Abstract

In this article we present results on the glass transition, crystallization and molecular dynamics in relatively novel oligomers, oligo-ethylene glycol methacrylate (OEGMA), with short and long chains, as well as in the corresponding nanostructured comb-like polymers (POEGMA, short and long), the latter being prepared via the RAFT polymerization process. For the investigation we employed conventional and temperature modulated differential scanning calorimetry in combination with high resolving power dielectric spectroscopy techniques, broadband dielectric relaxation spectroscopy (BDS) and thermally stimulated depolarization currents (TSDC). Under ambient conditions short OEGMA (475 g mol-1, ∼4 nm in length) exhibits a remarkable low glass transition temperature, Tg, of -91 °C, crystallization temperature Tc = -24 °C and a significant crystalline fraction, CF, of ∼30%. When doubling the number of monomers (OEGMA-long, 950 g mol-1, chain length ∼8 nm) the Tg increases by about 20 K and CF increases to ∼53%, whereas, the Tc migrates to a room-like temperature of 19 °C. Upon formation of comb-like POEGMA structures the grafted OEGMA short chains, strikingly, are not able to crystallize, while in POEGMA-long the crystallization behaviour changes significantly as compared to OEGMA. Our results indicate that in the comb-like architecture the chain diffusion of the amorphous fractions is also strongly affected. The semicrystalline systems exhibit significant melt memory effects, this being stronger in the comb-like architecture. It is shown that these effects are related to the inter- and intra-chain interactions of the crystallizable chains. The dielectric techniques allowed the molecular dynamics mapping of these new systems from the linear oligomers to POEGMAs for the first time. BDS and TSDC detected various dynamics processes, in particular, the local polymer dynamics (γ process) to be sensitive to the Tg, local dynamics triggered in the hydrophilic chain segments by water traces (β), as well as the segmental dynamics (α) related to glass transition. Interestingly, both the short and long linear OEGMAs exhibit an additional relaxation process that resembles the Normal-Mode process appearing in polyethers. In the corresponding POEGMAs this process could not be resolved, this being an effect of the one-side grafted chain on the comb backbone. The revealed variations in molecular mobility and crystallization behavior suggest the potentially manipulable diffusion of small molecules throughout the polymer volume, via both the molecular architecture as well as the thermal treatment. This ability is extremely useful for these novel materials, envisaging their future applications in biomedicine (drug encapsulation).

Highlights

  • Olga Vassiliadou, a Varvara Chrysostomou, b Stergios Pispas, b Panagiotis A

  • In the present work we investigate, for the first time, the crystallization behavior, thermal transitions and molecular dynamics of Poly(oligo ethylene glycol methacrylate) (POEGMA) homopolymers with poly(ethylene glycol) (PEG) side chains of two different and rather short lengths

  • oligo-ethylene glycol methacrylate (OEGMA)-short crystallizes at Tc = À24 1C, exhibits a glass transition at a remarkable very low temperature, Tg B À91 1C, and complex melting peaks between À60 and À2 1C, with the maxima being located at Tm1 = À31 1C and Tm2 = À7 1C

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Summary

Introduction

Olga Vassiliadou, a Varvara Chrysostomou, b Stergios Pispas, b Panagiotis A. BDS and TSDC detected various dynamics processes, in particular, the local polymer dynamics (g process) to be sensitive to the Tg, local dynamics triggered in the hydrophilic chain segments by water traces (b), as well as the segmental dynamics (a) related to glass transition Both the short and long linear OEGMAs exhibit an additional relaxation process that resembles the Normal-Mode process appearing in polyethers. ‘graft-like’ structures composed of carbon–carbon backbones (hydrophobic) and multiple oligo(ethylene glycol) side-chains (branches)[1,2,3] which are hydrophilic Such materials are usually addressed as brush- or comb-like polymers[4,5,6,7,8] being the nonlinear poly(ethylene glycol) (PEG) analogues.[2] For short side chains, which occur for less than B10 ethylene glycol units, the POEGMA homopolymers are considered thermoresponsive, as upon thermally induced dehydration they undergo a nanophase transition.[2,9] This transition is due to the distinct chemical nature between the backbone and the branches so that, in the presence of solvents, selective chain associations are favored. Brush copolymers consisting of an amorphous main chain and crystallizable side chains can phase separate into a variety of morphologies resulting in copolymers with interesting properties.[5,8,15,16,17] The crystallization behavior of such brush polymers has been investigated in the past decades by various groups, and according to the generally most accepted model the main chain and a fraction of side chains in the vicinity of the main chain constitute the amorphous phase whereas the side chains are incorporated into crystalline lamella separated by amorphous domains.[5,16] It is widely accepted that factors such as the backbone rigidity, the nature of the linking groups, and the length of the side chains affect significantly the side chain crystallization.[5,18] In the case of PEG side chains, the reported results have indicated that the crystallization temperature, Tc, decreases as compared to linear long PEG [poly(ethylene oxide), PEO] macromolecular chains and the degree of supercooling depends strongly on the length of the side chains, with Tc ranging from slightly below 0 1C to about 65 1C.6,14–16 it has been shown that crystallization in the brush copolymers was hindered by frustration in packing of the crystallizable PEG chains which can be realized either in the interdigitating or the end-to-end form.[5,15]

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