UBC Faculty Research and Publications

A β-NMR study of the depth, temperature and molecular-weight dependence of secondary dynamics in polystyrene. Entropy-enthalpy compensation and dynamic gradients near the free surface McKenzie, Iain; Fujimoto, Derek; Karner, Victoria L.; Li, Ruohong; MacFarlane, W. Andrew; McFadden, Ryan M. L.; Morris, Gerald D.; Pearson, Matthew R.; Raegen, Adam N.; Stachura, Monika; Ticknor, John O.; Forrest, James A.

Abstract

We investigated the depth, temperature and molecular-weight (MW) dependence of the γ-relaxation in polystyrene glasses using implanted 8Li+ and β-detected NMR (β-NMR). Measurements were performed on thin films with MW ranging from 1.1 to 641 kg/mol. The temperature dependence of the average 8Li spin-lattice relaxation time (Tavg1) was measured near the free surface and in the bulk. Spin-lattice relaxation is caused by phenyl ring flips, which involve transitions between local minima over free-energy barriers with enthalpic and entropic contributions. We used transition state theory to model the temperature dependence of the γ-relaxation, and hence Tavg1. There is no clear correlation of the average entropy of activation (∆‡S) and enthalpy of activation (∆‡H) with MW, but there is a clear correlation between ∆‡S and ∆‡H, i.e. entropy-enthalpy compensation. This results in the average Gibbs energy of activation, ∆‡G, being approximately independent of MW. Measurements of the temperature dependence of Tavg1 as a function of depth below the free surface indicate the inherent entropic barrier, i.e. the entropy of activation corresponding to ∆‡H = 0, has an exponential dependence on distance from the free surface before reach ing the bulk value. This results in ∆‡G near the free surface being lower than the bulk. Combining these observations results in a model where the average fluctuation rate of the γ-relaxation has a “double-exponential” depth dependence. This model can explain the depth dependence of 1/Tavg1in polystyrene films. The characteristic length of enhanced dynamics is ∼6 nm and approximately independent of MW near room temperature.

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