Finite Amplitude Effects on Landau Damping and Diminished Transportation of Trapped Electrons

2014 ◽  
Vol 83 (7) ◽  
pp. 074502
Author(s):  
Chang Woo Myung ◽  
Im Hee Won ◽  
Ho Young Kim ◽  
Jeong-Soo Lee ◽  
Gun Su Yun ◽  
...  
1991 ◽  
Vol 69 (2) ◽  
pp. 102-106
Author(s):  
A. Hirose

Analysis, based on a local kinetic dispersion relation in the tokamak magnetic geometry incorporating the ion transit frequency and trapped electrons, indicates that modes with positive frequencies are predominant. Unstable "drift"-type modes can have frequencies well above the diamagnetic frequency. They have been identified as the destabilized ion acoustic mode suffering little ion Landau damping even when [Formula: see text].


1970 ◽  
Vol 4 (4) ◽  
pp. 819-824
Author(s):  
F. Einaudi ◽  
W. I. Axford

In this note we comment and extend the results of a previous analysis in which the non-linear behaviour of one-dimensional electrostatic oscillations in a homogeneous, unbounded, collisionless and fully ionized plasma was considered. The evolution of a monochromatic wave of small, but finite amplitude is studied by expanding the dependent variables as well as the independent variable tin the form of asymptotic series; an ordering parameter e proportional to the initial amplitude of the electric field is introduced. The expansion of the independent variable in such a series allows us to eliminate secular terms from the part of the distribution function which does not depend on the free-streaming terms. This, in turn, allows us to determine corrections to the complex frequency a. Results of a previous note on non-linear Landau damping for an initially Maxwellian. distribution function are confirmed, but it is indicated that they apply to values of time up to a value τ1 rather than for all times. One can proceed to larger values of time in the manner of the multiple time-scale method. In particular it is found that the Landau damping is increased with respect to the linear value only initially during the first time scale.


1998 ◽  
Vol 81 (26) ◽  
pp. 5824-5827 ◽  
Author(s):  
M. V. Medvedev ◽  
P. H. Diamond ◽  
M. N. Rosenbluth ◽  
V. I. Shevchenko

1987 ◽  
Vol 65 (2) ◽  
pp. 173-184 ◽  
Author(s):  
E. Marquis ◽  
J. Teichmann

The stability of a steady finite-amplitude whistler wave penetrating a collisionless, unbounded, homogeneous plasma is studied. The supporting wave as well as the excited side-band waves are assumed to propagate parallel to an uniform magnetostatic field B0. For a general form of the distribution function of trapped electrons, the growth (damping) rates of side-band modes are calculated.It is shown that a particular distribution of trapped electrons gives rise to strongly unstable side-band electromagnetic modes having right-hand polarization. The spectrum of unstable electrostatic and electromagnetic satellite waves is analyzed.


Sign in / Sign up

Export Citation Format

Share Document