Solution: 10.8.4.4
?ω
Im(s)
Re(s)
-2 -1
θ
1
θ
4
θ
2
θ
3
α
β
(a)
3
Im(s)
Re(s)
(b)
?3
2
?20
?10
γ
Figure 1: Bode Magnitude and Phase Plots
The angle contributions of eachofthe poles and zeros along GH(I
) can be
determined from part (a) the vector diagram of Figure 2. For ! small, ,
2
and
3
are each0
.Thetwopoles at the origin eachcontribute ;90
each
at all values of !.Ifweevaluate GH at ! = j,where is arbitrarily small,
weobtain
lim
!0
6
GH(j)=;180
The only remaining question is how
6
GH(;j) approaches ;180
. That
is, does it approach ;180
from the second quadrantorthe third quadrant?
The table below gives some values ofjGH(j!)jand
6
GH(j!)forK =20.
These values help us sketchinthe rst portion of the Nyquist plot.
! -0.2 -1 -2
jGH(j!)j 84.4 4.0 1.09
6
GH(j!) 178:2
180
195
1
?ω
Im(s)
Re(s)
-2 -1
θ
1
θ
4
θ
2
θ
3
α
β
(a)
3
Im(s)
Re(s)
(b)
?3
2
?20
?10
γ
Figure 2: Vector Representation of Components of GH
2
Im(GH)
Re(GH)
Figure 3: Plot of GH(I)
The alternativeistojust take the negatives of the angles on the Bode
phase plot. As ! !;1, ,
1
,and
2
all appproch ;90
,Sothat
lim
!!1
6
GH(j!)=270
:
At the same time the magnitude of eachofthe vectors in Figure 2 be-
comes innite in length. Since one of the vectors is in the numerator of GH
and four are in the denominator, clearly
lim
!!1
jGH(j!)j=0
The rst part of the plot is shown in Figure 3 Wesee that the plot crosses
the negativerealaxis twice.
As weevaluate GH along part 2 of
, weremainessentially at the origin.
To draw the portion of the Nyquist plot that corresponds to evaluating GH
along part 1 of the
contour wesimplytakethe mirror image through the
real axis of the rst part of the Nyquist contour shown above. Thus, the
contour generated byevaluating GH along portions I, II, and I
is shown
in Figure 4.
To complete the contour, wemust evaluate GH along the semicircle of
radius . Figure 5 depicts this evaluation. Note that all the vectors except
that drawn from the origin have nite length, and associated angles of zero.
The angles are zero, because the radius of the semicircle is arbitrarily small.
This doesn't appear to be the case because the semicircle has a large radius
in the picture, while in reality this radius goes to zero. Thus, along the
3
Im(GH)
Re(GH)
Figure 4: Plot of GH(I), GH(II), GH(III)
XXXX
q
2
Re(GH)
Im(GH)
Figure 5: Evaluation of GH(III)
4
Im(GH)
Re(GH)
I II III
Figure 6: Completed Nyquist Plot
semicircle
GH(
6
)
20
6
1
6
6
= 1
6
;2
As wetraverse the semicircle clockwise( cw), evaluating GH,theplot of
GH will rotate counterclockwise (ccw) through twice the angle we traversed
along the semicircle, or 360
.The nal Nyquist plot is shown in Figure 6.
For a gain of 50, GH crosses the negativerealaxis twice. From the Bode
plot we see that the rst crossing occurs for s = j2:5, and the magnitude is
jGH(j2:5)j=10
;15=20
=0:1778:
The second crossing is at s = j10 with a magnitude of
jGH)j10)j=10
;34=20
=0:01995:
Tomakethcrossing at ! =2:5occur at (;1;;;)inthe GH plane wemust
increase the gain to
50
0:1778
=281:
To makethe crossing at ! =10reach the point(;1;;0) wemust increase
the gain to
50
0:01995
=2506:
5
For 0 <K;;281 the point(;1;;0) is in region I and the Nyquist equation
is
Z = ;2+P
= ;2+4
= 2
This means there are twoclosed loop poles inside
in the s-plane. Since
encloses the left half of the s-plane, there are two unstable poles for gains
below K<281.
For 281 <K;;2506 the point(;1;;0) is in region II,where wehaveone
clockwise and one counterclockwise encirclement, and the Nyquist equation
is
Z = N +4
= ;1+1+4
= 4
This means there are four closed loop poles inside
in the s-plane. Since
encloses the left half of the s-plane, there are no unstable poles for 281K<
2505.
For 2506 <K, the point(;1;;0) is in region III,wehavetwocounter-
clockwise encirclementof(;1;;0). The Nyquist equation is
Z = ;N +P
= ;2+4
= 2
This means that for 2506 <Kthere are twoclosed loop poles inside the
contour
, that is tw0 closed loop poles in the left half plane.
Note that the root locus crosses the imaginary axis at w 2:5, and
! 10, as shown in Figure 7
6
-30 -25 -20 -15 -10 -5 0
-10
-5
0
5
10
Figure 7: Root Locus
7