Page 188 - Master Handbook of Acoustics
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FIGURE 10-3   Comb filtering of signals having distributed spectra. (A) Instantaneous spectrum of
   music signal. (B) Replica of A, which is delayed 0.1 msec from A. (C) The summation of A and C
   showing typical comb filtering. A linear frequency scale is used.



  Combing of Direct and Reflected Sound


  The 0.1-msec delay in Fig. 10-3 could have been from a digital-delay device, or a reflection from a
  wall or other object. The spectral shape of a signal will be changed somewhat upon reflection,
  depending on the angle of incidence, the acoustical characteristics of the reflecting surface, and so on.
  When a direct sound is combined with its reflection, a comb filter is produced, with characteristic
  nulls (also called notches) in the frequency response. Nulls result when two signals are out of phase;
  they are one-half wavelength apart in time. The frequency of the nulls (and peaks) is determined by
  the delay between the direct and reflected sound. The frequency of the first null occurs where the

  period is twice the delay time. This is given by f = 1/(2t), where t is the delay in seconds. Each
  successive null occurs at odd multiples thus: f = n/(2t), where n = 1, 3, 5, 7, and so on. The first peak
  occurs at f = 1/t and successive peaks occur at f = n/t, where n = 1, 2, 3, 4, 5, and so on. The spacing
  between nulls or between peaks is 1/t.

      A reflection delayed 0.1 msec will have traveled (1,130 ft/sec) (0.0001 sec) = 0.113 ft farther
  than the direct signal. This difference in path length, only about 1.35 in, could result from a grazing
  angle with both source and listener, or microphone, close to the reflecting surface. Greater delays are
  expected in more normal situations such as those of Fig. 10-4. The spectrum of Fig. 10-4A is from a
  random noise generator driving a loudspeaker and received by an omnidirectional microphone in free
  space. Noise of this type is widely used in acoustical measurements because it is a continuous signal,
  its energy is distributed throughout the audible frequency range, and it is more similar to speech and
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