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Materials for engineering, 3rd Edition - (Malestrom)

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58<br />

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

σ a<br />

σ m σ Y σ UTS<br />

σ fo<br />

Gerber<br />

Goodman<br />

Soderberg<br />

2.16 Models relating mean stress to fatigue stress range.<br />

The Soderberg model, which provides a conservative estimate of fatigue life<br />

<strong>for</strong> most <strong>engineering</strong> alloys, predicts a linear decrease in the fatigue stress<br />

with increasing mean stress up to σ y :<br />

σ fm = (1 – σ m /σ y ) [2.26]<br />

Low-cycle fatigue<br />

The stresses associated with low-cycle fatigue are generally high enough to<br />

cause appreciable plastic de<strong>for</strong>mation be<strong>for</strong>e fracture and, in these<br />

circumstances, the fatigue life is characterized in terms of the strain range.<br />

Coffin (1954) and Manson (1954) noted that when the logarithm of the<br />

plastic strain amplitude, ∆ε p /2, was plotted against the logarithm of the<br />

number of load reversals to failure, 2N f , <strong>for</strong> metallic materials, a linear result<br />

was obtained, i.e.<br />

∆ε /2 = ε′ (2 N )<br />

c [2.27]<br />

p f f<br />

where ε f ′ is the fatigue ductility coefficient and c the fatigue ductility exponent.<br />

The total strain amplitude ∆ε/2 is the sum of the elastic strain amplitude<br />

∆ε e /2 and ∆ε p /2, but

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