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Metal Foams: A Design Guide

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Chapter 7<br />

A constitutive model for metal foams<br />

The plastic response of metal foams differs fundamentally from that of fully<br />

dense metals because foams compact when compressed, and the yield criterion<br />

is dependent on pressure. A constitutive relation characterizing this plastic<br />

response is an essential input for design with foams.<br />

Insufficient data are available at present to be completely confident with<br />

the formulation given below, but it is consistent both with a growing body<br />

of experimental results, and with the traditional development of plasticity<br />

theory. It is based on recent studies by Deshpande and Fleck (1999, 2000),<br />

Miller (1999) and Gibson and co-workers (Gioux et al., 1999, and Gibson and<br />

Ashby, 1997).<br />

7.1 Review of yield behavior of fully dense metals<br />

Fully dense metals deform plastically at constant volume. Because of this,<br />

the yield criterion which characterizes their plastic behavior is independent<br />

of mean stress. If the metal is isotropic (i.e. has the same properties in all<br />

directions) its plastic response is well approximated by the von Mises criterion:<br />

yield occurs when the von Mises effective stress e attains the yield<br />

value Y.<br />

The effective stress, e, is a scalar measure of the deviatoric stress, and is<br />

defined such that it equals the uniaxial stress in a tension or compression test.<br />

On writing the principal stresses as ( I, II, III), e canbeexpressedby<br />

2 2 e D ⊲ I II⊳ 2 C ⊲ II III⊳ 2 C ⊲ III I⊳ 2<br />

⊲7.1⊳<br />

When the stress s is resolved onto arbitrary Cartesian axes Xi, not aligned with<br />

the principal axes of stress, s has three direct components ( 11, 22, 33) and<br />

three shear components ( 12, 23, 31), and can be written as a symmetric 3 ð 3<br />

matrix, with components ij. Then, the mean stress m, which is invariant with<br />

respect to a rotation of axes, is defined by<br />

m<br />

1<br />

3⊲ 11 C 22 C 33⊳ D 1<br />

3 kk ⊲7.2⊳<br />

where the repeated suffix, here and elsewhere, denotes summation from 1 to<br />

3. The stress s can be decomposed additively into its mean component m

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