Ph.D. thesis (pdf) - dirac
Ph.D. thesis (pdf) - dirac
Ph.D. thesis (pdf) - dirac
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Chapter 5<br />
Alpha Relaxation<br />
The two most distinctive features of the slow dynamics of liquids approaching the<br />
glass transition is the non-Arrhenius temperature dependence of the alpha relaxation<br />
time characterized by the fragility (section 2.2) and the non-Debye character of the<br />
alpha relaxation time (section 2.3) [Angell et al., 2000]. It could even be claimed<br />
that “understanding the glass transition” essentially means understanding these two<br />
phenomena [Dyre, 2006]. The hypo<strong>thesis</strong> that they might be correlated, is therefore<br />
appealing. Böhmer et al. [1993] correlates larger (isobaric) fragility with larger<br />
deviation from Debye relaxation, with the latter measured in terms of stretching<br />
and the paper has been cited 703 times, which is one illustration of the impact of<br />
this idea.<br />
In this chapter we present a study of the pressure and temperature dependence<br />
of the dielectric alpha relaxation time and peak shape in two molecular liquids.<br />
We rationalize the temperature and density dependence in terms of the scaling law<br />
presented in section 3.2 and determine isobaric and isochoric fragility.<br />
We combine our data with data from the literature to revisit the proposed correlation<br />
between stretching and fragility. We do this in terms of the ideas developed in<br />
section 3.3.<br />
5.1 Dielectric spectroscopy<br />
5.1.1 Experimentals<br />
The dielectric measurements were performed at the laboratory, LCP, in Orsay on a<br />
homebuilt setup. The pressure environment was developed prior to this work, while<br />
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