Characterization of beam ion loss in high poloidal beta regime on EAST. (1st September 2022)

• Record Type: Journal Article
• Authors: Fu, J; Huang, J; Wang, J F; Yu, L M; Van Zeeland, M A; Chang, J F; Hao, B L; Chen, J L; Wu, M Q; Hu, W H; Xu, Z; Gao, W; Gao, W; Su, J X; Sun, Y X; Liang, R R; Zang, Q; Liu, H Q; Lyu, B; Zhong, G Q; Zhang, B; Gong, X Z
• Is Part Of: Plasma physics and controlled fusion. Volume 64:Number 9(2022)
• Publication Date: 2022-09-01
• Subjects: beam ion loss -- wall load -- confinement -- high-βp -- tokamak; Plasma (Ionized gases) -- Periodicals; Controlled fusion -- Periodicals; 530.44
• DOI: 10.1088/1361-6587/ac77b7
• Languages: English
• ISSNs: 0741-3335

Abstract

Abstract: A critical issue for achieving the integrated operation of steady-state long-pulse high-confinement (H-mode) plasmas on experimental advanced superconducting tokamak (EAST) is to improve beam ion population confinement during neutral beam injection (NBI). To study the characterization of beam ion loss and improve beam ion confinement, the steady-state long pulse scenario discharges were conducted on EAST ( β p ⩾ 2.0, β N ⩾ 1.7, q 95 ⩾ 6.7 and H 98y2 ⩾ 1.1) with NBI heating. Based on neutron yield, the beam voltage and line-averaged electron density were adjusted from 50 kV to 60 kV and 4.4 × 1019 m −3 to 5.0 × 10 19 m −3, respectively. The results show that the dominant mechanisms of beam ion loss are shine-through loss, prompt loss, and stochastic ripple loss. The shine-through loss fraction is determined by initial velocity, flight time and entire beam path. The change in prompt loss fraction is caused by the change in the deposition of beam ions. The change in stochastic ripple loss fraction is caused by the change in the initial fraction of trapped-confined ions. Detailed physics shows that the prompt loss fraction during counter-Ip injections (∼45%) is far larger than during co-Ip injections (∼5%) due to the finite orbit width. The lost ions are mainly deposited on the lower divertor or below the midplane since the direction of magnetic drift is vertical down. The orbit types of prompt loss during counter-Ip injections are mainly trapped-lost and ctr-passing lost. To minimize the prompt loss fraction during counter-Ip injections, a reversed Ip configuration (rev-Ip) discharge #94758 was conducted. The result suggests that the beam ion wall load fraction during counter-Ip tangential injection (∼3%) is far lower than that in normal Ip configuration (nor-Ip) discharge #94820. It is also found that the confinement of beam ion population in the counter-Ip injection #94758 was greatly improved when compared to #94820. This study can provide unique support for the improvement of beam ion population confinement and for the performance evaluation of the NBI system on EAST and future tokamaks.