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Introduction to Acoustics

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316 Part C Architectural <strong>Acoustics</strong><br />

Part C 9.5<br />

• Real-time (1/3 and 1/1 octave) analyzers or sound<br />

level meters with sufficient memory for s<strong>to</strong>rage of<br />

a series of short time-averaged root-mean-square<br />

(RMS)values<br />

• Fast Fourier transform (FFT) analysers capable of<br />

recording adequately long records<br />

• Tape recorders, preferably a digital audio tape (DAT)<br />

recorder, or even MP3 recorders given that the data<br />

reduction does not deteriorate the signal.<br />

Of these, real-time analyzers and sound level meters<br />

will process the signal through an RMS detec<strong>to</strong>r before<br />

9.5 Prediction of Room Acoustic Parameters<br />

Beyond theoretical calculation of the reverberation time,<br />

the prediction techniques presented in this section range<br />

from computer simulations and scale model measurements<br />

<strong>to</strong> simple linear models based on empirical data<br />

collected from existing halls.<br />

In all cases, the main objective is the prediction of the<br />

acoustic conditions described in terms of the acoustic parameters<br />

presented in Sect. 9.3. Just as we can record the<br />

sound in a hall, both scale models and numerical computer<br />

simulations can also provide auralizations,which<br />

are synthesized audible signals that allow the client and<br />

architect <strong>to</strong> listen <strong>to</strong> and participate in the acoustic evaluation<br />

of proposed design alternatives. Such audible<br />

simulations will often have much greater impact and be<br />

more convincing than the acoustician’s verbal interpretation<br />

of the numerical results. Therefore, the acoustician<br />

must be very careful <strong>to</strong> judge the fidelity and the degree<br />

of realism before presenting auralizations.<br />

9.5.1 Prediction of Reverberation Time<br />

by Means<br />

of Classical Reverberation Theory<br />

Reverberation time as defined in Sect. 9.3.1 is still the<br />

most important objective parameter for the characterization<br />

of the acoustics of a room. Consequently, the<br />

prediction of T is a basic <strong>to</strong>ol in room acoustic design.<br />

Calculation of reverberation time according <strong>to</strong> the<br />

Sabine equation was the first attempt in this direction and<br />

<strong>to</strong>day is still the most commonly used. However, during<br />

the 100 years since its invention, several other reverberation<br />

time formulae have been suggested (by Eyring,<br />

Fitzroy, Miller<strong>to</strong>n and Sette, Metha and Mulholland Kut-<br />

s<strong>to</strong>rage, which means that not the full signal, but only<br />

energy with a limited time resolution will be recorded.<br />

Today, calculation of the objective parameters will<br />

always be carried out by a PC or by a computer built in<strong>to</strong><br />

a dedicated instrument. A large number of PC-based systems<br />

and software packages particularly suited for room<br />

acoustic measurements are available. Some systems<br />

come with a specific analog-<strong>to</strong>-digital (A/D), digital-<strong>to</strong>analog<br />

(D/A) and signal-processing card, which must be<br />

installed in or connected <strong>to</strong> the PC, while others can use<br />

the sound card already available in most PCs aswellas<br />

external sound cards for hobby music use.<br />

truff and others), all with the purpose of correcting some<br />

obvious shortcomings of the Sabine method.<br />

The Sabine equation has been described in<br />

Sect. 11.1.4. In larger rooms, the absorption in the air<br />

plays a major role at high frequencies. If we include this<br />

fac<strong>to</strong>r, the Sabine equation reads:<br />

T = 0.161V<br />

Sα∗ , (9.21)<br />

+ 4mV<br />

where V is the room volume, S is the <strong>to</strong>tal area of the<br />

room surfaces, α∗ is the area-weighted average absorption<br />

coefficient of the room surfaces<br />

α ∗ = α = 1 �<br />

Siαi<br />

(9.22)<br />

S<br />

i<br />

and m accounts for the air absorption, which is a function<br />

of the relative humidity and increases rapidly with fre-<br />

Fig. 9.11 Two types of omnidirectional sound sources for<br />

room acoustic measurements: blank pis<strong>to</strong>l (in the raised<br />

hand of the seated person) and an omnidirectional loudspeaker<br />

(icosahedron with 20 units)

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