12.02.2013 Views

Metal Foams: A Design Guide

Metal Foams: A Design Guide

Metal Foams: A Design Guide

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

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

Using the relation vD D cplεD and the momentum balance D D pl C cplvD,<br />

the downstream compressive stress, D, exerted on the impacting mass is<br />

D D<br />

MV<br />

pl C<br />

εD<br />

2 0 2 plAℓεD/⊲1 εD⊳<br />

M C Aℓ/⊲1 εD⊳<br />

⊲11.25⊳<br />

Thus, the compressive stress decelerating the mass M decreases with the length<br />

of foam compacted, ℓ/⊲1<br />

on the mass is<br />

εD⊳. In the limit ℓ D 0 the peak compressive stress<br />

⊲ D⊳peak D pl C V2 0<br />

εD<br />

⊲11.26⊳<br />

in agreement with the findings of the shock wave analysis above. The length of<br />

foam ℓ/⊲1 εD⊳ required to arrest the mass is determined by putting vD D 0<br />

in the above equation, giving<br />

1<br />

ℓ<br />

εD<br />

D MV20 2 plεDA<br />

⊲11.27⊳<br />

On noting that plεD equals the energy, W, absorbed by the foam per<br />

unit volume, we see that the minimum length of foam required for energy<br />

absorption is obtained by selecting a foam with a maximum value of W,<br />

consistent with a value of upstream stress pl which does not overload the<br />

structure to which the foam is attached. The plots of W versus pl for metallic<br />

foams (Figures 11.3, 11.4 and 11.5) are useful for this selection process.<br />

11.6 Blast and projectile protection<br />

Explosives create a pressure wave of approximately triangular profile, known<br />

as a ‘blast’ (Smith and Hetherington, 1994). Protection against blast involves<br />

new features. The blast imparts an impulse, Ji, per unit area of a structure,<br />

equal to the integral of the pressure over time:<br />

�<br />

Ji D pdt ⊲11.28⊳<br />

The blast wave is reflected by a rigid structure, and the details of the<br />

pressure–time transient depend on the orientation of the structure with respect<br />

to the pressure wave. In design, it is conservative to assume that the structure<br />

is at normal incidence and fully reflects the blast. Figure 11.15 shows the<br />

peak pressure, p0, and the resulting impulse, Ji, caused by the detonation of<br />

a charge of TNT, at a radial distance, R, from the charge. Curves are shown<br />

for a reflected blast in air, and in water. The impulse and the distance are<br />

normalized by the cube root of the mass, M, of the charge in kg. As an

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!