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Sound Propagation Indoor

Reference data and engineering information about sound propagation indoor for acoustics applications.

soundpropagationindoor

Overview

Engineering reference data for Sound Propagation Indoor in acoustics.

Key Formulas

Speed of Sound

c=γRTc = \sqrt{\gamma R T}

Speed of sound in an ideal gas.

Sound Level

L=10log10(I/I0)L = 10 \log_{10}(I/I_0)

Decibel level.

Wavelength

λ=c/f\lambda = c / f

Wavelength = speed / frequency.

Variables

SymbolDescriptionUnit
ccSpeed of soundm/s
LLSound leveldB
λ\lambdaWavelengthm
ffFrequencyHz

Worked Example

The following calculation demonstrates how to apply the fundamental sound propagation equations for a source in a reverberant room.

Given:

  • Source Sound Power Level (LNL_N): 90 dB
  • Total Room Absorption (AA): 12.2 m² Sabine
  • Mean Absorption Coefficient (αm\alpha_m): 0.2
  • Directivity Coefficient (DD): 1 (receiver in the middle of the room)
  • Distance from Source (rr): 2 m

Step 1: Calculate the Room Constant (RR) The room constant defines the acoustic character of the space. R=A1αmR = \frac{A}{1 - \alpha_m} R=12.2 m210.2=15.25 m2 SabineR = \frac{12.2 \ \text{m}^2}{1 - 0.2} = 15.25 \ \text{m}^2 \ \text{Sabine}

Step 2: Calculate the Received Sound Pressure Level (LpL_p) The received level is the sum of direct and reverberant sound energy. Lp=LN+10log10(D4πr2+4R)L_p = L_N + 10 \log_{10} \left( \frac{D}{4\pi r^2} + \frac{4}{R} \right) Lp=90+10log10(14π(2)2+415.25)L_p = 90 + 10 \log_{10} \left( \frac{1}{4\pi (2)^2} + \frac{4}{15.25} \right) Lp=90+10log10(0.01989+0.2623)L_p = 90 + 10 \log_{10} \left( 0.01989 + 0.2623 \right) Lp=90+10log10(0.2822)L_p = 90 + 10 \log_{10} (0.2822) Lp=905.584.5 dBL_p = 90 - 5.5 \approx 84.5 \ \text{dB}

Note: The result (84.5 dB) is consistent with the value (84.8 dB) from the source material, with minor differences due to rounding in intermediate steps.

References