Ion-Electron Relaxation of Plasmas in a Magnetic Field, II
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概要
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Relaxation between ion and electron temperatures, T_1 and T_2, of dilute fully ionized gases in a magnetic field has been treated by force-correlation method. The rate R of the relaxation, defined by d(T_2-T_1)/dt = -(T_1-T_1)R, increases with increasing magnetic field from R = R^0ln(t_p/t_s) for ω_2t_p≦1 to R = R^0[ln(t_p/t_s) + 1/2(lnω_2t_p)^2] for ω_2t_p〓1, in which R^0 = (n_1+n_2)(8m_2/3m_1)(2πkT_2/m_2)^<1/2>(Ze^2/kT_2)^2. Here m_1, Ze and n_1 are the mass, charge and number density of the ion respectively; m_2, -e, and n_2 are those of the electron; t_p is the period of plasma oscillation and t_s is the mean time of passage through a sphere of strong interaction, t_s〜(m_2/kT_2)^<1/2>Ze^2/kT_2; ω_2 is the electron gyration frequency.
- 社団法人日本物理学会の論文
- 1960-04-05
著者
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Sakuma Kyoko
Department Of Physics Faculty Of Science University Of Tokyo
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KIHARA Taro
Department of Physics, Faculty of Science, University of Tokyo
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MIDZUNO Yukio
Department of Physics, Faculty of Science, University of Tokyo
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SHIZUME Toshio
Department of Physics, Faculty of Science, University of Tokyo
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Midzuno Yukio
Department Of Physics Faculty Of Science University Of Tokyo
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Kihara Taro
Department Of Physics Faculity Of Science University Of Tokyo
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Shizume Toshio
Department Of Physics Faculty Of Science University Of Tokyo
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