong Li(李红东). Chin. Phys. B, 2023, 32(7): 077301.
[8] Thermal transport properties of two-dimensional boron dichalcogenides from a first-principles and machine learning approach
Zhanjun Qiu(邱占均), Yanxiao Hu(胡晏箫), Ding Li(李顶), Tao Hu(胡涛), Hong Xiao(肖红),Chunbao Feng(冯春宝), and Dengfeng Li(李登峰). Chin. Phys. B, 2023, 32(5): 054402.
[9] Suppression and compensation effect of oxygen on the behavior of heavily boron-doped diamond films
Li-Cai Hao(郝礼才), Zi-Ang Chen(陈子昂), Dong-Yang Liu(刘东阳), Wei-Kang Zhao(赵伟康),Ming Zhang(张鸣), Kun Tang(汤琨), Shun-Ming Zhu(朱顺明), Jian-Dong Ye(叶建东),Rong Zhang(张荣), You-Dou Zheng(郑有炓), and Shu-Lin Gu(顾书林). Chin. Phys. B, 2023, 32(3): 038101.
[10] Direct observation of the distribution of impurity in phosphorous/boron co-doped Si nanocrystals
Dongke Li(李东珂), Junnan Han(韩俊楠), Teng Sun(孙腾), Jiaming Chen(陈佳明), Etienne Talbot, Rémi Demoulin, Wanghua Chen(陈王华), Xiaodong Pi(皮孝东), Jun Xu(徐骏), and Kunji Chen(陈坤基). Chin. Phys. B, 2023, 32(12): 126102.
[11] Effects of oxygen/nitrogen co-incorporation on regulation of growth and properties of boron-doped diamond films
Dong-Yang Liu(刘东阳), Kun Tang(汤琨), Shun-Ming Zhu(朱顺明), Rong Zhang(张荣), You-Dou Zheng(郑有炓), and Shu-Lin Gu(顾书林). Chin. Phys. B, 2023, 32(11): 118102.
[12] Improving efficiency of n-i-p perovskite solar cells enabled by 3-carboxyphenylboronic acid additive
Bin-Jie Li(李斌杰), Jia-Wen Li(李嘉文), Gen-Jie Yang(杨根杰), Meng-Ge Wu(吴梦鸽), and Jun-Sheng Yu(于军胜). Chin. Phys. B, 2023, 32(10): 107801.
[13] Determination of band alignment between GaOx and boron doped diamond for a selective-area-doped termination structure
Qi-Liang Wang(王启亮), Shi-Yang Fu(付诗洋), Si-Han He(何思翰), Hai-Bo Zhang(张海波),Shao-Heng Cheng(成绍恒), Liu-An Li(李柳暗), and Hong-Dong Li(李红东). Chin. Phys. B, 2022, 31(8): 088104.
[14] Experimental investigation on divertor tungsten sputtering with neon seeding in ELMy H-mode plasma in EAST tokamak
Dawei Ye(叶大为), Fang Ding(丁芳), Kedong Li(李克栋), Zhenhua Hu(胡振华), Ling Zhang(张凌), Xiahua Chen(陈夏华), Qing Zhang(张青), Pingan Zhao(赵平安), Tao He(贺涛), Lingyi Meng(孟令义), Kaixuan Ye(叶凯萱), Fubin Zhong(钟富彬), Yanmin Duan(段艳敏), Rui Ding(丁锐), Liang Wang(王亮), Guosheng Xu(徐国盛), Guangnan Luo(罗广南), and EAST team. Chin. Phys. B, 2022, 31(6): 065201.
[15] Accurate prediction of the critical heat flux for pool boiling on the heater substrate
Fengxun Hai(海丰勋), Wei Zhu(祝薇), Xiaoyi Yang(杨晓奕), and Yuan Deng(邓元). Chin. Phys. B, 2022, 31(6): 064401.
No Suggested Reading articles found!