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dB<br />

Output Power. dBs Average value 160<br />

in watts.<br />

300<br />

100<br />

30<br />

10<br />

3<br />

1<br />

0.3<br />

0.1<br />

0.03<br />

0.01<br />

0.003<br />

0.001<br />

0.0003<br />

0.0002 µ bar of pressure<br />

150<br />

140<br />

130<br />

120<br />

110<br />

100<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

Jet engine<br />

Community siren<br />

Pneumatic riveter<br />

Threshold of pain<br />

Loud rock band, punch press<br />

Chain saw<br />

Very loud music<br />

Loud music, heavy truck, subway train<br />

Orchestra, highway traffic<br />

Average conversation<br />

Quiet music<br />

Average residence, computer system<br />

Background music<br />

Quiet office, computer hard drive<br />

Whispering<br />

Faint sounds, paper rustling<br />

Threshold of hearing<br />

FIG. 23.5<br />

Typical sound levels and their decibel levels.<br />

Dynamic range ≅ 120 dB s<br />

A common question regarding audio levels is how much the power<br />

level of an acoustical source must be increased to double the sound<br />

level received by the human ear. The question is not as simple as it<br />

first seems due to considerations such as the frequency content of the<br />

sound, the acoustical conditions of the surrounding area, the physical<br />

characteristics of the surrounding medium, and—of course—the<br />

unique characteristics of the human ear. However, a general conclusion<br />

can be formulated that has practical value if we note the power<br />

levels of an acoustical source appearing to the left of Fig. 23.5. Each<br />

power level is associated with a particular decibel level, and a change<br />

of 10 dB in the scale corresponds with an increase or a decrease in<br />

power by a factor of 10. For instance, a change from 90 dB to 100 dB<br />

is associated with a change in wattage from 3 W to 30 W. Through<br />

experimentation it has been found that on an average basis the<br />

loudness level will double for every 10-dB change in audio level—a<br />

conclusion somewhat verified by the examples to the right of Fig.<br />

23.5. Using the fact that a 10-dB change corresponds with a tenfold<br />

increase in power level supports the following conclusion (on an<br />

approximate basis): Through experimentation it has been found that on<br />

an average basis, the loudness level will double for every 10-dB<br />

change in audio level.<br />

To double the sound level received by the human ear, the power<br />

rating of the acoustical source (in watts) must be increased by a<br />

factor of 10.<br />

DECIBELS ⏐⏐⏐ 1025

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