Dynamic characteristics of edge plasma profiles during the opening of edge islands on the J-TEXT tokamak

J. Yang; Y. Liang; P. Shi; N.C. Wang; S. Zhou; Z.P. Chen; Z.H. Jiang; F.Y. Mao; Q.H. Yang; J.K. Hua; D. Li; Z.Y. Chen; Y.H. Ding; P. Drews; A. Knieps; E. Wang; S. Xu; H.M. Xiang; J.Q. Cai; J. Huang; Y.C. Gao; J.W. Liu; Y. Luo; L. Liao; the J-TEXT team

doi:10.1088/1741-4326/ad37cc

Nuclear Fusion (Jan 2024)

Dynamic characteristics of edge plasma profiles during the opening of edge islands on the J-TEXT tokamak

J. Yang,
Y. Liang,
P. Shi,
N.C. Wang,
S. Zhou,
Z.P. Chen,
Z.H. Jiang,
F.Y. Mao,
Q.H. Yang,
J.K. Hua,
D. Li,
Z.Y. Chen,
Y.H. Ding,
P. Drews,
A. Knieps,
E. Wang,
S. Xu,
H.M. Xiang,
J.Q. Cai,
J. Huang,
Y.C. Gao,
J.W. Liu,
Y. Luo,
L. Liao,
the J-TEXT team

Affiliations

J. Yang: State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China; Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
Y. Liang: ORCiD; State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China; Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
P. Shi: United Kingdom Atomic Energy Authority, Culham Centre for Fusion Energy, Culham Science Centre , Abingdon, Oxon OX14 3 DB, United Kingdom of Great Britain and Northern Ireland
N.C. Wang: ORCiD; State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
S. Zhou: ORCiD; State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
Z.P. Chen: ORCiD; State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
Z.H. Jiang: ORCiD; State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
F.Y. Mao: State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
Q.H. Yang: State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
J.K. Hua: State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
D. Li: State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
Z.Y. Chen: ORCiD; State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
Y.H. Ding: State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China
P. Drews: ORCiD; Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
A. Knieps: ORCiD; Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
E. Wang: Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
S. Xu: ORCiD; Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
H.M. Xiang: Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
J.Q. Cai: Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
J. Huang: Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
Y.C. Gao: Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
J.W. Liu: ORCiD; Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
Y. Luo: Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany
L. Liao: Forschungszentrum Jülich GmbH, Institut für Energie- und Klimaforschung—Plasmaphysik, Partner of the Trilateral Euregio Cluster (TEC) , 52425 Jülich, Germany; Institute of Plasma Physics, Chinese Academy of Sciences , Hefei 230031, China
the J-TEXT team: State Key Laboratory of Advanced Electromagnetic Engineering and Technology, International Joint Research Laboratory of Magnetic Confinement Fusion and Plasma Physics, School of Electrical and Electronic Engineering, Huazhong University of Science and Technology , Wuhan 430074, China

DOI: https://doi.org/10.1088/1741-4326/ad37cc
Journal volume & issue: Vol. 64, no. 5
p. 056030

Abstract

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On the J-TEXT tokamak, the dynamics of edge magnetic topology during the opening of the edge magnetic islands induced by the external Resonant Magnetic Perturbation (RMP) are investigated. The edge island chain is pushed outward by increasing plasma toroidal current to intersect the poloidally and toroidally localized divertor plate, forming an open magnetic island in the Scrape-Off Layer (SOL). The location of the strike points on the divertor plate predicted by the HINT code is in agreement with the experimental observations. The influence of the magnetic topology on edge plasma profiles has also been investigated using Langmuir probes. The properties of edge ${T_{\text{e}}}$ , ${n_{\text{e}}}$ , ${P_{\text{e}}}$ and ${E_{\text{r}}}$ profiles are studied as function of three magnetic structures in ${q_{\text{a}}}$ -dependence experiments and two magnetic structures in RMP configuration-dependence experiments. Some common features are observed. Inside the edge closed and SOL remnant islands, flat ${P_{\text{e}}}$ but non-flat ${T_{\text{e}}}$ and ${n_{\text{e}}}$ profiles are detected. When transitioning from the edge closed island to the partially open island with remnant island, the local flat ${P_{\text{e}}}$ profile is shifted outward accompanied by a narrower flattened ${P_{\text{e}}}$ region. The steep slopes of ${T_{\text{e}}}$ , ${n_{\text{e}}}$ and ${P_{\text{e}}}$ are measured in the SOL regions characterized by a long connection length ${L_{\text{c}}}$ , and the longer ${L_{\text{c}}}$ , the steeper slopes. ${E_{\text{r}}}$ exhibits a negative well inside the remnant island with infinite ${L_{\text{c}}}$ and in the SOL regions where ${L_{\text{c}}}$ significantly exceeds than the electron mean free path ${\lambda _{\text{e}}}$ , but develops a positive value in the SOL regions where ${L_{\text{c}}}$ is relatively short.

Published in Nuclear Fusion

ISSN: 0029-5515 (Print); 1741-4326 (Online)
Publisher: IOP Publishing
Country of publisher: United Kingdom
LCC subjects: Science: Physics: Nuclear and particle physics. Atomic energy. Radioactivity
Website: https://iopscience.iop.org/journal/0029-5515

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