Unified Theory of Relaxations in Plasmas, I. Basic Theorem
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概要
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Two approximate theories-the impact theory and wave theory- of relaxation phenomena in hot plasmas are united into an exact theory, in which no cut-off procedure of the diverging integrals is needed, and which gives Coulomb logarithms with exact nurnerical factors in the arguments. When a relaxation rate is given by a diverging integral ∫B(b)db with respect to the impact parameter b in the impact theory and by a diverging integral ∫K(k)dk with respect to the wave number k in the wave theory, then the present theory gives the rate in the form ∫^∞_0B(b) exp(-1/2b^2/b_0^2)db+∫^∞_0K(k)exp(-1/2k^2/b_0^2)dk. Here b_0 is any length much longer than the close impact radius but much shorter than the Debye radius ; and the final results are independent of b_0. Simple examples are treated.
- 社団法人日本物理学会の論文
- 1963-06-05
著者
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Aono Osamu
Department Of Phycics 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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Kihara T.
Department Of Anatomy Kinki University School Of Medicine
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Kihara T.
Department of Physics, Faculty of Science, University of Tokyo
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