Carnot Cycle at Finite Power: Attainability of Maximal Efficiency

Armen E. Allahverdyan, Karen V. Hovhannisyan, Alexey V. Melkikh, and Sasun G. Gevorkian
Phys. Rev. Lett. 111, 050601 – Published 1 August 2013
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Abstract

We want to understand whether and to what extent the maximal (Carnot) efficiency for heat engines can be reached at a finite power. To this end we generalize the Carnot cycle so that it is not restricted to slow processes. We show that for realistic (i.e., not purposefully designed) engine-bath interactions, the work-optimal engine performing the generalized cycle close to the maximal efficiency has a long cycle time and hence vanishing power. This aspect is shown to relate to the theory of computational complexity. A physical manifestation of the same effect is Levinthal’s paradox in the protein folding problem. The resolution of this paradox for realistic proteins allows to construct engines that can extract at a finite power 40% of the maximally possible work reaching 90% of the maximal efficiency. For purposefully designed engine-bath interactions, the Carnot efficiency is achievable at a large power.

  • Received 28 March 2013

DOI:https://doi.org/10.1103/PhysRevLett.111.050601

© 2013 American Physical Society

Authors & Affiliations

Armen E. Allahverdyan1, Karen V. Hovhannisyan2,1, Alexey V. Melkikh3, and Sasun G. Gevorkian4

  • 1Yerevan Physics Institute, Alikhanian Brothers Street 2, Yerevan 375036, Armenia
  • 2ICFO-Institut de Ciències Fotòniques, Mediterranean Technology Park, 08860 Castelldefels (Barcelona), Spain
  • 3Ural Federal University, Mira Street 19, Yekaterinburg 620002, Russia
  • 4Institute of Physics, Academia Sinica, Nankang, Taipei 11529, Taiwan

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Issue

Vol. 111, Iss. 5 — 2 August 2013

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