Kinetic Equations for Fully Ionized, Inhomogenous Plasmas
dc.contributor.author | Osborn, Richard K. | en_US |
dc.date.accessioned | 2011-09-02T18:54:13Z | |
dc.date.available | 2011-09-02T18:54:13Z | |
dc.date.issued | 1963-06-15 | en_US |
dc.identifier.citation | Phys. Rev. 130, 2142Ð2155 (1963) <http://hdl.handle.net/2027.42/86128> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/86128 | |
dc.description.abstract | It is shown that, in the sense of certain procedures for successively approximating the quantum Liouville equation, the Boltzmann-Vlasov-Maxwell equations for the description of the fully ionized plasma are a natural first approximation. The nature of some of the approximations inherent in the use of such a description of the plasma is indicated, but little attention is given to their quantitative evaluation. An H theorem for the particle-photon system is demonstrated. | en_US |
dc.publisher | American Physical Society | en_US |
dc.rights | © 1963 The American Physical Society | en_US |
dc.title | Kinetic Equations for Fully Ionized, Inhomogenous Plasmas | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Nuclear Engineering and Radiological Sciences | en_US |
dc.subject.hlbtoplevel | Engineering | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | Department of Nuclear Engineering | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/86128/1/PhysRev.130.2142-RKO.pdf | |
dc.identifier.doi | 10.1103/PhysRev.130.2142 | en_US |
dc.identifier.source | Physical Review | en_US |
dc.owningcollname | Nuclear Engineering and Radiological Sciences, Department of (NERS) |
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