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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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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