On the Electrodynamics of Moving Permanent Dipoles in External Electromagnetic Fields

TL;DR

This paper explores how the rest-mass of moving permanent dipoles varies in external electromagnetic fields to maintain energy conservation, highlighting the interplay between internal and external fields in classical electrodynamics.

Contribution

It demonstrates that the rest-mass of dipoles must change in response to external fields, ensuring energy conservation within classical electrodynamics frameworks.

Findings

Rest-mass varies with external electromagnetic fields.

Internal and external field interference explains mass variation.

Consistent behavior across different theoretical formulations.

Abstract

The classical theory of electrodynamics is built upon Maxwell's equations and the concepts of electromagnetic field, force, energy and momentum, which are intimately tied together by Poynting's theorem and the Lorentz force law. Whereas Maxwell's macroscopic equations relate the electric and magnetic fields to their material sources (i.e., charge, current, polarization and magnetization), Poynting's theorem governs the flow of electromagnetic energy and its exchange between fields and material media, while the Lorentz law regulates the back-and-forth transfer of momentum between the media and the fields. The close association of momentum with energy thus demands that the Poynting theorem and the Lorentz law remain consistent with each other, while, at the same time, ensuring compliance with the conservation laws of energy, linear momentum, and angular momentum. This paper shows how a consistent application of the aforementioned laws of electrodynamics to moving permanent dipoles (both electric and magnetic) brings into play the rest-mass of the dipoles. The rest mass must vary in response to external electromagnetic fields if the overall energy of the system is to be conserved. The physical basis for the inferred variations of the rest-mass appears to be an interference between the internal fields of the dipoles and the externally applied fields. We use two different formulations of the classical theory in which energy and momentum relate differently to the fields, yet we find identical behavior for the rest-mass in both formulations.