{"data":{"id":"10.6084/m9.figshare.6968138.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6968138.v1","prefix":"10.6084","suffix":"m9.figshare.6968138.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Lopez-Hirata, Victor Manuel","givenName":"Victor Manuel","familyName":"Lopez-Hirata","affiliation":[],"nameIdentifiers":[]},{"name":"Hernandez-Santiago, Felipe","givenName":"Felipe","familyName":"Hernandez-Santiago","affiliation":[],"nameIdentifiers":[]},{"name":"Saucedo-Muñoz, Maribel Leticia","givenName":"Maribel Leticia","familyName":"Saucedo-Muñoz","affiliation":[],"nameIdentifiers":[]},{"name":"Dorantes-Rosales, Hector Javier","givenName":"Hector Javier","familyName":"Dorantes-Rosales","affiliation":[],"nameIdentifiers":[]},{"name":"Paniagua-Mercado, Ana Maria","givenName":"Ana Maria","familyName":"Paniagua-Mercado","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Analysis of β´(Cu4Ti) Precipitation During Isothermal Aging of a Cu-4wt.%Ti Alloy"}],"publisher":"SciELO journals","container":{},"publicationYear":2018,"subjects":[{"subject":"90499 Chemical Engineering not elsewhere classified","schemeUri":"http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E","subjectScheme":"FOR"},{"subject":"FOS: Chemical engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"91207 Metals and Alloy Materials","schemeUri":"http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E","subjectScheme":"FOR"},{"subject":"FOS: Materials engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"91299 Materials Engineering not elsewhere classified","schemeUri":"http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E","subjectScheme":"FOR"}],"contributors":[],"dates":[{"date":"2018-08-15","dateType":"Created"},{"date":"2022-06-07","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-2018-0121","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.6968138","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["3396343 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":"This work analyzed experimental and numerically the growth kinetics of β´precipitation of a Cu-4wt.%Ti alloy after aging at 400, 500 and 600 ºC for times from 0.0166 h to 200 h. Results indicated that the precipitation process is almost controlled by nucleation and growth during aging at 400 ºC, originating a slow growth kinetics of precipitation. In contrast, the coarsening of precipitates dominates the precipitation process during aging at 500 and 600 ºC. The interfacial energy of interface between the a matrix phase and β´ precipitates was determined to be about 0.1135, 0.0980 and 0.0725 Jm-2 for aging at 400, 500 and 600 ºC, respectively. These values suggest a coherent interface which is in agreement with the flat faces of β´ cuboid precipitates. Calculated Time-Temperature-Precipitation diagram for the β´ precipitation indicated good agreement with experimental results. Precipitation hardening was higher for the slower growth kinetics of precipitation.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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