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Influence of plasticizer on Poisson's ratio of epoxy polymers

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dc.contributor.author Theocaris, PS en
dc.date.accessioned 2014-03-01T01:05:46Z
dc.date.available 2014-03-01T01:05:46Z
dc.date.issued 1979 en
dc.identifier.issn 0032-3861 en
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/8973
dc.subject poisson's ratio en
dc.subject.classification Polymer Science en
dc.subject.other MATERIALS TESTING - Tensile Tests en
dc.subject.other MATHEMATICAL TECHNIQUES en
dc.subject.other PLASTICIZERS en
dc.subject.other PLASTICS - Creep en
dc.subject.other THERMODYNAMICS en
dc.subject.other EPOXY RESINS en
dc.title Influence of plasticizer on Poisson's ratio of epoxy polymers en
heal.type journalArticle en
heal.identifier.primary 10.1016/0032-3861(79)90308-2 en
heal.identifier.secondary http://dx.doi.org/10.1016/0032-3861(79)90308-2 en
heal.language English en
heal.publicationDate 1979 en
heal.abstract A series of simultaneous isothermal tensile creep measurements of the longitudinal extension and the lateral contraction in standard thin tension specimens yielded individual curves for the variation of the lateral contraction ratio (Poisson's ratio) at different loading and temperature steps throughout the viscoelastic spectrum for a series of pure and plasticized cold-setting epoxy polymers. By applying the principle of reduced variables and shifting the isothermal creep curves along the log(time) scale, composite curves were obtained for Poisson's ratio which have the shape of sigmoid curves, thus proving the dependence of this viscoelastic function on time and temperature. It was shown that the corresponding transition regions were shifted towards the origin (t = 0) as the amount of plasticizer was increased, while the shape of the corresponding composite curves did not change and the variation of the logarithmic time factor remained essentially the same but with steeper gradients for increasing amounts of plasticizer. Comparison of the viscoelastic spectra for this function with the corresponding spectra for creep extension, shear and bulk compliances found previously indicated that the spectrum of this function is broader than the others and while it starts to appear earlier than the shear compliance spectrum it disappears after the corresponding bulk compliance spectrum. Finally, glass transition temperatures for the various mixtures were found to be lower by 5° to 10°C than those obtained from measurements using a thermal analyser. © 1979. en
heal.publisher ELSEVIER SCI LTD en
heal.journalName Polymer en
dc.identifier.doi 10.1016/0032-3861(79)90308-2 en
dc.identifier.isi ISI:A1979HL84600023 en
dc.identifier.volume 20 en
dc.identifier.issue 9 en
dc.identifier.spage 1149 en
dc.identifier.epage 1154 en


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