Temperature dependence of free volume in pure and silica-filled poly(dimethyl siloxane) from positron lifetime and PVT experiments

被引:51
作者
Dlubek, G
De, U
Pionteck, J
Arutyunov, NY
Edelmann, M
Krause-Rehberg, R
机构
[1] ITA Inst Innovat Technol, Branch Off Halle, D-06120 Halle An Der Saale, Germany
[2] Univ Halle Wittenberg, Dept Phys, D-06099 Halle An Der Saale, Germany
[3] Ctr Variable Energy Cyclotron, Kolkata 700064, W Bengal, India
[4] Leibinz Inst Polymer Res Dresden, D-01069 Dresden, Germany
[5] Inst Elect, Tashkent 700170, Uzbekistan
关键词
free volume; lattice-hole model; lattice models; nanocomposites; polysiloxanes; positron lifetime;
D O I
10.1002/macp.200400546
中图分类号
O63 [高分子化学(高聚物)];
学科分类号
070305 ; 080501 ; 081704 ;
摘要
The microstructure of the free volume and its temperature dependence in two poly(dimethyl siloxane)s (PDMS), one in the pure state and the other filled with 35 wt.-% of an in situ hydrophobized fumed silica with a specific surface area of 200-300 m(2) - g(-1), were studied by pressure volume-temperature experiments (PVT, T = 22-156 degrees C, P = 10-200 MPa) and positron annihilation lifetime spectroscopy (PALS, T = -173-100 degrees C, P = 10(-5) MPa). The Simha-Somcynsky equation of state was used to estimate the hole free volume fraction, h, and free and occupied volumes, V-f = hV and V-occ = (1 - h)V, from the specific total volume, V. The PALS spectra were analyzed with the routine LT9.0, which allowed for a dispersion, sigma(i), in all three of the lifetimes: the para-positronium, (p-Ps, tau(1)), positron (e(+), tau(2)) and orthopositronium (o-Ps) lifetime This kind of analysis delivered correct p-Ps lifetime parameters, tau(1), sigma(1), and I-1. It was speculated that e+, like o-Ps, undergoes Anderson localization at empty sites of the, static or dynamic, disordered structure. The hole size distribution, its mean value, < v(h)>, and dispersion, at,, were calculated from the o-Ps lifetimes. A comparison of < v(h)> with Vf was used to estimate the specific hole number, N-h('). During melting of the semicrystalline samples at-38 degrees C (T-m), < v(h)> increased abruptly, and sigma(h) suddenly decreased. Both effects are explained by the disappearance of the rigid-amorphous fraction (RAF) and, thus, a reduction in the dynamic heterogeneity. The following leveling-off in (v(h)) and the low value of sigma(h) are attributed to the fast segmental relaxation in the PDMS melts which leads to a smearing of the molecule density distribution around a hole during the o-Ps lifetime.
引用
收藏
页码:827 / 840
页数:14
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