470 Chapter 7 / Control Systems Analysis and Design by the Frequency-Response MethodResonant Peak Magnitude Mrand Resonant Frequency Vr. Consider the
standard second-order system shown in Figure 7–73. The closed-loop transfer function
is
(7–16)
wherezandvnare the damping ratio and the undamped natural frequency, respectively.
The closed-loop frequency response is
where
As given by Equation (7–12), for 0z0.707, the maximum value of Moccurs at
the frequency vr, where
(7–17)
The frequency vris the resonant frequency. At the resonant frequency, the value of M
is maximum and is given by Equation (7–13), rewritten
(7–18)
whereMris defined as the resonant peak magnitude. The resonant peak magnitude is
related to the damping of the system.
The magnitude of the resonant peak gives an indication of the relative stability of the
system. A large resonant peak magnitude indicates the presence of a pair of dominant
closed-loop poles with small damping ratio, which will yield an undesirable transient
response. A smaller resonant peak magnitude, on the other hand, indicates the absence
of a pair of dominant closed-loop poles with small damping ratio, meaning that the
system is well damped.
Remember that vris real only if z<0.707. Thus, there is no closed-loop resonance
ifz>0.707. [The value of Mris unity only if z>0.707. See Equation (7–14).] Since
the values of Mrandvrcan be easily measured in a physical system, they are quite useful
for checking agreement between theoretical and experimental analyses.
Mr=
1
2 z 21 - z^2
vr=vn 21 - 2 z^2
M=
1
B
a 1 -
v^2
v^2 n
b2+ a 2 z
v
vn
b2, a=-tan-^1
2 z
v
vn
1 -
v^2
v^2 n
C(jv)
R(jv)
=
1
a 1 -
v^2
v^2 n
b +j2z
v
vn
=Meja
C(s)
R(s)
=
v^2 n
s^2 + 2 zvn s+v^2 n
R(s) vn C(s)
s(s+ 2 z vn)2
+- Figure 7–73
Standard second-
order system.
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