{"data":{"id":"10.6084/m9.figshare.6857777","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6857777","prefix":"10.6084","suffix":"m9.figshare.6857777","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Nieva, Nicolás","nameType":"Personal","givenName":"Nicolás","familyName":"Nieva","affiliation":[],"nameIdentifiers":[]},{"name":"Tolosa, Martín Rodrigo","nameType":"Personal","givenName":"Martín Rodrigo","familyName":"Tolosa","affiliation":[],"nameIdentifiers":[]},{"name":"Corvalán, Carolina","nameType":"Personal","givenName":"Carolina","familyName":"Corvalán","affiliation":[],"nameIdentifiers":[]},{"name":"Arias, Delia","nameType":"Personal","givenName":"Delia","familyName":"Arias","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Diagrama de fases experimental Fe-Sn-Zr. Nuevos resultados del corte isotérmico de 800 °C"}],"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/s1517-707620180002.0373","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["1340892 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 The Zr-based alloys are extensively applied in the field of nuclear technology. Alloyed with Sn and Fe, Zr is the main element in the zircaloy-type alloys, currently vastly used as structural elements and as containers of burnable elements in nuclear reactors. This ternary metallurgical system is also a component of more recently developed alloys such as Zirlo (USA). Although Zr is a major component in all of them, it is most important to know the phase diagrams of their components as best as possible. The Fe-Sn-Zr phase diagram has been systematically studied by our research team for many years. Considerable advancement has been made in the design of the phase diagram at 800°C, however, some regions in the Gibbs triangle are still unsolved. In order to evaluate these regions experimentally, a ternary alloy set was designed and prepared. These alloys were thermally treated at the chosen temperature for 2928 hours, and characterized by applying metallography techniques, X-ray diffraction and microanalysis. The presence of Y and Fe6Sn6Zr was confirmed, the presence of phase X” was verified, and 2- and 3-phase existence fields were determined. Finally, phase balance boundaries in the regions under study were traced, completing, to a great extent, the phase diagram for the isothermal cut analysed.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://scielo.figshare.com/articles/Diagrama_de_fases_experimental_Fe-Sn-Zr_Nuevos_resultados_del_corte_isot_rmico_de_800_C/6857777","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","reason":null,"vi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