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Metal Foams: A Design Guide

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

It is the fraction of the incident energy of the sound wave which is absorbed by<br />

the material. The upper figure shows the value of ˛ for a good absorber, glass<br />

wool: at frequencies above 1000 Hz the absorption coefficient is essentially<br />

1, meaning that the sound is almost completely absorbed. The central figure<br />

shows absorption in a sample of Alporas foam in the as-received (virgin) state:<br />

Absorption<br />

Absorption<br />

Absorption<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

800<br />

b<br />

a<br />

400<br />

1200<br />

600<br />

800<br />

1600<br />

1000<br />

Frequency<br />

Alporas compressed 10%<br />

2000<br />

Frequency<br />

1200<br />

Glass Wool<br />

1400<br />

2400<br />

1800<br />

Alporas as received<br />

Figure 12.1 Sound absorption, measured in a plane-wave impedance tube,<br />

for glass fiber, Alporas foam in the as-received condition, and Alporas foam<br />

after 10% compression to rupture the cell faces<br />

2800

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