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Developments in Ceramic Materials Research

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168<br />

Dimitris Skarlatos, Tilemachos Zak<strong>in</strong>th<strong>in</strong>os and Ioanis Koumanoudis<br />

Measurements of absorption by Carvalho et al showed that the absorption <strong>in</strong>creases at<br />

low frequencies when the pots are located at the corners of the room. Acord<strong>in</strong>g to Carvalho<br />

this conclusion confirms the relevance of the tradition that often <strong>in</strong>volves the lay<strong>in</strong>g out of the<br />

acoustic pots <strong>in</strong> the churches especially near the angles.<br />

Figure 23 shows the change of Clarity and Def<strong>in</strong>ition <strong>in</strong> 1/1 octave band analysis due to<br />

resonators. It is clear that there is a decrease of both <strong>in</strong>dexes <strong>in</strong> the low frequency region with<br />

the presence of resonators. The effect of resonators <strong>in</strong> the mid and high frequency region is<br />

mixed.<br />

x100%<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

Def<strong>in</strong>ition (D50)<br />

0_bottles<br />

480_bottles<br />

0.4<br />

63 125 250 500 1000 2000 4000<br />

dB<br />

8<br />

7<br />

6<br />

5<br />

4<br />

3<br />

2<br />

Clarity (C80)<br />

0_ bott<br />

480 _bott<br />

1<br />

63 125 250 500 1000 2000 4000<br />

(a) 1/1 octave band center frequency (Hz) (b) 1/1 octave band center frequency (Hz)<br />

Figure 23. Effects of resonators on Def<strong>in</strong>ition and Clarity.<br />

X100%dB<br />

0.3<br />

0.25<br />

0.2<br />

0.15<br />

0.1<br />

Lateral fraction (LF)<br />

0_bottles<br />

480_bottles<br />

0.05<br />

63 125 250 500 1000 2000 4000<br />

(a)<br />

1/1 octave band center frequency (Hz)<br />

Figure 24. Of resonators on LF and IACC.<br />

1<br />

0.9<br />

0.8<br />

Interaural cross correlation (IACC)<br />

0_ bott<br />

480 _bott<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

63 125 250 500 1000 2000 4000<br />

(b)<br />

1/1 octave band center frequency (Hz)<br />

For the third octave band that conta<strong>in</strong>s the resonant frequency, us<strong>in</strong>g a vary<strong>in</strong>g number of<br />

resonators D50 can be expressed by the follow<strong>in</strong>g regression equation (R-squared=0.96) is:<br />

D50 = 0.533+ 0.139bv<br />

(18)<br />

where bv is the number of resonators per unit volume.<br />

Similarly C80 can be written (R-squared=0.9).

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