The role of geodesic acoustic mode on reducing the turbulent transport in the edge plasma of tokamak

2018 ◽  
Vol 25 (1) ◽  
pp. 012317 ◽  
Author(s):  
K. N. Geng ◽  
D. F. Kong ◽  
A. D. Liu ◽  
T. Lan ◽  
C. X. Yu ◽  
...  
2008 ◽  
Vol 15 (5) ◽  
pp. 052309 ◽  
Author(s):  
Kazuhiro Miki ◽  
Yasuaki Kishimoto ◽  
Jiquan Li ◽  
Naoaki Miyato

2008 ◽  
Vol 100 (21) ◽  
Author(s):  
X. Q. Xu ◽  
Z. Xiong ◽  
Z. Gao ◽  
W. M. Nevins ◽  
G. R. McKee

2014 ◽  
Vol 21 (10) ◽  
pp. 102506 ◽  
Author(s):  
Haijun Ren ◽  
Chao Dong

2015 ◽  
Vol 81 (3) ◽  
Author(s):  
Sakineh Meshkani ◽  
Mahmood Ghoranneviss ◽  
Mansoureh Lafouti

For understanding the effect of resonant helical magnetic field (RHF) and bias on the edge plasma turbulent transport, the radial and poloidal electric field (Er, EP), poloidal and toroidal magnetic field (BP, Br) were detected by the Langmuir probe, magnetic probe and diamagnetic loop. The poloidal, toroidal and radial velocity (VP, Vr, Vt) can be determined from the electric and magnetic field. In the present work, we have investigated the effect of the magnitude of bias (Vbias = 200v, Vbias = 320v) on Er, EP, BP, Bt, VP, Vr, Vt. Moreover, we applied RHF with L = 2, L = 3 and L = 2 and 3 and investigate the effect of the helical windings radius on above parameters. Also, the experiment was repeated by applying the positive biasing potentials and RHF's simultaneously. The results show that by applying bias to the plasma at t = 15 msec at r/a = 0.9, Er, BP and Bt increase while EP decreases. The best modification occurs at Vbias = 200v. By applying RHF to the plasma, both the electric and magnetic field vary. Er reaches the highest in the presence of RHF with L = 3. The same results are obtained for BP, Bt, VP and Vt. While the inverse results are obtained for EP and Vr. Finally, RHF and bias are applied simultaneously to the plasma. With applied bias with Vbias = 200v and RHF with L = 2 and 3, we reach to the ideal circumstance. The same results obtain in the situation with Vbias = 320v and RHF with L = 2 and 3.


2010 ◽  
Author(s):  
N. Chakrabarti ◽  
P. N. Guzdar ◽  
R. G. Kleva ◽  
R. Singh ◽  
P. K. Kaw ◽  
...  

Author(s):  
Yahui Wang ◽  
Tao Wang ◽  
Shizhao Wei ◽  
Zhiyong Qiu

Abstract The parametric decay process of a reversed shear Alfv\'{e}n eigenmeode (RSAE) into a geodesic acoustic mode (GAM) and a kinetic reversed shear Alfv\'{e}n eigenmode (KRSAE) is investigated using nonlinear gyrokinetic theory. The excitation conditions mainly require the pump RSAE amplitude to exceed a certain threshold, which could be readily satisfied in burning plasmas operated in steady-state advanced scenario. This decay process can contribute to thermal plasma heating and confinement improvement.


2021 ◽  
Vol 61 (6) ◽  
pp. 066009
Author(s):  
H.J. Sun ◽  
R.J. Goldston ◽  
A. Huber ◽  
X.Q. Xu ◽  
J. Flanagan ◽  
...  

2017 ◽  
Vol 57 (12) ◽  
pp. 126048 ◽  
Author(s):  
J. Seidl ◽  
J. Krbec ◽  
M. Hron ◽  
J. Adamek ◽  
C. Hidalgo ◽  
...  

2015 ◽  
Vol 22 (6) ◽  
pp. 062508 ◽  
Author(s):  
A. Storelli ◽  
L. Vermare ◽  
P. Hennequin ◽  
Ö. D. Gürcan ◽  
G. Dif-Pradalier ◽  
...  

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