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Chapter 6: Impedance measurements

Chapter 6: Impedance measurements

Chapter 6: Impedance measurements

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Acoustic impedance <strong>measurements</strong><br />

Kundt’s tube reference<br />

As a reference the same sample is also measured with the PU probe<br />

Kundt’s tube method [1], [4], [5], see Fig. 6.57. The Kundt’s tube has a 46<br />

x 46 mm square profile and sound waves will travel only in one dimension<br />

below the cut-off frequency of 3500Hz. The plate with resonator can directly<br />

be mounted at the end of the Kundt’s tube so there is no risk of repositioning<br />

the sample and to change its acoustical properties.<br />

The absorbing properties of a wall resonator is dependent of the ratio<br />

between the tube diameter and the distance between the tubes [8]. The<br />

measurement shows that one tube in a relatively large plate absorbs nearly<br />

all sound at one single frequency (1320 Hz). Nearly the same frequency as<br />

measured close to the tube with the local free field <strong>measurements</strong> (1330<br />

Hz).<br />

1<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

α [ - ]<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

1000 1320<br />

Frequency [ Hz ]<br />

Fig. 6.57: Kundt’s tube absorption of one quarter lambda resonator.<br />

Three quarter lambda samples<br />

The entire surface of the same sample, but now with three quarter<br />

lambda tubes is measured 3mm from the surface with a 5x5mm grid (81<br />

<strong>measurements</strong>), see Fig. 6.58. Each tube will cause the sample to absorb at<br />

its particular resonant frequency.<br />

Because each segment of the sample is observed, the combination of<br />

these <strong>measurements</strong> should represent the behavior of the total sample. The<br />

result can than be compared with the Kundt’s tube.<br />

6-51

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