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Materials for engineering, 3rd Edition - (Malestrom)

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Organic polymeric materials 165<br />

5.5 Rotations about bonds in a polymer chain.<br />

The mechanical properties of polymers are there<strong>for</strong>e time and temperature<br />

dependent and Fig. 5.6 illustrates schematically how, <strong>for</strong> a constant loading<br />

time, the elastic modulus of a polymer will change with the temperature of<br />

de<strong>for</strong>mation normalized with respect to T g . At temperatures well below T g ,<br />

it will be brittle-elastic, then, passing through the T g range, it becomes viscoelastic,<br />

then rubbery and eventually viscous. As indicated in Fig. 5.6, the<br />

modulus can change by a factor of 10 3 or more over this range.<br />

10 4<br />

10 3<br />

Glassy plateau<br />

Constant<br />

loading<br />

time (t)<br />

Modulus (MPa)<br />

10 2<br />

10<br />

1<br />

10 –1<br />

Secondary<br />

transitions<br />

Glass transition<br />

Rubbery plateau<br />

Viscous flow<br />

10 –2<br />

0 0.5 1.0 1.5 2.0 2.5<br />

Normalized temperature (T/T g )<br />

5.6 Showing <strong>for</strong> a constant loading time how the elastic modulus of a<br />

polymer changes with temperature.

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