to accompany
Communication
Systems
An Introduction to Signals and Noise in
Electrical Communication
Fourth Edition
A. Bruce Carlson
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Rensselaer Polytechnic Institute
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Paul B. Crilly rp rp
University of Tennessee rp rp
Janet C. Rutledge rp rp
University of Maryland at Baltimore
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,Solutions Manual to accompany
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COMMUNICATION SYSTEMS: AN INTRODUCTION TO SIGNALS AND NOISE IN ELECTRICAL COMMUNICATION,FOUR
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TH EDITION
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A. BRUCE CARLSON, PAUL B. CRILLY, AND JANET C. RUTLEDGE
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Published by McGraw-Hill Higher Education, an imprint of The McGraw-
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Hill Companies, Inc., 1221 Avenue of the Americas,New York, NY 10020. Copyright © The McGraw-
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Hill Companies, Inc., 2002, 1986, 1975, 1968. All rights reserved.
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The contents, or parts thereof, may be reproduced in print form solely for classroom use with COMMUNICATION SYSTEMS: AN IN
rp rp rp rp rp rp rp rp rp rp rp rp rp rp rp rp rp rp rp
TRODUCTION TO SIGNALS AND NOISE IN ELE CTRICAL COMMUNICATION, provided such reproductions bear copyrightnotic
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e, but may not be reproduced in any other form or for any other purpose without the prior written consent of The McGraw-
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Hill Companies, Inc., including, but not limited to, in any network or other electronic storage or transmission, or broadcast for distance
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learning.
www.mhhe.com
,Chapter 2 rp
2.1-1
jf Ae jf n =m
cn =Ae dt =Ae sinc(m−n) =
+e
T0rp/2rp rp
j2pr p (rpm−nrp)frp 0tr p p
r rp rp
rp
r p
jf rp rp rp
−rpT0r p /2rp
T0 0 otherwise
2.1-2
c0 v(t) =0
T 2p nt T0 /2 2p nt 2A p n
c = dt + dt = sin
rp rp rp r p rp
2 Acos
rp
(− A)cos
rp rp rp rp pr rp
r p rp rp rp rp rp rp rp
T
n
0 T T /4
0
T pn 2 rprp rp rp
0rpr p 0 0
n 0 1 2 3 4 5 6 7
cn 0 2A/p
rp pr rp 0 2A/ 3p
rp pr rp 0 2A/ 5p
rp pr rp 0 2A/ 7prp pr rp
argcn rp
0 180 0 180
2.1-3
c0 = v(t) =A /2
r p r p r p rp rp
c =
2 2At 2p nt A A
r p T /2 rp 0rp rp rp rp rp
n
T0 0
A −
T0
cos
dt = sinp n − (cosp n −1)
rp
T0 pn (p n)2
rp
rp rp
rp rp rp
rp
r p
rp rp
n 0 1 2 3 4 5 6
cn 0.5A 0.2A 0 0.02A 0 0.01A 0
argcn rp
0 0 0 0
2.1-4
2
c =
rpr p rp
T0rp /2 r p
Acos
2p t rp r p
= (cont.)
0 rp
0
T rprp
0 T
0 0
2-1
, 22 2pt 2p nt 2A sin (p −p n ) 2t /T sin (p +p n)2t /T T0rp/ 2rp
Tr p /
rp rp rp r p rp rp rp rp rp rp rp rp
rprpr p rp
rp
dt =
0
cn Acos cos 0r p
+ 0
rp
=
rp
rp
T0 rprprp
T0 T0 T0 r p
4(p −p n) /T0 r p rp rp rp 4(p +p n) /T0 rp rp rp
0
A
0
= sinc(1−n)+ sinc(1+n) A/2 n =1
rp pr
rp rp rp rp rp rp p
r rp rp
=
0
r p
2 otherwise
2.1-5
c0 = v(t)2=0
rp T0 /2 rp
2p nt A rp
c =− j dt =− j
rp rp r p
rp
Asin (1− cosp n)
r p rp r p rp rp rp rp rp rp
n
T 0 T pn rpr p rp
0 0
n 1 2 3 4 5
cn 2A/p rp pr rp 0 2A/ 3p rp pr rp 2A/ 5p
rp pr rp
argcn rp
−90 −90 −90
2.1-6
c0 = v(t) =0
2A sin (p −p n ) 2t /T0 sin(p +p n )2t /T
rp rp rp
T0rprp/ 2rp
c =− j
2 r p
T /2 2p t 2p nt
dt =− j −
0rp
0
r p rp rp rp rp rp rp rp rp r p rp rp rp rp rp rp rp rp rprp
Asin sin rpr p
4(p −p n)/ T 4(p +p n)/ T
rp rp rp rp rp rpr p rp
n
T T T r p rp rp rp rp
T0 0
0 0
0
rprp
0 0
0
m jA/ 2 n =1
rpr p
A
=− j sinc(1−n) −sinc(1+n ) =
pr pr rp pr rp rp
rp rp pr rp rp rp
2 0 otherwise
2.1-7
1
c = T0 /2
r p − jnw0 t
rp
T0
− jnw 0t rp rp rp rp
p
r
n
T00 v(t)e dt +
rprp
v(t)e dt rp rp rp pr
T 0 /2 rpr p rp
T0rp/2 rp
− jnw l
v(t)e −jnw0 t dt v(l + T0 /2)e e− jnw
0rprprprprpr p T0rp/2rp
where rp
rp
rp
rp rp
rp pr0 r p rp rp0
dl
=
T 0
Trprp/rp
0
T0r p /2rp
=−e v(t)e− jnw0 t dt
jnprprprprpr p rp
rp
rp
2 rp pr
0
since ejnp =1 for even n, cn =0 for even n
pr r p r p rp rp
rprp
r p rp rp
2-2