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What it is. Sum of independent sound levels by adding energies (not dB directly).
Formula. \( L_{\mathrm{add}} = 10\log_{10}\!\big(\sum_i 10^{L_i/10}\big) \)
Tip. The result is slightly above the largest input; two equal sources add ≈ \(+3.0\ \mathrm{dB}\).
What it is. Remove a known component from a total level (e.g., subtract background).
Condition. Defined only if \( L_{\mathrm{comp}} < L_{\mathrm{tot}} \).
Formulas. \( E_{\mathrm{remain}} = 10^{L_{\mathrm{tot}}/10} – 10^{L_{\mathrm{comp}}/10} \),
\( L_{\mathrm{remain}} = 10\log_{10}(E_{\mathrm{remain}}) \)
What it is. Logarithmic mean: average energies, then convert back to dB.
Formulas. \( E_{\mathrm{avg}} = \frac{1}{n}\sum_i 10^{L_i/10} \),
\( L_{\mathrm{avg}} = 10\log_{10}(E_{\mathrm{avg}}) \)
Note. Do not take an arithmetic mean of dB; dB are logarithmic. Energy-averaging preserves the physics.
What it is. Convert between dB(Z), dB(A) and dB(C) at the 1/3-octave center frequency \(f\) using tabulated corrections \(A(f)\) and \(C(f)\).
Conversions.
From Z: \( A = Z + A(f) \), \( C = Z + C(f) \).
From A: \( Z = A – A(f) \), \( C = Z + C(f) \).
From C: \( Z = C – C(f) \), \( A = Z + A(f) \).
Interpretation. A ≈ human sensitivity at moderate levels (attenuates lows); C is flatter at low frequencies; Z is flat (instrument bandwidth).
Notes common to all. \(E\) denotes an energy-equivalent linear quantity (e.g., power or mean-square pressure). Numeric outputs use a fixed one-decimal format.
| Center frequency (Hz) | A-weighting A(f) [dB] | C-weighting C(f) [dB] | Z-weighting Z(f) [dB] | A − C [dB] |
|---|---|---|---|---|
| 6.3 | -85.4 | -21.3 | 0.0 | -64.1 |
| 8 | -77.8 | -17.7 | 0.0 | -60.1 |
| 10 | -70.4 | -14.3 | 0.0 | -56.1 |
| 12.5 | -63.4 | -11.2 | 0.0 | -52.2 |
| 16 | -56.7 | -8.5 | 0.0 | -48.2 |
| 20 | -50.5 | -6.2 | 0.0 | -44.3 |
| 25 | -44.7 | -4.4 | 0.0 | -40.3 |
| 31.5 | -39.4 | -3.0 | 0.0 | -36.4 |
| 40 | -34.6 | -2.0 | 0.0 | -32.6 |
| 50 | -30.2 | -1.3 | 0.0 | -28.9 |
| 63 | -26.2 | -0.8 | 0.0 | -25.4 |
| 80 | -22.5 | -0.5 | 0.0 | -22.0 |
| 100 | -19.1 | -0.3 | 0.0 | -18.8 |
| 125 | -16.1 | -0.2 | 0.0 | -15.9 |
| 160 | -13.4 | -0.1 | 0.0 | -13.3 |
| 200 | -10.9 | 0.0 | 0.0 | -10.9 |
| 250 | -8.6 | 0.0 | 0.0 | -8.6 |
| 315 | -6.6 | 0.0 | 0.0 | -6.6 |
| 400 | -4.8 | 0.0 | 0.0 | -4.8 |
| 500 | -3.2 | 0.0 | 0.0 | -3.2 |
| 630 | -1.9 | 0.0 | 0.0 | -1.9 |
| 800 | -0.8 | 0.0 | 0.0 | -0.8 |
| 1000 | 0.0 | 0.0 | 0.0 | 0.0 |
| 1250 | 0.6 | 0.0 | 0.0 | 0.6 |
| 1600 | 1.0 | -0.1 | 0.0 | 1.1 |
| 2000 | 1.2 | -0.2 | 0.0 | 1.4 |
| 2500 | 1.3 | -0.3 | 0.0 | 1.6 |
| 3150 | 1.2 | -0.5 | 0.0 | 1.7 |
| 4000 | 1.0 | -0.8 | 0.0 | 1.8 |
| 5000 | 0.5 | -1.3 | 0.0 | 1.8 |
| 6300 | -0.1 | -2.0 | 0.0 | 1.9 |
| 8000 | -1.1 | -3.0 | 0.0 | 1.9 |
| 10000 | -2.5 | -4.4 | 0.0 | 1.9 |
| 12500 | -4.3 | -6.2 | 0.0 | 1.9 |
| 16000 | -6.6 | -8.5 | 0.0 | 1.9 |
| 20000 | -9.3 | -11.2 | 0.0 | 1.9 |