Achievement of Reactor-Relevant Performance in Negative Triangularity Shape in the DIII-D Tokamak

被引:148
作者
Austin, M. E. [1 ]
Marinoni, A. [2 ]
Walker, M. L. [3 ]
Brookman, M. W. [3 ]
deGrassie, J. S. [3 ]
Hyatt, A. W. [3 ]
McKee, G. R. [4 ]
Petty, C. C. [3 ]
Rhodes, T. L. [5 ]
Smith, S. P. [3 ]
Sung, C. [6 ]
Thome, K. E. [3 ]
Turnbull, A. D. [3 ]
机构
[1] Univ Texas Austin, Austin, TX 78712 USA
[2] MIT, Plasma Sci & Fus Ctr, 77 Massachusetts Ave, Cambridge, MA 02139 USA
[3] Gen Atom, San Diego, CA 92186 USA
[4] Univ Wisconsin, Madison, WI 53706 USA
[5] Univ Calif Los Angeles, Los Angeles, CA 90095 USA
[6] Lam Res Corp, Fremont, CA 94538 USA
关键词
PLASMAS; LIMITS;
D O I
10.1103/PhysRevLett.122.115001
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Plasma discharges with a negative triangularity (delta = -0.4) shape have been created in the DIII-D tokamak with a significant normalized beta (beta(N) = 2.7) and confinement characteristic of the high confinement mode (H-98y2 = 1.2) despite the absence of an edge pressure pedestal and no edge localized modes (ELMs). These inner-wall-limited plasmas have a similar global performance as a positive triangularity (delta = +0.4) ELMing H-mode discharge with the same plasma current, elongation and cross sectional area. For cases both of dominant electron cyclotron heating with T-e/T-i > 1 and dominant neutral beam injection heating with T-e/T-i = 1, turbulent fluctuations over radii 0.5 < rho < 0.9 were reduced by 10-50% in the negative triangularity shape compared to the matching positive triangularity shape, depending on the radius and conditions.
引用
收藏
页数:5
相关论文
共 24 条
[1]   Role of Plasma Elongation on Turbulent Transport in Magnetically Confined Plasmas [J].
Angelino, P. ;
Garbet, X. ;
Villard, L. ;
Bottino, A. ;
Jolliet, S. ;
Ghendrih, Ph. ;
Grandgirard, V. ;
McMillan, B. F. ;
Sarazin, Y. ;
Dif-Pradalier, G. ;
Tran, T. M. .
PHYSICAL REVIEW LETTERS, 2009, 102 (19)
[2]  
[Anonymous], NUCL FUSION
[3]   GATO - AN MHD STABILITY CODE FOR AXISYMMETRIC PLASMAS WITH INTERNAL SEPARATRICES [J].
BERNARD, LC ;
HELTON, FJ ;
MOORE, RW .
COMPUTER PHYSICS COMMUNICATIONS, 1981, 24 (3-4) :377-380
[4]   Discovery of stationary operation of quiescent H-mode plasmas with net-zero neutral beam injection torque and high energy confinement on DIII-D [J].
Burrell, K. H. ;
Barada, K. ;
Chen, X. ;
Garofalo, A. M. ;
Groebner, R. J. ;
Muscatello, C. M. ;
Osborne, T. H. ;
Petty, C. C. ;
Rhodes, T. L. ;
Snyder, P. B. ;
Solomon, W. M. ;
Yan, Z. ;
Zeng, L. .
PHYSICS OF PLASMAS, 2016, 23 (05)
[5]   Quiescent double barrier high-confinement mode plasmas in the DIII-D tokamak [J].
Burrell, KH ;
Austin, ME ;
Brennan, DP ;
DeBoo, JC ;
Doyle, EJ ;
Fenzi, C ;
Fuchs, C ;
Gohil, P ;
Greenfield, CM ;
Groebner, RJ ;
Lao, LL ;
Luce, TC ;
Makowski, MA ;
McKee, GR ;
Moyer, RA ;
Petty, CC ;
Porkolab, M ;
Rettig, CL ;
Rhodes, TL ;
Rost, JC ;
Stallard, BW ;
Strait, EJ ;
Synakowski, EJ ;
Wade, MR ;
Watkins, JG ;
West, WP .
PHYSICS OF PLASMAS, 2001, 8 (05) :2153-2162
[6]   Impact of plasma triangularity and collisionality on electron heat transport in TCV L-mode plasmas [J].
Camenen, Y. ;
Pochelon, A. ;
Behn, R. ;
Bottino, A. ;
Bortolon, A. ;
Coda, S. ;
Karpushov, A. ;
Sauter, O. ;
Zhuang, G. .
NUCLEAR FUSION, 2007, 47 (07) :510-516
[7]   A high-accuracy Euleriangyrokinetic solver for collisional plasmas [J].
Candy, J. ;
Belli, E. A. ;
Bravenec, R. V. .
JOURNAL OF COMPUTATIONAL PHYSICS, 2016, 324 :73-93
[8]   Localized measurement of short wavelength plasma fluctuations with the DIII-D phase contrast imaging diagnostic [J].
Dorris, J. R. ;
Rost, J. C. ;
Porkolab, M. .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2009, 80 (02)
[9]   Dependence of the L-Mode scrape-off layer power fall-off length on the upper triangularity in TCV [J].
Faitsch, M. ;
Maurizio, R. ;
Gallo, A. ;
Coda, S. ;
Eich, T. ;
Labit, B. ;
Merle, A. ;
Reimerdes, H. ;
Sieglin, B. ;
Theiler, C. .
PLASMA PHYSICS AND CONTROLLED FUSION, 2018, 60 (04)
[10]   The effect of triangularity on fluctuations in a tokamak plasma [J].
Fontana, M. ;
Porte, L. ;
Coda, S. ;
Sauter, O. .
NUCLEAR FUSION, 2018, 58 (02)