Special Relativity in the proper time of the source
Tepper Gill
In this talk, I report on a new
implementation of the first two explicit postulates of special relativity in
which the coordinate, geometric (or proper time) of the observer is replaced by
the proper time of the source. This approach does not require self-interaction,
and radiation appears directly as dissipation in the proper time version of Maxwell’s
equations. (These equations are mathematically but not physically equivalent to
the conventional ones, and shows explicitly that the second postulate is a
convention imposed by the mathematical formulation, which is not required by
physics.)/bigger>/fontfamily> A number of
natural and physically interesting conclusions follow from this approach. Among
others, we conclude that the classical self-energy divergency is not intrinsic
to the physics, radiation has mass, only retarded solutions are admissible, and
that Ritz was not completely wrong. (Recall that Ritz argued that the speed of
light should depend on the motion of the source.)