{"data":{"id":"10.6084/m9.figshare.7020530.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.7020530.v1","prefix":"10.6084","suffix":"m9.figshare.7020530.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Arruda, Salim Abdelnor","givenName":"Salim Abdelnor","familyName":"Arruda","affiliation":[],"nameIdentifiers":[]},{"name":"Sousa, Jokderléa Correa de","givenName":"Jokderléa Correa de","familyName":"Sousa","affiliation":[],"nameIdentifiers":[]},{"name":"Lima, Juliana Cisneiros","givenName":"Juliana Cisneiros","familyName":"Lima","affiliation":[],"nameIdentifiers":[]},{"name":"Vitorino, Maria do Bom Conselho","givenName":"Maria do Bom Conselho","familyName":"Vitorino","affiliation":[],"nameIdentifiers":[]},{"name":"Canedo, Eduardo Luis","givenName":"Eduardo Luis","familyName":"Canedo","affiliation":[],"nameIdentifiers":[]},{"name":"Almeida, Yêda Medeiros Bastos de","givenName":"Yêda Medeiros Bastos de","familyName":"Almeida","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Nonisothermal Melt Crystallization Kinetics of PHB/babassu Compounds"}],"publisher":"SciELO journals","container":{},"publicationYear":2018,"subjects":[{"subject":"90499 Chemical Engineering not elsewhere classified","schemeUri":"http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E","subjectScheme":"FOR"},{"subject":"FOS: Chemical engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"91207 Metals and Alloy Materials","schemeUri":"http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E","subjectScheme":"FOR"},{"subject":"FOS: Materials engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"91299 Materials Engineering not elsewhere classified","schemeUri":"http://www.abs.gov.au/ausstats/abs@.nsf/0/6BB427AB9696C225CA2574180004463E","subjectScheme":"FOR"}],"contributors":[],"dates":[{"date":"2018-08-29","dateType":"Created"},{"date":"2022-06-07","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-2018-0213","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.7020530","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["1158229 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":"PHB has interesting features such as biodegradability, sustainability and durability. However, it has a high cost, in addition to being hard, brittle and thermally unstable during processing. Therefore, it was found convenient to study the crystallization of PHB/20% babassu compounds, with the intention of reducing the cost of the composite, in addition to seeking improvements in thermal properties. In this work, the parameters of melt crystallization were studied for PHB/20% babassu compounds driven at different cooling rates under a nitrogen flow. Subsequently, crystallization parameters were compared for different cooling rates. A kinetic analysis of data obtained for melt crystallization was performed. Among the models studied, Pseudo-Avrami showed the best correlation with experimental data, with discrepancy between +6% and -4%. The Mo model presented a discrepancy between +15% and -8%. A modified Mo model discrepancies are reduced to +3% and -4% within the range of validity of the model.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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