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Metal Foams: A Design Guide

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138 <strong>Metal</strong> <strong>Foams</strong>: A <strong>Design</strong> <strong>Guide</strong><br />

Weight index, Y<br />

1<br />

0.1<br />

0.002<br />

Π = 10−4 εf = 0.007<br />

Y<br />

0.001<br />

Inaccessible<br />

domains<br />

A<br />

Face<br />

yield<br />

Global weight minimum<br />

A<br />

Core<br />

yield<br />

0.01<br />

Stiffness index, X<br />

Weight/stiffness<br />

Y = 3.19 X 3/5<br />

Figure 10.14 The relationship between X and Y showing the region<br />

bounded by core and face yield<br />

For specific conditions, the equality of (10.38) corresponds to a point on<br />

the curve of weight versus stiffness (Figure 10.14) below which the elastic<br />

predictions are no longer valid. For values of the stiffness index below this<br />

point, weights in excess of the global minimum would be needed to ensure that<br />

the beam remains elastic. Logarithmic axes have been used in Figure 10.14<br />

to highlight the inadmissible range.<br />

Analogous conditions exist for core yielding (equation 10.24(c)). The coefficient<br />

B4 is defined such that the maximum shear stress in the core is P/⊲B4bc⊳,<br />

and thus yielding occurs when<br />

P>B4bc c y<br />

0.1<br />

⊲10.39⊳<br />

This condition can also be written in terms of X for the case of the globally<br />

optimized beams. Core yielding invalidates the results based on the elastic<br />

optimization if<br />

X � 1<br />

48<br />

� 1<br />

�<br />

B1<br />

B4 ˛2B2<br />

� 1/2 � P<br />

bℓ c y<br />

�� 5<br />

Elastic wrinkling of the face sheets may also occur (equation (10.24b)).<br />

⊲10.40⊳

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