instantaneously transfer energy from the input to the output. In addition, since
noise is almost always present in one form or another, a system with a unity transfer
function is not desirable. A desired control system, in many practical cases, may
have one set of dominant complex-conjugate closed-loop poles with a reasonable
damping ratio and undamped natural frequency. The determination of the significant
part of the closed-loop pole-zero configuration, such as the location of the domi-
nant closed-loop poles, is based on the specifications that give the required system
performance.
Cancellation of Undesirable Complex-Conjugate Poles. If the transfer func-
tion of a plant contains one or more pairs of complex-conjugate poles, then a lead, lag,
or lag–lead compensator may not give satisfactory results. In such a case, a network that
has two zeros and two poles may prove to be useful. If the zeros are chosen so as to
cancel the undesirable complex-conjugate poles of the plant, then we can essentially
replace the undesirable poles by acceptable poles. That is, if the undesirable complex-
conjugate poles are in the left-half splane and are in the form
then the insertion of a compensating network having the transfer function
will result in an effective change of the undesirable complex-conjugate poles to ac-
ceptable poles. Note that even though the cancellation may not be exact, the com-
pensated system will exhibit better response characteristics. (As stated earlier, this
approach cannot be used if the undesirable complex-conjugate poles are in the right-
halfsplane.)
Familiar networks consisting only of RCcomponents whose transfer functions pos-
sess two zeros and two poles are the bridged-Tnetworks. Examples of bridged-Tnet-
works and their transfer functions are shown in Figure 7–117. (The derivations of the
transfer functions of the bridged-Tnetworks were given in Problem A–3–5.)
s^2 + 2 z 1 v 1 s+v^21
s^2 + 2 z 2 v 2 s+v^22
1
s^2 + 2 z 1 v 1 s+v^21
520 Chapter 7 / Control Systems Analysis and Design by the Frequency-Response MethodC 2RR
C 1R 2CC
ei eo ei R 1 eo(a) (b)Eo(s)
Ei(s)RC 1 RC 2 s^2 + 2 RC 2 s+ 1
RC 1 RC 2 s^2 + (RC 1 + 2 RC 2 )s+ 1= Eo(s)
Ei(s)R 1 CR 2 Cs^2 + 2 R 1 Cs+ 1
R 1 CR 2 Cs^2 + (R 2 C+ 2 R 1 C)s+ 1=
Figure 7–117
Bridged-Tnetworks.Openmirrors.com