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Metal Foams: A Design Guide

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<strong>Design</strong> analysis for material selection 59<br />

Using equations (5.2) and (5.3) to eliminate t in equation (5.1) gives the<br />

performance equation for the performance metric, m:<br />

m ½<br />

� �<br />

Ł 2<br />

1/3<br />

12S b<br />

B1<br />

�<br />

2<br />

ℓ<br />

E1/3 �<br />

⊲5.4⊳<br />

This equation for the performance metric, m, is the objective function – it is<br />

the quantity we wish to minimize.<br />

All the quantities in equation (5.4) are specified by the design except the<br />

group of material properties in the last bracket, /E1/3 . This is the material<br />

index for the problem. The values of the performance metric for competing<br />

materials scale with this term. Taking material M0 as the reference (the incumbent<br />

in an established design, or a convenient standard in a new one), the<br />

performance metric of a competing material M1 differs from that of M0 by<br />

the factor<br />

m1<br />

D<br />

m0<br />

⊲ 1/E 1/3<br />

1 ⊳<br />

⊲ 0/E 1/3<br />

0 ⊳<br />

⊲5.5⊳<br />

where the subscript ‘0’ refers to M0 and the ‘1’ to M1.<br />

Panel of specified strength and minimum mass<br />

If, for the panel of Figure 5.1, the constraint were that of bending strength<br />

rather than stiffness, the constraining equation becomes that for failure load,<br />

Ff, per unit width, meaning the onset of yielding:<br />

Ff D B2 yI<br />

btℓ ½ FŁ f ⊲5.6⊳<br />

where B2, like B1, is a constant that depends only on the distribution of the<br />

load; it is tabulated in Chapter 6, Section 6.4. The performance metric, again,<br />

is the mass, m:<br />

� �<br />

m �<br />

�<br />

Ł<br />

6Ffb 2<br />

�1/2 ℓ<br />

B2<br />

3/2<br />

1/2<br />

y<br />

⊲5.7⊳<br />

where y the yield strength of the material of which the panel is made and F Ł f b<br />

is the desired minimum failure load. Here the material index is / 1/2<br />

y .Taking<br />

material M0 as the reference again, the performance metric of a competing<br />

material M1 differs from that of M0 by the factor<br />

m1<br />

m0<br />

D ⊲ 1/ 1/2<br />

y,1 ⊳<br />

⊲ 0/ 1/2<br />

y,0 ⊳<br />

⊲5.8⊳

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