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Materials for engineering, 3rd Edition - (Malestrom)

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210<br />

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

But l c /r = σ f /τ y , so<br />

W f f l c<br />

= σ l 12<br />

f c<br />

[6.11]<br />

l<br />

For maximum work of fracture, there<strong>for</strong>e, l c should be maximized and<br />

fibre length should be equal to l c . If the fibre length is less than l c , the work<br />

of fracture is obtained by setting l c = l in the integral:<br />

ff<br />

W =<br />

πr<br />

2<br />

∫<br />

lc /2 2<br />

0<br />

(2 πrτx<br />

) d x<br />

l<br />

= f f πτ l 2 /12r. [6.12]<br />

Thus, <strong>for</strong> fibres of a given constant value of critical length, as the fibre<br />

length in the composite is increased, the work of pullout initially increases<br />

as l 2 (equation [6.12]). When the fibre length is greater than the critical<br />

length, the work of pullout decreases as l –1 , (equation [6.11]), as more fibres<br />

break rather than pull out. These relationships are illustrated in Fig. 6.20.<br />

6.4.4 Fatigue behaviour of fibre composites<br />

The introduction of short fibres into a polymer can enhance its resistance to<br />

both the nucleation and the growth of fatigue cracks. Thus, Fig. 6.21 presents<br />

a series of S–N curves <strong>for</strong> injection moulded PSF with increasing volume<br />

I 2 1<br />

Pull-out energy<br />

l<br />

I c<br />

Fibre length (I)<br />

6.20 Pull-out energy as a function of fibre length.

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