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dc.contributor.otherUniversidad San Pablo-CEU. Facultad de Farmacia-
dc.creatorAzcondo Sánchez, María Teresa-
dc.creatorOrfila, María-
dc.creatorLinares, María-
dc.creatorMolina, Raúl-
dc.creatorMarugán, Javier-
dc.creatorAmador Elizondo, Ulises Julio-
dc.creatorBoulahya, Khalid-
dc.creatorBotas, Juan Ángel-
dc.creatorSanz, Raúl-
dc.date.accessioned2024-01-10T16:40:26Z-
dc.date.available2024-01-10T16:40:26Z-
dc.date.issued2021-08-09-
dc.identifier.citationVíctor Zapata-Ramírez, Paula Rosendo-Santos, Ulises Amador, Clemens Ritter, Glenn C. Mather, Domingo Pérez-Coll, Optimisation of high-performance, cobalt-free SrFe1-xMoxO3-y cathodes for solid oxide fuel cells prepared by spray pyrolysis, Renewable Energy, 2022 185, 1167-1176. DOI: 10.1016/j.renene.2021.12.121es_ES
dc.identifier.issn2574-0962-
dc.identifier.urihttp://hdl.handle.net/10637/14774-
dc.description.abstractThe oxides Ca0.5Sr0.5CoO3-δ and SrCoO3-δ, which present perovskite or perovskite-related phases in different temperature domains, have been tested as materials for thermochemical energy storage. The first one, Ca0.5Sr0.5CoO3-δ, experiences a reversible phase transition upon consecutive cycles under air flow at a maximum operating temperature of 1196 K. Unfortunately, the heat stored in this process, associated to an oxygen loss/gain and a structural phase transition, is very small hindering its use for thermochemical heat storage. The as-prepared oxide SrCoO3-δ, which displays a brownmillerite structure like the Ca-containing compound, in the first heating step irreversibly segregates some Co3O4 at 823 K to yield a 2H hexagonal-perovskite. This phase reversibly transforms at 1073 K into a cubic-perovskite. These 2H⇄C transition occurs from the second to, at least, thirty cycles. The average absorbed and released heat are ~104.1±0.06 J/g and ~68.8±1.8 J/g, respectively, and therefore SrCoO3-δ presents a high exo/endo ratio. The exergy efficiency is, on average for the 30 cycles performed, as high as 63.9±1.2%. The mechanism of the phase 2H⇄C transition of SrCoO3-δ explains the good performance of this material for thermochemical energy storage.en_EN
dc.formatapplication/pdf-
dc.language.isoen-
dc.publisherAmerican Chemical Society-
dc.relation.ispartofACS Applied Energy Materials-
dc.rightshttp://creativecommons.org/licenses/by-nc-nd/4.0/deed.eses_ES
dc.subjectThermochemical energy storageen_EN
dc.subjectPerovskiteen_EN
dc.subjectBrownmilleriteen_EN
dc.subjectCyclabilityen_EN
dc.subjectThermal hysteresisen_EN
dc.subjectStructural transitionen_EN
dc.subjectRedox processesen_EN
dc.titleThermochemical Energy Storage Using the Phase Transitions Brownmillerite -2H Perovskite - Cubic Perovskite in the CaxSr1–xCoO3−δ (x = 0 and 0.5) Systemen_EN
dc.typeArtículo-
dc.identifier.doi10.1021/acsaem.1c01235-
dc.relation.projectIDProyecto PID2019-
dc.centroUniversidad San Pablo-CEU-
Aparece en las colecciones: Facultad de Farmacia




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