{"data":{"id":"10.4121/uuid:e42844b3-e9f8-420a-b896-d35106530793","type":"dois","attributes":{"doi":"10.4121/uuid:e42844b3-e9f8-420a-b896-d35106530793","prefix":"10.4121","suffix":"uuid:e42844b3-e9f8-420a-b896-d35106530793","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Pascoe, John-Alan","nameType":"Personal","givenName":"John-Alan","familyName":"Pascoe","nameIdentifiers":[{"nameIdentifier":"0000-0003-2771-8285","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]}],"titles":[{"title":"Damage Tolerance of Adhesive Bonds - Dataset Ia"}],"publisher":"TU Delft","container":{},"publicationYear":2014,"subjects":[{"subject":"Construction Materials Performance and Processes","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"8703"},{"subject":"Aerospace Engineering","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"0901"},{"subject":"FOS: Mechanical engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Adhesive Bonding"},{"subject":"Aerospace engineering"},{"subject":"Bonded joints"},{"subject":"Collection: Damage Tolerance of Adhesive Bonds - Datasets"},{"subject":"Crack Propagation"},{"subject":"DCB"},{"subject":"Damage Tolerance"},{"subject":"Double Cantilever Beam"},{"subject":"FM 94 epoxy"},{"subject":"Fatigue Disbond Growth"},{"subject":"Fatigue crack growth"},{"subject":"Fatigue test"},{"subject":"Mode I test"},{"subject":"Strain Energy Release Rate"},{"subject":"dissertation"},{"subject":"Time: March 2013 - July 2014"}],"contributors":[{"name":"Alderliesten, R.C.","nameType":"Personal","givenName":"R.C.","familyName":"Alderliesten","affiliation":[],"contributorType":"Other","nameIdentifiers":[]},{"name":"Benedictus, R.","nameType":"Personal","givenName":"R.","familyName":"Benedictus","affiliation":[],"contributorType":"Other","nameIdentifiers":[]}],"dates":[{"date":"2014-07-21","dateType":"Issued"}],"language":"en","types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"References","relatedIdentifier":"https://doi.org/10.4233/uuid:ebbf552a-ce98-4ab6-b9cc-0b939e12ba8b","relatedIdentifierType":"URL"},{"relationType":"References","relatedIdentifier":"https://doi.org/10.1016/j.engfracmech.2014.10.027","relatedIdentifierType":"URL"},{"relationType":"References","relatedIdentifier":"https://doi.org/10.1016/j.ijfatigue.2016.12.033","relatedIdentifierType":"URL"},{"relationType":"References","relatedIdentifier":"https://doi.org/10.1016/j.mspro.2014.06.101","relatedIdentifierType":"URL"}],"relatedItems":[],"sizes":[],"formats":["media types: application/octet-stream, application/pdf, application/zip, text/plain"],"version":"1","rightsList":[{"rights":"4TU General Terms of Use","rightsUri":"https://doi.org/10.4121/resource:terms_of_use"}],"descriptions":[{"description":"Supplementary data in addition to the data included in data set I. The data includes a more refined curve fit of the crack length versus cycle number for specimens B-002-I and B-002-II, as well as the values calculated (e.g. strain energy release rate) using that fit. Also included are calculated strain energy release rates using individual calibration parameters for each specimen, and the calculated release of strain energy per cycle for each specimen. Parent item: Damage Tolerance of Adhesive Bonds - Datasets Quasi-static and fatigue tests of metal-metal adhesive bonds. Both raw data (crack length, force and displacement) and derived data (e.g. strain energy release rate) are included.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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