{"data":{"id":"10.6084/m9.figshare.6857510.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6857510.v1","prefix":"10.6084","suffix":"m9.figshare.6857510.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Leonard, Martín Eduardo","nameType":"Personal","givenName":"Martín Eduardo","familyName":"Leonard","affiliation":[],"nameIdentifiers":[]},{"name":"Signorelli, Javier Walter","nameType":"Personal","givenName":"Javier Walter","familyName":"Signorelli","affiliation":[],"nameIdentifiers":[]},{"name":"Stout, Michael George","nameType":"Personal","givenName":"Michael George","familyName":"Stout","affiliation":[],"nameIdentifiers":[]},{"name":"Roatta, Analía","nameType":"Personal","givenName":"Analía","familyName":"Roatta","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Time-dependent methods for limit strains determination of sheet metal"}],"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/s1517-707620180002.0332","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.6857510","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["1213800 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 forming limit diagram (FLD) –broadly used to characterize sheet-metal formability– is made by means of strain measurement over the surface of stretched samples and the subsequent determination of limit-strain values associated with the onset of necking. Currently, researchers can make strain measurements with digital image-correlation analysis (DIC). Data measured by DIC easily adapt to the traditional position-dependent method for evaluating limit strains, but this method is not applicable to materials that exhibit inhomogeneous deformation, like multiple necking. DIC analysis allows for the application of time-dependent methods, which are based on analysis of the temporal evolution of strains to define the onset of necking. This article compares three recently proposed time-dependent techniques for determining limit strains: a thickness-control method, the strain-control method and an acceleration-correlation method. For experimental purposes, duplex 2205 stainless-steel sheet, 0.92mm thick, was tested in uniaxial tension. The standard position-dependent method (ISO 12004-2) provides a reference for comparing results. We attribute differences in limit-strain values to the difficulty in objectively setting each method’s parameters. These differences show that there are still aspects of the temporal analyses that must be improved on before a precise and generalized methodology is available.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://scielo.figshare.com/articles/Time-dependent_methods_for_limit_strains_determination_of_sheet_metal/6857510/1","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOverTime":[],"referenceCount":1,"citationCount":0,"citationsOverTime":[],"partCount":0,"partOfCount":0,"versionCount":0,"versionOfCount":0,"created":"2018-07-25T02:51:32.000Z","registered":"2018-07-25T02:52:53.000Z","published":"2018","updated":"2020-08-28T16:24:14.000Z"},"relationships":{"client":{"data":{"id":"figshare.ars","type":"clients"}},"provider":{"data":{"id":"otjm","type":"providers"}},"media":{"data":{"id":"10.6084/m9.figshare.6857510.v1","type":"media"}},"references":{"data":[{"id":"10.1590/s1517-707620180002.0332","type":"dois"}]},"citations":{"data":[]},"parts":{"data":[]},"partOf":{"data":[]},"versions":{"data":[]},"versionOf":{"data":[]}}}}