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3/18/2014
1
Communication Systems
Instructor: Engr. Dr. Sarmad Ullah Khan
Assistant ProfessorAssistant Professor
Electrical Engineering Department
CECOS University of IT and Emerging Sciences
Sarmad@cecos.edu.pk
Chapter 4
Dr. Sarmad Ullah Khan
Amplitude Modulations and
Demodulations
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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
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
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Baseband versus Carrier Communication
• Modulation is a process that moves signal into a
specific 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 g
power above a certain threshold (typically half of
the maximum power)
5
Baseband versus Carrier Communication
• Communication systems that do not use modulation
are 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
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Baseband versus Carrier Communication
• Baseband Communication
Message signals are directly transmitted without any
Dr. Sarmad Ullah Khan
Message signals are directly transmitted without any
modulation
Dedicated user channels are assigned to each long distance
communication
Baseband signals have overlapping bands
Severe interference
Waste of channel resourcesWaste of channel resources
Modulation and shifting to non overlapping bands save
channel resources
7
Baseband versus Carrier Communication
• Carrier Communication
Modulation techniques is used to shift the frequency
Dr. Sarmad Ullah Khan
Modulation techniques is used to shift the frequency
spectrum of message signal
Modulation changes one of the basic parameter of carrier
signal (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 linearAmplitude modulation is linear
Frequency and Phase modulations are non linears
PAM, PWM, PPM, PCM and DM are baseband signals
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Baseband versus Carrier Communication
• Amplitude Modulation and Angle Modulation
Amplitude modulation (AM) varies the amplitude of a
Dr. Sarmad Ullah Khan
Amplitude modulation (AM) varies the amplitude of a
carrier signal according to a modulating
signal m(t).
 The modulated signal is
)cos(
c
t
c
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
1
cos)( ccc wwMwwMtwtm 
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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
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
1
2cos)( ccc ffMffMtftm 
 The modulated signal is composed of two parts, above
fc and below fc
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Double Sideband Amplitude Modulation
• Amplitude Modulation and Angle Modulation
The 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 this
reason this is called double sideband suppressedreason this is called double-sideband suppressed
carrier (DSB-SC) modulation
13
Double Sideband Amplitude Modulation
• Amplitude Modulation and Angle Modulation
B vs f
Dr. Sarmad Ullah Khan
B vs fc
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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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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
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Double Sideband Amplitude Modulation
• Modulation and Demodulation
Dr. Sarmad Ullah Khan
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Double Sideband Amplitude Modulation
• Modulation and Demodulation
Dr. Sarmad Ullah Khan
 )2cos()()(
2
1cos)()( 2
twtmtmtwtmte cc

20
 )2()2(
4
1)(
2
1)( cc
wwMwwMwMwE 
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Double Sideband Amplitude Modulation
• Modulators
Multiplier Modulators
Dr. Sarmad Ullah Khan
Multiplier Modulators
Modulation 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
• Modulators
Non Linear Modulators
Dr. Sarmad Ullah Khan
Non Linear Modulators
Modulation can be achieved by using non linear device
For example, diodes or transistors
Input-output characteristics of NL element is approx. by
power series as
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Double Sideband Amplitude Modulation
• Modulators
Non Linear Modulators
Dr. Sarmad Ullah Khan
Non Linear Modulators
The summer output z(t) is given by
23
Double Sideband Amplitude Modulation
• Modulators
Non Linear Modulators
Dr. Sarmad Ullah Khan
Non Linear Modulators
Substitution of x1(t)=coswct+m(t) and x2(t)=coswct-m(t)
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Double Sideband Amplitude Modulation
• Modulators
Non Linear Modulators
Dr. Sarmad Ullah Khan
Non Linear Modulators
Spectrum of m(t) is centered at origin
Spectrum of m(t) coswct is centered at ±ω
The 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 signal
4bm(t)coswct pass without distortion
25
Double Sideband Amplitude Modulation
• Modulators
Non Linear Modulators (summary)
Dr. Sarmad Ullah Khan
Non Linear Modulators (summary)
Two inputs m(t) and coswct
The summer output does not contain one of the input coswct
Circuits 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) still
appear at the filter input, which must reject it…….for that reason it is
called a single balanced modulator
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Double Sideband Amplitude Modulation
• Modulators
Modulation through any periodic signal
Dr. Sarmad Ullah Khan
Modulation through any periodic signal
Modulated 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 Fourier
Series
Spectrum of the modulated signal is the spectrum M(w) shifted to
±fc , ±2fc , ±3fc , ±4fc , …… ±nfc ,……
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Double Sideband Amplitude Modulation
• Modulators
Modulation through any periodic signal
Dr. Sarmad Ullah Khan
Modulation through any periodic signal
If we pass this modulated signal through band-pass filter of
bandwidth 2B tuned to wc
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Double Sideband Amplitude Modulation
• Modulators
Switching Modulators
Dr. Sarmad Ullah Khan
Switching Modulators
Multiplication 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
1
5cos
5
1
3cos
3
1
cos
2
2
1
)( twtwtwtwtw cccc

From example 2.8
Double Sideband Amplitude Modulation
• Modulators
Switching Modulators
Dr. Sarmad Ullah Khan
Switching Modulators
The modulated signal m(t)w(t) is given by






 ....7cos)(
7
1
5cos)(
5
1
3cos)(
3
1
cos)(
2
)(
2
1
)()( twtmtwtmtwtmtwtmtmtwtm cccc

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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, ccc
www
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, ccc
www 
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
twtm c
cos)(
c
w
31
gives the required modulated signal twtm c
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
• Modulators
Diode Bridge Modulator
Dr. Sarmad Ullah Khan
Diode Bridge Modulator
Consider 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
• Modulators
Diode Bridge Modulator
Dr. Sarmad Ullah Khan
Diode Bridge Modulator
Therefore the the circuit act as a desired electronic switch, where
the terminal a & b open and close periodically with the carrier
frequency fc. When is applied across the terminal ab
To obtain m(t)w(t) we may place terminal ab in series or in parallel
as:
twA ccos
Switching on and off m(t) for each cycle of the carrier, resulting in
the switched signal m(t)w(t) and passing through band pass filter
gives the desired signal:
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Series-bridge diode modulator Shunt-bridge diode modulator
Double Sideband Amplitude Modulation
• Modulators
Ring 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 and
D2 & D4 conduct, hence terminal a is connected to d & b to c
Output is proportional to m(t) during positive cycle & -m(t) during
negative cycle
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Double Sideband Amplitude Modulation
• Modulators
Ring Modulator
Dr. Sarmad Ullah Khan
Ring Modulator
The Fourier series of bipolar square wave is given by:






 ....7cos
7
1
5cos
5
1
3cos
3
1
cos
4
)(0 twtwtwtwtw cccc







 ....7cos)(
7
1
5cos)(
5
1
3cos)(
3
1
cos)(
4
)()( 0 twtmtwtmtwtmtwtmtwtm cccc

Filtering 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 the
final 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 Signals
The demodulation involve multiplication of DSB SC
Dr. Sarmad Ullah Khan
The demodulation involve multiplication of DSB-SC
with carrier signal
At receiver incoming signal multiply with local carrier
Local carrier must have frequency and phase
synchronization with incoming signal
Product is passed to low pass filter
Such demodulators are called synchronous or coherent
or homodyne demodulators
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Problem 4.2‐4
Dr. Sarmad Ullah Khan
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Problem 4.2‐4
Dr. Sarmad Ullah Khan
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Problem 4.2‐4
Dr. Sarmad Ullah Khan
At point b
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At point c
Problem 4.2‐4
The minimum value of wc is to avoid overlapping
Dr. Sarmad Ullah Khan
pp g
40
Will 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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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 a
carrier 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 the
receiver
45
Amplitude Modulation
• This type of modulation is called AM modulation and
denoted by and given by
Dr. Sarmad Ullah Khan
)(ty g y
• Its Fourier spectrum is
)(tAM

• The spectrum of is the same as m(t)coswct plus two
additional 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 envelop
would 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
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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 is
A ≥ - mmin = mp
Modulation index μ is
μ = mp/A
F l d t ti t b di t ti lFor envelop detection to be distortion less
0 ≤ μ ≤ 1
This is required condition for distortion less
demodulation 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 offset
Maximum mmax and minimum mmin are not symmetric
mmin ≠ mmax
Change in offset does not change the envelop detector
output and
0 ≤ μ ≤ 1μ
But
μ = (mmax - mmin) / (2A + mmax + mmin)
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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 of
power waste, as the carrier term does not contain any
information
The carrier power Pc and sideband power Ps is given by
Power efficiency is given by
51
Amplitude Modulation
• Sideband and Carrier Power
For 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 signals
the efficiency is even worst
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Amplitude Modulation
• Generation of AM signal
AM 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:
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Amplitude Modulation
• Demodulation of AM signal
The AM signal can be demodulated coherently by a locally
Dr. Sarmad Ullah Khan
The AM signal can be demodulated coherently by a locally
generated carrier. E.g.
There are two well known methods of demodulation of AM
signals:
 1) Rectifier detection 2) Envelope detection
   twtwtmA cc coscos)( No benefit of sending carrier on the channel
 1) Rectifier detection 2) Envelope detection
Rectifier detector:
AM signal is applied to a diode and resistor circuit, the negative
part of the AM wave will be suppressed.
The output across the resistor is the half wave rectified version of
the AM signal means multiplying AM with w(t).
55
Amplitude Modulation
• Demodulation of AM signal
Rectifier detector:
Dr. Sarmad Ullah Khan
Rectifier detector:
The rectified output VR
  
56
   )(cos)( twt
c
wtmAvR

  











 ...5cos
5
1
3cos
3
1
cos
2
2
1
cos)( t
c
wt
c
wt
c
wt
c
wtmA

  otherTermstmA  )(
1

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Amplitude Modulation
• Demodulation of AM signal
Rectifier detector:
Dr. Sarmad Ullah Khan
Rectifier detector:
57
Amplitude Modulation
• Demodulation of AM signal
Envelop detector:
Dr. Sarmad Ullah Khan
Envelop detector:
In an envelope detector, the output follows the envelope
of the modulated signal
The following circuit act as an envelope detector
During the positive cycle of the input signal, the diode
conducts and the capacitor C charges up to the peak
voltage of the input signal
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Amplitude Modulation
• Demodulation of AM signal
Envelop detector:
Dr. Sarmad Ullah Khan
Envelop detector:
When input signal falls below this peak value, the diode
i t ff (b th di d lt hi h i l this cut off. (because the diode voltage which is nearly the
peak voltage is greater than the input signal voltage
causing 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 signal
Envelop detector:
Dr. Sarmad Ullah Khan
p
During each positive cycle the capacitor charges up to theDuring each positive cycle the capacitor charges up to the
peak voltage of the input signal and then decays slowly until
the next positive cycle
This behavior of the capacitor makes output voltage Vc(t)
follow the envelope of the input signal
Capacitor discharges during each positive peaks causes a
ripple signal of frequency wc at the output
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Amplitude Modulation
• Demodulation of AM signal
Envelop detector:
Dr. Sarmad Ullah Khan
Envelop detector:
The ripple can be reduced by increasing the time
constant RC so the capacitor discharges very little
between positive peaks of the input signals
Making RC too large, makes capacitor voltage
impossible to follow the envelope
61
Amplitude Modulation
• Demodulation of AM signal
Envelop 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)
B2
1
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
3/18/2014
33
Bandwidth Efficient Amplitude 
Modulation
• Single Sideband (SSB) Modulation
LSB 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 half
compared to DSB signalp g
– An SSB signal can be coherently (synchronously)
demodulated. E.g
– For example multiplying USB signal by coswct
shifts its spectrum to the left and right by wc
65
Bandwidth Efficient Amplitude 
Modulation
• Single Sideband (SSB) Modulation
L filt i ill i th i d b b d
Dr. Sarmad Ullah Khan
– Low pass filtering will give the required baseband
signal at the receiver
66
3/18/2014
34
Bandwidth Efficient Amplitude 
Modulation
• Single Sideband (SSB) Modulation
Hilb 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) Modulation
Hilb t T f
Dr. Sarmad Ullah Khan
– Hilbert Transform
– xh(t) and H{x(t)} to denote Hilbert transform of
x(t)
68
3/18/2014
35
Bandwidth Efficient Amplitude 
Modulation
• Single Sideband (SSB) Modulation
Ti 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 plus
sign applies to LSB
twtmtwtmt chcSSB sin)(cos)()( 
69
Bandwidth Efficient Amplitude 
Modulation
• Single Sideband (SSB) Modulation
Dr. Sarmad Ullah Khan
70
3/18/2014
36
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
)(SSB
twtm mcos)( 
Solution:
twtmtwtmt chcSSB sin)(cos)()( 
72
3/18/2014
37
Example 4.7  p‐174
Hence
Dr. Sarmad Ullah Khan
73
Example 4.7  p‐174
Dr. Sarmad Ullah Khan
74
3/18/2014
38
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 SSB
signals
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 undesired
sidebandsideband
– To obtain USB, the filter should pass all components
above wc, attenuated and completely suppress all
components below wc
– Such an operation requires an ideal filter that is
practically not possible
75
Bandwidth Efficient Amplitude 
Modulation
• Single Sideband (SSB) Modulation
Thi th d f ti SSB i l b d
Dr. Sarmad Ullah Khan
– This method of generating SSB signal can be used
when there is some separation between the passband
and stopband
– In some application this can be achieved e.g. voice
signals
– Voice signals spectrum shows little power content at
th i i Th filt i th t d id b d ithe origin. Thus filtering the unwanted sideband is
relatively easy
76
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
3/18/2014
39
Bandwidth Efficient Amplitude 
Modulation
• Single Sideband (SSB) Modulation
The basis of Phase shifting network method is the
Dr. Sarmad Ullah Khan
– The basis of Phase shifting network method is the
following equation
twtmtwtmt chcSSB sin)(cos)()( 
77
Bandwidth Efficient Amplitude 
Modulation
• Single Sideband (SSB) Modulation
The basis of Phase shifting network method is the
Dr. Sarmad Ullah Khan
– The basis of Phase shifting network method is the
following equation
78
3/18/2014
40
Bandwidth Efficient Amplitude 
Modulation
• Quadrature Amplitude Modulation
The DSB signals of AM require twice the bandwidth
Dr. Sarmad Ullah Khan
– The DSB signals of AM require twice the bandwidth
required for the baseband signal
– Try to send two signals m1(t) and m2(t) simultaneously by
modulating them with two carrier signals of same
frequency but shifted in phase by –/2
– The combined signal is
twtmtwtmtmtm sin)(cos)()()( 
79
twtmtwtmtmtm cc sin)(cos)()()( 2121 
Bandwidth Efficient Amplitude 
Modulation
• Quadrature Amplitude Modulation
Both 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
80
3/18/2014
41
Bandwidth Efficient Amplitude 
Modulation
• Quadrature Amplitude Modulation
Thus two baseband signals each of bandwidth B can be
Dr. Sarmad Ullah Khan
– Thus, two baseband signals, each of bandwidth B, can be
simultaneously transmitted over a channel with bandwidth
2B
– This principle is called quadrature amplitude
modulation (QAM), because the carrier frequencies are in
phase quadrature
81
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
82
3/18/2014
42
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 avoid
disadvantages at small cost
• Its generation is relatively easy and bandwidth requirement is
25% greater than SSB
83
Amplitude Modulation: Vestigial 
Sideband (VSB)
Dr. Sarmad Ullah Khan
• If vestigial shaping filter produce VBS from DSB is Hi(f), Its
spectrum will bespectrum will be
• VBS filter allows transmission of one sideband but suppress
other side band gradually, NOT completely
84
3/18/2014
43
Amplitude Modulation: Vestigial 
Sideband (VSB)
Dr. Sarmad Ullah Khan
• For demodulation,
85

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Chapter 4

  • 1. 3/18/2014 1 Communication Systems Instructor: Engr. Dr. Sarmad Ullah Khan Assistant ProfessorAssistant Professor Electrical Engineering Department CECOS University of IT and Emerging Sciences Sarmad@cecos.edu.pk Chapter 4 Dr. Sarmad Ullah Khan Amplitude Modulations and Demodulations 2
  • 2. 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
  • 3. 3/18/2014 3 Baseband versus Carrier Communication • Modulation is a process that moves signal into a specific 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 g power above a certain threshold (typically half of the maximum power) 5 Baseband versus Carrier Communication • Communication systems that do not use modulation are 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
  • 4. 3/18/2014 4 Baseband versus Carrier Communication • Baseband Communication Message signals are directly transmitted without any Dr. Sarmad Ullah Khan Message signals are directly transmitted without any modulation Dedicated user channels are assigned to each long distance communication Baseband signals have overlapping bands Severe interference Waste of channel resourcesWaste of channel resources Modulation and shifting to non overlapping bands save channel resources 7 Baseband versus Carrier Communication • Carrier Communication Modulation techniques is used to shift the frequency Dr. Sarmad Ullah Khan Modulation techniques is used to shift the frequency spectrum of message signal Modulation changes one of the basic parameter of carrier signal (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 linearAmplitude modulation is linear Frequency and Phase modulations are non linears PAM, PWM, PPM, PCM and DM are baseband signals 8
  • 5. 3/18/2014 5 Baseband versus Carrier Communication • Amplitude Modulation and Angle Modulation Amplitude modulation (AM) varies the amplitude of a Dr. Sarmad Ullah Khan Amplitude modulation (AM) varies the amplitude of a carrier signal according to a modulating signal m(t).  The modulated signal is )cos( c t c 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 1 cos)( ccc wwMwwMtwtm 
  • 6. 3/18/2014 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 1 2cos)( ccc ffMffMtftm   The modulated signal is composed of two parts, above fc and below fc 12
  • 7. 3/18/2014 7 Double Sideband Amplitude Modulation • Amplitude Modulation and Angle Modulation The 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 this reason this is called double sideband suppressedreason this is called double-sideband suppressed carrier (DSB-SC) modulation 13 Double Sideband Amplitude Modulation • Amplitude Modulation and Angle Modulation B vs f Dr. Sarmad Ullah Khan B vs fc 14
  • 8. 3/18/2014 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  
  • 9. 3/18/2014 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
  • 10. 3/18/2014 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()()( 2 1cos)()( 2 twtmtmtwtmte cc  20  )2()2( 4 1)( 2 1)( cc wwMwwMwMwE 
  • 11. 3/18/2014 11 Double Sideband Amplitude Modulation • Modulators Multiplier Modulators Dr. Sarmad Ullah Khan Multiplier Modulators Modulation 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 • Modulators Non Linear Modulators Dr. Sarmad Ullah Khan Non Linear Modulators Modulation can be achieved by using non linear device For example, diodes or transistors Input-output characteristics of NL element is approx. by power series as 22
  • 12. 3/18/2014 12 Double Sideband Amplitude Modulation • Modulators Non Linear Modulators Dr. Sarmad Ullah Khan Non Linear Modulators The summer output z(t) is given by 23 Double Sideband Amplitude Modulation • Modulators Non Linear Modulators Dr. Sarmad Ullah Khan Non Linear Modulators Substitution of x1(t)=coswct+m(t) and x2(t)=coswct-m(t) 24
  • 13. 3/18/2014 13 Double Sideband Amplitude Modulation • Modulators Non Linear Modulators Dr. Sarmad Ullah Khan Non Linear Modulators Spectrum of m(t) is centered at origin Spectrum of m(t) coswct is centered at ±ω The 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 signal 4bm(t)coswct pass without distortion 25 Double Sideband Amplitude Modulation • Modulators Non Linear Modulators (summary) Dr. Sarmad Ullah Khan Non Linear Modulators (summary) Two inputs m(t) and coswct The summer output does not contain one of the input coswct Circuits 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) still appear at the filter input, which must reject it…….for that reason it is called a single balanced modulator
  • 14. 3/18/2014 14 Double Sideband Amplitude Modulation • Modulators Modulation through any periodic signal Dr. Sarmad Ullah Khan Modulation through any periodic signal Modulated 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 Fourier Series Spectrum of the modulated signal is the spectrum M(w) shifted to ±fc , ±2fc , ±3fc , ±4fc , …… ±nfc ,…… 27 Double Sideband Amplitude Modulation • Modulators Modulation through any periodic signal Dr. Sarmad Ullah Khan Modulation through any periodic signal If we pass this modulated signal through band-pass filter of bandwidth 2B tuned to wc 28
  • 15. 3/18/2014 15 Double Sideband Amplitude Modulation • Modulators Switching Modulators Dr. Sarmad Ullah Khan Switching Modulators Multiplication 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 1 5cos 5 1 3cos 3 1 cos 2 2 1 )( twtwtwtwtw cccc  From example 2.8 Double Sideband Amplitude Modulation • Modulators Switching Modulators Dr. Sarmad Ullah Khan Switching Modulators The modulated signal m(t)w(t) is given by        ....7cos)( 7 1 5cos)( 5 1 3cos)( 3 1 cos)( 2 )( 2 1 )()( twtmtwtmtwtmtwtmtmtwtm cccc  30
  • 16. 3/18/2014 16 Modulated signal m(t)w(t) consists of the component m(t) plus infinite numbers of modulated signals with carrier frequencies ,.....5,3, ccc www 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, ccc www  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 twtm c cos)( c w 31 gives the required modulated signal twtm c 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 • Modulators Diode Bridge Modulator Dr. Sarmad Ullah Khan Diode Bridge Modulator Consider 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.
  • 17. 3/18/2014 17 Double Sideband Amplitude Modulation • Modulators Diode Bridge Modulator Dr. Sarmad Ullah Khan Diode Bridge Modulator Therefore the the circuit act as a desired electronic switch, where the terminal a & b open and close periodically with the carrier frequency fc. When is applied across the terminal ab To obtain m(t)w(t) we may place terminal ab in series or in parallel as: twA ccos Switching on and off m(t) for each cycle of the carrier, resulting in the switched signal m(t)w(t) and passing through band pass filter gives the desired signal: 33 Series-bridge diode modulator Shunt-bridge diode modulator Double Sideband Amplitude Modulation • Modulators Ring 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 and D2 & D4 conduct, hence terminal a is connected to d & b to c Output is proportional to m(t) during positive cycle & -m(t) during negative cycle 34
  • 18. 3/18/2014 18 Double Sideband Amplitude Modulation • Modulators Ring Modulator Dr. Sarmad Ullah Khan Ring Modulator The Fourier series of bipolar square wave is given by:        ....7cos 7 1 5cos 5 1 3cos 3 1 cos 4 )(0 twtwtwtwtw cccc         ....7cos)( 7 1 5cos)( 5 1 3cos)( 3 1 cos)( 4 )()( 0 twtmtwtmtwtmtwtmtwtm cccc  Filtering 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 the final 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 Signals The demodulation involve multiplication of DSB SC Dr. Sarmad Ullah Khan The demodulation involve multiplication of DSB-SC with carrier signal At receiver incoming signal multiply with local carrier Local carrier must have frequency and phase synchronization with incoming signal Product is passed to low pass filter Such demodulators are called synchronous or coherent or homodyne demodulators 36
  • 20. 3/18/2014 20 Problem 4.2‐4 Dr. 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 40 Will not work
  • 21. 3/18/2014 21 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
  • 22. 3/18/2014 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
  • 23. 3/18/2014 23 Amplitude Modulation • The demodulation requires the receiver to possess a carrier 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 the receiver 45 Amplitude Modulation • This type of modulation is called AM modulation and denoted by and given by Dr. Sarmad Ullah Khan )(ty g y • Its Fourier spectrum is )(tAM  • The spectrum of is the same as m(t)coswct plus two additional impulses at ±ω 46 )(tAM 
  • 24. 3/18/2014 24 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 envelop would 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
  • 25. 3/18/2014 25 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 is A ≥ - mmin = mp Modulation index μ is μ = mp/A F l d t ti t b di t ti lFor envelop detection to be distortion less 0 ≤ μ ≤ 1 This is required condition for distortion less demodulation 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 offset Maximum mmax and minimum mmin are not symmetric mmin ≠ mmax Change in offset does not change the envelop detector output and 0 ≤ μ ≤ 1μ But μ = (mmax - mmin) / (2A + mmax + mmin) 50
  • 26. 3/18/2014 26 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 of power waste, as the carrier term does not contain any information The carrier power Pc and sideband power Ps is given by Power efficiency is given by 51 Amplitude Modulation • Sideband and Carrier Power For 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 signals the efficiency is even worst 52
  • 27. 3/18/2014 27 Amplitude Modulation • Generation of AM signal AM 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
  • 28. 3/18/2014 28 Amplitude Modulation • Demodulation of AM signal The AM signal can be demodulated coherently by a locally Dr. Sarmad Ullah Khan The AM signal can be demodulated coherently by a locally generated carrier. E.g. There are two well known methods of demodulation of AM signals:  1) Rectifier detection 2) Envelope detection    twtwtmA cc coscos)( No benefit of sending carrier on the channel  1) Rectifier detection 2) Envelope detection Rectifier detector: AM signal is applied to a diode and resistor circuit, the negative part of the AM wave will be suppressed. The output across the resistor is the half wave rectified version of the AM signal means multiplying AM with w(t). 55 Amplitude Modulation • Demodulation of AM signal Rectifier detector: Dr. Sarmad Ullah Khan Rectifier detector: The rectified output VR    56    )(cos)( twt c wtmAvR                 ...5cos 5 1 3cos 3 1 cos 2 2 1 cos)( t c wt c wt c wt c wtmA    otherTermstmA  )( 1 
  • 29. 3/18/2014 29 Amplitude Modulation • Demodulation of AM signal Rectifier detector: Dr. Sarmad Ullah Khan Rectifier detector: 57 Amplitude Modulation • Demodulation of AM signal Envelop detector: Dr. Sarmad Ullah Khan Envelop detector: In an envelope detector, the output follows the envelope of the modulated signal The following circuit act as an envelope detector During the positive cycle of the input signal, the diode conducts and the capacitor C charges up to the peak voltage of the input signal 58
  • 30. 3/18/2014 30 Amplitude Modulation • Demodulation of AM signal Envelop detector: Dr. Sarmad Ullah Khan Envelop detector: When input signal falls below this peak value, the diode i t ff (b th di d lt hi h i l this cut off. (because the diode voltage which is nearly the peak voltage is greater than the input signal voltage causing 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 signal Envelop detector: Dr. Sarmad Ullah Khan p During each positive cycle the capacitor charges up to theDuring each positive cycle the capacitor charges up to the peak voltage of the input signal and then decays slowly until the next positive cycle This behavior of the capacitor makes output voltage Vc(t) follow the envelope of the input signal Capacitor discharges during each positive peaks causes a ripple signal of frequency wc at the output 60
  • 31. 3/18/2014 31 Amplitude Modulation • Demodulation of AM signal Envelop detector: Dr. Sarmad Ullah Khan Envelop detector: The ripple can be reduced by increasing the time constant RC so the capacitor discharges very little between positive peaks of the input signals Making RC too large, makes capacitor voltage impossible to follow the envelope 61 Amplitude Modulation • Demodulation of AM signal Envelop 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) B2 1 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.
  • 32. 3/18/2014 32 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
  • 33. 3/18/2014 33 Bandwidth Efficient Amplitude  Modulation • Single Sideband (SSB) Modulation LSB 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 half compared to DSB signalp g – An SSB signal can be coherently (synchronously) demodulated. E.g – For example multiplying USB signal by coswct shifts its spectrum to the left and right by wc 65 Bandwidth Efficient Amplitude  Modulation • Single Sideband (SSB) Modulation L filt i ill i th i d b b d Dr. Sarmad Ullah Khan – Low pass filtering will give the required baseband signal at the receiver 66
  • 34. 3/18/2014 34 Bandwidth Efficient Amplitude  Modulation • Single Sideband (SSB) Modulation Hilb 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) Modulation Hilb t T f Dr. Sarmad Ullah Khan – Hilbert Transform – xh(t) and H{x(t)} to denote Hilbert transform of x(t) 68
  • 35. 3/18/2014 35 Bandwidth Efficient Amplitude  Modulation • Single Sideband (SSB) Modulation Ti 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 plus sign applies to LSB twtmtwtmt chcSSB sin)(cos)()(  69 Bandwidth Efficient Amplitude  Modulation • Single Sideband (SSB) Modulation Dr. Sarmad Ullah Khan 70
  • 36. 3/18/2014 36 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 )(SSB twtm mcos)(  Solution: twtmtwtmt chcSSB sin)(cos)()(  72
  • 38. 3/18/2014 38 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 SSB signals 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 undesired sidebandsideband – To obtain USB, the filter should pass all components above wc, attenuated and completely suppress all components below wc – Such an operation requires an ideal filter that is practically not possible 75 Bandwidth Efficient Amplitude  Modulation • Single Sideband (SSB) Modulation Thi th d f ti SSB i l b d Dr. Sarmad Ullah Khan – This method of generating SSB signal can be used when there is some separation between the passband and stopband – In some application this can be achieved e.g. voice signals – Voice signals spectrum shows little power content at th i i Th filt i th t d id b d ithe origin. Thus filtering the unwanted sideband is relatively easy 76 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
  • 39. 3/18/2014 39 Bandwidth Efficient Amplitude  Modulation • Single Sideband (SSB) Modulation The basis of Phase shifting network method is the Dr. Sarmad Ullah Khan – The basis of Phase shifting network method is the following equation twtmtwtmt chcSSB sin)(cos)()(  77 Bandwidth Efficient Amplitude  Modulation • Single Sideband (SSB) Modulation The basis of Phase shifting network method is the Dr. Sarmad Ullah Khan – The basis of Phase shifting network method is the following equation 78
  • 40. 3/18/2014 40 Bandwidth Efficient Amplitude  Modulation • Quadrature Amplitude Modulation The DSB signals of AM require twice the bandwidth Dr. Sarmad Ullah Khan – The DSB signals of AM require twice the bandwidth required for the baseband signal – Try to send two signals m1(t) and m2(t) simultaneously by modulating them with two carrier signals of same frequency but shifted in phase by –/2 – The combined signal is twtmtwtmtmtm sin)(cos)()()(  79 twtmtwtmtmtm cc sin)(cos)()()( 2121  Bandwidth Efficient Amplitude  Modulation • Quadrature Amplitude Modulation Both 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 80
  • 41. 3/18/2014 41 Bandwidth Efficient Amplitude  Modulation • Quadrature Amplitude Modulation Thus two baseband signals each of bandwidth B can be Dr. Sarmad Ullah Khan – Thus, two baseband signals, each of bandwidth B, can be simultaneously transmitted over a channel with bandwidth 2B – This principle is called quadrature amplitude modulation (QAM), because the carrier frequencies are in phase quadrature 81 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 82
  • 42. 3/18/2014 42 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 avoid disadvantages at small cost • Its generation is relatively easy and bandwidth requirement is 25% greater than SSB 83 Amplitude Modulation: Vestigial  Sideband (VSB) Dr. Sarmad Ullah Khan • If vestigial shaping filter produce VBS from DSB is Hi(f), Its spectrum will bespectrum will be • VBS filter allows transmission of one sideband but suppress other side band gradually, NOT completely 84