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dc.contributor.authorİdemen, Mehmet Mithaten_US
dc.date.accessioned2015-01-15T23:00:21Z
dc.date.available2015-01-15T23:00:21Z
dc.date.issued2005
dc.identifier.citationİdemen, M. M. (2005). Derivation of the lorentz transformation from the maxwell equations. Journal of Electromagnetic Waves and Applications, 19(4), 451-451. doi:10.1163/1569393053303884en_US
dc.identifier.issn0920-5071
dc.identifier.urihttps://hdl.handle.net/11729/194
dc.identifier.urihttp://dx.doi.org/10.1163/1569393053303884
dc.descriptionThis work was supported by the Turkish Academy of Sciences (TUBA).en_US
dc.description.abstractThe Special Theory of Relativity had been established nearly one century ago to conciliate some seemingly contradictory concepts and experimental results such as the Ether, universal time, contraction of dimensions of moving bodies, absolute motion of the Earth, speed of the light, etc. Hence the fundamental revolutionary formulas of the Theory, i.e., the Lorentz Formulas, had been derived first by Einstein by dwelling on a postulate which stipulated the constancy of the speed of the light. To this end he had first postulated that every reference system has a time proper to itself and then redefined the notions of simultaneity, synchronous clocks, time interval, the length of a rod in a system at rest, the length in a moving system, etc. A second postulate of Einstein, which stated that every physical theory is invariant under the Lorentz transformation, enabled him to claim that the Theory of Electromagnetism is correct but the Newtonian Mechanics has to be re-established. Since then the Theory was almost always presented in this way by both Einstein and others except only a few. The aim of this paper is to show that the Lorentz formulas can be derived from the Maxwell equations if one pstulates that the total electric charge of an isolated body does not change if it is in motion. To this end one dwells only on the permanence principle of functional equations, which is not a physical but purely mathematical concept. Thus, from one side the Special Relativity becomes a natural issue (or a part) of the Maxwell Theory and, from the other side, the derivation of the transformation rules pertinent to the electromagnetic field becomes straightforward and easy.en_US
dc.description.sponsorshipTürkiye Bilimler Akademisien_US
dc.language.isoengen_US
dc.publisherVSP BV, Brill Academic Publishersen_US
dc.relation.isversionof10.1163/1569393053303884
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectElectromagnetic-wavesen_US
dc.subjectTranslational motionen_US
dc.subjectScatteringen_US
dc.subjectReflectionen_US
dc.subjectVelocityen_US
dc.subjectCylinderen_US
dc.subjectWedgeen_US
dc.subjectTransmissionen_US
dc.subjectElectric chargeen_US
dc.subjectFunctionsen_US
dc.subjectLight velocityen_US
dc.subjectMaxwell equationsen_US
dc.subjectSynchronous machineryen_US
dc.subjectFunctional equationsen_US
dc.subjectLorentz transformationsen_US
dc.subjectNewtonian Mechanicsen_US
dc.subjectSpecial theory of relativityen_US
dc.subjectMathematical transformationsen_US
dc.titleDerivation of the Lorentz transformation from the Maxwell equationsen_US
dc.typearticleen_US
dc.description.versionPublisher's Versionen_US
dc.relation.journalJournal of Electromagnetic Waves and Applicationsen_US
dc.contributor.departmentIşık Üniversitesi, Mühendislik Fakültesi, Elektrik-Elektronik Mühendisliği Bölümüen_US
dc.contributor.departmentIşık University, Faculty of Engineering, Department of Electrical-Electronics Engineeringen_US
dc.contributor.authorID0000-0002-1225-7482
dc.identifier.volume19
dc.identifier.issue4
dc.identifier.startpage451
dc.identifier.endpage467
dc.peerreviewedYesen_US
dc.publicationstatusPublisheden_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.contributor.institutionauthorİdemen, Mehmet Mithaten_US
dc.relation.indexWOSen_US
dc.relation.indexScopusen_US
dc.relation.indexScience Citation Index Expanded (SCI-EXPANDED)en_US
dc.description.qualityQ4
dc.description.wosidWOS:000228023800002


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