{"data":{"id":"10.6084/m9.figshare.6857513","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6857513","prefix":"10.6084","suffix":"m9.figshare.6857513","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Kociubzyk, Alex Iván","nameType":"Personal","givenName":"Alex Iván","familyName":"Kociubzyk","affiliation":[],"nameIdentifiers":[]},{"name":"Rozicki, Roberto Samuel","nameType":"Personal","givenName":"Roberto Samuel","familyName":"Rozicki","affiliation":[],"nameIdentifiers":[]},{"name":"Ares, Alicia Esther","nameType":"Personal","givenName":"Alicia Esther","familyName":"Ares","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Movement of the interphases during the horizontal solidification of tin-zinc alloys"}],"publisher":"SciELO journals","container":{},"publicationYear":2018,"subjects":[{"subject":"90502 Construction Engineering","subjectScheme":"FOR"},{"subject":"FOS: Civil engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Civil 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":"2018-07-25","dateType":"Created"},{"date":"2018-07-25","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/s1517-707620180002.0330","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["2465187 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":"ABSTRACT Solidification processing is one of the important routes to produce materials, especially metals and alloys. The parameters for the transformation from liquid to solid, such as the temperature gradient, the growth rate, the cooling rate, the interphase velocity, vary from process to process and in one process also as a function of time and space. These variations together with the different alloy compositions, lead to a multitude of microstructures and therefore, affect the behavior of the material. In this work the evolution of the interphases is studied in Sn-Zn (Sn-6wt.% Zn (hypoeutectic) and Sn-15wt.% Zn (hypereutectic)) when the specimens were unidirectionally horizontally solidified through heat extraction in two opposite directions. Sn-Zn specimens shaped in cylindrical segments were obtained, with an average length between 13 cm-17 cm, an average width between 3 cm-3.2 cm and an average thickness of 0.8 cm – 1.2 cm, depending on the experience. The thermal parameters (cooling rates, temperature gradients, positions and velocities of the present interfaces) were determined and related to the final structures resulting from the solidification. It was found that the value of the velocity of the interphase is maximum when opposing fronts of solidification collide, advancing in opposite directions in the specimens. The values were superior to 2 mm/s for both analyzed Sn-Zn alloys.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://scielo.figshare.com/articles/Movement_of_the_interphases_during_the_horizontal_solidification_of_tin-zinc_alloys/6857513","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","re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