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Ph.D. thesis (pdf) - dirac

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8 Slow and fast dynamics<br />

glass. The volume of the glass is also dependent on temperature, but its temperature<br />

dependence is weaker than that of the liquid. This is so because the molecules in<br />

the liquid rearrange upon cooling while the glass contracts only due to a decrease<br />

in the distance between the molecules. The difference between the liquid and the<br />

glass responses to temperature changes gives rise to an abrupt change in slope on a<br />

T − V plot. A typical plot is shown in figure 2.1. The change in the temperature<br />

dependence of the volume gives rise to a discontinuity in the expansivity when passing<br />

T g . The heat capacity and other thermodynamical derivatives have equivalent<br />

discontinuities at T g . If the glass is kept below T g the liquid approaches equilibrium,<br />

though it happens slowly, and the volume and other properties are therefore time<br />

dependent; the glass ages. This means that strictly speaking the thermodynamic<br />

derivatives are not strictly well defined in the glass. It also leads to hysteresis in<br />

the system. The hysteresis is seen in the re-heating curve which is also indicated in<br />

figure 2.1.<br />

The relaxation time increases very rapidly in the vicinity of T g ; this means that the<br />

aging processes are very slow already a few degrees below T g . When considered at<br />

times shorter than the relaxation time the glass behaves like a solid in all senses.<br />

It is therefore possible to measure and assign meaningful “apparent” values to the<br />

properties of the glass, including the thermodynamical derivatives (figure 2.1).<br />

V or H<br />

αP or cP<br />

T g<br />

Temperature<br />

T g<br />

Temperature<br />

Figure 2.1: Illustration of the temperature dependence of volume, enthalpy and their<br />

temperature derivatives when passing the glass transition.<br />

The freezing in of the liquid at T g has the consequence that the structure of the<br />

glass is that of the liquid when it fell out of equilibrium at T g . The glass is hence<br />

a disordered solid, and it cannot be distinguished from a liquid from a structural<br />

point of view.<br />

A liquid has a T g that depends on the cooling rate (lower cooling rates give lower T g ).

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