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The power of a critical heat engine

Since its inception about two centuries ago thermodynamics has sparkled continuous interest and fundamental questions. According to the second law no heat engine can have an efficiency larger than Carnot's efficiency. The latter can be achieved by the Carnot engine, which however ideally operat...

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Autores principales: Campisi, Michele, Fazio, Rosario
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4915125/
https://www.ncbi.nlm.nih.gov/pubmed/27320127
http://dx.doi.org/10.1038/ncomms11895
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author Campisi, Michele
Fazio, Rosario
author_facet Campisi, Michele
Fazio, Rosario
author_sort Campisi, Michele
collection PubMed
description Since its inception about two centuries ago thermodynamics has sparkled continuous interest and fundamental questions. According to the second law no heat engine can have an efficiency larger than Carnot's efficiency. The latter can be achieved by the Carnot engine, which however ideally operates in infinite time, hence delivers null power. A currently open question is whether the Carnot efficiency can be achieved at finite power. Most of the previous works addressed this question within the Onsager matrix formalism of linear response theory. Here we pursue a different route based on finite-size-scaling theory. We focus on quantum Otto engines and show that when the working substance is at the verge of a second order phase transition diverging energy fluctuations can enable approaching the Carnot point without sacrificing power. The rate of such approach is dictated by the critical indices, thus showing the universal character of our analysis.
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spelling pubmed-49151252016-06-29 The power of a critical heat engine Campisi, Michele Fazio, Rosario Nat Commun Article Since its inception about two centuries ago thermodynamics has sparkled continuous interest and fundamental questions. According to the second law no heat engine can have an efficiency larger than Carnot's efficiency. The latter can be achieved by the Carnot engine, which however ideally operates in infinite time, hence delivers null power. A currently open question is whether the Carnot efficiency can be achieved at finite power. Most of the previous works addressed this question within the Onsager matrix formalism of linear response theory. Here we pursue a different route based on finite-size-scaling theory. We focus on quantum Otto engines and show that when the working substance is at the verge of a second order phase transition diverging energy fluctuations can enable approaching the Carnot point without sacrificing power. The rate of such approach is dictated by the critical indices, thus showing the universal character of our analysis. Nature Publishing Group 2016-06-20 /pmc/articles/PMC4915125/ /pubmed/27320127 http://dx.doi.org/10.1038/ncomms11895 Text en Copyright © 2016, Nature Publishing Group, a division of Macmillan Publishers Limited. All Rights Reserved. http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article's Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/
spellingShingle Article
Campisi, Michele
Fazio, Rosario
The power of a critical heat engine
title The power of a critical heat engine
title_full The power of a critical heat engine
title_fullStr The power of a critical heat engine
title_full_unstemmed The power of a critical heat engine
title_short The power of a critical heat engine
title_sort power of a critical heat engine
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4915125/
https://www.ncbi.nlm.nih.gov/pubmed/27320127
http://dx.doi.org/10.1038/ncomms11895
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