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54 MUSICAL ApPLICATIONS OF MICROPROCESSORS<br />

different frequency are fed in, the output spectfum contains not only harmonic<br />

frequencies <strong>of</strong> each tone, but every possible combination <strong>of</strong> sum and<br />

difference frequencies between the tones and their harmonics. For musical<br />

instrument use, the resulting sound is close to garbage unless the input<br />

frequencies are simply related such as a 3:2 ratio. For more abstract goals,<br />

however I anything is potentially llseful even if it is not predictable.<br />

Filters<br />

While nonlinear circuits are relatively simple spectrum modifiers, theif<br />

action is indirect. A different class <strong>of</strong> device calledfilters acts directly on the<br />

spectrum changing the amplitude and phase <strong>of</strong> each sine wave component <strong>of</strong><br />

the input signal by a predictable amount. Furthermore, theif action on the<br />

spectrum is unaffected by the actual spectrum <strong>of</strong> the input signal.<br />

Filters can be completely specified by giving a plot <strong>of</strong> their amplitude<br />

response and phase response as a function <strong>of</strong> frequency. Nearly always, the<br />

amplitude response is termed, incorrecdy, the frequency response but the<br />

former term will be used exclusively in this book. The test setup shown in<br />

Fig. 2-3 can be used to make such plots. Here we have a variable-frequency<br />

sine wave signal generaror, a calibrated oscilloscope with dual-trace capability,<br />

and the filter under test. The gain <strong>of</strong> the fil ter at a parricular frequency<br />

may be determined by measuring the amplitude <strong>of</strong> the signal at the filter<br />

VARIABLE -FREQUENCY<br />

SINE WAVE<br />

GENERATOR<br />

FILTER<br />

UNDER<br />

TEST<br />

A<br />

B<br />

DUAL- TRACE<br />

OSCILLOSCOPE<br />

INPUT<br />

OSCILLOSCOPE PRESENTATION<br />

Fig. 2-3. Experimental setup for characterizing a filter

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