Comparison of MHD stability properties between QH-mode and ELMy H-mode plasmas by considering plasma rotation and ion diamagnetic drift effects

被引:4
作者
Aiba, N. [1 ]
Chen, X. [2 ]
Osborne, T. H. [2 ]
Burrell, K. H. [2 ]
机构
[1] Natl Inst Quantum Sci & Technol, Naka Ku, Ibaraki 3110193, Japan
[2] Gen Atom, POB 85608, San Diego, CA 92186 USA
关键词
quiescent H-mode; extended MHD model; linear stability; rotation; NUMERICAL-ANALYSIS; EQUILIBRIUM;
D O I
10.1088/1741-4326/acbc35
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
Magnetohydrodynamic (MHD) stability at tokamak edge pedestal in a quiescent H-mode (QH-mode) and type-I ELMy H-mode plasmas in DIII-D experiment was analyzed by considering plasma rotation and ion diamagnetic drift effects. QH-mode plasma is marginally stable to kink/peeling mode (K/PM), but ELMy H-mode one is almost unstable to peeling-ballooning mode (PBM). It was identified that there are three physics features responsible for the difference in the MHD stability properties between QH-mode plasma and ELMy H-mode one. These are the distance of pedestal foot from the last closed flux surface (LCFS), the amount of the ion diamagnetic drift frequency at pedestal, and impact of coupled rotation and ion diamagnetic drift effects. These features were confirmed through the numerical experiments that the stability properties of the QH-mode plasma can be changed to that of the ELMy H-mode one by shifting the plasma profiles inward in the radial direction and halving the ion diamagnetic drift frequency. The reasons of the change in the stability properties are thought as that K/PM is stabilized due to the inward shift of the bootstrap current profile, and PBM is destabilized due to the reduction of the coupled rotation and ion diamagnetic drift stabilizing effect. Importance of these features was validated through numerical experiments with experimental data of other QH-mode plasmas in DIII-D. All the results show that MHD stability properties of QH-mode plasma can be obtained in case that pedestal foot is close to LCFS, ion diamagnetic drift frequency is large due to high ion temperature, and strong rotation shear exists near pedestal.
引用
收藏
页数:9
相关论文
共 25 条
[1]   Stabilization of kink/peeling modes by coupled rotation and ion diamagnetic drift effects in quiescent H-mode plasmas in DIII-D and JT-60U [J].
Aiba, N. ;
Chen, X. ;
Kamiya, K. ;
Honda, M. ;
Osborne, T. H. ;
Burrell, K. H. ;
Snyder, P. B. .
NUCLEAR FUSION, 2021, 61 (12)
[2]   Impact of rotation and ion diamagnetic dxc vmrift on MHD stability at edge pedestal in quiescent H-mode plasmas [J].
Aiba, N. ;
Chen, X. ;
Osborne, T. H. ;
Honda, M. ;
Burrell, K. H. ;
Snyder, P. B. .
NUCLEAR FUSION, 2020, 60 (09)
[3]   Numerical analysis of ELM stability with rotation and ion diamagnetic drift effects in JET [J].
Aiba, N. ;
Giroud, C. ;
Honda, M. ;
Delabie, E. ;
Saarelma, S. ;
Frassinetti, L. ;
Lupelli, I. ;
Casson, F. J. ;
Pamela, S. ;
Urano, H. ;
Maggi, C. F. ;
Abduallev, S. ;
Abhangi, M. ;
Abreu, P. ;
Afzal, M. ;
Aggarwal, K. M. ;
Ahlgren, T. ;
Ahn, J. H. ;
Aho-Mantila, L. ;
Aiba, N. ;
Airila, M. ;
Albanese, R. ;
Aldred, V. ;
Alegre, D. ;
Alessi, E. ;
Aleynikov, P. ;
Alfier, A. ;
Alkseev, A. ;
Allinson, M. ;
Alper, B. ;
Alves, E. ;
Ambrosino, G. ;
Ambrosino, R. ;
Amicucci, L. ;
Amosov, V. ;
Sunden, E. Andersson ;
Angelone, M. ;
Anghel, M. ;
Angioni, C. ;
Appel, L. ;
Appelbee, C. ;
Arena, P. ;
Ariola, M. ;
Arnichand, H. ;
Arshad, S. ;
Ash, A. ;
Ashikawa, N. ;
Aslanyan, V. ;
Asunta, O. ;
Auriemma, F. .
NUCLEAR FUSION, 2017, 57 (12)
[4]   Impact of ion diamagnetic drift on MHD stability at edge pedestal in JT-60U rotating plasmas [J].
Aiba, N. ;
Honda, M. ;
Kamiya, K. .
NUCLEAR FUSION, 2017, 57 (02)
[5]   Impact of ion diamagnetic drift on ideal ballooning mode stability in rotating tokamak plasmas [J].
Aiba, N. .
PLASMA PHYSICS AND CONTROLLED FUSION, 2016, 58 (04)
[6]   Reactor-relevant quiescent H-mode operation using torque from non-axisymmetric, non-resonant magnetic fields [J].
Burrell, K. H. ;
Garofalo, A. M. ;
Solomon, W. M. ;
Fenstermacher, M. E. ;
Osborne, T. H. ;
Park, J-K ;
Schaffer, M. J. ;
Snyder, P. B. .
PHYSICS OF PLASMAS, 2012, 19 (05)
[7]   Quiescent H-Mode Plasmas with Strong Edge Rotation in the Cocurrent Direction [J].
Burrell, K. H. ;
Osborne, T. H. ;
Snyder, P. B. ;
West, W. P. ;
Fenstermacher, M. E. ;
Groebner, R. J. ;
Gohil, P. ;
Leonard, A. W. ;
Solomon, W. M. .
PHYSICAL REVIEW LETTERS, 2009, 102 (15)
[8]   Advances in understanding quiescent H-mode plasmas in DIII-D [J].
Burrell, KH ;
West, WP ;
Doyle, EJ ;
Austin, ME ;
Casper, TA ;
Gohil, P ;
Greenfield, CM ;
Groebner, RJ ;
Hyatt, AW ;
Jayakumar, RJ ;
Kaplan, DH ;
Lao, LL ;
Leonard, AW ;
Makowski, MA ;
McKee, GR ;
Osborne, TH ;
Snyder, PB ;
Solomon, WM ;
Thomas, DM ;
Rhodes, TL ;
Strait, EJ ;
Wade, MR ;
Wang, G ;
Zeng, L .
PHYSICS OF PLASMAS, 2005, 12 (05)
[9]   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
[10]   Rotational shear effects on edge harmonic oscillations in DIII-D quiescent H-mode discharges [J].
Chen, Xi ;
Burrell, K. H. ;
Ferraro, N. M. ;
Osborne, T. H. ;
Austin, M. E. ;
Garofalo, A. M. ;
Groebner, R. J. ;
Kramer, G. J. ;
Luhmann, N. C., Jr. ;
McKee, G. R. ;
Muscatello, C. M. ;
Nazikian, R. ;
Ren, X. ;
Snyder, P. B. ;
Solomon, W. M. ;
Tobias, B. J. ;
Yan, Z. .
NUCLEAR FUSION, 2016, 56 (07)