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Feldgleichungen für lokalisierte Photonen und relativistische Feldgleichungen für bewegende lokalisierte massive Teilchen


Michaud, André


Research Papers


Mechanics / Electrodynamics



Date Published:

November 20, 2016






Berechnung der Energie lokalisierter elektromagnetischer Teilchen mittels der Integrationsmethode, die annimmt, dass ihre Energie-Felder mathematisch radial bis zu Unendlichkeit abnehmen (),von einem maximalen Intensitätsniveau, das an einer inneren Grenze /2 von ihrem Zentrum entfernt ist, wodurch diskrete lokale elektromagnetische Felder definiert werden können, die mit permanent lo-kalisierten bewegenden elektromagnetischen Partikeln zusammenhängend sind. Außerdem, in einem Papier veröffentlicht im International IFNA-ANS Journal 2003, hat Paul Marmet mit Hilfe der Biot-Savart-Gleichung geklärt, wie sich die Intensität des Magnetfeldes, das eng zu Teil der Masse eines Elektrons in Bewe-gung verbunden ist, als das Quadrat seiner relativistischen Geschwindigkeit ver-größert. Diese direkte Abhängigkeit zwischen Geschwindigkeit eines Elektrons und In-tensität der umgebenden magnetischen und elektrischen Felder wird bereits durch der Lorentz-Kraft-Gleichung gegründet. Jedoch definiert die Gleichung von Marmet das innewohnende Magnetfeld des Elektrons in Bewegung, mit dem die umgebenden magnetischen und elektrischen Felder der Lorentz Gleichung aufei-nander wirken, seine Geschwindigkeit zu definieren. Wir werden hier die Eigen-schaften dieses innewohnenden Magnetfeldes des Elektrons in Bewegung, eben-sogut wie denjenigen seines eng verbundenen elektrischen Feldes studieren.


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