Page 101 - The Master Handbook Of Acoustics
P. 101

76   CHAPTER THREE



                                   less than this, the reflection is inaudible; for levels greater than this,
                                   the reflection is clearly audible.
                                      As the reflection level is gradually increased above the threshold
                                   value, a sense of spaciousness is imparted to the combined sound. This
                                   sense of spaciousness prevails, even though the experiment is conducted
                                   in an anechoic space. As the level of the reflection is increased about
                                   10 dB above the threshold value, another change is noticed in the sound;
                                   a broadening of the sound image and possibly a shifting of the image
                                   toward the direct loudspeaker is now added to the increasing spacious-
                                   ness. As the reflection level is increased another 10 dB or so above the
                                   image broadening threshold, another change is noted; discrete echoes are
                                   heard.
                                      This is all very interesting, but what practical value does it have?
                                   Consider a specific example: a listening room in which recorded music
                                   will be played. Figure 3-20 contains answers to the effect of sound
                                   reflected from floor, ceiling, and walls being added to the direct sound
                                   from the loudspeakers. Reflections below the threshold of perception are
                                   unusable; reflections perceived as discrete echoes are also unusable. The
                                   usable area is the unshaded area between those two threshold curves, A
                                   and C. Simple calculations can give estimates of the level and delay of
                                   any specific reflection, knowing the speed of sound, the distance trav-
                                   eled and applying the inverse square law. Figure 3-20 gives the subjec-
                                   tive reactions the listener will probably have to the combination of any
                                   reflection and the direct sound.
                                      To assist in the “simple” calculations mentioned previously, the
                                   following equations can be applied:
                                                              (reflected path, ft) – (direct path, ft)
                                           Reflection delay
                                                                         1,130 ft/sec
                                   This assumes 100% reflection at the reflecting surface.
                                                                                   direct distance, ft
                                     Reflection level at listening position   20 log
                                                                                 reflection distance, ft
                                   This assumes the inverse square propagation.


                                   Occupational and Recreational Deafness

                                   The hearing of workers in industry is now protected by law. The
                                   higher the environmental noise, the less exposure allowed (Table 3-2).
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