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Boltzmann entropy
In thermodynamics, Boltzmann entropy refers to the H-theorem, introduced by Austrian physicist Ludwig Boltzmann in his famous 1872 paper “Further Studies on the Thermal Equilibrium of Gas Molecules”, which statistically quantifies the entropy of an ideal gas system. [1]
See also
● Clausius entropy
● Gibbs entropy
References
1. Boltzmann, Ludwig. (1872). "Further Studies on the Thermal Equilibrium of Gas Molecules" (“Weitere Studien über das Wärmegleichgewicht unter Gasmolekülen”), in Sitzungsberichte der Akademie der Wissenschaften, Mathematische-Naturwissenschaftliche Klasse (pgs. 275-370), Bd. 66, Dritte Heft, Zweite Abteilung, Vienna: Gerold.
External links
● Boltzmann entropy – Wikipedia.
See also
● Clausius entropy
● Gibbs entropy
References
1. Boltzmann, Ludwig. (1872). "Further Studies on the Thermal Equilibrium of Gas Molecules" (“Weitere Studien über das Wärmegleichgewicht unter Gasmolekülen”), in Sitzungsberichte der Akademie der Wissenschaften, Mathematische-Naturwissenschaftliche Klasse (pgs. 275-370), Bd. 66, Dritte Heft, Zweite Abteilung, Vienna: Gerold.
External links
● Boltzmann entropy – Wikipedia.
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