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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 Contents Index
Miller Puckette 2005-07-11