Effect of runaway electrons on tearing mode stability: with or without favorable curvature stabilization

2021 ◽  
Author(s):  
Li Li ◽  
Yueqiang Liu ◽  
Yuling He ◽  
Yanfei Wang ◽  
Liangjia Guo ◽  
...  
2022 ◽  
Author(s):  
Yue Ming ◽  
Deng Zhou ◽  
Jinfang Wang

Abstract The effect of equilibrium poloidal flow and pressure gradient on the m/n = 2/1 (m is the poloidal mode number and n is the toroidal mode number) tearing mode instability for tokamak plasmas is investigated. Based on the condition of ≠0 ( is plasma pressure), the radial part of motion equation is derived and approximately solved for large poloidal mode numbers (m). By solving partial differential equation (Whittaker equation) containing second order singularity, the tearing mode stability index Δ′ is obtained. It is shown that, the effect of equilibrium poloidal flow and pressure gradient has the adverse effect on the tearing mode instability when the pressure gradient is nonzero. The poloidal equilibrium flow with pressure perturbation partially reduces the stability of the classical tearing mode. But the larger pressure gradient in a certain poloidal flow velocity range can abate the adverse influence of equilibrium poloidal flow and pressure gradient. The numerical results do also indicate that the derivative of pressure gradient has a significant influence on the determination of instability region of the poloidal flow with pressure perturbation.


1982 ◽  
Vol 24 (1) ◽  
pp. 97-107 ◽  
Author(s):  
W Kerner ◽  
H Tasso

1984 ◽  
Vol 31 (3) ◽  
pp. 447-463 ◽  
Author(s):  
Moshe Rosenblum

Detailed computational results are presented for the stability of linear tearing modes in low-q cylindrical tokamaks with various radial profiles. The stability properties of a widely used ‘classical’ profile are compared with those of a ‘piecewise’ profile. It is shown that the stability properties of low-q tokamak discharges show a sensitive dependence on small changes in the current density profile near the singular surface. While the ‘classical’ profile is stable for a large range of q0, where q0 is the value of the safety factor on the magnetic axis, a similar ‘piecewise’ profile is unstable for the same set of parameters.


1981 ◽  
Author(s):  
W.W. Heidbrink ◽  
S.C. Jardin ◽  
M.S. Chance
Keyword(s):  

1995 ◽  
Vol 2 (9) ◽  
pp. 3335-3340 ◽  
Author(s):  
H. X. Xie ◽  
A. Bondeson
Keyword(s):  

2010 ◽  
Vol 52 (7) ◽  
pp. 075008 ◽  
Author(s):  
M James ◽  
H R Wilson ◽  
J W Connor

2019 ◽  
Vol 146 ◽  
pp. 1476-1479 ◽  
Author(s):  
K.E.J. Olofsson ◽  
B.S. Sammuli ◽  
D.A. Humphreys

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