Classical Electromagnetism as a Consequence of Coulomb's Law, Special Relativity and Hamilton's Principle and its Relationship to Quantum Electrodynamics
J. H. Field
Abstract
It is demonstrated how all the mechanical equations of classical electrodynamics (CEM) may be derived from only Coulomb's inverse square force law, special relativity and Hamilton's Principle. The instantaneous nature of the Coulomb force in the centre-of-mass frame of two interacting charged objects, mediated by the exchange of space-like virtual photons, is predicted by QED. The interaction Lagrangian of QED is shown to be identical, in the appropriate limit, to the potential energy term in the Lorentz-invariant Lagrangian of CEM. A comparison is made with the Feynman-Wheeler action-at-a-distance formulation of CEM.
Create a lesson
Related papers
Covariant Electrodynamics with a Scalar Degree of Freedom
Seil Sautbekov
Electromagnetic Radiation from a Neutralized Polarized Sphere with Two Conserved Currents for One Charge History
Natan Rentzber
The Photon Gas in Classical Mechanics: A Statistical-Mechanical Treatment of Classical Field Theory
Farhang Loran, Saman Moghimi-Araghi
Hydrogen Molecular Ion and Molecule in Classical Electrodynamics with Classical Zero-Point Radiation
Timothy H. Boyer
Spheroid rolling up on diverging inclines
Khanh P. M. Hoang, Duy V. Nguyen
Scalar-Longitudinal Radiation in Extended Electrodynamics with Multipole Theory and a Compensated Source Model
Natan Rentzber