Carnot cycle: Difference between revisions
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The '''Carnot cycle''' is a hypothetical cycle in which the efficiency is a maximum. It was proposed by Nicolas Léonard Sadi Carnot <ref>Nicolas Léonard Sadi Carnot "Reflexions sur la Puissance Motrice de Feu et sur les Machines Propres a Développer cette Puissance" (1824), printed in [http://www.numdam.org/item?id=ASENS_1872_2_1__393_0 Annales scientifiques de l'École Normale Supérieure Sér. '''2''', 1 pp. 393-457 (1872)]</ref>. | |||
The Carnot cycle consists of four distinct operations: | |||
#A reversible isothermal expansion of the gas at the "hot" temperature, ''T''<sub>''Hot''</sub> | |||
#An isentropic reversible adiabatic expansion of the gas | |||
#A reversible isothermal compression of the gas at the "cold" temperature, ''T''<sub>''Cold''</sub> | |||
#Finally an isentropic compression of the gas | |||
<br>[[Image:Carnot_TS.png|500px]] | |||
==See also== | |||
*[[Clausius theorem]] | |||
==References== | ==References== | ||
<references/> | |||
[[Category: Classical thermodynamics]] | [[Category: Classical thermodynamics]] | ||
Latest revision as of 13:38, 20 July 2011
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The Carnot cycle is a hypothetical cycle in which the efficiency is a maximum. It was proposed by Nicolas Léonard Sadi Carnot [1]. The Carnot cycle consists of four distinct operations:
- A reversible isothermal expansion of the gas at the "hot" temperature, THot
- An isentropic reversible adiabatic expansion of the gas
- A reversible isothermal compression of the gas at the "cold" temperature, TCold
- Finally an isentropic compression of the gas
See also[edit]
References[edit]
- ↑ Nicolas Léonard Sadi Carnot "Reflexions sur la Puissance Motrice de Feu et sur les Machines Propres a Développer cette Puissance" (1824), printed in Annales scientifiques de l'École Normale Supérieure Sér. 2, 1 pp. 393-457 (1872)