11/5/2010 1 ELECTRONIC COMMUNICATIONS SYSTEMS Chapter 3 Amplitude Modulation Transmission
Oct 07, 2014
11/5/20101
ELECTRONIC COMMUNICATIONSSYSTEMS
Chapter 3
Amplitude Modulation Transmission
11/5/20102
• BASEBAND COMMUNICATION: COMMUNICATION THATDOES NOT USE MODULATION (TRANSMIT INFORMATIONIN ITS ORIGINAL FORM) - NO SHIFT IN THERANGE OF FREQUENCIES OF THE SIGNAL.(NO FREQUENCY TRANSLATION)
• CARRIER COMMUNICATION: COMMUNICATION THATUSES MODULATION - SHIFTING OF THE RANGE OFFREQUENCIES IN THE SIGNAL.(FREQUENCY TRANSLATION)
• (AM, FM, PM, FSK, PSK, QAM, ……)
BASEBAND AND CARRIER COMMUNICATION
11/5/20103
• THE TERM BASEBAND IS USED TO DESIGNATE THEBAND OF FREQUENCIES OF THE SIGNAL DELIVEREDBY THE SOURCE
• TELEPHONY: BASEBAND IS THE AUDIO BAND (BAND OFVOICE SIGNALS) OCCUPYING 0 - 4000 Hz
• TELEVISION: BASEBAND IS THE VIDEO BAND (BAND OFVIDEO SIGNALS) OCCUPYING 0 - 6 MHz
• DIGITAL DATA/PCM (A-TO-D CONVERTION):USING BIPOLAR SIGNALING AT A RATE OF BITS/SEC,THE BASEBAND IS 0 - Hz
BASEBAND COMMUNICATION
0f0f
11/5/20104
• PULSE MODULATED SIGNALS SUCH AS:
• PAM (PULSE AMPLITUDE MODULATION)• PWM (PULSE WIDTH MODULATION)• PPM (PULSE POSITION MODULATION)• PCM (PULSE CODE MODULATION)
• DESPITE THE TERM MODULATION, THE ABOVE SIGNALSARE BASEBAND CODING SCHEMES AND THEY YIELDBASEBAND SIGNALS
BASEBAND COMMUNICATION
11/5/20105
• BASEBAND SIGNALS HAVE SIZABLE POWER AT LOWFREQUENCIES
• BASEBAND SIGNALS CANNOT BE TRANSMITTEDOVER A RADIO LINK (FREE SPACE)
• BASEBAND SIGNALS ARE SUITABLE FOR TRANSMISSIONOVER COPPER (PAIR OF WIRES, COAXIAL CABLE) ORGLASS (FIBER). EXAMPLES:
• LOCAL TELEPHONE COMMUNICATION• SHORT-HAUL PCM COMMUNICATION (BETWEEN
LOCAL EXCHANGES)
BASEBAND COMMUNICATION
11/5/20106
• MODULATION IS USED WHEN IT IS IMPRACTICAL TOPROPAGATE LOW-FREQUENCY BASEBAND SIGNALSOVER FREE SPACE
• MODULATION USES HIGH FREQUENCY CARRIERS TOACHIEVE SIMULTANEOUS TRANSMISSION WITH NOINTERFERENCE (MULTIPLEXING OF VARIOUSSIGNALS)
• MODULATION ALLOWS CONSTRUCTION OF SMALLANTENNAS (i.e. 1/4 WAVELENGTH)
MODULATION COMMUNICATION
11/5/20107
IN AMPLITUDE MODULATION, THE AMPLITUDE OF THEHIGH FREQUENCY CARRIER SIGNAL(UNMODULATED WAVE) IS MODULATED (VARIED)PROPORTIONAL TO THE INSTANTANEOUS AMPLITUDEOF THE MESSAGE BEARING SIGNAL (MODULATING WAVE) SUCH AS TO GENERATING AN ENVELOPE(MODULATED WAVE) WHICH CARRIES THEINFORMATION.
THE REPETITION RATE OF THE AM ENVELOPE EQUALSTHE FREQUENCY OF THE MODULATING SIGNAL.
AMPLITUDE MODULATIONAMPLITUDE MODULATION
11/5/20108
AM MODULATORS: NONLINEAR DEVICES (MIXER)WITH: TWO INPUTS, ONE OUTPUT
AMPLITUDE MODULATIONAMPLITUDE MODULATION
AM MODULATOR(NON LINEAR
DEVICE, MIXER,MULTIPLIER)
HIGH FREQUENCYCARRIER SIGNAL(UNMODULATED WAVE)
LOW FREQUENCYINFORMATION SIGNAL(MODULATING WAVE)
• SINGLE FREQUENCY WAVE (TONE)OR
• COMPLEX WAVE (MULTIPLE FREQENCIES) - VOICE (SPEECH): 0 Hz - 4000 Hz
AM MODULATED WAVE
AM BROADCAST RADIO(550 kHz - 1600 kHz)
11/5/20109
• AMPLITUDE MODULATION IS RELATIVELYINEXPENSIVE
• AMPLITUDE MODULATION PROVIDES A LOW QUALITYFORM OF MODULATION (POOR PERFORMANCE INNOISY ENVIRONMENTS)
• AMPLITUDE MODULATION IS USED FOR COMMERCIALBROADCASTING (AM RADIO)
• AMPLITUDE MODULATION IS USED FOR TWO-WAYMOBILE RADIO COMMUNICATIONS (CB RADIO)
AMPLITUDE MODULATIONAMPLITUDE MODULATION
11/5/201010
• THERE ARE SEVERAL TYPES OF AMPLITUDEMODULATION SCHEMES
• DSB-SC (DOUBLE SIDEBAND SUPPRESS CARRIER)• DSB-FC (DOUBLE SIDEBAND FULL CARRIER)• SSB-SC (SINGLE SIDEBAND SUPPRESS CARRIER)
(ALSO KNOWN AS: USBAM OR LSBAM)• SSB-FC (SINGLE SIDEBAND FULL CARRIER)• VSB (VESTIGIAL SIDEBAND)
DSB-FC IS THE MOST COMMONLY USED SCHEME.IT IS ALSO CALLED CONVENTIONAL AM OR SIMPLY AM
AMPLITUDE MODULATION TYPESAMPLITUDE MODULATION TYPES
11/5/201011
AMPLITUDE MODULATIONAMPLITUDE MODULATION
DSB-FC AM(AM)
11/5/201012
[ ] ttmEtV ccam ωcos)()( +=
AMPLITUDE MODULATION (DSBAMPLITUDE MODULATION (DSB--FC)FC)
AMAM
MODULATING THE AMPLITUDE OF THE CARRIER WITHTHE MODULATING SIGNAL
11/5/201013
( ) ( )( ) ( )
[ ]tfftffEtfEtV
givesWhichtftfEtfEtVgetWe
YXYXYXGiven
tftfEtVtftfEEtVSignalModulated
mcmcc
ccam
mccccam
cmcam
cmmcam
)(2cos)(2cos2
2cos)(
:2cos2cos2cos)(:
)cos(21)cos(
21))(cos(cos:
2cos2cos1)(2cos2cos)(:
++−+=
+=
++−=
+=+=
ππβπ
ππβπ
ππβππ
tfEtEFor ccc π2cos)( = tfEtE mmm π2cos)( =
AMPLITUDE MODULATION (DSBAMPLITUDE MODULATION (DSB--FC)FC)
AND
c
m
EE
=β
11/5/201014
AMPLITUDE MODULATION (DSBAMPLITUDE MODULATION (DSB--FC)FC)
tEtE mmm ωcos)( =
MULTIPLIERMODULATOR
tcωcos
∑
SUMMER
cE
[ ]tfftffEtfE mcmcc
cc )(2cos)(2cos2
2cos ++−+ ππβπ
• THE AMPLITUDE OF THECARRIER IS UNAFFECTED BYTHE AM PROCESS
11/5/201015
DOUBLEDOUBLE--SIDEBAND FULL CARRIER (DSBSIDEBAND FULL CARRIER (DSB--FC)FC))(ωMMESSAGE
)(ωϑDSB
MODULATED SIGNAL(DSB-FC AM)
BANDWITH:
mmf ωπ =2mω−
mm fB =
cω mc ωω +mc ωω −
USBLSB
mB0
0
mBmB
mBB 2=BW OF THE MODULATED SIGNAL IS:
CARRIER
11/5/201016
DOUBLEDOUBLE--SIDEBAND FULL CARRIER (DSBSIDEBAND FULL CARRIER (DSB--FC)FC)THE MODULATED CARRIER SPECTRUM CENTEREDAT fc IS COMPOSED OF AN UPPER SIDEBAND ABOVEfc, (USB), AND A LOWER SIDEBAND BELOW fc, (LSB).
USBLSB
2 fmMODULATED SIGNAL COMPRISES A COMPONENT AT fc, INTHIS CASE THE SCHEME IS CALLED DSB-FC MODULATION
[ ]tfftffEtfE mcmcc
cc )(2cos)(2cos2
2cos ++−+ ππβπ
11/5/201017
DOUBLEDOUBLE--SIDEBAND FULL CARRIER (DSBSIDEBAND FULL CARRIER (DSB--FC)FC)
[ ]tfftffEtfE mcmcc
cc )(2cos)(2cos2
2cos ++−+ ππβπ
β=mlet
11/5/201018
AMPLITUDE MODULATION (DSB-FC)
11/5/201019
AMPLITUDE MODULATION (DSB-FC)
UNMODULATED CARRIER:
MODULATING SIGNAL:
MODULATION INDEX:
PERCENT MODULATION:
tfEORtfEtV cccc c ππ 2cos2sin)( =
tfEORtfEtV mmmmm ππ 2cos2sin)( =
{c
m
EE
=β
%100xEEM
c
m=
RANGE OF M: 0% 100% WHERE:
M < 100%, UNDERMODULATIONM = 100%, 100% MODULATIONM > 100%, OVERMODULATION (i.e. DISTORTION)
• Modulation Coefficient• Modulation Factor• Modulation Index
11/5/201020
PERCENT MODULATION (M)
PERCENT MODULATION GIVES THE PERCENTAGE CHANGE IN THE AMPLITUDEOF THE OUTPUT WAVE WHEN THE CARRIER IS ACTED ON BY A MODULATINGSIGNAL.
%100xEEM
c
m=
11/5/201021
AMPLITUDE MODULATION (DSB-FC)
MODULATED CARRIER AMPLITUDE: { mmc EEEV ±+=
mcmc EEVEEV −=+= minmax ;
WE KNOW: cmc
m EEEE ββ =∴=
ccc
ccc
EEEVEEEV
)1()1(
min
max
ββββ
−=−=+=+=THUS:
WITH:
100% MODULATION:
50% MODULATION:
0% MODULATION
0;2;1 minmax === VEV cβcc EVEV 5.;5.1;5.0 minmax ===β
cc EVEV === minmax ;;0β
11/5/201022
AMPLITUDE MODULATION
11/5/201023
AMPLITUDE MODULATION (DSB_FC)
minmax
minmax
VVVV
EE
c
m
+−
==β
)(21
minmax VVE m −=
)(21
minmax VVE c +=
)(41
2minmax VVEEE m
lsfusf −===
EUSF = PEAK AMPLITUDE OF THE UPPER SIDE FREQUENCY
ELSF = PEAK AMPLITUDE OF THE LOWER SIDE FREQUENCY
mcmc EEVEEV −=+= minmax ;
ASSUMPTIONS:• MODULATING SIGNAL IS A TONE• MODULATING PROCESS IS SYMMETRICAL
(EQUAL + and – ENVELOPE EXCURCIONS)
11/5/201024
AMPLITUDE MODULATION (DSB-FC)
Modulating Signal
Unmodulated Carrier
50% Modulation
100% Modulation
11/5/201025
DSB-FC EXAMPLE 1FOR AN AM DSB-FC MODULATOR, WITH CARRIER FREQUENCYOF 100 kHz, AND A MAXIMUM MODULATING SIGNAL OF 5 kHz,DETERMINE:
(100 - 5) kHz TO 100 kHz = 95 kHz TO 100 kHz = LSB100 kHz TO (100 + 5) kHz = 100 kHz TO 105 kHz = USB
BANDWITH OF THE MODULATED SIGNAL
B = 2 fm = 2 x 5 kHz = 10 kHz
FREQUENCY LIMITS FOR THE UPPER AND LOWER SIDEBANDS
UPPER AND LOWER SIDE FREQUENCIES WHEN MODULATING SIGNALIS A 3 kHz TONE
(100 - 3) kHz = 97 kHz = LSF(100 + 3) kHz = 103 kHz = USF
11/5/201026
DSB-FC EXAMPLE 2FOR THE AM WAVEFORM BELOW:
DETERMINE:
11/5/201027
DSB-FC EXAMPLE 2PEAK AMPLITUDE OF THE UPPER AND LOWER SIDE FREQUENCIES
)(41
2minmax VVEEE m
lsfusf −===
VEE lsfusf 4)218(41
=−==
PEAK AMPLITUDE OF THE UNMODULATED CARRIER
VVVE c 10)218(21)(
21
minmax =+=+=
PEAK CHANGE IN THE AMPLITUDE OF THE ENVELOPE
VVVE m 8)218(21)(
21
minmax =−=−=
11/5/201028
DSB-FC EXAMPLE 2COEFFICIENT INDEX
8.0108
minmax
minmax==
+−
==VVVV
EE
c
mβ
PERCENT MODULATION
%80%1008.0%100 === xxEEM
c
m
%80%100218218%100
minmax
minmax=
+−
=+−
= xxVVVVM
11/5/201029
DSB-FC EXAMPLE 3ONE INPUT TO A CONVENTIONAL MODULATOR IS A 500 kHzCARRIER WITH AN AMPLITUDE OF 20 Vp. THE SECOND INPUTIS A 10 kHz MODULATING SIGNAL THAT IS OF SUFFICIENT AMPLITUDE TO CAUSE A CHANGE IN THE OUTPUT WAVEOF . DETERMINE:
UPPER AND LOWER SIDE FREQUENCIES
MODULATION COEFFICIENT AND PERCENT MODULATION
(500 + 10) kHz = 510 kHz = USF(500 - 10) kHz = 490 kHz = LSF
Vp5.7±
375.020
5.7==β
%5.37%10020
5.7== xM
11/5/201030
DSB-FC EXAMPLE 3PEAK AMPLITUDE OF THE MODULATED CARRIER
UPPER AND LOWER SIDE FREQUENCY VOLTAGES
Ec (MODULATED) = Ec (UNMODULATED) = 20 Vp
VpEEEE cmlsfusf 75.3
2)20(375.0
22=====
β
MAXIMUM AND MINIMUM AMPLITUDES OF THE ENVELOPE
mcmc EEVEEV −=+= minmax ;VpV 5.275.720max =+=VpV 5.125.720min =−=
11/5/201031
DSB-FC POWER DISTRIBUTION
22cm
lsfusfEEEE β
===
THE POWER DISSIPATION OF AN UNMODULATED CARRIERIN LOAD RESISTANCE R:
RE
REP cc
c2
)707.0( 22
==
FROM:
cc
lsbusb PREPP
48
22 2 ββ===
THE TOTAL POWER IN AN AM DSB-FC ENVELOPE IS:
lsbusbct PPPP ++=
11/5/201032
DSB-FC POWER DISTRIBUTIONFOR A DSB-FC MODULATED WAVE, THE TOTAL POWER INAN AM DSB-FC ENVELOPE IS:
lsbusbct PPPP ++=
244
222c
ccc
ctPPPPPP βββ
+=++=
)2
1(2β
+= ct PP
MODULATED WAVE CARRIER POWER = UNMODULATED WAVE CARRIER POWER(POWER OF THE CARRIER IS UNAFFECTED BY THE MODULATION PROCESS)
11/5/201033
DSB-FC POWER DISTRIBUTION
)2
1(2β
+= ct PP
THE TOTAL POWER IN AN AM DSB-FC ENVELOPE INCREASES WITHMODULATION
tP↑↑ β
cc
lsbusb PREPP
48
22 2 ββ===
11/5/201034
DSB-FC POWER DISTRIBUTION)
21(
2β+= ct PP clsbusb PPP
4
2β==
β=mlet
11/5/201035
DSB-FC POWER DISTRIBUTION
)2
1(2β
+= ct PP clsbusb PPP4
2β==
WITH 100% MODULATION, :
clsbusb PPP41
== clsbusb PPP21
=+
cct PPP 5.1)211( =+=
DSB-FC DISADVANTAGE: THE INFORMATION IS CONTAINED INTHE SIDEBANDS ALTHOUGH MOST OF THE POWER IS WASTEDIN THE CARRIER (DSB-SC ELIMINATES THIS DISADVANTAGE)
1=β
11/5/201036
DSB-FC POWER DISTRIBUTION
THE ADVANTAGE OF ENVELOPE DETECTION IN AMHAS ITS PRICE.
IN AM, THE CARRIER COMPONENT DOES NOT CARRYANY INFORMATION,HENCE, THE CARRIER POWERIS WASTED.
11/5/201037
DSB-FC EXAMPLEFOR AN AM DSB-FC WAVE WITH A PEAK UNMODULATEDCARRIER VOLTAGE Vc = 10 Vp, A LOAD RESISTANCE OFRL = 10 Ohms, AND A MODULATION INDEX OF 1, DETERMINE:
CARRIER POWER
UPPER AND LOWER SIDEBAND POWER
WR
EP cc 5
)10(210
2
22
===
WPPP clsbusb 25.14
)5(14
2
====β
TOTAL SIDEBAND POWER
WPPP clsbusb 5.22
)5(12
2
===+β
11/5/201038
DSB-FC EXAMPLEFOR AN AM DSB-FC WAVE WITH A PEAK UNMODULATEDCARRIER VOLTAGE Vc = 10 Vp, A LOAD RESIATANCE OFRL = 10 Ohms, AND A MODULATION INDEX OF 1, DETERMINE:
TOTAL POWER IN THE MODULATED WAVE
WPP ct 5.7)2
11(5)2
1(22
=+=+=β
POWER SPECTRUM:
11/5/201039
MODULATION BY A COMPLEX SIGNALMODULATION BY A COMPLEX SIGNAL
IN ALL THE ANALYSIS PRESENTED SO FAR FOR AM, WE ASSUMED A SINGLE_FREQUENCY MODULATINGSIGNAL (TONE).
IN PRACTICE, THE MODULATING SIGNAL IS OFTENA COMPLEX WAVEFORM (IT CONSISTS OF MANYFREQUENCY COMPONENTS WITH ASSOCIATED AMPLITUDES)
11/5/201040
IF A MODULATING SIGNAL CONTAINS TWOFREQUENCIES, THEN, THE MODULATED WAVE WILL CONTAIN THE CARRIER AND 2 SETS OF SIDE FREQUENCIES:
[ ]
[ ]tfftffEtfE
tfftffEtfE
mcmcc
cc
mcmcc
cc
)(2cos)(2cos2
2cos
)(2cos)(2cos2
2cos
222
111
++−+
+
++−+
ππβπ
ππβπ
MODULATION BY A COMPLEX SIGNALMODULATION BY A COMPLEX SIGNAL
11/5/201041
WE LEAVE IT TO THE IMAGINATION OF THEREADER TO TAKE THIS FURTHER WHEN MORE THAN TWO FREQUENCIES ARE PRESENT. WHEN SEVERAL FREQUENCIES ARE USED TO MODULATETHE CARRIER, THE TOTAL MODULATION INDEX ISGIVEN AS FOLLOWS:
2222121 nt βββββ ++++= L
MODULATION BY A COMPLEX SIGNALMODULATION BY A COMPLEX SIGNAL
11/5/201042
DSB-FC POWER DISTRIBUTIONTHE POWER DISSIPATION OF AN UNMODULATED CARRIERBECOMES:
ctct
lsbtusbt PREPP
48
22 2 ββ===
THE TOTAL SIDEBAND POWER IS:
22cm
lsfusfEEEE β
===
RE
REP cc
c2
)707.0( 22
==REMEMBERING:
THEN:
ct
sbt PP2
2β=
11/5/201043
DSB-FC POWER DISTRIBUTIONTHE TOTAL POWER IS:
sbtct PPP +=
)2
1(2
tct PP β
+=
CARE MUST BE TAKEN TO INSURE THAT THE COMBINEDVOLTAGES OF ALL THE MODULATING SIGNALS DO NOTOVERMODULATE THE CARRIER !!
11/5/201044
DSB-FC EXAMPLEFOR AN AM DSB-FC TRANSMITTER WITH AN UNMODULATEDCARRIER POWER Pc = 100 W, THAT IS MODULATEDSIMULTANEOUSLY BY 3 MODULATING SIGNALS WITH
DETERMINE:
TOTAL COEFFICENT OF MODULATION:
TOTAL SIDEBAND POWER:
WPP ct
sbt 445.222
)100(67.02
2
===β
5.0,4.0,2.0 321 === βββ
67.05.04.02.0 222 =++=tβ
TOTAL TRANSMITTED POWER:
WP t 445.122)267.01(100
2
=+=
11/5/201045
GENERATION OF AM SIGNALSONE CAN GENERATE AN AM SIGNAL (DSB-FC) USINGANY DSB-SC GENERATOR IF THE MODULATING SIGNAL IS:
[ ] )()( tmofinsteadtmE c +
)(tmEc +
ttC cωcos)( =
)()( tCtm MULTIPLIERMODULATOR
11/5/201046
GENERATION OF AM SIGNALSHOWEVER, AM CAN BE GENERATED IN SIMPLERWAYS …………
BAND-PASS
FILTERRm(t)
+
+tcωcos
E1
I1
)(tVo+
AM MODULATOR: USE ONLY THE UPPER BRANCH OF THEDSB-SC BALANCED MODULATOR
cω±
11/5/201047
DSBDSB--SC NONLINEAR MODULATORSC NONLINEAR MODULATOR
)(cos1 tmtE c += ω 2111 EbEaI +=
[ ] [ ]21 )(cos)(cos tmtbtmtaI cc +++= ωω
SUPPRESSED USING BP FILTER TUNED TO cω±
[ ] [ ] =+++= 21 )(cos)(cos tmtRbtmtRaRI cc ωω
tbRtbRmtaRmttbRmtaR ccc ωωω 22 cos)()(cos)(2cos ++++
Vo(t)=AM SIGNAL
11/5/201048
GENERATION OF AM SIGNALSHOWEVER, AM CAN BE GENERATED IN SIMPLERWAYS ………
BAND-PASS
FILTERR
m(t)+
+tc cωcos
)(tVo+
AM MODULATOR: USE SWITCHING MODULATOR
DIODE ACTS AS ASWITCH
cω±
11/5/201049
GENERATION OF AM SIGNALS• THE DIODE ACTS A SWITCH THAT TURNS ON/OFF.
• THE INPUT SIGNAL IS:
)()(cos tmcwithtmtc c >>+ωSO THAT THE SWITCHING ACTION OF THE DIODE ISCONTROLLED BY:
tc cωcos• THE DIODE SHORTS & OPENS PERIODICALLY IN EFFECT
MULTIPLYING THE INPUT SIGNAL BY S(t)
11/5/201050
GENERATION OF AM SIGNALS• THE SIGNAL ACROSS R IS:
[ ] )()(cos tstmtcV cR += ω
⎥⎦⎤
⎢⎣⎡ ++++= LtttVVts ccc ωωω
π5sin
513sin
31sin2
2)(WITH:
GIVING:
termsotherttmtcV ccR ++= ωπ
ω cos)(2cos2
SUPPRESSED BY BP FILTER
Vo(t)=AM SIGNAL
11/5/201051
GENERATION OF AM SIGNALS• LOW-LEVEL MODULATION: IT TAKES PLACE
PRIOR TO THE OUTPUT ELEMENT OF THE FINAL STAGE(ANTENNA IS NEXT STAGE) OF THE TRANSMITTER(i.e. EMITTER IN A TRANSISTORIZED XMITTER)
• ADVANTAGE: LESS MODULATING SIGNAL POWERIS REQUIRED TO ACHIEVE HIGH PERCENTAGE OFMODULATION:
tm PE ↑↑↑ β• DISADVANTAGE: AMPLIFIER AFTER MODULATOR
STAGE MUST BE LINEAR
11/5/201052
GENERATION OF AM SIGNALS• HIGH-LEVEL MODULATION: IT TAKES PLACE
IN THE FINAL ELEMENT OF THE FINAL STAGEOF THE TRANSMITTER (i.e. COLLECTOR OUTPUT)( CARRIER SIGNAL IS AT ITS MAXIMUM AMPLITUDE)
• REQUIRES A MUCH HIGHER AMPLITUDE MODULATINGSIGNAL TO ACHIEVE A REASONABLE M
• THE FINAL MODULATING SIGNAL AMPLIFIER MUSTSUPPLY ALL THE SIDEBAND POWER – BUT CAN BE ANON-LINEAR AMPLIFIER (PROVIDES MODULATION)
100xEEM
c
m=
11/5/201053
LOW-LEVEL MODULATOR
CARRIER SIGNAL
MODULATING SIGNALVARIES THE GAIN OF THEAMPLIFIER AT A RATE EQUALTO THAT OF THE FREQUENCYOF THE MODULATING SIGNALCOLLECTOR VOLTAGE
AM DSBFC ENVELOPE
EMITTER MODULATOR
MODULATING SIGNAL
COUPLING CAPACITORREMOVES COMPONENT mf
DISADVANTAGES:• CLASS A AMPLIFIER
(NOT EFFICIENT)• LOW POWER OUTPUT
COLLECTOR: OUTPUT ELEMENT
11/5/201054
EMITTER MODULATOR
[ ]tAA cqV ωβ sin1+=
VOLTAGE GAIN IS GIVEN BY:
GAIN WITH MODULATION
GAIN WITHOUT MODULATION (QUIESCENT)
[ ]β±= 1qV AATHUS:
⎩⎨⎧
==
=02
1v
qv
AAA
FOR β
11/5/201055
EXAMPLEFOR THE AM EMITTER MODULATOR WITH MODULATIONINDEX OF 0.8, QUIESCIENT VOLTAGE GAIN OF 100, INPUTCARRIER FREQUENCY OF 500 kHz WITH AMPLITUDE OF 5 mVAND A 1000 Hz MODULATING SIGNAL, DETERMINE:
MAXIMUM & MINIMUM VOLTAGE GAINS:
180)8.01(100max =+=A20)8.01(100min =−=A
MAXIMUM & MINIMUM Vout AMPLITUDES:
VV out 9.0)005.0(180(max) ==
VV out 1.0)005.0(20(min) ==
11/5/201056
MEDIUM LEVEL MODULATORMEDIUM POWERAM MODULATOR
MODULATION AT Q OUTPUT ELEMENT(COLLECTOR MODULATOR)
MODULATING SIGNAL
CLASS C AMPLIFIER• HIGHER POWER EFFICIENCY
CARRIER SIGNAL
REQUIRES HIGHERAMPLITUDES
DISADVANTAGE:• M < 100%
11/5/201057
LINEAR IC MODULATOR
RCfc
1=
MODULATINGSIGNAL
MODULATEDSIGNAL
LOW POWEROUTPUT
FUNCTION GENERATOR
11/5/201058
LINEAR IC MODULATOR - EXAMPLE
kHzuFk
fc 100)001(.10
1==
11/5/201059
AMPLITUDE MODULATIONAMPLITUDE MODULATION
DSB-SC AM
11/5/201060
• MESSAGE SIGNAL =
• CARRIER SIGNAL =
• MODULATED SIGNAL =
AMPLITUDE MODULATION (DSBAMPLITUDE MODULATION (DSB--SC)SC)
)(cos)( ωω MtEtm mm ↔=
)(cos)( ωω CtEtC cc ↔=
ttEEtCtm cmcm ωω coscos)()( =
[ ]ttEEmcmc
cm )cos()cos(2
ωωωω −++
[ ])()(2
cos)( mcmccm
cEEttm ωωϑωωϑω −++↔
fπω 2= )cos(21)cos(
21))(cos(cos YXYXYX −++=
11/5/201061
AMPLITUDE MODULATION (DSBAMPLITUDE MODULATION (DSB--SC)SC)
ttm mωcos)( =
ttC cωcos)( =
)()( tCtm
[ ]ttEEmcmc
cm )cos()cos(2
ωωωω −++
MULTIPLIERMODULATOR
11/5/201062
DOUBLEDOUBLE--SIDEBAND SUPPRESS CARRIER (DSBSIDEBAND SUPPRESS CARRIER (DSB--SC)SC)
)(ωMMESSAGE
)(ωϑDSB
MODULATED SIGNAL(DSB-SC AM)
BANDWITH:
mmf ωπ =2mω−
mm fB =
cω mc ωω +mc ωω −cω mc ωω +mc ωω −
USBLSB
mB0
0
mBmB
mBB 2=BW OF THE MODULATED SIGNAL IS:
11/5/201063
DOUBLEDOUBLE--SIDEBAND SUPPRESS CARRIER (DSBSIDEBAND SUPPRESS CARRIER (DSB--SC)SC)
THE MODULATED CARRIER SPECTRUM CENTEREDAT fc IS COMPOSED OF AN UPPER SIDEBAND ABOVEfc, (USB), AND A LOWER SIDEBAND BELOW fc, (LSB).
USBLSB
2 fm
[ ]ttEEmcmc
cm )cos()cos(2
ωωωω −++
MODULATED SIGNAL DOES NOT HAVE A COMPONENT AT fc, INTHIS CASE THE SCHEME IS CALLED DSB-SC MODULATION
11/5/201064
DSB-SC MODULATORS• MULTIPLIER MODULATORS
• ANALOG MULTIPLIERS (i.e. VARIABLE GAINAMPLIFIER USING OP-AMPS OR TRANSISTORS,WHEREBY THE GAIN PARAMETER IS CONTROLLEDBY ONE OF THE SIGNALS (i.e. S1(t) )
VARIABLE GAINK S1(t)
S1(t)
S2(t)
K S1(t) S2(t)
LINEAR TIME-VARYING MODULATOR
11/5/201065
DSB-SC MODULATORS• NONLINEAR MODULATORS
MODULATION CAN BE ACHIEVED BY USINGNONLINEAR DEVICES (SQUARE LAW DEVICE = DIODE,TRANSISTOR)
I
V
2bVaVI +≈
11/5/201066
DSB-SC NONLINEAR MODULATOR
BAND-PASS
FILTER
R
R
m(t)
m(t)
+
+
+tcωcos
E1
E2
I1
I2
V
cω±ttKm
tVocωcos)(
)( =
+
+
11/5/201067
DSBDSB--SC NONLINEAR MODULATORSC NONLINEAR MODULATOR
)(cos1 tmtE c += ω )(cos2 tmtE c −= ω
2111 EbEaI += 2
222 EbEaI +=
[ ] [ ]21 )(cos)(cos tmtbtmtaI cc +++= ωω
[ ] [ ]22 )(cos)(cos tmtbtmtaI cc −+−= ωω
RIRIV 21 −=
[ ])(cos)(22 tmattmbRV c += ω
[ ] ttKmttmbRV cco ωω cos)(cos)(22 ==
FILTER USING BP FILTERTUNED TO cω±
11/5/201068
DOUBLEDOUBLE--SIDEBAND SUPPRESS CARRIER (DSBSIDEBAND SUPPRESS CARRIER (DSB--SC)SC)
MODULATED SIGNAL(DSB-SC AM)
cω mc ωω +mc ωω −cω mc ωω +mc ωω − 0
BP FILTER
11/5/201069
DSB-SC MODULATORS• SWITCHING MODULATOR
A MODULATED SIGNAL CAN BE REALIZED BYMULTIPLYING m(t) BY ANY PERIODIC SIGNAL OF THEFUNDAMENTAL FREQUENCY (i.e. SQUARE PULSETRAIN)
cω
VV
00 T/2T/2 TT timetime
S(t)S(t)
⎩⎨⎧
<<−<<+
=02/,02/0,
)(tTTtV
ts
SQUARE WAVE: 50% DUTY CYCLESQUARE WAVE: 50% DUTY CYCLE
--T/2T/2
NEITHER FUNCTION
11/5/201070
FOURIER SERIES OF THE SQUARE WAVEFOURIER SERIES OF THE SQUARE WAVE
VV
00 T/2T/2 TT timetime
S(t)S(t)
⎩⎨⎧
<<−<<+
=02/,02/0,
)(tTTtV
ts
SQUARE WAVE: 50% DUTY CYCLESQUARE WAVE: 50% DUTY CYCLE
∑∞
=
++=1
sincos)(n
cncno tnBtnAAts ωω
∫=T
cn dttntsT
B0
sin)(2 ω
--T/2T/2
∫=T
o dttsT
A0
)(1
∫=T
cn dttntsT
A0
cos)(2 ω
NEITHER FUNCTION
11/5/201071
FOURIER SERIES OF THE SQUARE WAVEFOURIER SERIES OF THE SQUARE WAVE
VV
00 T/2T/2 TT timetime
S(t)S(t) SQUARE WAVE: 50% DUTY CYCLESQUARE WAVE: 50% DUTY CYCLE
⎥⎦⎤
⎢⎣⎡= ∫ 2
0sin2 T
cn dttnVT
B ω
dtndutnuuduu oob
a
ba ωω ==−=∫ ;;cossin
--T/2T/2
22111 2/
02
0
VTVT
VtT
dtVT
A TTo ===⎥⎦
⎤⎢⎣⎡= ∫
⎥⎦⎤
⎢⎣⎡−= 2
0cos2 Tc
cn tn
TnVB ωω
11/5/201072
FOURIER SERIES OF THE SQUARE WAVEFOURIER SERIES OF THE SQUARE WAVE
timetime
⎪⎩
⎪⎨⎧
=
++===
0;0
;22
t
nTtT
tntn cππω
[ ])0coscos( +−= ππ
nn
VBn
[ ]ππ
nn
VBn cos1−=
⎥⎦⎤
⎢⎣⎡−= 2
0cos2 Tc
cn tn
TnVB ωω
VV
00 T/2T/2 TT
S(t)S(t) SQUARE WAVE: 50% DUTY CYCLESQUARE WAVE: 50% DUTY CYCLE
--T/2T/2
⎩⎨⎧ −
=1;
1;cos
evennoddn
nπ
⎪⎩
⎪⎨⎧
0;
2;
evennnVoddnπ
11/5/201073
FOURIER SERIES OF THE SQUARE WAVEFOURIER SERIES OF THE SQUARE WAVE
VV
00 T/2T/2 TT timetime
S(t)S(t) SQUARE WAVE: 50% DUTY CYCLESQUARE WAVE: 50% DUTY CYCLE
⎥⎦⎤
⎢⎣⎡= ∫ 2
0cos2 T
cn dttnVT
A ω
dtndutnuuduu oob
a
ba ωω ===∫ ;;sincos
--T/2T/2
⎥⎦⎤
⎢⎣⎡= 2
0sin2 Tc
cn tn
TnVA ωω
11/5/201074
FOURIER SERIES OF THE SQUARE WAVEFOURIER SERIES OF THE SQUARE WAVE
timetime
⎪⎩
⎪⎨⎧
=
++===
0;0
;22
t
nTtT
tntn cππω
[ ])0sin(sin −= ππ
nn
VAn
[ ] 0sin == ππ
nn
VAn
VV
00 T/2T/2 TT
S(t)S(t) SQUARE WAVE: 50% DUTY CYCLESQUARE WAVE: 50% DUTY CYCLE
--T/2T/2
⎥⎦⎤
⎢⎣⎡= 2
0sin2 Tc
cn tn
TnVA ωω
11/5/201075
FOURIER SERIES OF THE SQUARE WAVEFOURIER SERIES OF THE SQUARE WAVE
timetime
VV
00 T/2T/2 TT
S(t)S(t) SQUARE WAVE: 50% DUTY CYCLESQUARE WAVE: 50% DUTY CYCLE
--T/2T/2
2VAo =
∑∞
=
++=1
sincos)(n
cncno tnBtnAAts ωω
0=nA
∑∞
=
+=oddn
c tnnVVts ωπ
sin22
)(
⎪⎩
⎪⎨⎧
=0;
2;
evennnVoddn
Bn π
11/5/201076
⎥⎦⎤
⎢⎣⎡ ++++= LtttVVts ccc ωωω
π5sin
513sin
31sin2
2)(
FOURIER SERIES OF THE SQUARE WAVEFOURIER SERIES OF THE SQUARE WAVE
timetime
VV
00 T/2T/2 TT
S(t)S(t) SQUARE WAVE: 50% DUTY CYCLESQUARE WAVE: 50% DUTY CYCLE
--T/2T/2
∑∞
=
+=oddn
c tnnVVts ωπ
sin22
)(
11/5/201077
∑∞
=
+=oddn
c tntmnVtVmtstm ωπ
sin)(22
)()()(
)()( tstmTHE SPECTRUM OF THE PRODUCT :
)()(22
)()()( cmcnodd
mm nMnM
nVVMtstm ωωωωπ
ω−+++↔ ∑
∞
IS:
SWITCHING MODULATORS
MULTIPLICATION OF TWO WAVES
IF THIS SIGNAL IS PASSED THROUGH A BANDPASS FILTEROF BANDWITH 2B AND TUNED TO THEN WE GETTHE DESIRED MODULATED SIGNAL:
cω
)()( tstKmV o =
11/5/201078
SUPPRESS CARRIER SYSTEMCHARACTERISTICS
• SC SYSTEMS NEED SOPHISTICATED CIRCUITRYAT THE RECEIVER SO TO GENERATE A LOCAL CARRIEROF EXACTLY THE RIGHT FREQUENCY AND PHASE FOR SYNCHRONOUS DEMODULATION (NEED TOSUPPRESS THE CARRIER FREQUENCY AT THETRANSMITTER)
• SC SYSTEMS ARE VERY EFFICIENT FROM THE POINTOF VIEW OF POWER REQUIREMENTS AT THETRANSMITTER (COMPARED TO DSB-FC/SSB-FC)
11/5/201079
SUPPRESS CARRIER SYSTEMCHARACTERISTICS
• SC SYSTEMS ARE JUSTIFIED IN POINT-TO-POINT COMMUNICATIONS (ONE RECEIVER FOR EACH TRANSMITTER)
• FOR BROADCAST SYSTEMS WITH A MULTITUDE OFRECEIVERS FOR EACH TRANSMITTER, IT IS MOREECONOMICAL TO HAVE SIMPLER, LESS EXPENSIVERECEIVERS (INEXPENSIVE DEMODULATOR), THUS
FULL CARRIER SYSTEMS (i.e. DSB-FC)