Effects of Strong Confinement on the Glass-Transition Temperature in Simulated Atactic Polystyrene Films

被引:99
作者
Hudzinskyy, Dmytro [1 ,2 ]
Lyulin, Alexey V. [1 ]
Baljon, Arlette R. C. [3 ,4 ]
Balabaev, Nikolay K.
Michels, Matthias A. J. [2 ]
机构
[1] Tech Univ Eindhoven, Dept Appl Phys, NL-5600 MB Eindhoven, Netherlands
[2] Dutch Polymer Inst, NL-5600 AX Eindhoven, Netherlands
[3] San Diego State Univ, Dept Phys, San Diego, CA 92182 USA
[4] Inst Math Problems Biol, Pushchino 142290, Russia
关键词
MOLECULAR-DYNAMICS SIMULATION; ULTRATHIN POLYMER-FILMS; THIN-FILMS; MECHANICAL-PROPERTIES; ORIENTATIONAL ORDER; SURFACE-LAYERS; MONTE-CARLO; CHAIN; INTERFACE; RELAXATIONS;
D O I
10.1021/ma102567s
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
We have performed molecular dynamics simulations to explore the influence of confinement on the glass-transition temperature T-g for supported atactic-polystyrene (aPS) thin films of different thickness (1-10 nm) and different strengths of attraction to the substrate (0.1-3.0 kcal/mol). The aPS films have been equilibrated in a melt at 540 K and further cooled down with a constant cooling velocity of 0.01 K/ps below T-g to room temperature, 300 K. On the basis of the density measurements, we have defined three different (substrate, middle, and surface) layers for each film. We found that the monomers close to the surface and in the substrate layer are partially oriented, which leads to more effective monomer packing. For the whole film the average density-based T-g value remains almost constant for films down to 2 nm thickness, where the middle layer vanishes. For the middle layer itself T-g does not depend on the total film thickness, while an increase up to 70 K is measured for the substrate layer depending on the strength of attraction to the actual substrate. The surface layer remains liquidlike in the whole temperature range (300-540 K). We claim that the redistribution of mass in the three film layers may explain the change with film thickness of the average T-g, if the latter is determined from linear fits of the average glass and melt densities.
引用
收藏
页码:2299 / 2310
页数:12
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