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

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214 MUSICAL ApPLICATIONS OF MICROPROCESSORS<br />

required for any degree <strong>of</strong> sharpness. There exists, however, a very versatile<br />

filter structure that not only simulates exactly an R-L-C filter in the resonant<br />

(bandpass) mode but simultaneously simulates the other three possible filtering<br />

functions that could be built with one resistor, one inductor, and one<br />

capacitor as shownin Fig. 6-22. The family <strong>of</strong> amplitude response curves<br />

represents low, medium, and high Q cases corresponding to high, medium,<br />

and low values <strong>of</strong> RQ.<br />

The circuit configuration in Fig. 6-23, which requires two integrators<br />

and a summing amplifier, is well known to analog computer users but only<br />

fairly recently has gained popularity as a cost-effective active filter circuit. This<br />

is called a "two-pole filter" because two energy storage elements (capacitors)<br />

are present in the signal path. The basic circuit is called a "state-variable" or<br />

"integrator-loop" filter and provides simultaneous high-pass, bandpass, and<br />

low-pass filtering functions <strong>of</strong> the same input. A band-reject output is obtained<br />

by summing (they are 180 0<br />

out <strong>of</strong> phase at resonance) the high-pass<br />

and low-pass outputs with an additional op-amp. Figure 6-24 shows the<br />

amplitude responses <strong>of</strong> each <strong>of</strong> the outputs for both low Q (1.5) and moderately<br />

high Q (15). Note that the low-pass and high-pass functions have<br />

cut<strong>of</strong>fs that are twice as sharp as the single-pole filters discussed earlier and<br />

that they develop a prominent peak just before the cut<strong>of</strong>f point for high Q<br />

settings.<br />

Besides simultaneous filtering functions, the circuit has the advantage<br />

that frequency and Qfactor (or bandwidth in hertz with a different configuration)<br />

are independently variable. In other words, RQ only affects the Q factor<br />

and RF only affects the center or cut<strong>of</strong>f frequency. Note that two resistors<br />

affect frequency. Actually, the frequency is inversely proportional to the<br />

square root <strong>of</strong> their product. If they are equal and varied together, however,<br />

the square root drops out al}d the frequency-resistance relationship is linear.<br />

R<br />

HIGH-PASS<br />

OUTPUT<br />

C<br />

BANDPASS<br />

OUTPUT<br />

C<br />

INPUT<br />

R<br />

R<br />

RF<br />

RF<br />

LOW-PASS<br />

OUTPUT<br />

R<br />

R<br />

R<br />

R<br />

F=_I­<br />

2rrRFC<br />

BAND-REJECT<br />

OUTPUT<br />

0= RO+R<br />

R<br />

Fig. 6-23. Two-pole tunable active filter

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