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Ph.D. thesis (pdf) - dirac

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7.3. Relation to alpha relaxation 127<br />

Glycerol is known to be a case where the temperature dependence of the mean<br />

square displacement passes smoothly through T g at atmospheric pressure. This is<br />

seen in figure 7.6, where we also display the mean square displacement at 300 MPa.<br />

The slope changes rapidly at about 1.25T g in both cases (figure 7.7).<br />

0.25<br />

0.2<br />

P=0.1 MPa<br />

300 MPa<br />

Tg<br />

Tg @ 300 MPa<br />

[A 2 ]<br />

0.15<br />

0.1<br />

0.05<br />

0<br />

0 50 100 150 200<br />

T [K]<br />

Figure 7.6: The 〈u 2 〉 of glycerol at ambient pressure and at 300 MPa.<br />

0.5<br />

0.45<br />

0.4<br />

0.35<br />

P=0.1 MPa<br />

300 MPa<br />

Tg<br />

Tg @ 300 MPa<br />

[A 2 ]<br />

0.3<br />

0.25<br />

0.2<br />

0.15<br />

0.1<br />

0.05<br />

0<br />

0 50 100 150 200 250 300<br />

T [K]<br />

Figure 7.7: The 〈u 2 〉 of glycerol at ambient pressure and at 300 MPa.<br />

7.3 Relation to alpha relaxation<br />

From the data shown in the previous section it is seen that the mean square displacement<br />

at the nanosecond timescale often has a change in its temperature dependence<br />

in the vicinity of T g , which is governed by the dynamics on the time scale of hundreds<br />

of seconds. This is a general observation and it is probably the most clear example<br />

of a coupling between fast and slow dynamics [Buchenau and Zorn, 1992; Angell,<br />

1995; Casalini and Ngai, 2001; Ngai, 2000]. The origin of this coupling is considered

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