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VOLTAGE-CONTROL METHODS 89<br />

two is rare in the smaller systems. Voltage-controlled filters <strong>of</strong> adequate<br />

performance are a recent development, and there is still considerable room for<br />

improvement.<br />

The signal inputs and controls are similar to those <strong>of</strong> the VeA, although<br />

there may be only one or two provided. There are usually several<br />

signal outputs, however, each corresponding to a different filter mode. The<br />

most popular filtering circuit simultaneously generates a low-pass, highpass)<br />

and bandpass output from a single input. A band-reject output may<br />

also be provided at very little additional cost. Sometimes the multiple outputs<br />

are applied to a tapped potentiometer, and the user seleCts a mixture <strong>of</strong><br />

these filtering functions to be sent to a single output.<br />

Although there are multiple outputs, there is only one frequency<br />

parameter. Under the proper operating conditions (low Qfactor) the low-pass<br />

and high-pass - 3-dB frequencies and the center frequencies <strong>of</strong> the bandpass<br />

and band-reject outputs are all the same. At higher Qs, the low-pass and<br />

high-pass filtering functions undergo a phenomenon called corner peaking,<br />

which is illustrated in Fig. 3-5. At very high Qs, the corner peaking becomes<br />

excessive, and the audible filtering effect <strong>of</strong> low-pass, bandpass, and<br />

high-pass outputs becomes similar. The notch output under these conditions<br />

becomes so narrow that its effect on the sound is hardly noticeable.<br />

Since the Q factor has such an important effect, it must be variable. The<br />

most common configuration is a single panel control for Q. It is desirable,<br />

however, to have a voltage-controlled Q probably with an exponential relationship,<br />

since the useful range for Q is from 0.5 to several hundred at least.<br />

One common imperfection in existing filters is that high Q factors lead to<br />

instability and may even cause the filter to break into intermittent oscillation.<br />

If this was not such a problem, Qs up in the thousands would be useful<br />

for generating slowly decaying ringing sounds in response to a short input<br />

pulse.<br />

Normally, the frequency control inputs are straightforward and essentially<br />

identical to the frequency control inputs on the VCO. However, there<br />

is an interaction between frequency and Q that must be conSIdered. Taking<br />

the bandpass output as an example, there are two things that may happen<br />

when the center frequency is varied. In a constant Q filter, the Q factor<br />

remains constant as center frequency is changed. This is desirable if one is<br />

filtering white noise to give it a sense <strong>of</strong> pitch, since the same degree <strong>of</strong><br />

"pitchedness" will be retained regardless <strong>of</strong> the center frequency. However, if<br />

the filter is used to create ringing sounds, the ringing time will be much<br />

longer at lower frequencies than it will be at high frequencies. This is because<br />

Q is really related to the rate <strong>of</strong> ringing decay in terms <strong>of</strong> number <strong>of</strong> cycles<br />

rather than seconds. A constant bandwidth filter actually has a Q that is<br />

proportional to center frequency. Thus, if the bandwidth is set to 100 Hz<br />

and the center frequency to 300 Hz, the effective Q is low, but if the center<br />

frequency is 5 kHz, the laO-Hz bandwidth represents a relatively high Q.<br />

Although there are applications for both types <strong>of</strong> frequency control, most

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