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

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DIGITAL FILTERING 483<br />

Input Samples Output Samples<br />

.000 .000<br />

.309 .309<br />

.588 .897<br />

.809 1.706<br />

.951 2.657<br />

1.000 3.657<br />

.951 4.608<br />

.809 5.417<br />

.588 6.005<br />

.309 6.314<br />

.000 6.314<br />

-.309 6.005<br />

-.588 5.417<br />

-.809 4.608<br />

-.951 3.657<br />

-1.000 2.657<br />

-.951 1.706<br />

-.809 .897<br />

-.588 .309<br />

-.309 .000<br />

.000 .000<br />

.309 .309<br />

.588 .397<br />

.809 1.706<br />

(A)<br />

Input Samples Output Samples<br />

.000 .000<br />

.588 .588<br />

.951 1.539<br />

.951 2.490<br />

.588 3.078<br />

.000 3.078<br />

-.588 2.490<br />

-.951 1.539<br />

-.951 .588<br />

-.588 .000<br />

.000 .000<br />

.588 .588<br />

.951 1.539<br />

(8)<br />

Fig. 14-2. Filtering action <strong>of</strong> a digital integrator. (A) Response to sine wave<br />

samples at 0.05 Fs. (B) Response to sine wave samples at 0.1 Fs.<br />

resistance. The dc gain is simply the leak resistance divided by the inputgain-determining<br />

resistor.<br />

In the previous chapter, it was mentioned that a digital accumulator<br />

acts like an integrator when nu~bers are repeatedly added to it. This is just.<br />

as true when the numbers being accumulated are samples <strong>of</strong> some arbitrary<br />

waveform as when they represent a constant "current" in a digital oscillator.

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