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Entropy

Physical Sciences

Entropy is the measure of a system's thermal energy per unit temperature that is unavailable for doing useful work, and so also a measure of the disorder, or randomness, of a system. The entropy of an isolated system never decreases, which is the physical content of the second law of thermodynamics. Ludwig Boltzmann later gave entropy a statistical meaning, relating it to the number of microscopic arrangements consistent with a system's observable state.

Facts
Proposed Year
1865 1
Proposed By
Rudolf Clausius, who introduced the term in 1865 for the thermodynamic quantity; Ludwig Boltzmann gave it a statistical formulation in the 1870s, relating entropy to the number of microscopic arrangements of a system. 1
Connections

Associated With

Belongs To

Source Entropy (Britannica)

Proposed By

Boltzmann's specific contribution is the statistical formulation of entropy (the Boltzmann entropy formula), distinct from Clausius's original 1865 thermodynamic definition of the term.

Source Ludwig Boltzmann (Britannica)
Source Rudolf Clausius (Britannica)

Studied In

Source Sadi Carnot (Britannica)
Sources
1. Entropy (Britannica)
Encyclopaedia Britannica
Sadi Carnot (Britannica)
Encyclopaedia BritannicaStudied In: ThermodynamicsView the Source
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