Engineering Acoustics. Malcolm J. Crocker

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3.18 Sound pressure level in an interior sound field.

      3.14.2 Sound Absorption

      The sound absorption coefficient α of sound‐absorbing materials (curtains, drapes, carpets, clothes, fiberglass, acoustical foams, etc.), is defined as

equation equation

      (3.73)equation

Graph depicts the sound absorption coefficient alpha of typical absorbing materials as a function of frequency.

      If all the sound energy is absorbed, α = 1 (none reflected). If no sound energy is absorbed, α = 0:

equation

      If α = 1, the sound absorption is perfect (e.g. an open window).

      The behavior of sound‐absorbing materials is described in more detail in Chapter 9 of this book.

      3.14.3 Reverberation Time

equation

      where V is room volume (m3), c is the speed of sound (m/s), S is wall area (m2), and images is the angle‐averaged wall absorption coefficient, or

      (3.74)equation

      where Si is ith wall area of absorption coefficient αi.

Graph depicts the measurement of reverberation time TR. Graph depicts a few examples of recommended reverberation times.

      Example 3.13

      A room has dimensions 5 × 6 × 10 m3. What is the reverberation time T60 if the floor (6 × 10 m) has absorbing material images = 0.5 placed on it?

      Solution

      We will assume that images = 0 on the other surfaces (that are made of hard painted concrete.)

equation

      Example 3.14

      A classroom has dimensions 4 × 6 × 10 m3 and a reverberation time of 1.5 seconds. (a) Determine the total sound absorption of the classroom; (b) if 35 students are in the classroom, and each is equivalent to 0.45 sabins (m2) sound absorption, what is the new reverberation time of the classroom?

      Solution

      1 the volume of the classroom is V = 240 m3. Therefore

      2 The total sound absorption is now 25.8 + 35(0.45) = 41.55 sabins (m2). Then

Schematic illustration of sound source in anechoic room.

      If we have a diffuse sound field (the same sound energy at any point in the room) and the field is also reverberant (the sound waves may come from any direction, with equal probability), then the sound intensity striking the wall of the room is found by integrating the plane wave intensity over all angles θ, 0 < θ < 90°. This involves a weighting of each wave by cos θ, and the average intensity for the wall in a reverberant field becomes

      (3.75)equation

      Note

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