Establishment of a system of equations for quantum electrodynamics in which an electron, like any other charge, has an electric and a magnetic field. Description of the eigenvector fields using scalar and vector potentials satisfying the equations.
Lorentz electrodynamics (brief overview) In classical electrodynamics, an electron, just like any other charge, has the electric and magnetic field. To describe self-fields of the electron Lorentz [1] using scalar and vector potentials satisfying the equations: (1) Here - the speed of light, the charge density and the velocity of the electron, respectively. In the special case of motion with constant velocity vector potential is expressed through the scalar potential in the form [1] (2) Hence, the problem of determining the fields of the electron is reduced to the problem of congestion charges potential with a given density and velocity of center of mass. As it know, to solve this problem, Lorenz [1] used transformation of variables (Lorentz transformation), which allows reducing the problem to the Poisson equation: electron quantum electrodynamic scalar (3) Here ? = u / c. (4) Thus, the problem of finding the potential of moving charges reduced to the problem of finding the electrostatic potential of fixed c
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