Active filters are frequently realized as grounded threeterminal networks. It will be shown that one can create the complementary transfer function t' = 1 - t by first synthesizing t with a threeterminal network and then interchanging the network's input and ground leads, i.e., the former network ground is the new input and the former input is grounded. The output voltage continues to be taken with respect to common ground. If the active element in the network is a differential-input op amp, then this maneuver can be carried out without changing the dc power-supply common-ground connection. It is shown that this is not true in general of finite-gain amplifier networks or of single-input op amp networks. Several uses are suggested and the example of a 360° all-pass section is examined in detail. It is shown that in the particular case of a multiinput biquad all-pass section there is a small increase in the variability of the delay due to resistor changes, and experimental results are given which confirm this. Both the all-pass and band-reject realizations are attractive because the zero frequency is guaranteed to track the pole frequency. A proof of the results for an N -terminal network is outlined.
[1]
P. E. Fleischer,et al.
Design formulas for biquad active filters using three operational amplifiers
,
1973
.
[2]
J. Tow.
Design formulas for active RC filters using operational-amplifier biquad
,
1969
.
[3]
D. Hilberman,et al.
An approach to the sensitivity and statistical variability of biquadratic filters
,
1973
.
[4]
D. Hilberman,et al.
Synthesis of Rational Transfer and Admittance Matrices with Active RC Common-Ground Networks Containing Unity-Gain Voltage Amplifiers
,
1968
.
[5]
R. Sallen,et al.
A practical method of designing RC active filters
,
1955,
IRE Transactions on Circuit Theory.