Second stable regime of internal kink modes excited by barely passing energetic ions in tokamak plasmas

2010 ◽  
Vol 17 (8) ◽  
pp. 082512 ◽  
Author(s):  
H. D. He ◽  
J. Q. Dong ◽  
G. Y. Fu ◽  
G. Y. Zheng ◽  
Z. M. Sheng ◽  
...  
2015 ◽  
Vol 22 (9) ◽  
pp. 092510 ◽  
Author(s):  
Guo Meng ◽  
Xian-Qu Wang ◽  
Xiaogang Wang ◽  
Rui-Bin Zhang

2021 ◽  
Author(s):  
Hanzheng Li ◽  
Y Todo ◽  
Hao Wang ◽  
Malik Idouakass ◽  
Jialei Wang

Abstract Kinetic-magnetohydrodynamic hybrid simulations were performed to investigate the linear growth and the nonlinear evolution of off-axis fishbone mode (OFM) destabilized by trapped energetic ions in tokamak plasmas. The spatial profile of OFM is mainly composed of m/n = 2/1 mode inside the q = 2 magnetic flux surface while the m/n = 3/1 mode is predominant outside the q = 2 surface, where m and n are the poloidal and toroidal mode numbers, respectively, and q is the safety factor. The spatial profile of the OFM is a strongly shearing shape on the poloidal plane, suggesting the nonperturbative effect of the interaction with energetic ions. The frequency of the OFM in the linear growth phase is in good agreement with the precession drift frequency of trapped energetic ions, and the frequency chirps down in the nonlinear phase. Two types of resonance conditions between trapped energetic ions and OFM are found. For the first type of resonance, the precession drift frequency matches the OFM frequency, while for the second type, the sum of the precession drift frequency and the bounce frequency matches the OFM frequency. The first type of resonance is the primary resonance for the destabilization of OFM. The resonance frequency which is defined based on precession drift frequency and bounce frequency of the nonlinear orbit for each resonant particle is analyzed to understand the frequency chirping. The resonance frequency of the particles that transfer energy to the OFM chirps down, which may result in the chirping down of the OFM frequency. A detailed analysis of the energetic ion distribution function in phase space shows that the gradient of the distribution function along the E′ = const. line drives or stabilizes the instability, where E′ is a combination of energy and toroidal canonical momentum and conserved during the wave-particle interaction. The distribution function is flattened along the E′ = const. line in the nonlinear phase leading to the saturation of the instability.


2017 ◽  
Vol 57 (5) ◽  
pp. 056013
Author(s):  
Feng Wang ◽  
L.M. Yu ◽  
G.Y. Fu ◽  
Wei Shen

Author(s):  
R R Ma ◽  
Liu Chen ◽  
Fulvio Zonca ◽  
Yueyan Li ◽  
Zhiyong Qiu

Abstract Linear wave properties of the low-frequency Alfvén modes (LFAMs) observed in the DIII-D tokamak experiments with reversed magnetic shear [Nucl. Fusion 61, 016029 (2021)] are theoretically studied and delineated based on the general fishbone-like dispersion relation. By adopting the representative experimental equilibrium parameters, it is found that, in the absence of energetic ions, the LFAM is a kinetic ballooning mode instability of reactive-type with a dominant Alfvénic polarization. More specifically, due to diamagnetic and trapped particle effects, the LFAM can be coupled with the beta-induced Alfvén-acoustic mode in the low-frequency region (frequency much less than the thermal-ion transit and/or bounce frequency); or with the beta-induced Alfvén eigenmode in the high frequency region (frequency higher than or comparable to the thermal-ion transit frequency); resulting in reactive-type instabilities. Moreover, the ‘Christmas light’ and ‘mountain peak’ spectral patterns of LFAMs as well as the dependence of instability drive on the electron temperature observed in the experiments can be theoretically interpreted by varying the relevant physical parameters. Conditions when dissipative-type instabilities may set in are also discussed.


2018 ◽  
Vol 58 (12) ◽  
pp. 126023
Author(s):  
Hongda He ◽  
Junyi Cheng ◽  
J.Q. Dong ◽  
Wenlu Zhang ◽  
Chenxi Zhang ◽  
...  

2012 ◽  
Vol 3 (1) ◽  
Author(s):  
J.P. Graves ◽  
I.T. Chapman ◽  
S. Coda ◽  
M. Lennholm ◽  
M. Albergante ◽  
...  

2014 ◽  
Vol 21 (6) ◽  
pp. 062509 ◽  
Author(s):  
Hongda He ◽  
J. Q. Dong ◽  
K. Zhao ◽  
Zhixiong He ◽  
G. Y. Zheng ◽  
...  

2017 ◽  
Vol 57 (11) ◽  
pp. 114005
Author(s):  
Erzhong Li ◽  
L. Hu ◽  
H. Zhao ◽  
T. Shi ◽  
Y. Liu ◽  
...  

Author(s):  
Xiaolong Zhu ◽  
Feng Wang ◽  
Wei Chen ◽  
Zhengxiong Wang

Abstract Based on the conventional tokamak HL-2A-like parameters and profiles, the linear properties and the nonlinear dynamics of non-resonant kink mode (NRK) and non-resonant fishbone instability (NRFB) in reversed shear tokamak plasmas are investigated by using the global hybrid kinetic-magnetohydrodynamic (MHD) nonlinear code M3D-K. This work mainly focuses on the effect of passing energetic-ions on the NRK and NRFB instabilities, which is different from the previous works. It is demonstrated that the NRFB can be destabilized by the passing energetic-ions when the energetic-ion beta $\beta_h$ exceeds a critical value. The transition from NRK to NRFB occurs when the energetic-ion beta $\beta_h$ increases to above a critical value. The resonance condition responsible for the excitation of NRFB is interestingly found to be satisfied at $\omega_t+\omega_p\approx\omega$, where $\omega_t$ is the toroidal motion frequency, $\omega_p$ is the poloidal motion frequency and $\omega$ is the mode frequency. The nonlinear evolutions of NRFB's mode structures and Poincar\'{e} plots are also analyzed in this work and it is found that the NRFB can induce evident energetic-ion loss/redistribution, which can degrade the performance of the plasmas. These findings are conducive to understanding the mechanisms of NRFB-induced energetic-ion loss/redistribution through nonlinear wave-particle interaction.


2014 ◽  
Vol 134 (9) ◽  
pp. 523-524
Author(s):  
Hideya Koike ◽  
Masanobu Annoura ◽  
Kento Nishida ◽  
Hiroshi Tanabe ◽  
Michiaki Inomoto ◽  
...  

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