scholarly journals KINETIC BALLOONING MODE ANALYSIS OF TOKAMAK PLASMAS WITH THE SECOND STABILITY REGIME INCLUDED

1984 ◽  
Vol 33 (11) ◽  
pp. 1546
Author(s):  
SHI BING-REN ◽  
SUI GUO-FANG
2013 ◽  
Vol 15 (6) ◽  
pp. 499-505 ◽  
Author(s):  
Zebin Li ◽  
Guoya Sun ◽  
Ihor Holod ◽  
Yong Xiao ◽  
Wenlu Zhang ◽  
...  

2002 ◽  
Vol 80 (12) ◽  
pp. 1517-1523 ◽  
Author(s):  
A Hirose ◽  
M Elia

The existence of kinetic-ballooning modes in the regime that is stable against the ideal MHD (magnetohydrodynamic) mode has been confirmed by nonlocal analysis based on integral-equation formalism. In contrast to the previous results based on differential-shooting codes, the kinetic-ballooning mode in the second stability regime does not require a finite ion-temperature gradient. PACS Nos.: 52.35Kt, 52.55Fa


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.


1988 ◽  
Vol 39 (1) ◽  
pp. 11-25 ◽  
Author(s):  
Guoyong Fu ◽  
J. W. Van Dam

Using the ballooning-mode transport model proposed by Connor, Taylor & Turner (1984), we derive the thermal conductivity induced by ideal ballooning instability and compare it to experimental observations from auxiliary-heated tokamaks. We show how this model can be improved by means of a finite-beta equilibrium and also apply it to obtain a confinement scaling law for high-beta, purely Ohmically heated tokamaks. Finally, we employ this transport mode to find that tokamaks with supplemental stabilization, for example due to gyroradius, energetic particle or shaping effects, can self-consistently access the second stability regime at rather high heating power.


2000 ◽  
Vol 40 (7) ◽  
pp. 1411-1418 ◽  
Author(s):  
J.R Ferron ◽  
L.L Lao ◽  
T.C Luce ◽  
R.L Miller ◽  
T.H Osborne ◽  
...  

2018 ◽  
Vol 25 (3) ◽  
pp. 032505 ◽  
Author(s):  
X. D. Peng ◽  
J. Q. Xu ◽  
H. B. Jiang ◽  
G. Wang

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