Biomedical Engineering Reference
In-Depth Information
From the graph, t
¼
0.17 s. Thus, we have
u ð t Þ:
t
y ð t Þ¼
2
:
88 1
e
0
:
17
13.10.3 Identification of a Linear Second-Order System
Consider estimating the parameters of a second-order system, such as
M þ B y þ Ky ¼ f ð t Þ
.
It is often convenient to rewrite the original differential equation in the standard form for ease
in analysis as
o 2
þ
2zo n y þ
n y ¼ f ð t Þ
ð
13
:
71
Þ
where o n is the undamped natural frequency and z is the damping ratio. The roots of the
characteristic equation are
q
z 2
q
1
z 2
s 1 , 2 ¼
zo n
o n
1
¼
zo n j
o n
¼
zo n j
o d
ð
13
:
72
Þ
A system with 0
<
z
<
1 is called underdamped, with z
¼
1 critically damped and with
z
>
1 overdamped.
Step Response
The complete response of the system in Eq. (13.72) to a step input with arbitrary initial
conditions is given in Table 13.5, where
is the steady-state value of
(
), and
A 1 ,
A 2 ,
B 1 ,
y ss
y
t
f
C 2 are the constants that describe the system evaluated from the initial condi-
tions. For the underdamped system, one can estimate z and o n
,C 1 ,and
to a step input with magni-
tude g from data as follows. Consider the step response in Figure 13.67. A suitable model
for the system is a second-order underdamped model (i.e., 0
<
z
<
1), with solution
"
#
e zo n t
1
y ð t Þ¼ C
1
þ
p
cos o d t þ
ð
f
Þ
ð
13
:
73
Þ
z 2
p
1
z
1
z 2
tan 1
where
C
is the steady-state response,
y ss
, and o d ¼
o n
and f
¼
p
þ
p
.
z 2
The following terms illustrated in Figure 13.67 are typically used to describe, quantita-
tively, the response to a step input:
TABLE 13.5
Step Response for a Second-Order System
Damping
Natural Response Equation
e s
t þ A
e s
t
Overdamped
y ð t Þ¼ y ss þ A
1
2
1
2
e
zo n t cos o d t þ
Underdamped
y ðÞ¼ y ss þ B
ð
f
Þ
1
Þ e
zo n t
Critically damped
y ð t Þ¼ y ss þ C 1 þ C 2 t
ð
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