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

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BASIC ANALOG MODULES 219<br />

+15 V0-------'-'-1<br />

- I5 V 0-------------­ '-t;:---;-j----:H:---+:----+-*---+:-,---t-!.,.,---+---+J<br />

5<br />

0.001 :J<br />

200 n<br />

200 n<br />

Fig. 6--30. Voltage-controlled four-pole low-pass filter with corner peaking<br />

impedance buffers are provided. The gain cells have a predistortion circuit<br />

and therefore can accept input signals as large as 80 mV and still generate less<br />

than 1% distortion. The four gain cells are fed equal control currents from a<br />

built-in multioutput exponential converter. The integrating capacitors are<br />

supplied by the user, however, and should be 1,000 pF or larger. One<br />

limitation to keep in mind is that the buffer amplifiers are only capable <strong>of</strong> a<br />

I-V peak output swing and can only supply 500 !LA <strong>of</strong> load current.<br />

Figure 6-30 shows a voltage-controlled filter circuit using the 2040.<br />

This is properly termed a "four-pole low-pass filter with corner peaking" and<br />

is quite popular, although not as much so as the state-variable type described<br />

earlier. The main difference is that the low-pass cut<strong>of</strong>f <strong>of</strong> 24 dB/octave is<br />

much sharper than the state-variable cut<strong>of</strong>f <strong>of</strong> 12 dB/octave. A bandpass<br />

function is obtained by feeding a portion <strong>of</strong> the filter's output back to its<br />

input to create a resonance. Enough <strong>of</strong> this feedback will cause a pure sine<br />

wave oscillation at the center frequency. Note that a true bandpass response<br />

is not produced by the feedback because there is appreciable very-Iowfrequency<br />

gain. This resonance technique is <strong>of</strong>ten called corner peaking to<br />

distinguish it from true bandpass filtering, which has zero response at both<br />

frequency extremes. At moderate to high Q settings, however, the audible<br />

difference can be quite subtle.<br />

The filter is really four identical single-pole low-pass sections in cascade<br />

all tracking the same control voltage. Each low-pass section is functionally<br />

equivalent to the VCF in Fig. 6-21D discussed earlier. When cascaded as<br />

shown, each section contributes a cut<strong>of</strong>f slope <strong>of</strong> 6 dB/octave; thus, simultaneous<br />

outputs <strong>of</strong> 6, 12, 18, and 24 dB/octave are available. When the

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