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120   CHAPTER SIX



                                   impossible. This chapter is a very brief overview of both analog and
                                   digital sound processing principles and practice, especially the prin-
                                   ciples.


                                   Resonance

                                   The man on the stage is doing the old trick of breaking the wine glass
                                   with sound. Instead of doing it with the diva’s voice, he holds the gob-
                                   let in front of the loudspeaker, which shatters it as a high-intensity
                                   tone is emitted. The secret lies in the brief preparation made before the
                                   audience was assembled. At that time he placed a small coin in the
                                   goblet and held it in front of the loudspeaker as the frequency of the
                                   sine generator was varied at a low level. He carefully adjusted the gen-
                                   erator until the frequency was found at which the coin danced wildly
                                   in the glass. During the demonstration no tuning was necessary, a blast
                                   of sound at this predetermined frequency easily shattered the glass.
                                      The wild dancing of the coin in the glass in the preliminary adjust-
                                   ment indicated that the excitation frequency from the loudspeaker was
                                   adjusted to the natural frequency or resonance of the goblet. At that
                                   frequency of resonance a modest excitation resulted in very great
                                                              vibration of the glass, exceeding its break-
                                                              ing point. As shown in Fig. 6-1, the ampli-
                                         f o                  tude of the vibration of the glass changes
                                                              as the frequency of excitation is varied,
                                                              going through a peak response at the fre-
                                                              quency of resonance, f o.
                                                                 Such resonance effects appear in a
                       Amplitude                              wide variety of systems: the interaction of

                                                              mass and stiffness of a mechanical system,
                                                              such as a tuning fork, or the acoustical res-
                                                              onance of the air in a bottle, as the mass of
                                                              the air in the neck of the bottle reacts with
                                                              the springiness of the air entrapped in the
                                     Frequency
                                                              body of the bottle. See Helmholtz res-
                     FIGURE 6-1
                                                              onators, Chap. 9.
                   The amplitude of vibration of any resonant system is  Resonance effects are also dominant in
                   maximum at the  natural frequency or  resonant fre-
                   quency (f) and is less at frequencies below and above  electronic circuits as the inertia effect of
                   that frequency.                            an inductance reacts with the storage
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