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Metal Foams: A Design Guide

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

F<br />

Mode<br />

A<br />

F = F A<br />

Mode A Mode B<br />

H t<br />

Overhang, H<br />

Mode B<br />

F = F B<br />

Figure 10.5 The competition between collapse modes A and B for core<br />

shear<br />

In order to gage the practical significance of the overhang, let us take some<br />

representative values for a typical sandwich panel comprising aluminum skins<br />

c and a metallic foam core, with c/ℓ D 0.1, t/c D 0.1, y / f y D 0.005. Then,<br />

the transition overhang length, Ht, isgivenbyHtD0.1ℓ: that is, an overhang<br />

of length 10% that of the sandwich panel span ℓ is sufficient to switch the<br />

collapse mode from mode A to mode B. Furthermore, the enhancement in<br />

collapse load due to plastic bending of the face sheets above the load required<br />

to shear the core is about 20% for a small overhang, H − Ht, and is about<br />

40% for H>Ht. In much of the current literature on sandwich panels, a gross<br />

approximation is made by neglecting the contribution of the face sheets to the<br />

collapse load.<br />

Parallel expressions can be derived for the collapse of a sandwich beam in<br />

four-point bending by core shear. The collapse load for mode A becomes<br />

FA D 2bt2 f<br />

y<br />

ℓ s<br />

C 2bc c �<br />

y 1 C 2H<br />

�<br />

⊲10.20⊳<br />

ℓ s<br />

and that for mode B is<br />

FB D 4bt2<br />

ℓ s<br />

f<br />

y C 2bc c y<br />

⊲10.21⊳<br />

The transition length of overhang at which the expected collapse mode<br />

switches from mode A to mode B is given by the same expression (10.19) as<br />

for a beam in three-point bending.<br />

10.3 Collapse mechanism maps for sandwich panels<br />

It is assumed that the operative collapse mechanism for a sandwich beam is the<br />

one associated with the lowest collapse load. This can be shown graphically

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