Solution 5.8.1.27
G
H
C
R
+
-
Figure 1:
For the system shown abovewehave
GH(s)=
K
s(s +6)(s +20)
:
The rst step is to plot the poles and zeros of GH in the s-plane and
then nd the root locus on the real axis. The shaded regions of the real axis
in Figure 2 showwhere the root locus occurs. The rule is that root locus
occurs on the real axis to the left of an odd countofpoles and zeros. That
is, if you stand on the real axis and look to your right you must countan
odd numberofpoles and zeros.
The next step is to compute the asymptotes. The numberofasymptotes
is
p
ex
=Number of poles of GH ;Numberofnite zeros of GH:
Im(s)
Re(s)
-6
-20
Figure 2:
The asymptotes occur at the angles
`
=
1+2`
p
ex
180
` =0;;1;;:::p
ex
;1:
In the present case there are three poles and no nite zeros so p
ex
=3.Thus,
there are three asymptotes at
0
=
1+(2)(0)
3
180
=60
1
=
1+(2)(1)
3
180
=180
1
=
1+(2)(2)
3
180
=300
The asymptotes intersect the real axis at
i
=
Sum of poles of GH ;Sum of zeros of GH
p
ex
=
[(;6)+ (;20)];[0]
3
= ;8:67
Since there are no nite zeros and three poles, three closed loop poles
will migrate to zeros at innity,onesuchzero at the `end' of eachasymptote.
The root locus is shown in Figure 3
To nd where the root locus crosses the raycorresponding to =1=
p
2,
remember that
6
GH(s)=;180
at all points on the root locus, including
the point where it crosses the ray.Figure 4 shows the angles made byeach
of the poles and zeros along this ray.Thatis,
;
1
;
2
;
3
= ;180
:
Since
1
= ;135
the equation reduces to
2
+
3
=45
:
Nowitismerely a matter picking some points along the rayandevaluating
the angles. For starters, weknowthatthe pointmust lie to the rightof
s = ;3+j3since at this point
2
=45
.Sowechoose as a starting point
s = ;2+j2. Then
2
+
3
= tan
;1
(2=4)+ tan
;1
(2=18)
= 32:91
Im(s)
Re(s)
-20 -6
Figure 3: Completed Root Locus
Im(s)
Re(s)
θ
1
θ
3
-6
-20
θ
2
Figure 4: Satisfaction of Angle Condition Along RayofConstantDamping
=0:707
s ;2:6+j2:6 ;2:57 + j2:57 ;2:56+ j2:56
2
+
3
45:9
45:23
45:01
Table 1: SearchforMaximum in Gain
s -22 -21 -20.5 -20.7 -20.8 -20.9
K 704 315 148 213 246 280
Table 2: Searchforclosedlooppole
This means that wemust makeour next guess to the left. Table 1 sumarizes
the searchfor the solution to this equation. The gain to place the poles on
imaginary axis is then
K = jsjjs +6jjs+20j
=
p
2:56
2
+2:56
2
q
(6;2:56)
2
+2:56
2
q
(20;2:56)
2
+2:56
2
)
= 273:6
The third closed loop pole can be found byavarietyofmethods. One is
to search along the negativerealaxistotheleft of s = ;20 until a gain of
275 is found. The Table 2 summarizes that search. Thus, the third closed
loop pole is around s = ;20:9. It is clear that the closed loop pole associated
with the loop transfer function pole at s = ;20 migrates very slowly towards
;1.