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Magnetic monopole as the shadow side of the electric charge
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AbstractIt is shown that a magnetic monopole appears as the tension state of the primary electric charge at its motion through each section of the path equal to the particle’s de Broglie wavelength. This conclusion is followed from a submicroscopic consideration of particles and their motion in the framework of the theory of physical space in the form of a tessellattice developed by Michel Bounias and the author. The periodical change of the particle’s charged state to its monopole state can easily be introduced in the conventional Maxwell equations and the magnetic monopole automatically shows up in the structure of Maxwell’s equations. The monopole is also presented in any quark system as a quark obeys dynamics that are also characterized by the appropriate de Broglie wavelength and hence the electric charge changes periodically to the magnetic monopole. A (anti)neutrino emerges as the typical electron’s monopole. When the charged particle becomes the monopole, it also loses its mass (the mass passes to the particle’s inerton cloud) and thus the neutrino is a massless particle, or more correctly massless monopole.
Title: Magnetic monopole as the shadow side of the electric charge
Description:
AbstractIt is shown that a magnetic monopole appears as the tension state of the primary electric charge at its motion through each section of the path equal to the particle’s de Broglie wavelength.
This conclusion is followed from a submicroscopic consideration of particles and their motion in the framework of the theory of physical space in the form of a tessellattice developed by Michel Bounias and the author.
The periodical change of the particle’s charged state to its monopole state can easily be introduced in the conventional Maxwell equations and the magnetic monopole automatically shows up in the structure of Maxwell’s equations.
The monopole is also presented in any quark system as a quark obeys dynamics that are also characterized by the appropriate de Broglie wavelength and hence the electric charge changes periodically to the magnetic monopole.
A (anti)neutrino emerges as the typical electron’s monopole.
When the charged particle becomes the monopole, it also loses its mass (the mass passes to the particle’s inerton cloud) and thus the neutrino is a massless particle, or more correctly massless monopole.
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