Abstract

In classical electrodynamics, it can be challenging to demonstrate the balance between minus of power of radiating particles and retarded radiation energy flux for radiation in the free-space because of the field’s singularity. In an alternative radiation theory of Wheeler–Feynman absorber theory, which is based on a first principle of time-symmetric interaction between radiating particles surrounded by the absorber at large distance, the singularity is eliminated but the balance cannot be preserved due to advanced effects. This is quantitatively demonstrated with an argument of consequent non-classical light radiated by classical current.