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Elementary non-recirculating filter
We generalize the non-recirculating comb
filter to the design shown in figure 8.7, called the
non-recirculating elementary filter,
of the first form.
Figure 8.7:
A delay network with a single-sample delay and a complex
gain . This is the non-recirculating elementary filter, first form. Compare
the simpler non-recirculating comb filter shown in Figure 7.3,
which corresponds to choosing here.
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To find the frequency response, as in Chapter 7 we feed the delay network
a complex sinusoid
whose frequency is
,
so that as before,
.
The th sample of the input is and that of the output
is
so the transfer function is
This can be represented graphically as shown in Figure 8.8. Suppose
we write the coefficient in polar form:
Then the gain of the filter is the distance from the point to the point
in the complex plane. Analytically we can see this because
Graphically, the number is just the number rotated backwards
(clockwise) by the angular frequency of the incoming sinusoid. The
value
is the distance from to in the complex
plane, which is equal to the distance from to .
Figure 8.8:
Diagram for calculating the frequency response of the
non-recirculating elementary filter
(Figure 8.7). The frequency response is given by the length of the
segment connecting to in the complex plane.
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As the frequency of the input sweeps from 0 to , the point travels
couterclockwise around the unit circle. At the point where
,
the distance is at a minimum, equal to . The maximum occurs which is
at the opposite point of the circle. Figure 8.9 shows the transfer
function for three different values of .
Figure 8.9:
Frequency response of the elementary non-recirculating filter
Figure 8.7. Three values of are used, all with the
same argument (-2 radians), but with varying absolute value.
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Next: Non-recirculating filter, second form
Up: Designing filters
Previous: Designing filters
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Miller Puckette
2006-03-03