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Metal Foams: A Design Guide

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Chapter 14<br />

Electrical properties of metal foams<br />

The electrical conductivity of a metal foam is less than that of the metal from<br />

which it is made for the obvious reason that the cell interiors, if gas-filled, are<br />

non-conducting. One might guess that the conductivity should vary linearly<br />

with the relative density, but the real dependence is stronger than linear, for<br />

reasons explained below. Though reduced, the conductivity of metal foams<br />

is more than adequate to provide good electrical grounding and shielding of<br />

electromagnetic radiation.<br />

The large, accessible surface area of open cell metal foams makes them<br />

attractive as electrodes for batteries (see Case Study 17.6). Nickel foams are<br />

extensively used in this application.<br />

14.1 Measuring electrical conductivity or resistivity<br />

The electrical resistivity of a thick metal foam sheet can be measured using a<br />

four-point probe technique sketched in Figure 14.1. Two probes (P1 and P4)<br />

are used to introduce a current, I, into the sample while a pair of different<br />

probes (P2 and P3) are used to measure the potential drop, V, between them.<br />

If the plate is sufficiently thick, the electrical resistivity, 2, of the foam<br />

(commonly measured in units of µ . cm) is given by:<br />

2 D 2<br />

where<br />

� �<br />

V<br />

IS<br />

⊲14.1⊳<br />

S D 1<br />

C<br />

s1<br />

1<br />

s3<br />

1<br />

s1 C s2<br />

1<br />

s2 C s3<br />

⊲14.2⊳<br />

and s1, s2 and s3, are the probe spacings shown in the figure.<br />

The electrical conductivity, (units, 1 1 . m ), is the reciprocal of the<br />

resistivity. The resistance, R, of a piece of foam of length ℓ and a crosssectional<br />

area A normal to the direction of current flow is given by:<br />

R D 2 ℓ ℓ<br />

D<br />

A A<br />

⊲14.3⊳

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