Chapter one Introduction Analog and Digital Communicatione4uhu.com/down/Analog/analog-slides.pdf ·...

414
١ Chapter one Introduction Analog and Digital Communication

Transcript of Chapter one Introduction Analog and Digital Communicatione4uhu.com/down/Analog/analog-slides.pdf ·...

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Chapter one

Introduction

Analog and Digital Communication

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Introduction to Communication Systems

What is a communication system?

Any means for transmission of information.

Examples: Telephone, Telegraph, Mobile phone, TV, Radio, Internet, hard disk in a PC, Radar, Satellite, microwave link,…

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Elements of a Communication System

Communication involves the transfer of information

or intelligence

from a source

to a recipient

via a channel

or medium.•

Basic block diagram of a communication system:

Source Transmitter Receiver Recipient

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Brief Description

Source: emits analog or digital data.•

Transmitter: transducer, amplifier, modulator, oscillator, power amp., antenna

Channel: e.g. cable, optical fiber, waveguide, radio link (free space)

Receiver: antenna, amplifier, demodulator, oscillator, power amplifier, transducer

Recipient: e.g. person, speaker, computer

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Transmitter•

It may include transducer, amplifier, modulator, oscillator, power amplifier and antenna.

It modifies the message or the baseband

signal for efficient transmission by a process called modulation.

Other functions: filtering, amplification, radiation

Presenter
Presentation Notes
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Modulation

Modulation: the process by which the base band signal is used to modify some parameter of a high frequency carrier.

Types of modulation•

Continuous wave (CW) modulation.–

RF sinusoidal carrier wave(30K-300GHz).

Pulse modulation.–

RF pulse carrier wave.

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Why modulation?

For ease of radiation.•

Modulation for multiplexing.

For exchange of SNR with B.•

To over come equipment limitation.

To match channel characteristics.

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Example of analog modulation

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Channel•

It is the physical medium between the transmitter and the receiver. It can be guided, as optical fiber cables, waveguide, or unguided as radio link, water, free space.

Whatever the medium, the signal is corrupted in a random manner by noise and interference (thermal noise, lightning discharge, automobile ignition noise, interference from other users …)

Both additive and nonadditive

signal distortions are usually characterized as random phenomena and described in statistical terms.

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Elements of Communication System

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Mathematical Model of Channel

Presenter
Presentation Notes
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i/o of a comm. channel

)()()(

)()(*)()(

tndtsh

tnthtstr

+−=

+=

∫∞+

∞−

τττ

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Channel Bandwidth

The bandwidth of a channel is the range of frequencies that it can transmit with reasonable fidelity.

For example, the bandwidth of– twisted pair: several hundred kHz– coax cable: several hundred MHz– wave guide: few GHz– optic fiber: very wide

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Receiver•

Its main function is to recover the message from the received signal.

It includes antenna, amplifier, demodulator, oscillator, power amplifier, transducer

Demodulation: inverse of the modulation•

Operates in the presence of noise & interference. Hence, some distortions are unavoidable.

Some other functions: filtering, suppression of noise & interference

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Types of Communication Systems

guided & unguided (wireless). •

Digital & analog,

Point-to-point & broadcasting,

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Types of comm. systemsTypes of comm. systems••

Analog comm. systemAnalog comm. system

Transport analog information using analog modulation techniques (AM,FM,PM).

••

Digital comm. system.Digital comm. system.Transport digital information using digital modulation techniques (ASK,FSK,PSK).

••

Hybrid comm. system.Hybrid comm. system.Transport digitized analog information using one of the following digital techniques:

1.

Analog pulse modulation schemes (PAM,PDM,PPM).

2.

digital modulation schemes (ASK,FSK,PSK).3.

Pulse code modulation schemes (PCM,DPCM, δ).

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Types of Transmission

Base-band transmission:–

Short distance.

No modulation is needed.•

Band-pass transmission:–

long distance.

Modulation is needed.–

Analog or digital.

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Digital versus analog transmission

Immunity to noise and distortion.•

Viability of regenerative repeaters.

Digital hardware implementation is flexible and scalable.

Digital signals can be encoded to yield low BER.•

Multiplexing is easier and more efficient.

Realization of exchange SNR and B is more efficient.

Digital storage easier and cheaper.•

cost of digital hardware is cheaper.

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Transmission Terminology

Simplex transmission–

One direction

e.g. Radio and television broadcast.

Half duplex transmission–

Either direction, but only one way at a time

e.g. police radio(walki-talki)

Full duplex transmission–

Both directions at the same time

e.g. telephone,

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Simplex vs. Duplex

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Data and Signals

Usually use digital signals for digital data and analog signals for analog data

Can use analog signal to carry digital data–

Modem

Can use digital signal to carry analog data –

codec

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Analog Signals Carrying Analog and Digital Data

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Digital Signals Carrying Analog and Digital Data

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Analog Transmission

Analog signal transmitted without regard to their content (May be analog or digital data)

Attenuated over distance •

Use amplifiers to boost signal

Also amplifies noise, thus received signal will be distorted.

If digital data is encoded then amplifiers will increase BER (bit error rate).

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Digital Transmission

Concerned with content of the signal.•

Integrity endangered by noise, attenuation etc.

Repeaters used to achieve greater distance.

Repeater receives signal-Extracts bit pattern-Retransmits new signal-Attenuation is overcome-Noise is not amplified

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Transmission Impairments

Signal received may differ from signal transmitted

Analog -

degradation of signal quality•

Digital -

bit errors

Caused by–

Attenuation and attenuation distortion

Delay distortion–

Noise

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Attenuation

Signal strength falls off with distance•

Depends on medium

-guided: attenuation is logarithmic.-unguided: attenuation depends on atmospheric

structure.•

Received signal strength:–

must be enough to be detected

must be sufficiently higher than noise to be received without error

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Atten. Cont.

Attenuation is an increasing function of frequency.

-attenuation distortion affects analog signals much more than digital signals.

Fading channel.•

Equalizers: reduce attenuation distortion.

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Delay Distortion

Only in guided media•

Caused by: Propagation velocity varies

with frequency.-different frequency components arrive at

the receiver at different times causing phase shifts.

for digital data delay distortion introduces inter-symbol interference (ISI).

Equalizers : reduce delay distortion.

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Noise•

Additional signals inserted between transmitter and receiver

Thermal–

Due to thermal agitation of electrons

Uniformly distributed–

White noise

Intermodulation–

produce signals at frequency that is the sum

and difference of original frequencies sharing a medium.

Caused by nonlinearity in Tx, Rx, or channel because of signal strength.

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Noise cont.

Crosstalk–

A signal from one line is picked up by another

Impulse–

Irregular pulses or spikes

e.g. External electromagnetic interference–

Short duration

High amplitude–

Severe effect on digital signal of high data rate.

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Channel capacityChannel capacity•

Two primary resources : channel bandwidth and transmitted power.

Limitation imposed on the transmission rate by channel bandwidth B, and SNR is given by

C: channel capacity (maximum rate at no error)M: #of signaling levels

2

2

log (1 ) bps (Shannon equation)2 log bps (Nyquist equation)

C B SNRC B M= +=

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Channel capacity cont.•

Transmitted power (SNR) and channel bandwidth are exchangeable.

1

22 1( )

BBS N R S N R≈

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Radio Communication Channels

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Chapter 2

Introduction to Signals and systems

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Outlines•

Classification of signals and systems

Some useful signal operations•

Some useful signals.

Frequency domain representation for periodic signals

Fourier Series Coefficients•

Power content of a periodic signal and Parseval’ s theorem for the Fourier series

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Classification of Signals•

Continuous-time and discrete-time signals

Analog and digital signals•

Deterministic and random signals

Periodic and aperiodic

signals•

Power and energy signals

Causal and non-causal.•

Time-limited and band-limited.

Base-band and band-pass.•

Wide-band and narrow-band.

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Continuous-time and discrete-time periodic signals

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Continuous-time and discrete-time aperiodic

signals

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Analog & digital signals

If a continuous-time signal can take on any values in a continuous time interval, then is called an analog signal.

If a discrete-time signal can take on only a finite number of distinct values, { }then the signal is called a digital signal.

)(tg)(tg

( )g n

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Analog and Digital Signals

0 1 1 1 1 0 1

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Deterministic signal

A

Deterministic signal is

uniquely described by a mathematical expression.

They are reproducible, predictable and well-behaved mathematically.

Thus, everything is known about the signal for all time.

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A deterministic signal

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Deterministic signal

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Random signal

Random signals are unpredictable. •

They are generated by systems that contain randomness.

At any particular time, the signal is a random variable, which may have well defined average and variance, but is not completely defined in value.

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A random signal

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Periodic and aperiodic Signals•

A signal is a periodic signal if

Otherwise, it is aperiodic signal.

0( ) ( ), , is integer.x t x t nT t n= + ∀

( )x t

0

00

: period(second)1 ( ), fundamental frequency

2 (rad/sec), angulr(radian) frequency

T

f HzT

fω π

=

=

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١٤-2 0 2-3

-2

-1

0

1

2

3

Time (s)

Square signal

Presenter
Presentation Notes
Period= 1 sec
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١٥-1 0 1

-2

-1

0

1

2

Time (s)

Square signal

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١٦-1 0 1

-2

-1

0

1

2

Time (s)

Sawtooth signal

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• A simple harmonic oscillation is mathematically described by

x (t)= A cos (ω

t+ θ), for - ∞

< t < ∞• This signal is completely characterized by three

parameters:A: is the amplitude (peak value) of x(t).ω:

is the radial frequency in (rad/s),

θ: is the phase in radians (rad)

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Example:Determine whether the following signals are

periodic. In case a signal is periodic, specify its fundamental period.

a) x1

(t)= 3 cos(3π

t+π/6), b) x2

(t)= 2 sin(100π

t), c) x3

(t)= x1(t)+ x2(t)d) x4

(t)= 3 cos(3π

t+π/6) + 2 sin(10 t), e) x5

(t)= 2 exp(-j 20 π

t)

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Power and Energy signals

A signal with finite energy is an energy signal

A signal with finite power is a power signal

∞<= ∫+∞

∞−

dttgEg2)(

∞<= ∫+

−∞→

2/

2/

2)(1limT

TTg dttg

TP

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Power of a Periodic Signal

The power of a periodic signal x(t) with period T0

is defined as the mean-

square value over a period

0

0

/ 22

0 / 2

1 ( )T

xT

P x t dtT

+

= ∫

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Example•

Determine whether the signal g(t) is power or energy signals or neither

0 2 4 6 80

1

2g(t)

2 exp(-t/2)

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Exercise•

Determine whether the signals are power or energy signals or neither

1) x(t)= u(t)2) y(t)= A sin t3) s(t)= t u(t)4)z(t)= 5) 6)

)(tδ( ) cos(10 ) ( )v t t u tπ=( ) sin 2 [ ( ) ( 2 )]w t t u t u tπ π= − −

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Exercise

Determine whether the signals are power or energy signals or neither

1)

2)

3)

1 1 2 2( ) cos( ) cos( )x t a t b tω θ ω θ= + + +

1 1 1 2( ) cos( ) cos( )x t a t b tω θ ω θ= + + +

1( ) co s( )n n n

ny t c tω θ

=

= +∑

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٢٤-1 0 1

-2

-1

0

1

2

Time (s)

Sawtooth signalDetermine the suitable measures for the signal x(t)

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Some Useful Functions•

Unit impulse function

Unit step function •

Rectangular function

Triangular function•

Sampling function

Sinc

function•

Sinusoidal, exponential and logarithmic functions

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Unit impulse function•

The unit impulse function, also known as the dirac delta function, δ(t), is defined by

⎩⎨⎧

≠=∞

=0,00,

)(tt

tδ 1)( =∫+∞

∞−

dttand δ

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Δ 0

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Multiplication of a function by δ(t)

We can also prove that

)0()()( sdttts =∫+∞

∞−

δ

)()0()()( tgttg δδ =)()()()( τδττδ −=− tgttg

)()()( ττδ sdttts =−∫+∞

∞−

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Unit step function•

The unit step function u(t) is

u(t) is related to δ(t) by

⎩⎨⎧

<≥

=0,00,1

)(tt

tu

∫∞−

=t

dtu ττδ )()( )(tdtdu δ=

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Unit step

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Rectangular function

A single rectangular pulse is denoted by

⎪⎩

⎪⎨

>

=

<

=⎟⎠⎞

⎜⎝⎛

2/,0

2/,5.0

2/,1

τ

τ

τ

τt

t

ttrect

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٣٢-3 -2 -1 0 1 2 30

0.5

1

1.5

2

2.5

3

Time (s)

Rectangular signal

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Triangular function

A triangular function is denoted by

⎪⎪⎩

⎪⎪⎨

>

<−=⎟

⎠⎞

⎜⎝⎛Δ

21,0

21,21

τ

τττ t

ttt

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Sinc

function

Sampling function

sin( )sinc( ) xxxπ

π=

( ) ( ), : samplig intervalsT s s

nt t nT Tδ δ

=−∞

= −∑

Presenter
Presentation Notes
In some other book, sinc(x)=sin(px)/px
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٣٥-5 0 5

-0.5

0

0.5

1

1.5

2

2.5

3

Time (s)

Sinc signal

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Some Useful Signal Operations•

Time shifting

(shift right or delay)

(shift left or advance)•

Time scaling

( )g t τ−

( )g t τ+

ta

ta

( ) , 1 is co m p ress io n

( ), 1 is ex p an s io n

g ( ), 1 is ex p an s io n

g ( ), 1 is co m p ress io n

g at a

g at a

a

a

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Signal operations cont.

Time inversion

( ) : mirror image of ( ) about Y-axisg t g t−

( ) : shift right of ( )( ) : shift left of ( )

g t g tg t g t

ττ

− + −− − −

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٣٨-10 -5 0 5

0

1

2

3

Time (s)

g(t)g(t-5)g(t)g(t-5)g(t)g(t-5)

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٣٩-10 -5 0 5

0

1

2

3

Time (s)

g(t+5)

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٤٠

Scaling

-5 0 5

024

-5 0 5

024

-5 0 5

024

g(t)

g(2t)

g(t/2)

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٤١

Time Inversion

-5 -4 -3 -2 -1 0 1 2 3 4 50

0.5

1

1.5

2

-5 -4 -3 -2 -1 0 1 2 3 4 50

0.5

1

1.5

2

g(t)

g(-t)

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٤٢

Inner product of signals

Inner product of two complex signals x(t), y(t) over the interval [t1,t2] is

If inner product=0, x(t), y(t) are orthogonal.

2

1

( ( ), ( )) ( ) ( )t

t

x t y t x t y t dt∗= ∫

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٤٣

Inner product cont.

The approximation of x(t) by y(t) over the interval is given by

The optimum value of the constant C that minimize the energy of the error signal

is given by

( ) ( ) ( )e t x t cy t= −2

1

1 ( ) ( )t

y t

C x t y t dtE

= ∫

1 2[ , ]t t

( ) ( )x t cy t=

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٤٤

Power and energy of orthogonal signals

The power/energy of the sum of mutually orthogonal signals is sum of their individual powers/energies. i.e

if

Such that are mutually orthogonal, then

1

( ) ( )n

ii

x t g t=

= ∑

( ), 1,....ig t i n=

1i

n

x gi

p p=

= ∑

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٤٥

Time and Frequency Domains representations of signals

Time domain: an oscilloscope displays the amplitude versus time

Frequency domain: a spectrum analyzer displays the amplitude or power versus frequency

Frequency-domain display provides information on bandwidth and harmonic components of a signal

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٤٦

Benefit of Frequency Domain Representation

Distinguishing a signal from noisex(t) = sin(2π 50t)+sin(2π 120t);y(t) = x(t) + noise;

Selecting frequency bands in Telecommunication system

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٤٧0 10 20 30 40 50-5

0

5Signal Corrupted with Zero-Mean Random Noise

Time (seconds)

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٤٨0 200 400 600 800 10000

20

40

60

80Frequency content of y

Frequency (Hz)

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٤٩

Fourier Series Coefficients

The frequency domain representation of a periodic signal is obtained from the Fourier series expansion.

The frequency domain representation of a non-periodic signal is obtained from the Fourier transform.

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٥٠

The Fourier series is an effective technique for describing periodic functions. It provides a method for expressing a periodic function as a linear combination of sinusoidal functions.

Trigonometric Fourier Series

Compact trigonometric Fourier Series

Complex Fourier Series

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٥١

Trigonometric Fourier Series

0

00

2 ( ) cos(2 )nT

a x t n f t dtT

π= ∫

( )0 0 01

( ) cos 2 sin 2n kn

x t a a n f t b n f tπ π∞

=

= + +∑

0

00

2 ( ) sin(2 )nT

b x t n f t dtT

π= ∫

Presenter
Presentation Notes
k in an integer
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٥٢

Trigonometric Fourier Series cont.

0

00

1 ( )T

a x t dtT

= ∫

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٥٣

Compact trigonometric Fourier series

0 01

2 20 0

1

( ) cos(2 )

,

tan

n nk

n n n

nn

n

x t c c n f t

c a b c a

ba

π θ

θ

=

= + +

= + =

⎛ ⎞−= ⎜ ⎟

⎝ ⎠

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٥٤

Complex Fourier Series

If x(t) is a periodic signal with a fundamental period T0

=1/f0

• are called the Fourier coefficients

2( ) oj n f tn

nx t D e π

=−∞

= ∑

0

0

2

0

1 ( ) j n f tn

T

D x t e dtT

π−= ∫

nD

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٥٥

Complex Fourier Series cont.

1212

n

n

n n

jn n

jn n

j jn n n n

D c e

D c e

D D e and D D e

θ

θ

θ θ

−−

−−

=

=

= =

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٥٦

Frequency Spectra

A plot of |Dn

| versus the frequency is called the amplitude spectrum of x(t).

A plot of the phase versus the frequency is called the phase spectrum of x(t).

The frequency spectra of x(t) refers to the amplitude spectrum and phase spectrum.

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٥٧

Example•

Find the exponential Fourier series and sketch the corresponding spectra for the sawtooth

signal with period 2 π

- 1 0 - 5 0 5 1 00

0 . 5

1

1 . 5

2

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٥٨

Dn

= j/(π

n);

for n≠0•

D0

= 1;

02

0

1 ( )o

j n f tn

T

D x t e dtT

π−= ∫

( )12 −=∫ taaedtet

tata

Presenter
Presentation Notes
Use Table of integral in Appendix D
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٥٩

-5 0 500.5

11.5 Amplitude Spectrum

-5 0 5-100

0

100 Phase spectrum

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٦٠

Power Content of a Periodic Signal

The power content of a periodic signal x(t) with period T0

is defined as the mean-

square value over a period

∫+

=2/

2/

2

0

0

0

)(1 T

T

dttxT

P

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٦١

Parseval’s

Power Theorem

Parseval’

s power theorem series states that if x(t) is a periodic signal with period T0

, then

0

0

2

/ 2 22 2

010 / 2

2 220

1 1

1 ( )2

2 2

nn

Tn

nT

n n

n n

D

cx t dt cT

a ba

=−∞+ ∞

=−∞ ∞

= =

⎧⎪⎪⎪

= +⎨⎪⎪

+ +⎪⎩

∑∫

∑ ∑

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٦٢

Example 1

Compute the complex Fourier series coefficients for the first ten positive harmonic frequencies of the periodic signal f(t) which has a period of 2π

and

defined as

( ) 5 ,0 2tf t e t π−= ≤ ≤

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٦٣

Example 2

Plot the amplitude spectrum of x(t) if T1

= T/4

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٦٤

Example 3

Plot the spectra of x(t).

0( ) ( )n

x t t nTδ∞

=−∞

= −∑

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٦٥

Suggested problems

2.1.1,2.1.2,2.1.4,2.1.8•

2.3.1,2.3.3,2.3.4

2.4.2,2.4.3•

2.5.2, 2.5.5

2.8.1,2.8.4,2.8.5•

2.9.2,2.9.3

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Chapter 3

Analysis and Transmission of Signals

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Outline

• Introduction• Fourier transform and its inverse• Fourier transform of some useful functions• Properties of Fourier transform

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Introduction

• Fourier series works for periodic signals only. What’s about aperiodic signals? This is very large & important class of signals

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Introduction (cont.)• Aperiodic signal can be considered as

periodic for T ∞• Fourier series changes to Fourier transform,

complex exponents are infinitesimally close in frequency

• Discrete spectrum becomes a continuous one, also known as spectral density

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Fourier Transform and Its Inverse

• Fourier transform: if g(t) is aperiodic signal then

∫∞

∞−

−= dtetgfG tfj π2)()(

2( ) ( ) j f tg t G f e dfπ∞

−∞

= ∫

( ) ( )g t G f⇔

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• For real g(t),

:amplitude spectrum:phase spectrum

( )G f

( )( ) ( ) j fG f G f e θ=

* ( )( ) ( ) ( ) j fG f G f G f e θ−− = =

( )fθ

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Example

• Find the Fourier transform and plot amplitude and phase spectra.

1)

2)

( ) ( )atg t e u t−=

( ) ( )atx t e u t= −

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Fourier Transform of Some Useful Functions

1)2) 3)4) 5) 6)

( ) 1tδ ⇔

1 ( )fδ⇔2

2

( )

( )

c

c

j f tc

j f tc

e f f

e f f

π

π

δ

δ−

⇔ −

⇔ +

( ) sin ( )tTrect T c fT⇔

2( ) sin ( )tT T c fT∆ ⇔

121

2

cos(2 ) [ ( ) ( )]sin(2 ) [ ( ) ( )]

c c c

c c cj

f t f f f ff t f f f f

π δ δπ δ δ

⇔ − + +

⇔ − − +

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Spectra of 0( ) sin 2v t A f tπ=

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rect

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Properties of Fourier Transform

• Linearity:

• Time shifting:

• Time reversal:

• Time scaling:

1 1 2 2 1 1 2 2( ) ( ) ( ) ( )ax t a x t aX f a X f+ ↔ +

20( ) ( ) j f tx t t X f e π−− ↔

( ) ( )x t X f− ↔ −1( ) ( )f

ax at Xa

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• Frequency shift (modulation):

• Time differentiation:

• Time integration:

( ) 2 ( )d x t j f X fdt

π↔

12

1( ) ( ) (0) ( )2

t

x d X f X fj f

τ τ δπ−∞

↔ +∫

2( ) ( )cj f tcx t e X f fπ ↔ −

2( ) ( )cj f tcx t e X f fπ− ↔ +

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• Time Convolution:

• Time Multiplication (Frequency convolution)

( ) ( ) ( )* ( )x t y t X f Y f↔

( )* ( ) ( ) ( )x t h t X f H f↔

∫∞

∞−

−= τττ dthxthtx )()()(*)(

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• Duality

• Differentiation in frequency

If ( ) ( )then ( ) ( )

x t X fX t x f

↔↔ −

( )( 2 ) ( ) dX fj t x tdf

π− ↔

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Examples

• Use the Fourier transform properties to find the Fourier transform of the following:

1) 2) 3)4)5)6)

( ) tx t e −=( ) sin (2 )g t c Bt=

/ 2( ) ( )t TTy t rect −=

( ) sin(2 ) ( )tcv t e f t u tπ−=

( ) sgn( )x t t=

( ) ( )g t u t=

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Fourier transform of periodic signal

• If is periodic signal of period then

Then the Fourier transform of is

( )px t0T

0

0

210 0( ) ( ) ( ) j nf t

p Tm m

x t x t mT X nf e π∞ ∞

=−∞ =−∞

= − =∑ ∑

0

10 0 0( ) ( ) ( )T

m n

x t mT X nf f nfδ∞ ∞

=−∞ =−∞

− ↔ −∑ ∑( )px t

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Signal Transmission Through a Linear Time Invariant System

• System representation• Impulse response and transfer

function• Distortionless transmission

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System Representation• A system is defined mathematically as a

transformation or operator that maps an input x(t) into an output y(t).

( )x tSystem

T[ ]( )y t

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Impulse Response of an LTI system

• The impulse response of an LTI system is defined as the response of the system when the input is δ(t). i.e

• For any arbitrary input signal x(t), the response

( ) ( )* ( ) ( ) ( )y t x t h t x h t dτ τ τ+∞

−∞

= = −∫

( ) ( )( ) ( ) x t th t y t δ== ↓

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Frequency response of an LTI system

• The transfer function of an LTI system is

• The response to an input x(t) is

2( )

( )( )( ) j ftx t e

y tH fx t π=

= ↓

( )( ) ( ) j fH f H f e θ=

( ) ( ) ( )Y f X f H f=

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Signal Distortion during Transmission• The transmission of an input signal x(t) through

a system changes it into the output signal y(t).

• During transmission through the system, some frequency components may be boosted in amplitude while others may be attenuated.

• The relative phases of the various components also change due to different delays.

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Distortionless Transmission

• Transmission is said to be distortionless if

( ) ( )dy t k x t t= −

2( ) dj f tH f k e π−→ =

2( ) ( ) ( ) ( ) dj ftY f X f H f kX f e π−= =

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Dispersive channel

• Channel which adds distortion is dispersive channel.

-Amplitude distortion: when ,channel is a fading channel.

-phase distortion: when , channel is a jittering channel.

( )H f k≠

( )f fθ α≠

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The Nature of Distortion in Audio and Video Signals

• The human ear can perceive amplitude distortion but it is relatively insensitive to phase distortion.

• The human eye is sensitive to phase distortion but is relatively insensitive to amplitude distortion.

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3.5 Ideal and Practical Filters

• A filter is a system whose transfer function takes significant values only in certain frequency bands. Filter are usually classified as– Low-pass, – high-pass, – Band-pass, or – Band-stop

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Ideal Low-Pass Filter( )H f

cf

f

0

0cf−

( )fθ

f

f

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Transfer function of an ideal LPF

2( )2

( ) 2 sin (2 ( ))unrealizable

dj f tLPF

c

c c d

fH f rect ef

h t f c f t t

π−⎛ ⎞= ⎜ ⎟

⎝ ⎠→ = −

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Ideal High-Pass Filter( )H f

cfcf− 0 ω

0 ω

( )fθ

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Ideal Band-Pass Filter

0 ωω1−ω1

|H(ω)|

ω2−ω2

ω

θh (ω)

0ω1

−ω1−ω2

ω2

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Ideal Band-Stop Filter

0 ωω1−ω1

|H(ω)|

−ω2 ω2

0 ωω1

−ω2

θh (ω)

ω2−ω1

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2

21 2

,( )

0,

,( )

0,

d

d

j f tc

HPF

j f t

BPF

e for f fH f

otherwise

e for f f fH f

otherwise

π

π

⎧ ≥⎪= ⎨⎪⎩

⎧ ≤ ≤⎪= ⎨⎪⎩

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Ideal versus Practical Low-Pass Filter

( )x t ( ) ( )dy t x t t= −

LPF

h(t)

[ ]( ) 2 sinc 2 ( )c c dh t f f t t= −

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td t

h(t)

0

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• For a physical realizable system, h(t) must be causal; that is,

• One practical approach is to cut off the tail of h(t) for t<0

• If td is sufficient large

)()()(ˆ tuthth =

)()(ˆ thth ≈

( ) 0, 0h t t= ∀ ≺

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Filter or System Bandwidth

• The bandwidth of an ideal low-pass filter

• The bandwidth of an ideal band-pass filter

• No bandwidth for high-pass and band-stop filters.

• For practical filters, a common definition of filter bandwidth is the 3-dB bandwidth (HPBW).

cBw f=

h lBw f f= −

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Signal Bandwidth

• The bandwidth of a signal can be defined as the range of frequencies in which most of the energy or power lies.

• It can also be defined in terms of the 3-dB bandwidth.

• The signal bandwidth is also called the essential bandwidth of the signal

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Signal distortion over a communication channel

• Linear distortion– Non ideal characteristics of either the magnitude, the

phase or both• Distortion caused by channel nonlinearities-interference with signals on same channel

• Distortion caused by multipath effects– Causes non-idealities in the magnitude and phase of

• Fading channels– Channels characteristics changes with time

( )H f

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Distortion caused by multipath effects

Delay td

Delay td+∆tα

s(t) r(t)

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Signal Energy and Energy Spectral Density

• The signal energy can be determined from its Fourier transform using Parseval’s theorem

2 2( ) ( )gE g t dt G f df+∞ ∞

−∞ −∞

= =∫ ∫

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Example

• Verify Parseval’s theorem for the signal

1)

2)

( ) ( )atg t e u t−=

( ) sin (2 )x t c wt=

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Energy Spectral Density (ESD)

is called the energy spectral density (ESD)

2

( )

where ( ) ( )

g g

g

E f df

f G f

−∞

= Ψ

Ψ =

( )g fΨ

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Example

• Estimate the essential bandwidth B of the signal

if the essential bandwidth is required to contain 95% of the signal energy.

( ) ( )atg t e u t−=

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Correlation of Energy Signals• There are applications where it is

necessary to compare one reference signal with one or more signals to determine the similarity between the pair from which some information will be extracted.

• This comparison can be done by computing the correlation between these signals.

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Cross-correlation

• A measure of similarity between a pair of energy signals, is given by the cross-correlation function expressed as

( ) ( ) ( )xy x t y t dtψ τ τ∞

−∞

= −∫

( ) and ( ) x t y t

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Cross-correlation cont.

• If we wish to make the reference signal, then the corresponding cross-correlation function is given by

( ) ( ) ( )y x y t x t d tψ τ τ∞

−∞

= −∫

( )y t

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Autocorrelation function

• In the special case where , we have

the autocorrelation of which is defined as

( ) ( ) y t x t=

( ) ( ) ( )x x t x t d tψ τ τ∞

−∞

= −∫

( )x t

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Properties of Crosscorrelation and

Autocorrelation functions

( ) ( )

( ) ( )(0)

xy yx

x x

x xE

ψ τ ψ τ

ψ τ ψ τψ

= −

= −=

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• Time autocorrelation function and the energy spectral density

• ESD of the Input and the Output

2( ) ( )x t X fψ ↔

2( ) ( ) ( )y xf H f fΨ = Ψ

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Signal Power and Power Spectral Density

• For a real power signal g(t)

• The time-averaged autocorrelation function of g(t) is defined as

∫+

−∞→

=2/

2/

2 )(1limT

TTg dttg

TP

/ 2

/ 2

1( ) lim ( ) ( )T

g TT

g t g t dtT

τ τ+

→∞−

ℜ = −∫

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Autocorrelation of periodic signal

• If g(t) is periodic with period T

/ 2

/ 2

1( ) ( ) ( )T

gT

g t g t dtT

τ τ+

ℜ = −∫

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• The power spectral density (PSD) of g(t), Sg(ω), is the Fourier transform of ℜg(τ)

2

2

( ) ( )

( ) ( )

j fg g

j fg g

S f e d

S f e df

π τ

π τ

τ τ

τ

∞−

−∞

−∞

= ℜ

ℜ =

/ 22

/ 2

1(0) lim ( ) ( )T

g g gTT

g t dt S f df PT

+ ∞

→∞− −∞

ℜ = = =∫ ∫

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• Input and output spectral densities

2( ) ( ) ( )y xS f H f S f=

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Example

Find the autocorrelation function and spectral density of

1)

2)

( ) ( )tx t e u tα−=

( ) sin(2 )cg t f tπ=

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Example

• Find the crosscorrelation function and ESD .check for orthogonality.

( ) ( )( ) ( )

t

t

x t e u ty t e u t

α

α

−=

= −

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Chapter 4

Amplitude (Linear) Modulation

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٢

Outlines•

Introduction

Base-band and Carrier Communication•

Amplitude Modulation (AM):DSB-Large Carrier

Amplitude Modulation: Double sideband-

Suppressed Carrier (DSBSC)

Quadrature

amplitude Modulation (QAM)•

Single Sideband Modulation (SSB)

Vestigial Sideband (VSB)•

Frequency mixing

Superhetrodyne

AM radio.•

Frequency division multilplexing

(FDM).

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٣

Introduction•

Modulation is a process that causes a shift in the range of frequencies of a message signal.

A communication that does not use modulation is called baseband communication

A communication that uses modulation is called Carrier communication

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٤

Example of AM transmitter

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٥

Example of AM (radio) Receiver

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٦

Baseband

and Carrier Communication

Baseband

signal: is message signal (information bearing signal) delivered by the information source or the input transducer .it is usually low frequency signal.

Communication that uses modulation to shift the frequency spectrum of message signal is known as carrier communication.– Amplitude modulation (AM), – Frequency modulation (FM)– Phase modulation (PM)

Presenter
Presentation Notes
In telephony, the baseband is the audio band(0-3.5 kHz). In television, the baseband is the video band (0-4.3 MHz) For digital data or PCM using bipolar signaling at a rate of Rb pulses per sec, the baseband is 0 to Rb Hz. Consider a sinusoidal signal x(t)= A cos(2 f t+ ) A change in A is AM A change in f is FM A change in is PM
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٧

Amplitude Modulation (AM) Double Sideband Large Carrier (DSB-LC)

( ) ( ) cos 2 cos 2AM c cs t m t f t A f tπ π= +

Presenter
Presentation Notes
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٨

Presenter
Presentation Notes
Consider the information signal m(t) shown above. Here, we have two cases depending on A Case1: A+m(t) > 0 for all t Case2: A+m(t) not positive for all t Observe both cases and tell me your remarks? In case 1, the envelope has the same shape as m(t) In case 2, the envelope is not the shape of m(t) How can we benefit from these observation? In the 1st case, we can detect m(t) by detecting the envelope. So demodulation is obtained by envelope detection. Envelope detection is not suitable for case 2.
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٩

Another example of AM Waveform

( ) sin 2( ) sin 2

c

m

c t Ec f tm t Em f t

ππ

==

( ) ( ( ))sin 2 cS t Ec m t f tπ= +

( ) sin 2( ) sin 2

c

m

c t Ec f tm t Em f t

ππ

=

=( ) ( ( ))sin 2 cs t Ec m t f tπ= +

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١٠

Modulation Index

The amount of modulation in AM signal is given by its modulation index:

max min

max min

, min ( )pp

m E Eor m m tA E E

μ −= =

+

When mp

= A ,

μ

=1 or 100% modulation.OverOver--modulation, i.e. mmodulation, i.e. mpp

>A>A

, should be avoided, should be avoided

because it will create distortions.because it will create distortions.

max min,p pE A m E A m= + = −

Presenter
Presentation Notes
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١١

Effect of Modulation Index

μ

<1

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١٢

μ

>1

μ

=1

Presenter
Presentation Notes
for modulation index>1 distortion of the envelope is observed..
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١٣

Effects of Modulation Index

μ

= 1 μ

> 1

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١٤

Sideband and Carrier Power

Carrier Power

Sideband Power •

Total power

Power efficiency

For single tone modulation

2

2cAP =

sc

s

PPP+

22

22 100%, [1 ]2 tot cP P μμη

μ= = +

+

2m

sPP =

tot c sp P P= +

Presenter
Presentation Notes
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١٥Modulation index

Presenter
Presentation Notes
Note that as , . Since is between 0 and 1 max=33% , for =1 Note that most of the power is wasted and not used
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١٦

Example•

Conventional AM signal with a sinusoidal message has the following parameters:

A=10, μ=0.5, fc

= 1MHz, and fm

= 1kHz1.

Find time-domain expression

2. Find its Fourier transform3. Sketch its spectrum 4. Find the signal power, carrier power and the

power efficiency5. Find the AM signal bandwidth

( )Ams t

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١٧

Example•

A given AM (DSB-LC) broadcast station transmits an average carrier power output of 40kW and uses a modulation index of 0.707 for sine-wave modulation. Calculate

a) the total output powerb) the power efficiencyc) the peak amplitude of the output if the

antenna is represented by a 50-Ω resistance load.

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١٨

Generation of AM Signals diode as NLE or as switch

Presenter
Presentation Notes
The bandpass filter tuned to fc suppresses all the other term
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Square-law modulator2( ) ( ) ( )o i iv t av t bv t= +

' ( ) [ 2 ( )]cos 2o cv t aA Abm t f tπ= +

3cf B≥ To avoid overlap the spectrum of

2 ( ) and ( )cm t M f f−

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Switching modulator

Assume

1

1

'

( ) ( ) ( ),

1 2 ( 1)( ) cos 2 (2 1)2 2 1

2( ) [ ( )]cos 22

o in

cn

o c

v t v t w t where

w t f n tn

Av t m t f t

ππ

ππ

−∞

=

=

−= + −

⇒ = +

( ) ,and diode an ideal switchm t A

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٢١

Demodulation of AM signals

AM signals can be demodulated by– Envelope detector– Rectifier detector– Coherent (synchronous) detector.

Presenter
Presentation Notes
Coherent or synchronous demodulation method is more expensive and will defeat the very purpose of AM, so it is seldom used in practice. We will focus on the envelope and rectifier detector
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٢٢

Envelope Detector

Presenter
Presentation Notes
The figure shows the simplest form of an envelope detector consisting of a diode and a resistor capacitor combination During the positive cycle of the input signal, the diode conducts and the capacitor charges up to the peak voltage of the input signal. RsC<1/fc. As the input voltage fall below the maximum, the diode turns off. The capacitor now gets slowly discharged through the resistor R. The process of charging and discharging alternate with each cycle. Thus the output voltage y(t) closely follows the envelope of the input
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٢٣

Envelope Detector (Cont.)

Presenter
Presentation Notes
Notice in the Figure how the output voltage y(t) closely follows the envelope of the input. The ripple can be reduced by increasing the time constant RC so that the capacitor discharges very little between positive peaks. RC >1/fc and RC < 1/B Where B is the highest frequency in m(t). The ripple may be reduced further by another low pass (RC) filter.
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٢٤

Rectifier Detector

Presenter
Presentation Notes
The negative part of the AM wave will be suppressed. The output across the resistor is a half-wave rectified version of the AM signal. Diode function as ideal switch. The output of the LPF of bandwidth B is [ A+ m(t)]/ The dc term (A/) is blocked by the capacitor
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٢٥

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Coherent detector

cos(2 )cA f tπ θ+

LPFV(t)

Local oscillator

2 ( ) cosA m t θ

( )Ams t

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٢٧

Advantages/Disadvantages of Conventional AM (DSB-LC)

Advantages–

Very simple demodulation (envelope detector)

“Linear”

modulation

Disadvantages–

Low power efficiency

Transmission bandwidth twice the message bandwidth.

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٢٨

Double-sideband suppressed carrier DSBSC

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٢٩

The modulating signal m(t)

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٣٠

Modulated signal m(t) cos(ωc

t)

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٣١

Modulated signal m(t) cos(ωc

t)

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٣٢

Example.

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٣٣

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٣٤

DSBSC Modulators

DSBSC signal can be generated using several types of modulators:– Multiplier Modulators– Nonlinear Modulators– Switching Modulators

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Multiplier modulator

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٣٦

Nonlinear Modulators

Presenter
Presentation Notes
Modulation can also be achieved by using nonlinear devices such as semiconductor diodes or transistors The Figure shows one possible scheme which uses 2 identical nonlinear elements.
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٣٧

Switching Modulators

( ) cos 2 ckm t f tπ

a b

BPFM(t)

+

-

v2

Presenter
Presentation Notes
Let w(t) be a periodic signal with fundamental radian frequency c. w(t) can be expressed by trigonometric Fourier series The switch (a-b) is controlled by w(t), and the output will be Output = m(t) w(t)
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٣٨

Switching Modulators

Presenter
Presentation Notes
In Figure, w(t) is a square pulse train. It can control the switch (a-b) on and off. Thus it involves switching the signal m(t) on and off periodically. The output is the product m(t) w(t) In chapter 2, it was shown that The signal m(t) w(t) is given by
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٣٩

Presenter
Presentation Notes
Therefore the spectrum of m(t) w(t) consists of the spectrum of M() and M() shifted to c, 3c, 5c,… The modulated component m(t) cos(ct) can be obtained by using a bandpass filter of bandwidth 2B Hz, centered at the frequency c.
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٤٠

Diode-bridge electronic switch

Presenter
Presentation Notes
This Figure shows an example of an electronic switch for the diode bridge modulator driven by the signal vcd= A cos (ct) When vcd>0, all diodes conducts and a-b is shorted, that is switch is on When vcd<0, all diodes opens and a-b is open circuit, that is switch is off. Thus the diode bridge serves as a desired electronic switch, where the terminals a and b are open and close periodically with the carrier frequency fc.
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٤١

Series-bridge diode modulator

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٤٢

Shunt-bridge diode modulator

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٤٣

Ring Modulator

Presenter
Presentation Notes
Another switching modulator is the ring modulator. When the carrier signal is >0, D1 and D3 conducts, D2 and D4 are open. Thus terminals a is connected to c and b is connected to d. Output is proportional to m(t). When the carrier signal is <0, D2 and D4 conducts, D1 and D3 are open. Thus terminals a is connected to d and b is connected to c. Output is proportional to [-m(t)]. The voltage vi(t)=m(t) w0(t) where w0(t) is a square pulse train.
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٤٤

Ring modulator

Presenter
Presentation Notes
The voltage vi(t)=m(t) w0(t) where w0(t) is a square pulse train. The modulated component m(t) cos(ct) can be obtained by using a bandpass filter of bandwidth 2B Hz, centered at the frequency c.
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٤٥

Demodulation of DSBSC

( ) cos(2 )cm t f tπ

cos(2 )cA f tπ θ+

LPFV(t)

Local oscillator

2 ( ) cosA m t θ

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٤٦

Quadrature

Amplitude Modulation (QAM)

Presenter
Presentation Notes
We have seen that DSB signals require a transmission bandwidth (2B) equal to twice the bandwidth of the message signal m(t). To increase the transmission bandwidth efficiency, it is possible to send two DSB signals using carriers of the same frequency but in phase quadrature. Both modulated signals occupy the same frequency band. Yet they can be separated at the receiver by synchronous detection using two local carriers in phase quadrature. The technique is known as Quadrature Amplitude Modulation (QAM) or quadrature multiplexing and the arrangement is shown in Figure.
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٤٧

Transmitter

Presenter
Presentation Notes
The QAM signal is
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٤٨

Receiver

Presenter
Presentation Notes
If we suppress the high-frequency components by LPF, y1(t)= m1(t)and y2(t)= m2(t) Upper channel in-phase channel and lower channel is quadrature channel Any phase error produces loss, distortion and interference.
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٤٩

QAM cont.

Quadrature

multiplexing is used in color television to multiplex the signals which carry the information about colors.

Presenter
Presentation Notes
Suppose that the local carrier signal is cos (2 fct + 0), then the multiplier output in the upper portion of the circuit becomes If we suppress the second and the last terms by a LPF The desired signal m1(t) and the unwanted signal m2(t) appear in the upper portion of the circuit. Also, it can be shown that y2(t) contains the desired signal m2(t) and the unwanted signal m1(t). Modulated signals having the same carrier frequency now interfere with each other. This is called co-channel interference and must be avoided. Worse problems arise when the local carrier frequency is in error. Therefore, the local carrier must not only be of the same frequency but must be synchronized in phase with the carrier signal.
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٥٠

Single Sideband (SSB)

Presenter
Presentation Notes
Ordinary AM and DSB signals require a transmission bandwidth equal to twice the bandwidth of the message signal m(t) and waste more power. The upper sideband (USB) or the lower sideband (LSB) contains the complete information of the message signal. We can conserve bandwidth and save power by transmitting only one sideband. The modulation is called single-sideband (SSB) modulation. It is widely used by the military and by radio amateurs in high-frequency (HF) communication systems. There are two common methods to generate a single-sideband signal: Selective filtering method (also called frequency discrimination method) and Phase–shift method.
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SSB time representation

ˆ( ) ( ) cos 2 ( )sin 2 ,::

1ˆ ( ) ( ) Hilpert transform of ( )

SSB c cS t m t f t m t f tUSBLSB

m t m t m tt

π π

π

=−+

= ∗

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٥٢

Selective filtering method

Presenter
Presentation Notes
In the filter method, a balanced modulator is used to generate a DSB-SC signal, and the desired sideband signal is then selected by a bandpass filter for transmission. Figures here and next slide show the generation of a SSB signal using the filter method, and the spectra associated with it.
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٥٣

Selective filtering method (Cont.)

Presenter
Presentation Notes
The technique is suitable for message signals with very little frequency content down to dc and hence does not require sharp filter cut-off characteristics. Demodulation of SSB signals can be accomplished by using a synchronous detector as used in the demodulation of normal AM and DSB signals.
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٥٤

Phase–Shift Method

Presenter
Presentation Notes
M+(): the upper sideband of M() M+()= ½ M() u()=1/2 M() [1+sgn()] = ½ M()+1/2 M() sgn()
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٥٥

Phase–Shift Method

Presenter
Presentation Notes
Generating SSB signal using phasing method. A single-sideband signal is given by where the (-) sign is associated with the USB and the (+) sign is associated with the LSB. m^ (t) is obtained by shifting the phase of all frequency components of m(t) by -90o. m^ (t) is called the Hilbert transform of m(t) and is defined as
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٥٦

Hilbert transform

Presenter
Presentation Notes
Block diagram of a 90o phase-shift network can be obtained using Hilbert transform. m^ (t) is called the Hilbert transform of m(t) and is defined as The inverse Hilbert transform of m^ (t) is
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٥٧

Phase–Shift Method (Cont.)

Advantages:– Does not deploy bandpass

filter.

– Suitable for message signals with frequency content down to dc.

Disadvantage:– Practical realization of a wideband 90o

phase shift circuit is difficult.

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٥٨

Demodulation of SSB Signals•

Demodulation of SSB signals can be accomplished by using a synchronous detector as used in the demodulation of normal AM and DSBSC signals.

If we want to use an envelope detector, it can be shown that we must insert a pilot carrier signal Acos(2 πfc t) to the SSB signal, where A >> m(t) and A >> m^(t).

The pilot signal carries most of the transmission power which becomes inefficient.

Presenter
Presentation Notes
Application for SSB communications: Telephone Channel Multiplexing voice channel 4 kHz Envelope detection of SSB signals with a carrier (SSB+C)
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٥٩

Example

A DSB-LC signal is generated using a 1-kHz carrier and the input is m(t)= cos(200πt). The modulation index is 80%. The lower sideband is attenuated (assume ideal filter). Find an expression for the resulting SSB-LC signal if it develops 0.58 W across a one-Ohm resistive load.

Presenter
Presentation Notes
Drill Problem 5.4.1 (Stremler, 2nd Ed., pp. 244)
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٦٠

Vestigial-Sideband Modulation (VSB)

Presenter
Presentation Notes
Vestigial sideband modulation is a compromise between DSB and SSB modulations. It relaxes the sharp cutoff requirement of a SSB signal by retaining a trace of the other sideband in the transmitted signal. Typically, the bandwidth of a VSB modulated signal is about 1.25 times that of the corresponding SSB modulated signal. It is commonly used for transmission of video signals in commercial television broadcasting. This slide and next slide show the generation of a VSB signal, and the spectra associated with it. By inspection of spectrum , the Fourier transform of a VSB modulated signal Sc(f)=[ M(f-fc)+ M(f+fc)] H(f)/2 where H(f) is the transfer function of the bandpass filter.
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٦١

VSB modulator

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٦٢

Demodulation of VSB•

Demodulation of VSB signals can be accomplished by using a synchronous detector.

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٦٣

Vestigial-Sideband Modulation (VSB)

Presenter
Presentation Notes
Vestigial sideband modulation is a compromise between DSB and SSB modulations. It relaxes the sharp cutoff requirement of a SSB signal by retaining a trace of the other sideband in the transmitted signal. Typically, the bandwidth of a VSB modulated signal is about 1.25 times that of the corresponding SSB modulated signal. It is commonly used for transmission of video signals in commercial television broadcasting. This slide and next slide show the generation of a VSB signal, and the spectra associated with it. By inspection of spectrum , the Fourier transform of a VSB modulated signal Sc(f)=[ M(f-fc)+ M(f+fc)] H(f)/2 Or Sc()=0.5 [ M(+ c)+ M(- c)] * H() where H(f) is the transfer function of the bandpass filter.
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٦٤

VSB modulator

Presenter
Presentation Notes
Sc()=0.5 [ M(+ c)+ M(- c)] * H() Demodulation of VSB signals can be accomplished by using a synchronous detector.
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٦٥

Demodulation of VSB•

Demodulation of VSB signals can be accomplished by using a synchronous detector.

Presenter
Presentation Notes
Let sc(t) be the input signal to the synchronous detector. At the receiving end, the bandpass signal is multiplied by a locally generated carrier signal cos(2fct), which is in synchronism with the transmitted carrier signal. The output of the multiplier is x(t)= sc(t) cos(c t) X()= 0.5 [ Sc(+ c)+ Sc(- c)] = 0.25*[ M() H(- c)+ M(- 2c) H(- c)] + 0.25*[ M() H(+ c)+ M(+2c) H(+ c)] X()= 0.25*M() [H(- c)+ H(+ c)] +0.25*[M(- 2c) H(- c)+ M(+2c) H(+ c)] To be able to recover m(t) by a LPF, we need H(- c)+ H(+ c)= const, for | |< 2B
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Transfer function of LPF in VSB receiver

1( ) ,( ) ( )LPF

BPF c BPF c

H f f BH f f H f f

= ≤− + +

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٦٧

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٦٨

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٦٩

VSB+C

VSB modulated signals can also be detected by an envelope detector.

As in the demodulation of a SSB signal, we need to send a pilot carrier signal, resulting an inefficient use of available transmitted power.

Presenter
Presentation Notes
Envelope detection of VSB signals with a large carrier (VSB+C) xVSB+C(t)= xVSB(t)+ A cos(ct), where A is larger than AM case and smaller than the SSB+C
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٧٠

Comparison of conventional AM, DSB-SC, SSB and VSB.

Conventional AM: simple to modulate and to demodulate, but low power efficiency (50% max) and double the bandwidth

DSB-SC: high power efficiency, more complex to modulate & demodulate, double the bandwidth

SSB: high power efficiency, the same (message) bandwidth, more difficult to modulate & demodulate.

VSB: lower power efficiency & larger bandwidth but easier to implement.

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٧١

Multiplexing•

Multiplexing: combining a number of message signals into a composite signal to transmit them simultaneously over a wideband channel.

Two commonly-used types: time-division multiplexing (TDM) and frequency division multiplexing (FDM).

TDM: transmit different message signals in different time slots (mostly digital).

FDM: transmit different message signals in different frequency slots (bands) using different carrier frequencies.

Presenter
Presentation Notes
One of the basic problems in communication engineering is the design of a system which allows many individual signals from users to be transmitted simultaneously over a single communication channel.
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٧٢

FDM

Presenter
Presentation Notes
Suppose that we have several different signals of the same bandwidth. If we translate each one of the signals to a different frequency region such that the translated signal spectra do not overlap each other, then all these signals can now be transmitted along a single communication channel. At the receiving end, the signals can be separated and recovered. We now have a frequency multiplexed system. Such a multiplexing technique is called frequency division multiplexing (FDM).
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٧٣

Presenter
Presentation Notes
Frequency translation can be accomplished by multiplying a low frequency modulating signal with a high-frequency sinusoidal carrier signal. This slide and next ones, shows the transmitter, the receiver, and the spectrum of a 5-user FDM system with carrier frequencies fc1 < fc2 < ... < fc5.
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٧٤

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٧٥

Time Division Multiplexing

Presenter
Presentation Notes
Similar to FDM, the signals are separated in time (instead of frequency)
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٧٦

TDM

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٧٧

AM receiver for many radio stations ?

Presenter
Presentation Notes
Suppose we would like to receive 100 stations. If we use the set-up above, we will need to build 100 bandpass filters and 100 demodulator which is not practical. To use one demodulator and few filters, we can utilize the Superheterodyne AM Receiver
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Frequency mixing

It is desired in communication system to translate the spectrum of the modulated signal up word or down word in frequency to be centered around desired frequency

0

0

: up conversio: down conversio

l c

l c

c l

f f f

f f nf

f f n

= −

−⎧⇒ = ⎨ −⎩

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٧٩

Superheterodyne

AM Receiver

Presenter
Presentation Notes
Most popular type of a radio receiver so far. It is used for AM/FM & TV broadcasting, cellular & satellite systems, radars, GPS etc. Main idea: downconvert RF signal to some fixed lower (intermediate) frequency, then amplify it and detect. RF amplifier: amplifies a weak RF signal coming out of the antenna. Rejects the unwanted one. Bandwidth: much wider than the signal bandwidth. • Mixer: together with the local oscillator downconverts the RF signal to the IF frequency band. • IF amplifier: amplifies the IF signal significantly (up to 106) and rejects adjacent channel signals and interference. Its bandwidth is the same as the signal bandwidth. • Detector (demodulator): demodulates (recovers) the message signal. Local oscillator: allows tuning the receiver to a desired channel (frequency). AGC limits the amplification to prevent overload and distortion.
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٨٠

The RF amplifier amplifies the incoming signal and start the process of selecting the wanted station and rejecting the unwanted ones.

Presenter
Presentation Notes
The antenna not only provides very low amplitude input signals but it picks up all available transmissions at the same time + the added noise. The RF amplifier amplifies the incoming signal above the level of the internally generated noise and also start the process of selecting the wanted station and rejecting the unwanted ones. The overall effect of the selectivity is that whereas the incoming signals each have the same amplitude, the outputs vary between 1mV and 50 mV so we can select, or 'tune', the amplifier to pick out the desired station.
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٨١

The Mixer and the IF Amplifier

Presenter
Presentation Notes
The mixer in the receiver combines the signal from the RF amplifier and the frequency input from the local oscillator to produce three frequencies: flo-fc, flo+fc, and fc The same tuning control is used to adjust the frequency of both the local oscillator and the center frequency of the RF amplifier so that fIF =flo-fc=455 kHz E.g. If the radio transmits at 800 kHz, fc= 800 kHz, fLo= fIF+fc=455+800=1255kHz If fc= 700 kHz, fLo= fIF+fc=1155kHz If for another station fc=1.61 MHz, fLO=fc-fIF=1155 MHz? So I am receiving two stations at the same time? It is called image frequency. Note fimg= fc+2fIF Image stations can be removed by the RF amplifier.
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٨٢

Presenter
Presentation Notes
fc=850 kHz, fLO=fc1+fIF=1.305 MHz fimg=fc+2fIF=1.760 MHz Note the RF amplifier will select only the desired station.
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٨٣

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٨٤

Presenter
Presentation Notes
The AGC is used to prevent overload and distortion
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٨٥

Introduction to Carrier Acquisition

Consider a DSB-SC demodulator where a received signal is m(t) cos(ωc

t) and the local carrier is 2 cos[(ωc

+Δω) t+δ

] . Find the LPF output ifa) Δω=0, and b) δ=0

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٨٦

Carrier Acquisition•

To ensure identical carrier frequencies at the transmitter and the receiver, we can use quartz crystal oscillators, which are generally very stable.

At very high carrier frequencies, the quartz- crystal performance may not be adequate, we

can use the phased-locked loop (PLL)

Presenter
Presentation Notes
very high carrier frequencies: (>1GHz). See next article NEL Frequency Controls Introduces Ultra High Frequency Crystal Oscillator ��New Oscillator Provides Frequencies up to 2.0 GHz in a 9 x 14 mm package��Burlington, WI (March 9, 2005) NEL Frequency Controls, Inc. announces the release of its new patent pending Ultra High Frequency Crystal Oscillator available at frequencies up to 2 GHz with either Differential Sine or PECL outputs. This frequency control solution is ideal for high speed digital designs where signal integrity is critical. The surface mount package measures 9x14mm.��“Now design engineers have a better solution available in obtaining a high frequency clock reference,” notes Chuck Ulland, Vice President of Sales and Marketing at NEL Frequency Controls. “Typical approaches of attaining higher frequencies are either using a lower frequency clock with a PLL frequency multiplier or using a SAW oscillator. Both of these approaches have problems: PLL’s introduce added jitter, while SAW’s have poor stability over temperature performance. NEL’s solution offers extremely low jitter and outstanding stability over temperature characteristics.”��RMS Random jitter performance is less than 1 psec, from 12 KHz to 10 MHz. Stabilities are from +/-20ppm over a temperature range of 0 to 70 C. The Ultra High Frequency Crystal Oscillator undergoes the rigors of NEL’s HALT/ HASS reliability program.��NEL Frequency Controls is a U.S. based manufacturer of crystal oscillators, located in Burlington, WI. The company is recognized worldwide for its leading edge frequency control solutions and supports mission critical applications through its HALT/HASS reliability program that ensures oscillator robustness and start-up reliability. NEL Frequency Controls is ISO 9001-2000 certified. For more information about NEL, call the company at 262-763-3591 or visit their Web site at www.nelfc.com. Company Information:�NEL Frequency Controls, Inc.�357 Beloit St., Burlington, WI 53105-0457,USA�Phone: 262-763-3591, FAX: 262-763-2881�http://www.nelfc.com/Contact Information: Andrea Weitzenfeld �
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٨٧

Phased-Locked Loop (PLL)•

Phase-locked loop is one of the most commonly used circuit in both telecommunication and measurement engineering.

PLL can be used to track the phase and the frequency of the carrier component of an incoming signal.

Presenter
Presentation Notes
PLL is a useful device for synchronous demodulation of AM signals with suppressed carrier or with little carrier (the pilot). It can also be used for the demodulation of angle modulated signals.
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٨٨

A PLL has three basic components:1.

A voltage controlled oscillator

2.

A multiplier3.

A loop filter H(s)

recovered carrier signal

vout

(t)

vin

(t) e0

(t)x(t) Loop Filter

H(s)

Voltage-Controlled Oscillator (VCO)

Presenter
Presentation Notes
Voltage-controlled oscillator (VCO): VCO generates a sinusoidal signal The instantaneous VCO frequency is controlled linearly by its input voltage. Eg. (t)= c+ c e0(t) where c is constant. Multiplier: A multiplier serves as a phased detector (PD) or phase comparator It produces an error signal that is proportional to the phase error, i.e., to the difference between the phases of input and output signals of the phase-locked loop Loop filter: It is a Low-pass filter characterized by its transfer function H(s) LPF suppresses the noise and unwanted PD outputs. It determines the dynamics of phase-locked loop
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٨٩

In every application, the PLL tracks the frequency and the phase of the input signal. However, before a PLL can track, it must first reach the phase-locked condition.

In general, the VCO center frequency differs from the frequency of the input signal.

First the VCO frequency has to be tuned to the input frequency by the loop. This process is called frequency pull-in.

Then the VCO phase has to be adjusted according to the input phase. This process is known as phase lock-in.

Presenter
Presentation Notes
This slide is about Carrier acquisition using PLL Both the frequency pull-in and phase lock-in processes are parts of acquisition which is a highly nonlinear process and is very hard to analyze After acquisition the PLL achieves the phase-locked condition, where the PLL tracks the input phase. Under this phase-locked condition, the VCO frequency is equal to the input frequency
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٩٠

How the PLL works?

)sin()( icin tAtv θω +=

)cos()( ocout tBtv θω +=

vout

(t)

vin

(t) e0

(t)x(t) Loop Filter

H(s)

Voltage-Controlled Oscillator (VCO)

Presenter
Presentation Notes
x(t)=AB/2 [sin(i-o)+sin(2ct+ i+o)] The output of the LPF is e0(t)=0.5 AB sin(i-o)= 0.5 AB sin(e) where e= i-o Phase detector (PD) compares the phase of the input signal vin(t) against the phase of the VCO output v0(t) and produces an error signal x(t) This error signal is then filtered, in order to remove noise and other unwanted components of the input spectrum. The filter output e0(t) controls the instantaneous VCO frequency: (t)= c+ c e0(t)
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٩١

Signal Squaring Method

( )2BPF

@ 2 ωc

PLL

2:1 Frequency divider

m(t) cos(ωc

t)

k cos(ωc

t)

c cos(2ωc

t)

Presenter
Presentation Notes
One method for carrier regeneration at the receiver in DSB-SC. The incoming signal is squared and then passed through a narrow bandpass filter tuned to c. The output of the filter is the sinusoid k cos(2ct) with some residual unwanted signal. This signal is applied to a PLL to obtain a cleaner sinusoid of twice the carrier frequency, which passed through a 2:1 frequency divider to obtain a local carrier in phase and frequency synchronism with the incoming carrier. Other methods Costas loop (see textbook for details)
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٩٢

Suggested Problems

4.2-1

4.2-2

4.2-3

4.2-4

4.2-6, 4.2-8•

4.3-1 4.3-2

4.3-3

4.3-4

4.3-7 4.3-8

4.5-1

4.5-2

4.5-3

4.5-5, 4.5-6 •

4.6-1

4.8-1

4.8-2

Read Section 4.9 (Television)

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Chapter 5

ANGLE MODULATION:FREQUENCY and PHASEMODULATIONS(FM,PM)

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Outlines

• Introduction• Concepts of instantaneous frequency• Bandwidth of angle modulated signals• Narrow-band and wide-band frequency

modulations• Generation of FM signals• Demodulation of FM signals• superhetrodyne FM radio

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Introduction• Angle modulation: either frequency modulation

(FM) or phase modulation (PM).

• Basic idea: vary the carrier frequency (FM) orphase (PM) according to the message signal.

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• While AM is linear process, FM and PM arehighly nonlinear.

• FM/PM provide many advantages (main –noise immunity, interference, exchange ofpower with bandwidth ) over AM, at a cost oflarger transmission bandwidth.

• Demodulation may be complex, but modernICs allow cost-effective implementation.Example: FM radio (high quality, notexpensive receivers).

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Concepts of InstantaneousFrequency

• A general form of an angle modulated signal is givenby

is the instantaneous angleis the instantaneous phase deviation.

• The instantaneous angular frequency of

( ) cos ( ) cos(2 ( ))EM i c iS t A t A f t t

( ) ( )( ) i i

i c

d t d tt

dt dt

( )i t

( )i t( )EMS t

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• The instantaneous frequency of

• The instantaneous frequency deviation

( ) ( )1 1( )

2 2i i

i c

d t d tf t f

dt dt

( )1( )

2i

i

d tf t

dt

( )EMS t

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Example

• for the signal below find the instantaneousfrequency and maximum frequencydeviation.

2( ) cos(10 )x t A t t

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• For phase modulation (PM), the instantaneousphase deviation is

•kp is the phase sensitivity of the PM modulator

expressed in (rad/ V) if m(t) is in Volts• The instantaneous frequency of

( )( )i c p

dm tf t f k

dt

Phase modulation (PM)

( ) ( )i t kp m t

( ) cos [2 ( )]PM c pS t A f t k m t

( )PMS t

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• For Frequency Modulation (FM), theinstantaneous phase deviation is

• kf is the frequency sensitivity of the FMmodulator expressed in rad/ V s if m(t) in Volts.

• The instantaneous frequency of

( ) cos 2 ( )t

FM c fS t A f t k m d

Frequency Modulation (FM)

( ) ( )t

i ft k m d

( )FMS t

( ) ( )2

fi c

kf t f m t

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Angle modulation viewed as FM orPM

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PhaseModulator

FrequencyModulator

PhaseModulator

FrequencyModulator

( )m t ( )PMS t

( )m t( )FMS t

( )m t ( )FMS t

( )PMS t( )m t d

d t

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• A PM/FM modulator may be used togenerate an FM/PM waveform

• FM is much more frequently used than PM• All the properties of a PM signal may be

deduced from that of an FM signal• In the remaining part of the chapter we

deal mainly with FM signals.

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Example 5.1• Sketch FM and PM waves for the modulating

signal m(t) shown in Fig. 5.4a. The constants kfand kp are 2πx105 and 10π ,respectively, andthe carrier frequency fc is 100 MHz..

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Example

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Bandwidth of Angle ModulatedSignals

1) FM signals

2 3

2 3

( ) cos(2 ) ( )sin(2 )

( ) cos(2 ) ( )sin(2 ) ...2! 3!

FM c f c

f fc c

S t A f t k a t f t

k kA a t f t a t f t

where ( ) ( )t

a t m d

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• Narrow-Band Frequency Modulation (NBFM):

• Narrow-Band Phase Modulation (NBPM):

( ) cos(2 ) ( )sin(2 )NBFM c f cS t A f t k a t f t

( ) cos(2 ) ( )sin(2 )NBPM c p cS t A f t k m t f t

BBNBFM 2

| ( ) | 1fk a t

2N BPMB B

| ( ) | 1Pk m t

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Generation of NBFM

m(t)

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Generation of NBPM

m(t)

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• If

∆f: maximum carrier frequency deviationβ: deviation ratio or modulation index

• Wide- Band Frequency Modulation (WBFM)|kf a(t)|>>1 or β>100 fBWBFM 2

2pf mk

f

)1(2)(2 BBfBFM

B

f

| ( ) | 1fk a t

max ( )Pm m t

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• For phase modulation: if

2

'ppmk

f

| ( ) | 1Pk m t

2( ) 2 ( 1)PMB f B B

' 'max ( )Pm m t

2WBPMB f

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Single tone modulation

• Let

)2sin(2cos)( tftfAtx mcFM

n

mcnFM tfnfJAtx )(2cos)()(

( ) cos 2 mm t f t

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• The results is valid only for sinusoidal signal

• The single tone method can be used forfinding the spectrum of an FM wave whenm(t) is any periodic signal.

2 ( 1)

2

FM m

f

m

B f

kf

f

f

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Example 1• A single tone FM signal is

Determinea) the carrier frequency fc

b) the modulation index βc) the peak frequency deviationd) the bandwidth of xFM(t)

6 3FMx (t)=10 cos[ 2 (10 )t+ 8 sin(2 (10 )t)]

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Example 2

• A 10 MHz carrier is frequency modulated bya sinusoidal signal such that the peakfrequency deviation is ∆f=50 KHz. Determinethe approximate bandwidth of the FM signal ifthe frequency of the modulating sinusoid fm isa) 500 kHz, b) 500 Hz, c) 10 kHz.

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Example 3• An angle modulated signal with carrier

frequency 100kHz is

Finda) the power of xFM(t)b) the frequency deviation ∆fc) The deviation ratio βd) the phase deviation ∆ φe) the bandwidth of xFM(t).

EM cx (t)=10 cos[ 2 f t+ 5 sin(3000 t)+10 sin(2000 t) ]

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Example 5.3 (Txt book)

a) Estimate BFM and BPM for m(t) whenkf= 2πx105 rad/sV and kp= 5π rad/V

b) Repeat the problem if the amplitude of m(t)is doubled.

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Features of Angle Modulation• Channel bandwidth may be exchanged for

improved noise performance. Such trade-offis not possible with AM

• Angle modulation is less vulnerable than AMto small signal interference from adjacentchannels and more resistant to noise.

• Immunity of angle modulation tononlinearities thus used for high powersystems as microwave radio.

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• FM is used for: radio broadcasting, soundsignal in TV, two-way fixed and mobileradio systems, cellular telephone systems,and satellite communications.

• PM is used extensively in datacommunications and for indirect FM.

• WBFM is used widely in space andsatellite communication systems.

• WBFM is also used for high fidelity radiotransmission over rather limited areas.

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Generation of FM Signals

• There are two ways of generating FMwaves:

–Indirect generation

–Direct generation

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Indirect Generation of NBFM

m(t)

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Indirect Generation ofWideband FM

• In this method, a narrowband frequency-modulated signal is first generated and then afrequency multiplier is used to increase themodulation index.

m(t)NBFM

xFM(t)FrequencyMultiplier

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m(t)

N fcNBFM Frequency

Multiplier

BPF

Local Oscillator(fLo)

xFM(t)

fc

Frequency Converter

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m(t)NBFM

FrequencyMultiplier

x64

PowerAmplifier

CrystalOscillator10.9 MHz

fc1=200 kHz∆f1= 25 Hz

FrequencyMultiplier

x48

fc2=12.8MHz∆f2= 1.6 kHz

fc3=1.9 MHz∆f3= 1.6 kHz

fc4= 91.2MHz∆f4= 76.8 kHz

Armstrong Indirect FM Transmitter

BPF

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Direct Generation• The modulating signal m(t) directly controls

the carrier frequency. [ ]• A common method is to vary the inductance or

capacitance of a voltage controlled oscillator.

( ) ( )i c ff t f k m t

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• In Hartley or Colpitt oscillator , the frequency isgiven by

• We can show that for k m(t) << C0

LC

1

02

)(1

C

tmkc

0

1

LCc

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Varactor Modulator Circuit

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• Advantage - Large frequency deviations arepossible and thus less frequency multiplicationis needed.

• Disadvantage - The carrier frequency tends todrift and additional circuitry is required forfrequency stabilization.

To stabilize the carrier frequency, a phase-locked loop can be used.

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Example 5.6

• Discuss the nature of distortion inherent in theArmstrong FM generator

– Amplitude distortion– Frequency distortion

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Example• A given angle modulated signal has a peak

frequency deviation of 20 Hz for an inputsinusoid of unit amplitude and a frequency of50 Hz. Determine the required frequencymultiplication factor, N, to produce a peakfrequency deviation of 20 kHz when the inputsinusoid has unit amplitude and a frequencyof 100Hz, and the angle-modulation used is(a) FM; (b) PM

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Demodulation of FM Signals

• Demodulation of an FM signal requires asystem that produces an output proportional tothe instantaneous frequency deviation of theinput signal.

• Such system is called a frequencydiscriminator.

FM

Demodulator

)(cos)( ttAtx c

dt

tdkty

)()(

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• A frequency-selective network with a transferfunction of the form |H(ω)|= a ω+b over theFM band would yield an output proportionalto the instantaneous frequency.

• There are several possible examples forfrequency discriminator, the simplest is theFM demodulator by direct differentiation

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FM demodulator by direct differentiation

• The basic idea is to convert FM into AMand then use AM demodulator.

' ( ) 2 ( ) sin 2 ( )t

c c f c fs t A f k m t f t k m d

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Bandpass Limiter

• Input-output characteristic of a hard limiter

HardLimiter

BPF

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• Any signal which exceeds the preset limits aresimply chopped off

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Practical Frequency Demodulators

• There are several possible networks forfrequency discriminator– FM slope detector– Balanced discriminator– Quadrature Demodulator

• Another superior technique for thedemodulation of the FM signal is to use thePhased locked loop (PLL)

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FM Slope Detector

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FM Slope Detector

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FM Slope Detector

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Balanced Discriminator

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Balanced Discriminator (Cont.)

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Balanced Discriminator (Cont.)

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Quadrature Demodulator• FM is converted into PM

• PM detector is used to recover messagesignal

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Quadrature Demodulator

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Transfer function ofQuadrature demodulator

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Phase-Locked Loop (PLL)

)sin()( icin tAtv

)cos()( ocout tBtv

vout(t)

vin(t) e0(t)x(t) Loop Filter

H(s)

Voltage-ControlledOscillator (VCO)

dt

tdkte i )(

)(0

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Zero-Crossing Detectors• Zero-Crossing Detectors are also used because

of advances in digital integrated circuits.• These are the frequency counters designed to

measure the instantaneous frequency by thenumber of zero crossings.

• The rate of zero crossings is equal to theinstantaneous frequency of the input signal

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Summary• Concepts of instantaneous frequency• FM and PM signals• Bandwidth of angle modulated signals

NBFM and WBFM• Generation of FM signals

– Direct and indirect generation• Demodulation of FM signals

– frequency discriminator– PLL

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Suggested Problems

• 5.1-1 5.1-2 5.1-3 5.2-1 5.2-2 5.2-3 5.2-4 , 5.2-5 5.2-6 .

• 5.2-7 5.3-1 5.3-2 5.4-1 5.4-2

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Chapter 6

Sampling and PulseCode Modulation

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Outline• introduction• Sampling and sampling theorem• Practical sampling and pulse amplitude

modulation (PAM)• Pulse code modulation (PCM)• Differential pulse code modulation (DPCM)• Delta modulation.

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Introduction• There is an increase use of digital

communication systems• Digital communications offer several

important advantages compared to analogcommunications such as higher performance,higher security and greater flexibility.

• digital transmission of analog signals requireAnalog to digital conversion (AD).

• digital pulse modulation

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Analog to Digital converter

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PCM system

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Sampling• A typical method for obtaining a discrete-

time sequence x(n) from a continuous-time signal x(t) is through periodicsampling.

x(n)= x(nTs), for -∞ < n < ∞• Ts : sampling period.

• fs: sampling frequency

or sampling rates

s

fT

1

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x(t)

s(t)

xs (t)

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Spectrum of Xs(f)X(f)

k

ss

s fkfXT

fX )(1)(

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• Is it possible to reconstruct the analogsignal from the sampled valued?

Samplerx(t) x(nTs)

LPFx(t)

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• Given any analog signal, how should we selectthe sampling period Ts (or the samplingfrequency fs) without losing the importantinformation contained in the signal.

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Spectrum of Xs(f)

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Sampling Theorem• Let m(t) be a real valued band-limited signal

having a bandwidth B, and m(nTs) be thesample values of m(t) where n is an integer.

• The sampling theorem states that the signalm(t) can be reconstructed from m(nTs) with nodistortion if the sampling frequency

fs ≥2B

• The minimum sampling rate 2B is called theNyquist sampling rate.

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Typical sampling rates for somecommon applications

Application B fs

Speech 4 kHz 8 kHzAudio 20 kHz 40 kHzVideo 4 MHz 8 MHz

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Example

Determine the Nyquist rate of the followinganalog signal and plot the spectrum of thesampled signal for :

1. fs=150Hz 2. fs=300Hz 3. fs=500 Hzx(t) = 3cos(50t) + 10sin(300t) - cos(100t)

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To Avoiding aliasing• Band-limiting signals (by filtering) before

sampling.• Sampling at a rate that is greater than the

Nyquist rate.

Anti-Aliasing

Filter

Sampler

fs≥ 2B

x(t) xs(t)

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Practical Sampling

• In practice, we multiply a signal x(t) by a train ofpulses of finite width.

• There are two types of practical sampling

– Natural Sampling (Gating)

– Instantaneous Sampling. Also known as flat-top PAM or sample-and-hold.

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Natural Sampling

s(t)

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Generation of PAM with natural sampling

X(t)

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Another example of natural sampling

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Sample-and-Hold

τxs(t)

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Sample-and-hold (S/H) circuit.

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Natural Sampling (Gating)

)()()( tstxtxs

k

skTtrectts

)(

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Natural Sampling (Gating): Spectrum

• The spectrum (FT) of the sampled (PAM)signal is

( ) sinc( ) ( )s sk

X f d kd X f kf

sTd Duty cylce of s(t)

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Natural Sampling (Gating): Spectrum

d X( f )

d sinc(kd)

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Sample-and-Hold( flat-top sampling)

τxs(t)

k

sss

kTtrectTkxtx

)()(

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Sample and hold: Spectrum

kss

k

sss

kTtTkxtrect

kTtrectTkxtx

)()(*

)()(

1( ) sin ( ) ( )s sks

X f c f X f kfT

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Sample and hold: Spectrum

sinc(τf) X(f)

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• we see that by using flat-top sampling wehave introduced amplitude distortion, and theprimary effect is an attenuation of high-frequency components. This effect is knownas the aperture effect.

• If <<Ts, then H( f) represents a LPF.

• Else, we can use a LPF such thatHeq( f)= 1/H(f)

The LPF is called an equalization filter.

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Reasons for intentionally lengthening the durationof each sample are:

• Reduce the required transmission bandwidth:B is inversely proportional to pulse duration.

• To get the exact signal value, the transient mustfade away

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Pulse Modulation• Pulse modulation results when some

characteristic of a pulse is made to vary in one-to-one correspondence with the messagesignal.

• A pulse is characterized by three qualities:– Amplitude– Width– Position

• Pulse amplitude modulation, Pulse widthmodulation, and Pulse position modulation

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Pulse amplitude modulation (PAM)• In Pulse Amplitude Modulation, a pulse is

generated with an amplitude corresponding tothat of the modulating waveform.

• There are two types of PAM sampling

– Natural Sampling (Gating)

– Flat-top or sample-and-hold.

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PAM System

• A system transmitting sample values of theanalog signal is called a pulse-amplitudemodulation (PAM) system.

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• Like AM, PAM is very sensitive to noise.

• While PAM was deployed in early AT&TDimension PBXs, there are no practicalimplementations in use today. However, PAM isan important first step in a modulation schemeknown as Pulse Code Modulation.

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Note

• PBX: Short for private branch exchange, aprivate telephone network used within anenterprise.

• Users of the PBX share a certain numberof outside lines for making telephone callsexternal to the PBX.

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Pulse Width Modulation (PWM)

• In PWM, pulses are generated at a regular rate.The length of each pulse is controlled by themodulating signal amplitude at that samplinginstant.

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Pulse Position Modulation (PPM)

• A PPM signal consists of pulsesin which the pulse displacementfrom a specific time reference isproportional to the sample valuesof the information bearing signal.

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Pulse Code Modulation(PCM)

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Advantages of PCM• Inexpensive digital circuitry may be used in

the system.• All-digital transmission.• Further digital signal processing such as

encryption is possible.• Errors may be minimized by appropriate

coding of the signals.• Signals may be regularly reshaped or

regenerated using repeaters at appropriateintervals.

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A single-channel PCM transmission system

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Advantages of PCM• Inexpensive digital circuitry may be used in

the system.• All-digital transmission.• Further digital signal processing such as

encryption is possible.• Errors may be minimized by appropriate

coding of the signals.• Signals may be regularly reshaped or

regenerated using repeaters at appropriateintervals.

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A single-channel PCM transmission system

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Quantization

• Quantizer converts the discrete time signalinto a sampled and quantized signal that isdiscrete in both time and amplitude

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m(t) and its sampled value m(kTs)

0 0.002 0.004 0.006 0.008 0.01-8

-6

-4

-2

0

2

4

6

8

D

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Input-output characteristics of the quantizer

Output

Input

L=8

mq=8-mq=-8

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• Quantization can be uniform andnonuniform

• The quantization discussed so far is said to beuniform since all of the steps are of equalsize.

• Nonuniform quantization uses unequal steps

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Uniform Quantization• The amplitude of ms(t) can be confined to the

range [-mq, mq]

• This range can be divided in L zones, each ofstep such that

= 2 mq / L

• The sample amplitude value is approximated bythe midpoint of the interval in which it lies.

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Quantization Noise• The difference between the input and output

signals of the quantizer becomes thequantizing error or quantizing noise

mq(t) mq(t)+D/2mq(t)-D/2

ms(t)ms(t)

2)(

2

tq

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Quantization Error or Noise

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• Assuming that the error is equally likely to lieanywhere in the range (-∆/2, ∆/2), the mean-square quantizing error is given by

121 22/

2/

22

dqqq

2

22

3 Lm

q q2

22 )(3

qo

o

mtmL

NS

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Example• For a full-scale sinusoidal modulating signal

m(t)= A cos(ωmt), show that

• or

23 2L

NS

o

o

)()(log2076.1 10 dBLNS

dBo

o

223

q

o

o

o

mSL

NS

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Nonuniform Quantization

• For many classes of signals the uniformquantizing is not efficient.

• Example: speech signal has large probability ofsmall values and small probability of large ones.

• Solution: allocate more levels for smallamplitudes and less for large. Thus, totalquantizing noise is greatly reduced

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Example of Nonuniform quantization

0 0.005 0.01 0.015 0.02

-6

-4

-2

0

2

4

6

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Nonuniform Quantization

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• The effect of nonuniform quantizing can beobtained by first passing the analog signalthrough a compression (nonlinear) amplifierand then into the PCM circuit that uses auniform quantizer.

• At the receiver end, demodulate uniform PCMand expand it.

• The technique is called companding.• Two common techniques

1. m-law companding2. A-law companding

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m-law Compression Characteristic

• where

qmmmy

1ln

)1ln()sgn(

1qm

m

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m-law Compression Characteristic

|m/mq|

y

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A-law Compression Characteristic

• where1

qmm

11,ln1ln1

)sgn(

1,ln11

qq

qq

mm

AmmA

Am

Amm

mm

Ay

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A-law Compression Characteristic

|m/mq|

y

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• The compressed samples must be restoredto their original values at the receiver byusing an expander with a characteristicscomplementary to that of the compressor.

• The combination of compression andexpansion is called companding

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• It can be shown that when a µ-lawcompander is used, the output SNR is

• where

22

)1ln(3

LNS

o

o

)(2

22

tmmq

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Coding of Quantized Samples• The coding process in an A/D converter

assigns a unique binary number to eachquantization level. For example, we can usebinary and gray coding.

• A word length of n bits can create L= 2n

different binary numbers.• The higher the number of bits, the finer the

quantization and the more expensive thedevice becomes.

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Binary and Gray coding of samples.

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Output SNR• SNR is controlled by the PCM bandwidth

)(6 dBnNS

dBo

o

c10log10

caseeduncompress

mtm

casecompressedc

q

,)(3

,)1(ln

3

2

2

2

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Comments About dB Scale• The decibel can be a measure of power ratio

• It can also be used for measuring power

NS

NS

dB10log10

mWPP

PP

WdBm

WdBW

1log10

log10

10

10

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ExamplesGain= (Pout/Pin) = 2 = +3 dB

Pout= 48 mW

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Bandwidth of PCM• What is the spectrum of a PCM signal?• The spectrum of the PCM signal depends on

the bit rate, the correlation of the PCM data,and on the PCM waveform pulse shape (usuallyrectangular) used to describe the bits.

• The dimensionality theorem [2] shows that thebandwidth of the PCM waveform is bounded by

BPCM ≥ R/2 = n fs/2where R: bit rate

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Transmission Bandwidth

• For L quantization levels and n bitsL= 2n or n= log2L

• The bandwidth of the PCM waveformBPCM ≥ n B Hz

• Minimum channel bandwidth or transmissionbandwidth

BT= n B Hz

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Example: PCM for Telephone System• Telephone spectrum: [300 Hz, 3400 Hz]• Min. sampling frequency: fs,min = 2 Fmax=6.8 kHz• Some guard band is required:

fs= 2 Fmax + ∆fg = 8 kHz• n=8-bit codewords are used L=256.• The transmission rate: R=n* fs =64 kbits/s• Minimum PCM bandwidth: ΒPCM = R/2=32 kHz

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Example 6.3• A signal m(t) of bandwidth B= 4 kHz is

transmitted using a binary companded PCMwith µ=100. Compare the case of L=64 with thecase of L=256 from the point of view oftransmission bandwidth and the output SNR.

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Differential PCM (DPCM)• Samples of a band-limited signal are correlated.• This can be used to improve PCM

performance: to decrease the number of bitsused (and, hence, the bandwidth) or to increasethe quantization SNR for a given bandwidth.

• Main idea: quantize and transmit the differencebetween two adjacent samples rather thansample values.

• Since two adjacent samples are correlated,they difference is small and requires less bits totransmit.

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DPCM System-Modulator

mq(k)

d(k)m(k) Quantizer

Predictor

dq(k)

)(ˆ kmq

)(ˆ)()( kmkmkd q )()()( kqkdkdq

)()(ˆ)( kdkmkm qqq

mq(k)= m(k)+ q(k) is the quantized version of m(k)

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DPCM System-Demodulator

Predictor

Output mq(k)

)(ˆ kmq

Input dq(k)

)(ˆ)()( kmkmkd qqq )(ˆ)()( kmkdkm qqq

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Time Division Multiplexing (TDM)

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Ten-Channel PCM System(a) Transmitter (b) Receiver

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Signal Shapes

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Bandwidth Requirements for TDM• If N band-limited signals are multiplexed

each with bandwidth B• The minimum TDM sampling rate is

fTDM= 2 N B• If each sample is coded with n bits, then the

minimum transmitted data rate isR= 2 n N B

• The minimum transmission bandwidth isBT = n N B

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TDM: Concept of Framing and Synchronization

• The time interval TF containing one sample from eachmessage signal is called a frame.

• an extra pulse (called marker) is transmitted forsynchronization

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Comparison of Time and FrequencyDivision Multiplexing

• Time division multiplexing: Individual TDMchannels are assigned to distinct time slots butjumbled together in the frequency domain.Channels are separated in the time domain

• Frequency division multiplexing: IndividualFDM channels are assigned to distinctfrequency regions but jumbled together in thetime domain. Channels are separated in thefrequency domain

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Comparison of Time and FrequencyDivision Multiplexing

• Many of the TDM advantages are technologydriven. The digital circuits are much cheaperand easier to implement

• In FDM, imperfect bandpass filtering andnonlinear cross-modulation cause cross talk.TDM is not sensitive to these problems.

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Example• A binary channel with bit rate Rb=36000 bits/s

is available for PCM transmission. Findappropriate values of the sampling rate fs, thequantizing level, and the binary digits n,assuming the signal bandwidth is B=3.2 kHz.

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Example• An analog signal is quantized and transmitted

by using a PCM system. If each sample at thereceiving end of the system must be known towithin 0.5% of the peak- to-peak full-scalevalue, how many binary digits must eachsample contain ?

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Example• For a full-scale sinusoidal modulating signal

m(t)= A cos(ωmt), show that

• or

23 2L

NS

o

o

)()(log2076.1 10 dBLNS

dBo

o

223

q

o

o

o

mSL

NS

Page 414: Chapter one Introduction Analog and Digital Communicatione4uhu.com/down/Analog/analog-slides.pdf · Viability of regenerative repeaters. • Digital hardware implementation is flexible

Suggested problems

• 6.1-1, 6.2-3 and 6.2-5.