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Metal Foams: A Design Guide

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

Strain, ε<br />

Primary<br />

Elastic<br />

Time, t (s)<br />

t R (Rupture)<br />

•<br />

εss Secondary<br />

Figure 9.1 Schematic of creep strain response of a metal under constant<br />

load<br />

dominant; the secondary creep rate, Pε, then depends on the stress, ,raisedto<br />

a power n>1:<br />

� �n Pε DPε0<br />

⊲9.1⊳<br />

where<br />

0<br />

Pε0 D A exp<br />

� �<br />

Q<br />

RT<br />

Here n, 0 and Q are properties of the material ( 0 is a reference stress and Q<br />

is the activation energy for the kinetic process controlling the rate of creep), A<br />

has the dimensions 1/second and R is the ideal gas constant (8.314 J/mole K).<br />

Typical values for n, 0 and Q for power-law creep of several solid metals<br />

are listed in Table 9.1.<br />

The time to rupture for a solid metal can be found by assuming that failure<br />

is associated with a constant critical strain in the material so that the product<br />

Table 9.1 Power law creep parameters for solid metals<br />

Material n 0 (MPa) Q (kJ/mole)<br />

Aluminum 4.4 0.12 142<br />

Nickel 4.6 0.5 284<br />

316 Stainless steel 7.9 33.5 270

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