Poloidal electric field generated by electron cyclotron heating in a collisional tokamak plasma

1987 ◽  
Vol 30 (3) ◽  
pp. 830 ◽  
Author(s):  
V. S. Chan ◽  
S. K. Wong
Keyword(s):  
Electric Field ◽  
Electron Cyclotron ◽  
Tokamak Plasma ◽  
Electron Cyclotron Heating

Transition of the radial electric field by electron cyclotron heating in the CHS heliotron/torsatron

1993 ◽  
Vol 71 (14) ◽  
pp. 2220-2223 ◽  
Author(s):  
H. Idei ◽  
K. Ida ◽  
H. Sanuki ◽  
H. Yamada ◽  
H. Iguchi ◽  
...  
Keyword(s):  
Electric Field ◽  
Radial Electric Field ◽  
Electron Cyclotron ◽  
Electron Cyclotron Heating

Bernstein rays in a Tokamak plasma in the electron-cyclotron heating conditions

1979 ◽  
Vol 21 (12) ◽  
pp. 1067-1072 ◽  
Author(s):  
F de Luca ◽  
C Maroli ◽  
V Petrillo
Keyword(s):  
Electron Cyclotron ◽  
Tokamak Plasma ◽  
Electron Cyclotron Heating

Formation of positive radial electric field by electron cyclotron heating in compact helical system

1994 ◽  
Vol 1 (10) ◽  
pp. 3400-3406 ◽  
Author(s):  
H. Idei ◽  
K. Ida ◽  
H. Sanuki ◽  
S. Kubo ◽  
H. Yamada ◽  
...  
Keyword(s):  
Electric Field ◽  
Radial Electric Field ◽  
Electron Cyclotron ◽  
Electron Cyclotron Heating

scholarly journals Sawtooth stabilization by localized electron cyclotron heating in a tokamak plasma

1990 ◽  
Author(s):  
K. Hanada ◽  
H. Tanaka ◽  
M. Iida ◽  
T. Minami ◽  
T. Maekawa ◽  
...  
Keyword(s):  
Electron Cyclotron ◽  
Tokamak Plasma ◽  
Electron Cyclotron Heating

Poloidal electric field due to electron-cyclotron resonance heating in tokamaks

1992 ◽  
Vol 47 (2) ◽  
pp. 261-269 ◽  
Author(s):  
M. Taguchi
Keyword(s):  
Electric Field ◽  
Cyclotron Resonance ◽  
Electron Cyclotron Resonance ◽  
Resonance Condition ◽  
Adjoint Equation ◽  
Planck Equation ◽  
Electron Cyclotron ◽  
Electron Cyclotron Resonance Heating ◽  
Tokamak Plasma ◽  
Linear Diffusion

The poloidal electric field generated by electron-cyclotron resonance heating is investigated for a tokamak plasma in the collisionless regime. This poloidal electric field is calculated by solving an adjoint equation to the linearized Fokker-Planck equation with a quasi-linear diffusion term. It is found from this calculation that the magnitude and the sign of the poloidal electric field depend strongly on the values of the inverse aspect ratio, the poloidal angle of the absorption point, the parallel velocity of resonant electrons normalized by the thermal velocity, and the strength of the relativistic correction to the resonance condition.

Sawtooth stabilization by localized electron cyclotron heating in a tokamak plasma

1991 ◽  
Vol 66 (15) ◽  
pp. 1974-1977 ◽  
Author(s):  
K. Hanada ◽  
H. Tanaka ◽  
M. Iida ◽  
S. Ide ◽  
T. Minami ◽  
...  
Keyword(s):  
Electron Cyclotron ◽  
Tokamak Plasma ◽  
Electron Cyclotron Heating
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