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Équations de champs pour photons localisés et équations relativistes de champs pour particules massives en mouvement


Michaud, André


Research Papers


Mechanics / Electrodynamics



Date Published:

June 17, 2017






Calcul de l'énergie des particules électromagnétiques localisées par la méthode d'intégration considérant que leur champs d'énergie décroit radialement jusqu'à l'infini à partir d'un niveau intensité maximale localisée à une distance limite de son centre égale à lambda alpha/2 pi, ce qui permet la définition de champs électromagnétiques localisés correspondant à ces particules localisées en mouvement. De plus, dans un article publié dans le International IFNA-ANS Journal, Paul Marmet a mis en évidence à l'aide de l'équation de Biot-Savart la manière dont le champ magnétique associé à une partie de la masse relativiste mesurable d'un électron en mouvement, s'accroit en intensité en fonction du carré de sa vitesse. Cette dépendance directe entre la vélocité d'un électron et l'intensité des champs magnétique et électrique ambiants est déjà établie par l'équation de Lorentz. Cependant, l'équation de Marmet définit le champ magnétique propre de l'électron en mouvement avec lequel les champs électrique et magnétique ambiants, définis par l'équation de Lorentz, interagissent pour définir sa vitesse. Nous allons étudier ici les caractéristiques ce champ magnétique intrinsèque de l'électron en mouvement ainsi que celles de son champ électrique associé.


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