Materials for engineering, 3rd Edition - (Malestrom)
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186<br />
<strong>Materials</strong> <strong>for</strong> <strong>engineering</strong><br />
6.2 Manufacture of composite materials<br />
As stated above, fibre composite materials represent a major part of this<br />
category: a wide range of possible fibres exists and Table 6.1 illustrates the<br />
range of properties they possess. The most widely used fibres are of carbon,<br />
glass and Kevlar and the method of their production is outlined below.<br />
6.2.1 Carbon fibres<br />
Carbon fibres consist of small crystallites of graphite, whose crystal structure<br />
is shown in Fig. 1.1(b). The atoms in the basal planes are held together by<br />
very strong covalent bonds, and there are weak van der Waals <strong>for</strong>ces between<br />
the layers. To obtain high modulus and high strength, the layer planes of the<br />
graphite have to be aligned parallel to the axis of the fibre and the modulus<br />
of carbon fibres depends on the degree of perfection of alignment of the<br />
atom planes. This varies considerably with the particular manufacturing route<br />
adopted, of which there are three main possibilities:<br />
(a) The polymer PAN (polyacrylonitrile), which closely resembles<br />
polyethylene in molecular con<strong>for</strong>mation, is converted into a fibre and<br />
then stretched to produce alignment of the molecular chains along the<br />
fibre axis. When the stretched PAN fibre is heated, the nitrile groups<br />
interact so that the flexible molecule is changed into a rigid ‘ladder’<br />
molecule. While still under tension, it is heated in oxygen, which leads<br />
to further cross-links between the ladder molecules. It is finally chemically<br />
reduced to give (at high temperatures) a graphitic structure. The final<br />
graphitization temperature determines whether the fibres have maximum<br />
stiffness but a relatively low strength (Type I fibres), or whether they<br />
develop maximum strength (Type II).<br />
Table 6.1 Mechanical properties of some rein<strong>for</strong>cing fibres<br />
Material Density ρ Young’s Tensile Fibre radius r<br />
(Mg m –3 ) modulus E strength σ* (µm)<br />
(GPa) (GPa)<br />
E-glass fibres 2.56 76 1.4–2.5 10<br />
Carbon fibres 1.75 390 2.2 8.0<br />
(high modulus)<br />
Carbon fibres 1.95 250 2.7 8.0<br />
(high strength)<br />
Kevlar fibres 1.45 125 3.2 12<br />
Silicon carbide 3.00 410 8.6 140<br />
(monofilament)<br />
Silicon carbide 2.50 180 5.9 14<br />
(Nicalon)<br />
Alumina (Saffil) 2.80 100 1.0 3