ABSTRACT
During 1903-04 the effect on the motion of a single particle due
to its self-field was studied by both Abraham and Lorentz. They
modelled the isolated electron as a charged spherical surface of finite radius and found inconsistencies with classical electromagnetic
theory as the radius approached zero. In 2005 the self-fields of
pairs of particles were finally understood as a mutual phenomenon. The singularity problem at the charge points was solved by using
motions that avoid the charge points, assuming that at equilibrium
the two particles rotate never residing at their own centres of
rotation. The self-field theory model1 for the electromagnetic
field as a cyclic stream of photons provides an analysis of the
hydrogen atom and yields a derivation of Planck’s number . The bi-
spinorial function for each particle provides a physically plausible
interpretation of relativity. The “beads on a string” stream-like
electromagnetic field modifies the macroscopic time-invariant field
laws of Coulomb and Ampere at the atomic level. The E-and
H-fields must be measured between centres of rotation rather
than between charge points and applied as a coupled complete
electromagnetic field. The atomic self-field motions are obtained
using the Maxwell-Lorentz (ML) equations. Quantum theory can be
reinterpreted to include the coupled bi-spinorial field to yield the
same deterministic closed form eigensolutions as self-field theory.
Space-time orthogonality shows the complete self-field theory outer
shell electronic structure to be analytic. Self-field theory allows
reinterpretation of theweak and strong nuclear forces via amodified
system of ML equations.