{"data":{"id":"10.6084/m9.figshare.6152246","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6152246","prefix":"10.6084","suffix":"m9.figshare.6152246","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Evora, Maria Cecilia","nameType":"Personal","givenName":"Maria Cecilia","familyName":"Evora","affiliation":[],"nameIdentifiers":[]},{"name":"Nitilaksha Hiremath","affiliation":[],"nameIdentifiers":[]},{"name":"Xinyi Lu","affiliation":[],"nameIdentifiers":[]},{"name":"Nam-Goo Kang","affiliation":[],"nameIdentifiers":[]},{"name":"Silva, Leonardo Gondin De Andrada E","nameType":"Personal","givenName":"Leonardo Gondin De Andrada E","familyName":"Silva","affiliation":[],"nameIdentifiers":[]},{"name":"Gajanan Bhat","affiliation":[],"nameIdentifiers":[]},{"name":"Mays, Jimmy","nameType":"Personal","givenName":"Jimmy","familyName":"Mays","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Effect of Electron Beam and Gamma Rays on Carbon Nanotube Yarn Structure"}],"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":"2018-04-18","dateType":"Created"},{"date":"2018-04-18","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-2017-0102","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["2714741 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":"Individual carbon nanotubes (CNTs) exhibit excellent mechanical, electrical and thermal properties, leading to development of a new generation of advanced lightweight materials and spacecraft electronics substituting the electronics based on silicon. The direct assembly of CNTs into macroscopic fibers or sheets has been a way to overcome their dispersion and processing challenges. Because of a wide range of applications of this material, we investigate effectively the defects on CNT yarns structures created by electron beam and gamma sources and their impact on the morphology and mechanical properties. The irradiated samples with electron beam at doses of 400, 600 and 800 kGy had a decrease in the strength from 219.60 ± 18.90 MPa for pristine yarn to 108.86 ± 23.77, 153.15 ± 21.63, 170.50 ± 25.78 MPa, respectively. The sample irradiated with gamma in air at dose of 100 kGy had the strength increased slightly as compared with the pristine sample and an increase in the elasticity modulus from 8.79 ± 1.19 to 19.63 ± 2.02 GPa as compared to CNT pristine yarn. The quality of the CNT yarns that was gamma irradiated in air with absorbed dose of 100 kGy was not affected by the radiation process with improvement of 123% of the Young’s modulus.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"PD94bWwgdmVyc2lvbj0iMS4wIiBlbmNvZGluZz0iVVRGLTgiPz4KPHJlc291cmNlIHhtbG5zPSJodHRwOi8vZGF0YWNpdGUub3JnL3NjaGVtYS9rZXJuZWwtNCIgeG1sbnM6eHNpPSJodHRwOi8vd3d3LnczLm9yZy8yMDAxL1hNTFNjaGVtYS1pbnN0YW5jZSIgeHNpOnNjaGVtYUxvY2F0aW9uPSJodHRwOi8vZGF0YWNpdGUub3JnL3NjaGVtYS9rZXJuZWwtNCBodHRwOi8vc2NoZW1hLmRhdGFjaXRlLm9yZy9tZXRhL2tlcm5lbC00LjEvbWV0YWRhdGEueHNkIj4KICA8aWRlbnRpZmllciBpZGVudGlmaWVyVHlwZT0iRE9JIj4xMC42MDg0L005LkZJR1NIQVJFLjYxNTIyNDY8L2lkZW50aWZpZXI+CiAgPGNyZWF0b3JzPgogICAgPGNyZWF0b3I+CiAgICAgIDxjcmVhdG9yTmFtZT5NYXJpYSBDZWNpbGlhIEV2b3JhPC9jcmVhdG9yTmFtZT4KICAgIDwvY3JlYXRvcj4KICAgIDxjcmVhdG9yPgogICAgICA8Y3JlYXRvck5hbWU+Tml0aWxha3NoYSBIaXJlbWF0aDwvY3JlYXRvck5hbWU+CiAgICA8L2NyZWF0b3I+CiAgICA8Y3JlYXRvcj4KICAgICAgPGNyZWF0b3JOYW1lPlhpbnlpIEx1PC9jcmVhdG9yTmFtZT4KICAgIDwvY3JlYXRvcj4KICAgIDxjcmVhdG9yPgogICAgICA8Y3JlYXRvck5hbWU+TmFtLUdvbyBLYW5nPC9jcmVhdG9yTmFtZT4KICAgIDwvY3JlYXRvcj4KICAgIDxjcmVhdG9yPgogICAgICA8Y3JlYXRvck5hbWU+TGVvbmFyZG8gR29uZGluIGRlIEFuZHJhZGEgZSBTaWx2YTwvY3JlYXRvck5hbWU+CiAgICA8L2NyZWF0b3I+CiAgICA8Y3JlYXRvcj4KICAgICAgPGNyZWF0b3JOYW1lPkdhamFuYW4gQmhhdDwvY3JlYXRvck5hbWU+CiAgICA8L2NyZWF0b3I+CiAgICA8Y3JlYXRvcj4KICAgICAgPGNyZWF0b3JOYW1lPkppbW15IE1heXM8L2NyZWF0b3JOYW1lPgogICAgPC9jcmVhdG9yPgogIDwvY3JlYXRvcnM+CiAgPHRpdGxlcz4KICAgIDx0aXRsZT5FZmZlY3Qgb2YgRWxlY3Ryb24gQmVhbSBhbmQgR2FtbWEgUmF5cyBvbiBDYXJib24gTmFub3R1YmUgWWFybiBTdHJ1Y3R1cmU8L3RpdGxlPgogIDwvdGl0bGVzPgogIDxkZXNjcmlwdGlvbnM+CiAgICA8ZGVzY3JpcHRpb24gZGVzY3JpcHRpb25UeXBlPSJBYnN0cmFjdCI+Jmx0O2RpdiZndDsmbHQ7cCZndDtJbmRpdmlkdWFsIGNhcmJvbiBuYW5vdHViZXMgKENOVHMpIGV4aGliaXQgZXhjZWxsZW50IG1lY2hhbmljYWwsIGVsZWN0cmljYWwgYW5kIHRoZXJtYWwgcHJvcGVydGllcywgbGVhZGluZyB0byBkZXZlbG9wbWVudCBvZiBhIG5ldyBnZW5lcmF0aW9uIG9mIGFkdmFuY2VkIGxpZ2h0d2VpZ2h0IG1hdGVyaWFscyBhbmQgc3BhY2VjcmFmdCBlbGVjdHJvbmljcyBzdWJzdGl0dXRpbmcgdGhlIGVsZWN0cm9uaWNzIGJhc2VkIG9uIHNpbGljb24uIFRoZSBkaXJlY3QgYXNzZW1ibHkgb2YgQ05UcyBpbnRvIG1hY3Jvc2NvcGljIGZpYmVycyBvciBzaGVldHMgaGFzIGJlZW4gYSB3YXkgdG8gb3ZlcmNvbWUgdGhlaXIgZGlzcGVyc2lvbiBhbmQgcHJvY2Vzc2luZyBjaGFsbGVuZ2VzLiBCZWNhdXNlIG9mIGEgd2lkZSByYW5nZSBvZiBhcHBsaWNhdGlvbnMgb2YgdGhpcyBtYXRlcmlhbCwgd2UgaW52ZXN0aWdhdGUgZWZmZWN0aXZlbHkgdGhlIGRlZmVjdHMgb24gQ05UIHlhcm5zIHN0cnVjdHVyZXMgY3JlYXRlZCBieSBlbGVjdHJvbiBiZWFtIGFuZCBnYW1tYSBzb3VyY2VzIGFuZCB0aGVpciBpbXBhY3Qgb24gdGhlIG1vcnBob2xvZ3kgYW5kIG1lY2hhbmljYWwgcHJvcGVydGllcy4gVGhlIGlycmFkaWF0ZWQgc2FtcGxlcyB3aXRoIGVsZWN0cm9uIGJlYW0gYXQgZG9zZXMgb2YgNDAwLCA2MDAgYW5kIDgwMCBrR3kgaGFkIGEgZGVjcmVhc2UgaW4gdGhlIHN0cmVuZ3RoIGZyb20gMjE5LjYwIMKxIDE4LjkwIE1QYSBmb3IgcHJpc3RpbmUgeWFybiB0byAxMDguODYgwrEgMjMuNzcsIDE1My4xNSDCsSAyMS42MywgMTcwLjUwIMKxIDI1Ljc4IE1QYSwgcmVzcGVjdGl2ZWx5LiBUaGUgc2FtcGxlIGlycmFkaWF0ZWQgd2l0aCBnYW1tYSBpbiBhaXIgYXQgZG9zZSBvZiAxMDAga0d5IGhhZCB0aGUgc3RyZW5ndGggaW5jcmVhc2VkIHNsaWdodGx5IGFzIGNvbXBhcmVkIHdpdGggdGhlIHByaXN0aW5lIHNhbXBsZSBhbmQgYW4gaW5jcmVhc2UgaW4gdGhlIGVsYXN0aWNpdHkgbW9kdWx1cyBmcm9tIDguNzkgwrEgMS4xOSB0byAxOS42MyDCsSAyLjAyIEdQYSBhcyBjb21wYXJlZCB0byBDTlQgcHJpc3RpbmUgeWFybi4gVGhlIHF1YWxpdHkgb2YgdGhlIENOVCB5YXJucyB0aGF0IHdhcyBnYW1tYSBpcnJhZGlhdGVkIGluIGFpciB3aXRoIGFic29yYmVkIGRvc2Ugb2YgMTAwIGtHeSB3YXMgbm90IGFmZmVjdGVkIGJ5IHRoZSByYWRpYXRpb24gcHJvY2VzcyB3aXRoIGltcHJvdmVtZW50IG9mIDEyMyUgb2YgdGhlIFlvdW5n4oCZcyBtb2R1bHVzLiZsdDsvcCZndDsmbHQ7L2RpdiZndDs8L2Rlc2NyaXB0aW9uPgogIDwvZGVzY3JpcHRpb25zPgogIDxzdWJqZWN0cz4KICAgIDxzdWJqZWN0IHNjaGVtZVVSST0iaHR0cDovL3d3dy5hYnMuZ292LmF1L2F1c3N0YXRzL2Fic0AubnNmLzAvNkJCNDI3QUI5Njk2QzIyNUNBMjU3NDE4MDAwNDQ2M0UiIHN1YmplY3RTY2hlbWU9IkZPUiI+OTA0OTkgQ2hlbWljYWwgRW5naW5lZXJpbmcgbm90IGVsc2V3aGVyZSBjbGFzc2lmaWVkPC9zdWJqZWN0PgogICAgPHN1YmplY3Qgc2NoZW1lVVJJPSJodHRwOi8vd3d3LmFicy5nb3YuYXUvYXVzc3RhdHMvYWJzQC5uc2YvMC82QkI0MjdBQjk2OTZDMjI1Q0EyNTc0MTgwMDA0NDYzRSIgc3ViamVjdFNjaGVtZT0iRk9SIj45MTIwNyBNZXRhbHMgYW5kIEFsbG95IE1hdGVyaWFsczwvc3ViamVjdD4KICAgIDxzdWJqZWN0IHNjaGVtZVVSST0iaHR0cDovL3d3dy5hYnMuZ292LmF1L2F1c3N0YXRzL2Fic0AubnNmLzAvNkJCNDI3QUI5Njk2QzIyNUNBMjU3NDE4MDAwNDQ2M0UiIHN1YmplY3RTY2hlbWU9IkZPUiI+OTEyOTkgTWF0ZXJpYWxzIEVuZ2luZWVyaW5nIG5vdCBlbHNld2hlcmUgY2xhc3NpZmllZDwvc3ViamVjdD4KICA8L3N1YmplY3RzPgogIDxwdWJsaXNoZXI+U2NpRUxPIGpvdXJuYWxzPC9wdWJsaXNoZXI+CiAgPHB1YmxpY2F0aW9uWWVhcj4yMDE4PC9wdWJsaWNhdGlvblllYXI+CiAgPGRhdGVzPgogICAgPGRhdGUgZGF0ZVR5cGU9IkNyZWF0ZWQiPjIwMTgtMDQtMTg8L2RhdGU+CiAgICA8ZGF0ZSBkYXRlVHlwZT0iVXBkYXRlZCI+MjAxOC0wNC0xODwvZGF0ZT4KICA8L2RhdGVzPgogIDxyZXNvdXJjZVR5cGUgcmVzb3VyY2VUeXBlR2VuZXJhbD0iRGF0YXNldCI+RGF0YXNldDwvcmVzb3VyY2VUeXBlPgogIDxzaXplcz4KICAgIDxzaXplPjI3MTQ3NDEgQnl0ZXM8L3NpemU+CiAgPC9zaXplcz4KICA8cmVsYXRlZElkZW50aWZpZXJzPgogICAgPHJlbGF0ZWRJZGVudGlmaWVyIHJlbGF0ZWRJZGVudGlmaWVyVHlwZT0iRE9JIiByZWxhdGlvblR5cGU9IklzU3VwcGxlbWVudFRvIj4xMC4xNTkwLzE5ODAtNTM3My1tci0yMDE3LTAxMDI8L3JlbGF0ZWRJZGVudGlmaWVyPgogIDwvcmVsYXRlZElkZW50aWZpZXJzPgogIDxyaWdodHNMaXN0PgogICAgPHJpZ2h0cyByaWdodHNVUkk9Imh0dHBzOi8vY3JlYXRpdmVjb21tb25zLm9yZy9saWNlbnNlcy9ieS80LjAvIj5DQyBCWSA0LjA8L3JpZ2h0cz4KICA8L3JpZ2h0c0xpc3Q+CjwvcmVzb3VyY2U+","url":"https://scielo.figshare.com/articles/Effect_of_Electron_Beam_and_Gamma_Rays_on_Carbon_Nanotube_Yarn_Structure/6152246","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":"2018-04-18T03:01:02.000Z","registered":"2018-04-18T03:01:02.000Z","published":"2018","updated":"2020-08-29T23:41:36.000Z"},"relationships":{"client":{"data":{"id":"figshare.ars","type":"clients"}},"provider":{"data":{"id":"otjm","type":"providers"}},"media":{"data":{"id":"10.6084/m9.figshare.6152246","type":"media"}},"references":{"data":[{"id":"10.1590/1980-5373-mr-2017-0102","type":"dois"}]},"citations":{"data":[]},"parts":{"data":[]},"partOf":{"data":[]},"versions":{"data":[]},"versionOf":{"data":[]}}}}