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Metal Foams: A Design Guide

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<strong>Design</strong> for creep with metal foams 111<br />

The shear deflection rate is calculated from the creep of the core. The<br />

power-law creep of the foam core under uniaxial stress is given by:<br />

� �nc Pε DPε0<br />

⊲9.16⊳<br />

0<br />

where Pε0, 0 and nc are the creep parameters of the core material. The core<br />

is subjected to both normal and shear loading; in general, for metallic foam<br />

cores, both are significant. The creep shear strain rate is calculated using<br />

equations (9.6) and (9.7):<br />

and<br />

Pε12 D f⊲ O ⊳<br />

O 2 D<br />

Noting that<br />

e D<br />

∂ O<br />

∂ 12<br />

⊲9.17⊳<br />

1<br />

1 C ⊲˛/3⊳ 2 [ 2 e C ˛2 2 m ] ⊲9.18⊳<br />

� 211 C 3<br />

2<br />

2 3<br />

12 C 2<br />

and that m D 11/3 gives<br />

O D<br />

�<br />

2<br />

21<br />

2<br />

11 C<br />

3<br />

2<br />

1 C ⊲˛/3⊳ 2 ⊲ 2 12 C 2 21⊳ �1/2 Taking the partial derivative with respect to 12 gives:<br />

∂ O<br />

∂ 12<br />

D<br />

3<br />

2 12<br />

1 C ⊲˛/3⊳ 2<br />

�<br />

211<br />

C<br />

3<br />

1 C ⊲˛/3⊳ 2<br />

� 1/2<br />

2<br />

12<br />

Using equation (9.9) for f⊲ O ⊳ gives:<br />

� �nc O 3 12<br />

P D 2 Pε12 DPε0<br />

1 C ⊲˛/3⊳ 2<br />

�<br />

211 3<br />

C<br />

1 C ⊲˛/3⊳ 2<br />

0<br />

� 1/2<br />

2<br />

12<br />

⊲9.19⊳<br />

⊲9.20⊳<br />

⊲9.21⊳<br />

Noting that the normal stress varies through the depth of the beam, in<br />

general the shear strain rate has to be integrated over the depth of the beam.<br />

The derivative of the shear deflection with respect to x, along the length of<br />

the beam, is given by (Allen, 1969):<br />

d Pυs<br />

dx DPc<br />

d<br />

⊲9.22⊳

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