Two-dimensional study of edge impurity transport in the Large Helical Device

被引:14
|
作者
Morita, S. [1 ,2 ]
Wang, E. H. [3 ]
Kobayashi, M. [1 ,2 ]
Dong, C. F. [4 ]
Oishi, T. [1 ,2 ]
Feng, Y. [5 ]
Goto, M. [1 ,2 ]
Huang, X. L. [2 ]
Masuzaki, S. [1 ]
Murakami, I. [1 ,2 ]
Suzuki, Y. [1 ,2 ]
Watanabe, T. [1 ]
机构
[1] Natl Inst Nat Sci, Natl Inst Fus Sci, Toki, Gifu 5095292, Japan
[2] Grad Univ Adv Studies, Dept Fus Sci, Toki, Gifu 5095292, Japan
[3] Acad Sinica, Inst Plasma Phys, Hefei 230031, Anhui, Peoples R China
[4] Southwestern Inst Phys, Chengdu 610041, Sichuan, Peoples R China
[5] Max Planck Inst Plasma Phys, D-17491 Greifswald, Germany
关键词
impurity transport; stochastic magnetic field; EUV spectroscopy; DIVERTOR PHYSICS; MAGNETIC-FIELD; BOUNDARY; PLASMA;
D O I
10.1088/0741-3335/56/9/094007
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
Edge impurity transport has been studied in the stochastic magnetic field layer called the ergodic layer of the Large Helical Device. Chord-integrated full vertical profiles of C IV (312.4 angstrom: 1s(2)3p-1s(2)2s) near edge X-points are observed at horizontally elongated plasma cross sections. Measured C IV profiles are almost flat at low density (<= 2 x 10(13) cm(-3)), while two peaks called the 'X-point peak' newly begin to appear near edge separatrix X-points with increase in density in addition to ordinary edge peaks. The X-point peaks become very clear at high-density range (>= 6 x 10(13) cm(-3)). The C3+ ions analyzed with three-dimensional edge plasma transport code, EMC3-EIRENE, move upstream at low density due to large thermal force. The widely expanded C3+ distribution makes the C IV profile flat. With increasing the density, the friction force becomes dominant and the impurity ions start to move downstream. The C3+ ions stay in the vicinity of the edge X-point where magnetic field lines are very short. The X-point peaks are then clearly formed with increase in the C3+ density. Two-dimensional C IV distribution is also observed for different plasma axis positions. It is found that the C IV emission becomes strong along the poloidal trajectory of X-points and the C IV poloidal trace moves from inboard to outboard X-point trajectories when the plasma axis is changed from 3.60 to 3.75 m. The three-dimensional simulation can well reproduce the enhancement of C IV trajectory along the X-point. However, a discrepancy with the experiment is still seen in the CIV intensity between inboard and outboard X-points.
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页数:10
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