Temperature dependence of the dynamics and interfacial width in nanoconfined polymers via atomistic simulations

Author:

Patsalidis Nikolaos1ORCID,Papamokos George2ORCID,Floudas George23ORCID,Harmandaris Vagelis145ORCID

Affiliation:

1. Computation-Based Science and Technology Research Center, The Cyprus Institute 1 , Aglantzia 2121, Nicosia Cyprus

2. Department of Physics, University of Ioannina 2 , 45110 Ioannina, Greece

3. University Research Center of Ioannina (URCI) - Institute of Materials Science and Computing, Ioannina 3 , 45110 Ioannina, Greece

4. Department of Mathematics and Applied Mathematics, University of Crete 4 , Heraklion GR-71110, Greece

5. Institute of Applied and Computational Mathematics, Foundation for Research and Technology - Hellas, Heraklion 5 , GR-71110 Crete, Greece

Abstract

We present a detailed computational study on the temperature effect of the dynamics and the interfacial width of unentangled cis-1,4 polybutadiene linear chains confined between strongly attractive alumina layers via long, several μs, atomistic molecular dynamics simulations for a wide range of temperatures (143–473 K). We examine the spatial gradient of the translational segmental dynamics and of an effective local glass temperature (TgL). The latter is found to be much higher than the bulk Tg for the adsorbed layer. It gradually reduces to the bulk Tg at about 2 nm away from the substrate. For distant regions (more than ≈1.2nm), a bulk-like behavior is observed; relaxation times follow a typical Vogel–Fulcher–Tammann dependence for temperatures higher than Tg and an Arrhenius dependence for temperatures below the bulk Tg. On the contrary, the polymer chains at the vicinity of the substrate follow piecewise Arrhenius processes. For temperatures below about the adsorbed layer’s TgL, the translational dynamics follows a bulk-like (same activation energy) Arrhenius process. At higher temperatures, there is a low activation energy Arrhenius process, caused by high interfacial friction forces. Finally, we compute the interfacial width, based on both structural and dynamical definitions, as a function of temperature. The absolute value of the interfacial width depends on the actual definition, but, regardless, the qualitative behavior is consistent. The interfacial width peaks around the bulk Tg and contracts for lower and higher temperatures. At bulk Tg, the estimated length of the interfacial width, computed via the various definitions, ranges between 1.0 and 2.7 nm.

Funder

Horizon 2020 Framework Program

Publisher

AIP Publishing

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