{"data":{"id":"10.6084/m9.figshare.6151790.v1","type":"dois","attributes":{"doi":"10.6084/m9.figshare.6151790.v1","prefix":"10.6084","suffix":"m9.figshare.6151790.v1","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Jheison Lopes Dos Santos","affiliation":[],"nameIdentifiers":[]},{"name":"Marçal, Rubens Lincoln Santana Blazutti","nameType":"Personal","givenName":"Rubens Lincoln Santana Blazutti","familyName":"Marçal","affiliation":[],"nameIdentifiers":[]},{"name":"Monteiro, Sérgio Neves","nameType":"Personal","givenName":"Sérgio Neves","familyName":"Monteiro","affiliation":[],"nameIdentifiers":[]},{"name":"Louro, Luis Henrique Leme","nameType":"Personal","givenName":"Luis Henrique Leme","familyName":"Louro","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"A New Dynamic Powder Consolidation Technique Using Shock Waves"}],"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-2016-1009","relatedIdentifierType":"DOI"},{"relationType":"IsIdenticalTo","relatedIdentifier":"10.6084/m9.figshare.6151790","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["1966828 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":"Techniques for shock consolidation of powders have been developed for different purposes, including the synthesis of diamond from carbon powder. In this work, a new device configuration for dynamic consolidation is proposed. It consists of three coaxial tubes, with a conical cover made of explosive at the top of the device. The inner tube contains the powder to be compacted. The second is accelerated towards the first in order to promote its collapse. The third confines the explosive. A conical cap at the top of the device triggers the explosive. For a preliminary evaluation, two types of explosives, TNT and Composition B, were used. Preliminary analytical results by the impedance matching method indicate that maximum pressures of 35.44 GPa and 48.16 GPa could be achieved using TNT and Composition B, respectively. Maximum temperatures around 1,600 K and 2,500 K for TNT and Composition B, respectively, are expected. These pressure and temperature values are adequate for transforming graphite into diamond. Preliminary Rietveld refinement indicated that nanodiamond is a fraction of approximately 54% of the detonation resulting powder.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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","url":"https://scielo.figshare.com/articles/A_New_Dynamic_Powder_Consolidation_Technique_Using_Shock_Waves/6151790/1","contentUrl":null,"metadataVersion":2,"schemaVersion":"http://datacite.org/schema/kernel-4","source":"mds","isActive":true,"state":"findable","reason":null,"viewCount":0,"viewsOverTime":[],"downloadCount":0,"downloadsOve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