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SOUND MODIFICATION METHODS 57<br />

FREQUENCY<br />

INPUT SPECTRUM<br />

FREQUENCY<br />

FILTER RESPONSE<br />

FREQ-lJENCY<br />

OUTPUT SPECTRUM<br />

Fig. 2-5. Effect <strong>of</strong> filtering on the spectrum<br />

The other two parameters are the two ultimate slopes <strong>of</strong> the sides <strong>of</strong> the<br />

bell-shaped curve. As before, they are usually multiples <strong>of</strong> 6 dB per octave.<br />

The slope just beyond the 3-dB points is usually steeper than the ultimate<br />

slope far from the center frequency and becomes more so for higher Qs<br />

(narrower bandwidths).<br />

The final basic filter shape is called a band-reject (or notch) response and<br />

is shown in Fig. 2--4D, The center frequency is, <strong>of</strong> course, the frequency <strong>of</strong><br />

greatest attenuation. Specification <strong>of</strong> the width parameter is not really standardized<br />

because the exact shape <strong>of</strong> the notch varies considerably with the<br />

filter circuit. However, one common specification is, again, the difference<br />

between the 3-dB down points. Often, a rough attempt at specifying the<br />

shape is made by specifying both the 3-dB and the 60-dB notch widths.<br />

The effect <strong>of</strong> a filter on the spectrum <strong>of</strong> a sound can be easily determined<br />

graphically as in Fig. 2-5. As a simple case, consider a sound with all<br />

o<br />

-5<br />

-10<br />

-15<br />

~ -20<br />

UJ -25<br />

t.::l<br />

:::><br />

~ -30<br />

a..<br />

~ -35<br />

-40<br />

-45<br />

-50<br />

-55<br />

-60<br />

5 7 9 II 12 13 17 19 21 23 25 '27 29 31<br />

HARMONIC NUMBER<br />

(A)<br />

Fig. 2-6. Effect <strong>of</strong> filters on a square wave. (A) Original square wave.<br />

,

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