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3/18/2014 1 Communication Systems Instructor: Engr. Dr. Sarmad Ullah Khan Assistant Professor Assistant Professor Electrical Engineering Department CECOS University of IT and Emerging Sciences [email protected] Chapter 4 Dr. Sarmad Ullah Khan Amplitude Modulations and Demodulations 2
43

Chapter 4

May 19, 2015

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Page 1: Chapter 4

3/18/2014

1

Communication Systems

Instructor: Engr. Dr. Sarmad Ullah Khan

Assistant ProfessorAssistant ProfessorElectrical Engineering Department

CECOS University of IT and Emerging [email protected]

Chapter 4

Dr. Sarmad Ullah Khan

Amplitude Modulations and Demodulations

2

Page 2: Chapter 4

3/18/2014

2

Outlines

• Baseband versus Carrier Communication

D bl id b d A lit d M d l ti

Dr. Sarmad Ullah Khan

• Double sideband Amplitude Modulation

• Amplitude Modulation

• Bandwidth Efficient Amplitude Modulation

• Amplitude Modulation: VESTIGIAL Sideband

3

Outlines

• Baseband versus Carrier Communication

D bl id b d A lit d M d l ti

Dr. Sarmad Ullah Khan

• Double sideband Amplitude Modulation

• Amplitude Modulation

• Bandwidth Efficient Amplitude Modulation

• Amplitude Modulation: VESTIGIAL Sideband

4

Page 3: Chapter 4

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3

Baseband versus Carrier Communication

• Modulation is a process that moves signal into aspecific frequency band

Dr. Sarmad Ullah Khan

specific frequency band• The bandwidth B represents a measure of frequency

range.• It is typically measured in Hz with 1 Hz = 1/sec.• The bandwidth of a signal indicates the frequency

range in which the signal‘s Fourier transform has ag gpower above a certain threshold (typically half ofthe maximum power)

5

Baseband versus Carrier Communication

• Communication systems that do not use modulationare called baseband communication

Dr. Sarmad Ullah Khan

are called baseband communication• Communication systems that use modulation are

called carrier communication• Baseband is original message frequency band• In telephony, baseband is audio band (0 – 3.5 kHz)• In NTSC television, video baseband is 0 – 4.3 MHzIn NTSC television, video baseband is 0 4.3 MHz

6

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4

Baseband versus Carrier Communication

• Baseband CommunicationMessage signals are directly transmitted without any

Dr. Sarmad Ullah Khan

Message signals are directly transmitted without anymodulation

Dedicated user channels are assigned to each long distancecommunication

Baseband signals have overlapping bandsSevere interferenceWaste of channel resourcesWaste of channel resourcesModulation and shifting to non overlapping bands save

channel resources

7

Baseband versus Carrier Communication

• Carrier CommunicationModulation techniques is used to shift the frequency

Dr. Sarmad Ullah Khan

Modulation techniques is used to shift the frequencyspectrum of message signal

Modulation changes one of the basic parameter of carriersignal (Amplitude, Frequency, Phase)

Carrier signal is a sinusoidal signal of high frequency fc

Parameter variation is proportional to message signal m(t)Amplitude modulation is linearAmplitude modulation is linearFrequency and Phase modulations are non linearsPAM, PWM, PPM, PCM and DM are baseband signals

8

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5

Baseband versus Carrier Communication

• Amplitude Modulation and Angle ModulationAmplitude modulation (AM) varies the amplitude of a

Dr. Sarmad Ullah Khan

Amplitude modulation (AM) varies the amplitude of acarrier signal according to a modulatingsignal m(t).

The modulated signal is

)cos(c

tc

wA

)cos()( twtm c

Source signal m(t) and its Fourier transform M(f)

9

Baseband versus Carrier Communication

• Amplitude Modulation and Angle Modulation

Dr. Sarmad Ullah Khan

Frequency Shifting Property

10 )()(

2

1cos)( ccc wwMwwMtwtm

Page 6: Chapter 4

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6

Outlines

• Baseband versus Carrier Communication

D bl id b d A lit d M d l ti

Dr. Sarmad Ullah Khan

• Double sideband Amplitude Modulation

• Amplitude Modulation

• Bandwidth Efficient Amplitude Modulation

• Amplitude Modulation: VESTIGIAL Sideband

11

Double Sideband Amplitude Modulation

• Amplitude Modulation and Angle Modulation

Dr. Sarmad Ullah Khan

1

M(f - fc) is M(f) shifted to the right of fc

M(f + fc) is M(f) shifted to the left of fc

The bandwidth changed from B to 2B The modulated signal is composed of two parts, above

)()(2

12cos)( ccc ffMffMtftm

The modulated signal is composed of two parts, abovefc and below fc

12

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7

Double Sideband Amplitude Modulation

• Amplitude Modulation and Angle ModulationThe upper sideband (USB) containing the frequencies

Dr. Sarmad Ullah Khan

The upper sideband (USB) containing the frequencies|f| > |fc|The lower sideband (LSB) containing the frequencies

|f| < |fc|The modulated signal in this scheme does not have a

discrete component of the carrier frequency fc. For thisreason this is called double sideband suppressedreason this is called double-sideband suppressedcarrier (DSB-SC) modulation

13

Double Sideband Amplitude Modulation

• Amplitude Modulation and Angle ModulationB vs f

Dr. Sarmad Ullah Khan

B vs fc

14

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8

Dr. Sarmad Ullah Khan

Double Sideband Amplitude Modulation

15

Dr. Sarmad Ullah Khan

Double Sideband Amplitude Modulation

Spectrum

Spectrum of the DSB-SC signal m(t)cos10,000t

)cos()cos(1

coscos

16

)cos()cos(2

coscos

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9

Spectrum

Dr. Sarmad Ullah Khan

Double Sideband Amplitude Modulation

Spectrum

Spectrum of the DSB-SC signal m(t)cos10,000t

17

Spectrum

Dr. Sarmad Ullah Khan

Double Sideband Amplitude Modulation

Spectrum

Spectrum of the DSB-SC signal m(t)cos10,000t

18

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10

Double Sideband Amplitude Modulation

• Modulation and Demodulation

Dr. Sarmad Ullah Khan

19

Double Sideband Amplitude Modulation

• Modulation and Demodulation

Dr. Sarmad Ullah Khan

)2cos()()(21cos)()( 2 twtmtmtwtmte

cc

20 )2()2(4

1)(21)(

ccwwMwwMwMwE

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11

Double Sideband Amplitude Modulation

• ModulatorsMultiplier Modulators

Dr. Sarmad Ullah Khan

Multiplier ModulatorsModulation is achieved directly by multiplying m(t) by

cos(wct) using an analog multiplier.The output is proportional to the product of two input

signals.Difficult to maintain linearity and are expansive.

21

Better to avoid

Double Sideband Amplitude Modulation

• ModulatorsNon Linear Modulators

Dr. Sarmad Ullah Khan

Non Linear ModulatorsModulation can be achieved by using non linear deviceFor example, diodes or transistors

Input-output characteristics of NL element is approx. bypower series as

22

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12

Double Sideband Amplitude Modulation

• ModulatorsNon Linear Modulators

Dr. Sarmad Ullah Khan

Non Linear Modulators

The summer output z(t) is given by

23

Double Sideband Amplitude Modulation

• ModulatorsNon Linear Modulators

Dr. Sarmad Ullah Khan

Non Linear Modulators

Substitution of x1(t)=coswct+m(t) and x2(t)=coswct-m(t)

24

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13

Double Sideband Amplitude Modulation

• ModulatorsNon Linear Modulators

Dr. Sarmad Ullah Khan

Non Linear Modulators

Spectrum of m(t) is centered at originSpectrum of m(t) coswct is centered at ±ωThe signal is ready for transmission but we do not need the

m(t) part of z(t)m(t) part of z(t)Z(t) passed through band pass filter tuned to ωc

am(t) is suppressed and desire modulated signal4bm(t)coswct pass without distortion

25

Double Sideband Amplitude Modulation

• ModulatorsNon Linear Modulators (summary)

Dr. Sarmad Ullah Khan

Non Linear Modulators (summary)

Two inputs m(t) and coswctThe summer output does not contain one of the input coswctCircuits which have this characteristic are called balanced

circuits.circuits.The previous circuitry is an example of balanced modulators.

26

This circuit is balanced to only one input carrier, the other input m(t) stillappear at the filter input, which must reject it…….for that reason it iscalled a single balanced modulator

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14

Double Sideband Amplitude Modulation

• ModulatorsModulation through any periodic signal

Dr. Sarmad Ullah Khan

Modulation through any periodic signalModulated signal can not only be obtained by a pure sinusoid but

by any periodic signal of fundamental frequency wc

Periodic signal can be expresses by trigonometric FourierSeries

Spectrum of the modulated signal is the spectrum M(w) shifted to±fc , ±2fc , ±3fc , ±4fc , …… ±nfc ,……

27

Double Sideband Amplitude Modulation

• ModulatorsModulation through any periodic signal

Dr. Sarmad Ullah Khan

Modulation through any periodic signalIf we pass this modulated signal through band-pass filter of

bandwidth 2B tuned to wc

28

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Double Sideband Amplitude Modulation

• ModulatorsSwitching Modulators

Dr. Sarmad Ullah Khan

Switching ModulatorsMultiplication operation of modulation can be replaced by

switching operation. If a periodic signal having Fourier series as:

carrier

Modulated signal

Now consider a periodic square pulse train with Fourier series as

29

Modulated signal

....7cos

7

15cos

5

13cos

3

1cos

2

2

1)( twtwtwtwtw cccc

From example 2.8

Double Sideband Amplitude Modulation

• ModulatorsSwitching Modulators

Dr. Sarmad Ullah Khan

Switching ModulatorsThe modulated signal m(t)w(t) is given by

....7cos)(

7

15cos)(

5

13cos)(

3

1cos)(

2)(

2

1)()( twtmtwtmtwtmtwtmtmtwtm cccc

30

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Modulated signal m(t)w(t) consists of the component m(t) plus infinite numbers of modulated signals with carrier frequencies ,.....5,3,

cccwww

Th f ( ) ( ) i f M( ) d M( ) hif d

Double Sideband Amplitude Modulation

Dr. Sarmad Ullah Khan

The spectrum of m(t)w(t) consists of M(w) and M(w) shifted to,.....5,3,

cccwww

As we are interested in modulated component only. To separate this component from others we pass m(t)w(t) through a bandpass filter of bandwidth 2BHz, centered at

twtmc

cos)(

cw

31

gives the required modulated signal twtmc

cos)(2

Therefore the multiplication of a signal by a square pulse train is is reality a switching operation means turning off and on signal m(t)periodically and can be accomplished by switching element controlled by w(t)

Double Sideband Amplitude Modulation

• ModulatorsDiode Bridge Modulator

Dr. Sarmad Ullah Khan

Diode Bridge ModulatorConsider the following electronic switch circuit driven by

to produce the switching action

4321 ,, DDDD and

are matched pairs

32

During the next half cycle d is positive with respect to c, all the diodes open, terminal a & b are open.

When terminal c is positive with respect to d, all the diodes conduct, terminal a & b are effectively shortened.

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Double Sideband Amplitude Modulation

• ModulatorsDiode Bridge Modulator

Dr. Sarmad Ullah Khan

Diode Bridge ModulatorTherefore the the circuit act as a desired electronic switch, where

the terminal a & b open and close periodically with the carrierfrequency fc. When is applied across the terminal ab

To obtain m(t)w(t) we may place terminal ab in series or in parallelas:

twA ccos

Switching on and off m(t) for each cycle of the carrier, resulting inthe switched signal m(t)w(t) and passing through band pass filtergives the desired signal:

33

Series-bridge diode modulator Shunt-bridge diode modulator

Double Sideband Amplitude Modulation

• ModulatorsRing Modulator

Dr. Sarmad Ullah Khan

Ring Modulator

Consider the following circuit

During the positive half cycle of the carrier D1 & D3 conduct and D2

& D4 are open, hence terminal a is connected to c & b to d

During the negative half cycle of the carrier D1 & D3 are open andD2 & D4 conduct, hence terminal a is connected to d & b to c

Output is proportional to m(t) during positive cycle & -m(t) duringnegative cycle

34

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18

Double Sideband Amplitude Modulation

• ModulatorsRing Modulator

Dr. Sarmad Ullah Khan

Ring ModulatorThe Fourier series of bipolar square wave is given by:

....7cos

7

15cos

5

13cos

3

1cos

4)(0 twtwtwtwtw cccc

....7cos)(

7

15cos)(

5

13cos)(

3

1cos)(

4)()( 0 twtmtwtmtwtmtwtmtwtm ccccFiltering this signal to bandpass filter tuned to wc gives the required

modulated signal:

35

In this circuit there are two inputs m(t) and coswct, the input of thefinal band pass filter does not contain either of the inputs……

This circuit is an example of double balanced modulator

Double Sideband Amplitude Modulation

• Demodulation of DSB-SC SignalsThe demodulation involve multiplication of DSB SC

Dr. Sarmad Ullah Khan

The demodulation involve multiplication of DSB-SCwith carrier signalAt receiver incoming signal multiply with local carrierLocal carrier must have frequency and phase

synchronization with incoming signalProduct is passed to low pass filterSuch demodulators are called synchronous or coherent

or homodyne demodulators

36

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Problem 4.2‐4

Dr. Sarmad Ullah Khan

37

Problem 4.2‐4Dr. Sarmad Ullah Khan

38

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Problem 4.2‐4Dr. Sarmad Ullah Khan

At point b

39

At point c

Problem 4.2‐4

The minimum value of wc is to avoid overlapping

Dr. Sarmad Ullah Khan

pp g

40Will not work

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Problem 4.2‐4

This may be verified that the identity for contains

Dr. Sarmad Ullah Khan

This may be verified that the identity for contains a term when n is odd. This is not true when n is even. Hence, the system works for a carrier only when n is odd.

41

Example 4.2

Frequency mixer or converter:

Frequency mixer or converter is used to change the carrier frequency of the

Dr. Sarmad Ullah Khan

modulated signal m(t)coswct to some other frequency wl

Can be achieved by multiplying m(t)coswct by

where or

42

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22

Example 4.2

In both cases the filter tuned to Wl will pass the term m(t)coswlt and suppress the other term and giving the required output

Dr. Sarmad Ullah Khan

m(t)coswct (the carrier frequency is translated to wl from wc)

43

Frequency mixing or frequency conversion is also known as heterodyning.

All the modulators discussed previously can be used for frequency mixing.

Frequency selected as operation called up-conversion Frequency selected as operation called down-conversion

Outlines

• Baseband versus Carrier Communication

D bl id b d A lit d M d l ti

Dr. Sarmad Ullah Khan

• Double sideband Amplitude Modulation

• Amplitude Modulation

• Bandwidth Efficient Amplitude Modulation

• Amplitude Modulation: VESTIGIAL Sideband

44

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Amplitude Modulation

• The demodulation requires the receiver to possess acarrier signal that is synchronized with incoming signal

Dr. Sarmad Ullah Khan

• It is difficult to achieve in practice• Unknown frequency shifts

• Require sophisticated receiver and costly• Transmit a carrier Acoswct along with the modulated

signal m(t)coswct so no need to generate a carrier at thereceiver

45

Amplitude Modulation

• This type of modulation is called AM modulation anddenoted by and given by

Dr. Sarmad Ullah Khan

)(ty g y

• Its Fourier spectrum is

)(tAM

• The spectrum of is the same as m(t)coswct plus twoadditional impulses at ±ω

46

)(tAM

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Amplitude Modulation

• DSB-SC signal m(t)coswct and AM signal are identical with A+m(t) as modulating signal instead of

Dr. Sarmad Ullah Khan

are identical with A+m(t) as modulating signal instead of m(t)

• To sketch ,we sketch A+m(t) & -(A+m(t) ) and fill in between the carrier frequency.

)(tAM

47

Amplitude Modulation

• For signal e(t)coswct, if e(t) varies slowly, its envelopwould be |e(t)|

Dr. Sarmad Ullah Khan

would be |e(t)|

• It means if A+m(t)≥0 for all t, the envelop of is

|A + m(t)| = A + m(t)

• For envelop detection to properly detect m(t)

• fc >> bandwidth of m(t)

)(tAM

• fc >> bandwidth of m(t)

• A + m(t) ≥ 0

48

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Amplitude Modulation

• Message signals m(t) with zero offset Let ±m be the maximum and minimum value of m(t)

Dr. Sarmad Ullah Khan

Let ±mp be the maximum and minimum value of m(t) m(t) ≥ -mp

Condition of envelop detection isA ≥ - mmin = mp

Modulation index μ isμ = mp/A

F l d t ti t b di t ti lFor envelop detection to be distortion less0 ≤ μ ≤ 1

This is required condition for distortion lessdemodulation of AM by envelop detector

49

Amplitude Modulation

• Message signals m(t) with nonzero offset It is rare that m(t) will have nonzero offset

Dr. Sarmad Ullah Khan

It is rare that m(t) will have nonzero offsetMaximum mmax and minimum mmin are not symmetric

mmin ≠ mmax

Change in offset does not change the envelop detectoroutput and

0 ≤ μ ≤ 1μBut

μ = (mmax - mmin) / (2A + mmax + mmin)

50

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Amplitude Modulation

• Sideband and Carrier Power Th i di d t f l d t ti i t f

Dr. Sarmad Ullah Khan

There is a disadvantage of envelope detection in terms ofpower waste, as the carrier term does not contain anyinformation

The carrier power Pc and sideband power Ps is given by

Power efficiency is given by

51

Amplitude Modulation

• Sideband and Carrier PowerFor the special case of tone modulation:

Dr. Sarmad Ullah Khan

For the special case of tone modulation:

Hence

With the condition 0 ≤ μ ≤ 1,Thus under best condition only one third of the transmitted

power is used for carrying message, for practical signalsthe efficiency is even worst

52

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Amplitude Modulation

• Generation of AM signalAM signals can be generated by any DSB SC modulators

Dr. Sarmad Ullah Khan

AM signals can be generated by any DSB-SC modulators. The input should be A + m(t) instead of just m(t). The modulating circuit do not have to be balanced because

there is no need to suppress the carrier

Switching action is provided by a single diode and controlled by                   with twc ccos

53

c

Amplitude Modulation

• Generation of AM signal

Dr. Sarmad Ullah Khan

The diode opens and short periodically with  infect multiplying the input signal by w(t).

The voltage across is:

54

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Amplitude Modulation

• Demodulation of AM signalThe AM signal can be demodulated coherently by a locally

Dr. Sarmad Ullah Khan

The AM signal can be demodulated coherently by a locallygenerated carrier. E.g.

There are two well known methods of demodulation of AMsignals:

1) Rectifier detection 2) Envelope detection

twtwtmA cc coscos)( No benefit of sending carrier on the channel

1) Rectifier detection 2) Envelope detectionRectifier detector:

AM signal is applied to a diode and resistor circuit, the negativepart of the AM wave will be suppressed.

The output across the resistor is the half wave rectified version ofthe AM signal means multiplying AM with w(t).

55

Amplitude Modulation

• Demodulation of AM signalRectifier detector:

Dr. Sarmad Ullah Khan

Rectifier detector:

The rectified output VR

56

)(cos)( twtc

wtmAvR

...5cos

5

13cos

3

1cos

2

2

1cos)( t

cwt

cwt

cwt

cwtmA

otherTermstmA )(1

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Amplitude Modulation

• Demodulation of AM signalRectifier detector:

Dr. Sarmad Ullah Khan

Rectifier detector:

57

Amplitude Modulation

• Demodulation of AM signalEnvelop detector:

Dr. Sarmad Ullah Khan

Envelop detector:In an envelope detector, the output follows the envelope

of the modulated signalThe following circuit act as an envelope detector

During the positive cycle of the input signal, the diodeconducts and the capacitor C charges up to the peakvoltage of the input signal

58

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Amplitude Modulation

• Demodulation of AM signalEnvelop detector:

Dr. Sarmad Ullah Khan

Envelop detector:

When input signal falls below this peak value, the diodei t ff (b th di d lt hi h i l this cut off. (because the diode voltage which is nearly thepeak voltage is greater than the input signal voltagecausing the diode to open )At this stage the capacitor discharge at the slew rate

(with a time constant RC)During the next positive cycle the process repeats 59

Amplitude Modulation

• Demodulation of AM signalEnvelop detector:

Dr. Sarmad Ullah Khan

p

During each positive cycle the capacitor charges up to theDuring each positive cycle the capacitor charges up to thepeak voltage of the input signal and then decays slowly untilthe next positive cycleThis behavior of the capacitor makes output voltage Vc(t)

follow the envelope of the input signalCapacitor discharges during each positive peaks causes a

ripple signal of frequency wc at the output60

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Amplitude Modulation

• Demodulation of AM signalEnvelop detector:

Dr. Sarmad Ullah Khan

Envelop detector:

The ripple can be reduced by increasing the timeconstant RC so the capacitor discharges very littlebetween positive peaks of the input signalsMaking RC too large, makes capacitor voltage

impossible to follow the envelope

61

Amplitude Modulation

• Demodulation of AM signalEnvelop detector:

Dr. Sarmad Ullah Khan

Envelop detector:

RC should be large compared to 1/wc, but should be small compared to

Where B is the highest frequency in m(t)

B21

Also requires a condition which is necessary for well defined envelope.

62

The envelope detector output is with a ripple of frequency wc

The DC term A can be blocked by a capacitor or a simple RC high pass filter, and the ripple may be reduced further by another low-pass RC filter.

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Outlines

• Baseband versus Carrier Communication

D bl id b d A lit d M d l ti

Dr. Sarmad Ullah Khan

• Double sideband Amplitude Modulation

• Amplitude Modulation

• Bandwidth Efficient Amplitude Modulation

• Amplitude Modulation: VESTIGIAL Sideband

63

Bandwidth Efficient Amplitude Modulation

• DSB spectrum has two sidebands (USB, LSB)• Both carry complete information

Dr. Sarmad Ullah Khan

• Both carry complete information• Bandwidth requirement is 2B• How to improve spectral efficiency?

– Utilize spectral redundancy– remove spectral redundancy

• Single Sideband (SSB) removes either LSB or USBSingle Sideband (SSB) removes either LSB or USB• Quadrature amplitude modulation (QAM) utilize

64

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Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) ModulationLSB USB b d b b d filt

Dr. Sarmad Ullah Khan

– LSB or USB can be suppressed by band pass filter– A scheme in which only one sideband is

transmitted is known as single-sideband ( SSB)transmission

– In SSB transmission the required bandwidth is halfcompared to DSB signalp g

– An SSB signal can be coherently (synchronously)demodulated. E.g

– For example multiplying USB signal by coswctshifts its spectrum to the left and right by wc

65

Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) ModulationL filt i ill i th i d b b d

Dr. Sarmad Ullah Khan

– Low pass filtering will give the required basebandsignal at the receiver

66

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Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) ModulationHilb t T f

Dr. Sarmad Ullah Khan

– Hilbert Transform– xh(t) and H{x(t)} to denote Hilbert transform of

x(t)

Hilbert Transform of m(t)

and delays the phase of each component by

)(tmh

2

67

Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) ModulationHilb t T f

Dr. Sarmad Ullah Khan

– Hilbert Transform– xh(t) and H{x(t)} to denote Hilbert transform of

x(t)

68

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Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) ModulationTi d i t ti f SSB i

Dr. Sarmad Ullah Khan

– Time domain representation of SSB is

– Where minus sign applies to USB and the plussign applies to LSB

twtmtwtmt chcSSB sin)(cos)()(

69

Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) Modulation

Dr. Sarmad Ullah Khan

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Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) Modulation

Dr. Sarmad Ullah Khan

71

Example 4.7  p‐174

Tone Modulation:

Find for a simple case of tone modulation that is when the)(tSSB

Dr. Sarmad Ullah Khan

Find for a simple case of tone modulation, that is, when the modulating signal is a sinusoid

)(SSBtwtm mcos)(

Solution:

twtmtwtmt chcSSB sin)(cos)()(

72

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37

Example 4.7  p‐174

Hence

Dr. Sarmad Ullah Khan

73

Example 4.7  p‐174

Dr. Sarmad Ullah Khan

74

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Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) Modulation– Two methods are generally used to generate SSB

Dr. Sarmad Ullah Khan

Two methods are generally used to generate SSBsignals

1) Sharp cutoff filters

2) Phase shifting networks– In Sharp cutoff method, the DSB-SC signal is passed

through a sharp cutoff filter to eliminate the undesiredsidebandsideband

– To obtain USB, the filter should pass all componentsabove wc, attenuated and completely suppress allcomponents below wc

– Such an operation requires an ideal filter that ispractically not possible

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Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) ModulationThi th d f ti SSB i l b d

Dr. Sarmad Ullah Khan

– This method of generating SSB signal can be usedwhen there is some separation between the passbandand stopband

– In some application this can be achieved e.g. voicesignals

– Voice signals spectrum shows little power content atth i i Th filt i th t d id b d ithe origin. Thus filtering the unwanted sideband isrelatively easy

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Tests have shown that frequency components below 300Hz are not important.

600Hz transition region around the cutoff frequency wc , makes filtering easy and minimize the channel interference

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Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) ModulationThe basis of Phase shifting network method is the

Dr. Sarmad Ullah Khan

– The basis of Phase shifting network method is thefollowing equation

twtmtwtmt chcSSB sin)(cos)()(

77

Bandwidth Efficient Amplitude Modulation

• Single Sideband (SSB) ModulationThe basis of Phase shifting network method is the

Dr. Sarmad Ullah Khan

– The basis of Phase shifting network method is thefollowing equation

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Bandwidth Efficient Amplitude Modulation

• Quadrature Amplitude ModulationThe DSB signals of AM require twice the bandwidth

Dr. Sarmad Ullah Khan

– The DSB signals of AM require twice the bandwidthrequired for the baseband signal

– Try to send two signals m1(t) and m2(t) simultaneously bymodulating them with two carrier signals of samefrequency but shifted in phase by –/2

– The combined signal is

twtmtwtmtmtm sin)(cos)()()(

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twtmtwtmtmtm cc sin)(cos)()()( 2121

Bandwidth Efficient Amplitude Modulation

• Quadrature Amplitude ModulationBoth modulated signals occupy the same band

Dr. Sarmad Ullah Khan

– Both modulated signals occupy the same band– At the receiver the two baseband signals can be separated

by using a second carrier that is shifted in phase by –/2– The first signal m1(t) can be detected by a multiplication

with 2cos(ct) followed by a low-pass filter– The second signal m2(t) can be detected accordingly by a

multiplication with sin( t) followed by a low-pass filtermultiplication with sin(ct) followed by a low pass filter

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Bandwidth Efficient Amplitude Modulation

• Quadrature Amplitude ModulationThus two baseband signals each of bandwidth B can be

Dr. Sarmad Ullah Khan

– Thus, two baseband signals, each of bandwidth B, can besimultaneously transmitted over a channel with bandwidth2B

– This principle is called quadrature amplitudemodulation (QAM), because the carrier frequencies are inphase quadrature

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Outlines

• Baseband versus Carrier Communication

D bl id b d A lit d M d l ti

Dr. Sarmad Ullah Khan

• Double sideband Amplitude Modulation

• Amplitude Modulation

• Bandwidth Efficient Amplitude Modulation

• Amplitude Modulation: VESTIGIAL Sideband

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Amplitude Modulation: Vestigial Sideband (VSB)

• VSB is a compromise between DSB and SSB• It combines the advantages of DSB and SSB while avoid

Dr. Sarmad Ullah Khan

It combines the advantages of DSB and SSB while avoiddisadvantages at small cost

• Its generation is relatively easy and bandwidth requirement is25% greater than SSB

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Amplitude Modulation: Vestigial Sideband (VSB)

Dr. Sarmad Ullah Khan

• If vestigial shaping filter produce VBS from DSB is Hi(f), Itsspectrum will bespectrum will be

• VBS filter allows transmission of one sideband but suppressother side band gradually, NOT completely

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Amplitude Modulation: Vestigial Sideband (VSB)

Dr. Sarmad Ullah Khan

• For demodulation,

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