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Metal Foams: A Design Guide

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

t<br />

c<br />

t<br />

b<br />

F<br />

d(= c +2t)<br />

Figure 9.6 Sandwich beam loaded in three-point bending<br />

and core are t and c, respectively. The faces have a Young’s modulus, Ef,<br />

and the core has a Young’s modulus, Ec, and a shear modulus Gc. The elastic<br />

and plastic deflection of a sandwich beam are analysed in Chapter 10. The<br />

creep deflection is found from the sum of the bending and shearing deflection<br />

rates. Consider the faces first. The power-law creep response of the faces is<br />

given by:<br />

Pε D Af nf ⊲9.10⊳<br />

where Af and nf are the creep parameters of the face material. Assuming that<br />

plane sections remain plane,<br />

Pε D y P ⊲9.11⊳<br />

and<br />

�<br />

y P<br />

D<br />

Af<br />

� 1/nf<br />

⊲9.12⊳<br />

Assuming also that the moment carried by the faces is much larger than<br />

that carried by the core, then<br />

� h/2 � �1/nf y P<br />

M D 2<br />

yb dy ⊲9.13⊳<br />

c/2<br />

Af<br />

D B 2b<br />

A 1/nf<br />

P<br />

f<br />

1/nf<br />

where<br />

1<br />

B D<br />

2 C 1<br />

nf<br />

� �h<br />

2<br />

� �<br />

2C⊲1/nf⊳ � c �2C⊲1/nf⊳ 2<br />

The bending deflection rate at the center of the beam is then:<br />

� �nf P ⊲ℓ/2⊳<br />

PυbmaxD Af<br />

4bB<br />

nfC2 � �<br />

1<br />

1<br />

nf C 1 nf C 2<br />

⊲9.14⊳<br />

⊲9.15⊳

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