Discovery of stationary operation of quiescent H-mode plasmas with net-zero neutral beam injection torque and high energy confinement on DIII-D

被引:65
作者
Burrell, K. H. [1 ]
Barada, K. [2 ]
Chen, X. [1 ]
Garofalo, A. M. [1 ]
Groebner, R. J. [1 ]
Muscatello, C. M. [1 ]
Osborne, T. H. [1 ]
Petty, C. C. [1 ]
Rhodes, T. L. [2 ]
Snyder, P. B. [1 ]
Solomon, W. M. [3 ]
Yan, Z. [4 ]
Zeng, L. [2 ]
机构
[1] Gen Atom Co, POB 85608, San Diego, CA 92186 USA
[2] Univ Calif Los Angeles, Los Angeles, CA 90024 USA
[3] Princeton Plasma Phys Lab, POB 451, Princeton, NJ 08543 USA
[4] Univ Wisconsin, Madison, WI 53706 USA
关键词
PEDESTAL PROFILES; ASDEX UPGRADE; STABILITY; ROTATION; REGIME; ELMS;
D O I
10.1063/1.4943521
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
Recent experiments in DIII-D [J. L. Luxon et al., in Plasma Physics and Controlled Nuclear Fusion Research 1996 (International Atomic Energy Agency, Vienna, 1987), Vol. I, p. 159] have led to the discovery of a means of modifying edge turbulence to achieve stationary, high confinement operation without Edge Localized Mode (ELM) instabilities and with no net external torque input. Eliminating the ELM-induced heat bursts and controlling plasma stability at low rotation represent two of the great challenges for fusion energy. By exploiting edge turbulence in a novel manner, we achieved excellent tokamak performance, well above the H98y2 international tokamak energy confinement scaling (H-98y2 = 1.25), thus meeting an additional confinement challenge that is usually difficult at low torque. The new regime is triggered in double null plasmas by ramping the injected torque to zero and then maintaining it there. This lowers E x B rotation shear in the plasma edge, allowing low-k, broadband, electromagnetic turbulence to increase. In the H-mode edge, a narrow transport barrier usually grows until MHD instability (a peeling ballooning mode) leads to the ELM heat burst. However, the increased turbulence reduces the pressure gradient, allowing the development of a broader and thus higher transport barrier. A 60% increase in pedestal pressure and 40% increase in energy confinement result. An increase in the E x B shearing rate inside of the edge pedestal is a key factor in the confinement increase. Strong double-null plasma shaping raises the threshold for the ELM instability, allowing the plasma to reach a transportlimited state near but below the explosive ELM stability boundary. The resulting plasmas have burning-plasma-relevant beta(N) = 1.6-1.8 and run without the need for extra torque from 3D magnetic fields. To date, stationary conditions have been produced for 2 s or 12 energy confinement times, limited only by external hardware constraints. Stationary operation with improved pedestal conditions is highly significant for future burning plasma devices, since operation without ELMs at low rotation and good confinement is key for fusion energy production. (C) 2016 AIP Publishing LLC.
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页数:11
相关论文
共 35 条
  • [11] Garofalo A. M., 2012, P 39 EUR PHYS SOC C
  • [12] Impurity confinement and transport in high confinement regimes without edge localized modes on DIII-D
    Grierson, B. A.
    Burrell, K. H.
    Nazikian, R. M.
    Solomon, W. M.
    Garofalo, A. M.
    Belli, E. A.
    Staebler, G. M.
    Fenstermacher, M. E.
    McKee, G. R.
    Evans, T. E.
    Orlov, D. M.
    Smith, S. P.
    Chrobak, C.
    Chrystal, C.
    [J]. PHYSICS OF PLASMAS, 2015, 22 (05)
  • [13] Response of impurity particle confinement time to external actuators in QH-mode plasmas on DIII-D
    Grierson, B. A.
    Burrell, K. H.
    Garofalo, A. M.
    Solomon, W. M.
    Diallo, A.
    O'Mullane, M.
    [J]. NUCLEAR FUSION, 2014, 54 (11)
  • [14] FLOW SHEAR-INDUCED FLUCTUATION SUPPRESSION IN FINITE ASPECT RATIO SHAPED TOKAMAK PLASMA
    HAHM, TS
    BURRELL, KH
    [J]. PHYSICS OF PLASMAS, 1995, 2 (05) : 1648 - 1651
  • [15] New Steady-State Quiescent High-Confinement Plasma in an Experimental Advanced Superconducting Tokamak
    Hu, J. S.
    Sun, Z.
    Guo, H. Y.
    Li, J. G.
    Wan, B. N.
    Wang, H. Q.
    Ding, S. Y.
    Xu, G. S.
    Liang, Y. F.
    Mansfield, D. K.
    Maingi, R.
    Zou, X. L.
    Wang, L.
    Ren, J.
    Zuo, G. Z.
    Zhang, L.
    Duan, Y. M.
    Shi, T. H.
    Hu, L. Q.
    [J]. PHYSICAL REVIEW LETTERS, 2015, 114 (05)
  • [16] Pedestal profiles and fluctuations in C-Mod enhanced D-alpha H-modes
    Hubbard, AE
    Boivin, RL
    Granetz, RS
    Greenwald, M
    Hughes, JW
    Hutchinson, IH
    Irby, J
    LaBombard, B
    Lin, Y
    Marmar, ES
    Mazurenko, A
    Mossessian, D
    Nelson-Melby, E
    Porkolab, M
    Snipes, JA
    Terry, J
    Wolfe, S
    Wukitch, S
    Carreras, BA
    Klein, V
    Pedersen, TS
    [J]. PHYSICS OF PLASMAS, 2001, 8 (05) : 2033 - 2040
  • [17] Luxon J. L., 1987, PLASMA PHYS CONTROLL, VI, P159
  • [18] Turbulence velocimetry of density fluctuation imaging data
    McKee, GR
    Fonck, RJ
    Gupta, DK
    Schlossberg, DJ
    Shafer, MW
    Holland, C
    Tynan, G
    [J]. REVIEW OF SCIENTIFIC INSTRUMENTS, 2004, 75 (10) : 3490 - 3492
  • [19] Enhanced H-mode pedestals with lithium injection in DIII-D
    Osborne, T. H.
    Jackson, G. L.
    Yan, Z.
    Maingi, R.
    Mansfield, D. K.
    Grierson, B. A.
    Chrobak, C. P.
    McLean, A. G.
    Allen, S. L.
    Battaglia, D. J.
    Briesemeister, A. R.
    Fenstermacher, M. E.
    McKee, G. R.
    Snyder, P. B.
    [J]. NUCLEAR FUSION, 2015, 55 (06)
  • [20] Edge stability of stationary ELM-suppressed regimes on DIII-D
    Osborne, T. H.
    Snyder, P. B.
    Burrell, K. H.
    Evans, T. E.
    Fenstermacher, M. E.
    Leonard, A. W.
    Moyer, R. A.
    Schaffer, M. J.
    West, W. P.
    [J]. 11TH IAEA TECHNICAL MEETING ON H-MODE PHYSICS AND TRANSPORT BARRIERS, 2008, 123