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dc.contributorState Key Laboratory of Powder Metallurgy, Central South University, Changsha Chinaen_US
dc.contributorDepartment of Materials Science and Engineering, The Pennsylvania State University, University Park, PA USA
dc.contributorState Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai, China
dc.contributor.authorDu, Y.
dc.contributor.authorLiu, Shuhong
dc.contributor.authorLiu, Z.-K.
dc.contributor.authorShang, S.-L.
dc.contributor.authorWang, Jiang
dc.contributor.authorWang, Peisheng
dc.contributor.authorXu, Honghui
dc.contributor.authorZhang, L.
dc.contributor.authorZhang, Weiqing
dc.contributor.otherliu@matse.psu.eduen_US
dc.date.accessioned2013-03-30T13:59:04Z
dc.date.accessioned2015-08-05T17:49:35Z
dc.date.available2013-03-30T13:59:04Z
dc.date.available2015-08-05T17:49:35Z
dc.date.issued2013-03-30
dc.identifier.citationCalphad Volume 35, Issue 2, June 2011, Pages 191–203en_US
dc.identifier.urihttp://hdl.handle.net/11115/85
dc.description.abstractThe isothermal section of the Cu–Si–Zn ternary system at 600 °C was experimentally determined with fifteen alloys by means of optical microscopy, X-ray diffraction, and the scanning electron microscopy with energy dispersive X-ray spectroscopy. At 600 °C, no ternary compounds were observed, and five three-phase equilibria were well determined. In particular, the longstanding controversy regarding the four three-phase equilibria in the Cu-rich corner involving the phases α, β, γ- Cu5Zn8, and κ- Cu7Si was resolved experimentally in the present work. In an effort to provide a compatible thermodynamic description of the Cu–Si–Zn system for the multi-component Al-based thermodynamic database, the Cu–Zn system was remodeled using the CALPHAD approach with a new sublattice model Zn4(Cu,Zn)1(Cu,Zn)8 for the γ- Cu5Zn8 phase. Besides, the temperature dependence of enthalpy of mixing was also taken into account for the liquid phase. Subsequently, a thermodynamic description of the Cu–Si–Zn system was obtained over the entire composition range based on the presently modeled Cu–Zn system and the experimental data from the literature and the present measurements. It is found that most reliable experimental data in this ternary system are satisfactorily reproduced by the present thermodynamic modeling.en_US
dc.description.sponsorshipNational Natural Science Foundation of China Creative Research Group No. 51021063 ; National Basic Research Program of China No. 2011CB610401 ; National Natural Science Foundation of China Key Program No. 50831007 ; National Natural Science Foundation of China Nos. 50971135 and 51028101 ; State Key Laboratory of High Performance Ceramics and Superfine Microstructure Shanghai Institute of Ceramics No. SKL200801SIC ; Ministry of Education of China over-sea student fellowship No. [2009] 3012 ; US National Science Foundation DMR-1006557en_US
dc.relation.urihttp://dx.doi.org/10.1016/j.calphad.2011.02.001en_US
dc.rightsAttribution-ShareAlike 3.0 United States*
dc.rights.urihttp://creativecommons.org/licenses/by-sa/3.0/us/*
dc.subjectCu-Si-Znen_US
dc.subjectDiamond_A4
dc.subjectGamma
dc.subjectFile Repository Categories::Phases::Disordered::BCC_A2
dc.subjectFile Repository Categories::Phases::Disordered::FCC_A1
dc.subjectFile Repository Categories::Phases::Disordered::HCP_A3
dc.subjectFile Repository Categories::Phases::Intermetallics
dc.subjectFile Repository Categories::Phases::Intermetallics::BCC_B2
dc.subjectFile Repository Categories::Phases::Liquid
dc.subjectFile Repository Categories::Property Classes::Thermodynamics
dc.titleCu–Si–Zn and Cu–Zn Experimental investigation and thermodynamic modelingen_US
dc.typeFunctional Descriptionen_US


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