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Introduction to Acoustics

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1040 Part H Engineering <strong>Acoustics</strong><br />

Part H 24.6<br />

becomes<br />

LC21 = (L2 + Lm1 + Ld + LWA)<br />

− (L1 + Lm2 + Ld + LWB) . (24.48)<br />

Subtracting (24.48) from (24.47), the difference in<br />

level between the two microphones is<br />

(L1 − L2) = 1/2(LC12 − LC21) . (24.49)<br />

If either L1or L2 is the sensitivity level of a calibrated<br />

reference microphone, then the sensitivity level<br />

of the other microphone (the test microphone) can be deduced.<br />

It is interesting <strong>to</strong> point out that with this method,<br />

the level Ld of the driving sound need not have a flat<br />

response or known levels.<br />

The above relatively simple theoretical consideration<br />

has assumed that the input capacitances of the two<br />

microphones are identical, i. e. the same model of microphones,<br />

and the same model of preamplifiers used for<br />

both channels such that their input capacitances have the<br />

same value.<br />

If the input capacitances Cm of the preamplifiers<br />

are the same but the two models of microphones are<br />

different, then a correction Lcorr should be added <strong>to</strong> the<br />

right-hand side of (24.49), where<br />

Lcorr = 20 log[C2/(Cm + C2)]<br />

− 20 log[C1/(Cm + C1)] . (24.50)<br />

The two terms in (24.50) are the capacitance corrections<br />

for the two microphones; and C1 and C2 are<br />

the capacitances of microphone 1 and microphone 2,<br />

respectively.<br />

It is important <strong>to</strong> realize that the physical positions<br />

of the reference microphone should be repeated accurately<br />

before and after the microphones are interchanged<br />

such that the sound field at the reference microphone<br />

is unchanged. The difference in level readings shown<br />

in (24.47) and(24.48) can be measured with the ratio<br />

provision of a precision AC voltmeter.<br />

Uncertainties<br />

The uncertainty for the above method depends on the reference<br />

microphone uncertainty that may be of the order<br />

of 0.05 dB. With very sophisticated measuring methods<br />

such as phase-lock amplifiers the uncertainty introduced<br />

by this comparison method <strong>to</strong> be added <strong>to</strong> the uncertainty<br />

of the reference microphone [24.57] is estimated <strong>to</strong> be<br />

less than 0.1dB.<br />

24.6.2 Comparison Method<br />

with a Calibra<strong>to</strong>r<br />

In general, there are five components and three basic<br />

steps in this comparison method [24.57]. The components<br />

are the reference microphone, the test microphone,<br />

a stable sound source, which is usually an acoustical calibra<strong>to</strong>r<br />

that generates a constant sound pressure level,<br />

a microphone preamplifier and an acoustical level indica<strong>to</strong>r<br />

such as a measuring amplifier or a voltmeter.<br />

Since the calibra<strong>to</strong>r is used as a transfer standard, its<br />

sound pressure level need not be known.<br />

The three basic steps are as follows<br />

1. The reference microphone which is connected <strong>to</strong> the<br />

preamplifier is inserted in<strong>to</strong> the acoustical calibra<strong>to</strong>r<br />

and a level reading Lr is noted.<br />

2. The reference microphone is replaced with the test<br />

microphone. With the same acoustical calibra<strong>to</strong>r,<br />

a second level reading Lt is noted.<br />

3. The test microphone is removed, and again with<br />

the reference microphone, step 1 is repeated <strong>to</strong> give<br />

a third level reading.<br />

The agreement between the first and third level readings<br />

with the reference microphone is a confirmation<br />

of the validity of the second level reading obtained<br />

with the test microphone, that is, <strong>to</strong> assure that nothing<br />

has changed after the first level reading is taken.<br />

The difference between the level readings, (Lt − Lr) is<br />

the difference in open-circuit sensitivities (expressed in<br />

decibels) between the two microphones if the following<br />

conditions are satisfied:<br />

1. The equivalent volumes of the two microphones are<br />

identical, or the equivalent volume of the sound calibra<strong>to</strong>r<br />

is much larger than that of the microphones,<br />

such that any difference in the front volumes of the<br />

microphones does not produce a significant change<br />

in the sound pressure levels measured in steps 1 and<br />

2 above.<br />

2. The capacitances of the two microphones are identical.<br />

Since the preamplifier has a finite input<br />

impedance (a very high resistance in parallel with<br />

a small known capacitance), the loading on the<br />

microphone will be different if the microphone capacitances<br />

were <strong>to</strong> be different, and this will produce<br />

a small change in the overall combined sensitivity of<br />

the microphone and preamplifier.<br />

3. The environmental conditions remain constant during<br />

the measurements.

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