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Danish Acoustical Society Round Robin on room acoustic computer ...

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The absorpti<strong>on</strong> coefficients used for walls by different participants ranged from 0,02 – 0,28 at low<br />

frequency and 0,02 – 0,10 at high frequency – a factor 5 – 14 depending <strong>on</strong> frequency, see Fig. 16.<br />

Figure 16. Some different absorpti<strong>on</strong> coefficients used for main parts of wall by different participants<br />

If absorpti<strong>on</strong> coefficients of the ceiling are very high, then there may not exist any vertical<br />

reflecti<strong>on</strong>s in the late part of the decay, i.e. the late reflecti<strong>on</strong>s are mainly defined by the reflecti<strong>on</strong>s<br />

from the walls. Therefore when ceiling absorpti<strong>on</strong> is close to 100%, changing the absorpti<strong>on</strong> of the<br />

walls can have a very significant effect <strong>on</strong> T30 and to some extent also <strong>on</strong> EDT, whereas early<br />

energy parameters such as C80 and D50 are not that sensitive.<br />

Ode<strong>on</strong> will show large difference in predicted T30 if the coefficients in the horiz<strong>on</strong>tal plane are<br />

altered whereas the Sabine formula by nature will hide the effect of a n<strong>on</strong>-diffuse sound field. The<br />

Sabine formula will have a tendency to under estimate reverberati<strong>on</strong> time in n<strong>on</strong>-diffuse sound<br />

fields where <strong>on</strong>e- or two dimensi<strong>on</strong>al modes are dominant. (In other cases the Sabine formula is<br />

known to overestimate the reverberati<strong>on</strong> time, though). Ode<strong>on</strong> does take into account that<br />

reverberati<strong>on</strong> in <strong>room</strong>s such as this class <strong>room</strong> will be dominated by wall reflecti<strong>on</strong>s – this does in<br />

principle allow better predicti<strong>on</strong>s than Sabine offers, however relative small changes to the total<br />

absorpti<strong>on</strong> area may have pr<strong>on</strong>ounced effects <strong>on</strong> reverberati<strong>on</strong> time – in simulati<strong>on</strong>s as well as in<br />

the real world. Indeed changes of a factor 5 or more for the wall material absorpti<strong>on</strong> as in this round<br />

robin has a pr<strong>on</strong>ounced effect.<br />

Although reverberati<strong>on</strong> time is often used for characterizati<strong>on</strong> of class <strong>room</strong>s (parallel walls and<br />

absorbing ceiling), the questi<strong>on</strong> is if it is good at describing the <strong>acoustic</strong> quality of such <strong>room</strong>s;<br />

there can be large differences in T30 and EDT with some variati<strong>on</strong>s in the absorpti<strong>on</strong> data, while STI<br />

virtually stay unchanged.<br />

12/20

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