Ion-Electron Relaxation of Plasmas in a Strong Magnetic Field : I
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Relaxation between ion and electron temperatures, T_1 and T_2, of dilute fully ionized gases in a magnetic field is discussed. The mean gyration radius, γ_g, is assumed to be much smaller than the Debye length, ι_D. The rate of relaxation, R, defined by d(T_2-T_1)/dt = -(T_2-T_1)R is calculated to be R = (n_1+n_2)(4m_2/3m_1)(2πkT_2/m_2)^<1/2>(Ze^2/kT_2)^2[In(ι_D/γ_g)]^2 for γ_g〜Ze^2/kT_2.
- 社団法人日本物理学会の論文
- 1959-12-05
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