Page 160 - The Master Handbook Of Acoustics
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135
                                                                                      REVERBERATION


                      7-3B is the same thing except that the ver-
                      tical scale is plotted in decibels, i.e., to a       Sound source
                      logarithmic scale.                                On             Off
                         During the growth of sound in the room,
                      power is being fed to the sound source.
                      During decay, the power to the source is
                      cut off, hence the difference in the shapes of                                A
                      the growth and decay curves. The decay         Sound pressure
                      of Fig. 7-3B is a straight line in this ideal-
                      ized form, and this becomes the basis for
                      measuring the reverberation time of an                       Time
                      enclosure.


                      Reverberation Time

                      Reverberation time is defined as that time
                      required for the sound in a room to decay     Sound pressure  level, dB       B
                      60 dB. This represents a change in sound
                      intensity or sound power of 1 million                        Time
                      (10 log 1,000,000 = 60 dB), or a change of
                                                                                             FIGURE 7-3
                      sound pressure or sound-pressure level
                      of 1,000 (20 log 1,000 = 60 dB). In very   The growth and decay of sound in a room. (A)
                                                                 Vertical scale in linear sound pressure units. (B) The
                      rough human terms, it is the time required  vertical scale in logarithmic units (decibels).
                      for a sound that is very loud to decay to
                      inaudibility. W. C. Sabine, the Harvard pioneer in acoustics who intro-
                      duced this concept, used a portable wind chest and organ pipes as a
                      sound source, a stopwatch, and a pair of keen ears to measure the time
                      from the interruption of the source to inaudibility. Today we have
                      better technical measuring facilities, but we can only refine our under-
                      standing of the basic concept Sabine gave us.
                         This approach to measuring reverberation time is illustrated in
                      Fig. 7-4A. Using a recording device that gives us a hardcopy trace of
                      the decay, it is a simple step to measuring the time required for the
                      60-dB decay. At least it is simple in theory. Many problems are
                      encountered in practice. For example, obtaining a nice, straight decay
                      spanning 60 dB or more as in Fig. 7-4A is a very difficult practical
                      problem. Background noise, an inescapable fact of life, suggests that a
                      higher source level is needed. This may occur if the background noise
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