Note 431(1) : Masses of the Elementary Particles and LENR

Note 431(1) : Masses of the Elementary Particles and LENR

This note shows that the masses of the elementary particles can be understood by Eq. (12), each particle is defined by its individual m ( r ) function. LENR is understood straightforwardly in terms of the Casimir force (24) of m space discussed in the immediately preceding paper UFT430. Under the condition (28) this force due to m space can easily become greater than the strong nuclear force binding protons and neutrons, so the nucleus splits apart, emitting the energy (32), and causing transmutation.This process is observed as heat. The process has been shown to be reproducible and repeatable many times, and is part of mainstream science. It was discovered in the University of Utah as is well known. There are industrial and military LENR plants, and it is hoped that domestic LENR heaters are just around the corner. The problem has been controlling the heat, so the container does not melt. It is blazingly obvious, to coin an awful pun, that the heat is there. LENR is vastly more efficient than conventional sources of power and heat. The heat can be used to drive turbines and produce electricity. In making a LENR device, the experimenter has effectively tuned to condition (28), discussed in great detail by Horst Eckardt in UFT417 and UFT430. The m(r) function is linked to the R function of the ECE wave equation in Eq. (17). So m(r) has been described self consistently in terns of Cartan geometry.

a431stpapernotes1.pdf

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