dc.contributorhttps://orcid.org/0000-0001-5324-1834
dc.contributorhttps://orcid.org/0000-0002-1478-7946
dc.creatorChubykalo, Andrew
dc.creatorEspinoza, Augusto
dc.creatorKosyakov, Boris Pavlovich
dc.date.accessioned2018-06-12T16:29:54Z
dc.date.available2018-06-12T16:29:54Z
dc.date.created2018-06-12T16:29:54Z
dc.date.issued2016
dc.identifier0143-0807
dc.identifier1361-6404
dc.identifierhttp://hdl.handle.net/20.500.11845/541
dc.identifierhttps://doi.org/10.48779/5x6m-m784
dc.description.abstractWe outline a regular way for solving Maxwell’s equations. We take, as the starting point, the notion of vector potentials. The rationale for introducing this notion in electrodynamics is that the set of Maxwell’s equations is seemingly overdetermined. We demonstrate the existence of two fundamental solutions to Maxwell’s equations whose linear combinations comprise the whole variety of classical electromagnetic field configurations.
dc.languageeng
dc.publisherIOP Publishing
dc.relationgeneralPublic
dc.relationhttp://iopscience.iop.org/journal/0143-0807
dc.rightshttp://creativecommons.org/licenses/by-nc-sa/3.0/us/
dc.rightsAtribución-NoComercial-CompartirIgual 3.0 Estados Unidos de América
dc.sourceEuropean Journal of Physics, Núm 37, 2016.
dc.titleThe pedagogical value of the fourdimensional picture: III. Solutions to Maxwell’s equations
dc.typeinfo:eu-repo/semantics/article


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