Dynamics of Low-Intermediate-High-Confinement Transitions in Toroidal Plasmas

被引:113
作者
Cheng, J. [1 ]
Dong, J. Q. [1 ,2 ]
Itoh, K. [3 ]
Yan, L. W. [1 ]
Xu, M. [1 ]
Zhao, K. J. [1 ,4 ]
Hong, W. Y. [1 ]
Huang, Z. H. [1 ]
Ji, X. Q. [1 ]
Zhong, W. L. [1 ]
Yu, D. L. [1 ]
Itoh, S. -I. [5 ]
Nie, L. [1 ,6 ]
Kong, D. F. [6 ]
Lan, T. [6 ]
Liu, A. D. [6 ]
Zou, X. L. [7 ]
Yang, Q. W. [1 ]
Ding, X. T. [1 ]
Duan, X. R. [1 ]
Liu, Yong [1 ]
机构
[1] Southwestern Inst Phys, Chengdu 610041, Peoples R China
[2] Zhejiang Univ, Inst Fus Theory & Simulat, Hangzhou 310027, Peoples R China
[3] Natl Inst Nat Sci, Natl Inst Fus Sci, Toki, Gifu 5095292, Japan
[4] Natl Fus Res Inst, WCI Ctr Fus Theory, Taejon 305333, South Korea
[5] Kyushu Univ, Appl Mech Res Inst, Fukuoka 8168580, Japan
[6] USTC, Dept Modern Phys, Hefei 230026, Peoples R China
[7] CEA, IRFM, F-13108 St Paul Les Durance, France
关键词
H-MODE TRANSITION; TOKAMAK; BEHAVIOR;
D O I
10.1103/PhysRevLett.110.265002
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The dynamic features of the low-intermediate-high-(L-I-H) confinement transitions on HL-2A tokamak are presented. Here we report the discovery of two types of limit cycles (dubbed type-Y and type-J), which show opposite temporal ordering between the radial electric field and turbulence intensity. In type-Y, which appears first after an L-I transition, the turbulence grows first, followed by the localized electric field. In contrast, the electric field leads type-J. The turbulence-induced zonal flow and pressure-gradient-induced drift play essential roles in the two types of limit cycles, respectively. The condition of transition between types-Y and -J is studied in terms of the normalized radial electric field. An I-H transition is demonstrated to occur only from type-J.
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页数:5
相关论文
共 18 条
[1]   Slow L-H transitions in DIII-D plasmas -: art. no. 255002 [J].
Colchin, RJ ;
Schaffer, MJ ;
Carreras, BA ;
McKee, GR ;
Maingi, R ;
Carlstrom, TN ;
Rudakov, DL ;
Greenfield, CM ;
Rhodes, TL ;
Doyle, EJ ;
Brooks, NH ;
Austin, ME .
PHYSICAL REVIEW LETTERS, 2002, 88 (25) :255002-255002
[2]   Mean and Oscillating Plasma Flows and Turbulence Interactions across the L-H Confinement Transition [J].
Conway, G. D. ;
Angioni, C. ;
Ryter, F. ;
Sauter, P. ;
Vicente, J. .
PHYSICAL REVIEW LETTERS, 2011, 106 (06)
[3]   Spatiotemporal Structure of the Interaction between Turbulence and Flows at the L-H Transition in a Toroidal Plasma [J].
Estrada, T. ;
Hidalgo, C. ;
Happel, T. ;
Diamond, P. H. .
PHYSICAL REVIEW LETTERS, 2011, 107 (24)
[4]   H mode transition threshold power scaling and its relation to the edge neutrals in JT-60U [J].
Fukuda, T ;
Takizuka, T ;
Tsuchiya, K ;
Kamada, Y ;
Nagashima, K ;
Sato, M ;
Takenaga, H ;
Ishida, S ;
Konoshima, S ;
Higashijima, S ;
Tobita, K ;
Kikuchi, M ;
Mori, M .
NUCLEAR FUSION, 1997, 37 (09) :1199-1213
[5]   Temporal behaviour of the potential and fluctuations at the L-H transition on JFT-2M [J].
Ido, T ;
Kamiya, K ;
Miura, Y ;
Hamada, Y ;
Nishizawa, A ;
Kawasumi, Y .
PLASMA PHYSICS AND CONTROLLED FUSION, 2000, 42 :A309-A315
[6]   EDGE LOCALIZED MODE ACTIVITY AS A LIMIT-CYCLE IN TOKAMAK PLASMAS [J].
ITOH, SI ;
ITOH, K ;
FUKUYAMA, A ;
MIURA, Y .
PHYSICAL REVIEW LETTERS, 1991, 67 (18) :2485-2488
[7]   MODEL OF L-MODE TO H-MODE TRANSITION IN TOKAMAK [J].
ITOH, SI ;
ITOH, K .
PHYSICAL REVIEW LETTERS, 1988, 60 (22) :2276-2279
[8]   Experimental investigations on the role of E x B flow shear in improved confinement [J].
Jachmich, S ;
Van Oost, G ;
Weynants, RR ;
Boedo, JA .
PLASMA PHYSICS AND CONTROLLED FUSION, 1998, 40 (06) :1105-1113
[9]   Zonal flows and transient dynamics of the L-H transition -: art. no. 185006 [J].
Kim, EJ ;
Diamond, PH .
PHYSICAL REVIEW LETTERS, 2003, 90 (18) :4
[10]   BI-SPECTRUM AND NON-LINEAR WAVE COUPLING [J].
KIM, YC ;
BEALL, JM ;
POWERS, EJ ;
MIKSAD, RW .
PHYSICS OF FLUIDS, 1980, 23 (02) :258-263