Derivation of the self-interaction force on an arbitrarily moving point-charge and of its related energy-momentum radiation rate: The Lorentz-Dirac equation of motion in a Colombeau algebra
Andre Gsponer

TL;DR
This paper rigorously derives the self-interaction force and energy-momentum radiation rate for an arbitrarily moving point-charge using Colombeau algebra, clarifying longstanding issues in classical electrodynamics and deriving the Lorentz-Dirac equation.
Contribution
It introduces a rigorous mathematical framework in Colombeau algebra to derive the Lorentz-Dirac equation and resolve issues related to the Schott term in classical electrodynamics.
Findings
Self-energy of a point charge is a delta-squared integral, not Coulomb energy.
Energy-momentum radiation rate equals negative self-interaction force.
Provides a clear derivation of the Lorentz-Dirac equation of motion.
Abstract
The classical theory of radiating point-charges is revisited: the retarded potentials, fields, and currents are defined as nonlinear generalized functions. All calculations are made in a Colombeau algebra, and the spinor representations provided by the biquaternion formulation of classical electrodynamics are used to make all four-dimensional integrations exactly and in closed-form. The total rate of energy-momentum radiated by an arbitrarily moving relativistic point-charge under the effect of its own field is shown to be rigorously equal to minus the self-interaction force due to that field. This solves, without changing anything in Maxwell's theory, numerous long-standing problems going back to more than a century. As an immediate application an unambiguous derivation of the Lorentz-Dirac equation of motion is given, and the origin of the problem with the Schott term is explained: it…
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Taxonomy
TopicsMathematical and Theoretical Analysis · Quantum Mechanics and Applications · History and Theory of Mathematics
