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dc.contributor.authorBallikaya, Sedat
dc.contributor.authorChi, Hang
dc.contributor.authorSalvador, James R.
dc.contributor.authorUher, Ctirad
dc.date.accessioned2021-03-05T09:13:44Z
dc.date.available2021-03-05T09:13:44Z
dc.date.issued2013
dc.identifier.citationBallikaya S., Chi H., Salvador J. R. , Uher C., "Thermoelectric properties of Ag-doped Cu2Se and Cu2Te", JOURNAL OF MATERIALS CHEMISTRY A, cilt.1, ss.12478-12484, 2013
dc.identifier.issn2050-7488
dc.identifier.othervv_1032021
dc.identifier.otherav_9ce2b043-18bd-4763-afea-ce43123c8b20
dc.identifier.urihttp://hdl.handle.net/20.500.12627/105408
dc.identifier.urihttps://doi.org/10.1039/c3ta12508d
dc.description.abstractCu2Se, Cu2Te and Ag-overstoichiometric compounds Cu1.98Ag0.2Se and Cu1.98Ag0.2Te were prepared by melting, annealing, followed by spark plasma sintering compaction. Low and high temperature thermoelectric properties were investigated by measuring the electrical conductivity, Seebeck coefficient, thermal conductivity and Hall coefficient between 2 K and 900 K. Structural analyses were performed by PXRD and SEM-EDX analyses. The Hall and Seebeck coefficients show that holes are the dominant carrier in all compounds. High temperature alpha-beta phase transition in Cu2Se and Cu1.98Ag0.2Se between 350 and 400 K and multiple phase transitions (alpha-beta, beta-gamma, gamma-delta, delta-is an element of) in Cu2Te and Cu1.98Ag0.2Te between 350 K and 900 K were observed in measurements of heat capacity, temperature dependent PXRD data, and transport coefficients. Low temperature transport measurements (Hall coefficient, electrical conductivity, carrier mobility) strongly suggest the presence of yet another phase transition in Cu2Se, Cu1.98Ag0.2Se, and Cu1.98Ag0.2Te compounds at temperatures between 85 K and 115 K, reported here for the first time. Based on the transport data and structural analysis we conclude that doping Cu2Se and Cu2Te by Ag reduces the density of holes and strongly suppresses the thermal conductivity not only due to a smaller electronic contribution but also due to enhanced point defect scattering of phonons that reduces the lattice portion of the thermal conductivity. Moreover, the phase transition temperature is shifted to lower temperatures upon doping with Ag. The presence of Ag enhances thermoelectric performance of Cu2Te at all temperatures and Cu2Se benefits from Ag doping over a broad range of temperatures up to 700 K. The maximum ZT value of 1.2 at 900 K; 0.52 at 650 K; 0.29 at 900 K; and 1.0 at 900 K were achieved for Cu2Se, Cu1.98Ag0.2Se, Cu2Te and Cu1.98Ag0.2Te, respectively, between 2 K and 900 K.
dc.language.isoeng
dc.subjectZiraat
dc.subjectTarımda Enerji
dc.subjectBiyoyakıt Teknolojisi
dc.subjectFizikokimya
dc.subjectTemel Bilimler
dc.subjectMühendislik ve Teknoloji
dc.subjectKİMYA, FİZİKSEL
dc.subjectKimya
dc.subjectTemel Bilimler (SCI)
dc.subjectENERJİ VE YAKITLAR
dc.subjectMühendislik
dc.subjectMühendislik, Bilişim ve Teknoloji (ENG)
dc.subjectMALZEME BİLİMİ, MULTIDISCIPLINARY
dc.subjectMalzeme Bilimi
dc.subjectTarımsal Bilimler
dc.subjectTarım Makineleri
dc.titleThermoelectric properties of Ag-doped Cu2Se and Cu2Te
dc.typeMakale
dc.relation.journalJOURNAL OF MATERIALS CHEMISTRY A
dc.contributor.departmentUniversity of Michigan System , ,
dc.identifier.volume1
dc.identifier.issue40
dc.identifier.startpage12478
dc.identifier.endpage12484
dc.contributor.firstauthorID81722


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