Exergy Dynamics of Systems in Thermal or Concentration Non-Equilibrium

The paper addresses the problem of the existence and quantification of the exergy of non-equilibrium systems. Assuming that both energy and exergy are a priori concepts, the Gibbs “available energy” A is calculated for arbitrary temperature or concentration distributions across the body, with an acc...

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Main Authors: Enrico Sciubba, Federico Zullo
Format: Article
Language:English
Published: MDPI AG 2017-06-01
Series:Entropy
Subjects:
Online Access:http://www.mdpi.com/1099-4300/19/6/263
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spelling doaj-8e61ce2c552841cca33b53317cd7b06f2020-11-25T01:09:04ZengMDPI AGEntropy1099-43002017-06-0119626310.3390/e19060263e19060263Exergy Dynamics of Systems in Thermal or Concentration Non-EquilibriumEnrico Sciubba0Federico Zullo1Department of Mechanical and Aerospace Engineering, Sapienza University of Rome, 00184 Roma, ItalyDepartment of Mathematics and Physics, Università Degli Studi Roma Tre, 00146 Roma, ItalyThe paper addresses the problem of the existence and quantification of the exergy of non-equilibrium systems. Assuming that both energy and exergy are a priori concepts, the Gibbs “available energy” A is calculated for arbitrary temperature or concentration distributions across the body, with an accuracy that depends only on the information one has of the initial distribution. It is shown that A exponentially relaxes to its equilibrium value, and it is then demonstrated that its value is different from that of the non-equilibrium exergy, the difference depending on the imposed boundary conditions on the system and thus the two quantities are shown to be incommensurable. It is finally argued that all iso-energetic non-equilibrium states can be ranked in terms of their non-equilibrium exergy content, and that each point of the Gibbs plane corresponds therefore to a set of possible initial distributions, each one with its own exergy-decay history. The non-equilibrium exergy is always larger than its equilibrium counterpart and constitutes the “real” total exergy content of the system, i.e., the real maximum work extractable from the initial system. A systematic application of this paradigm may be beneficial for meaningful future applications in the fields of engineering and natural science.http://www.mdpi.com/1099-4300/19/6/263non-equilibrium thermodynamicsexergynon-equilibrium diffusion
collection DOAJ
language English
format Article
sources DOAJ
author Enrico Sciubba
Federico Zullo
spellingShingle Enrico Sciubba
Federico Zullo
Exergy Dynamics of Systems in Thermal or Concentration Non-Equilibrium
Entropy
non-equilibrium thermodynamics
exergy
non-equilibrium diffusion
author_facet Enrico Sciubba
Federico Zullo
author_sort Enrico Sciubba
title Exergy Dynamics of Systems in Thermal or Concentration Non-Equilibrium
title_short Exergy Dynamics of Systems in Thermal or Concentration Non-Equilibrium
title_full Exergy Dynamics of Systems in Thermal or Concentration Non-Equilibrium
title_fullStr Exergy Dynamics of Systems in Thermal or Concentration Non-Equilibrium
title_full_unstemmed Exergy Dynamics of Systems in Thermal or Concentration Non-Equilibrium
title_sort exergy dynamics of systems in thermal or concentration non-equilibrium
publisher MDPI AG
series Entropy
issn 1099-4300
publishDate 2017-06-01
description The paper addresses the problem of the existence and quantification of the exergy of non-equilibrium systems. Assuming that both energy and exergy are a priori concepts, the Gibbs “available energy” A is calculated for arbitrary temperature or concentration distributions across the body, with an accuracy that depends only on the information one has of the initial distribution. It is shown that A exponentially relaxes to its equilibrium value, and it is then demonstrated that its value is different from that of the non-equilibrium exergy, the difference depending on the imposed boundary conditions on the system and thus the two quantities are shown to be incommensurable. It is finally argued that all iso-energetic non-equilibrium states can be ranked in terms of their non-equilibrium exergy content, and that each point of the Gibbs plane corresponds therefore to a set of possible initial distributions, each one with its own exergy-decay history. The non-equilibrium exergy is always larger than its equilibrium counterpart and constitutes the “real” total exergy content of the system, i.e., the real maximum work extractable from the initial system. A systematic application of this paradigm may be beneficial for meaningful future applications in the fields of engineering and natural science.
topic non-equilibrium thermodynamics
exergy
non-equilibrium diffusion
url http://www.mdpi.com/1099-4300/19/6/263
work_keys_str_mv AT enricosciubba exergydynamicsofsystemsinthermalorconcentrationnonequilibrium
AT federicozullo exergydynamicsofsystemsinthermalorconcentrationnonequilibrium
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