Materials for engineering, 3rd Edition - (Malestrom)
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
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.