We review our model of a proton that obeys the Schwarzschild condition. We find that only a very small percentage of the vacuum fluctuations available within a proton volume need be cohered and converted to mass‐energy in order for the proton to meet the Schwarzschild condition. This proportion is equivalent to that between gravitation and the strong force where gravitation is thought to be to weaker than the strong force. Gravitational attraction between two contiguous Schwarzschild protons can accommodate both nucleon and quark confinement. We calculate that two contiguous Schwarzschild protons would rotate at c and have a period of and a frequency of which is characteristic of the strong force interaction time and a close approximation of the gamma emission typically associated with nuclear decay. We include a scaling law and find that the Schwarzschild proton data point lies near the least squares trend line for organized matter. Using a semi‐classical model, we find that a proton charge orbiting at a proton radius at c generates a good approximation to the measured anomalous magnetic moment.
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Research Article| November 24 2010
The Schwarzschild Proton
AIP Conf. Proc. 1303, 95–100 (2010)
Nassim Haramein; The Schwarzschild Proton. AIP Conf. Proc. 24 November 2010; 1303 (1): 95–100. https://doi.org/10.1063/1.3527190
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