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Introduction to Acoustics

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F b<br />

d<br />

F n<br />

I<br />

S<br />

Fb Fn S<br />

d<br />

F n/F b<br />

d/d I<br />

<strong>Acoustics</strong> in Halls for Speech and Music 9.6 Geometric Design Considerations 325<br />

F b<br />

II III<br />

I II III IV<br />

0.63<br />

1<br />

0.55<br />

0.83<br />

Fig. 9.19 Mean stage–listener distance and net efficiency of floor area for four different room shapes. Fn is the net<br />

area occupied by the audience, Fb is the <strong>to</strong>tal floor area, d is the average source–listener distance; dI = d for case I<br />

(after [9.28])<br />

0.64<br />

0.78<br />

d<br />

0.67<br />

0.79<br />

1<br />

F n<br />

S<br />

s 3Modell<br />

Fig. 9.20 Calculated distributions of early lateral reflection levels in rooms of different plan shape: fan, hexagon,<br />

rectangular and reverse fan. Darker areas represent higher LEF levels (after [9.5])<br />

When building an audi<strong>to</strong>rium, efficient use of the<br />

available floor space and the average proximity of the<br />

audience <strong>to</strong> the performers are very important parameters.<br />

Depending on the plan shape of the room different<br />

values appear as shown in Fig. 9.19.<br />

Low average distance is the main reason for the frequent<br />

use of the fan shape (III and IV in Fig. 9.19),<br />

although the directivity of sound sources (like the human<br />

voice) as well as the quality of lines of sight sets<br />

limits on the opening angle of the fan.<br />

Another limitation of the fan shape is that it does<br />

not generate the strong lateral reflections so important<br />

in halls for classical music. This was already seen in<br />

the empirical equations in Sect. 9.5.6 and confirmed in<br />

Fig. 9.20, showing the calculated distributions of early<br />

lateral reflection levels in rooms of different plan shapes.<br />

The reason is that sound waves from the source hitting<br />

the side walls will produce reflections that will run<br />

almost parallel <strong>to</strong> the direct sound and so hit the listener<br />

from an almost frontal direction, therefore not contribut-<br />

F b<br />

d<br />

IV<br />

F n<br />

S<br />

Part C 9.6

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