نبذة مختصرة : The fundamental problem formulated by R. Feynman is solved: to establish a mechanism hidden behind the law of gravitation (Coulomb's law). Paradoxically, Coulomb's law has been an important tool for scientific research for several centuries, but the physical mechanism of interaction between particles is still unknown. The validity of the universal gravitation law is confirmed by the experiments of Cavendish for macrobodies and by the observations of the solar system planets motion. Most physicists believe that the Coulomb law describes the interaction not only between stars, planets and macrobodies, but also between individual particles, although there are no experimental data confirming its validity for individual particles. Disclosure of the physical mechanism of interaction between particles is one of the most important problems in physics. Ignorance of the physical nature of the interaction inhibits many studies - on cold nuclear fusion, on the control of gravity, on the creation of engines without the release of reactive mass, and others. It is shown that the introduction of a test point classical particle (considered as a measuring instrument) into the region of action of the Coulomb field produced by the initial point particle significantly distorts the Coulomb field and substantially changes the state of motion of the initial particle. The resultant Coulomb field arising when the Coulomb fields of the initial and probe particles are superimposed differs significantly from the Coulomb field of the original particle. This means that the Coulomb field generated by a point particle does not have the properties of an external field. In deriving the universal gravitation law, it is assumed that the Coulomb field of each particle acts on an adjacent particle as an external field. Consequently, the extrapolation of the universal gravitation law to the interaction between individual particles is inadmissible, its use in description of the interaction between particles is a serious error. The mechanism of ...
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