introduction to analog and digital communications 3.pdf · 3.5 quadrature-carrier multiplexing 3.6...
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Introduction to Analog And Digital Communications
Second Edition
Simon Haykin, Michael Moher
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Chapter 3 Amplitude Modulation
3.1 Amplitude Modulation3.2 Virtues, Limitations, and Modifications of Amplitude Modulation3.3 Double Sideband-Suppressed Carrier Modulation3.4 Costas Receiver3.5 Quadrature-Carrier Multiplexing3.6 Single-Sideband Modulation3.7 Vestigial Sideband Modulation3.8 Baseband Representation of Modulated Waves and Band-Pass Filters3.9 Theme Examples3.10 Summary and Discussion
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Modulation The process by which some characteristic of a carrier wave is varied in
accordance with an information-bearing signal. Continuous-wave modulation Amplitude modulation Frequency modulation
AM modulation family Amplitude modulation (AM) Double sideband-suppressed carrier (DSB-SC) Single sideband (SSB) Vestigial sideband (VSB)
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Lesson 1 : Fourier analysis provides a powerful mathematical tool for developing mathematical as well as physical insight into the spectral characterization of linear modulation strategies
Lesson 2 : The implementation of analog communication is significantly simplified by using AM, at the expense of transmitted power and channel bandwidth
Lesson 3 : The utilization of transmitted power and channel bandwidth is improved through well-defined modifications of an amplitude-modulated wave’s spectral content at the expense of increased system complexity.
There is no free lunch in designing a communication system: for every gain that is made, there is a price to be paid.
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3.1 Amplitude Modulation
Theory A sinusoidal carrier wave
An amplitude-modulated wave
The envelope of s(t) has essentially the same shape as the message signal m(t) provided that two conditions are satisfied : The amplitude of kam(t) is always less than unity
The carrier frequency fc is much greater than the highest frequency component W of the message signal
Envelope detector A device whose output traces the envelope of the AM wave acting as the input
signal
)1.3()2cos()( tfAtc cc π=
)2.3()2cos()](1[)( tftmkAts cac π+=
)3.3( allfor ,1)( ttmka <
)4.3(Wfc >>
Fig. 3.1
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Fig.3.1 Back Next
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The Fourier transform or spectrum of the AM wave s(t)
From the spectrum of Fig. 3.2(b) 1. As a result of the modulation process, the spectrum of the message signal m(t) for
negative frequencies extending from –W to 0 becomes completely visible for positive frequencies, provided that the carrier frequency satisfies the condition fc>W ; wherein lies the importance of the idea of “negative” frequencies, which was emphasized in chapter 2.
2. For positive frequencies, the portion of the spectrum of an AM wave lying above the carrier frequency fc is referred to as the upper sideband, whereas the symmetric portion below fc is referred to as the lower sideband.
)5.3()]()([2
)]()([2
)( ccca
ccc ffMffMAkffffAfS ++−+++−= δδ
)()2exp(
)]2exp()2[exp(21)2cos(
cc
ccc
fftfj
tfjtfjtf
−⇔
−+=
δπ
πππ
)()2exp()( cc ffMtfjtm −⇔π
Fig. 3.2
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3. For positive frequencies, the highest frequency component of the AM wave equals fc+W, and the lowest frequency component equals fc-W. The difference between these two frequencies defines the transmission bandwidth BT of the AM wave, which is exactly twice the message bandwidth W;
)6.3(2WBT =
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Fig.3.2 Back Next
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Fig. 3.3
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Fig.3.3 Back Next
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The average power delivered to a 1-ohm resistor by s(t) is comprised of three components
Figure 3.4 shows the percentage of total power in both side frequencies and in the carrier plotted versus the percentage modulation.
Notice that when the percentage modulation is less than 20 percent, the power in one side frequency is less than 1 percent of the total power in the AM wave.
22
22
2
81powerfrequency sideLower
81powerfrequency sideUpper
21power Carrier
c
c
c
A
A
A
µ
µ
=−
=−
=
Fig. 3.4
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Fig.3.4 Back Next
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Computation experiment : AM We will study sinusoidal modulation based on the following parameters
It is recommended that the number of frequency samples satisfies the condition
The modulation factor μ
HzfHzf
A
m
c
c
05.0frequency, Modulation4.0 frequency,Carrier
1 amplitude,Carrier
===
2000005.010
==≥r
s
ffM
tionovermodula toingcorrespond,0.2modulationpercent 100 toingcorrespond,0.1ationundermodul toingcorrespond,5.0
===
µµµ
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Modulation factor μ=0.5 The lower side frequency, the carrier, and the upper side frequency are
located at (fc-fm)=±0.35 Hz, fc=±0.4 Hz, and (fc+fm)=±0.45 Hz. The amplitude of both side frequencies is (μ/2)=0.25 times the amplitude of
the carrier
Modulation factor μ=1.0
Modulation factor μ=2.0
Fig. 3.5
Fig. 3.6
Fig. 3.7
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Fig.3.5 Back Next
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Fig.3.6 Back Next
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Fig.3.7 Back Next
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Enveloping detection Enveloping detector The AM wave is narrowband, which means that the carrier frequency is
large compared to the message bandwidth The percentage modulation in the AM wave is less than 100 percent
So that the capacitor C charges rapidly and thereby follows the applied voltage up to the positive peak when the diodes is conducting .
csf f
CRr 1)( <<+
WCR
f lc
11<<<<
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Computer experiment : Envelope detection for sinusoidal AM
The envelope detector output is shown in Fig. 3.9(c). The numerical values used in the computation of Fig. 3.9(c)
kHzfkHzW
FCkR
rR
c
l
f
s
20 frequency Carrier 1 bandwidth Message
01.0 eCapacitanc10 resistance Load
25 resistance Forwared75 resistance Source
===
Ω=
Ω=Ω=
µ
Fig. 3.9
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Fig.3.9 Back Next
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3.2 Virtues, Limitations, and Modifications of Amplitude Modulation
Practical Limitation Amplitude modulation is wasteful of transmitted power
The transmission of the carrier wave therefore represents a waste of power Amplitude modulation is wasteful of channel bandwidth
Insofar as the transmission of information is concerned, only one sideband is necessary, and the communication channel therefore needs to provide only the same bandwidth as the message signal.
It requires a transmission bandwidth equal to twice the message bandwidth
Three modifications of amplitude modulation Double sideband-suppressed carrier (DSB-SC) modulation
The transmitted wave consists of only the upper and lower sidebands But the channel bandwidth requirement is the same as before
Single sideband (SSB) modulation The modulated wave consists only of the upper sideband or the lower sideband To translate the spectrum of the modulating signal to a new location in the frequency
domain.
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Vestigial sideband (VSB) modulation One sideband is passed almost completely and just a trace, of the other
sideband is retained. The required channel bandwidth is slightly in excess of the message
bandwidth by an amount equal to the width of the vestigial sideband.
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3.3 Double sideband-suppressed carrier Modulation
Theory DSB-SC (product modulation) consists of the product of the message
signal and the carrier wave,
Fourier transform of s(t)
Its only advantage is saving transmitted power, which is important enough when the available transmitted power is at a premium
)8.3()()2cos( )()()(
tmtfAtmtcts
cc π==
)9.3()]()([21)( ccc ffMffMAfS ++−=
Fig. 3.10
Fig. 3.11
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Fig.3.10 Back Next
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Fig.3.11 Back Next
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Coherent detection (synchronous demodulation) The recovery of the message signal m(t) can be accomplished by first
multiplying s(t) with a locally generated sinusoidal wave and then low-pass filtering the product.
The product modulation output and the filter output are
)10.3()()cos(21)()4cos(
21
)()2cos()2cos()()2cos()(
''
'
'
tmAAtmtfAA
tmtftfAAtstfAtv
ccccc
cccc
cc
φφπ
φππφπ
++=
+=
+=
)2cos(21
21)(cos2 θθ +=
)cos(21)cos(
21)cos()cos( 212121 θθθθθθ −++=
)11.3()()cos(21)( '
0 tmAAtv cc φ=Fig. 3.12
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Fig.3.12 Back Next
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The quadrature null effect The zero demodulated signal, when occurs for Φ=±π/2 The phase error Φ in the local oscillator causes the detector output to be
attenuated by a factor equal to cos Φ
Fig. 3.13
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Fig.3.13 Back Next
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Computer experiment : DSB-SC1. Figure 3.14(a) displays 10 cycles of the DSB-SC modulated wave2. To perform coherent detection,
1. The product modulator’s otuput - Multiply the DSB-SC modulated wave by an exact replica of the carrier
2. The waveform of the coherent detector’s overall output - Pass the product through a low-pass filter
Fig. 3.14
Fig. 3.15(a)
Fig. 3.15(b)
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Fig.3.14 Back Next
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Fig.3.15(a) Back Next
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Fig. 3.15(b) Back Next
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3.4 Costas Receiver
Costas Receiver Consists of two coherent detectors supplied with the same input signal Two local oscillator signals that are in phase quadrature with respect to
each other I-channel : in-phase coherent detector Q-channel : quadrature-phase coherent detector
Phase control in the Costas receiver ceases with modulation, Which means that phase-lock would have to be re-established with the
reappearance of modulation
Fig. 3.16
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Fig.3.16 Back Next
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3.5 Quadrature-Carrier Multiplexing
Quadrature-Amplitude modulation (QAM) This scheme enables two DSB-SC modulated waves to occupy the same
channel bandwidth Bandwidth-conversion system This system send a pilot signal outside the passband of the modulated signal –
to maintain the synchronization
)12.3()2sin()()2cos()()( 21 tftmAtftmAts cccc ππ +=
Fig. 3.17
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Fig.3.17 Back Next
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3.6 Single-Sideband Modulation
Single-Sideband Modulation Suppress one of the two sideband in the DSB-SC modulated wave
Theory A DSB-SC modulator using the sinusoidal modulating wave
The resulting DSB-SC modulated wave is
Suppressing the second term in Eq. (3.13) the upper and lower SSB modulated wave are
)2cos()( tfAtm mm π=
)13.3(])(2cos[21])(2cos[
21
)2cos()2cos( )()()(
tffAAtffAA
tftfAAtmtctS
mcmcmcmc
mcmc
DSB
−++=
==
ππ
ππ
)14.3(])(2cos[21)( tffAAtS mcmcUSSB += π
)15.3()2sin()2sin(21)2cos()2cos(
21)( tftfAAtftfAAtS mcmcmcmcUSSB ππππ −=
)16.3()2sin()2sin(21)2cos()2cos(
21)( tftfAAtftfAAtS mcmcmcmcLSSB ππππ +=
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A sinusoidal SSB modulated wave
For a periodic message signal defined by the Fourier series, the SSB modulated wave is
For another periodic signal, the SSB modulated wave is
)18.3()2cos()( ∑=n
nn tfatm π
)17.3()2sin()2sin(21)2cos()2cos(
21)( tftfAAtftfAAtS mcmcmcmcSSB ππππ =
)19.3()2sin()2sin(21)2cos()2cos(
21)( tfatfAtfatfAtS n
nnccn
nnccSSB ππππ ∑∑=
)20.3()2sin()( ∑=∧
nnn tfatm π
)21.3()2sin()(2
)2cos()(2
)( tftmAtftmAtS cc
cc
SSB ππ∧
=
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1. Under appropriate conditions, the Fourier series representation of a periodic signal converges to the Fourier transform of a nonperiodic signal
2. A Hibert transformer is a wide-band phase-shifter whose frequency response is characterized in two parts as follows
The magnitude response is unity for all frequencies, both positive and negative
The phase response is +90 for positive frequencies.
)22.3()sgn()( fjfH −=
)23.3()2sin()(2
)2cos()(2
)( tftmAtftmAtS cc
cc ππ
∧
=
Fig. 3.18
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Fig.3.18 Back Next
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Modulators for SSB Frequency Discrimination Method For the design of the band-pass filter to be practically feasible, there must
be a certain separation between the two sidebands that is wide enough to accommodate the transition band of the band-pass filter.
Phase Discrimination Method Wide-band phase-shifter is designed to produce the Hilbert transform in
response to the incoming message signal. To interfere with the in-phase path so as to eliminate power in one of the
two sidebands, depending on whether upper SSB or lower SSB is the requirement.
Fig. 3.19
Fig. 3.20
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Fig.3.19 Back Next
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Fig.3.20 Back Next
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Coherent Detection of SSB Synchronization of a local oscillator in the receiver with the oscillator
responsible for generating the carrier in the transmitter The demodulation of SSB is further complicated by the additional
suppression of the upper or lower sideband. Frequency Translation Single sideband modulation is in fact a form of frequency translation Frequency changing Mixing Heterodyning
Up conversion : the unshaded part of the spectrum in Fig. 3.22(b)
Down conversion : the shaded part of the spectrum in Fig. 3.22(b)
Fig. 3.12
lfff += 12 12 fffl −=
lfff −= 12 21 fffl −=
Fig. 3.21
Fig. 3.22
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Fig.3.21 Back Next
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Fig.3.22 Back Next
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3.7 Vestigial Sideband Modulation
For the spectrally efficient transmission of wideband signals Typically, the spectra of wideband signals contain significant low frequencies,
which make it impractical to use SSB modulation. The spectral characteristics of wideband data befit the use of DSB-SC.
However, DSB-SC requires a transmission bandwidth equal to twice the message bandwidth, which violates the bandwidth conservation requirement.
Vestigial sideband (VSB) modulation Instead of completely removing a sideband, a trace of vestige of that sideband
is transmitted, the name “vestigial sideband” Instead of transmitting the other sideband in full, almost the whole of this
second band is also transmitted.
WfB vT +=
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Sideband Shaping Filter The band-pass filter is referred to as a sideband shaping filter The transmitted vestige compensates for the spectral portion missing from the
other sideband. The sideband shaping filter must itself satisfy the following condition.
Two properties of the sideband shaping filter1. The transfer function of the sideband shaping filter exhibits odd symmetry about the
carrier frequency
)26.3(for,1)()( WfWffHffH cc ≤≤−=−++
)27.3(for ),()()( WffffffHffufH cvccvc +<<−−−−=
)28.3(0for ,00for ,1
)(
<>
=ff
fu
)29.3()()( fHfH vv −=−
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2. The transfer function Hv(f) is required to satisfy the condition of Eq. (3.26) only for the frequency interval -W≤f ≤W
Fig. 3.23
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Fig.3.23 Back Next
Fig. 3.24
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Fig.3.24 Back Next
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Coherent Detection of VSB The demodulation of VSB consists of multiplying s(t) with a locally
generated sinusoid and then low-pass filtering the resulting product signal v(t)
Fourier transform of the product signal is
Shifting the VSB spectrum to the right and left
)32.3()]()([21)( '
ccc ffSffSAfV ++−=
)()( fSts ⇔
)33.3()()]()([21)( fHffMffMAfS ccc ++−=
)34.3()()]()2([21)( cccc ffHfMffMAffS −+−=−
)35.3()()]2()([21)( cccc ffHffMfMAffS +++=+
)2cos()()( ' tftsAtv cc π=
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The low-pass filter in the coherent detector has a cutoff frequency just slightly greater than the message bandwidth
The result demodulated signal is a scaled version of the desired message signal.
)]()2()()2([41
)]()()[(41)(
'
'
cccccc
cccc
ffHffMffHffMAA
ffHffHfMAAfV
+++−−+
++−=
)36.3()]()2()()2([41
)(41)(
'
'
cccccc
cc
ffHffMffHffMAA
fMAAfV
+++−−+
=
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3.8 Baseband Representation of Modulated Waves and Band=Pass Filters
Baseband Is used to designate the band of frequencies representing the original
signal as delivered by a source of information
Baseband Representation of Modulation Waves A linear modulated wave
The modulated wave in the compact form – canonical representation of linear modulated waves
)39.3()2sin()()2cos()()( 1 tftstftsts cQc ππ −=
)2cos()( tftc cπ=
)2sin()( tftc cπ=∧
)40.3()()()()()( tctstctsts QI
∧
−=
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The complex envelope of the modulated wave is
The complex carrier wave and the modulated wave is
The practical advantage of the complex envelope The highest frequency component of s(t) may be as large as fc+W, where fc is the
carrier frequency and W is the message bandwidth On the other hand, the highest frequency component of ŝ (t) is considerably smaller,
being limited by the message bandwidth W.
)41.3()()()(~
tjststs QI +=
)42.3( )2exp( )2sin()2cos(
)()()(~
tfjtfjtf
tcjtctc
c
cc
πππ
=+=
+=∧
)43.3()2exp()(Re
)()(Re)(
~
~~
=
=
tfjts
tctsts
cπ
Table. 3.1
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Table 3.1 Back Next
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Fig.3.25 Back Next
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Baseband Representation of Band-pass Filters The desire to develop the corresponding representation for band-pass filters,
including band-pass communication channels
We may determine Ĥ(f) by proceeding as follows Given the transfer function H(f) of a band-pass filter, which is defined for both
positive and negative frequencies, keep the part of H(f) that corresponds to positive frequencies; let H+(f) denote this part.
Shift H+(f) to the left along the frequency axis by an amount equal to fc, and scale it by the factor 2. The result so obtained defines the desired Ĥ(f).
Actual output y(t) is determined from the formula
(3.44)0for ),(2)(~
>=− ffHffH c
)45.3()2exp()(Re)(~
= tfjtyty cπ
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Fig.3.26 Back Next
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3.9 Theme Examples
Superheterodyne Receiver (supersht) Carrier-frequency tunning, the purpose of which is to select the desired
signal Filtering, which is required to separate the desired signal from other
modulated signals that may be picked up along the way. Amplification, which is intended to compensate for the loss of signal power
incurred in the course of transmission.
It overcomes the difficulty of having to build a tunable highly frequency-selective and variable filter
Intermediate frequency (IF) Because the signal is neither at the original input frequency nor at the final
baseband frequency
)46.3(LORFIF fff −=
Fig. 3.27
Table. 3.2
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Fig.3.27 Back Next
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table.3.2 Back Next
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Television Signals1. The video signal exhibits a large bandwidth and significant low-
frequency content, which suggest the use of vestigial sideband modulation.
2. The circuitry used for demodulation in the receiver should be simple and therefore inexpensive. This suggest the use of envelope detection, which requires the addition of a carrier to the VSB modulated wave.
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Fig.3.28 Back Next
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Frequency-Division Multiplexing To transmit a number of these signals over the same channel, the signals
must be kept apart so that they do not interfere with each other, and thus they can be separated at the receiving end.
Frequency-division multiplexing (FDM) Time-division multiplexing (TDM)
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Fig.3.29 Back Next
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Fig. 3.30
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Fig.3.30 Back Next
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3.10 Summary and Discussion
The example modulated wave is
1. Amplitude modulation (AM), in which the upper and lower sidebands are transmitted in full, accompanied by the carrier wave Demodulation of the AM wave is accomplished equally simply in the receiver by
using an envelope detector2. Double sideband-suppressed carrier (DSB-SC) modulation, in which only
the upper and lower sidebands are transmitted. This advantage of DSB-SC modulation over AM is, attained at the expense of
increased receiver complexity.3. Single sideband (SSB) modulation, in which only the upper sideband or
lower sideband is transmitted. It requires the minimum transmitted power and the minimum channel bandwidth
for conveying a message signal from one point to another.4. Vestigial sideband modulation, in which “almost” the whole of one
sideband and a “vestige” of the other sideband are transmitted in a prescribed complementary fashion VSB modulation requires an channel bandwidth that is intermediate between
that required for SSB and DSB-SC systems, and the saving in bandwidth can be significant if modulating signals with large bandwidths are being handled.
)47.3()2cos()()( tftmAts cc π=
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Fig.3.8 Back Next
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Fig.3.31 Back Next
81