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

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196 MUSICAL ApPLICATIONS OF MICROPROCESSORS<br />

reduced to the same order <strong>of</strong> magnitude as other circuit drifts in the typical<br />

studio environment.<br />

Two other minor errors are corrected by modifying the reference current<br />

regulator for the exponential converter. One <strong>of</strong> these is due to the finite<br />

"bulk" resistance in the converter transistors. The other is due to finite<br />

discharge time in the sawtooth oscillator. Both effects cause high frequencies<br />

to be lower than they should be. The magnitude <strong>of</strong> both errors is directly<br />

proportional to the magnitude <strong>of</strong> the control current from the converter. The<br />

addition <strong>of</strong> Oland R5 couples a voltage that is directly proportional to the<br />

control current back into the control input summer. This voltage is developed<br />

across the 10K protective resistor in series with the reference current<br />

regulator. The diode cancels a o.6-v <strong>of</strong>fset that exists at low values <strong>of</strong> control<br />

current. In use, R5 is adjusted for optimum high-frequency tracking.<br />

The sawtooth oscillator proper uses a high-speed, very-Iow-inputcurrent<br />

op-amp as the integrator. The odd power supply hookup for A3 is<br />

necessary because it cannot stand total supply voltages beyond 15 V. Note<br />

that the type 311 comparator has an open-collector output so that when its<br />

pullup resistor is tied to ground its output voltage swings between -15 V<br />

and a V, the range needed by Q4.<br />

Figure 6-11 shows the waveform standardizers and shapers with all<br />

adjustments and parts values. The sawtooth output is taken from the second<br />

inverter rather than the first shown earlier so that a positive going ramp is<br />

produced. The negative ramp at the output <strong>of</strong> A4 could also be brought out<br />

if desired. The glitch in the triangle wave mentioned earlier is largely cancelled<br />

by injecting an opposite polarity pulse derived from the rapid retrace <strong>of</strong><br />

the negative ramp. The rectangular-wave amplitude is standardized by the<br />

saturating complementary emitter follower, Q5 and Q6. Using this circuit,<br />

voltage levels <strong>of</strong> the rectangle will equal the ± 10-V system reference voltages<br />

to within a couple <strong>of</strong> millivolts.<br />

Adjustment<br />

Adjustment <strong>of</strong> the circuit is straightforward and need not require a lot<br />

<strong>of</strong> test equipment, although a frequency counter, accurate digital voltmeter,<br />

and oscilloscope are' helpful. For use in a precalibrated computer-controlled<br />

system, the adjustments should be made to the values listed in Table 6-1.<br />

These values <strong>of</strong>fer the most logical control relationship and widest possible<br />

range in a precalibrated system. Ideally, they should be set as accurately as<br />

possible and then rechecked every few months <strong>of</strong> operation. This will allow<br />

programming <strong>of</strong> the system to proceed with minimal concern over analog<br />

errors in the system. Also shown in the calibration table are performance<br />

parameters obtained from a breadboard <strong>of</strong> the circuit. As can be seen, the<br />

performance is excellent in nearly all respects and certainly much better than<br />

could be obtained just a few years ago at 10 times the cost.

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