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Solutions Manual for Communication Systems: An Introduction to Signals and Noise in Electrical Communication, 4th Edition

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Facilitate your understanding and learning with this comprehensive Solutions Manual for "Communication Systems: An Introduction to Signals and Noise in Electrical Communication, 4th Edition." This manual provides detailed solutions to the end-of-chapter problems and exercises found in the textbook. Key Features: Comprehensive Solutions: Detailed solutions to problems covering various aspects of communication systems, signals, and noise. Step-by-Step Explanations: Clear explanations that help you understand the concepts and methods used in solving each problem. Concept Reinforcement: Reinforce your understanding of signal processing, modulation techniques, noise, and their applications in communication systems. Aligned with the Textbook: Solutions are aligned with the 4th edition of the textbook, ensuring accuracy and relevance. This Solutions Manual is an essential companion for students studying communication systems and professionals looking to deepen their understanding of signal processing and electrical communication concepts.

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Institution
Accompany Communication System 4th Ed
Course
Accompany Communication System 4th ed











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Uploaded on
October 23, 2024
Number of pages
315
Written in
2024/2025
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Exam (elaborations)
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Solutions Manual
to accompany


Communication
Systems
An Introduction to Signals and Noise in
Electrical Communication
Fourth Edition


A. Bruce Carlson
z z

RensselaerzPolytechniczInstitute

Paul B. Crilly
z z

UniversityzofzTennessee

Janet C. Rutledge
z z

UniversityzofzMarylandzatzBaltimore

,SolutionszManualztozaccompany
COMMUNICATIONzSYSTEMS:zANzINTRODUCTIONzTOzSIGNALSzANDzNOISEzINzELECTRICALzCOMMUNICATION,zFOUR
THzEDITION
A.zBRUCEzCARLSON,zPAULzB.zCRILLY,zANDzJANETzC.zRUTLEDGE

PublishedzbyzMcGraw-HillzHigherzEducation,zanzimprintzofzThezMcGraw-
HillzCompanies,zInc.,z1221zAvenuezofzthezAmericas,zNewzYork,zNYz10020.zCopyrightz©zThezMcGraw-
HillzCompanies,zInc.,z2002,z1986,z1975,z1968.z Allzrightszreserved.

Thezcontents,zorzpartszthereof,zmayzbezreproducedzinzprintzformzsolelyzforzclassroomzusezwithzCOMMUNICATIONzSYSTEMS:zANzI
NTRODUCTIONzTOzSIGNALSzANDzNOISEzINzELEzCTRICALzCOMMUNICATION,zprovidedz suchz reproductionszbearz copyrightzno
tice,zbutzmayznotzbezreproducedzinzanyzotherzformzorzforzanyzotherzpurposezwithoutzthezpriorzwrittenzconsentzofzThezMcGraw-
HillzCompanies,zInc.,zincluding,zbutznotzlimitedzto,zinzanyznetworkzorzotherzelectroniczstoragezorztransmission,zorzbroadcastzforzdistance
zlearning.


www.mhhe.com

,Chapterz2

2.1-1
 
Ae jf Aezjf nzm
cnz 
ef z dtz Aez sinc(mzzn)z
T0z/2z
j2p z (zmn z)fz tz j 0


T0
zT0z /2
0 otherwise
z



2.1-2




2 z 0
c0z v(t) T0z/z4z 2pznt T0z /2 z 2pzntz 2A z pzn
cz z  Acosz dtz (zA)cosz dtz  sinz

T0zz 

n 0 T




Tzz/ 4z
0
T pzn 2
0 0


n 0 1 2 3 4 5 6 7
cn 0 2zAz/zp 0 2zAz/z3p 0 2zAz/z5p 0 2zAz/z7p
argzcn 0 180 0 180


2.1-3




c0z z v(t)z A z/2 z
2
cz z 2zAtz 2pznt A A
 
T z/2z 0


n  A
T0 0  T0 
z cos dtz  sinpznzz





(cospznz1)
T0 pznz (pzn)2z
n 0 1 2 3 4 5 6
cn 0.5A 0.2A 0 0.02A 0 0.01A 0
argzcn 0 0 0 0


2.1-4




2 T0z /2 z 2pztz
czz z Acosz 0 (cont.)
T
0
zz 0 T
0 0



2-1

, 2z zzz Tz /2 2zAzsinzpz pzn  2tz/zT
2pt 2pznt sinzp pznz2tz/zT T0z/ 2z

cnz   Acos dtz  0z 
0
cos 0z
 
T0z z z T0 T0 T0z 4(pz pzn)z/zT0 4(p zpzn) /zT0 0
0
zAz

 sinc(1zzn)zzsinc(1zzn) Az/z2 nz1
z
2 0 otherwise

2.1-5




c0z z v(t)
2 z 0T0z /2 z 2pznt Az
cz zjz Asinz dtz zjz (1zcospzn)
Tzz 
n
0 T pzn
0 0


n 1 2 3 4 5
cn 2zAz/zp 0 2zAz/z3p 2zAz/z5p
argzcn 90 90 90

2.1-6




c0z z v(t)z 0
2zAzsinzpz pzn  2tz/zT0zz sinzp pzn z2tz/zTzz
z2 T0zz/ 2z
cz zj T z / 2z 2p tz 2pzntz
dtz zjz zz z 
0
Asinz sinz
n 
T0zz 0
T T T 4(pz pzn)/ zT 4(p pzn)/ zT 0 
0 0
0 0 0
0zz 
zAz mzjAz/z2 nz1
zjz sinc(1nz)zzsinc(1zn) 

2  0 otherwise

2.1-71
cz z zT0z /2z  jnw0zt
T0
 jnwz0t

n

T0zz 0 v(t)ze dtzz z
Tzz
v(t)e dtz
T0z/2 z
v(t)e zjnw0ztzdtz 
 v(l  T0 /2)ze e
0zzzzzz zjnwz lz z jnwz T z/2z
where 0
dl
0 0




T 0
Tzz/z
0
T0z /2z
ez jnpzzzzz v(tz)ezjnw0ztzdt
2

0

since ezjnpz 1z forzevenzn, cnzz0z forzevenzn

2-2

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