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Ecuaciones de campos para fotones localizados y ecuaciones relativistas de campos para partículas masivas en movimiento


Michaud, André


Research Papers


Mechanics / Electrodynamics



Date Published:

June 17, 2017






Cálculo de la energía de las partículas electromagnéticas localizadas por el método de integración teniendo en cuenta que sus campos de energía disminuye radialmente hacia el infinito, desde un nivel máximo de intensidad situado en un límite de distancia de su centro igual a (lambda alpha)/2pi, lo que permite definir unos campos electromagnéticos localizados para estas partículas localizadas en movimiento.. Por otra parte, en un artículo publicado en la Revista International IFNA-ANS Journal, Paul Marmet tuvo éxito usando la ecuación de Biot-Savart asociar el campo magnético con una porción específica de la masa relativista medible de un electrón en movimiento, un campo que aumenta en intensidad con el cuadrado de su velocidad relativista. Esta dependencia directa entre la velocidad de un electrón y la intensidad de los campos magnéticos y eléctricos ambiente ya está establecida con la ecuación de Lorentz. Sin embargo, la ecuación de Marmet define el campo magnético propio del electrón en movimiento con el cual los campos eléctrico y magnético ambientes definidos por la ecuación de Lorentz interactúan para definir su velocidad. Vamos a estudiar aquí las características de este campo magnético intrínseco del electrón en movimiento y las de su campo eléctrico asociado.


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