Relaxation processes and glass transition of confined polymer melts: A molecular dynamics simulation of 1,4-polybutadiene between graphite walls

被引:37
|
作者
Solar, M. [1 ]
Binder, K. [2 ]
Paul, W. [3 ]
机构
[1] Univ Strasbourg, Inst Charles Sadron, F-67034 Strasbourg, France
[2] Johannes Gutenberg Univ Mainz, Inst Phys, D-55099 Mainz, Germany
[3] Martin Luther Univ Halle Wittenberg, Inst Phys, D-06099 Halle, Germany
来源
JOURNAL OF CHEMICAL PHYSICS | 2017年 / 146卷 / 20期
关键词
GROWING LENGTH SCALES; DIELECTRIC-RELAXATION; COMPUTER-SIMULATIONS; THIN; FILMS; SURFACES; BEHAVIOR; BULK; TEMPERATURE; MOTION;
D O I
10.1063/1.4975390
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Molecular dynamics simulations of a chemically realistic model for 1,4-polybutadiene in a thin film geometry confined by two graphite walls are presented. Previous work on melts in the bulk has shown that the model faithfully reproduces static and dynamic properties of the real material over a wide temperature range. The present work studies how these properties change due to nano-confinement. The focus is on orientational correlations observable in nuclear magnetic resonance experiments and on the local intermediate incoherent neutron scattering function, F-s(q(z), z, t), for distances z from the graphite walls in the range of a few nanometers. Temperatures from about 2T(g) down to about 1.15T(g), where T-g is the glass transition temperature in the bulk, are studied. It is shown that weakly attractive forces between the wall atoms and the monomers suffice to effectively bind a polymer coil that is near the wall. For a wide regime of temperatures, the Arrhenius-like adsorption/desorption kinetics of the monomers is the slowest process, while very close to Tg the Vogel-Fulcher-Tammann-like alpha-relaxation takes over. The alpha-process is modified only for z <= 1.2 nm due to the density changes near the walls, less than expected from studies of coarse-grained (bead-spring-type) models. The weakness of the surface effects on the glass transition in this case is attributed to the interplay of density changes near the wall with the torsional potential. A brief discussion of pertinent experiments is given. Published by AIP Publishing.
引用
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页数:13
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