### 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 | American English |
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Pages (from-to) | 32-36 |

Number of pages | 28 |

Journal | Revista Mexicana de Fisica E |

State | Published - 1 Jan 2008 |

Externally published | Yes |