Please use this identifier to cite or link to this item: https://olympias.lib.uoi.gr/jspui/handle/123456789/16307
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dc.contributor.authorMierzwa, M.en
dc.contributor.authorFloudas, G.en
dc.contributor.authorWewerka, A.en
dc.date.accessioned2015-11-24T18:29:52Z-
dc.date.available2015-11-24T18:29:52Z-
dc.identifier.issn1063-651X-
dc.identifier.urihttps://olympias.lib.uoi.gr/jspui/handle/123456789/16307-
dc.rightsDefault Licence-
dc.subjectmolecular-weight dependenceen
dc.subjectspacer lengthen
dc.subjectrelaxationen
dc.subjectpressureen
dc.subjectbehavioren
dc.subjectorderen
dc.subjectpolymethacrylatesen
dc.subjectpolyisopreneen
dc.subjectphaseen
dc.titleDynamics of side-chain liquid-crystalline polymers: A dielectric spectroscopy investigationen
heal.typejournalArticle-
heal.type.enJournal articleen
heal.type.elΆρθρο Περιοδικούel
heal.identifier.secondary<Go to ISI>://000171136200041-
heal.languageen-
heal.accesscampus-
heal.recordProviderΠανεπιστήμιο Ιωαννίνων. Σχολή Επιστημών και Τεχνολογιών. Τμήμα Βιολογικών Εφαρμογών και Τεχνολογιώνel
heal.publicationDate2001-
heal.abstractWe have studied the dynamics in two side-chain liquid-crystalline derivatives of poly(norbornene diethylester) with dielectric spectroscopy within the temperature range 190-433 K and the pressure range 1-3000 bars. Optical microscopy, x-ray scattering, and differential scanning calorimetry (DSC) revealed the formation of a nematic- and a smectic-A phase, respectively, in the polymers with the shorter and longer spacers. Multiple relaxation processes exist originating from the backbone and mesogenic dipoles. In the smectic-A phase two relaxation processes exist above the DSC glass temperature (alpha and alpha') which merge with decreasing temperature or with increasing pressure. thus suggesting a common molecular mechanism. The faster process is the segmental (alpha) relaxation associated with the dynamic glass transition. whereas the slower process reflects mainly the side-chain dynamics within the smectic layers. Pressure was found to increase the glass temperature in the nematic and smectic phases and the dT(q)/dP was 18.7 and 16.9 K/kbar. respectively. However, the effect of pressure in inducing the isotropic-to-smectic transition is more drastic as dT(S1)/dP = 26.4 K/kbar.en
heal.journalNamePhysical Review Een
heal.journalTypepeer reviewed-
heal.fullTextAvailabilityTRUE-
Appears in Collections:Άρθρα σε επιστημονικά περιοδικά ( Ανοικτά)



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