Solution automatic control systems 8ed - kuo and golnaraghi - solutions manual
2-1 (a)
Poles: s = 0, 0, Zeros: s =
−1, −10;
(b)
Poles: s =
−2, −2; −1 cancel each other.
−2, ∞, ∞, ∞.
Zeros: s = 0. The pole and zero at s =
(c)
Poles: s = 0,
−1 + j, −1 − j; −2.
(d)
Poles: s = 0,
−1, −2, ∞.
Zeros: s =
2-2 (a) G (s) = (d)
G ( s)
(b) 5
(c) G ( s) = (e)
( s + 5)
1 s
2
2
(s
=
4s
2+4
∞
)
+
1 s+ 2
G (s)
=
4 s
2
+ 4s +8
=
+4
G (s)
∑e
k =0
kT ( s + 5 )
=
1
1
−e
−T ( s+5 )
2-3 (a)
g ( t ) = u s ( t ) − 2u s (t − 1) + 2 u s( t − 2) − 2 u s ( t − 3) + L G (s ) = 1 s
(1 − 2e − s + 2e−2 s − 2e −3s + L ) =
1 s
s 1+ e
(
1−e
−s −s
)
gT (t ) = u s (t ) − 2us ( − 1) + us (t − 2) t GT (s ) =
0≤ t ≤ 2
2(1 − 2e − s + e −2s ) = ( 1 − e − s )
1 s
1
g(t )
=
∑
k =0
∞
g
T
(t
− 2k )us (t − 2k )
G (s)
=
∑s
k =0
∞
1 (1
−e
−s
) e
2
−2 ks
=
1− e
−s −s
s (1 + e
)
(b) g ( t) = 2tu s ( t ) − 4(t − 0.5) u s (t − 0.5) + 4(t − 1) us (t − 1) − 4(t − 1.5)us (t − 1.5) + L G ( s) =
g
T
2 s
2
(1 − 2e
−0.5 s
+ 2e
−s
−2e
−1.5 s
( − 0.5 s ) + L) = 2 −0.5 s s (1 + e )
2 1−e
2
(t )
= 2 tu s ( t ) − 4 ( t − 0 . 5) u s ( t − 0 . 5) + 2( t − 1 ) u s ( t − 1 ) 2 s
2
0
≤ t ≤1
GT ( s ) =
∞
(1 − 2e−0.5 s + e− s ) = s 2 (1 − e−0.5 s )
2
∞
g (t ) =
∑
k=0
g T ( t − k )us ( t − k )
G(s ) =
k=0
∑ s2 (
2
1 −e
−0.5 s
)
2
e
− ks
=
( −0.5 s ) 2 −0.5s s (1+ e )
2 1−e
2-4
g(t )
= ( t + 1 ) u s ( t ) − ( t − 1 ) u s ( t − 1 ) − 2 u s ( t − 1 ) − ( t − 2 ) u s ( t − 2 ) + ( t − 3) u s ( t − 3) + u s ( t − 3)
G ( s) =
1 s
2
(1 − e − s − e −2 s + e −3 s ) + s (1 −2e − s + e −3 s )
1
1 6( s 1 3( s 1 2( s
2-5 (a)
Taking the Laplace transform of the differential equation, we get 1 1 2 ( s + 5s + 4) F ( s) = F (s) = s +2 ( s + 1)(s + 2 )( s f (t )
+4)
=
+ 4)
+
+ 1)
−
+ 2)
=
1 6
e
−4 t
+
1 3
e
−t
−
1 2
e
−2 t
t
≥0
sX (s)
(b)
sX ( s )
1
− x1( 0 ) =
X (s)
2
x (0)
1
=1
2
− x 2 ( 0 ) = −2 X 1 ( s ) − 3 X 2 ( s ) +
1 s
x (0)
2
=0
Solving for X1 (s) and X2 (s), we have X 1 ( s)
= =
s s( s
2
+ 3 s +1 −1
+ 1 )( s+ 2 )
= =
1 2s
+
1 s
+1
1 s
−
1 2( s
+ 2)
X (s)
2
−1
s
(s
+ 1 )( s + 2 )
−t
+1
+
+2
x (t )
2
Taking the inverse Laplace transform on both sides of the last equation, we get x (t )
1
= 0 .5 + e
− 0 .5 e
−2 t
t
≥0
= −e
−t
+e
−2 t
t
≥0
2
2-6 (a)
G (s)
=
1 3s
−
1 2( s
+ 2)
+
1 3( s
+3)
g (t )
=
1 3
−
1 2
e
−2 t
+
1 3
e
−3 t
t
≥0
(b)
G (s)
=
−2 . 5
s
+1
50 s
+
5 (s
+ 1)
2
+
2 .5 s
+3
g(t )
= −2 . 5 e
−t
+ 5 te
−t
+ 2 .5 e
−3 t
t
≥0
(c)
G (s ) =
(
1 s
−
20 s +1
s
−
30s + 20 s +4
1 s
2
)
2
e
−s
g (t ) = 50 − 20e
[
− (t −1)
− 30cos2(t− 1) − 5sin2(t − 1)
] us (t − 1)
(d)
G (s)
=
−
−1
−0.5 t
s
2
+s+2
=
+
1 s
g (t ) = 1 + 1.069e
[ sin1.323t + sin (1.323t − 69.3o ) ] = 1 + e−0.5 t (1.447sin1.323t − cos1.323t )
t
+s +2
−
s s
2
+s+2
Taking the inverse Laplace transform,
t≥0
(e)
g(t )
= 0 .5 t
2
e
−t
≥0
2-7
−1 2 0 A = 0 −2 3 −1 −3−1
0 0 B = 1 0 0 1
u (t ) =
u1( t) u ( t) 2
2-8
(a) Y (s ) R (s ) (c) Y (s ) R (s ) = s ( s + 2) s + 10 s + 2 s + s + 2
4 3 2
(b) = 3s + 1 s + 2 s +5s + 6
(d)
3 2
Y (s) R (s )
=
5 s + 10 s + s + 5 1+ 2e
2 −s 4 2
Y (s ) R (s )
=
2s + s + 5
3
4
5
6
7
8
9
10
11
12
13
Chapter 4...
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