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||American English|
|Number of pages||28|
|Journal||Revista Mexicana de Fisica E|
|State||Published - 1 Jan 2008|