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6–10 Dec 2021
Virtual Event
Europe/Vienna timezone
Official invitations and technical information that will enable designated participants to join the virtual event will be sent 1–2 weeks before the meeting.

Hybrid simulations of of beta-induced Alfven eigenmode with reversed safety factor profile

6 Dec 2021, 14:40
20m
Virtual Event

Virtual Event

Oral Effects of Energetic Particles in Magnetic Confinement Fusion Devices Effects of Energetic Particles in Magnetic Confinement Fusion Devices

Speaker

Sizhe Duan (University of Science and Technology of China)

Description

Based on the experimental parameters in HL-2A tokamak, the linear stability and nonlinear dynamics of BAE with reversed safety factor $q$ profile are investigated by using kinetic-MHD code M3D-K. It is found that the ($m/n=3/2$) BAE is excited by co-passing energetic ions with $q_{min}=1.5$ in linear simulation, and the mode frequency is consistent with experimental meuasurement. The simulation results show that the energetic ions $\beta_h$, the injection velocity $v_0$ and orbit width parameter $\rho_h$ of energetic ions are important parameters determining the drive on BAE. The effect of $\rho_h$ is determined by the orbital averaging, while the effect of $v_0$ is associated with the fraction of resonant ions. Furthermore, the effect of $q_{min}$ (with fixed shape of $q$ profile) is studied, and it is found that: when $q_{min} \le 1.5$, the excited modes are BAEs, which are located near $q=1.5$ rational surfaces; when $q_{min} > 1.5$, the excited modes are reversed-shear Alfven eigenmodes (RSAEs), which are localized around $q=q_{min}$ surfaces. Nonlinear simulation results show that the nonlinear dynamics of BAE depends on the EP drive. For strongly driven case, firstly, redistribution and transport of engetic ions are trigged by $3/2$ BAE, which raised the radial gradient of energetic ions distribution function near $q=2$ rational surface, and then an EPM ($m/n=4/2$) is driven in nonlinear phase. Finally, these two instabilities triggered significant redistribution of energetic ions, which results in the repetitive and mostly-downward frequency chirping of $3/2$ BAE. For weakly driven case, there are no $4/2$ EPM being driven and repetitive chirping in nonlinear phase, since the radial gradient near $q=2$ rational surface is small and almost unchanged.

Speaker's Affiliation University of Science and Technology of China, Hefei
Member State or IGO China, People’s Republic of

Primary authors

Sizhe Duan (University of Science and Technology of China) Guoyong Fu (Zhejiang University) Huishan Cai (University of Science and Technology of China)

Presentation materials

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