1973
DOI: 10.1119/1.1987559
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Introduction to the Principles of Electromagnetism

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Cited by 9 publications
(7 citation statements)
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“…We must observe that with the use of the classical Coulomb potential this situation never occurs, the interaction force between the proton and the electron is always attractive. The acceleration due to the electric force being null at this position, eliminates the argument or defiance against the Classical Laws of the Electrodynamic that an electron revolving the nucleus of the atom, lose energy by radiation [8][9][10]. The force being null at the equilibrium position r 1 0 , means that the electron cannot be orbiting the nucleus of the atom as predicted by Bohr theory.…”
Section: A New Electric Interaction Microscopic Forcementioning
confidence: 99%
“…We must observe that with the use of the classical Coulomb potential this situation never occurs, the interaction force between the proton and the electron is always attractive. The acceleration due to the electric force being null at this position, eliminates the argument or defiance against the Classical Laws of the Electrodynamic that an electron revolving the nucleus of the atom, lose energy by radiation [8][9][10]. The force being null at the equilibrium position r 1 0 , means that the electron cannot be orbiting the nucleus of the atom as predicted by Bohr theory.…”
Section: A New Electric Interaction Microscopic Forcementioning
confidence: 99%
“…4 A small change in the contents of a cavity affects the resonant frequency of the cavity. For electromagnetic cavities the Bethe-Schwinger relation 5,6 gives an explicit connection between this frequency shift and the permittivity and permeability of the perturbing inclusion,…”
Section: Introductionmentioning
confidence: 99%
“…Two reports exist about this work. 2,3 However, the derivation is given by Walter Hauser, 4 who terms the expression for the fractional frequency shift the Bethe-Schwinger cavity perturbation formula.…”
mentioning
confidence: 99%