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[Part 1 introduces the decibel and examines concepts underlying its use in sound systems. Part 2 looks at expressing power as an audio level, the decibel in acoustics, the inverse square law, directivity factor and Ohm's law.]
2.15 Combining Decibels
Adding Decibel Levels
The sum of two or more levels expressed in dB maybe found as follows:
LT = 10log(10L1/10 + 10L2/10 + ... + 10LN/10. (2-32)
If, for example, we have a noisy piece of machinery with an LP = 90 dB, and wish to turn on a second machine with an LP = 90 dB, we need to know the combined LP. Since both measured levels are the result of the power being applied to the machine, with some percentage being converted into acoustic power, we can determine LT by using Eq. 2-32. Therefore:
LT = 10log(1090/10 + 1090/10)
= 10log(109 + 109)
= 10log(2 x 109)
= 93 dB.
Doubling the acoustic power results in a 3 dB increase.
An alternative dB addition technique is given through the courtesy of Gary Berner.
LT = 10log(10-(diff in dB)/10 + 1) + smallest number (2-33)
Example
If we wish to add 90 dB to 96 dB, using Eq. 2-33, take the difference in dB (6 dB) and put it in the equation:
LT = 10log(106/10 +1) + 90
= 96.97 dB.
Input signals to a mixing network also combine in this same manner, but the insertion loss of the network must be subtracted. Two exactly phase-coherent sinewave signals of equal amplitude will combine to give a level 6 dB higher than either sine-wave.
The general case equation for adding either sound pressure, voltages, or currents is:
Combined LP =
20log√((10E1/20)2 + (10E2/20)2 + 2(10E1/20)(10E2/20)(cos[a1 - a2])) (2-34)
Table 2-9 shows the effects of adding two equal amplitude signals with different phase together using Eq. 2-34.
Table 2-9. Combining Pure Tones of the Same Frequency but Differing Phase Angles
Subtracting Decibels
The difference of two levels expressed in dB may be found as follows:
Ldiff = 10log(10Total Level/10 - Level with one source off/10). (2-35)
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