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Chapter 8 - Energy absorption in cellular materials

Published online by Cambridge University Press:  05 August 2014

Lorna J. Gibson
Affiliation:
Massachusetts Institute of Technology
Michael F. Ashby
Affiliation:
University of Cambridge
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Summary

Introduction and synopsis

Packaging surrounds most things we buy or do. Food is packaged, parcels through the post are packaged, and within a car or aeroplane, we ourselves are carefully packaged. It is hard to say how much is spent on it, or the worth of the goods damaged due to inadequate packaging, but the sums involved are certainly considerable, and the potential return on any improvement is large.

The essence of protective packaging is the ability to convert kinetic energy into energy of some other sort – usually, heat – via plasticity, viscosity, visco-elasticity or friction; and this must be done whilst keeping the peak force (and thus the deceleration or acceleration) on the packaged object below the threshold which will cause damage or injury. And there is more to it than that. The direction of impact may not be predictable; then the package must offer omni-directional protection, that is, it must absorb impact from any side. Since the package must be carried with the object it protects, light weight is important. And – since much packaging is discarded – it must (almost always) be cheap.

Foams are especially good at this. The energy-absorbing capacity of a foam is compared with that of the solid of which it is made in Fig. 8.1. For the same energy-absorption, the foam always generates a lower peak force. Energy is absorbed as the cell walls bend plastically, or buckle, or fracture (depending on the material of which the foam is made), but the stress is limited by the long, flat plateau of the stress-strain curve (Figs. 4.2 and 5.1).

Type
Chapter
Information
Cellular Solids
Structure and Properties
, pp. 309 - 344
Publisher: Cambridge University Press
Print publication year: 1997

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References

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