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 |