Collision-Induced Instability in a Magnetoactive Plasma
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概要
- 論文の詳細を見る
The dispersion relations for the waves propagating in a magnetoactive plasma are obtained from the Boltzmann eqation with a collision term of the electrons. Two cases in which the wave vector parallel and perpendicular to the uniform magnetic field are studied. Under the assumption that the unperturbed distribution is a spherical shell in velocity space in each case, and two dispersion relations to the zeroth approximation in K are obtained as follows: (A) ω(ω+iv)^2=ω_p^2(ω+iv-iV/3 <dv>/<dV>) and (B) ω(ω±ω_c+iv-iV/3 <dv>/<dV> where ω_c and ω_p are the cyclotron and the plasma frequencies respectively, and v is the collision frequency with the neutral particles. After some calculations under an assumption v(v)=const×v^h it is found that initial pertur bations grow exponentially for h>3 in (B) and the growth rate is the largest in the magnetic field-free case.
- 社団法人日本物理学会の論文
- 1966-07-05
著者
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Tanaka Shigetoshi
Yoshida College Kyoto University Kyoto And Institute Of Plasma Physics Nagoya University
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MITANI Kenji
Yoshida College, Kyoto University
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Mitani Kenji
Yoshida College Kyoto University
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Mitani Kenji
Yoshida College Kyoto University Kyoto And Institute Of Plasma Physics Nagoya University
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SHIMOMURA Noboru
Yoshida College, Kyoto University
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Shimomura Noboru
Yoshida College Kyoto University Kyoto And Institute Of Plasma Physics Nagoya University
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Shimomura Noboru
Yoshida College Kyoto University
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Shimomura N.
Yoshida College, Kyoto University, Kyoto and Institute of Plasma Physics, Nagoya, University
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