Elasticity and electromagnetism. Part 1: The Coulomb gauge

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dc.creatorDmitriyev, V. P.
dc.date2002-02-04
dc.date.accessioned2026-07-07T05:47:02Z
dc.date.available2026-07-07T05:47:02Z
dc.descriptionThe Maxwell's electromagnetic equations are isomorphic to the motion equation of a linear elastic continuum which is hard to compression though liable to shear deformation. The Coulomb gauge expresses the medium incompressibility. The magnetic vector potential corresponds to the medium velocity. The pressure stands for the electrostatic potential. The electric field is modeled by an external force whose origin is beyond the elastic model. The electric charge corresponds to a medium defect which produces the perturbation 1/r of the pressure field . The defects interact with each other due to the dilatation center in the core of the inclusion.
dc.descriptionsee http://aether.narod.ru/
dc.identifierhttps://arxiv.org/abs/physics/0202006
dc.identifierhttp://arxiv.org/abs/physics/0202006
dc.identifierMeccanica 39 No 6: 511-520, 2004.
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/84558
dc.subjectGeneral Physics
dc.subjectClassical Physics
dc.titleElasticity and electromagnetism. Part 1: The Coulomb gauge
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