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Ph.D. thesis (pdf) - dirac

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3.5. Summary 41<br />

assumption that the empirical scaling law (equation 3.2.1) holds, it moreover follows<br />

that the temperature and density dependence of G should be described in terms of<br />

an equivalent scaling law. This is most easily seen by inserting equation 3.4.1 in<br />

equation 3.2.2 (where Φ ′ below is proportional to Φ) :<br />

( ) T<br />

G(ρ, T) = e(ρ)Φ ′ e(ρ)<br />

(3.4.4)<br />

where e(ρ) is the same as in (equation 3.2.1). See also [Alba-Simionesco and Tarjus,<br />

2006] for similar ideas.<br />

3.5 Summary<br />

Fragility involves a variation with temperature that a priori depends on the thermodynamic<br />

path chosen, namely constant pressure (isobaric) versus constant density<br />

(isochoric) conditions. On the other hand, many quantities that have been correlated<br />

to fragility only depend on the thermodynamic state at which they are considered.<br />

It has been found empirically that the isochoric fragility is intrinsic in the sense that<br />

it is independent of pressure when evaluated along an isochrone. Based on these<br />

observation we conclude that a property which is related to the “pure” effect of<br />

temperature on the relaxation time, should correlate to the isochoric fragility (when<br />

comparing systems), and that it should possess the same type of intrinsic character;<br />

that is, they should be constant along an isochrone for a given system. Properties<br />

related to a combined effect of temperature and density are on the other hand expected<br />

to correlate with isobaric fragility and to have a pressure dependence that<br />

corresponds to its pressure dependence - that is most often decrease with increasing<br />

pressure. The ideas put forward in this chapter are a central part of the work and<br />

serve as a reference point for a large part of the analysis in the proceeding chapters.

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