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Materials for engineering, 3rd Edition - (Malestrom)

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Determination of mechanical properties 41<br />

2.2.2 The <strong>engineering</strong> stress–strain curve<br />

The load–elongation curve of Fig. 2.3 may be converted into the <strong>engineering</strong><br />

stress–strain curve as shown in Fig. 2.4 The <strong>engineering</strong>, or conventional,<br />

stress σ is given by dividing the load (L) by the original cross-sectional area<br />

of the gauge length (A o ), and the strain (e) is as defined above, namely the<br />

extension of the gauge length (l – l o ) divided by gauge length (l o ).<br />

The maximum conventional stress in Fig. 2.3 known as the Ultimate<br />

Tensile Stress (UTS) is defined as:<br />

UTS = L max /A o<br />

and this property is widely quoted to identify the strength of materials.<br />

The tensile test also provides a measure of ductility. If the fractured testpiece<br />

is reassembled, the final length (l f ) and final cross-section (A f ) of the<br />

gauge length may be measured and the ductility expressed either as the<br />

<strong>engineering</strong> strain at fracture:<br />

e f = (l f – l o )/l o ,<br />

or the reduction is cross-section at fracture, RA, where:<br />

RA = (A o – A f )/A o<br />

These quantities are usually expressed as percentages. Because much of<br />

the plastic de<strong>for</strong>mation will be concentrated in the necked region of the<br />

gauge length, the value of e f will depend on the magnitude of the gauge<br />

length – the smaller the gauge length the greater the contribution to e f from<br />

the neck itself. The value of the gauge length should there<strong>for</strong>e be stated<br />

when recording the value of e f .<br />

2.2.3 True stress–strain curve<br />

The fall in the <strong>engineering</strong> stress after the UTS is achieved, due to the<br />

UTS<br />

Engineering stress (σ)<br />

Strain (e)<br />

2.4 Engineering stress–strain curve.<br />

e f

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