Abstract
We study the significant entropy changes in supercooling and glass transition by developing a two (H and L) state cluster model, where the H-state represents the clusters with the coordination number z being larger than the reference size z R and the L-state those with z < z R , respectively. We exploit the excluded volume effect on the clustering behaviors of various glass-formers and the temperature dependence (at fixed pressure of 1 atmosphere) of the entropy difference Δ s o between the two cluster states on the basis of z R = 1 + z R o [ exp ( − Δ s o / k B ) − 1 ] , where z R o = 1.8 as taken universally for all the glass-formers investigated. The temperature dependence of the average size 〈 z c ∗ 〉 of clusters with z ≥ z R is then determined for some representative glass-formers, such as GeO 2, 1-propanol, glycerol, propylene carbonate, o-terphenyl, and so forth, covering the entire fragility spectrum studied experimentally. As a result, the temperature dependence of 〈 z c ∗ 〉 is found to highly depend on the fragility index ϑ associated with the temperature dependence of the excluded volume B ∗ ( ϕ , T ) of which statistical mechanical representation is given by the generic van der Waals equation of state. With decreasing T toward the glass transition temperature T g , 〈 z c ∗ 〉 increases to attain universally about 13 at T g regardless of the fragility and molecular details of the glass-formers. We specifically analyze in depth the theoretical predictions for the cluster sizes and the experimental estimations for the length scales associated with temporary clusters of slow segments in supercooled glycerol as about 1.4±0.5 nm for glycerol at 10 K above T g . Given the large uncertainties associated with the experiment, the present theory appears to be in good agreement with the experiment.
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More From: Physica A: Statistical Mechanics and its Applications
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