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Thermal irreversibility demystified
International Journal of Numerical Methods for Heat and Fluid Flow, Volume: 33, Issue: 2
Swansea University Author: Rajesh Ransing
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DOI (Published version): 10.1108/hff-02-2022-0079
Abstract
Purpose: This study aims to understand the difference between irreversibility in heat and work transfer processes. It also aims to explain that Helmholtz or Gibbs energy does not represent ‘free’ energy but is a measure of loss of Carnot (reversible) work opportunity. Approach: The entropy of mass i...
Published in: | International Journal of Numerical Methods for Heat and Fluid Flow |
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ISSN: | 0961-5539 0961-5539 |
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2022
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URI: | https://cronfa.swan.ac.uk/Record/cronfa60760 |
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<?xml version="1.0" encoding="utf-8"?><rfc1807 xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:xsd="http://www.w3.org/2001/XMLSchema"><bib-version>v2</bib-version><id>60760</id><entry>2022-08-05</entry><title>Thermal irreversibility demystified</title><swanseaauthors><author><sid>0136f9a20abec3819b54088d9647c39f</sid><ORCID>0000-0003-4848-4545</ORCID><firstname>Rajesh</firstname><surname>Ransing</surname><name>Rajesh Ransing</name><active>true</active><ethesisStudent>false</ethesisStudent></author></swanseaauthors><date>2022-08-05</date><deptcode>ACEM</deptcode><abstract>Purpose: This study aims to understand the difference between irreversibility in heat and work transfer processes. It also aims to explain that Helmholtz or Gibbs energy does not represent ‘free’ energy but is a measure of loss of Carnot (reversible) work opportunity. Approach: The entropy of mass is described as the net temperature-standardised heat transfer to mass under ideal conditions measured from a datum value. An expression for the ‘irreversibility’, is derived in terms of work loss (Wloss) in a work transfer process, unaccounted heat dissipation (Qloss) in a heat transfer process and loss of net Carnot work (CWnet) opportunity resulting from spontaneous heat transfer across a finite temperature difference during the process. The thermal irreversibility is attributed to not exploiting the capability for extracting work by interposing a combination of Carnot engine(s) and/or Carnot heat pump(s) that exchanges heat with the surrounding and operates across the finite temperature difference. Findings: It is shown, with an example, how the contribution of thermal irreversibility, in estimating reversible input work, amounts to a loss of an opportunity to generate net work output. The opportunity is created by exchanging heat with surroundings whilst transferring the same amount of heat across finite temperature difference. An entropy change is determined with a numerical simulation including calculation of local entropy generation values and results are compared with estimates based on an analytical expression.Originality: A new interpretation of entropy combined with an enhanced mental image of a combination of Carnot engine(s) and/or Carnot heat pump(s) is used to quantify thermal irreversibility.</abstract><type>Journal Article</type><journal>International Journal of Numerical Methods for Heat and Fluid Flow</journal><volume>33</volume><journalNumber>2</journalNumber><paginationStart/><paginationEnd/><publisher>Emerald</publisher><placeOfPublication/><isbnPrint/><isbnElectronic/><issnPrint>0961-5539</issnPrint><issnElectronic>0961-5539</issnElectronic><keywords>Entropy; Entransy; Exergy Destruction; Entropy Generation; The Second Law of Thermodynamics; Irreversibility.</keywords><publishedDay>14</publishedDay><publishedMonth>10</publishedMonth><publishedYear>2022</publishedYear><publishedDate>2022-10-14</publishedDate><doi>10.1108/hff-02-2022-0079</doi><url/><notes/><college>COLLEGE NANME</college><department>Aerospace, Civil, Electrical, and Mechanical Engineering</department><CollegeCode>COLLEGE CODE</CollegeCode><DepartmentCode>ACEM</DepartmentCode><institution>Swansea University</institution><apcterm>Not Required</apcterm><funders/><projectreference/><lastEdited>2024-07-09T11:05:55.4310534</lastEdited><Created>2022-08-05T14:08:29.7018312</Created><path><level id="1">Faculty of Science and Engineering</level><level id="2">School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering</level></path><authors><author><firstname>Rajesh</firstname><surname>Ransing</surname><orcid>0000-0003-4848-4545</orcid><order>1</order></author></authors><documents><document><filename>60760__25134__a3b4d10cc0984c638156306dc40c3c53.pdf</filename><originalFilename>60760.pdf</originalFilename><uploaded>2022-09-14T11:51:15.7362252</uploaded><type>Output</type><contentLength>1529648</contentLength><contentType>application/pdf</contentType><version>Accepted Manuscript</version><cronfaStatus>true</cronfaStatus><documentNotes>Released under the terms of a Creative Commons Attribution Non-Commercial License (CC-BY-NC) License.</documentNotes><copyrightCorrect>true</copyrightCorrect><language>eng</language><licence>https://creativecommons.org/licenses/by-nc/4.0/</licence></document></documents><OutputDurs/></rfc1807> |
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v2 60760 2022-08-05 Thermal irreversibility demystified 0136f9a20abec3819b54088d9647c39f 0000-0003-4848-4545 Rajesh Ransing Rajesh Ransing true false 2022-08-05 ACEM Purpose: This study aims to understand the difference between irreversibility in heat and work transfer processes. It also aims to explain that Helmholtz or Gibbs energy does not represent ‘free’ energy but is a measure of loss of Carnot (reversible) work opportunity. Approach: The entropy of mass is described as the net temperature-standardised heat transfer to mass under ideal conditions measured from a datum value. An expression for the ‘irreversibility’, is derived in terms of work loss (Wloss) in a work transfer process, unaccounted heat dissipation (Qloss) in a heat transfer process and loss of net Carnot work (CWnet) opportunity resulting from spontaneous heat transfer across a finite temperature difference during the process. The thermal irreversibility is attributed to not exploiting the capability for extracting work by interposing a combination of Carnot engine(s) and/or Carnot heat pump(s) that exchanges heat with the surrounding and operates across the finite temperature difference. Findings: It is shown, with an example, how the contribution of thermal irreversibility, in estimating reversible input work, amounts to a loss of an opportunity to generate net work output. The opportunity is created by exchanging heat with surroundings whilst transferring the same amount of heat across finite temperature difference. An entropy change is determined with a numerical simulation including calculation of local entropy generation values and results are compared with estimates based on an analytical expression.Originality: A new interpretation of entropy combined with an enhanced mental image of a combination of Carnot engine(s) and/or Carnot heat pump(s) is used to quantify thermal irreversibility. Journal Article International Journal of Numerical Methods for Heat and Fluid Flow 33 2 Emerald 0961-5539 0961-5539 Entropy; Entransy; Exergy Destruction; Entropy Generation; The Second Law of Thermodynamics; Irreversibility. 14 10 2022 2022-10-14 10.1108/hff-02-2022-0079 COLLEGE NANME Aerospace, Civil, Electrical, and Mechanical Engineering COLLEGE CODE ACEM Swansea University Not Required 2024-07-09T11:05:55.4310534 2022-08-05T14:08:29.7018312 Faculty of Science and Engineering School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering Rajesh Ransing 0000-0003-4848-4545 1 60760__25134__a3b4d10cc0984c638156306dc40c3c53.pdf 60760.pdf 2022-09-14T11:51:15.7362252 Output 1529648 application/pdf Accepted Manuscript true Released under the terms of a Creative Commons Attribution Non-Commercial License (CC-BY-NC) License. true eng https://creativecommons.org/licenses/by-nc/4.0/ |
title |
Thermal irreversibility demystified |
spellingShingle |
Thermal irreversibility demystified Rajesh Ransing |
title_short |
Thermal irreversibility demystified |
title_full |
Thermal irreversibility demystified |
title_fullStr |
Thermal irreversibility demystified |
title_full_unstemmed |
Thermal irreversibility demystified |
title_sort |
Thermal irreversibility demystified |
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0136f9a20abec3819b54088d9647c39f |
author_id_fullname_str_mv |
0136f9a20abec3819b54088d9647c39f_***_Rajesh Ransing |
author |
Rajesh Ransing |
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Rajesh Ransing |
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Journal article |
container_title |
International Journal of Numerical Methods for Heat and Fluid Flow |
container_volume |
33 |
container_issue |
2 |
publishDate |
2022 |
institution |
Swansea University |
issn |
0961-5539 0961-5539 |
doi_str_mv |
10.1108/hff-02-2022-0079 |
publisher |
Emerald |
college_str |
Faculty of Science and Engineering |
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Faculty of Science and Engineering |
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Faculty of Science and Engineering |
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School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering{{{_:::_}}}Faculty of Science and Engineering{{{_:::_}}}School of Aerospace, Civil, Electrical, General and Mechanical Engineering - Mechanical Engineering |
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description |
Purpose: This study aims to understand the difference between irreversibility in heat and work transfer processes. It also aims to explain that Helmholtz or Gibbs energy does not represent ‘free’ energy but is a measure of loss of Carnot (reversible) work opportunity. Approach: The entropy of mass is described as the net temperature-standardised heat transfer to mass under ideal conditions measured from a datum value. An expression for the ‘irreversibility’, is derived in terms of work loss (Wloss) in a work transfer process, unaccounted heat dissipation (Qloss) in a heat transfer process and loss of net Carnot work (CWnet) opportunity resulting from spontaneous heat transfer across a finite temperature difference during the process. The thermal irreversibility is attributed to not exploiting the capability for extracting work by interposing a combination of Carnot engine(s) and/or Carnot heat pump(s) that exchanges heat with the surrounding and operates across the finite temperature difference. Findings: It is shown, with an example, how the contribution of thermal irreversibility, in estimating reversible input work, amounts to a loss of an opportunity to generate net work output. The opportunity is created by exchanging heat with surroundings whilst transferring the same amount of heat across finite temperature difference. An entropy change is determined with a numerical simulation including calculation of local entropy generation values and results are compared with estimates based on an analytical expression.Originality: A new interpretation of entropy combined with an enhanced mental image of a combination of Carnot engine(s) and/or Carnot heat pump(s) is used to quantify thermal irreversibility. |
published_date |
2022-10-14T11:05:54Z |
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1804095512823988224 |
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11.035655 |