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The Classical Electron Problem

dc.contributor.authorLindesay, J.en_US
dc.contributor.authorZachary, W. W.en_US
dc.contributor.authorGill, Tepper L.en_US
dc.date.accessioned2006-09-11T14:50:16Z
dc.date.available2006-09-11T14:50:16Z
dc.date.issued2001-09en_US
dc.identifier.citationGill, Tepper L.; Zachary, W. W.; Lindesay, J.; (2001). "The Classical Electron Problem." Foundations of Physics 31(9): 1299-1355. <http://hdl.handle.net/2027.42/44465>en_US
dc.identifier.issn1572-9516en_US
dc.identifier.issn0015-9018en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/44465
dc.description.abstractIn this paper, we construct a parallel image of the conventional Maxwell theory by replacing the observer-time by the proper-time of the source. This formulation is mathematically, but not physically, equivalent to the conventional form. The change induces a new symmetry group which is distinct from, but closely related to the Lorentz group, and fixes the clock of the source for all observers. The new wave equation contains an additional term (dissipative), which arises instantaneously with acceleration. This shows that the origin of radiation reaction is not the action of a “charge” on itself but arises from inertial resistance to changes in motion. This dissipative term is equivalent to an effective mass so that classical radiation has both a massless and a massive part. Hence, at the local level the theory is one of particles and fields but there is no self-energy divergence (nor any of the other problems). We also show that, for any closed system of particles, there is a global inertial frame and unique (invariant) global proper-time (for each observer) from which to observe the system. This global clock is intrinsically related to the proper clocks of the individual particles and provides a unique definition of simultaneity for all events associated with the system. We suggest that this clock is the historical clock of Horwitz, Piron, and Fanchi. At this level, the theory is of the action-at-a-distance type and the absorption hypothesis of Wheeler and Feynman follows from global conservation of energy.en_US
dc.format.extent287668 bytes
dc.format.extent3115 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherKluwer Academic Publishers-Plenum Publishers; Plenum Publishing Corporation ; Springer Science+Business Mediaen_US
dc.subject.otherMechanicsen_US
dc.subject.otherCondensed Matteren_US
dc.subject.otherPhysicsen_US
dc.subject.otherPhysics, Generalen_US
dc.subject.otherQuantum Physicsen_US
dc.subject.otherRelativity and Cosmologyen_US
dc.subject.otherBiophysics/Biomedical Physicsen_US
dc.titleThe Classical Electron Problemen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelMathematicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Electrical Engineering, Department of Mathematics, and Department of Physics, University of Michigan, Ann Arbor, Michigan, 48109en_US
dc.contributor.affiliationotherDepartment of Electrical Engineering and Department of Mathematics and Statistics, University of Maryland University College, College Park, Maryland, 20742en_US
dc.contributor.affiliationotherDepartment of Physics, Howard University, Washington, DC, 20059en_US
dc.contributor.affiliationumcampusAnn Arboren_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/44465/1/10701_2004_Article_346165.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1023/A:1012222227710en_US
dc.identifier.sourceFoundations of Physicsen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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