ELECTROSTRONG INTERACTION OF THE NUCLEUS.

 

The certificate of the copyright ¹ 8493 – 30.09.2003ã.

The state department of the intellectual property,

The Ministry of Education and sciences of Ukraine

(has translated daughter Olga)

             Spaces it is considered as the form of a matter. Equations of Maxwell are mathematical true of the general equations of dynamics. In them, dynamics of an electric field of a charge causes an induction of a magnetic field, as real properties. Continuation of this mathematical true is the equations of dynamics of mass fields. In them, similarly to an induction of a magnetic field in a variable electric field, dynamics of a field of Strong or Gravitational Interaction causes an induction of mass trajectories. The equations of dynamics of mass fields of interaction, outside of electromagnetic fields, are similar to the equations of electromagnetic dynamics outside of mass fields, with equations of Maxwell.

             Similarly to electromagnetic waves, the equations specify gravitationally-mass waves. Mass fields are induced in a variable (quantum) field of Strong Interaction.

In a full kind, there is a mathematical true of interconnected dynamics electromagnetic, and mass fields of interaction in conditions of quantum relativistic dynamics their component.

             In both cases the question is mathematical true of such properties, with the conditions of such dynamics determined in everyone case.

             On examples the equations of stationary conditions of the closed mass trajectories in a field of Strong Interaction are considered. Within the limits of constants of interaction charges of quarks of the charged and neutral quantums of Strong Interaction of nucleons of a nucleus are calculated. The physical essence of quark models is considered.

             In decisions of the equations of a stationary condition of the closed contours of inductive mass trajectories in a field of Strong Interaction as structural forms of nucleons of a nucleus in a spectrum of atoms, are calculated specific energy of connection of nucleons of a nucleus of easy atoms. With high accuracy they coincide with real specific energy of connection of nucleons of a nucleus.