Anomalous d. c. Resistivity in a Turbulent Plasma
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Jon-wave turbulence is assumed isotropic and homogeneous. An applied electricfield Eg is so weak that the above assumption remains valid. The energy ratiop=(?f.?")/Snn.T. is considered of the order 10-" -IQ ', where E. is thefluctuation field. The diffusion equation for the average distribution f.(v, t) isderived on the basis of Dupree's and Weinstock's methods. The diffusion coeffi-cient i$ given as a solution of the Volterra integral equation of the second kind. -1The electric current induced by E, is readily calculated for the case r.<y.. .Here, r. is the time interval in which the phase relation between ion wave andelectron position is randomized and 7.." is the auto-correlation time for the ionwave. The anomalous d.c. resistivity is evaluated up to the order p" by takingaccount of the fourth order moment of E..
- 社団法人日本物理学会の論文
- 1977-04-15
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