Ph.D. thesis (pdf) - dirac
Ph.D. thesis (pdf) - dirac
Ph.D. thesis (pdf) - dirac
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116 High Q collective modes<br />
[Alba-Simionesco et al., 2004; Casalini and Roland, 2004], and the density dependence<br />
of the relaxation time, which is contained in<br />
d log e(ρ)<br />
d log ρ .<br />
m P<br />
/m ρ<br />
2<br />
1.9<br />
1.8<br />
1.7<br />
1.6<br />
1.5<br />
1.4<br />
1.3<br />
1.2<br />
1.1<br />
1<br />
0 0.2 0.4 0.6 0.8<br />
α<br />
m P<br />
/m ρ<br />
2.2<br />
2<br />
1.8<br />
1.6<br />
1.4<br />
1.2<br />
1<br />
0.55 0.6 0.65 0.7 0.75 0.8 0.85 0.9<br />
f(T g<br />
)<br />
Figure 6.24: The ratio between isochoric and isobaric fragility as a function of f Q (T g )<br />
and α. The legend is found in figure 6.21.<br />
dlog e(ρ)<br />
In figure 6.25 we show the f Q (T g ) value versus<br />
d log ρ<br />
. The amount of data is<br />
limited and the uncertainty on this type of data is large, but it is striking that we<br />
d log e(ρ)<br />
d log ρ<br />
. It is striking<br />
can be determined from the dynamics of the non-viscous<br />
obtain a new correlation. The smaller f Q (T g ) is the larger is<br />
most of all because<br />
d log e(ρ)<br />
d log ρ<br />
liquid at high temperatures [Alba-Simionesco et al., 2002]. We contemplate that<br />
the correlation proposed between f Q (T g ) and m P is a reminiscent signature of a<br />
dlog e(ρ)<br />
correlation between f Q (T g ) and<br />
d log ρ<br />
. An excellent test case for this hypo<strong>thesis</strong><br />
would be to measure f Q (T g ) on sorbitol which has a very high m P -value combined<br />
d log e(ρ)<br />
with an exceptionally low value of<br />
d log ρ<br />
[Roland et al., 2005].<br />
It appears that the anti-correlation between<br />
correlation between<br />
d log e(ρ)<br />
dlog ρ<br />
dlog e(ρ)<br />
d log ρ<br />
and f Q (T g ) is better than the<br />
and α. This is particularly true when considering the<br />
pressure dependence of the quantities in the case of cumene;<br />
d log e(ρ)<br />
dlog ρ<br />
does not depend<br />
on pressure and the pressure dependence of f Q (T g ) is weak whereas α has a<br />
significant pressure dependence. It is difficult to know if the pressure independence<br />
dlog e(ρ)<br />
of f Q (T g ) of cumene is a coincidence or if this could be general for systems with constant<br />
dlog ρ . f Q(T g ) decreases with pressure both in the case of PIB and DBP, the<br />
correlation suggested from figure 6.25 therefore implies that should increase<br />
dlog e(ρ)<br />
d log ρ<br />
with pressure. In section 5.2.1 we show that DBP is in fact a system where<br />
increases with pressure, and PIB could be a similar system (see appendix A).<br />
d log e(ρ)<br />
dlog ρ<br />
A physical significance of the correlation is that the larger the vibrational compressibility<br />
is relative to the total compressibility the more sensitive to density is the