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Solutions Manual
to accompany
Communication
Systems
An Introduction to Signals and Noise in
Electrical Communication
Fourth Edition
A. Bruce Carlson
Rensselaer Polytechnic Institute
Paul B. Crilly
University of Tennessee
Janet C. Rutledge
University of Maryland at Baltimore
Solutions Manual to accompany
COMMUNICATION SYSTEMS: AN INTRODUCTION TO SIGNALS AND NOISE IN ELECTRICAL COMMUNICATION,
FOURTH EDITION
A. BRUCE CARLSON, PAUL B. CRILLY, AND JANET C. RUTLEDGE
Published by McGraw-Hill Higher Education, an imprint of The McGraw-Hill Companies, Inc., 1221 Avenue of the Americas,
New York, NY 10020. Copyright © The McGraw-Hill Companies, Inc., 2002, 1986, 1975, 1968. All rights reserved.
The contents, or parts thereof, may be reproduced in print form solely for classroom use with COMMUNICATION SYSTEMS: AN
INTRODUCTION TO SIGNALS AND NOISE IN ELECTRICAL COMMUNICATION, provided such reproductions bear copyright
notice, but may not be reproduced in any other form or for any other purpose without the prior written consent of The McGraw-Hill
Companies, Inc., including, but not limited to, in any network or other electronic storage or transmission, or broadcast for distance
learning.
www.mhhe.com
2-1
Chapter 2
2.1-1
0
0
0
/2
2 ( )
/2
0
sinc( )
0 otherwise
jj
T
j m n f t j
n T
Ae n mAe
c e dt Ae m n
T
φφ
π φ−
−
 =
= = − = 

∫
2.1-2
0 0
0
0
/ 4 / 2
0 / 4
0 0 0
( ) 0
2 2 2 2
cos ( )cos sin
2
T T
n
T
c v t
nt nt A n
c A dt A dt
T T T n
π π π
π
=
= + − =∫ ∫
n 0 1 2 3 4 5 6 7
nc 0 2 /A π 0 2 / 3A π 0 2 / 5A π 0 2 / 7A π
arg nc 0 180± ° 0 180± °
2.1-3
0
0
/2
20
0 0 0
( ) / 2
2 2 2
cos sin (cos 1)
( )
T
n
c v t A
At nt A A
c A dt n n
T T T n n
π
π π
π π
= =
 
= − = − − 
 
∫
n 0 1 2 3 4 5 6
nc 0.5A 0.2A 0 0.02A 0 0.01A 0
arg nc 0 0 0 0
2.1-4
0 / 2
0
0
0 0
2 2
cos 0
T t
c A
T T
π
= =∫ (cont.)
2-2
( ) ( )
[ ]
0
0
/2
/2
0 0
0
0 0 0 0 0 0 0
sin 2 / sin 2 /2 2 2 2
cos cos
4( ) / 4( ) /
/ 2 1
sinc(1 ) sinc(1 )
0 otherwise2
T
T
n
n t T n t Tt nt A
c A dt
T T T T n T n T
A nA
n n
π π π ππ π
π π π π
− + 
= = + 
− + 
= ±
= − + + = 

∫
2.1-5
0
0
/ 2
0
0 0
( ) 0
2 2
sin (1 cos )
T
n
c v t
nt A
c j A dt j n
T T n
π
π
π
= =
= − = − −∫
n 1 2 3 4 5
nc 2 /A π 0 2 / 3A π 2 / 5A π
arg nc 90− ° 90− ° 90− °
2.1-6
0 ( ) 0c v t= =
( ) ( )
[ ]
0
0
/2
/2
0 0
0
0 0 0 0 0 0 0
sin 2 / sin 2 /2 2 2 2
sin sin
4( )/ 4( )/
/ 2 1
sinc(1 ) sinc(1 )
0 otherwise2
T
T
n
n t T n t Tt nt A
c j A dt j
T T T T n T n T
jA nA
j n n
π π π ππ π
π π π π
− + 
= − = − − 
− + 
= ±
= − − − + = 

∫
m
2.1-7
]
0 0
0 0
0
/ 2
0 / 2
0
1
( ) ( )
T T
jn t jn t
n
T
c v t e dt v t e dt
T
ω ω− −= +
∫ ∫
0 0
0 0 0 0
0
0
0
/ 2
/ 2
0
/ 2 0
/ 2
0
where ( ) ( /2)
( )
T T
jn t jn jn T
T
T
jn tjn
v t e dt v T e e d
e v t e dt
ω ω λ ω
ωπ
λ λ− − −
−
= +
= −
∫ ∫
∫
since 1 for even , 0 for evenjn
ne n c nπ
= =
2-3
2.1-8
2 2 2 2 2 2
0 0 0 0 0 0 0 0
1
0
2
2 2 2 2
2
2 2 2 2 2 2
2 2 sinc 2 sinc2 2 sinc3
1
where 4
1 1 1 3
1 2sinc 2sinc 2sinc 0.23
16 4 2 4
2 1 1 3 5 3 7
1 2sinc 2sinc 2sinc 2sinc 2sinc 2sinc
16 4 2 4 4 2 4
n
n
P c c Af Af f Af f Af f
f
A
f P A
A
f P
τ τ τ τ τ τ τ
τ
τ
τ
∞
=
= + = + + + +
=
 
> = + + + = 
 
 
> = + + + + + +

∑ L
2
2
2 2 2
0.24
1 1 1
1 2sinc 2sinc 0.21
2 16 4 2
A
A
f P A
τ
=

 
> = + + =  
2.1-9
0 0
0
2
2 2
/ 2 / 2
/ 2 0
0 0 0 0
2 2 2
2 2 2
0 02 2 2
0 even
2
odd
n
41 2 4 1
a) 1 1
3
4 4 4
2 2 2 0.332 so / 99.6%
9 25
8 8 8
b) ( ) cos cos3 cos5
9 25
n
T T
T
n
c
n
t t
P dt dt
T T T T
P P P
v t t t
π
π π π
ω ω ω
π π π
−


=  
 
 
   
= − = − =   
  
     
′ ′= + + = =     
     
′ = + +
∫ ∫
0t
2.1-10
( )
0
0
2 2 2
/ 2 2
/ 2
0
0 even
2
odd
1 2 2 2
a) 1 1 2 0.933 so / 93.3%
3 5
n
T
T
n
c j
n
n
P dt P P P
T
π
π π π−


= −

      
′ ′= = = + + = =      
       
∫
(cont.)
2-4
( ) ( ) ( )
( ) ( ) ( )
0 0 0
0 0 0
4 4 4
b) ( ) cos 90 cos 3 90 cos 5 90
3 5
4 4 4
sin sin 3 sin 5
3 5
v t t t t
t t t
ω ω ω
π π π
ω ω ω
π π π
′ = − ° + − ° + − °
= + +
2.1-11
0
2
0
0 0
1/2 01 1
1/2 03
T
n
nt
P dt c
n nT T π
=  
= = =  
≠ 
∫
4 4
4 4 4
odd
2 2 1 1 1 1
2 2
1 3 5 3n
P
nπ π
∞
     
= = + + + =     
     
∑ L
2 2
2 2 2
1 1 1 4 1 1
Thus,
1 2 3 2 3 4 6
π π 
+ + + = − = 
 
L
2.1-12
0
2
/ 2
20
0 0
0 even2 4 1
1
(2/ ) odd3
T
n
nt
P dt c
n nT T π
  
= − = =  
 
∫
2 2
2 2 2 2
1
1 1 1 2 1 1 1 1
2
2 2 4 4 1 2 3 3n
P
nπ π
∞
=
     
= + = + + + + =     
     
∑ L
4 4
4 4 4 4
1 1 1 1
Thus,
1 3 5 2 2 3 96
π π
+ + + = =
⋅
L
2.2-1
( )
( )
( )
( )
[ ]
/ 2
0
( ) 2 cos cos2
sin 2 sin 2
2 22 sinc( 1/2) sinc( 1/2)
22 2 2 2
t
V f A ftdt
f f
A
A f f
f f
τ
π π
τ τ
π π
τ τ
π
π
τ
τ τ
π π
τ
τ τ
π π
+
+
=
 
− 
= + = − + + 
− 
 
∫
(cont.)
2-5
2.2-2
( )
( )
( )
( )
[ ]
/ 2
0
2 2
2 2
2
( ) 2 sin cos2
sin 2 sin 2
2 22 sinc( 1) sinc( 1)
22 2 2 2
t
V f j A ftdt
f f
A
j A j f f
f f
τ
π π
τ τ
π π
τ τ
π
π
τ
τ τ
π π
τ
τ τ
π π
+
+
= −
 
− 
= − − = − − − + 
− 
 
∫
2.2-3
2 2
20
2
( ) 2 cos 2sin 1 1 sinc
( ) 2
t A
V f A A tdt A f
τ τ ωτ
ω τ τ
τ ωτ
    
= − = − + =    
    
∫
2.2-4
20
2
( ) 2 sin (sin cos )
( )
(sinc2 cos2 )
t A
V f j A tdt j
A
j f f
f
τ τ
ω ωτ ωτ ωτ
τ ωτ
τ π τ
π
= − = − −
= − −
∫
2.2-5
2
2
2
1
( ) sinc2
2 2
1 1 1
sinc2
2 2 4 2
f
v t Wt
W W
f
Wt dt df df
W W W W
∞ ∞ ∞
−∞ −∞ −∞
 
= ↔ Π 
 
 
= Π = = 
 ∫ ∫ ∫
2-6
2.2-6
( )
2 2 2
2
2 20 0
2
2 arctan
2 (2 )
W
bt A A A W
E Ae dt E df
b b f b b
π
π π
∞
−
′= = = =
+∫ ∫
50% / 22 2
arctan
84% 2 /
W bE W
W bE b
ππ
ππ
=′ 
= = 
=
2.2-7
( )
( ) ( ) ( ) ( )
( ) ( ) ( ) ( )
j t
j t
v t w t dt v t W f e df dt
W f v t e dt df W f V f df
ω
ω
∞ ∞ ∞
−∞ −∞ −∞
∞ ∞ ∞
− −
−∞ −∞ −∞
 =
  
 = = −
  
∫ ∫ ∫
∫ ∫ ∫
22
( ) *( ) when ( ) is real, so ( ) ( ) *( ) ( )V f V f v t v t dt V f V f df V f df
∞ ∞ ∞
−∞ −∞ −∞
− = = =∫ ∫ ∫
2.2-8
2 2 2 ( )
( ) ( ) ( ) ( )
Let ( ) ( ) so ( ) ( ) and ( ) ( )
Hence ( ) ( ) ( ) ( )
j ft j ft j f t
w t e dt w t e dt w t e dt W f
z t w t Z f W f W f Z f
v t z t dt V f Z f df
π π π
∗ ∗
∞ ∞ ∞
∗ − − − ∗
−∞ −∞ −∞
∗ ∗ ∗
∞ ∞
−∞ −∞
   = = =
      
= = − = −
= −
∫ ∫ ∫
∫ ∫
2.2-9
1
sinc so sinc
2 2
( ) sinc ( ) for
2 2
t f
A Af At
A A A
t f
v t V f A
τ τ
τ τ
   
Π ↔ ↔ Π   
   
 
= ↔ = Π = 
 
2.2-10
[ ]
[ ]
[ ]
cos sinc( 1/2) sinc( 1/2)
2
( )
so sinc( 1/2) sinc( 1/2) cos cos
2
Let and 2 ( ) sinc(2 1/2) sinc(2 1/2)
t t B
B f f
B f f f f
t t B B
B A W z t AW Wt Wt
π τ
τ τ
τ τ
τ π π
τ τ
τ τ τ τ
τ
 
Π ↔ − + + 
 
− −   
− + + ↔ Π = Π   
   
= = ⇒ = − + +
2.2-11
[ ]
[ ]
[ ]
2
sin sinc( 1) sinc( 1)
2
2 ( ) 2
so sinc( 1) sinc( 1) sin sin
2
Let and 2 ( ) sinc(2 1) sinc(2 1)
t t B
B j f f
B f f f f
j t t B B
B jA W z t AW Wt Wt
π τ
τ τ
τ τ
τ π π
τ τ
τ τ τ τ
τ
 
Π ↔ − − + + 
 
− −   
− − + + ↔ Π = − Π   
   
= − = ⇒ = − + +
2-7
2.2-12
( )
( )
( )
2
2 2 2 2 2 2
2
2
2
22 2 0 2 2
2
2 30 2 2
2 4 /
(2 ) (2 ) (2 )
1 /
2
2
1 1
Thus,
2 2 4
b t a t
a t
b a a
e e
b f a f a f
a a df
e dt df
a a f a f
dx
a a aa x
π
π
π π
π π π
π
π π
π π
π
− −
∞ ∞ ∞−
−∞ −∞
∞
↔ ⇒ ↔ =
+ + +
 
= = =  
+   +
 
= = 
 +
∫ ∫ ∫
∫
2.3-1
( ) ( ) ( ) where v( ) ( / ) sinc
so Z( ) ( ) ( ) 2 sinc cos2j T j T
z t v t T v t T t A t A f
f V f e V f e A f fTω ω
τ τ τ
τ τ π−
= − + + = Π ↔
= + =
2.3-2
2 2
( ) ( 2 ) 2 ( ) ( 2 ) where v( ) ( / ) sinc
( ) ( ) ( ) ( ) 2 (sinc )(1 cos4 )j T j T
z t v t T v t v t T t a t A f
Z f V f e V f V f e A f fTω ω
τ τ τ
τ τ π−
= − + + + = Π ↔
= + + = +
2.3-3
2 2
( ) ( 2 ) 2 ( ) ( 2 ) where ( ) ( / ) sinc
( ) ( ) 2 ( ) ( ) 2 (sinc )(cos4 1)j T j T
z t v t T v t v t T v t a t A f
Z f V f e V f V f e A f fTω ω
τ τ τ
τ τ π−
= − − + + = Π ↔
= − + = −
2.3-4
/ 2
/ 2
( ) ( )
2
( ) 2 sinc2 ( ) sincj T j T
t T t T
v t A B A
T T
V f AT fTe B A T fTeω ω− −
− −   
= Π + − Π   
   
= + −
2-8
2.3-5
2 2
2 2
( ) ( )
4 2
( ) 4 sinc4 2( ) sinc2j T j T
t T t T
v t A B A
T T
V f AT fTe B A T fTeω ω− −
− −   
= Π + − Π   
   
= + −
2.3-6
/ /
1
Let ( ) ( ) ( ) ( / )
1
Then ( ) [ ( / )] ( / ) so ( ) ( ) ( / )d dj t a j t a
d d
w t v at W f V f a
a
z t v a t t a w t t a Z f W f e V f a e
a
ω ω− −
= ↔ =
= − = − = =
2.3-7
2 ( )
( ) ( ) ( ) ( )c c cj t j t j f f tj t
cv t e v t e e dt v t e dt V f fω ω πω
∞ ∞ − −−
−∞ −∞
  = = = −  ∫ ∫F
2.3-8
[ ]
( ) ( / )cos with 2 /
( ) sinc( ) sinc( ) sinc( 1/2) sinc( 1/2)
2 2 2
c c c
c c
v t A t t f
A A A
V f f f f f f f
τ ω ω π π τ
τ τ τ
τ τ τ τ
= Π = =
= − + + = − + +
2.3-9
[ ]
/ 2 /2
( ) ( / )cos( /2) with 2 2 /
( ) sinc( ) sinc( )
2 2
sinc( 1) sinc( 1)
2
c c c
j j
c c
v t A t t f
e e
V f A f f A f f
A
j f f
π π
τ ω π ω π π τ
τ τ τ τ
τ
τ τ
−
= Π − = =
= − + +
= − − − +
2.3-10
2
2 2 2 2
2
( ) ()cos ( )
1 (2 )
1 1
( ) ( ) ( )
2 2 1 4 ( ) 1 4 ( )
t
c
c c
c c
A
z t v t t v t Ae
f
A A
Z f V f f V f f
f f f f
ω
π
π π
−
= = ↔
+
= − + + = +
+ − + +
2.3-11
/ 2 / 2
( ) ()cos( /2) ( ) for 0
1 2
/ 2 / 2
( ) ( ) ( )
2 2 1 2 ( ) 1 2 ( )
/ 2 / 2
2 ( ) 2 ( )
t
c
j j
c c
c c
c c
A
z t v t t v t Ae t
j f
e e jA jA
Z f V f f V f f
j f f j f f
A A
j f f j f f
π π
ω π
π
π π
π π
−
−
= − = ≥ ↔
+
−
= − + + = +
+ − + +
= −
− − − +
2-9
2.3-12
( )
2
2
( ) ( ) ( ) 2 sinc2
sin2 2
( ) 2 (2 ) cos2 2 sin2
2 (2 )
1
( ) ( ) sinc2 cos2
2
A t
v t t z t z t A f
d d f A
Z f A f f f
df df f f
d jA
V f Z f f f
j df f
τ
τ τ
π τ
πτ π τ πτ π τ
π τ π τ
τ π τ
π π
 
= = Π ↔ 
 
 
 = = −   
 
−
= = −
−
2.3-13
2 2
22 2 2 2
2
( ) ( ) ( )
(2 )
1 2 2
( )
2 (2 ) (2 )
b t Ab
z t tv t v t Ae
b f
d Ab j Abf
Z f
j df b f b f
π
π π π
−
= = ↔
+
 
= = 
− +    + 
2.3-14
( ) [ ]
2
2 3
( ) ( ) ( ) for 0
2
1 2
( )
22 2
t A
z t t v t v t Ae t
b j f
d A A
Z f
df b j fj f b j f
π
ππ π
−
= = ≥ ↔
+
 
= = +− + 
2.3-15
2 2
2 2
2 2
2 2
( ) ( / )
2 ( ) ( / )
( ) ( / )
( ) ( / )
1
( ) ( )
2
( ) ( ) 2
1
( ) ( )
2
Both results are equivalent to
bt f b
bt f b
bt f b
bt f b
v t e V f e
b
d j f
a v t b te e
dt b
d f
b te V f e
j df jb
bte jf e
π π
π π
π π
π π
π
π
π
− −
− −
− −
− −
= ↔ =
= − ↔
↔ =
−
↔ −
2.4-1
2
0
2
0
( ) 0 0
0 2
2
2 2
t
y t t
At
A d t
A d A t
λ λ
λ λ
= <
= = < <
= = >
∫
∫
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communication-systems-4th-edition-2002-carlson-solution-manual

  • 1. Solutions Manual to accompany Communication Systems An Introduction to Signals and Noise in Electrical Communication Fourth Edition A. Bruce Carlson Rensselaer Polytechnic Institute Paul B. Crilly University of Tennessee Janet C. Rutledge University of Maryland at Baltimore
  • 2. Solutions Manual to accompany COMMUNICATION SYSTEMS: AN INTRODUCTION TO SIGNALS AND NOISE IN ELECTRICAL COMMUNICATION, FOURTH EDITION A. BRUCE CARLSON, PAUL B. CRILLY, AND JANET C. RUTLEDGE Published by McGraw-Hill Higher Education, an imprint of The McGraw-Hill Companies, Inc., 1221 Avenue of the Americas, New York, NY 10020. Copyright © The McGraw-Hill Companies, Inc., 2002, 1986, 1975, 1968. All rights reserved. The contents, or parts thereof, may be reproduced in print form solely for classroom use with COMMUNICATION SYSTEMS: AN INTRODUCTION TO SIGNALS AND NOISE IN ELECTRICAL COMMUNICATION, provided such reproductions bear copyright notice, but may not be reproduced in any other form or for any other purpose without the prior written consent of The McGraw-Hill Companies, Inc., including, but not limited to, in any network or other electronic storage or transmission, or broadcast for distance learning. www.mhhe.com
  • 3. 2-1 Chapter 2 2.1-1 0 0 0 /2 2 ( ) /2 0 sinc( ) 0 otherwise jj T j m n f t j n T Ae n mAe c e dt Ae m n T φφ π φ− −  = = = − =   ∫ 2.1-2 0 0 0 0 / 4 / 2 0 / 4 0 0 0 ( ) 0 2 2 2 2 cos ( )cos sin 2 T T n T c v t nt nt A n c A dt A dt T T T n π π π π = = + − =∫ ∫ n 0 1 2 3 4 5 6 7 nc 0 2 /A π 0 2 / 3A π 0 2 / 5A π 0 2 / 7A π arg nc 0 180± ° 0 180± ° 2.1-3 0 0 /2 20 0 0 0 ( ) / 2 2 2 2 cos sin (cos 1) ( ) T n c v t A At nt A A c A dt n n T T T n n π π π π π = =   = − = − −    ∫ n 0 1 2 3 4 5 6 nc 0.5A 0.2A 0 0.02A 0 0.01A 0 arg nc 0 0 0 0 2.1-4 0 / 2 0 0 0 0 2 2 cos 0 T t c A T T π = =∫ (cont.)
  • 4. 2-2 ( ) ( ) [ ] 0 0 /2 /2 0 0 0 0 0 0 0 0 0 0 sin 2 / sin 2 /2 2 2 2 cos cos 4( ) / 4( ) / / 2 1 sinc(1 ) sinc(1 ) 0 otherwise2 T T n n t T n t Tt nt A c A dt T T T T n T n T A nA n n π π π ππ π π π π π − +  = = +  − +  = ± = − + + =   ∫ 2.1-5 0 0 / 2 0 0 0 ( ) 0 2 2 sin (1 cos ) T n c v t nt A c j A dt j n T T n π π π = = = − = − −∫ n 1 2 3 4 5 nc 2 /A π 0 2 / 3A π 2 / 5A π arg nc 90− ° 90− ° 90− ° 2.1-6 0 ( ) 0c v t= = ( ) ( ) [ ] 0 0 /2 /2 0 0 0 0 0 0 0 0 0 0 sin 2 / sin 2 /2 2 2 2 sin sin 4( )/ 4( )/ / 2 1 sinc(1 ) sinc(1 ) 0 otherwise2 T T n n t T n t Tt nt A c j A dt j T T T T n T n T jA nA j n n π π π ππ π π π π π − +  = − = − −  − +  = ± = − − − + =   ∫ m 2.1-7 ] 0 0 0 0 0 / 2 0 / 2 0 1 ( ) ( ) T T jn t jn t n T c v t e dt v t e dt T ω ω− −= + ∫ ∫ 0 0 0 0 0 0 0 0 0 / 2 / 2 0 / 2 0 / 2 0 where ( ) ( /2) ( ) T T jn t jn jn T T T jn tjn v t e dt v T e e d e v t e dt ω ω λ ω ωπ λ λ− − − − = + = − ∫ ∫ ∫ since 1 for even , 0 for evenjn ne n c nπ = =
  • 5. 2-3 2.1-8 2 2 2 2 2 2 0 0 0 0 0 0 0 0 1 0 2 2 2 2 2 2 2 2 2 2 2 2 2 2 sinc 2 sinc2 2 sinc3 1 where 4 1 1 1 3 1 2sinc 2sinc 2sinc 0.23 16 4 2 4 2 1 1 3 5 3 7 1 2sinc 2sinc 2sinc 2sinc 2sinc 2sinc 16 4 2 4 4 2 4 n n P c c Af Af f Af f Af f f A f P A A f P τ τ τ τ τ τ τ τ τ τ ∞ = = + = + + + + =   > = + + + =      > = + + + + + +  ∑ L 2 2 2 2 2 0.24 1 1 1 1 2sinc 2sinc 0.21 2 16 4 2 A A f P A τ =    > = + + =   2.1-9 0 0 0 2 2 2 / 2 / 2 / 2 0 0 0 0 0 2 2 2 2 2 2 0 02 2 2 0 even 2 odd n 41 2 4 1 a) 1 1 3 4 4 4 2 2 2 0.332 so / 99.6% 9 25 8 8 8 b) ( ) cos cos3 cos5 9 25 n T T T n c n t t P dt dt T T T T P P P v t t t π π π π ω ω ω π π π −   =           = − = − =             ′ ′= + + = =            ′ = + + ∫ ∫ 0t 2.1-10 ( ) 0 0 2 2 2 / 2 2 / 2 0 0 even 2 odd 1 2 2 2 a) 1 1 2 0.933 so / 93.3% 3 5 n T T n c j n n P dt P P P T π π π π−   = −         ′ ′= = = + + = =               ∫ (cont.)
  • 6. 2-4 ( ) ( ) ( ) ( ) ( ) ( ) 0 0 0 0 0 0 4 4 4 b) ( ) cos 90 cos 3 90 cos 5 90 3 5 4 4 4 sin sin 3 sin 5 3 5 v t t t t t t t ω ω ω π π π ω ω ω π π π ′ = − ° + − ° + − ° = + + 2.1-11 0 2 0 0 0 1/2 01 1 1/2 03 T n nt P dt c n nT T π =   = = =   ≠  ∫ 4 4 4 4 4 odd 2 2 1 1 1 1 2 2 1 3 5 3n P nπ π ∞       = = + + + =            ∑ L 2 2 2 2 2 1 1 1 4 1 1 Thus, 1 2 3 2 3 4 6 π π  + + + = − =    L 2.1-12 0 2 / 2 20 0 0 0 even2 4 1 1 (2/ ) odd3 T n nt P dt c n nT T π    = − = =     ∫ 2 2 2 2 2 2 1 1 1 1 2 1 1 1 1 2 2 2 4 4 1 2 3 3n P nπ π ∞ =       = + = + + + + =            ∑ L 4 4 4 4 4 4 1 1 1 1 Thus, 1 3 5 2 2 3 96 π π + + + = = ⋅ L 2.2-1 ( ) ( ) ( ) ( ) [ ] / 2 0 ( ) 2 cos cos2 sin 2 sin 2 2 22 sinc( 1/2) sinc( 1/2) 22 2 2 2 t V f A ftdt f f A A f f f f τ π π τ τ π π τ τ π π τ τ τ π π τ τ τ π π + + =   −  = + = − + +  −    ∫ (cont.)
  • 7. 2-5 2.2-2 ( ) ( ) ( ) ( ) [ ] / 2 0 2 2 2 2 2 ( ) 2 sin cos2 sin 2 sin 2 2 22 sinc( 1) sinc( 1) 22 2 2 2 t V f j A ftdt f f A j A j f f f f τ π π τ τ π π τ τ π π τ τ τ π π τ τ τ π π + + = −   −  = − − = − − − +  −    ∫ 2.2-3 2 2 20 2 ( ) 2 cos 2sin 1 1 sinc ( ) 2 t A V f A A tdt A f τ τ ωτ ω τ τ τ ωτ      = − = − + =          ∫ 2.2-4 20 2 ( ) 2 sin (sin cos ) ( ) (sinc2 cos2 ) t A V f j A tdt j A j f f f τ τ ω ωτ ωτ ωτ τ ωτ τ π τ π = − = − − = − − ∫ 2.2-5 2 2 2 1 ( ) sinc2 2 2 1 1 1 sinc2 2 2 4 2 f v t Wt W W f Wt dt df df W W W W ∞ ∞ ∞ −∞ −∞ −∞   = ↔ Π      = Π = =   ∫ ∫ ∫
  • 8. 2-6 2.2-6 ( ) 2 2 2 2 2 20 0 2 2 arctan 2 (2 ) W bt A A A W E Ae dt E df b b f b b π π π ∞ − ′= = = = +∫ ∫ 50% / 22 2 arctan 84% 2 / W bE W W bE b ππ ππ =′  = =  = 2.2-7 ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) j t j t v t w t dt v t W f e df dt W f v t e dt df W f V f df ω ω ∞ ∞ ∞ −∞ −∞ −∞ ∞ ∞ ∞ − − −∞ −∞ −∞  =     = = −    ∫ ∫ ∫ ∫ ∫ ∫ 22 ( ) *( ) when ( ) is real, so ( ) ( ) *( ) ( )V f V f v t v t dt V f V f df V f df ∞ ∞ ∞ −∞ −∞ −∞ − = = =∫ ∫ ∫ 2.2-8 2 2 2 ( ) ( ) ( ) ( ) ( ) Let ( ) ( ) so ( ) ( ) and ( ) ( ) Hence ( ) ( ) ( ) ( ) j ft j ft j f t w t e dt w t e dt w t e dt W f z t w t Z f W f W f Z f v t z t dt V f Z f df π π π ∗ ∗ ∞ ∞ ∞ ∗ − − − ∗ −∞ −∞ −∞ ∗ ∗ ∗ ∞ ∞ −∞ −∞    = = =        = = − = − = − ∫ ∫ ∫ ∫ ∫ 2.2-9 1 sinc so sinc 2 2 ( ) sinc ( ) for 2 2 t f A Af At A A A t f v t V f A τ τ τ τ     Π ↔ ↔ Π          = ↔ = Π =    2.2-10 [ ] [ ] [ ] cos sinc( 1/2) sinc( 1/2) 2 ( ) so sinc( 1/2) sinc( 1/2) cos cos 2 Let and 2 ( ) sinc(2 1/2) sinc(2 1/2) t t B B f f B f f f f t t B B B A W z t AW Wt Wt π τ τ τ τ τ τ π π τ τ τ τ τ τ τ   Π ↔ − + +    − −    − + + ↔ Π = Π        = = ⇒ = − + + 2.2-11 [ ] [ ] [ ] 2 sin sinc( 1) sinc( 1) 2 2 ( ) 2 so sinc( 1) sinc( 1) sin sin 2 Let and 2 ( ) sinc(2 1) sinc(2 1) t t B B j f f B f f f f j t t B B B jA W z t AW Wt Wt π τ τ τ τ τ τ π π τ τ τ τ τ τ τ   Π ↔ − − + +    − −    − − + + ↔ Π = − Π        = − = ⇒ = − + +
  • 9. 2-7 2.2-12 ( ) ( ) ( ) 2 2 2 2 2 2 2 2 2 2 22 2 0 2 2 2 2 30 2 2 2 4 / (2 ) (2 ) (2 ) 1 / 2 2 1 1 Thus, 2 2 4 b t a t a t b a a e e b f a f a f a a df e dt df a a f a f dx a a aa x π π π π π π π π π π π π π − − ∞ ∞ ∞− −∞ −∞ ∞ ↔ ⇒ ↔ = + + +   = = =   +   +   = =   + ∫ ∫ ∫ ∫ 2.3-1 ( ) ( ) ( ) where v( ) ( / ) sinc so Z( ) ( ) ( ) 2 sinc cos2j T j T z t v t T v t T t A t A f f V f e V f e A f fTω ω τ τ τ τ τ π− = − + + = Π ↔ = + = 2.3-2 2 2 ( ) ( 2 ) 2 ( ) ( 2 ) where v( ) ( / ) sinc ( ) ( ) ( ) ( ) 2 (sinc )(1 cos4 )j T j T z t v t T v t v t T t a t A f Z f V f e V f V f e A f fTω ω τ τ τ τ τ π− = − + + + = Π ↔ = + + = + 2.3-3 2 2 ( ) ( 2 ) 2 ( ) ( 2 ) where ( ) ( / ) sinc ( ) ( ) 2 ( ) ( ) 2 (sinc )(cos4 1)j T j T z t v t T v t v t T v t a t A f Z f V f e V f V f e A f fTω ω τ τ τ τ τ π− = − − + + = Π ↔ = − + = − 2.3-4 / 2 / 2 ( ) ( ) 2 ( ) 2 sinc2 ( ) sincj T j T t T t T v t A B A T T V f AT fTe B A T fTeω ω− − − −    = Π + − Π        = + −
  • 10. 2-8 2.3-5 2 2 2 2 ( ) ( ) 4 2 ( ) 4 sinc4 2( ) sinc2j T j T t T t T v t A B A T T V f AT fTe B A T fTeω ω− − − −    = Π + − Π        = + − 2.3-6 / / 1 Let ( ) ( ) ( ) ( / ) 1 Then ( ) [ ( / )] ( / ) so ( ) ( ) ( / )d dj t a j t a d d w t v at W f V f a a z t v a t t a w t t a Z f W f e V f a e a ω ω− − = ↔ = = − = − = = 2.3-7 2 ( ) ( ) ( ) ( ) ( )c c cj t j t j f f tj t cv t e v t e e dt v t e dt V f fω ω πω ∞ ∞ − −− −∞ −∞   = = = −  ∫ ∫F 2.3-8 [ ] ( ) ( / )cos with 2 / ( ) sinc( ) sinc( ) sinc( 1/2) sinc( 1/2) 2 2 2 c c c c c v t A t t f A A A V f f f f f f f τ ω ω π π τ τ τ τ τ τ τ τ = Π = = = − + + = − + + 2.3-9 [ ] / 2 /2 ( ) ( / )cos( /2) with 2 2 / ( ) sinc( ) sinc( ) 2 2 sinc( 1) sinc( 1) 2 c c c j j c c v t A t t f e e V f A f f A f f A j f f π π τ ω π ω π π τ τ τ τ τ τ τ τ − = Π − = = = − + + = − − − + 2.3-10 2 2 2 2 2 2 ( ) ()cos ( ) 1 (2 ) 1 1 ( ) ( ) ( ) 2 2 1 4 ( ) 1 4 ( ) t c c c c c A z t v t t v t Ae f A A Z f V f f V f f f f f f ω π π π − = = ↔ + = − + + = + + − + + 2.3-11 / 2 / 2 ( ) ()cos( /2) ( ) for 0 1 2 / 2 / 2 ( ) ( ) ( ) 2 2 1 2 ( ) 1 2 ( ) / 2 / 2 2 ( ) 2 ( ) t c j j c c c c c c A z t v t t v t Ae t j f e e jA jA Z f V f f V f f j f f j f f A A j f f j f f π π ω π π π π π π − − = − = ≥ ↔ + − = − + + = + + − + + = − − − − +
  • 11. 2-9 2.3-12 ( ) 2 2 ( ) ( ) ( ) 2 sinc2 sin2 2 ( ) 2 (2 ) cos2 2 sin2 2 (2 ) 1 ( ) ( ) sinc2 cos2 2 A t v t t z t z t A f d d f A Z f A f f f df df f f d jA V f Z f f f j df f τ τ τ π τ πτ π τ πτ π τ π τ π τ τ π τ π π   = = Π ↔       = = −      − = = − − 2.3-13 2 2 22 2 2 2 2 ( ) ( ) ( ) (2 ) 1 2 2 ( ) 2 (2 ) (2 ) b t Ab z t tv t v t Ae b f d Ab j Abf Z f j df b f b f π π π π − = = ↔ +   = =  − +    +  2.3-14 ( ) [ ] 2 2 3 ( ) ( ) ( ) for 0 2 1 2 ( ) 22 2 t A z t t v t v t Ae t b j f d A A Z f df b j fj f b j f π ππ π − = = ≥ ↔ +   = = +− +  2.3-15 2 2 2 2 2 2 2 2 ( ) ( / ) 2 ( ) ( / ) ( ) ( / ) ( ) ( / ) 1 ( ) ( ) 2 ( ) ( ) 2 1 ( ) ( ) 2 Both results are equivalent to bt f b bt f b bt f b bt f b v t e V f e b d j f a v t b te e dt b d f b te V f e j df jb bte jf e π π π π π π π π π π π − − − − − − − − = ↔ = = − ↔ ↔ = − ↔ − 2.4-1 2 0 2 0 ( ) 0 0 0 2 2 2 2 t y t t At A d t A d A t λ λ λ λ = < = = < < = = > ∫ ∫ To get the fully access of the document please click here.