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Musical-Applications-of-Microprocessors-2ed-Chamberlin-H-1987

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572 MUSICAL ApPLICATIONS OF MICROPROCESSORS<br />

OSCILLATOR<br />

-+-J[rJ<br />

FILTER<br />

(EXCITATION<br />

(SYSTEM<br />

FUNCTION)<br />

FUNCTION)<br />

OUTPUT<br />

FREJENCY<br />

WAVEFORM<br />

REJONSE<br />

SHAPE<br />

(A)<br />

FREQUENCY<br />

SPECTRUM OF OSCILLATOR<br />

FREQUENCY<br />

AMPLlTUOE RESPONSE OF FILTER<br />

SPECTRUM OF OUTPUT<br />

(8)<br />

Fig. 16--14. Natural sound modeling. (A) Simple model <strong>of</strong> natural sound process.<br />

(B) Spectral interpretation <strong>of</strong> simple model.<br />

ternatively, the excitation function can be white noise, which does invalidate<br />

the pitch parameter but has no effect on anything else. The system function<br />

may be either fixed or variable depending on the sound being modeled.<br />

The range <strong>of</strong> natural sounds to which this model is applicable is actually<br />

very large. Most wind instruments, such as the bassoon, and bowed<br />

string instruments, such as the violin, are well described by this model. The<br />

human voice is a prime example. In these examples, a harmonic-rich excitation<br />

function is generated by a vibrating element such as a reed, sticky<br />

string, or flapping folds <strong>of</strong> flesh. Resonators in the instruments, such as the<br />

folded tube <strong>of</strong> the bassoon, wood panels with odd-shaped cutouts, or oral and<br />

nasal cavities filter the excitation function before it actually escapes into the<br />

air. Musical instruments usually have fixed resonators (notable exceptions are<br />

muted brass instruments), whereas the human voice depends on a highly<br />

variable resonator for its expression. All <strong>of</strong> these resonators may have a<br />

number <strong>of</strong> distinct resonant frequencies (peaks in the amplitude response)

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