{"data":{"id":"10.6084/m9.figshare.6273137","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6273137","prefix":"10.6084","suffix":"m9.figshare.6273137","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Rocha, Eduardo José Fernandes","nameType":"Personal","givenName":"Eduardo José Fernandes","familyName":"Rocha","affiliation":[],"nameIdentifiers":[]},{"name":"Antonino, Tiago De Sousa","nameType":"Personal","givenName":"Tiago De Sousa","familyName":"Antonino","affiliation":[],"nameIdentifiers":[]},{"name":"Guimarães, Pablo Batista","nameType":"Personal","givenName":"Pablo Batista","familyName":"Guimarães","affiliation":[],"nameIdentifiers":[]},{"name":"Ferreira, Ricardo Artur Sanguinetti","nameType":"Personal","givenName":"Ricardo Artur Sanguinetti","familyName":"Ferreira","affiliation":[],"nameIdentifiers":[]},{"name":"Barbosa, José Maria Andrade","nameType":"Personal","givenName":"José Maria Andrade","familyName":"Barbosa","affiliation":[],"nameIdentifiers":[]},{"name":"Janardan Rohatgi","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Modeling of the temperature field generated by the deposition of weld bead on a steel butt joint by FEM techniques and thermographic images."}],"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-2016-0796","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["2681416 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 aim of this work is to predict the temperature field generated by welding a steel butt joint (API 5L X80). The prediction was modeled by finite element software Abaqus where the subroutine was developed in Fortran so that heat source motion may be included. The motion was based on the Goldak's double ellipsoid. In the model material nonlinearities were included such as thermophysical properties (coefficient of thermal expansion, specific heat, thermal diffusivity and thermal conductivity), which are dependent on temperature and latent heat, heat exchange by convection and radiation and mechanical boundary conditions. The thermal field predicted by the model was validated by infrared thermography. GMAW simulations with the use of an \"evenmatched\" solid wire (filler metal) carried out the welding process. The results obtained from the numerical model and thermography were in good agreement.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://scielo.figshare.com/articles/Modeling_of_the_temperature_field_generated_by_the_deposition_of_weld_bead_on_a_steel_butt_joint_by_FEM_techniques_and_thermographic_images_/6273137","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,"part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