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CLIOwin 7 PCI User's Manual - Audiomatica

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Now things look much better and this is almost the anechoic response of the speaker.<br />

However nothing comes for free. The low frequency part of the response seems quite<br />

optimistic for such a little speaker. The price we paid in setting the impulse tail to 0 is<br />

that we lost information on the lower part of the spectrum. The transition frequency<br />

between meaningful and meaningless data is calculated as 1 divided by the selected<br />

impulse length. In our case we selected a 6.8ms long impulse. 1/0.0068=147Hz right?<br />

Wrong. We have to remember the first 2 ms of the impulse, which is the time the sound<br />

takes to reach the microphone and hence does not carry any information. We could<br />

have selected the impulse as in Fig.10.18 without affecting the frequency response at<br />

all however phase response would have been greatly affected.<br />

0.50<br />

V<br />

CLIO<br />

0.40<br />

0.30<br />

0.20<br />

0.100<br />

0.00<br />

-0.10<br />

-0.20<br />

-0.30<br />

-0.40<br />

-0.50<br />

0.00 1.1 2.3 3.4 4.6 5.7 6.8 8.0 9.1 10 11<br />

ms<br />

Figure 10.18<br />

The right calculation is 1/(0.0068-0.002)=208.33Hz. In our room the smallest<br />

dimension is floor to ceiling. This is indeed the most frequent case. This dimension is<br />

however 4m. The best location for the speaker would have been at 2m both from the<br />

floor and the ceiling. The second consideration is microphone distance. The further away<br />

it is, the more you have to subtract from the impulse length due to sound travel time<br />

to the microphone. In practice we do not encourage distance below 70cm for complete<br />

speaker measurement and you should increase to 1m for bigger ones. However single<br />

driver measurement can take advantage from a reduced distance.<br />

Chapter 10 - MLS 119

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