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Metal Foams: A Design Guide

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Chapter 4<br />

Properties of metal foams<br />

The characteristics of a foam are best summarized by describing the material<br />

from which it is made, its relative density, / s (the foam density, , divided<br />

by that of the solid material of the cell wall, s), and stating whether it has<br />

open or closed cells. Beyond this, foam properties are influenced by structure,<br />

particularly by anisotropy and by defects – by which we mean wiggly, buckled<br />

or broken cell walls, and cells of exceptional size or shape.<br />

<strong>Metal</strong> foams are still inadequately characterized, but the picture is changing<br />

rapidly. An overview of the range spanned by their properties is given by<br />

Table 4.1 and the property charts of Section 4.3. The primary links between<br />

properties, density and structure are captured in scaling relations, listed in<br />

Section 4.4. They allow foam properties to be estimated, at an approximate<br />

level, when solid properties are known.<br />

The producers of metal foams have aggressive development programs for<br />

their materials. The properties described here are those of the currently available<br />

generation of foams, and should be regarded as a basis for initial, scoping,<br />

calculations and designs. The next generation of foams will certainly be better.<br />

Final design calculations must be based on data provided by the supplier.<br />

4.1 Foam structure<br />

Figures 4.1(a)–(c) show the structure of metal foams from three different<br />

suppliers: Cymat, Mepura (Alulight) and Shinko (Alporas). The structures are<br />

very like those of soap films: polyhedral cells with thin cell faces bordered<br />

by thicker cell edges (‘Plateau borders’). Some of the features appear to be<br />

governed by surface energy, as they are in soap films: the Plateau borders are<br />

an example. But others are not: many faces have non-uniform curvature or<br />

are corrugated, and have occasional broken walls that still hang in place.<br />

The three figures are ordered such that the relative density increases from<br />

the top to the bottom. The Cymat (Al–SiC) foam in Figure 4.4(a) has a relative<br />

density / s D 0.05, and an average cell size approaching 5 mm; foams<br />

from this source are available in the range 0.02 < / s < 0.2. The Alporas<br />

(Al–Ca) foam in Figure 4.4(b) has smaller cells and comes in a narrower<br />

range of relative density: 0.08 < / s < 0.2; that shown here has a value of

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