Metal Foams: A Design Guide
Metal Foams: A Design Guide
Metal Foams: A Design Guide
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42 <strong>Metal</strong> <strong>Foams</strong>: A <strong>Design</strong> <strong>Guide</strong><br />
by structure too. This influence, imperfectly understood at present, is a topic of<br />
intense current study. Better understanding will lead to greater process control<br />
and improved properties. But for now we must accept the structures as they<br />
are, and explore how best to design with the present generation of foams.<br />
With this in mind, we document here the properties of currently available,<br />
commercial, metal foams.<br />
4.2 Foam properties: an overview<br />
The ranges of properties offered by currently available metal foams are documented<br />
in Table 4.1. Many suppliers offer a variety of densities; the properties,<br />
correspondingly, exhibit a wide range. This is one of the attractive aspects of<br />
such materials: a desired profile of properties can be had by selecting the<br />
appropriate foam material with the appropriate density.<br />
Nomenclature and designation<br />
It is important to distinguish between the properties of the metfoam and<br />
those of the solid from which it is made. Throughout this <strong>Guide</strong>, properties<br />
subscripted with s refer to the solid from which the foam is made (e.g.<br />
solid density: s); properties without the subscript s are those of the metfoam<br />
(foam density: ).<br />
Data sources<br />
Data can be found in the literature cited in Section 1.4, and in recent publications<br />
in leading materials journals. The most comprehensive data source is<br />
the CES (1999) database and associated literature; it draws on manufacturers’<br />
data sheets, on published literature, and on data supplied by research groups,<br />
worldwide (Evans, 1997/1998/1999; Banhart, 1999; Degisher, 1999; Simancik,<br />
1999). The CES database has been used to create the material property charts<br />
showninSection4.3 andlater chapters.<br />
Mechanical properties<br />
Figures 4.2 and 4.3 show a schematic stress–strain curve for compression,<br />
together with two sets of real ones. Initial loading apears to be elastic but<br />
the initial loading curve is not straight, and its slope is less than the true<br />
modulus, because some cells yield at very low loads. The real modulus E, is<br />
best measured dynamically or by loading the foam into the plastic range, then<br />
unloading and determining E from the unloading slope. Young’s modulus, E,