Radial diffusion equation for collision-affected plasma
The equation for radial diffusion in a planetary magnetosphere is developed for the case in which the mean collision time is longer than the bounce time but shorter than the characteristic time scale of diffusion. An intuitive, mean‐free‐time method is used on the assumption that the coherence time...
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Published in | Geophysical research letters Vol. 5; no. 1; pp. 63 - 64 |
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Main Author | |
Format | Journal Article |
Language | English |
Published |
Blackwell Publishing Ltd
01.01.1978
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Subjects | |
Online Access | Get full text |
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Summary: | The equation for radial diffusion in a planetary magnetosphere is developed for the case in which the mean collision time is longer than the bounce time but shorter than the characteristic time scale of diffusion. An intuitive, mean‐free‐time method is used on the assumption that the coherence time of the perturbation electric field is longer than the mean collision time. The equation can be applied to ambient plasma in the Jovian magnetosphere. |
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Bibliography: | ArticleID:7L1075 istex:08D2E386D84BEB79B2169BBBD257DFF4864EE437 ark:/67375/WNG-L7BH1VB6-P ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 ObjectType-Article-2 ObjectType-Feature-1 |
ISSN: | 0094-8276 1944-8007 |
DOI: | 10.1029/GL005i001p00063 |