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

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SOUND MODIFICATION METHODS 55<br />

output and dividing it by the input amplitude, which usually remains const~nt.<br />

The phase shift at a particular frequency may be determined by comparing<br />

the two waveforms on the oscilloscope face. Note that phase shifts greater<br />

than 180 0<br />

leading or lagging cannot be uniquely determined at an arbitrary<br />

frequency with this setup. However, a point <strong>of</strong> zero phase shift can usually be<br />

found and the trend away from zero followed.<br />

The amplitude response then is plotted simply by varying the input<br />

frequency over the audible range and plotting the gain facror. Customarily,<br />

the frequency axis is logarithmic in order to accurately represent a wide range<br />

<strong>of</strong> frequencies, and the amplitude axis is scaled in decibels, which effectively<br />

makes it a log scale also. The phase response may be plotted similarly,<br />

01----_.<br />

~-~5<br />

~ -10<br />

«<br />

~ -15<br />

-20<br />

-25 '"---cu-r-o-rr-F6-R-EO-U-EN-C-Y--------'------<br />

FREQUENCY<br />

(Al<br />

o<br />

!-~5<br />

~ -10<br />

« -15<br />

-20<br />

_25L------L...------'-----___<br />

FREOUENCY<br />

(8)<br />

o<br />

~-~5<br />

~ -10<br />

«<br />

-/5<br />

-20<br />

-25'------'-----+--------"-------<br />

CENTER FREQUENCY<br />

o<br />

~-~5<br />

z -10<br />

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