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Materials for engineering, 3rd Edition - (Malestrom)

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164<br />

<strong>Materials</strong> <strong>for</strong> <strong>engineering</strong><br />

2<br />

3<br />

4<br />

Stress<br />

1<br />

Strain<br />

5.4 Schematic stress–strain curves <strong>for</strong> various polymers (see text<br />

<strong>for</strong> key).<br />

Curve 2 is typical of polystyrene below its T g , showing near linear elastic<br />

behaviour up to brittle fracture. Curve 3 is typified by (amorphous)<br />

polycarbonate, which yields in a ductile manner, exhibiting tough behaviour.<br />

We will now consider the mechanical properties in more detail. We have<br />

so far assumed that the mechanical properties of polymers are independent<br />

of the rate of testing, which is not the case because the properties are governed<br />

by the mobility of the constituent polymer chains. This mobility is in turn<br />

dependent on the inherent stiffness of the chain, the degree of chain<br />

entanglement, the extent of cross-linking and the degree of crystallinity.<br />

5.4.1 Stiffness<br />

Consider an individual molecule in an amorphous polymer. When a stress is<br />

applied, de<strong>for</strong>mation can take place by two processes, bond stretching and<br />

bond angle opening, and rotation of segments of chain about the chain<br />

backbone. Below the glass transition temperature, the <strong>for</strong>mer are the main<br />

de<strong>for</strong>mation mechanisms. As the temperature increases above T g , however,<br />

individual backbone bonds are able to rotate (Fig. 5.5) and, since the carbon–<br />

carbon bonds are at an angle of 109° 28′ to one another, this ability to rotate<br />

can bring about enormous shape changes in the polymer chain, which becomes<br />

randomly kinked. Additionally, individual chains can slide locally relative to<br />

each other, with other regions remaining elastically de<strong>for</strong>med. On unloading,<br />

these elastic regions pull the polymer back to its original shape. This viscous<br />

process takes time and the polymer will exhibit leathery properties whose<br />

response can be modelled empirically by ‘spring-and-dashpot’ combinations<br />

as described in Chapter 2.

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