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OFFICIAL SOLUTIONS MANUAL FOR COMMUNICATION SYSTEMS BY CARLSON, CRILLY & RUTLEDGE (4TH EDITION)

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Stop struggling with tough signal processing, modulation, and noise problems! This verified solutions manual provides step-by-step answers to every end-of-chapter problem in Carlson’s classic "Communication Systems" text. From Fourier analysis and AM/FM to digital communications and coding theory, you’ll see exactly how experts solve each problem—helping you check your work, master complex concepts, and ace your exams. Perfect for electrical engineering students who want higher grades and a deeper understanding of signals and noise. Get the edge your classmates wish they had!

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SolutionsmManualmtomaccompany
COMMUNICATIONmSYSTEMS:mANmINTRODUCTIONmTOmSIGNALSmANDmNOISEmINmELECTRICALmCOMMUNICA
TION,mFOURTHmEDITION
A.mBRUCEmCARLSON,mPAULmB.mCRILLY,mANDmJANETmC.mRUTLEDGE

PublishedmbymMcGraw-HillmHighermEducation,manmimprintmofmThemMcGraw-
HillmCompanies,mInc.,m1221mAvenuemofmthemAmericas,mNewmYork,mNYm 10020.m Copyrightm©mThemMcGraw-
HillmCompanies,mInc.,m2002,m1986,m1975,m1968.m Allmrightsmreserved.

Themcontents,mormpartsmthereof,mmaymbemreproducedminmprintmformmsolelymformclassroommusemwithm COMMUNICATIONmSYS
TEMS:mANmINTRODUCTIONmTOmSIGNALSmANDmNOISEmINmELEmCTRICALmCOMMUNICATION,mprovidedmsuchmreproduc
tionsmbearmcopyrightmnotice,mbutmmaymnotmbemreproducedminmanymothermformmormformanymothermpurposemwithoutmthempriormw
rittenmconsentmofmThemMcGraw-
Hillm Companies,mInc.,mincluding,mbutmnotmlimitedmto,minmanymnetworkmormothermelectronicmstoragemormtransmission,mormbroad
castmformdistancem learning.

www.mhhe.com

,Chapterm2

2.1-1  
Aejϕ
 Aemj nmm
cnm

Tm/
emj2πjϕm(mmnm)fm tmdtm
0
m2m
0 ϕ
Aem sinc(mmn)m
T0
T0m /
0 otherwise
2m


2.1-2




2m Tm0m0
c0m v(t) /m4m m2πnt T0m/2 m 2πntm 2Am πn
cm  Acosm dtmm (A)cosm dtm sinm
Tm T T πn 2
n


0
T
mm

/m4m
0
0 0 0


n 0 1 2 3 4 5 6 7
cn 0 2mAm/mπ 0 2mAm/m3π 0 2mAm/m5π 0 2mAm/m7π
argmcn 0 180 0 180


2.1-3




2
cm  T m/2m 2mAtm 2πnt A A

0

n
Tm 0  A m  cos m dtm sinπn m 2m (cosπmnm1)

T T πn
0  0m  0 (πmn)

n 0 1 2 3 4 5 6
cn 0.5A 0.2A 0 0.02A 0 0.01A 0
argmcn 0 0 0 0


2.1-4




2-1

, 2 T0m/2 m
cm  Acosm
2πmtm (cont.)
0
Tm
0
0 T
0 0




2-2

, 2/2 mm m Tm 2mAmsinmπmπmn2t
2πt 2πnt sinmπmπmn2tm/ T m/2m 0




cnm  0 Acos cos m/mT mT

dtm  0m

0m

T T T T  4(π
mπmn)m/mT0
 4(πmπn)/mT0 0
0 0m m
Am A / 2mn 1
 sinc(1mn)msinc(1mn)m
0 0 0m m m


m
2  0 otherwise

2.1-5




2 T0m/2m 2πnt Am
cm jm Asinm dtmjm (1cosπmn)
Tm
n
0 T πn
0 0


n 1 2 3 4 5
cn 2mAm/mπ 0 2mAm/m3π 2mAm/m5π
argmcn 90 90 90

2.1-6




2mAmsinmπmπmn2t
mm/mT0sinmπmπmn
T0m /2m
2 2πtm m2πntm
T0m/2m 2tm/mTm 
cnm j dtmjm m
Tm
m m m
Asin sinm 4(πmπmn)/mT
4(πmπmn)/
m m 0
0 T T T
mT
0 0 0
0 0 0
0m 
mAm mmjAm/m2 nm1
jm sinc(1nm)msinc(1n)m

2 m 0 otherwise

2.1-71
cm  2mT0m / jnω0mt
T0
jnω0t

n 0 v(t)me dtmTm0 /m2m v(t)e dtm
T0m

T0
v(t)ejnω0mtmdtm  T m/2 v(λmTm/2)mejnω0λmejnω0/mT20m
m dλ

0
where
T
m m /0m2 
0
0
T0m /m2m
emjnπm v(tm)ejnω0mtmdt

0
sincem emjnπm1m formevenmn,m cm 0m formevenmn
n




2-3

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