Abstract

For poly(2,6-dimethyl-1,4-phenylene)oxide (PPO) films exhibiting nanoporous-crystalline (NC) phases, c⊥ orientation (i.e., crystalline polymer chain axes being preferentially perpendicular to the film plane) is obtained by crystallization of amorphous films, as induced by sorption of suitable low-molecular-mass guest molecules. The occurrence of c⊥ orientation is relevant for applications of NC PPO films because it markedly increases film transparency as well as guest diffusivity. Surprisingly, we show that the known crystallization procedures lead to c⊥ oriented thick (50–300 μm) films and to unoriented thin (≤20 μm) films. This absence of crystalline phase orientation for thin films is rationalized by fast guest sorption kinetics, which avoid co-crystallization in confined spaces and hence inhibit formation of flat-on lamellae. For thick films exhibiting c⊥ orientation, sigmoid kinetics of guest sorption and of thickening of PPO films are observed, with inflection points associated with guest-induced film plasticization. Corresponding crystallization kinetics are linear with time and show that co-crystal growth is poorly affected by film plasticization. An additional relevant result of this study is the linear relationship between WAXD crystallinity index and DSC melting enthalpy, which allows evaluation of melting enthalpy of the NC α form of PPO (ΔHmο = 42 ± 2 J/g).

Highlights

  • Orientation of polymer chain axes (c axes) in crystalline lamellae are perpendicular or nearly perpendicular to the lamellar planes.Crystalline lamellae can be oriented with respect to the polymer film plane, mainly for films having a thickness lower than 1 μm

  • For films as obtained by guest-induced crystallization of amorphous films, we study the dependence of planar orientation on film thickness

  • The planar orientation exhibiting crystalline chain axes preferentially perpendicular to the film plane (c⊥ orientation), which is observed for CC and NC PPO films as obtained by bulky guest-induced crystallization, depends on the thickness of the starting amorphous film

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Summary

Introduction

Crystalline lamellae can be oriented with respect to the polymer film plane, mainly for films having a thickness lower than 1 μm. Can be achieved for polymer films exhibiting co-crystalline (CC) phases, i.e., where a host polymer includes low-molecular-mass guest molecules in crystalline cavities [15–21]. Even for thickness of several hundredths of microns, different kinds of planar and uniplanar orientations (i.e., preferential orientations of a crystalline axis or of a crystalline plane with respect to the film plane, respectively) have been observed for films exhibiting CC phases of syndiotactic polystyrene [15–17], poly-(L-lactic acid) [18,19] and poly(2,6-dimethyl-1,4-phenylene)oxide (PPO) [20,21]. In CC films, the orientation of the host polymer can induce orientation of active guest molecules, being fluorescent [22–25], magnetic [26,27], ferroelectric [28], photo-reactive [29] or chiral-optical [30]

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