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A simple example illustrating the application of thermodynamic extremum principles

dc.contributor.authorVelasco Maíllo, Santiago
dc.contributor.authorFernández Pineda, Cristóbal
dc.date.accessioned2023-06-20T18:53:17Z
dc.date.available2023-06-20T18:53:17Z
dc.date.issued2002-09
dc.descriptionSV thanks the Comisión Interministerial de Ciencia y Tecnología (CICYT) of Spain for financial support under grant nº PB 98-0261 and the Junta de CyL-FSE of Spain for financial support under grant nº SA097/01.
dc.description.abstractA composite system consisting of two identical ideal gases separated by a movable, frictionless, diathermic piston is used to illustrate the application of different extremum principles in thermodynamics. The time evolution of the system from an initial constrained equilibrium state to the final equilibrium state is analysed by means of a very simple phenomenological model.
dc.description.departmentDepto. de Estructura de la Materia, Física Térmica y Electrónica
dc.description.facultyFac. de Ciencias Físicas
dc.description.refereedTRUE
dc.description.sponsorshipComisión Interministerial de Ciencia y Tecnología (CICYT) of Spain
dc.description.sponsorshipJunta de CyL-FSE of Spain
dc.description.statuspub
dc.eprint.idhttps://eprints.ucm.es/id/eprint/23651
dc.identifier.doi10.1088/0143-0807/23/5/307
dc.identifier.issn0143-0807
dc.identifier.officialurlhttp://dx.doi.org/10.1088/0143-0807/23/5/307
dc.identifier.relatedurlhttp://iopscience.iop.org/
dc.identifier.urihttps://hdl.handle.net/20.500.14352/58863
dc.issue.number5
dc.journal.titleEuropean Journal of Physics
dc.language.isoeng
dc.page.final511
dc.page.initial501
dc.publisherIOP Publishing Ltd.
dc.relation.projectIDPB 98-0261
dc.relation.projectIDSA 097/01
dc.rights.accessRightsopen access
dc.subject.cdu536
dc.subject.ucmTermodinámica
dc.subject.unesco2213 Termodinámica
dc.titleA simple example illustrating the application of thermodynamic extremum principles
dc.typejournal article
dc.volume.number23
dcterms.references[1] Gibbs J W 1961 The Scientific Papers of J W Gibbs Thermodynamics vol 1 (New York: Dover) p 56, 65 [2] Tisza L 1966 Generalized Thermodynamics (Cambridge, MA: MIT Press) pp 41–8 [3] Kestin J V 1979 A Course of Thermodynamics vol 2 (New York: McGraw-Hill) ch 14 (revised printing) [4] Callen H B 1985 Thermodynamics and an Introduction to Thermostatistics 2nd edn (New York: Wiley) ch 5, 8 [5] Bailyn M V A Survey of Thermodynamics (New York: American Institute of Physics) pp 223–32 [6] Kazes E and Cutler P H 1988 Implications of the entropy maximum principle Am. J. Phys. 56 560–1 [7] Bailyn M V A Survey of Thermodynamics (New York: American Institute of Physics) p 236 [8] Dunning-Davies J 1993 Comment on ‘Implications of the entropy maximum principle’ by Kazes E and Cutler P H 1988 (Am. J. Phys. 56 560–1)’ Am. J. Phys. 61 88–9 [9] Fernández-Pineda C and Velasco S 2001 Application of thermodynamic extremum principles Am. J. Phys. 69 1160–5 [10] Bazarov I P 1964 Thermodynamics (Oxford: Pergamon) p 158 [11] Callen H B 1985 Thermodynamics and an Introduction to Thermostatistics 2nd edn (New York: Wiley) ch 5, 8 pp 66–8 [12] Gruber Ch 1999 Thermodynamics of systems with internal adiabatic constraints: time evolution of the adiabatic piston Eur. J. Phys. 20 259–66 [13] Gruber Ch and Frachebourg L 1999 On the adiabatic properties of a stochastic adiabatic wall: evolution, stationary non-equilibrium, and equilibrium states Physica A 272 392–428
dspace.entity.typePublication
relation.isAuthorOfPublicationae625a23-ad7c-4def-ac08-a08f29fbf9c6
relation.isAuthorOfPublication.latestForDiscoveryae625a23-ad7c-4def-ac08-a08f29fbf9c6

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