Born: 1831. Died: 1879.
- Electricity and magnetism are two aspects of a single unified force of nature, best described as dynamical as dynamical fields.
- Light consists of transverse electromagnetic waves, and is but one portion of a broad spectrum of such waves.
- Thermodynamic laws and properties of gases may be derived from a statistical description of molecular motion.
- Analogies are a valid and important tool in physical theory.
The Scottish physicist James Clerk Maxwell did revolutionary work in electromagnetism and the kinetic theory of gases. After graduating (1854) with a degree in mathematics from Trinity College, Cambridge, he held professorships at Marischal College in Aberdeen (1856) and King's College in London (1860) and became the first Cavendish Professor of Physics at Cambridge in 1871.
Maxwell's first major contribution to science was a study of the planet Saturn's rings, the nature of which was much debated. Maxwell showed that stability could be achieved only if the rings consisted of numerous small solid particles, an explanation still accepted. Maxwell next considered molecules of gases in rapid motion. By treating them statistically he was able to formulate (1866), independently of Ludwig Boltzmann, the Maxwell-Boltzmann kinetic theory of gases. This theory showed that temperatures and heat involved only molecular movement. Philosophically, this theory meant a change from a concept of certainty--heat viewed as flowing from hot to cold--to one of statistics--molecules at high temperature have only a high probability of moving toward those at low temperature. This new approach did not reject the earlier studies of thermodynamics; rather, it used a better theory of the basis of thermodynamics to explain these observations and experiments.
Maxwell's most important achievement was his extension and mathematical formulation of Michael Faraday's theories of electricity and magnetic lines of force. In his research, conducted between 1864 and 1873, Maxwell showed that a few relatively simple mathematical equations could express the behavior of electric and magnetic fields and their interrelated nature; that is, an oscillating electric charge produces an electromagnetic field. These four partial differential equations first appeared in fully developed form in Electricity and Magnetism (1873). Since known as Maxwell's equations they are one of the great achievements of 19th-century physics.
Maxwell also calculated that the speed of propagation of an electromagnetic field is approximately that of the speed of light. He proposed that the phenomenon of light is therefore an electromagnetic phenomenon. Because charges can oscillate with any frequency, Maxwell concluded that visible light forms only a small part of the entire spectrum of possible electromagnetic radiation.
Maxwell used the later-abandoned concept of the ether to explain that electromagnetic radiation did not involve action at a distance. He proposed that electromagnetic-radiation waves were carried by the ether and that magnetic lines of force were disturbances of the ether. Heinrich Hertz discovered such waves in 1888.
- A Dynamical Theory of the Electromagnetic Field, 1865
- A Treatise on Electricity and Magnetism, 1873
- An Elementary Treatise on Electricity, 1881, 1888
- Illustrations of the Dynamical Theory of Gases, 1860
- Matter and Motion, 1876
- On Faraday's Lines of Force, 1856
- On Physical Lines of Force, 1861
- On the Results of Bernoulli's Theory of Gases as Applied to their Internal Friction, their Diffusion, and their Conductivity for Heat
- On the Stability of the Motion of Saturn's Rings, 1859
- Theory of Heat, 1871
- 1846, On the Description of Oval Curves, and those having a plurality of Foci, Proceedings of the Royal Society of Edinburgh
- 1867–1868, On Governors, Proceedings of the Royal Society
- 1867, On the Dynamical Theory of Gases, Philosophical Transactions of the Royal Society of London
- 1871, On the Focal Lines of a Refracted Pencil, Proceedings of the London Mathematical Society
- 1873, Molecules, Nature
- 1874, On Hamilton's Characteristic Function for a Narrow Beam of Light, Proceedings of the London Mathematical Society
- 1875–89, Ether, Encyclopaedia Britannica, Ninth Edition