{"data":{"id":"10.6084/m9.figshare.6693317.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6693317.v1","prefix":"10.6084","suffix":"m9.figshare.6693317.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Furtado, Glória Tamiris Farias da Silva","givenName":"Glória Tamiris Farias da Silva","familyName":"Furtado","affiliation":[],"nameIdentifiers":[]},{"name":"Fideles, Thiago Bizerra","givenName":"Thiago Bizerra","familyName":"Fideles","affiliation":[],"nameIdentifiers":[]},{"name":"Cruz, Rita de Cassia Alves Leal","givenName":"Rita de Cassia Alves Leal","familyName":"Cruz","affiliation":[],"nameIdentifiers":[]},{"name":"Souza, José William de Lima","givenName":"José William de Lima","familyName":"Souza","affiliation":[],"nameIdentifiers":[]},{"name":"Rodriguez Barbero, Miguel Angel","givenName":"Miguel Angel","familyName":"Rodriguez Barbero","affiliation":[],"nameIdentifiers":[]},{"name":"Fook, Marcus Vinicius Lia","givenName":"Marcus Vinicius Lia","familyName":"Fook","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Chitosan/NaF Particles Prepared Via Ionotropic Gelation: Evaluation of Particles Size and Morphology"}],"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":"2018-06-27","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-2018-0101","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.6693317","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["1753743 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 was to perform an analysis of the influence of Sodium Fluoride (NaF) on chitosan particles size and morphology produced via ionotropic gelation with higher rotational stirring speed. Samples were characterized by Fourier Transform Infrared Spectroscopy (FTIR), Dynamic Light Scattering (DLS), Zeta Potential (ζ), Scanning Electron Microscopy and Energy Dispersive Spectroscopy (SEM/EDS). Chitosan/TPP particles diameter obtained was in the order of 3.8 µm. When NaF was added in different concentration (0.05%, 0.2% and 2%), the particle size diameter values, Zeta Potential and Poly Dispersive Index measures consequently decreased. Even so, no further modification in morphology was found. An exception was made for the samples with higher NaF concentration. After 21 days, occurred an increase in the particle size diameter. In the future, the proposed methodology could provide a dentistry application, especially on delivering particles of NaF.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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