dc.creator | | |
dc.creator | | |
dc.creator | Andrew Chubykalo | |
dc.creator | | |
dc.date | 2016 | |
dc.date.accessioned | 2022-10-12T19:49:26Z | |
dc.date.available | 2022-10-12T19:49:26Z | |
dc.identifier | 0143-0807 | |
dc.identifier | 1361-6404 | |
dc.identifier | http://hdl.handle.net/20.500.11845/541 | |
dc.identifier.uri | https://repositorioslatinoamericanos.uchile.cl/handle/2250/4122782 | |
dc.description | We 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.description | Producción Científica de la Universidad Autónoma de Zacatecas UAZ | |
dc.format | application/pdf | |
dc.language | eng | |
dc.rights | info:eu-repo/semantics/openAccess | |
dc.rights | http://creativecommons.org/licenses/by-nc-nd/4.0 | |
dc.subject | info:eu-repo/classification/cti/1 | |
dc.subject | fundamental solutions of Maxwell’s equations | |
dc.subject | gauge fields | |
dc.subject | vector potentials | |
dc.title | The pedagogical value of the fourdimensional picture: III. Solutions to Maxwell’s equations | |
dc.type | info:eu-repo/semantics/article | |
dc.audience | generalPublic | |