Orbit-following simulations of fast-ion transport and losses due to the Alfvén eigenmode burst in the Large Helical Device

被引:0
|
作者
Seki, R. [1 ]
Todo, Y. [1 ]
Suzuki, Y. [2 ]
Spong, D. A. [3 ]
Ogawa, K. [1 ,4 ]
Isobe, M. [1 ,4 ]
Osakabe, M. [1 ,4 ]
机构
[1] Natl Inst Fus Sci, Natl Inst Nat Sci, Toki, Gifu 5095292, Japan
[2] Hiroshima Univ, Higashihiroshima, Hiroshima 7313194, Japan
[3] Oak Ridge Natl Lab, Oak Ridge, TN 37831 USA
[4] Grad Univ Adv Studies, SOKENDAI, Toki, Gifu 5095292, Japan
关键词
ENERGETIC-PARTICLE-TRANSPORT; HYBRID SIMULATIONS; ALFVEN EIGENMODES; INSTABILITIES;
D O I
10.1063/5.0221069
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
Orbit-following simulations of fast-ion transport and losses with time-dependent electromagnetic perturbations are performed to clarify the roles of Alfv & eacute;n eigenmodes (AEs) and the low-frequency magnetohydrodynamic (MHD) mode observed in the kinetic-MHD hybrid simulation of AE bursts in the Large Helical Device. Fast-ion pressure profile flattening in the kinetic-MHD hybrid simulation can be reproduced by an orbit-following simulation with only the primary single AE of the time-dependent amplitude following the kinetic-MHD hybrid simulation result, while orbit-following simulations with constant AE amplitude of average level during AE burst cannot reproduce the fast-ion pressure profile flattening observed. The effects of other modes are negligible on the fast-ion pressure profile flattening. The fast-ion losses in kinetic-MHD hybrid simulation can be reproduced by an orbit-following simulation with time-dependent amplitude when the low-frequency MHD mode is considered in addition to multiple AEs. This indicates the synergetic effect of multiple AEs and the low-frequency MHD mode on fast-ion losses. (c) 2024 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution-NonCommercial 4.0International (CC BY-NC) license
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页数:9
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