| Display title | Physics:Covariant formulation of classical electromagnetism |
| Default sort key | Covariant formulation of classical electromagnetism |
| Page length (in bytes) | 26,814 |
| Namespace ID | 3020 |
| Namespace | Physics |
| Page ID | 372215 |
| Page content language | en - English |
| Page content model | wikitext |
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| Page creator | imported>JOpenQuest |
| Date of page creation | 05:42, 5 February 2024 |
| Latest editor | imported>JOpenQuest |
| Date of latest edit | 05:42, 5 February 2024 |
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Description | Content |
Article description: (description)
This attribute controls the content of the description and og:description elements. | The covariant formulation of classical electromagnetism refers to ways of writing the laws of classical electromagnetism (in particular, Maxwell's equations and the Lorentz force) in a form that is manifestly invariant under Lorentz transformations, in the formalism of special relativity using rectilinear... |
