4/3 problem, Poynting theorem, and electromagnetic energy-momentum tensor

dc.authoridYarman, Tolga/0000-0003-3209-2264
dc.authorscopusid7004016669
dc.authorscopusid55893162300
dc.authorscopusid6602787345
dc.authorwosidYarman, Tolga/Q-9753-2019
dc.contributor.authorKholmetskii, Alexander L.
dc.contributor.authorMissevitch, Oleg V.
dc.contributor.authorYarman, Tolga
dc.contributor.otherEnerji Sistemleri Mühendisliği / Energy Systems Engineering
dc.date.accessioned2024-05-25T11:18:24Z
dc.date.available2024-05-25T11:18:24Z
dc.date.issued2015
dc.departmentOkan Universityen_US
dc.department-temp[Kholmetskii, Alexander L.] Belarusian State Univ, Dept Phys, Minsk 220030, BELARUS; [Missevitch, Oleg V.] Inst Nucl Problems, Minsk 220030, BELARUS; [Yarman, Tolga] Okan Univ, Istanbul, Turkey; [Yarman, Tolga] Savronik, Eskisehir, Turkeyen_US
dc.descriptionYarman, Tolga/0000-0003-3209-2264en_US
dc.description.abstractWe show that the familiar 4/3 problem originates from the incorrect determination of the momentum of the electromagnetic field generated by an isolated charged particle, which results from an incorrect application of the Poynting theorem to the field. To demonstrate this, we consider a macroscopic problem: splitting a charged oil droplet into two identical smaller droplets in the rest frame K of the original droplet, and in another inertial frame K' moving with respect to K with some constant velocity, and arrive at a physically senseless solution in the framework of the standard approach. To solve this problem in a correct way, we suggest a modified Poynting theorem for an isolated charge and recalculate the momentum of the electromagnetic field of this charge, which yields the usual relativistic relationship between the field energy and momentum. Our approach is not at odds with the idea about "Poincare stresses"; however, in contrast to the standard method, it provides a usual relationship between the "Poincare stress-energy" and the associated momentum stress component. Finally, the continuity equation in four-dimensional form for the case of isolated moving charge is also proposed, which completely resolves the 4/3 problem.en_US
dc.identifier.citation5
dc.identifier.doi10.1139/cjp-2014-0533
dc.identifier.endpage697en_US
dc.identifier.issn0008-4204
dc.identifier.issn1208-6045
dc.identifier.issue6en_US
dc.identifier.scopus2-s2.0-84930712162
dc.identifier.scopusqualityQ3
dc.identifier.startpage691en_US
dc.identifier.urihttps://doi.org/10.1139/cjp-2014-0533
dc.identifier.urihttps://hdl.handle.net/20.500.14517/330
dc.identifier.volume93en_US
dc.identifier.wosWOS:000355596100015
dc.identifier.wosqualityQ4
dc.institutionauthorYarman, Nuh Tolga
dc.language.isoen
dc.publisherCanadian Science Publishingen_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subject[No Keyword Available]en_US
dc.title4/3 problem, Poynting theorem, and electromagnetic energy-momentum tensoren_US
dc.typeArticleen_US
dspace.entity.typePublication
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relation.isAuthorOfPublication.latestForDiscoverye8750528-f58f-486e-9a0a-eb4ab45fb468
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