Abstract

The electron on a trajectory around a nucleus radiates energy since it is accelerated and, following the classical theories of physics, should fall on the nucleus. But since it does not fall, it exists a cause, not taken into account by these theories, that prevents it from this fall. Indeed, in our precedent publications we showed that the fields and the particles are changes in a specific elastic medium called "ether". In particular, that a particle is a globule called “single-particle wave” that vibrates in the ether and is denoted . This that moves at the velocity V of the particle, contains all the parameters relative to it, and modulates the amplitude of the superposition of a wave called “phase-wave”, denoted , (and not ) of phase velocity V_p . In the present paper, one considers that the electron moves on a circle of circumference C, under the attraction of a nucleus. is then present simultaneously several times, e.g., N times, at each point of this circle, that is, in , which is influenced by these N superpositions, due to the fact that interferes with itself at each round. It appears then the two possible cases: the resonant and the nonresonant.In the resonant case, C contains an integer number of wave lengths of that therefore superposes itself at each round in a constructive addition, and creates a relatively large , i.e., of a relatively large energy. The electron that radiates then only a limited percentage of its large energy, does not fall on the nucleus.In the nonresonant case, C contains a non-integer number of , then superposes itself at each round in a destructive addition, and creates a much smaller , i.e., of much smaller energy. The electron that radiates then almost the same energy as in the resonant case, loses in fact a much larger percentage of its energy than in the resonant case, cannot remain in this state.

Highlights

  • The electron on a trajectory around a nucleus radiates energy since it is accelerated and, following the classical theories of physics, should fall on the nucleus

  • Contains an integer number of wave lengths of that superposes itself at each round in a constructive addition, and creates a relatively large, i.e., of a relatively large energy

  • Contient un nombre entier de longueurs d’onde de qui donc se superposent elles même à chaque tour en une addition constructive, et créent une relativement grande, i.e., de relativement grande énergie

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Summary

The Nonresonant Electron Phase-Wave

This nonresonant case is the one where strictly 0 < < 1. In this case, the explicit expression for the term. It appears, for example, that for = 0.5, Eq (17) becomes (− ) = 0.5[1 − (−1) ] ,. Which is much smaller than (1 + ) as it appears in the case where = 0, i.e., in (15)

The Nonresonant Electron Single-Particle Wave
Conclusion
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