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Optimal Thermodynamics—New Upperbounds

Laboratoire d'Energétique et de Mécanique Théorique et Appliquée (LEMTA-ENSEM); Vandoeuvre 2, avenue de la Forêt de Haye 54516, France
Entropy 2009, 11(4), 529-547;
Received: 31 August 2009 / Accepted: 23 September 2009 / Published: 28 September 2009
(This article belongs to the Special Issue Exergy: Analysis and Applications)
This paper reviews how ideas have evolved in this field from the pioneering work of CARNOT right up to the present. The coupling of thermostatics with thermokinetics (heat and mass transfers) and entropy or exergy analysis is illustrated through study of thermomechanical engines such as the Carnot heat engine, and internal combustion engines. The benefits and importance of stagnation temperature and irreversibility parameters are underlined. The main situations of constrained (or unconstrained) optimization are defined, discussed and illustrated. The result of this study is a new branch of thermodynamics: Finite Dimensions Optimal Thermodynamics (FDOT). View Full-Text
Keywords: optimal thermodynamics; upperbound; combined heat and power; internal combustion engine optimal thermodynamics; upperbound; combined heat and power; internal combustion engine
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MDPI and ACS Style

Feidt, M. Optimal Thermodynamics—New Upperbounds. Entropy 2009, 11, 529-547.

AMA Style

Feidt M. Optimal Thermodynamics—New Upperbounds. Entropy. 2009; 11(4):529-547.

Chicago/Turabian Style

Feidt, Michel. 2009. "Optimal Thermodynamics—New Upperbounds" Entropy 11, no. 4: 529-547.

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