Ph.D. thesis (pdf) - dirac
Ph.D. thesis (pdf) - dirac
Ph.D. thesis (pdf) - dirac
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128 Mean squared displacement<br />
a central question for understanding the glass transition phenomenon [Angell et al.,<br />
2000].<br />
Several more specific relations between the temperature dependence of the alpha<br />
relaxation time and the mean square displacement have been proposed. It is common<br />
to these relations that they associate a larger mean square displacement to a shorter<br />
alpha relaxation time, and hence expect the change of the mean square displacement<br />
just above T g to be more dramatic the more fragile the liquid is. The physical<br />
pictures and starting points vary, but the conclusions can essentially be condensed<br />
to two different hypo<strong>thesis</strong>.<br />
One view is, that the activation energy related to the alpha relaxation time, should<br />
be proportional to T and inversely proportional to the total temperature dependent<br />
T<br />
mean square displacement, E(ρ, T) ∝ , where a is a characteristic distance<br />
a 2 〈u 2 〉(T)<br />
between the relaxing entity. This yields:<br />
( ) Ca<br />
2<br />
τ(T) = τ 0 exp<br />
〈u 2 〉(T)<br />
(7.3.1)<br />
where C is a constant. This view point has mainly been based on so called elastic<br />
models [Dyre and Olsen, 2004], (for a review see [Dyre, 2006]), but it has also been<br />
proposed by Starr et al [Starr et al., 2002] based on a Voronoi volume analysis and<br />
computer simulations.<br />
The other view is that it is a non-harmonic part of 〈u 2 〉 that should be considered<br />
instead of the total 〈u 2 〉. That is E ∝<br />
T<br />
〈u 2 〉 loc (T) , where 〈u2 〉 loc (T) =<br />
〈u 2 〉(T) − 〈u 2 〉 harm (T). It is a little over-simplifying to call this one view, as the<br />
definitions proposed for 〈u 2 〉 loc (T) are not completely equivalent - however this has<br />
minor importance in the present context. This second view point leads to<br />
where K is a constant.<br />
(<br />
τ(T) = τ 0 exp<br />
K<br />
〈u 2 〉 loc (T)<br />
)<br />
, (7.3.2)<br />
We refer to this viewpoint as the relaxational hypo<strong>thesis</strong>. The relaxational hypo<strong>thesis</strong><br />
was originally proposed from a phenomenological relation found between viscosity<br />
and 〈u 2 〉 in selenium [Buchenau and Zorn, 1992]. It has later been supported by Ngai<br />
and coworkers, based on qualitative analysis of data-compilations and an extension<br />
of the coupling model [Ngai, 2000, 2004].