The development of the dynamic glass transition in
poly(n-alkyl methacrylate)s is
investigated with broad-band dielectric spectroscopy in the frequency
range from 10-4 to 109 Hz.
The
experimental data were analyzed by adjustment with one or a sum of two
Havriliak Negami functions.
Upon decreasing the temperature, the high-temperature relaxation
(a) changes into the local β relaxation
(Johari Goldstein mode), and the cooperative α relaxation sets in
close to this aβ transition. For poly(n-butyl methacrylate) a separate onset (zero intensity) of
the α process and a parallel course of both
traces in the Arrhenius diagram were observed. The activation
energy of the β process does not change
in spite of the parallel development of the α process. On the
other hand, for poly(ethyl methacrylate) the
α onset is close to a bend in the local process, i.e., the activation
energy of the latter changes after the α
onset. In both materials the intensity of the α process linearly
increases with falling temperatures but
with different intensity. Several scenarios for the
αβ-splitting region are suggested.
Dynamic heterogeneity is an active field of glass-transition research. The length scale of this heterogeneity is called the characteristic length. It can be calculated from complex heat capacity curves in the equilibrium liquid or from dynamic calorimetry curves corrected with regard to nonequilibrium. No molecular parameters or microscopic models are necessary for obtaining the length. We report the characteristic length near glass temperature for about 30 glass formers including small-molecule liquids, polymers, silicate glasses, a metallic glass, a liquid crystal, and a plastic crystal. The lengths are between 1.0 and 3.5 nm with certain cumulations between 1.0 and 2.0 nm and between 2.5 and 3.5 nm. To try a correlation to other properties, we find that at least two should be included, e.g., Angell's fragility and the distance of T g from the crossover temperature, T c .
Shear data in the temperature range from −145 °C to the flow zone are presented for the
poly(n-alkyl methacrylate)s from methyl (C = 1) to lauryl (C = 12). Three qualitatively different glass
transitions are observed in the shear curves at 10 rad/s: (i) the conventional α process in the C < 5
members, (ii) the high temperature a process in the C > 5 members, and (iii) an additional polyethylene-like glass transition, αPE, in the C ≥ 3 members. All three processes depend systematically on side chain
length. Two alternative empirical pictures for the coexistence of two glass transitions are discussed: (a)
a static nanophase separation between main chains and side chains and (b) a dynamic heterogeneity
with two different time and length scales.
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