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


Michaud, André


Research Papers


Mechanics / Electrodynamics



Date Published:

October 11, 2019






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 lokalisierten bewegenden elektromagnetischen Partikeln zusammenhängend sind. Außerdem hat Paul Marmet in einem 2003 im International IFNA-ANS Journal veröffentlichten Beitrag mit Hilfe der Biot-Savart-Gleichung geklärt, wie die Intensität des Magnetfeldes, das einem Teil der Masse eines sich bewegenden Elektrons zugeordnet ist, mit dem Quadrat seiner Geschwindigkeit zunimmt. Diese direkte Abhängigkeit zwischen der Geschwindigkeit eines Elektrons und der Intensität der magnetischen und elektrischen Umgebungsfelder wird bereits durch die Lorentz-Kraftgleichung hergestellt. Die Marmet-Gleichung definiert jedoch das intrinsische Magnetfeld des sich bewegenden Elektrons, mit dem die magnetischen und elektrischen Umgebungsfelder der Lorentz-Gleichung interagieren, um seine Geschwindigkeit zu definieren. Wir werden hier die Eigenschaften dieses innewohnenden Magnetfeldes des Elektrons in Bewegung, ebensogut wie denjenigen seines eng verbundenen elektrischen Feldes studieren.


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