James Clerk Maxwell (1831 to 1879) is best known for unifying electricity, magnetism and light into a single theory, but in thermal physics he opened an equally consequential line of work. Around 1866 he formulated, independently of Ludwig Boltzmann, a kinetic theory of gases showing that heat and temperature are statistical properties of molecular motion rather than a substance flowing between bodies: molecules at a given temperature move at a range of speeds distributed according to a definite law, so a hotter body's molecules are only more likely, not certain, to be the faster ones. This statistical reframing did not overturn the existing laws of thermodynamics but gave them a mechanical foundation, and the distribution he derived, later completed and rigorously derived by Boltzmann, is named for them both.
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FieldKinetic Theory and Statistical Mechanics 1 Connections
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Maxwell formulated the underlying kinetic theory around 1866, independently of Boltzmann's later rigorous derivation.
Source James Clerk Maxwell (MacTutor)
Additional Source Maxwell's Equations (Wikipedia)Lead section (edge: proposed-by, Maxwell)
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1. James Clerk Maxwell (MacTutor)
MacTutor History of Mathematics, University of St AndrewsQuick Info summary
James Clerk Maxwell was a Scottish mathematician who did revolutionary work on electricity, magnetism, optics and on the kinetic theory of gases.
Founded: Electromagnetism, Biography section
One of Maxwell's most important achievements was his extension and mathematical formulation of Michael Faraday's theories of electricity and magnetic lines of force.
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WikipediaProposed: Maxwell's Equations, Lead section (edge: proposed-by, Maxwell)Quote, Proposed: Maxwell's Equations, Lead section (edge: proposed-by, Maxwell)
Maxwell's equations are named after the physicist and mathematician James Clerk Maxwell, who, in 1861 and 1862, published an early form of the equations that included the Lorentz force law.
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