A Chamberlin filter is a simple two-pole IIR filter with the
transfer function given in Equation 1:
Hz=
F
z
2z-11−(2−(
F
c
Q
c
−
F
c
2))z-1−1z-2
H
z
F
z
2
z
-1
1
2
F
c
Q
c
F
c
2
z
-1
1
F
c
Q
c
z
-2
(1) where
Fc
F
c
determines the frequency where the filter peaks, and
Q
c
1Q
Q
c
1
Q
determines the rolloff.
Q is
defined as the positive ratio of the center frequency to the
bandwidth. A derivation and more detailed explanation is
given in
Dattorro. The
topology of the filter is shown in
Figure 1.
Note that the final feedback stage puts a pole just inside the
unit circle on the real axis. For a response with smaller
bandwidth, move the pole closer to the unit circle, but do not
move it so far that the filter becomes unstable. Multiple
second-order sections can be cascaded to yield a sharper
rolloff.
Figure 2 and Figure 3 show how
the response of the filter varies with
Q
c
Q
c
and
F
c
F
c
.
"Doug course at UIUC using the TI C54x DSP has been adopted by many EE, CE and CS depts Worldwide "