Abstract
By using simple concepts of special relativity and the differential representations of the Faraday and Ampère-Maxwell laws, we deduce their Gelman-Monsivais integral representation. The relativistic transformation laws of the electromagnetic field are also obtained without using tensorial analysis or covariant concepts.
Original language | English |
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Pages (from-to) | 32-36 |
Number of pages | 5 |
Journal | Revista Mexicana de Fisica E |
Volume | 54 |
Issue number | 1 |
State | Published - Jun 2008 |
Externally published | Yes |
Keywords
- Integral representation
- Maxwell equations
- Special relativity