dorsal/arxiv
View SchemaElasticity and electromagnetism. Part 1: The Coulomb gauge
| Authors | V. P. Dmitriyev |
|---|---|
| Categories | |
| ArXiv ID | physics/0202006 |
| URL | https://arxiv.org/abs/physics/0202006 |
| Journal | Meccanica 39 No 6: 511-520, 2004. |
Abstract
The 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.
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"abstract": "The Maxwell\u0027s electromagnetic equations are isomorphic to the motion equation\nof a linear elastic continuum which is hard to compression though liable to\nshear deformation. The Coulomb gauge expresses the medium incompressibility.\nThe magnetic vector potential corresponds to the medium velocity. The pressure\nstands for the electrostatic potential. The electric field is modeled by an\nexternal force whose origin is beyond the elastic model. The electric charge\ncorresponds to a medium defect which produces the perturbation 1/r of the\npressure field . The defects interact with each other due to the dilatation\ncenter in the core of the inclusion.",
"arxiv_id": "physics/0202006",
"authors": [
"V. P. Dmitriyev"
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"physics.gen-ph",
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"journal_ref": "Meccanica 39 No 6: 511-520, 2004.",
"title": "Elasticity and electromagnetism. Part 1: The Coulomb gauge",
"url": "https://arxiv.org/abs/physics/0202006"
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