Quantum Mechanics: Genesis and Achievements pp 195-232 | Cite as

# Electrodynamics and Special Relativity

## Abstract

The classical electrodynamics is a well established field theory, starting from formalization by Maxwell in 1855–1861 of previously known empirical facts. It serves up to now as a safe ground and a model for all subsequent field theories.

In 1862, Maxwell put forward the electromagnetic theory of light. In 1884, Heaviside recasted Maxwell’s mathematical analysis from its original form to modern vector terminology, and in the same year Poynting discovered the energy propagation in a Maxwell field. In 1886, Hertz experimentally discovered electromagnetic waves and calculated the dipole radiation. Einstein in 1905 discovered the special relativity and the covariant electrodynamics, by postulating invariance of the Maxwell equations in all inertial frames—this was justified by the Michelson and Morley crucial experiments.

The next fundamental question arises on the interaction of the Maxwell field with matter. In 1890s Lorentz introduced the *electron theory* of polarization and magnetization of matter; this enabled one to avoid ‘sharp questions’, reducing the problem of the matter reaction to *constitutive equations*.

Alternatively, one should consider all details of the interaction of charged particles with a Maxwell field. However, this question cannot be solved in the classical theory, since for a point particle, the field energy is infinite—this effect is nowadays known as the ‘ultraviolet divergence’.

To fix the situation, Abraham in 1905 introduced the model of ‘extended electron’. However, this suggestion leads to next question on the shape of electron. This question was partially clarified after the discovery of quantum mechanics (1926); however a complete answer is still a matter for the future.

## Keywords

Maxwell Equation Lorentz Transformation Lagrangian Density Lorentz Group Multipole Expansion## Bibliography

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