Double glass transition in polyethylene naphthalate by MDSC, BDS, and TSDC

Author:

Cañadas Juan Carlos1ORCID,Diego José Antonio1ORCID,Diez-Berart Sergio2ORCID,López David Orencio2ORCID,Mudarra Miguel1ORCID,Salud Josep2ORCID,Sellarès Jordi1ORCID

Affiliation:

1. DILAB, Departament de Física, ESEIAAT, Universitat Politècnica de Catalunya, Colom 11 1 , 08222 Terrassa, Spain

2. Grup de les Propietats Físiques del Materials (GRPFM), Departament de Física, ETSEIB, Universitat Politècnica de Catalunya 2 , Diagonal, 647, 08028 Barcelona, Spain

Abstract

In this work, we present an experimental study of the primary and secondary relaxations of the semi-crystalline polymer polyethylene naphthalate by modulated differential scanning calorimetry, Thermally Stimulated Depolarization Currents (TSDCs), and Broadband Dielectric Spectroscopy (BDS) and how they are affected by physical aging. Three dipolar relaxation modes can be observed: from slowest to fastest: the primary α relaxation, which vitrifies at the glass transition temperature, Tgα, and two secondary relaxations, named β* and β. Modulated differential scanning calorimetry results show how the secondary β* relaxation also vitrifies, giving rise to an additional glass transition at Tgβ* < Tgα. In fact, the α and β* relaxations can be considered as part of a very broad and distributed relaxation. Its main part is the primary α relaxation with a shoulder at the high-frequency region corresponding to a complex secondary β* relaxation. BDS results about β* can be modeled by a main contribution (β3*) and two additional ones (β1* and β2*) with a weaker dielectric strength. TSDC results show that each single mode of the relaxation has its own glass transition temperature and they are compatible with the structure inferred by BDS. This scenario gives rise to an extended glass transition dually centered in the Tgβ* ∼ 305 K and Tgα ∼ 387 K temperatures.

Publisher

AIP Publishing

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