{"data":{"id":"10.6084/m9.figshare.6273791","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6273791","prefix":"10.6084","suffix":"m9.figshare.6273791","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Djordjević, Aleksandar","nameType":"Personal","givenName":"Aleksandar","familyName":"Djordjević","affiliation":[],"nameIdentifiers":[]},{"name":"Premović, Milena","nameType":"Personal","givenName":"Milena","familyName":"Premović","affiliation":[],"nameIdentifiers":[]},{"name":"Duško Minić","affiliation":[],"nameIdentifiers":[]},{"name":"Ćosović, Vladan","nameType":"Personal","givenName":"Vladan","familyName":"Ćosović","affiliation":[],"nameIdentifiers":[]},{"name":"Živković, Milutin","nameType":"Personal","givenName":"Milutin","familyName":"Živković","affiliation":[],"nameIdentifiers":[]},{"name":"Manasijević, Dragan","nameType":"Personal","givenName":"Dragan","familyName":"Manasijević","affiliation":[],"nameIdentifiers":[]},{"name":"Kolarević, Milan","nameType":"Personal","givenName":"Milan","familyName":"Kolarević","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Experimental Evaluation of 300 ºC section of Cu-In-Ni Phase Diagram, Hardness and Electrical Conductivity of Selected Alloy"}],"publisher":"SciELO journals","container":{},"publicationYear":2018,"subjects":[{"subject":"90499 Chemical Engineering not elsewhere classified","subjectScheme":"FOR"},{"subject":"FOS: Chemical engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Chemical engineering","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"91207 Metals and Alloy Materials","subjectScheme":"FOR"},{"subject":"FOS: Materials engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Materials engineering","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"91299 Materials Engineering not elsewhere classified","subjectScheme":"FOR"}],"contributors":[],"dates":[{"date":"2018-05-16","dateType":"Created"},{"date":"2018-05-16","dateType":"Updated"},{"date":"2018","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsSupplementTo","relatedIdentifier":"10.1590/1980-5373-mr-2017-0699","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["2636939 Bytes"],"formats":[],"version":null,"rightsList":[{"rights":"Creative Commons Attribution 4.0 International","rightsUri":"https://creativecommons.org/licenses/by/4.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc-by-4.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"The paper reports comparative experimental and thermodynamic calculation of a Cu-In-Ni ternary system. An isothermal section of the Cu-In-Ni system at 300 ºC was extrapolated using optimized thermodynamic parameters for the constitutive binary systems from literature. Microstructural and phase composition analysis were carried out using scanning electron microscopy coupled with energy dispersive spectrometry (SEM-EDS) and X-ray powder diffraction (XRD) technique. Brinell hardness and electrical conductivity of a selected number of alloy samples with compositions along three vertical sections (Cu-In0.5Ni0.5, In-Cu0.8Ni0.2, and x(In) = 0.4) of the studied Cu-In-Ni system were experimentally determined. Based on the obtained experimental results and by using appropriate mathematical models values of hardness and electrical conductivity for the whole ternary system were predicted. A close agreement between calculations and experimental results was obtained both in case of thermodynamic, electrical conductivity and hardness predictions.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://scielo.figshare.com/articles/Experimental_Evaluation_of_300_C_section_of_Cu-In-Ni_Phase_Diagram_Hardness_and_Electrical_Conductivity_of_Selected_Alloy/6273791","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":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