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Developments in Ceramic Materials Research

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The Use of <strong>Ceramic</strong> Pots <strong>in</strong> Old Worship Places 155<br />

a.10. Cavernous churches- The sound vases are situated on every part of the church,<br />

without determ<strong>in</strong>ism or acoustic purpose.<br />

a.11. Hexagonal churches- The vases are walled-<strong>in</strong> <strong>in</strong> every dome structure and are of<br />

any shape, ma<strong>in</strong>ly on the crests of domes and of bucklers <strong>in</strong> general. The number of walled-<strong>in</strong><br />

vases does not depend on the size of the churches, or their position.<br />

The difference between Greece and other countries – not neighbour<strong>in</strong>g - that the vases are<br />

walled-<strong>in</strong> at different positions, <strong>in</strong> the walls and domes. Perhaps this arises from the fact that<br />

there are different architectural types of the churches.<br />

4. QUALITY OF SOUND IN ROOMS<br />

The propriety of the sound field that is related to certa<strong>in</strong> hear<strong>in</strong>g impressions is an object<br />

of psychoacoustics. The physical parameters that describe the so-called “sound quality” <strong>in</strong> a<br />

room can be described by a set of objective parameters called <strong>in</strong>dexes. These <strong>in</strong>dexes<br />

accord<strong>in</strong>g to the procedure from which they can be derived, are divided <strong>in</strong>to categories. All of<br />

them can be evaluated from the impulse response of the room.<br />

In the acoustical assessment of concert halls, and other public spaces, reverberation time<br />

has long been known to be the most important parameter to judge the acoustic quality of a<br />

room. The reverberation time T60 is derived from the decay curve and is def<strong>in</strong>ed as the time<br />

for the sound to die away to a level 60 dB below its orig<strong>in</strong>al level. This quantity can be<br />

measured us<strong>in</strong>g the Schroeder <strong>in</strong>tegrated impulse response technique [40].<br />

Instead of reverberation time T10, T20 and T30 are measured. The three reverberation<br />

times are used when the impulse is of low level and T60 cannot be measured. These<br />

parameters show the reverberation time <strong>in</strong> a part of the response curve, which is usually more<br />

useful. T10 is derived from the decay curve section between –5 dB and –15 dB below the<br />

<strong>in</strong>itial level. From the correspond<strong>in</strong>g slope, T10 is calculated as the time to reach –60dB. T10<br />

can be used to measure for <strong>in</strong>stance vibrations or loss factors <strong>in</strong> build<strong>in</strong>g structures. Most<br />

practical T10 values range from 0.005 to 10 s.<br />

Proportionally, T20 is derived from the decay curve section between –5 dB and –25 dB<br />

below the <strong>in</strong>itial level. For T30 the same holds, but with –35 <strong>in</strong>stead of –25 dB. From the<br />

correspond<strong>in</strong>g slope, T20 and T30 are calculated as the time to reach –60 dB. Most practical<br />

T20 and T30 values range from 0.1 to 10 s. Most of the time, these three parameters don’t have<br />

the same value for the same room and that is because of the field which is not diffuse.<br />

Besides, for the same time, for different po<strong>in</strong>ts <strong>in</strong> a room, accord<strong>in</strong>g to the spot of the<br />

microphone, the three parameters have different values due to the different types of the fields<br />

<strong>in</strong> the room. Thus, <strong>in</strong> order to measure an unreliable reverberation time, we measure it at<br />

many po<strong>in</strong>ts and we calculate the mean value.<br />

Another useful <strong>in</strong>dex is the EDT. The EDT is a magnitude that takes <strong>in</strong>to account the<br />

early reflections, which are the most important, and affect a lot the acoustics of a room. We<br />

use it when the slope of the reduction rate is not smooth enough. The EDT is derived from the<br />

decay curve section between 0 dB and –10 dB below the <strong>in</strong>itial level. From the correspond<strong>in</strong>g<br />

slope, the EDT is calculated as the time to reach –60dB. It is closely related to the <strong>in</strong>itial and

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