Relaxation of sawtooth stability criterion on magnetic shear due to alpha particle pressure

1995 ◽  
Vol 35 (10) ◽  
pp. 1225-1230
Author(s):  
M Yamagiwa
1997 ◽  
Vol 4 (11) ◽  
pp. 4001-4008 ◽  
Author(s):  
M. H. Redi ◽  
R. B. White ◽  
S. H. Batha ◽  
F. M. Levinton ◽  
D. C. McCune

1968 ◽  
Vol 39 (7) ◽  
pp. 1013-1018 ◽  
Author(s):  
R. L. Howard ◽  
S. W. Nelson ◽  
J. R. Winckler

2020 ◽  
Vol 86 (6) ◽  
Author(s):  
Xiang Zhu ◽  
Long Zeng ◽  
Zhiyong Qiu ◽  
Baolong Hao ◽  
Wei Shen ◽  
...  

The dependence of fishbone cycle on energetic particle intensity has been investigated in EAST low-magnetic-shear plasmas. It is observed that the fishbone mode growth rate, saturation amplitude as well as fishbone cycle frequency clearly increase with increasing neutral beam injection (NBI) power. Moreover, enhanced electron density and temperature perturbations as well as energetic particle loss were observed with greater injected NBI power. Simulation results using M3D-K code show that as the NBI power increases, the resonant frequency and the energy of the resonant particles become higher, and the saturation amplitude of the mode also changes, due to the non-perturbative energetic particle contribution. The relationship between the calculated energetic particle pressure ratio and fishbone cycle frequency is obtained as ${f_{\textrm{FC}}} = 2.2{(1000{\beta _{\textrm{ep,calc}}} - 0.1)^{5.9 \pm 0.5}}$ . Results consistent with the experimental observations have been achieved based on a predator–prey model.


1997 ◽  
Author(s):  
M.H. Redi ◽  
R.B. White ◽  
S.H. Batha ◽  
F.M. Levinton ◽  
D.C. McCune

1979 ◽  
Vol 44 ◽  
pp. 307-313
Author(s):  
D.S. Spicer

A possible relationship between the hot prominence transition sheath, increased internal turbulent and/or helical motion prior to prominence eruption and the prominence eruption (“disparition brusque”) is discussed. The associated darkening of the filament or brightening of the prominence is interpreted as a change in the prominence’s internal pressure gradient which, if of the correct sign, can lead to short wavelength turbulent convection within the prominence. Associated with such a pressure gradient change may be the alteration of the current density gradient within the prominence. Such a change in the current density gradient may also be due to the relative motion of the neighbouring plages thereby increasing the magnetic shear within the prominence, i.e., steepening the current density gradient. Depending on the magnitude of the current density gradient, i.e., magnetic shear, disruption of the prominence can occur by either a long wavelength ideal MHD helical (“kink”) convective instability and/or a long wavelength resistive helical (“kink”) convective instability (tearing mode). The long wavelength ideal MHD helical instability will lead to helical rotation and thus unwinding due to diamagnetic effects and plasma ejections due to convection. The long wavelength resistive helical instability will lead to both unwinding and plasma ejections, but also to accelerated plasma flow, long wavelength magnetic field filamentation, accelerated particles and long wavelength heating internal to the prominence.


1971 ◽  
Vol 32 (C6) ◽  
pp. C6-185-C6-187
Author(s):  
A. DUDEK ◽  
P. E. HODGSON

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