Page 265 - The Master Handbook Of Acoustics
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240   CHAPTER TEN



                                   Reflections Inside a Cylinder

                                   St. Paul’s Cathedral in London boasts a whispering gallery. The way this
                                   whispering gallery works is explained in the diagram of Fig. 10-8. Reflec-
                                   tions from the exterior surfaces of cylindrical shapes have been men-
                                   tioned in the treatment of “polys.” In this case the source and receiver are
                                   both inside a mammoth, hard-surfaced cylindrical room.
                                      At the source, a whisper directed tangentially to the surface is
                                   clearly heard on the receiver side. The phenomenon is assisted by the
                                   fact that the walls are dome-shaped. This means that upward-directed
                                   components of the whispered sounds tend to be reflected downward
                                   and conserved rather than lost above.


                                   Standing Waves

                                   The concept of standing waves is directly dependent on the reflection
                                   of sound as emphasized in Chap. 15. Assume two flat, solid parallel
                                   walls separated a given distance. A sound source between them radi-
                                   ates sound of a specific frequency. The wavefront striking the right
                                   wall is reflected back toward the source, striking the left wall where it
                                   is again reflected back toward the right wall, and so on. One wave trav-
                                   els to the right, the other toward the left. The two traveling waves
                                   interact to form a standing wave. Only the standing wave, the interac-
                                   tion of the two, is stationary. The frequency of the radiated sound is
                                   such as to establish this resonant condition between the wavelength of
                                   the sound and the distance between the two surfaces. The pertinent
                                   point at the moment is that this phenomenon is entirely dependent on
                                   the reflection of sound at the two parallel surfaces.


                                   Reflection of Sound
                                   from Impedance Irregularities

                                   The television repairman is concerned about matching the electrical
                                   impedance of the television receiver to that of the transmission line,
                                   and matching the transmission line to the impedance of the antenna
                                   (or cable). Mismatches of impedance give rise to reflections, which
                                   cause numerous undesirable effects.
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