{"data":{"id":"10.6084/m9.figshare.6448208","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6448208","prefix":"10.6084","suffix":"m9.figshare.6448208","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Weidenfeller, Bernd","nameType":"Personal","givenName":"Bernd","familyName":"Weidenfeller","affiliation":[],"nameIdentifiers":[]},{"name":"Lambri, Osvaldo Agustín","nameType":"Personal","givenName":"Osvaldo Agustín","familyName":"Lambri","affiliation":[],"nameIdentifiers":[]},{"name":"Bonifacich, Federico Guillermo","nameType":"Personal","givenName":"Federico Guillermo","familyName":"Bonifacich","affiliation":[],"nameIdentifiers":[]},{"name":"Arlic, Uwe","nameType":"Personal","givenName":"Uwe","familyName":"Arlic","affiliation":[],"nameIdentifiers":[]},{"name":"Gargicevich, Damian","nameType":"Personal","givenName":"Damian","familyName":"Gargicevich","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Damping of the Woodwind Instrument Reed Material Arundo donax L"}],"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":"2018-06-06","dateType":"Created"},{"date":"2018-06-06","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-2017-0795","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["2589764 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 viscoelastic properties (E', G', tanΦ, δ) of Arundo donax (AD) and a polypropylene-beech fiber composite (PPC) were measured from RT to 580K for various frequencies and strains. E' of AD varies between 5250-6250MPa depending on ageing at RT while E'(RT)=2250MPa of PPC is signifcantly lower. E' of the AD is higher than E' of PPC in the whole investigated temperature range with the exception of AD after a heat treatment up to 575K. Damping spectra exhibit peaks around 340K (Q=234kJ/mol) and 415K for the PPC related to relaxations in the crystalline part of polypropylene and the relaxation at melting temperature. For AD damping peaks were found at 350K (Q=320kJ/mol) related to the glass-rubber transition of lignin, at 420K due to a reorganization in the amorphous phase of lignin, at 480K related to micro-Brownian motions in the non-crystalline region of cell-wall polymers and reduction of the crystallinity of cellulose, and at 570K due to the polymeric compounds of wood and/or a decomposition of lignin. The course of E' and tanΦ of AD and PPC is comparable from 20-200Hz, whereas tanΦ of AD is lower than tanΦ of PPC while E' of AD is higher than E' of PPC.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://scielo.figshare.com/articles/Damping_of_the_Woodwind_Instrument_Reed_Material_Arundo_donax_L/6448208","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":[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