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Metal Foams: A Design Guide

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H<br />

H<br />

Core shear<br />

Core shear<br />

Collapse mode A<br />

F<br />

;;<br />

a;;<br />

;;<br />

;;<br />

Collapse mode B<br />

F<br />

a;;<br />

;;<br />

;;<br />

;;<br />

M p<br />

M p<br />

H<br />

H<br />

Sandwich structures 119<br />

Figure 10.4 Competing collapse modes A and B for core shear of a<br />

sandwich beam in three-point bending<br />

We note from equation (10.17) that FA increases linearly with the length of<br />

overhang, H, beyond the outer supports.<br />

Second, consider collapse mode B. As sketched in Figure 10.4, this collapse<br />

mechanism involves the formation of plastic hinges in the face sheets at both<br />

mid-span and at the outer supports. The core undergoes simple shear over the<br />

length, L, between the outer supports, with no deformation beyond the outer<br />

supports. A work calculation gives for the plastic collapse load FB,<br />

FB D 4bt2<br />

ℓ<br />

f<br />

y C 2bc c y<br />

⊲10.18⊳<br />

Since the two calculations given above are upper bounds for the actual<br />

collapse load, the lower is taken as the best estimate for the actual collapse<br />

load. It is instructive to compare the collapse loads as a function of overhang<br />

length H, as sketched in Figure 10.5. Collapse mode A is activated for small<br />

lengths of overhang, whereas collapse mode B has the lower collapse load<br />

and is activated for large overhangs. The transition length of overhang, Ht, is<br />

determined by equating (10.17) and (10.18), giving<br />

Ht D 1 t<br />

2<br />

2<br />

c<br />

f<br />

y<br />

c<br />

y<br />

⊲10.19⊳

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