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Communication Systems Unit -I Amplitude Modulation

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Page 1: Unit -I Amplitude Modulation - WordPress.com · 2016-09-19 · Angle modulation AM DSB-SC SSB VSB FM PM . Communication Systems Continuous-Wave Modulation 3 2.1 Introduction Figure

Communication Systems

Unit -I

Amplitude Modulation

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contents • Time-domain and frequency-domain

descriptions of continuous-wave modulation

• Noise performance pertaining to modulation

schemes

Amplitude modulation

Angle modulation

AM

DSB-SC

SSB

VSB

FM

PM

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2.1 Introduction

Figure 2.1

Components of a continuous-wave modulation system:

(a) transmitter, and (b) receiver.

In addition to the signal received from the transmitter, the

receiver input includes channel noise. The degradation in

receiver performance due to channel noise is determined by the

type of modulation used. So, it is necessary to study various

modulation types and their noise performance.

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Basic concepts about modulation

Message signal

Information-bearing signal

Baseband signal

Modulating signal/wave

Carrier, sinusoidal wave

Modulated signal/wave

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Modulation and Demodulation

• Modulation: refers to the process by which

some characteristic of a carrier is varied in

accordance with a modulating signal. It is

also a process of shifting frequency range.

• Demodulation: is the reverse of the

modulation process.

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(a) Carrier wave

(b) Sinusoidal

modulating signal

(c) Amplitude-

modulated signal

(d) Frequency-

modulated signal

Demo for AM and FM signals

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2.2 Amplitude Modulation AM

Carrier wave c(t): ( ) cos(2 )c c

c t A f t

Ac: carrier amplitude fc: carrier frequency

Amplitude-modulated wave s(t)

( ) 1 ( ) cos(2 )c a c

s t A k m t f t

Ka : amplitude sensitivity

AM is defined as a process in which the

amplitude of the carrier wave c(t) is varied about

a mean value, linearly with the baseband signal.

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Baseband signal m(t)

AM wave for | kam(t) | < 1 AM wave for | kam(t) | > 1

Figure 2.3

Illustrating the amplitude modulation process.

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Observations from figure 2.3

• If |kam(t)|<1 for all t, the envelope of modulated

signal s(t) is linear with the modulating signal m(t).

Therefore, we can use envelope detector to recover

the message signal in the receiver.

• If |kam(t)|>1 for any t, carrier phase reversals

happen. This is called as overmodulation. In this

case, the envelope of modulated signal s(t) is no

longer linear with the modulating signal m(t).

Message signal can not be recovered by envelope

detector.

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In AM, two requirements must be satisfied:

1. , W: message bandwidth, so that the

envelope of s(t) can be visualized satisfactorily.

Wfc

2. , so that

overmodulation can be avoided.

( ) 1 for all t a

k m t

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Descriptions of AM signal

Time-domain description:

Frequency-domain description:

( ) 1 ( ) cos(2 )c a c

s t A k m t f t

m(t) M(f) FT

IFT

( ) [ ( ) ( )] [ ( ) ( )]2 2

c a cc c c c

A k AS f f f f f M f f M f f

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(a) Spectrum of baseband signal (b) Spectrum of AM wave

Negative frequency

Upper band and lower band

Transmission bandwidth

BT=2W

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AM practical circuits

In transmitter, it is accomplished using a

nonlinear device. In receiver, it is also

accomplished using a nonlinear device.

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Virtues and Limitations of AM

Virtue:

Simplicity of implementation

Limitations:

1. AM is wasteful of power

2. AM is wasteful of bandwidth

(a) Spectrum of baseband signal (b) Spectrum of AM wave

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How to overcome these limitations ?

Step 1: Suppress the carrier: DSB-SC

Step 2: Modify the sidebands: SSB, VSB

DSB-SC: double sideband-suppressed carrier,where only

the upper and lower sidebands are transmitted. No carrier

frequency component.

SSB: single sideband, where only one sideband (the lower

sideband or the upper sideband) is transmitted.

VSB: vestigial sideband, where only a vestige of one of the

sidebands and a corresponding modified version of the other

sideband are transmitted.

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2.3 linear Modulation Schemes

Linear modulation is defined by: (Narrowband signal)

( ) ( )cos(2 ) ( )sin(2 )I c Q c

s t s t f t s t f t

SI(t): in-phase component of s(t) SQ(t): quadrature component of s(t)

In linear modulation, both SI(t) and SQ(t) are low-pass

signals that are linearly related to the message signal m(t).

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Linear modulation is defined by

( ) ( )cos(2 ) ( )sin(2 )I c Q c

s t s t f t s t f t

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0 1+kam(t) AM

-½m’(t) ½ m(t) V-USB

+½ m’(t) ½ m(t) V-LSB VSB

-½ ½ m(t) LSB

+½ ½ m(t) USB SSB

0 m(t) DSB-SC

SQ(t) SI(t) Type of modulation

ˆ ( )m t

ˆ ( )m t

Table 2.1 different forms of linear modulation

m(t)=message signal

=Hilbert transform of m(t) ˆ ( )m t

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Descriptions of AM signals

AM: ( ) 1 ( ) cos(2 )c a c

s t A k m t f t

DSB: ( ) ( )cos(2 )c c

s t A m t f t

SSB:

VSB: 1 1cos 2 cos 2

2 2c c c c

s t A m t f t m t A m t f t

+ vestige of the upper sideband

- vestige of the lower sideband

)2sin()(ˆ2

1)2cos()(

2

1)( tftmAtftmAts cccc

+ lower sideband transmitted

- upper sideband transmitted

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Two important points from table 2.1

1. The in-phase component SI(t) is solely dependent

on the message signal m(t).

2. The quadrature component SQ(t) is a filtered

version of m(t). The spectral modification of the

modulated wave s(t) is solely due to SQ(t).

To be more specific, the role of the quadrature component is

merely to interfere with the in-phase component, so as to

reduce or eliminate power in one of the sidebands of the

modulated signal s(t), depending on how the quadrature

component is defined.

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DSB-SC Double Sideband-Suppressed

Carrier Modulation

AM:

( ) 1 ( ) cos(2 )c a c

s t A k m t f t

)]()([2

)]()([2

)( ccca

ccc ffMffM

Akffff

AfS

DSB:

( ) ( )cos(2 )c c

s t A m t f t

1( ) ( ) ( )

2c c c

S f A M f f M f f

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Figure 2.5 (a) Block diagram of product modulator.

(b) Baseband signal. (c) DSB-SC modulated wave.

The DSB modulated signal undergoes a phase reversal

whenever the message signal crosses zero. Consequently, the

envelope of DSB signal is different from the message signal.

This is unlike the case of AM wave.

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(a) Spectrum of baseband signal (b) Spectrum of DSB wave

(a) Spectrum of baseband signal (b) Spectrum of AM wave

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Demodulation of DSB

The baseband signal m(t) can be recovered from a DSB wave by using

coherent detection.

Can we use envelope detector to demodulate

DSB signals? Why?

How to demodulate DSB signals?

NO. The envelope of DSB signal is no longer

linear with modulating signal.

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Coherent Detection

Coherent detection

Synchronous demodulation

Why is it called Coherent Detection?

Local oscillator signal is exactly synchronized with

carrier in both frequency and phase.

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Coherent Detection Process

cos 2 ( )

cos 2 cos 2

1 1cos 4 cos

2 2

c c

c c c c

c c c c c

v t A f t s t

A A f t f t m t

A A f t m t A A m t

Then, output of product modulator is

the local oscillator signal is supposed as

DSB signal: ( ) ( )cos(2 )c c

s t A m t f t

' cos(2 )c c

A pf t f

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Output of low-pass filter

)(cos'2

1)(0 tmAAtv cc

1 1cos 4 cos

2 2c c c c c

v t A A f t m t A A m t

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Discussion :

Phase difference )( cos'

2

1)(0 tmAAtv cc

m(t) can be recovered without any distortion.

0

1constant, ( ) ' ( )

2

c cv t A A km t

Case 1:

0

10, ( ) ' ( )

2

c cv t A A m t Maximum

0

090 , ( ) 0 v t Maximum

Quadrature Null Effect

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In practice, varies randomly with time. So

synchronism must be ensured both in frequency

and phase.

Case 2:

How to keep synchronization?

Phase Lock Loop

Square Loop

Costas Loop

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Virtues and limitations of DSB

Virtue: saving transmitted power

The resulting system complexity is the price

that must be paid for suppressing the carrier

wave to save transmitted power.

Limitations:

Complexity

Waste of bandwidth

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Quadrature-Carrier Multiplexing

Quadrature Amplitude Modulation QAM

Theory basis: quadrature null effect

The quadrature null effect of the coherent

detector may also be put to good use in the

construction of quadrature-carrier multiplexing.

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QAM is a bandwidth-conservation scheme.

why?

This scheme enables two DSB signals to

occupy the same channel bandwidth, and

yet it allows for the separation of the two

message signals at the output. It is therefore

a bandwidth-conservation scheme.

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Figure 2.10

Quadrature-carrier multiplexing system

Transmitter Receiver.

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1 2cos 2 sin 2c c c c

s t A m t f t m t A m t f t

Modulation and Demodulation process

The transmitted signal s(t) consists of sum of two

product modulator outputs, as shown by

m1(t) and m2(t) are two different message signals.

demodulation

)()2cos(2)( 1 tmALPFtfts cc

)()2sin(2)( 2 tmALPFtfts cc

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Single-Sideband Modulation SSB

SSB: single sideband, where only one

sideband (the lower sideband or the upper

sideband) is transmitted.

ttmttm

tmtmts

cc

tc

sin )(ˆ cos )(=

}e ])(ˆ j)(Re{[=)( j

SSB

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Hilbert Transform

Definition : 1ˆ( ) ( )x t x tt

, 01sgn( )

, 0

FTj

jjt

( )x t ˆ( )x t1

( )h tt

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Methods to generate SSB signals

1) Frequency-discrimination method to

generate SSB

2) Phase-shift method to generate SSB

3) Weaver’s method to generate SSB

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Energy Gap

Figure 2.11 (a) Spectrum of a message signal m(t) with an

energy gap of width 2fa centered on the origin. (b) Spectrum

of corresponding SSB signal containing the upper sideband.

Typical example: telephone voice

f ~(300, 3100Hz) energy gap: 600 Hz

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SSB Coherent Detection

tA cc cos'

)(SSB ts Low Pass filter )(tm

How to keep synchronization between local

oscillator and carrier in the transmitter?

1. A low-power pilot carrier

2. A highly stable oscillator

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Vestigial Sideband Modulation VSB

One of the sideband is partially suppressed and a

vestige of the other sideband is transmitted to

compensate for that suppression.

Vestige of lower sideband

Vestige of upper sideband

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Frequency Discrimination Method to

Generate VSB

Key: the design of band-pass filter

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Magnitude response of VSB filter

Odd symmetry

around the fc

1. The sum of the values of the magnitude response

|H(f)| at any two frequencies equally displaced

above and below fc is unity.

2. The phase response arg(H(f)) is linear.

( ) ( ) 1 for W f W c c

H f f H f f

BT=W+fv

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VSB description in time-domain

+ vestige of the upper sideband

- vestige of the lower sideband

phase –shift method to generate VSB

-π/ 2

tccos

)(tm

)(' tm

)(VSB ts)(1

fHj

Q

1 1( ) ( )cos(2 ) '( )sin(2 )

2 2c c c c

s t A m t f t A m t f t

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2.4 Frequency Translation

• The basic operation in SSB is in fact a form

of frequency translation.

• SSB modulation is also called frequency

changing, mixing, or heterodyning.

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Mixer

tftf l 2cos2cos 1

Sum frequency

Difference frequency

lfff 12

lfff 12

The mixer is a device that consists of a product

modulator followed by a band-pass filter.

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Up conversion

1212 ffffff ll or

2112 ffffff ll or

Down conversion

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Figure 2.17 Mixer

Spectrum of modulated signal s1(t) at the mixer input

Spectrum of the corresponding signal s´(t) at the output of the

product modulator in the mixer

BPF

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2.5 Frequency-Division Multiplexing FDM

Multiplexing refers to a number of independent

signals are combined into a composite signal

suitable for transmission over a common channel.

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Types of Multiplexing

• FDM

Separate the signals according to frequency.

• TDM

Separate the signals according to time.

• CDM

Separate the signals according to code.

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Block diagram of FDM system

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Figure 2.19 Illustrating the modulation steps in an FDM system.

Example 2.1 Carrier Telephone System SSB/FDM

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2.9 Superheterodyne Receiver =superhet

Since Armstrong invented the superheterotyne

radio receiver in 1918, almost all radio and TV

receivers now being made are of the

superhetrodyne type.

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Receivers in a broadcasting system performs

following functions:

• Carrier-frequency tuning

• Filtering

• amplification

Seperhet is a special type of receiver that fulfills

all three functions in an elegant and practical

fashion.

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Image frequency

co

coc

ffff

fffff

LIF

LIF

如果

如果象频

2

2

c

Image Interference

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Figure 2.32 Basic elements of an AM radio receiver of the

superheterodyne type.

IF LO RFf f f

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Communication Systems

Unit -II

Angle Modulation

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2.6 Angle Modulation

• Definition:

The angle of the carrier wave is varied

according to the baseband signal. Whereas,

the amplitude of the carrier is maintained

constant. It consists of PM and FM.

• An important feature:

It provides better discrimination against

noise and interference than amplitude

modulation.

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Tradeoff

This improvement in performance is achieved

at the expense of increased transmission

bandwidth.

That is, angle modulation provides us with a

practical means of exchanging channel

bandwidth for improved noise performance.

Such a tradeoff is not possible with amplitude

modulation, regardless of its form.

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Basic Definition of Angle Modulation

Let i(t) denote the angle of a modulated carrier,

then angle-modulated wave can be expressed as

( ) cosc i

s t A t )()( tmti

If i(t) increases monotonically with time, the

average frequency in Hertz, over an interval

from t to t+t, is given by

( )

2

i i

t

t t tf t

t

2. 20

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Instantaneous frequency

0

0

( ) lim ( )

lim2

1 2.21

2

i tt

i i

t

i

f t f t

t t t

t

d t

dt

dttft ii )(2)(

In the simple case of an unmodulated carrier, the

angle i(t) is :

2i c c

t f t

The constant c is the value of i(t) at t=0. Usually it is

assumed to be zero for convenience.

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Angle modulation is defined as the angle of the

carrier wave varying with modulating signal .

There are an infinite number of ways in which

the angle may be varied in some manner with

the message signal.

However, we shall consider only two commonly

used methods. They are FM and PM.

)()( tmti

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Phase Modulation PM

The angle i(t) is varied linearly with the message

signal m(t)

2 ( )i c p

t f t k m t

kp: phase sensitivity

PM signal is described in the time domain by

( ) cos[ ( )] cos[2 ( )] 2.23PM c i c c p

s t A t A f t k m t

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Frequency Modulation FM

The instantaneous frequency fi(t) is varied

linearly with the message signal m(t)

kf: frequency sensitivity

FM signal is described in the time domain by

( ) 2.24i c f

f t f k m t

t

fcii dmktfdttft0

)(22)(2)( 2.25

0

( ) cos[ ( )]

cos[2 2 ( ) ] 2.26

FM c i

t

c c f

s t A t

A f t k m d

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Relationship between FM and PM

dttft ii )(2)( dt

tdtf i

i

)(

2

1)(

)](2cos[)( tmktfAts pccPM 2.23

So, we may deduce all the properties of PM signals

from those of FM signals and vice versa. Hence, we

concentrate our attention on FM signals.

0( ) cos[2 2 ( ) ] 2.26

t

FM c c fs t A f t k m d

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Modulating

signal Integrator

Phase modulator

cos(2 )c c

A f t

FM signal

Modulating

signal Frequency modulator

cos(2 )c c

A f t

FM signal

Direct method to generate FM signal

Indirect method to generate FM signal

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Modulating

signal Differentiator

Frequency modulator

cos(2 )c c

A f t

PM signal

Modulating

signal Phase modulator

cos(2 )c c

A f t

PM signal

Direct method to generate PM signal

Indirect method to generate PM signal

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2.7 Frequency Modulation FM

• The FM signal s(t) is a nonlinear function of

the modulating signal m(t), which makes the

frequency modulation a nonlinear modulation

process.

• Consequently, unlike amplitude modulation,

the spectrum of an FM signal is not related in

a simple manner to that of the modulating

signal; rather, its analysis is much more

difficult than that of an AM signal.

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How can we tackle the spectral analysis

of an FM signal?

1. First consider the simplest case:

a single-tone modulation, narrowband FM

2. Then consider more general case:

a single-tone modulation, wideband FM

Objective: to establish an empirical formula between

the transmission bandwidth of an FM signal and the

bandwidth of message signal.

We propose to provide an empirical answer to this

question by proceeding in the following manner:

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Single-tone frequency modulation

A single tone modulating signal is defined by

The instantaneous frequency of the FM signal:

Where f m

f k A f : Frequency deviation

2.27 )2cos()( tfAtm mm

cos 2

cos 2 2.28

i c f m m

c m

f t f k A f t

f f f t

fm: modulation frequency of modulating signal

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m

f

f

2 sin 2i c m

t f t f t

FM signal for single-tone modulating signal:

( ) cos 2 sin 2 2.33c c m

s t A f t f t

0

2 2 sin 2 2.30t

i i c m

m

ft f d f t f t

f

We define Modulation index

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Modulation index

f : Frequency deviation

Two important concepts in FM Page 110

maximum departure of the instantaneous

frequency of the FM signal from the carrier

frequency fc. It is proportional to the amplitude

of the modulating signal and is independent of

the modulation frequency fm.

Phase deviation, the maximum departure of the

angle i(t) from the angle 2fct of the unmodulated

carrier.

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Narrowband and Wideband FM

Depending on the value of the modulation index ,

there are two cases of frequency modulation:

Narrowband FM: <<1

Wideband FM: otherwise

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2.7.1 Narrowband Frequency Modulation NBFM

( ) cos 2 sin 2c c m

s t A f t f t

When <<1

Hence, NBFM signal can be expressed as:

FM signal for single-tone m(t):

Expanding it:

1)]2sin(cos[ tfm

)2sin()]2sin(sin[ tftf mm

( ) cos 2 cos sin 2

sin 2 sin sin 2 2.34

c c m

c c m

s t A f t f t

A f t f t

( ) ( ) cos(2 ) sin(2 )sin(2 )NBFM c c c m c

s t s t A f t A f t f t

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)2sin()2sin()2cos()( tftfAtfAts cmcccNBFM

Narrowband Frequency Modulator

Modulating

signal Integrator

sin(2 )c c

A f t

NBFM signal

-π/ 2

phase-shifter cos(2 )

c cA f tCarrier wave

-

+

NBPM modulator

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NBFM is different from ideal FM. Why?

1. The envelope contains a residual amplitude

modulation

2. The angle contains harmonic distortion

If <0.3 radians, the effects of residual AM and

harmonic PM are limited to negligible levels.

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NBFM is similar to AM.

Basic difference:

the algebraic sign of the lower side frequency

]})(2cos[])(2{cos[2

1)2cos(

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

tfftffAtfA

tftfAtfAts

mcmcccc

mccccNBFM

2.36

]})(2cos[])(2{cos[2

1)2cos(

)2cos()]2cos(1[

)2cos()](1[)(

tfftffAktfA

tftfAkA

tftmkAts

mcmccacc

cmmac

cacAM

2.37

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2.7.2 Wideband Frequency Modulation WBFM

For convenience, we use complex form to

describe band pass signal. It is changed into:

We have known that single-tone FM signal is:

( ) Re exp 2 sin 2

Re exp 2 2.38

c c m

c

s t A j f t j f t

s t j f t

( ) cos 2 sin 2 2.33c c m

s t A f t f t

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Where, Fourier coefficient cn

Complex envelope

exp sin 2 2.39c m

s t A j f t

exp 2 2.40n m

s t c j nf t

1/ 2

1/ 2

1/ 2

1/ 2

exp 2

exp sin 2 2

m

m

m

m

f

n m mf

f

m c m mf

c f s t j nf t dt

f A s t j f t j nf t dt

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2m

x f t

Hence, we may rewrite equation 2.41 in new form

exp sin2

c

n

Ac j x nx dx

So, we may reduce Cn

1exp sin 2.44

2n

J j x nx dx

2.45n c n

c A J

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exp 2c n m

s t A J j nf t

Therefore,

Re exp 2 2.48c n c m

s t A J j f nf t

2

c

n c m c m

AS f J f f nf f f nf

FT

Substituting Cn in , we get ( )s t

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Figure 2.23 Plots of Bessel functions of the first kind for

varying order.

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Bessel Function Properties

1. 1 for all n ,both positive and negative n

n nJ J

3. 2 1n

n

J

2.52

2. For small values of modulation index ,

2,0)(2

)(

1)(

1

0

nJ

J

J

n

2.51

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Observations About FM

1. The spectrum of an FM signal contains a

carrier component and an infinite set of side

frequencies.

21

2c

P A

2. If <1, the FM signal is effectively composed of

a carrier and a single pair of side frequencies at

fc±fm. This situation corresponds to NBFM.

3. The average power of FM signal is constant.

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How to estimate transmission bandwidth of FM signals?

• Percent method

• Cason’s rule

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mT fnB max2

percent method

Carson’s Rule

12 2 2 (1 ) 2 (1 )

2( 1) 2( 1) 2.55

m

T m

m m

m

fB f f f f

f

ff f

f

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Single tone signal arbitrary signal

Deviation ratio

W

fD

frequency modulationhighest

deviationfrequency

WDD

fWfBT )1(2)1

1(222

Carson’s rule is modified

D is similar to .

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Example 2.3

FM radio broadcasting:

W=15 kHz, f=75 kHz, BT =?

Deviation ratio is: D=75/15=5

1) According to Carson’s rule, we get transmission bandwidth:

BT=2(75+15)=180 kHz

2) According to percent method, universal curve tells:

BT=3.2 f=3.275=240 kHz

In practice, a bandwidth of 200 kHz is

allocated to each FM transmitter.

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Generation of FM signals

Two basic methods:

Voltage-controlled

Oscillator m(t) sFM(t)

2. Indirect FM

m(t) NBFM Modulator

Frequency Multiplier sFM(t)

1. Direct FM

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Figure 2.27 Block diagram of the indirect

method of generating a wideband FM signal

NBFM

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Why can a frequency multiplier change

NBFM into WBFM?

Figure 2.28 Block diagram of frequency multiplier

2

1 2

n

nt a s t a s t a s t

The input-output relation of a nonlinear device may

be expressed in the general form

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Instantaneous frequency is

i c ff t f k m t

Instantaneous frequency of output signal s’(t) is

Output signal s’(t) is

0

cos 2 2t

c c fs t A nf t nk m d

i c ff t nf nk m t

So cc nffnfnf '

NBFMWBFM

0

cos 2 2t

c c fs t A f t k m d

The input is an FM signal defined by

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Demodulation of FM Signals Page 121

Two basic methods:

2. Direct method: frequency discriminator

1. Indirect method: phase-locked loop

FM wave Slope circuit

Envelope Detector

Baseband signal

Figure 2.51

X

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Fig. 2.30 balanced frequency discriminator

+

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Communication Systems

Unit –III

Random Process

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Review of last lecture

• The point worth noting are :

– The source coding algorithm plays an

important role in higher code rate

(compressing data)

– The channel encoder introduce redundancy

in data

– The modulation scheme plays important role

in deciding the data rate and immunity of

signal towards the errors introduced by the

channel

– Channel can introduce many types of errors

due to thermal noise etc.

95

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Review:

Layering of Source Coding

• Source coding includes

– Sampling

– Quantization

– Symbols to bits

– Compression

• Decoding includes

– Decompression

– Bits to symbols

– Symbols to sequence of numbers

– Sequence to waveform (Reconstruction)

96

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Review:

Layering of Source Coding

97

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Review:

Layering of Channel Coding

• Channel Coding is divided into

– Discrete encoder\Decoder • Used to correct channel Errors

– Modulation\Demodulation • Used to map bits to waveform for transmission

98

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Review:

Layering of Channel Coding

99

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Review:

Resources of a Communication System

• Transmitted Power

– Average power of the transmitted signal

• Bandwidth (spectrum)

– Band of frequencies allocated for the signal

• Type of Communication system

– Power limited System • Space communication links

– Band limited Systems • Telephone systems

100

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Review:

Digital communication system • Important features of a DCS:

– Transmitter sends a waveform from a finite set of possible waveforms during a limited time

– Channel distorts, attenuates the transmitted signal and adds noise to it.

– Receiver decides which waveform was transmitted from the noisy received signal

– Probability of erroneous decision is an important measure for the system performance

101

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Review of Probability

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Sample Space and Probability

• Random experiment: its outcome, for

some reason, cannot be predicted with

certainty.

– Examples: throwing a die, flipping a coin and

drawing a card from a deck.

• Sample space: the set of all possible

outcomes, denoted by S. Outcomes are

denoted by E’s and each E lies in S, i.e., E ∈ S.

• A sample space can be discrete or

continuous.

103

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Three Axioms of Probability

• For a discrete sample space S, define a

probability measure P on as a set function

that assigns nonnegative values to all

events, denoted by E, in such that the

following conditions are satisfied

• Axiom 1: 0 ≤ P(E) ≤ 1 for all E ∈ S

• Axiom 2: P(S) = 1 (when an experiment is

conducted there has to be an outcome).

• Axiom 3: For mutually exclusive events

E1, E2, E3,. . . we have

104

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Conditional Probability

• We observe or are told that event E1 has occurred but are actually interested in event E2: Knowledge that of E1 has occurred changes the probability of E2 occurring.

• If it was P(E2) before, it now becomes P(E2|E1), the probability of E2 occurring given that event E1 has occurred.

• This conditional probability is given by

• If P(E2|E1) = P(E2), or P(E2 ∩ E1) = P(E1)P(E2), then E1 and E2 are said to be statistically independent.

• Bayes’ rule

– P(E2|E1) = P(E1|E2)P(E2)/P(E1) 105

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Mathematical Model for Signals

Mathematical models for representing signals Deterministic

Stochastic

Deterministic signal: No uncertainty with respect to the signal value at any time. Deterministic signals or waveforms are modeled by explicit mathematical

expressions, such as

x(t) = 5 cos(10*t). Inappropriate for real-world problems???

Stochastic/Random signal: Some degree of uncertainty in signal values before it actually occurs. For a random waveform it is not possible to write such an explicit expression.

Random waveform/ random process, may exhibit certain regularities that can be described in terms of probabilities and statistical averages.

e.g. thermal noise in electronic circuits due to the random movement of electrons 106

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107

Energy and Power Signals

• The performance of a communication system depends on the

received signal energy: higher energy signals are detected more

reliably (with fewer errors) than are lower energy signals.

• An electrical signal can be represented as a voltage v(t) or a current

i(t) with instantaneous power p(t) across a resistor defined by

OR

)(

)(2

tvtp

)()( 2titp

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108

Energy and Power Signals

• In communication systems, power is often normalized by assuming R to be 1.

• The normalization convention allows us to express the instantaneous power as

where x(t) is either a voltage or a current signal.

• The energy dissipated during the time interval (-T/2, T/2) by a real signal with

instantaneous power expressed by Equation (1.4) can then be written as:

• The average power dissipated by the signal during the interval is:

)()( 2txtp

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109

Energy and Power Signals

• We classify x(t) as an energy signal if, and only if, it has nonzero but

finite energy (0 < Ex < ∞) for all time, where

• An energy signal has finite energy but zero average power

• Signals that are both deterministic and non-periodic are termed as Energy

Signals

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110

Energy and Power Signals

• Power is the rate at which the energy is delivered

• We classify x(t) as an power signal if, and only if, it has nonzero but

finite energy (0 < Px < ∞) for all time, where

• A power signal has finite power but infinite energy

• Signals that are random or periodic termed as Power Signals

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Random Variable

• Functions whose domain is a sample

space and whose range is a some set of

real numbers is called random variables.

• Type of RV’s

– Discrete • E.g. outcomes of flipping a coin etc

– Continuous • E.g. amplitude of a noise voltage at a particular instant of time

111

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112

Random Variables

Random Variables

• All useful signals are random, i.e. the receiver does not know a priori

what wave form is going to be sent by the transmitter

• Let a random variable X(A) represent the functional relationship

between a random event A and a real number.

• The distribution function Fx(x) of the random variable X is given by

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Random Variable

• A random variable is a mapping from the

sample space to the set of real numbers.

• We shall denote random variables by

boldface, i.e., x, y, etc., while individual

or specific values of the mapping x are

denoted by x(w).

113

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Random process

• A random process is a collection of time functions, or signals,

corresponding to various outcomes of a random experiment. For each

outcome, there exists a deterministic function, which is called a sample

function or a realization.

Sample functions

or realizations

(deterministic

function)

Random

variables

time (t)

Rea

l n

um

ber

114

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Random Process

• A mapping from a sample space to a set of time functions.

115

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Random Process contd

• Ensemble: The set of possible time functions that one

sees.

• Denote this set by x(t), where the time functions x1(t,

w1), x2(t, w2), x3(t, w3), . . . are specific members of

the ensemble.

• At any time instant, t = tk, we have random variable

x(tk).

• At any two time instants, say t1 and t2, we have two

different random variables x(t1) and x(t2).

• Any realationship b/w any two random variables is

called Joint PDF

116

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Classification of Random Processes

• Based on whether its statistics change

with time: the process is non-stationary or

stationary.

• Different levels of stationary:

– Strictly stationary: the joint pdf of any order

is independent of a shift in time.

– Nth-order stationary: the joint pdf does not

depend on the time shift, but depends on time

spacing 117

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Cumulative Distribution Function (cdf)

• cdf gives a complete description of the random variable.

It is defined as:

FX(x) = P(E ∈ S : X(E) ≤ x) = P(X ≤ x). • The cdf has the following properties:

– 0 ≤ FX(x) ≤ 1 (this follows from Axiom 1 of the probability measure).

– Fx(x) is non-decreasing: Fx(x1) ≤ Fx(x2) if x1 ≤ x2 (this is because event x(E) ≤ x1 is contained in event x(E) ≤ x2).

– Fx(−∞) = 0 and Fx(+∞) = 1 (x(E) ≤ −∞ is the empty set, hence an impossible event, while x(E) ≤ ∞ is the whole sample space, i.e., a certain event).

– P(a < x ≤ b) = Fx(b) − Fx(a).

118

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Probability Density Function

• The pdf is defined as the derivative of the cdf: fx(x) = d/dx Fx(x)

• It follows that:

• Note that, for all i, one has pi ≥ 0 and ∑pi = 1.

119

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Cumulative Joint PDF Joint PDF

• Often encountered when dealing with combined experiments or repeated trials of a single experiment.

• Multiple random variables are basically multidimensional functions defined on a sample space of a combined experiment.

• Experiment 1 – S1 = {x1, x2, …,xm}

• Experiment 2 – S2 = {y1, y2 , …, yn}

• If we take any one element from S1 and S2 – 0 <= P(xi, yj) <= 1 (Joint Probability of two or more outcomes) – Marginal probabilty distributions

• Sum all j P(xi, yj) = P(xi) • Sum all i P(xi, yj) = P(yi)

120

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Expectation of Random Variables

(Statistical averages) • Statistical averages, or moments,

play an important role in the characterization of the random variable.

• The first moment of the probability distribution of a random variable X is called mean value mx or expected value of a random variable X

• The second moment of a probability distribution is mean-square value of X

• Central moments are the moments of the difference between X and mx, and second central moment is the variance of x.

• Variance is equal to the difference between the mean-square value and the square of the mean

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Contd

• The variance provides a measure of the

variable’s “randomness”. • The mean and variance of a random

variable give a partial description of its

pdf.

122

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Time Averaging and Ergodicity

• A process where any member of the

ensemble exhibits the same statistical

behavior as that of the whole ensemble.

• For an ergodic process: To measure

various statistical averages, it is sufficient

to look at only one realization of the

process and find the corresponding time

average.

• For a process to be ergodic it must be

stationary. The converse is not true.

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Gaussian (or Normal) Random Variable

(Process)

• A continuous random variable whose pdf

is:

μ and are parameters. Usually denoted as

N(μ, ) . • Most important and frequently

encountered random variable in

communications.

124

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Central Limit Theorem

• CLT provides justification for using

Gaussian Process as a model based if

– The random variables are statistically

independent

– The random variables have probability with

same mean and variance

125

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CLT

• The central limit theorem states that

– “The probability distribution of Vn approaches a normalized Gaussian

Distribution N(0, 1) in the limit as the

number of random variables approach

infinity”

• At times when N is finite it may provide a

poor approximation of for the actual

probability distribution

126

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127

Autocorrelation

Autocorrelation of Energy Signals

• Correlation is a matching process; autocorrelation refers to the

matching of a signal with a delayed version of itself

• The autocorrelation function of a real-valued energy signal x(t) is

defined as:

• The autocorrelation function Rx() provides a measure of how closely

the signal matches a copy of itself as the copy is shifted units in time.

• Rx() is not a function of time; it is only a function of the time

difference between the waveform and its shifted copy.

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Autocorrelation

• symmetrical in about zero

• maximum value occurs at the

origin

• autocorrelation and ESD

form a Fourier transform

pair, as designated by the

double-headed arrows

• value at the origin is equal to

the energy of the signal

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AUTOCORRELATION OF A PERIODIC (POWER)

SIGNAL

• The autocorrelation function of a real-valued

power signal x(t) is defined as:

• When the power signal x(t) is periodic with

period T0, the autocorrelation function can be

expressed as:

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130

Autocorrelation of power signals

• symmetrical in about zero

• maximum value occurs at the

origin

• autocorrelation and PSD

form a Fourier transform

pair, as designated by the

double-headed arrows

• value at the origin is equal to

the average power of the

signal

The autocorrelation function of a real-valued periodic signal

has properties similar to those of an energy signal:

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Spectral Density

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SPECTRAL DENSITY

• The spectral density of a signal characterizes the

distribution of the signal’s energy or power, in the frequency domain

• This concept is particularly important when considering

filtering in communication systems while evaluating the

signal and noise at the filter output.

• The energy spectral density (ESD) or the power spectral

density (PSD) is used in the evaluation.

• Need to determine how the average power or energy of

the process is distributed in frequency.

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Spectral Density

• Taking the Fourier transform of the

random process does not work

135

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ENERGY SPECTRAL DENSITY

• Energy spectral density describes the energy per unit bandwidth

measured in joules/hertz

• Represented as x(t), the squared magnitude spectrum

x(t) =|x(f)|2

• According to Parseval’s Relation

• Therefore

• The Energy spectral density is symmetrical in frequency about origin

and total energy of the signal x(t) can be expressed as

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Power Spectral Density

• The power spectral density (PSD) function Gx(f) of the periodic

signal x(t) is a real, even ad nonnegative function of frequency that

gives the distribution of the power of x(t) in the frequency domain.

• PSD is represented as (Fourier Series):

• PSD of non-periodic signals:

• Whereas the average power of a periodic signal x(t) is represented

as:

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Noise in the Communication System

• The term noise refers to unwanted electrical signals that are always

present in electrical systems: e.g. spark-plug ignition noise, switching

transients and other electro-magnetic signals or atmosphere: the sun and

other galactic sources

• Can describe thermal noise as zero-mean Gaussian random process

• A Gaussian process n(t) is a random function whose value n at any

arbitrary time t is statistically characterized by the Gaussian probability

density function

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WHITE NOISE

• The primary spectral characteristic of thermal noise is that its power

spectral density is the same for all frequencies of interest in most

communication systems

• A thermal noise source emanates an equal amount of noise power per

unit bandwidth at all frequencies—from dc to about 1012 Hz.

• Power spectral density G(f)

• Autocorrelation function of white noise is

• The average power P of white noise if infinite

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WHITE NOISE

140

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White Noise

• Since Rw( T) = 0 for T = 0, any two

different samples of white noise, no

matter how close in time they are taken,

are uncorrelated.

• Since the noise samples of white noise are

uncorrelated, if the noise is both white and

Gaussian (for example, thermal noise)

then the noise samples are also

independent. 141

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• The effect on the detection process of a channel

with Additive White Gaussian Noise (AWGN) is

that the noise affects each transmitted symbol

independently

• Such a channel is called a memoryless channel

• The term “additive” means that the noise is simply superimposed or added to the signal—that there are

no multiplicative mechanisms at work

ADDITIVE WHITE GAUSSIAN NOISE

(AWGN)

142

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Random Processes and Linear Systems

• If a random

process

forms the

input to a

time-

invariant

linear

system, the

output will

also be a

random

process 143

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Distortion less Transmission

Remember linear and non-linear

group delays in DSP

144

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DISTORTION LESS

TRANSMISSION

What is required of a network for it to behave

like an ideal transmission line?

• The output signal from an ideal

transmission line may have some time delay

and different amplitude as compared with

the input

• It must have no distortion—it must have the

same shape as the input

• For idea distortion less transmission

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Ideal Distortion Less Transmission

• The overall system response must have a constant magnitude response

• The phase shift must be linear with frequency

• All of the signal’s frequency components must also arrive with identical time delay in order to add up correctly

• The time delay t0 is related to the phase shift and the radian frequency

= 2f by

• A characteristic often used to measure delay distortion of a signal is

called envelope delay or group delay, which is defined as

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BANDWIDTH OF DIGITAL DATA

• Baseband signals

– Signals containing frequencies ranging from 0 to

some frequency fs

• Bandpass or Passband Signals

– Signals containing frequencies ranging from fs1 to

some frequency fs2

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Communication Systems

Unit –IV

Noise Characterization

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2.10 Noise in CW Modulation Systems

Formulating two models:

1. Channel model

2. Receiver model

AWGN: additive white Gaussian noise

Band-pass

filter Modulated

signal s (t) Demodulator

Output

signal

Noise w(t)

x(t)

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Signal-to-Noise Ratio: Basic Definitions

average power of signal

average power of noise SNR

Power spectral density of White noise w(t):

),(2

)( 0 - fN

fSW

N0 is the average noise power per unit

bandwidth.

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Furthermore, the output noise of filter can be

regarded as narrowband noise

cos 2 sin 2I c Q c

n t n t f t n t f t

Ideal band-pass filtered noise

Average noise power N0BT

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x t s t n t

The input of the demodulator is

s(t) is useful modulated signal

n(t) is narrowband noise

Band-pass

filter Modulated

signal s (t) Demodulator

Output

signal

Noise w(t)

x(t)

SNRI SNRO

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Requirements of Fair comparison:

1. The modulated signal s(t) has the same

average power.

2. The channel noise w(t) has the same average

power measured in the message bandwidth W.

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Figure 2.35 The baseband transmission model, assuming a message signal of

bandwidth W, used for calculating the channel signal-to-noise ratio.

C

O

(SNR)

(SNR)merit of Figure

SNRc

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2.11 Noise in Linear Receivers Using Coherent

Detection

• Linear receiver:

DSB-SC and SSB coherent detector

• Nonlinear receiver:

AM envelope detector

Take DSB for example to analyze noise

performance of coherent detection.

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cos 2DSB c c

s t CA m t f t

C: system-dependent scaling factor

设消息信号m(t)的功率谱密度为SM(f), 则它的平均功率P 为

W

MW

P S f df

Model of DSB-SC receiver using coherent detection

BPF DSB signal

s (t) LPF

y(t)

Noise w(t)

x(t) v(t)

cos2c

f t

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Average power of DSB 2

22 PACS c

DSB

Average noise power 0WNN

,

2 2

0

SNR 2.842

c

C DSB

C A P

WN

02i

N WN

so 2 2

0

SNR4

c

I

C A P

WN

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SNRO ?

cos 2 cos 2 cos 2

c c I c Q c

x t s t n t

CA f t m t n t f t n t f t

The output of the product-modulator is

cos 2

1 1

2 2

1 1cos 4 sin 4

2 2

c

c I

c I c Q c

v t x t f t

CA m t n t

CA m t n t f t n t f t

Output of LPF 1 1 2.86

2 2c I

y t CA m t n t

Input of the product-modulator is

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Output message signal:

The receiver output 1 1

2 2c I

y t CA m t n t

)(2

1)( tmCAts co

Power of output signal PACS co22

4

1

Noise output )(

2

1)(0 tntn I

Average Power of filtered noise n(t)

Average power of the in-phase noise component nI(t) is

the same as that of the filtered noise n(t).

Output noise power 00

2

2

12)

2

1( WNWNNout

WNNi 02

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The output SNR for a DSB-SC receiver using

coherent detection is therefore

,

2 2 2 2

_0 0

/ 4SNR 2.87

/ 2 2

c c

O DSB SC

C A P C A P

WN WN

Therefore SNR

Figure of merit= 1SNR

O

C DSB

SNR

Figure of merit= 1SNR

O

C SSB

Similar analysis to SSB demodulator Problem

2.49, we can get

SSB has the same figure of merit as DSB.

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2.12 Noise in AM receivers Using

Envelope Detection

AM signal 1 cos 2c a c

s t A k m t f t

Power of AM signal )1(2

1 22 PkAS acAM

Noise power 0WNN

Figure 2.37 Model of AM receiver.

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02I

N WN

2 2

,0

1SNR

4

c aI AM

I AMI I

A k PS S

N N WN

Channel SNR

2 2

,0

1SNR 2.90

2

c a

C AM

A k P

WN

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It’s difficult to get the relationship between

signal and noise. So, we just discuss it under

different conditions.

cos 2 sin 2

c c a I c Q c

x t s t n t

A A k m t n t f t n t f t

2.91

2 2

envelope of x t

= 2.92c c a I Q

y t

A A k m t n t n t

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1) When Signal>>Noise

2 2 c c a I Q

y t A A k m t n t n t

2 2 2 2 c c a c c a I I Q

A A k m t A A k m t n t n t n t

2

2 c c a c c a I

A A k m t A A k m t n t

( ) ( ) ( )c a I

y t A k m t n t

2 2[1 ( )] ( ) ( )c a I Q

A k m t n t n t

2 1

I

c c a

c c a

n tA A k m t

A A k m t

时当++ 1<< 2111 xxx

1

I

c c a

c c a

n tA A k m t

A A k m t

( ) ( ) ( ) c c a I

y t A A k m t n t

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Output SNR 0

22

,2

)(WN

PkASNR ac

AMO

2 2

O c aS A K P

02O

N WN

2

2

( )figure of merit =

( ) 1

O a

C aAM

SNR k P

SNR k P

2

2

2

1

o a

AM

I a

SNR k PG

SNR k P

( ) ( ) ( )c a I

y t A k m t n t

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• the figure of merit of DSB and SSB receivers

using coherent detection are always unity, the

corresponding figure of merit of an AM

receiver using envelope detection is always

less than unity.

Comparison: DSB SSB AM

• In other words, the noise performance of a

full AM receiver is always inferior to that of

a DSB or SSB receiver. This is due to the

wastage of transmission power, which results

from transmitting the carrier as a

component of the AM wave.

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Example 2.4 Single-tone Modulation

Single-tone modulating signal

cos 2m m

m t A f t

The corresponding AM wave

1 cos 2 cos 2AM c m c

s t A f t f t Modulation factor

ma Ak

Average power of m(t)

21

2m

P A

2 22

22 2

1SNR 2

1SNR 21

2

a mO

C AM a m

k A

k A

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discussion

2 22

22 2

1SNR 2

1SNR 21

2

a mO

C AM a m

k A

k A

• When =1, it corresponds to 100%

modulation, we get a figure of merit equal

to 1/3.

• This means that, other factors being equal,

an AM system must transmit three times as

much as average power as a suppressed-

carrier system to achieve the same quality

of noise performance.

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Figure 2.37 Model of AM receiver.

2 2

envelope of x t

= 2.92c c a I Q

y t

A A k m t n t n t

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2) When Signal<<Noise

cos 2c

n t r t f t t

In this case, the detector output has no component

strictly proportional to the message signal m(t).

)](cos[)()](cos[)()( ttmkAtAtrty acc

2 2[1 ( )] ( ) ( ) ( )c a I Q

A k m t n t n t r t

( )t( )r t

[1 ( )]c a

A k m t( )y t

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Threshold effect: the loss of a message in an

envelope detector that operates at a low SNR is

referred to as threshold effect.

Threshold Effect

Threshold : we mean a value of the SNR

below which the noise performance of a

detector deteriorates much more rapidly than

proportionately to the SNR.

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Communication Systems

Unit –IV

Noise Characterization

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2.13 Noise in FM Receivers

BPF

sFM (t)

LPF

y(t)

Noise w(t)

x(t) v(t)

Limiter Discriminator

Figure 2.40 Model of an FM receiver.

In theory, discriminator consists two parts;

In practice, these two parts are usually implemented

as integral parts as a single physical unit.

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cos 2 sin 2I c Q c

n t n t f t n t f t

cos 2c

n t r t f t t

In terms of its envelope and phase

1/ 22 2

I Qr t n t n t

1tan

Q

I

n tt

n t

r(t) is Rayleigh distributed, (t) is uniformly distributed.

BPF

sFM (t)

LPF

y(t)

Noise w(t)

x(t) v(t)

Limiter Discriminator

Figure 2.40 Model of an FM receiver.

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The incoming

FM signal

0cos 2 2

t

c c fs t A f t k m d

We define 0

2t

ft k m d

thus cos 2c c

s t A f t t

cos 2 cos 2

c c c

x t s t n t

A f t t r t f t t

The noisy signal at the band-pass filter output

BPF sFM (t)

LPF

y(t)

Noise w(t)

x(t) v(t)

Limiter Discriminator

Figure 2.40 Model of an FM receiver.

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Figure 2.41 Phasor diagram for FM wave plus narrowband noise

for the case of high carrier-to-noise ratio.

1sin

tancos

c

r t t tt t

A r t t t

2.137

The envelope of x(t) is of no interest to us, because any

envelope variations at the band-pass filter output are

removed by the limiter. So, we only focus on the phase

of x(t).

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The discriminator output

When CNR >>1, that is r(t)<<Ac CNR: Carrier-to-noise

)]()(sin[)(

)(2

)]()(sin[)(

)()(

0tt

A

trdmk

ttA

trtt

t

cf

c

2.139

Noise term of V(t)

1

2f d

d tv t k m t n t

dt

2.140

sin1

2d

c

d r t t tn t

A dt

2.141

Equation 2.140 shows that if CNR is large, the output of

the discriminator consists of message signal plus noise.

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Then, we may simplify Equation 2.141 as:

)]}(sin[)({2

1)( ttr

dt

d

Atn

cd

2.142

Because

)](sin[)()( ttrtnQ Thus

)(t is uniformly distributed over 2 radians. IF:

If CNR is high, it can be proved that )()( tt

is also uniformly distributed over 2 radians.

Then:

This means that the additive noise nd(t) is determined

by the carrier amplitude Ac and the quadrature

component nQ(t) of the narrowband noise n(t).

dt

tdn

Atn

Q

cd

)(

2

1)(

2.144

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To calculate SNRO

outputreceiver theat noise the ofpower average

signal ddemodulate the ofpower average)( OSNR

Output 1

2f d

d tv t k m t n t

dt

Output signal= )(tmk f Average signal power= Pk f2

P is the power of m(t).

nQ(t) Differentiator

H(f) nd(t)

cc A

jf

A

fjfH

2

2)(

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To calculate output noise power

2

2d QN N

c

fS f S f

A

The power spectral density of nd(t):

2( ) ( ) ( )Y XS f H f S f 1.58

Because

nQ(t) is low-pass filtered

noise. Thus

Power spectral density of n0(t) at the receiver out

(after low-pass filter)

2

0

2,

0,

oN c

N ff W

S f A

otherwise

2.147

2

0

2,

2

0,

d

T

N c

N f Bf

S f A

otherwise

2.146

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Figure 2.42 Noise analysis of FM receiver.

(a) Power spectral density of quadrature component nQ(t) of

narrowband noise n(t).

(b) Power spectral density of noise nd(t) at the discriminator output.

(c) Power spectral density of noise no(t) at the receiver output.

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Average signal power= Pk f2

Average power of FM

2

2c

FM

AS

Average noise power

0WNN

Therefore, 2

,0

2.1502

c

C FM

ASNR

N W

2 2

3,0

32.149

2

c f

O FM

A k PSNR

N W Therefore,

320 0

2 2

2Average power of output noise

3

W

Wc c

N N Wf df

A A 2.148

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2

2

3fO

C FM

SNR k P

SNR W

2 2

3,0

3

2

c f

O FM

A k PSNR

N W

2

,02

c

C FM

ASNR

N W

2.151

Deviation ratio 偏移率, 频偏比

W

fD

frequency modulationhighest

deviationfrequency

WDD

fWfBT )1(2)1

1(222

Since fkf Thus W

kD

f

So 23

)(

)(merit figure PD

SNR

SNR

FMC

O

D is similar to

modulation

index .

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• when carrier-to-noise is high, an increase in the

transmission bandwidth BT provides a

corresponding quadratic increase in the output

signal-to-noise ratio of figure of merit.

• FM improves noise performance at the cost of

transmission bandwidth.

23)(

)(merit figure PD

SNR

SNR

FMC

O

D Figure merit Good !

D Transmission bandwidth BT Bad !

Conclusion

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FM Threshold Reduction

Figure 2.47 FM demodulator with negative feedback.

Threshold reduction in FM receivers may be achieved

by using an FM demodulator with negative feedback,

or by using a phase-locked loop demodulator.

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Pre-Emphasis and De-Emphasis in FM

Figure 2.48 (a) Power spectral density of noise at FM receiver output.

(b) Power spectral density of a typical message signal.

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Fig. 2.49 Use of pre-emphasis and de-emphasis in an FM system.

Pre-emphasis

Hpe(f)

m(t) Noise w(t)

FM

Transmitter

FM

receiver

De-emphasis

Hde(f)

Recoverd

signal m(t)

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• Pre-emphasize the high-frequency components of

the message signal only in the transmitter;

• De-emphasize the high-frequency components of

the message signal and noise in the receiver.

• So effectively increase the output SNR

Frequency response Hpe(f) of the pre-emphasis filter

and frequency response Hde(f) satisfy following form:

WfWfH

fHpe

de ,)(

1)(

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Without pre- and depre-

2

0

2,

2

0,

d

T

N c

N f Bf

S f A

otherwise

2.146

With pre- and depre-

2

20

2 2| ( ) | ,

| ( ) | 2

0,

d

Tde

de N c

N f BH f f

H f S f A

otherwise

After Low Pass filter (-W,W),

2W

2 20

2

Average output noise power with de-emphasis

= | ( ) |de

Wc

N ff H f df

A

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Average output noise power pre-emphasis and de-emphasis

Average output noise power pre-emphasis and

wit

de

hout

wit -emp ish hasI

2

2 2

2 2.160

3 | ( ) |W

deW

WI

f H f df

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Example 2.6

(a) Pre-emphasis filter. (b) De-emphasis filter.

0

1pe

jfH f

f

0

1

1 /de

H fjf f

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32

0

2 1

0 0

2

0

( / )2

3[( / ) tan ( / )]3

1 ( / )

W

W

W fWI

f W f W fdf

f f

In commercial FM broadcasting:

0 2.1 , 15f kHz W kHz

22 13I dB

The improvement is Remarkable.

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Unit – 1: Information Theory

1.1 Introduction:

• Communication

Communication involves explicitly the transmission of information from one point to another, through a succession of processes.

• Basic elements to every communication system

o Transmitter

o Channel and

o Receiver

• Information sources are classified as:

• Source definition

Analog : Emit a continuous – amplitude, continuous – time electrical wave from.

Discrete : Emit a sequence of letters of symbols.

The output of a discrete information source is a string or sequence of symbols.

1.2 Measure the information:

To measure the information content of a message quantitatively, we are required to arrive at an intuitive concept of the amount of information.

Consider the following examples:

A trip to Mercara (Coorg) in the winter time during evening hours,

1. It is a cold day

2. It is a cloudy day

3. Possible snow flurries

INFORMATION SOURCE

ANALOG DISCRETE

Message signal

Receiver

User of

information

Transmitter

Source of information

CHANNEL

Transmitted signal

Received signal

Estimate of message signal

Communication System

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Amount of information received is obviously different for these messages.

o Message (1) Contains very little information since the weather in coorg is ‘cold’ for most part of the time during winter season.

o The forecast of ‘cloudy day’ contains more information, since it is not an event that occurs often.

o In contrast, the forecast of ‘snow flurries’ conveys even more information, since the occurrence of snow in coorg is a rare event.

� On an intuitive basis, then with a knowledge of the occurrence of an event, what can be said about the amount of information conveyed?

It is related to the probability of occurrence of the event.

� What do you conclude from the above example with regard to quantity of information?

Message associated with an event ‘least likely to occur’ contains most information.

� The information content of a message can be expressed quantitatively as follows:

The above concepts can now be formed interns of probabilities as follows:

Say that, an information source emits one of ‘q’ possible messages m1, m2 …… mq with p1, p2 …… pq as their probs. of occurrence.

Based on the above intusion, the information content of the kth message, can be written as

I (mk) α kp

1

Also to satisfy the intuitive concept, of information.

I (mk) must � zero as pk � 1

Therefore,

I (mk) > I (mj); if pk < pj

I (mk) � O (mj); if pk � 1 ------ I

I (mk) ≥ O; when O < pk < 1

Another requirement is that when two independent messages are received, the total information content is –

Sum of the information conveyed by each of the messages.

Thus, we have

I (mk & mq) I (mk & mq) = Imk + Imq ------ I

∴ We can define a measure of information as –

I (mk ) = log

kp

1 ------ III

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Unit of information measure

Base of the logarithm will determine the unit assigned to the information content.

Natural logarithm base : ‘nat’

Base - 10 : Hartley / decit

Base - 2 : bit

Use of binary digit as the unit of information?

Is based on the fact that if two possible binary digits occur with equal proby (p1 = p2 = ½) then the correct identification of the binary digit conveys an amount of information.

I (m1) = I (m2) = – log2 (½ ) = 1 bit

∴ One bit is the amount if information that we gain when one of two possible and equally likely events occurs.

Illustrative Example

A source puts out one of five possible messages during each message interval. The probs. of

these messages are p1 = 2

1 ; p2 =

4

1 ; p1 =

4

1 : p1 =

16

1, p5

16

1

What is the information content of these messages?

I (m1) = - log2

2

1 = 1 bit

I (m2) = - log2

4

1 = 2 bits

I (m3) = - log

8

1 = 3 bits

I (m4) = - log2

16

1 = 4 bits

I (m5) = - log2

16

1 = 4 bits

HW: Calculate I for the above messages in nats and Hartley

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SJBIT/ECE 8

Digital Communication System:

Entropy and rate of Information of an Information Source /

Model of a Mark off Source

1.3 Average Information Content of Symbols in Long Independence Sequences

Suppose that a source is emitting one of M possible symbols s0, s1 ….. sM in a statically independent sequence

Let p1, p2, …….. pM be the problems of occurrence of the M-symbols resply. suppose further that during a long period of transmission a sequence of N symbols have been generated.

On an average – s1 will occur NP1 times

S2 will occur NP2 times

: :

si will occur NPi times

The information content of the i th symbol is I (si) = log

ip

1 bits

∴ PiN occurrences of si contributes an information content of

PiN . I (si) = PiN . log

ip

1 bits

∴ Total information content of the message is = Sum of the contribution due to each of

Source of information

Source encoder

Channel encoder

Modulator

Channel

User of information

Source decoder

Channel decoder

Demodulator

Message signal

Transmitter Receiver

Source code word

Channel code word

Estimate of source codeword

Waveform Received

signal

Estimate of channel codeword

Estimate of the Message signal

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M symbols of the source alphabet

i.e., Itotal = ∑=

M

1i i1 p

1logNP bits

bygiveninsymbolerp

contentninforamtioAverage∴ H = ∑

=

=

M

1i i1

total

p

1logNP

N

I symbol

per bits ---- IV

This is equation used by Shannon

Average information content per symbol is also called the source entropy.

1.4 The average information associated with an extremely unlikely message, with an extremely likely message and the dependence of H on the probabilities of messages

consider the situation where you have just two messages of probs. ‘p’ and ‘(1-p)’.

Average information per message is H = p1

1log)p1(

p

1logp

−−+

At p = O, H = O and at p = 1, H = O again,

The maximum value of ‘H’ can be easily obtained as,

Hmax = ½ log2 2 + ½ log2 2 = log2 2 = 1

∴ Hmax = 1 bit / message

Plot and H can be shown below

The above observation can be generalized for a source with an alphabet of M symbols.

Entropy will attain its maximum value, when the symbol probabilities are equal,

i.e., when p1 = p2 = p3 = …………………. = pM = M

1

∴ Hmax = log2 M bits / symbol

Hmax = ∑M

M p

1logp

Hmax = ∑M

M 11

logp

H

1

O ½ P

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∴ Hmax = ∑ = MlogMlogM

122

• Information rate

If the source is emitting symbols at a fixed rate of ‘’rs’ symbols / sec, the average source information rate ‘R’ is defined as –

R = rs . H bits / sec

• Illustrative Examples

1. Consider a discrete memoryless source with a source alphabet A = { so, s1, s2} with respective probs. p0 = ¼, p1 = ¼, p2 = ½. Find the entropy of the source.

Solution: By definition, the entropy of a source is given by

H = ∑=

M

i ii p

p1

1log bits/ symbol

H for this example is

H (A) = ∑=

2

0

1log

i ii p

p

Substituting the values given, we get

H (A) = op log oP

1 + P1 log

22

1

1log

1

pp

p+

= ¼ 2log 4 + ¼ 2log 4 + ½ 2log 2

=

2

3 = 1.5 bits

if sr = 1 per sec, then

H′ (A) = sr H (A) = 1.5 bits/sec

2. An analog signal is band limited to B Hz, sampled at the Nyquist rate, and the samples are quantized into 4-levels. The quantization levels Q1, Q2, Q3, and Q4 (messages) are assumed independent and occur with probs.

P1 = P2 = 8

1 and P2 = P3 =

8

3. Find the information rate of the source.

Solution: By definition, the average information H is given by

H = 1p log 1

1

p + 2p log

2

1

p + 3p log

3

1

p+ 4p log

4

1

p

Substituting the values given, we get

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H = 8

1 log 8 +

8

3 log

3

8 +

8

3 log

3

8 +

8

1 log 8

= 1.8 bits/ message.

Information rate of the source by definition is

R = sr H

R = 2B, (1.8) = (3.6 B) bits/sec

3. Compute the values of H and R, if in the above example, the quantities levels are so chosen that they are equally likely to occur,

Solution:

Average information per message is

H = 4 (¼ log2 4) = 2 bits/message

and R = sr H = 2B (2) = (4B) bits/sec

1.5 Mark off Model for Information Sources

Assumption

A source puts out symbols belonging to a finite alphabet according to certain probabilities

depending on preceding symbols as well as the particular symbol in question.

• Define a random process

A statistical model of a system that produces a sequence of symbols stated above is and which

is governed by a set of probs. is known as a random process.

Therefore, we may consider a discrete source as a random process

And the converse is also true.

i.e. A random process that produces a discrete sequence of symbols chosen from a finite set

may be considered as a discrete source.

• Discrete stationary Mark off process?

Provides a statistical model for the symbol sequences emitted by a discrete source.

General description of the model can be given as below:

1. At the beginning of each symbol interval, the source will be in the one of ‘n’ possible states 1, 2,

….. n

Where ‘n’ is defined as

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n ≤ (M)m

M = no of symbol / letters in the alphabet of a discrete stationery source,

m = source is emitting a symbol sequence with a residual influence lasting

‘m’ symbols.

i.e. m: represents the order of the source.

m = 2 means a 2nd order source

m = 1 means a first order source.

The source changes state once during each symbol interval from say i to j. The probabilityy of

this transition is Pij. Pij depends only on the initial state i and the final state j but does not depend on

the states during any of the preceeding symbol intervals.

2. When the source changes state from i to j it emits a symbol.

Symbol emitted depends on the initial state i and the transition i � j.

3. Let s1, s2, ….. sM be the symbols of the alphabet, and let x1, x2, x3, …… xk,…… be a sequence of

random variables, where xk represents the kth symbol in a sequence emitted by the source.

Then, the probability that the kth symbol emitted is sq will depend on the previous symbols x1, x2,

x3, …………, xk–1 emitted by the source.

i.e., P (Xk = sq / x1, x2, ……, xk–1)

4. The residual influence of

x1, x2, ……, xk–1 on xk is represented by the state of the system at the beginning of the kth symbol

interval.

i.e. P (xk = sq / x1, x2, ……, xk–1) = P (xk = sq / Sk)

When Sk in a discrete random variable representing the state of the system at the beginning of the

kth interval.

Term ‘states’ is used to remember past history or residual influence in the same context as the use

of state variables in system theory / states in sequential logic circuits.

System Analysis with regard to Markoff sources

Representation of Discrete Stationary Markoff sources:

o Are represented in a graph form with the nodes in the graph to represent states and the transition between states by a directed line from the initial to the final state.

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o Transition probs. and the symbols emitted corresponding to the transition will be shown marked along the lines of the graph.

A typical example for such a source is given below.

o It is an example of a source emitting one of three symbols A, B, and C

o The probability of occurrence of a symbol depends on the particular symbol in question and the symbol immediately proceeding it.

o Residual or past influence lasts only for a duration of one symbol.

Last symbol emitted by this source

o The last symbol emitted by the source can be A or B or C. Hence past history can be represented by three states- one for each of the three symbols of the alphabet.

• Nodes of the source

o Suppose that the system is in state (1) and the last symbol emitted by the source was A.

o The source now emits symbol (A) with probability ½ and returns to state (1).

OR

o The source emits letter (B) with probability ¼ and goes to state (3)

OR

o The source emits symbol (C) with probability ¼ and goes to state (2).

State transition and symbol generation can also be illustrated using a tree diagram.

Tree diagram

• Tree diagram is a planar graph where the nodes correspond to states and branches correspond to transitions. Transitions between states occur once every Ts seconds.

Along the branches of the tree, the transition probabilities and symbols emitted will be indicated.Tree diagram for the source considered

P1(1) = 1/3

P2(1) = 1/3

P3(1) = 1/3

½

¼

½

¼ B

¼

B

A ¼

¼ C

½ A 1

C

2

3

C

A

¼

B

1 A

½ B ¼

C ¼

To state 3

To state 2

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1

1

3

1

2

3

1

2

3

2

1

2

3

1/3

½

¼

¼

A

½

¼

¼

A

C

B

AA

AC

AB

A

C

B

CA

CC

CB

A

C

B

BA

BC

BB

C

B

2

1

3

1

2

3

1

2

3

2

1

2

3

1/3

¼

½

¼

A

A

C

B

AA

AC

AB A

C

B

CA

CC

CB

A

C

B

BA

BC

BB

C

B

3

1

3

1

2

3

1

2

3

2

1

2

3

1/3

¼

¼

½

A

A

C

B

AA

AC

AB

A

C

B

CA

CC

CB

A

C

B

BA

BC

BB

C

B

Symbol probs.

Symbols emitted

State at the end of the first symbol internal

State at the end of the second symbol internal

Symbol sequence

Initial state

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Use of the tree diagram

Tree diagram can be used to obtain the probabilities of generating various symbol sequences.

Generation a symbol sequence say AB

This can be generated by any one of the following transitions:

OR

OR

Therefore proby of the source emitting the two – symbol sequence AB is given by

P(AB) = P ( S1 = 1, S2 = 1, S3 = 3 )

Or

P ( S1 = 2, S2 = 1, S3 = 3 ) ----- (1)

Or

P ( S1 = 3, S2 = 1, S3 = 3 )

Note that the three transition paths are disjoint.

Therefore P (AB) = P ( S1 = 1, S2 = 1, S3 = 3 ) + P ( S1 = 2, S2 = 1, S3 = 3 )

+ P ( S1 = 2, S2 = 1, S3 = 3 ) ----- (2)

The first term on the RHS of the equation (2) can be written as

P ( S1 = 2, S2 = 1, S3 = 3 )

= P ( S1 = 1) P (S2 = 1 / S1 = 1) P (S3 = 3 / S1 = 1, S2 = 1)

= P ( S1 = 1) P (S2 = 1 / S1= 1) P (S3 = 3 / S2 = 1)

1 2 3

2 1 3

3 1 3

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Recall the Markoff property.

Transition probability to S3 depends on S2 but not on how the system got to S2.

Therefore, P (S1 = 1, S2 = 1, S3 = 3 ) = 1/3 x ½ x ¼

Similarly other terms on the RHS of equation (2) can be evaluated.

Therefore P (AB) = 1/3 x ½ x ¼ + 1/3 x ¼ x ¼ + 1/3 x ¼ x ¼ = 48

4 =

12

1

Similarly the probs of occurrence of other symbol sequences can be computed.

Therefore,

In general the probability of the source emitting a particular symbol sequence can be computed by summing the product of probabilities in the tree diagram along all the paths that yield the particular sequences of interest.

Illustrative Example:

1. For the information source given draw the tree diagram and find the probs. of messages of lengths 1, 2 and 3.

Source given emits one of 3 symbols A, B and C

Tree diagram for the source outputs can be easily drawn as shown.

C ¼

C ¼

2 B 3/4 1 A

3/4

p1 = ½ P2 = ½

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Messages of length (1) and their probs

A � ½ x ¾ = 3/8

B � ½ x ¾ = 3/8

C � ½ x ¼ + ½ x ¼ = 8

1

8

1 + = ¼

Message of length (2)

How may such messages are there?

Seven

Which are they?

AA, AC, CB, CC, BB, BC & CA

What are their probabilities?

Message AA : ½ x ¾ x ¾ = 32

9

Message AC: ½ x ¾ x ¼ = 32

3 and so on.

1 ½ ¾

¼

A 1 2 ¼

1

2

AAA

AAC

ACC

ACB

1 1

2 ¾

A

C

¾ A

¼ C ¼ C 3/4 B

2 2

¼

1

2

CCA

CCC

CBC

CBB

1 1

2

¾

C

B

A

C C

B

¾

¼ ¼

3/4

C

2 ½ ¼

¾

C 1 2 ¼

1

2

CAA

CAC

CCC

CCB

1 1

2 ¾

A

C

¾ A

¼ C ¼ C 3/4 B

2 2

¼

1

2

BCA

BCC

BBC

BBB

1 1

2

¾

C

B

A

C C

B

¾

¼ ¼

3/4

B

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Messages of Length (1) Messages of Length (2) Messages of Length (3)

A

8

3 AA

32

9 AAA

128

27

B

8

3 AC

32

3 AAC

128

9

C

4

1 CB

32

3 ACC

128

3

CC

32

2 ACB

128

9

BB

32

9 BBB

128

27

BC

32

3 BBC

128

9

CA

32

3 BCC

128

3

BCA

128

9

CCA

128

3

CCB

128

3

CCC

128

2

CBC

128

3

CAC

128

3

CBB

128

9

CAA

128

9

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• A second order Markoff source Model shown is an example of a source where the probability of occurrence of a symbol

depends not only on the particular symbol in question, but also on the two symbols proceeding it.

No. of states: n ≤ (M)m; 4 ≤ M2

∴ M = 2 m = No. of symbols for which the residual influence lasts

(duration of 2 symbols) or

M = No. of letters / symbols in the alphabet. Say the system in the state 3 at the beginning of the symbols emitted by the source were BA. Similar comment applies for other states.

1.6 Entropy and Information Rate of Markoff Sources

• Definition of the entropy of the source

Assume that, the probability of being in state i at he beginning of the first symbol interval is the same as the probability of being in state i at the beginning of the second symbol interval, and so on.

The probability of going from state i to j also doesn’t depend on time, Entropy of state ‘i’ is defined as the average information content of the symbols emitted from the i-th state.

∑=

=n

j ijij p

p1

2i

1logH bits / symbol ------ (1)

Entropy of the source is defined as the average of the entropy of each state.

i.e. H = E(Hi) = ∑=

n

1jii Hp ------ (2)

Where,

Pi = the proby that the source is in state ‘i'.

Using eqn (1), eqn. (2) becomes,

(AA)

1/8

B

A

7/8

1 2

3 4 1/8

7/8

1/4

1/4

(AA)

(AB)

(BB)

P1 (1) 18

2

P2 (1) 18

7

P3 (1) 18

7

P4 (1) 18

2

B

3/4

3/4

A

B

B B

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H =

∑∑

==

n

j ijij

n

ii p

pp11

1log bits / symbol ------ (3)

Average information rate for the source is defined as

R = rs . H bits/sec

Where, ‘rs’ is the number of state transitions per second or the symbol rate of the source.

The above concepts can be illustrated with an example

Illustrative Example:

1. Consider an information source modeled by a discrete stationary Mark off random process shown in the figure. Find the source entropy H and the average information content per symbol in messages containing one, two and three symbols.

• The source emits one of three symbols A, B and C.

• A tree diagram can be drawn as illustrated in the previous session to understand the various symbol sequences and their probabilities.

1 ½ ¾

¼

A 1 2 ¼

1

2

AAA

AAC

ACC

ACB

1 1

2 ¾

A

C

¾ A

¼ C ¼ C 3/4 B

2 2

¼

1

2

CCA

CCC

CBC

CBB

1 1

2

¾

C

B

A

C C

B

¾

¼ ¼

3/4

C

2 ½ ¼

¾

C 1 2 ¼

1

2

CAA

CAC

CCC

CCB

1 1

2 ¾

A

C

¾ A

¼ C ¼ C 3/4 B

2 2

¼

1

2

BCA

BCC

BBC

BBB

1 1

2

¾

C

B

A

C C

B

¾

¼ ¼

3/4

B

C ¼

C ¼

2 B 3/4 1 A

3/4

p1 = ½ P2 = ½

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As per the outcome of the previous session we have Messages of Length (1) Messages of Length (2) Messages of Length (3)

A

8

3 AA

32

9 AAA

128

27

B

8

3 AC

32

3 AAC

128

9

C

4

1 CB

32

3 ACC

128

3

CC

32

2 ACB

128

9

BB

32

9 BBB

128

27

BC

32

3 BBC

128

9

CA

32

3 BCC

128

3

BCA

128

9

CCA

128

3

CCB

128

3

CCC

128

2

CBC

128

3

CAC

128

3

CBB

128

9

CAA

128

9

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By definition Hi is given by

∑=

=n

1j ijiji p

1logpH

Put i = 1,

∑=

==

2n

1j j1j1i p

1logpH

12

1211

11

1log

p

1 log

ppp +

Substituting the values we get,

( )

+=4/1

1log

4

1

4/3

1log

4

3221H

= ( )4log4

1

3

4log

4

322

+

H1 = 0.8113

Similarly H2 = 4

1 log 4 +

4

3log

3

4 = 0.8113

By definition, the source entropy is given by,

∑∑==

==2

1iii

n

1iii HpHpH

= 2

1 (0.8113) +

2

1 (0.8113)

= (0.8113) bits / symbol

To calculate the average information content per symbol in messages containing two symbols.

• How many messages of length (2) are present? And what is the information content of these messages?

There are seven such messages and their information content is:

I (AA) = I (BB) = log )(

1

AA = log

)(

1

BB

i.e., I (AA) = I (BB) = log )32/9(

1 = 1.83 bits

Similarly calculate for other messages and verify that they are

I (BB) = I (AC) =

I (CB) = I (CA) = log

)32/3(

1 = 3.415 bits

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I (CC) = log = )32/2(P

1 = 4 bits

• Computation of the average information content of these messages.

Thus, we have

H(two) = .sym/bitsP

1logP

i

7

1ii∑

=

= i

7

1ii I.P∑

=

Where Ii = the I’s calculated above for different messages of length two

Substituting the values we get,

)83.1(x32

9)415.3(x

32

3

)415.3(x32

3)4(

32

2)415.3(

32

3)415.3(x

32

3)83.1(

32

9 H (two)

++

++++=

bits56.2 H(two) =∴

• Computation of the average information content per symbol in messages containing two symbols using the relation.

GN = messagetheinsymbolsofNumber

Nlength of messages theofcontent n informatio Average

Here, N = 2

∴ GN = 2

(2)length of messages theofcontent n informatio Average

= 2

H )two(

= symbol/bits28.12

56.2 =

28.1G2 =∴

Similarly compute other G’s of interest for the problem under discussion viz G1 & G3.

You get them as

G1 = 1.5612 bits / symbol

And G3 = 1.0970 bits / symbol

• from the values of G’s calculated

We note that,

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SJBIT/ECE 24

G1 > G2 > G3 > H

• Statement

It can be stated that the average information per symbol in the message reduces as the length of the message increases.

• The generalized form of the above statement

If P (mi) is the probability of a sequence mi of ‘N’ symbols form the source with the average information content per symbol in the messages of N symbols defined by

GN = N

)m(Plog)m(Pi

ii∑−

Where the sum is over all sequences mi containing N symbols, then GN is a monotonic decreasing function of N and in the limiting case it becomes.

Lim G N = H bits / symbol

N ���� ∞

Recall H = entropy of the source

The above example illustrates the basic concept that the average information content per symbol from a source emitting dependent sequence decreases as the message length increases.

• It can also be stated as,

Alternatively, it tells us that the average number of bits per symbol needed to represent a message decreases as the message length increases.

Problems:

Example 1

The state diagram of the stationary Mark off source is shown below

Find (i) the entropy of each state

(ii) The entropy of the source (iii) G1, G2 and verify that G1 ≥ G2 ≥ H the entropy of the source.

Example 2

P(state1) = P(state2) =

P(state3) = 1/3

½

¼

½

¼ B

¼

B

A ¼

¼ C

½ A 1

C 2

3

C

A

¼

B

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For the Mark off source shown, calculate the information rate.

Solution:

By definition, the average information rate for the source is given by

R = rs . H bits/sec ------ (1)

Where, rs is the symbol rate of the source

And H is the entropy of the source.

To compute H

Calculate the entropy of each state using,

sym/bitsp

1logpH

ij

n

1jiJi ∑

== ----- (2)

For this example,

3,2,1i;p

1logpH

ij

3

1jiji ==∑

= ------ (3)

Put i = 1

jj

ji ppH 1

3

11 log∑

==∴

= - p11 log p11 – p12 log p12 – p13 log p13

Substituting the values, we get

H1 = - 2

1 x log

2

1 -

2

1 log

2

1 - 0

= + 2

1 log (2) +

2

1 log (2)

∴ H1 = 1 bit / symbol

Put i = 2, in eqn. (2) we get,

H2 = - ∑=

3

1jj2j2 plogp

i.e., H2 = - [ ]232322222121 plogpplogpplogp ++

Substituting the values given we get,

R ¼

S ½

3 R 1/2 L ¼

S ½

2 1 L

½

p1 = ¼ P2 = ½

S ½

P3 = ¼

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H2 = -

+

+

4

1log

4

1

2

1log

2

1

4

1log

4

1

= + 4

1 log 4 +

2

1 log 2 +

4

1 log 4

= 2

1 log 2 +

2

1 + log 4

∴ H2 = 1.5 bits/symbol

Similarly calculate H3 and it will be

H3 = 1 bit / symbol

With Hi computed you can now compute H, the source entropy, using.

H = ∑=

3

1iii

HP

= p1 H1 + p2 H2 + p3 H3

Substituting the values we get,

H = 41

x 1 + 21

x 1.5 + 41

x 1

= 41

+ 25.1

+ 41

= 2

1 +

2

5.1 =

2

5.2 = 1.25 bits / symbol

∴ H = 1.25 bits/symbol

Now, using equation (1) we have

Source information rate = R = rs 1.25

Taking ‘rs’ as one per second we get

R = 1 x 1.25 = 1.25 bits / sec

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Review questions:

(1) Explain the terms (i) Self information (ii) Average information (iii) Mutual Information.

(2) Discuss the reason for using logarithmic measure for measuring the amount of information.

(3) Explain the concept of amount of information associated with message. Also explain what infinite information is and zero information.

(4) A binary source emitting an independent sequence of 0’s and 1’s with probabilities p and (1-

p) respectively. Plot the entropy of the source.

(5) Explain the concept of information, average information, information rate and redundancy as referred to information transmission.

(6) Let X represents the outcome of a single roll of a fair dice. What is the entropy of X?

(7) A code is composed of dots and dashes. Assume that the dash is 3 times as long as the dot and

has one-third the probability of occurrence. (i) Calculate the information in dot and that in a dash; (ii) Calculate the average information in dot-dash code; and (iii) Assume that a dot lasts for 10 ms and this same time interval is allowed between symbols. Calculate the average rate of information transmission.

(8) What do you understand by the term extension of a discrete memory less source? Show that

the entropy of the nth extension of a DMS is n times the entropy of the original source.

(9) A card is drawn from a deck of playing cards. A) You are informed that the card you draw is spade. How much information did you receive in bits? B) How much information did you receive if you are told that the card you drew is an ace? C) How much information did you receive if you are told that the card you drew is an ace of spades? Is the information content of the message “ace of spades” the sum of the information contents of the messages ”spade” and “ace”?

(10) A block and white TV picture consists of 525 lines of picture information. Assume that each

consists of 525 picture elements and that each element can have 256 brightness levels. Pictures are repeated the rate of 30/sec. Calculate the average rate of information conveyed by a TV set to a viewer.

(11) A zero memory source has a source alphabet S= {S1, S2, S3} with P= {1/2, 1/4, 1/4}. Find

the entropy of the source. Also determine the entropy of its second extension and verify that H (S2) = 2H(S).

(12) Show that the entropy is maximum when source transmits symbols with equal probability.

Plot the entropy of this source versus p (0<p<1).

(13) The output of an information source consists OF 128 symbols, 16 of which occurs with probability of 1/32 and remaining 112 occur with a probability of 1/224. The source emits 1000 symbols/sec. assuming that the symbols are chosen independently; find the rate of information of the source.

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2

1

3

1

2

3

2

1

2

3

1/3

¼

½

¼

A

A

C

B

A

C

B

BA

BC

BB

C

B

3

1

3

1

2

3

1

2

3

2

1

2

3

1/3

¼

¼

½

A

A

C

B

AA

AC

AB

A

C

B

CA

CC

CB

A

C

B

BA

BC

BB

C

B

State at the end of the first symbol internal

State at the end of the second symbol internal

Symbol sequence

Initial state

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Unit - 2: SOURCE CODING

Syllabus:

Encoding of the source output, Shannon’s encoding algorithm. Communication Channels, Discrete communication channels, Continuous channels.

Text Books:

• Digital and analog communication systems, K. Sam Shanmugam, John Wiley, 1996.

Reference Books:

• Digital Communications - Glover and Grant; Pearson Ed. 2nd Ed 2008

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Unit - 2: SOURCE CODING

2.1 Encoding of the Source Output:

• Need for encoding

Suppose that, M – messages = 2N, which are equally likely to occur. Then recall that average information per messages interval in H = N.

Say further that each message is coded into N bits,

∴ Average information carried by an individual bit is = 1N

H = bit

If the messages are not equally likely, then ‘H’ will be less than ‘N’ and each bit will carry less than one bit of information.

• Is it possible to improve the situation?

Yes, by using a code in which not all messages are encoded into the same number of bits. The more likely a message is, the fewer the number of bits that should be used in its code word.

• Source encoding

Process by which the output of an information source is converted into a binary sequence.

• If the encoder operates on blocks of ‘N’ symbols, the bit rate of the encoder is given as

Produces an average bit rate of GN bits / symbol

Where, GN = – ∑i

ii )m(plog)m(pN

1

)m(p i = Probability of sequence ‘m i’ of ‘N’ symbols from the source,

Sum is over all sequences ‘mi’ containing ‘N’ symbols.

GN in a monotonic decreasing function of N and

∞→N

Lim GN = H bits / symbol

Performance measuring factor for the encoder

Coding efficiency: ηc

Definition of ηc = encoder theof ratebit output Average

rateormationinf Source

ηc = ^

NH

)S(H

Symbol sequence emitted by the information source

Source Encoder

Input Output : a binary sequence

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2.2 Shannon’s Encoding Algorithm:

• Formulation of the design of the source encoder

Can be formulated as follows:

‘q’ messages : m1, m2, …..mi, …….., mq

Probs. of messages : p1, p2, ..…..pi, ……..., pq

ni : an integer

• The objective of the designer

To find ‘ni’ and ‘ci’ for i = 1, 2, ...., q such that the average number of bits per symbol ^

NH

used in the coding scheme is as close to GN as possible.

Where, ^

NH = ∑=

q

1iii pn

N

1

and GN = ∑=

q

1i ii p

1logp

N

1

i.e., the objective is to have

^

NH � GN as closely as possible

• The algorithm proposed by Shannon and Fano

Step 1: Messages for a given block size (N) m1, m2, ....... mq are to be arranged in decreasing order of probability.

Step 2: The number of ‘ni’ (an integer) assigned to message mi is bounded by

log2 i

2ii p

1log1n

p

1 +<<

Step 3: The code word is generated from the binary fraction expansion of ‘F i’ defined as

One of ‘q’ possible messages

A message

N-symbols

Source encoder

INPUT OUTPUTA unique binary code word ‘ci’ of length ‘ni’ bits for the message ‘mi’

Replaces the input message symbols by a sequence of

binary digits

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ITC 10EC55

32

Fi = ∑−

=

1i

1kkp , with F1 taken to be zero.

Step 4: Choose ‘n i’ bits in the expansion of step – (3)

Say, i = 2, then if ni as per step (2) is = 3 and

If the Fi as per stop (3) is 0.0011011

Then step (4) says that the code word is: 001 for message (2)

With similar comments for other messages of the source.

The codeword for the message ‘m i’ is the binary fraction expansion of Fi upto ‘ni’ bits.

i.e., Ci = (Fi)binary, ni bits

Step 5: Design of the encoder can be completed by repeating the above steps for all the messages of block length chosen.

• Illustrative Example

Design of source encoder for the information source given,

Compare the average output bit rate and efficiency of the coder for N = 1, 2 & 3.

Solution:

The value of ‘N’ is to be specified.

Case – I: Say N = 3 Block size

Step 1: Write the tree diagram and get the symbol sequence of length = 3.

Tree diagram for illustrative example – (1) of session (3)

C ¼

C ¼

2 B 3/4 1 A

3/4

p1 = ½ P2 = ½

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From the previous session we know that the source emits fifteen (15) distinct three symbol messages.

They are listed below:

Messages AAA AAC ACC ACB BBB BBC BCC BCA CCA CCB CCC CBC CAC CBB CAA

Probability

128

27

128

9

128

3

128

9

128

27

128

9

128

3

128

9

128

3

128

3

128

2

128

3

128

3

128

9

128

9

Step 2: Arrange the messages ‘mi’ in decreasing order of probability.

Messages

mi AAA BBB CAA CBB BCA BBC AAC ACB CBC CAC CCB CCA BCC ACC CCC

Probability

pi

128

27

128

27

128

9

128

9

128

9

128

9

128

9

128

9

128

3

128

3

128

3

128

3

128

3

128

3

128

2

Step 3: Compute the number of bits to be assigned to a message ‘mi’ using.

Log2 i

2ii p

1log1n

p

1 +<< ; i = 1, 2, ……. 15

Say i = 1, then bound on ‘ni’ is

log 27

128log1n

27

1281 +<<

1 ½ ¾

¼

A 1 2 ¼

1

2

AAA

AAC

ACC

ACB

1 1

2 ¾

A

C

¾ A

¼ C ¼ C 3/4 B

2 2

¼

1

2

CCA

CCC

CBC

CBB

1 1

2

¾

C

B

A

C C

B

¾

¼ ¼

3/4

C

2 ½ ¼

¾

C 1 2 ¼

1

2

CAA

CAC

CCC

CCB

1 1

2 ¾

A

C

¾ A

¼ C ¼ C 3/4 B

2 2

¼

1

2

BCA

BCC

BBC

BBB

1 1

2

¾

C

B

A

C C

B

¾

¼ ¼

3/4

B

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i.e., 2.245 < n1 < 3.245

Recall ‘ni’ has to be an integer

∴ n1 can be taken as,

n1 = 3

Step 4: Generate the codeword using the binary fraction expansion of Fi defined as

Fi = ∑−

=

1i

1kkp ; with F1 = 0

Say i = 2, i.e., the second message, then calculate n2 you should get it as 3 bits.

Next, calculate F2 = 128

27pp

1

1kk

12

1kk == ∑∑

=

=

. Get the binary fraction expansion of 128

27. You

get it as : 0.0011011

Step 5: Since ni = 3, truncate this exploration to 3 – bits.

∴ The codeword is: 001

Step 6: Repeat the above steps and complete the design of the encoder for other messages listed above.

The following table may be constructed

Message mi

pi Fi ni Binary expansion of

Fi Code word ci

AAA

BBB

CAA

CBB

BCA

BBC

AAC

ACB

128

27

128

27

128

9

128

9

128

9

128

9

128

9

128

9

128

3

0

27/128

54/128

63/128

72/128

81/128

90/128

99/128

3

3

4

4

4

4

4

4

.00000

.001101

0110110

0111111

.1001100

1010001

1011010

1100011

000

001

0110

0111

1001

1010

1011

1100

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CBC

CAC

CCB

CCA

BCC

ACC

CCC

128

3

128

3

128

3

128

3

128

3

128

2

108/128

111/128

114/128

117/128

120/128

123/128

126/128

6

6

6

6

6

6

6

110110

1101111

1110010

1110101

1111000

1111011

1111110

110110

110111

111001

111010

111100

111101

111111

• the average number of bits per symbol used by the encoder

Average number of bits = ∑ ii pn

Substituting the values from the table we get,

Average Number of bits = 3.89

∴ Average Number of bits per symbol = N

nnH ii

^

N∑=

Here N = 3,

∴ 3

89.3H

^

3 = = 1.3 bits / symbol

State entropy is given by

Hi =

= ij

n

1jij p

1logp bits / symbol

Here number of states the source can be in are two

i.e., n = 2

Hi =

= ij

2

1jij p

1logp

Say i = 1, then entropy of state – (1) is

Hi = ∑=

2

1jijp

1212

1111

j1 p

1logp

p

1logp

p

1log +=

Substituting the values known we get,

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H1 = ( ) 4/1

1log

4

1

4/3

1logx

4

3 +

= ( )4log4

1

3

4logx

4

3 +

∴ H1 = 0.8113

Similarly we can compute, H2 as

H2 = 22

2

12221

2121

1log

1log

ppp

pp

j∑

=

+=

Substituting we get,

H2 = ( )

+4/3

1log

4

3

4/1

1logx

4

1

= ( )

+3

4log

4

34log

4

1x

H2 = 0.8113

Entropy of the source by definition is

H = ;Hpn

1jii∑

=

Pi = Probability that the source is in the ith state.

H = ;2

1∑

=iii Hp = p1H1 + p2H2

Substituting the values, we get,

H = ½ x 0.8113 + ½ x 0.8113 = 0.8113

∴ H = 0.8113 bits / sym.

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• What is the efficiency of the encoder?

By definition we have

ηc = %4.621003.1

8113.0100100

^

3

^

2

==== xxH

Hx

H

H

∴ ηc for N = 3 is, 62.4%

Case – II

Say N = 2

The number of messages of length ‘two’ and their probabilities (obtained from the tree diagram) can be listed as shown in the table.

Given below

N = 2

Message pi ni ci

AA

BB

AC

CB

BC

CA

CC

9/32

9/32

3/32

3/32

3/32

3/32

2/32

2

2

4

4

4

4

4

00

01

1001

1010

1100

1101

1111

Calculate ^

NH and verify that it is 1.44 bits / sym.

∴ Encoder efficiency for this case is

ηc = 100xH

H^

N

Substituting the values we get,

ηc = 56.34%

Case – III: N = 1

Proceeding on the same lines you would see that

N = 1

Message pi ni ci

A

B

C

3/8

3/8

1/4

2

2

2

00

01

11

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^

1H = 2 bits / symbol and

ηc = 40.56%

• Conclusion for the above example

We note that the average output bit rate of the encoder

^

NH decreases as ‘N’ increases and

hence the efficiency of the encoder increases as ‘N’ increases.

Operation of the Source Encoder Designed:

I. Consider a symbol string ACBBCAAACBBB at the encoder input. If the encoder uses a block size of 3, find the output of the encoder.

Recall from the outcome of session (5) that for the source given possible three symbol sequences and their corresponding code words are given by –

Message

mi ni

Codeword

ci

Determination of the code words and their size as illustrated in the previous session

AAA

BBB

CAA

CBB

BCA

BBC

AAC

ACB

CBC

CAC

CCB

CCA

BCC

ACC

3

3

4

4

4

4

4

4

6

6

6

6

6

6

000

001

0110

0111

1001

1010

1011

1100

110110

110111

111001

111010

111100

111101

C ¼

C ¼

2 B 3/4 1 A

3/4

p1 = ½ P2 = ½

SOURCE ENCODER

OUTPUT

INFORMN. SOURCE

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CCC 6 111111

Output of the encoder can be obtained by replacing successive groups of three input symbols by the code words shown in the table. Input symbol string is

{ string symbol theof version Encoded BBB AAC BCA ACB

011101110011100 ←321321321

II. If the encoder operates on two symbols at a time what is the output of the encoder for the same symbol string?

Again recall from the previous session that for the source given, different two-symbol sequences and their encoded bits are given by

N = 2

Message

mi

No. of bits

ni

ci

AA

BB

AC

CB

BC

CA

CC

2

2

4

4

4

4

4

00

01

1001

1010

1100

1101

1111

For this case, the symbol string will be encoded as –

{ { { {{ { message Encoded BBCBAA CA BB AC

011010001101011001 ←

DECODING

• How is decoding accomplished?

By starting at the left-most bit and making groups of bits with the codewords listed in the table.

Case – I: N = 3

i) Take the first 3 – bit group viz 110 why?

ii) Check for a matching word in the table.

iii) If no match is obtained, then try the first 4-bit group 1100 and again check for the matching word.

iv) On matching decode the group.

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NOTE: For this example, step (ii) is not satisfied and with step (iii) a match is found and the decoding results in ACB.

Repeat this procedure beginning with the fifth bit to decode the remaining symbol groups. Symbol string would be ���� ACB BCA AAC BCA • Conclusion from the above example with regard to decoding

It is clear that the decoding can be done easily by knowing the codeword lengths apriori if no errors occur in the bit string in the transmission process.

• The effect of bit errors in transmission

Leads to serious decoding problems.

Example: For the case of N = 3, if the bit string, 1100100110111001 was received at the decoder input with one bit error as

1101100110111001

What then is the decoded message?

Solution: Received bit string is

For the errorless bit string you have already seen that the decoded symbol string is

ACB BCA AAC BCA ----- (2)

(1) and (2) reveal the decoding problem with bit error.

Illustrative examples on source encoding

1. A source emits independent sequences of symbols from a source alphabet containing five symbols with probabilities 0.4, 0.2, 0.2, 0.1 and 0.1.

i) Compute the entropy of the source

ii) Design a source encoder with a block size of two.

Solution: Source alphabet = (s1, s2, s3, s4, s5)

Probs. of symbols = p1, p2, p3, p4, p5

= 0.4, 0.2, 0.2, 0.1, 0.1

(i) Entropy of the source = H = symbol/bitsplogp5

1iii∑

=

Substituting we get,

H = - [p1 log p1 + p2 log p2 + p3 log p3 + p4 log p4 + p5 log p5 ]

= - [0.4 log 0.4 + 0.2 log 0.2 + 0.2 log 0.2 + 0.1 log 0.1 + 0.1 log 0.1]

1101 10 011 0 1 110 1

Error bit

CBC CAA CCB ----- (1)

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H = 2.12 bits/symbol

(ii) Some encoder with N = 2

Different two symbol sequences for the source are:

(s1s1) AA ( ) BB ( ) CC ( ) DD ( ) EE

A total of 25 messages

(s1s2) AB ( ) BC ( ) CD ( ) DE ( ) ED

(s1s3) AC ( ) BD ( ) CE ( ) DC ( ) EC

(s1s4) AD ( ) BE ( ) CB ( ) DB ( ) EB

(s1s5) AE ( ) BA ( ) CA ( ) DA ( ) EA

Arrange the messages in decreasing order of probability and determine the number of bits ‘ni’ as explained.

Messages Proby. pi

No. of bits ni

AA 0.16 3

AB AC BC BA CA

0.08 0.08 0.08 0.08 0.08

4

...

...

...

...

...

...

...

0.04 0.04 0.04 0.04 0.04 0.04 0.04

5

...

...

...

...

...

...

...

...

0.02 0.02 0.02 0.02 0.02 0.02 0.02 0.02

6

...

...

...

...

0.01 0.01 0.01 0.01

7

Calculate ^

1H =

Substituting, ^

1H = 2.36 bits/symbol

2. A technique used in constructing a source encoder consists of arranging the messages in decreasing order of probability and dividing the message into two almost equally probable

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groups. The messages in the first group are given the bit ‘O’ and the messages in the second group are given the bit ‘1’. The procedure is now applied again for each group separately, and continued until no further division is possible. Using this algorithm, find the code words for six messages occurring with probabilities, 1/24, 1/12, 1/24, 1/6, 1/3, 1/3

Solution: (1) Arrange in decreasing order of probability

m5 1/3 0 0

m6 1/3 0 1

m4 1/6 1 0

m2 1/12 1 1 0

m1 1/24 1 1 1 0

m3 1/24 1 1 1 1

∴ Code words are

m1 = 1110

m2 = 110

m3 = 1111

m4 = 10

m5 = 00

m6 = 01

Example (3)

a) For the source shown, design a source encoding scheme using block size of two symbols and variable length code words

b) Calculate ^

2H used by the encoder

c) If the source is emitting symbols at a rate of 1000 symbols per second, compute the output bit rate of the encoder.

R ¼

S ½

3 R 1/2 L ¼

S ½

2 1 L

½

p1 = ¼ P2 = ½

S ½

P3 = ¼

1st division

2nd division

3rd division

4th division

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Solution (a)

1. The tree diagram for the source is

2. Note, there are seven messages of length (2). They are SS, LL, LS, SL, SR, RS & RR.

3. Compute the message probabilities and arrange in descending order.

4. Compute ni, Fi. Fi (in binary) and ci as explained earlier and tabulate the results, with usual notations.

Message

mi pi ni Fi Fi (binary) ci

SS 1/4 2 0 .0000 00

LL 1/8 3 1/4 .0100 010

LS 1/8 3 3/8 .0110 011

SL 1/8 3 4/8 .1000 100

SR 1/8 3 5/8 .1010 101

RS 1/8 3 6/8 .1100 110

RR 1/8 3 7/8 .1110 111

1 ¼ ¼

¼

1

LL

LS

C

2 ½ ¼

¾

1

2

½

2 ½

1 ½

2 3

¼ 1

¼

2 ½

2 ½

1 ½

¼ 2

3

¼ 1 2

½

3 ½

2 ½

3 ¼ ½

½ 3

C

3 ½

2 ½

2 3

¼ 1

¼

2 ½

SL

SS SR

LL

LS

SL

SS

SR

RS

RS

RR

SL

SS

SR

(1/16)

(1/16)

(1/32)

(1/16) (1/32)

(1/16)

(1/16)

(1/16)

(1/8)

(1/16)

(1/8)

(1/16)

(1/16)

(1/32)

(1/16)

(1/32)

LL

LS

SL

SS

SR

RS

RR

Different Messages of Length Two

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G2 =

−∑

7

12log

2

1

iii pp = 1.375 bits/symbol

(b) ^

2H =

7

12

1

iii np = 1.375 bits/symbol

Recall, ^

NH ≤ GN + N

1 ; Here N = 2

∴ ^

2H ≤ G2 + 2

1

(c) Rate = 1375 bits/sec.

2.3 SOURCE ENCODER DESIGN AND COMMUNICATION CHANNELS

• The schematic of a practical communication system is shown.

Fig. 1: BINARY COMMN. CHANNEL CHARACTERISATION

• ‘Communication Channel’

Communication Channel carries different meanings and characterizations depending on its terminal points and functionality.

(i) Portion between points c & g:

� Referred to as coding channel

� Accepts a sequence of symbols at its input and produces a sequence of symbols at its output.

� Completely characterized by a set of transition probabilities pij. These probabilities will depend on the parameters of – (1) The modulator, (2) Transmission media, (3) Noise, and (4) Demodulator

Channel Encoder

Channel Encoder

Electrical Commun-

ication channel

OR Transmission medium

Demodulator Channel Decoder Σ

b c d e f g h

Noise

Data Communication Channel (Discrete)

Coding Channel (Discrete)

Modulation Channel (Analog)

Transmitter Physical channel Receiver

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� A discrete channel

(ii) Portion between points d and f:

� Provides electrical connection between the source and the destination.

� The input to and the output of this channel are analog electrical waveforms.

� Referred to as ‘continuous’ or modulation channel or simply analog channel.

� Are subject to several varieties of impairments –

� Due to amplitude and frequency response variations of the channel within the passband.

� Due to variation of channel characteristics with time.

� Non-linearities in the channel.

� Channel can also corrupt the signal statistically due to various types of additive and multiplicative noise.

2.4 Mathematical Model for Discrete Communication Channel:

Channel between points c & g of Fig. – (1)

• The input to the channel?

A symbol belonging to an alphabet of ‘M’ symbols in the general case is the input to the channel.

• he output of the channel

A symbol belonging to the same alphabet of ‘M’ input symbols is the output of the channel.

• Is the output symbol in a symbol interval same as the input symbol during the same symbol interval?

The discrete channel is completely modeled by a set of probabilities –

t

ip � Probability that the input to the channel is the ith symbol of the alphabet.

(i = 1, 2, …………. M)

and

ijp � Probability that the ith symbol is received as the jth symbol of the alphabet at the output of

the channel.

• Discrete M-ary channel

If a channel is designed to transmit and receive one of ‘M’ possible symbols, it is called a discrete M-ary channel.

• discrete binary channel and the statistical model of a binary channel

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Shown in Fig. – (2).

Fig. – (2)

• Its features

� X & Y: random variables – binary valued

� Input nodes are connected to the output nodes by four paths.

(i) Path on top of graph : Represents an input ‘O’ appearing

correctly as ‘O’ as the channel

output.

(ii) Path at bottom of graph :

(iii) Diogonal path from 0 to 1 : Represents an input bit O appearing

incorrectly as 1 at the channel output

(due to noise)

(iv) Diagonal path from 1 to 0 : Similar comments

Errors occur in a random fashion and the occurrence of errors can be statistically modelled by assigning probabilities to the paths shown in figure (2).

• A memory less channel:

If the occurrence of an error during a bit interval does not affect the behaviour of the system during other bit intervals.

Probability of an error can be evaluated as

p(error) = Pe = P (X ≠ Y) = P (X = 0, Y = 1) + P (X = 1, Y = 0)

Pe = P (X = 0) . P (Y = 1 / X = 0) + P (X = 1), P (Y = 0 / X= 1)

Can also be written as,

Pe = top p01 + t

1p p10 ------ (1)

We also have from the model

O P00 O

1 p11 1

Transmitted digit X

Received digit X

pij = p(Y = j / X=i) t

op = p(X = o);

t

1p P(X = 1)

r

op = p(Y = o);

r

1p P(Y = 1)

poo + po1 = 1 ; p11 + p10 = 1

P10

P01

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11t101

to

r1

10t100

to

ro

ppppp

and,p.pppp

+=

+= ----- (2)

• Binary symmetric channel (BSC)

If, p00 = p11 = p (say), then the channel is called a BSC.

• Parameters needed to characterize a BSC

• Model of an M-ary DMC.

This can be analysed on the same lines presented above for a binary channel.

∑=

=M

1iij

ti

rj ppp ----- (3)

• The p(error) for the M-ary channel

Generalising equation (1) above, we have

== ∑∑≠==

M

ij1j

ij

M

1i

tie ppP)error(P ----- (4)

• In a DMC how many statistical processes are involved and which are they?

Two, (i) Input to the channel and

(ii) Noise

1

2

j

M

1

2

i

M

INPUT X OUTPUT Y

t

ip = p(X = i)

rjp = p(Y = j)

ijp = p(Y = j / X = i)

Fig. – (3)

p11

p12

pij

piM

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• Definition of the different entropies for the DMC.

i) Entropy of INPUT X: H(X).

( ) ( )∑=

−=M

1i

ti

ti plogpXH bits / symbol ----- (5)

ii) Entropy of OUTPUT Y: H(Y)

( ) ( )∑=

−=M

1i

ri

ri plogpYH bits / symbol ----- (6)

iii) Conditional entropy: H(X/Y)

( ) ( )∑∑==

====−=M

1j

M

1i

)jY/iX(plog)jY,iX(PY/XH bits/symbol - (7)

iv) Joint entropy: H(X,Y)

( ) ( )∑∑==

====−=M

1i

M

1i

)jY,iX(plog)jY,iX(PY,XH bits/symbol - (8)

v) Conditional entropy: H(Y/X)

( )∑∑==

====−=M

1i

M

1i

)iX/jY(plog)jY,iX(P(Y/X)H bits/symbol - (9)

Representation of the conditional entropy

• H(X/Y) represents how uncertain we are of the channel input ‘x’, on the average, when we know

the channel output ‘Y’.

Similar comments apply to H(Y/X)

vi) H(X/Y) H(Y) H(Y/X) H(X) Y)H(X,Entropy Joint +=+= - (10)

ENTROPIES PERTAINING TO DMC

• To prove the relation for H(X Y)

By definition, we have,

H(XY) = ∑∑−M

j

M

i

)j,i(plog)j,i(p

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i � associated with variable X, white j � with variable Y.

H(XY) = [ ]∑∑−ji

)i/j(p)i(plog)i/j(p)i(p

=

+− ∑∑∑∑ )i(plog)i/j(p)i(p)i(plog)i/j(p)i(p

ji

Say, ‘i’ is held constant in the first summation of the first term on RHS, then we can write

H(XY) as

H(XY) =

+− ∑∑∑ )i/j(plog)ij(p)i(plog1)i(p

)X/Y(H)X(H)XY(H +=∴

Hence the proof.

1. For the discrete channel model shown, find, the probability of error.

P(error) = Pe = P(X ≠ Y) = P(X = 0, Y = 1) + P (X = 1, Y = 0)

= P(X = 0) . P(Y = 1 / X = 0) + P(X = 1) . P(Y = 0 / X = 1)

Assuming that 0 & 1 are equally likely to occur

P(error) = 2

1 x (1 – p) +

2

1 (1 – p) =

2

1 -

2

p +

2

1 -

2

p

∴ P(error) = (1 – p)

2. A binary channel has the following noise characteristics:

X Y

Transmitted digit

Received digit

0 0

1 1

p

p

Since the channel is symmetric, p(1, 0) = p(0, 1) = (1 - p) Proby. Of error means, situation when X ≠ Y

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If the input symbols are transmitted with probabilities ¾ & ¼ respectively, find H(X), H(Y), H(XY), H(Y/X).

Solution:

Given = P(X = 0) = ¾ and P(Y = 1) ¼

∴ H(X) = ∑ =+=−i

22ii symbol/bits811278.04log4

1

3

4log

4

3plogp

Compute the probability of the output symbols.

Channel model is-

p(Y = Y1) = p(X = X1, Y = Y1) + p(X = X2, Y = Y1) ----- (1)

To evaluate this construct the p(XY) matrix using.

P(XY) = p(X) . p(Y/X) =

=

6

1

12

1

4

1

y

2

1

y

x

x

4

1.

3

2

4

1.

3

1

4

3.

3

1

4

3.

3

221

2

1

----- (2)

∴ P(Y = Y1) = 12

7

12

1

2

1 =+ -- Sum of first column of matrix (2)

Similarly P(Y2) = 12

5 � sum of 2nd column of P(XY)

Construct P(X/Y) matrix using

P(Y/X) Y

0 1

X 0 2/3 1/3

1 1/3 2/3

x1 y1

x2

y2

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P(XY) = p(Y) . p(X/Y) i.e., p(X/Y) = )Y(p

)XY(p

∴ p ( )

( ) onsoand7

6

14

12

12

72

1

Yp

YXp

Y

X

1

11

1

1 ====

∴ p(Y/X) =

5

2

7

15

3

7

6

-----(3)

= ?

H(Y) = ∑ =+=i i

i 979868.05

12log

12

5

7

12log

12

7

p

1logp bits/sym.

H(XY) = ∑∑ji )XY(p

1log)XY(p

= 6log6

112log

12

14log

4

1 2 log

2

1 +++

∴ H(XY) = 1.729573 bits/sym.

H(X/Y) = ∑∑ )Y/X(p

1log)XY(p

= 2

5log

6

17log

12

1

3

5log

4

1

6

7 log

2

1 +++ = 1.562

H(X/Y) = ∑∑ )X/Y(p

1log)XY(p

= 2

3log

6

13log

12

13log

4

1

2

3 log

2

1 +++

3. The joint probability matrix for a channel is given below. Compute H(X), H(Y), H(XY), H(X/Y) & H(Y/X)

P(XY) =

1.0005.005.0

1.02.000

01.01.00

05.02.0005.0

Solution:

Row sum of P(XY) gives the row matrix P(X)

∴ P(X) = [0.3, 0.2, 0.3, 0.2]

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Columns sum of P(XY) matrix gives the row matrix P(Y)

∴ P(Y) = [0.1, 0.15, 0.5, 0.25]

Get the conditional probability matrix P(Y/X)

P(Y/X) =

5

20

3

1

2

15

2

5

200

02

1

2

10

6

1

3

20

6

1

Get the condition probability matrix P(X/Y)

∴ P(X/Y) =

5

20

3

1

2

15

2

5

200

05

1

3

20

5

1

5

20

2

1

Now compute the various entropies required using their defining equations.

(i) H(X) = ( ) ( )

+

=∑ 2.0

1log2.02

3.0

1log3.02

Xp

1log.Xp

i

∴ H (X) = 1.9705 bits / symbol

(ii) ( ) ( )

25.0

1log25.0

5.0

1log5.0

15.0

1log15.0

1.0

1log1.0

Yp

1log.Yp H(Y)

j

++

+==∑

∴ H (Y) = 1.74273 bits / symbol

(iii) H(XY) = ∑∑ )XY(p

1log)XY(p

+

+

=2.0

1log2.02

1.0

1log1.04

05.0

1log05.04

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∴ H(XY) = 3.12192

(iv) H(X/Y) = ∑∑ )Y/X(p

1log)XY(p

Substituting the values, we get.

∴ H(X/Y) = 4.95 bits / symbol

(v) H(Y/X) = ∑∑ )X/Y(p

1log)XY(p

Substituting the values, we get.

∴ H(Y/X) = 1.4001 bits / symbol

4. Consider the channel represented by the statistical model shown. Write the channel matrix and compute H(Y/X).

For the channel write the conditional probability matrix P(Y/X).

P(Y/X) =

3

1

3

1

6

1

6

1

6

1

6

1

3

1

3

1

x

x

yyyy

2

1

4321

NOTE: 2nd row of P(Y/X) is 1st row written in reverse order. If this is the situation, then channel is called a symmetric one.

First row of P(Y/X) . P(X1) = 6

1x

2

1

6

1x

2

1

3

1x

2

1

3

1x

2

1 ++

+

Second row of P(Y/X) . P(X2) = 3

1x

2

1

2

1x

6

1

6

1x

2

1

6

1x

2

1 +++

INPUT OUTPUT

X1

Y1

Y2

Y3

Y4

1/3

1/6 1/3

1/6 1/6

1/3 1/6 1/3

X2

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Recall

P(XY) = p(X), p(Y/X)

∴ P(X1Y1) = p(X1) . p(Y1X1) = 1 . 3

1

P(X1Y2) = 3

1, p(X1, Y3) =

6

1 = (Y1X4) and so on.

P(X/Y) =

6

1

6

1

12

1

12

1

12

1

12

1

6

1

6

1

H(Y/X) = ∑∑ )X/Y(p

1log)XY(p

Substituting for various probabilities we get,

3log6

13log

6

16log

12

1

6log12

16log

12

16log

12

13log

6

13log

6

1 H(Y/X)

+++

++++=

= 4 x 6log12

1x43log

6

1 +

= 2 x 6log3

13log

3

1 + = ∴ ?

5. Given joint proby. matrix for a channel compute the various entropies for the input and output rv’s of the channel.

P(X . Y) =

2.002.006.00

06.001.004.004.0

002.002.00

01.001.001.01.0

02.002.0

Solution:

P(X) = row matrix: Sum of each row of P(XY) matrix.

∴ P(X) = [0.4, 0.13, 0.04, 0.15, 0.28]

P(Y) = column sum = [0.34, 0.13, 0.26, 0.27]

1. H(XY) = ∑∑ =)XY(p

1log)XY(p 3.1883 bits/sym.

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2. H(X) = ∑ =)X(p

1log)X(p 2.0219 bits/sym.

3. H(Y) = ∑ =)Y(p

1log)Y(p 1.9271 bits/sym.

Construct the p(X/Y) matrix using, p(XY) = p(Y) p(X/Y)

or P(X/Y) = )Y(p

)XY(p =

27.0

2.0

26.0

02.0

13.0

06.00

27.0

06.0

26.0

01.0

13.0

04.0

34.0

04.0

026.0

02.0

13.0

02.00

27.0

01.0

26.0

01.0

13.0

01.0

34.0

1.0

036.0

2.00

34.0

2.0

4. H(X/Y) = ∑∑ =− )Y/X(plog)XY(p 1.26118 bits/sym.

Problem:

Construct p(Y/X) matrix and hence compute H(Y/X).

Rate of Information Transmission over a Discrete Channel :

• For an M-ary DMC, which is accepting symbols at the rate of rs symbols per second, the average amount of information per symbol going into the channel is given by the entropy of the input random variable ‘X’.

i.e., H(X) = ∑=

−M

1i

ti2

ti plogp ----- (1)

Assumption is that the symbol in the sequence at the input to the channel occur in a statistically independent fashion.

• Average rate at which information is going into the channel is

Din = H(X), rs bits/sec ----- (2)

• Is it possible to reconstruct the input symbol sequence with certainty by operating on the received sequence?

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• Given two symbols 0 & 1 that are transmitted at a rate of 1000 symbols or bits per second.

With 2

1p&

2

1p t

1t0 ==

Din at the i/p to the channel = 1000 bits/sec. Assume that the channel is symmetric with the probability of errorless transmission p equal to 0.95.

Rate of transmission of information:

• Recall H(X/Y) is a measure of how uncertain we are of the input X given output Y.

• What do you mean by an ideal errorless channel?

• H(X/Y) may be used to represent the amount of information lost in the channel.

• Define the average rate of information transmitted over a channel (Dt).

Dt ∆ srlostninformatio

ofAmount

channeltheintogoing

ninformatioofAmount

Symbolically it is,

Dt = [ ] sr.)Y/X(H)H(H − bits/sec.

When the channel is very noisy so that output is statistically independent of the input, H(X/Y) = H(X) and hence all the information going into the channel is lost and no information is transmitted over the channel.

DISCRETE CHANNELS:

1. A binary symmetric channel is shown in figure. Find the rate of information transmission

over this channel when p = 0.9, 0.8 & 0.6. Assume that the symbol (or bit) rate is

1000/second.

Input X

Output Y

1 – p

1 – p

p

p

p(X = 0) = p(X = 1) = 2

1

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Example of a BSC

Solution:

H(X) = .sym/bit12log2

12log

2

122 =+

sec/bit1000)X(HrD sin =∴

By definition we have,

Dt = [H(X) – H(X/Y)]

Where, H(X/Y) = ( ) ( )[ ]∑∑−i j

Y/XplogXYp . rs

Where X & Y can take values.

X Y

0

0

1

1

0

1

0

1

∴ H(X/Y) = - P(X = 0, Y = 0) log P (X = 0 / Y = 0)

= - P(X = 0, Y = 1) log P (X = 0 / Y = 1)

= - P(X = 1, Y = 0) log P (X = 1 / Y = 0)

= - P(X = 1, Y = 1) log P (X = 1 / Y = 1)

The conditional probability p(X/Y) is to be calculated for all the possible values that X & Y can

take.

Say X = 0, Y = 0, then

P(X = 0 / Y = 0) = 0) p(Y

0) p(X0) X/0 Y(p

====

Where

p(Y = 0) = p(Y = 0 / X = 0) . p(X = 0) + p (X = 1) . p

==

1X

0Y

= p . 2

1

2

1 + (1 – p)

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∴ p(Y = 0) = 2

1

∴ p(X = 0 /Y = 0) = p

Similarly we can calculate

p(X = 1 / Y = 0) = 1 – p

p(X = 1 / Y = 1) = p

p(X = 0 / Y = 1) = 1 – p

∴ H (X / Y) = -

−−+

+−−+

)p1(log)p1(2

1plogp

2

1

)p1(log)p1(2

1plogp

2

1

2

22

= - [ ])p1(log)p1(plogp 22 −−+

∴ Dt rate of inforn. transmission over the channel is = [H(X) – H (X/Y)] . rs

with, p = 0.9, Dt = 531 bits/sec.

p = 0.8, Dt = 278 bits/sec.

p = 0.6, Dt = 29 bits/sec.

• What does the quantity (1 – p) represent?

• What do you understand from the above example?

2. A discrete channel has 4 inputs and 4 outputs. The input probabilities are P, Q, Q, and P.

The conditional probabilities between the output and input are.

Write the channel model.

Solution: The channel model can be deduced as shown below:

Given, P(X = 0) = P

P(X = 1) = Q

P(X = 2) = Q

P(y/x) Y

0 1 2 3

X

0 1 – – – 1 – p (1–p) – 2 – (1–p) (p) – 3 – – – 1

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P(X = 3) = P

Off course it is true that: P + Q + Q + P = 1

i.e., 2P + 2Q = 1

∴ Channel model is

• What is H(X) for this?

H(X) = - [2P log P + 2Q log Q]

• What is H(X/Y)?

H(X/Y) = - 2Q [p log p + q log q]

= 2 Q . α

1. A source delivers the binary digits 0 and 1 with equal probability into a noisy channel at a

rate of 1000 digits / second. Owing to noise on the channel the probability of receiving a

transmitted ‘0’ as a ‘1’ is 1/16, while the probability of transmitting a ‘1’ and receiving a ‘0’

is 1/32. Determine the rate at which information is received.

Solution:

Rate of reception of information is given by –

R = H1(X) - H1(X/Y) bits / sec -----(1)

Where, H(X) = ∑−i

.sym/bits)i(plog)i(p

H(X/Y) = ∑∑−ji

.sym/bits)j/i(plog)ij(p -----(2)

H(X) = .sym/bit12

1log

2

1

2

1log

2

1 =

+−

Input X

Output Y

1 – p = q

(1 – p) = q

p

p

1 0

1

1

2

3

0

1

2

3

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Channel model or flow graph is

Probability of transmitting a symbol (i) given that a symbol ‘0’ was received was received is denoted

as p(i/j).

• What do you mean by the probability p

==

0j

0i?

• How would you compute p(0/0)

Recall the probability of a joint event AB p(AB)

P(AB) = p(A) p(B/A) = p(B) p(A/B)

i.e., p(ij) = p(i) p(j/i) = p(j) p(i/j)

from which we have,

p(i/j) = )j(p

)i/j(p)i(p -----(3)

• What are the different combinations of i & j in the present case?

Say i = 0 and j = 0, then equation (3) is p(0/0) )0j(p

)0/0(p)0(p

=

• What do you mean by p(j = 0)? And how to compute this quantity?

Substituting, find p(0/0)

Thus, we have, p(0/0) = )0(p

)0/0(p)0/0(p

=

64

3116

15x

2

1

= 31

30 = 0.967

∴ p(0/0) = 0.967

• Similarly calculate and check the following.

33

22

1

0p;

33

31

1

1p ,

31

1

0

1p =

=

=

Input Output

1/32

1/16

15/16

31/32

0

1

0

1

Index ‘i' refers to the I/P of the channel and index ‘j’ referes to the output (Rx)

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• Calculate the entropy H(X/Y)

+

+

+

−=

1

1plog)11(p

0

1plog)10(p

1

0plog)01(p

0

0plog)00(p H(X/Y)

Substituting for the various probabilities we get,

+

+

+

−=

31

1log

64

1

33

31plog

64

31

33

2log

32

1

31

30log

32

15 H(X/Y)

Simplifying you get,

H(X/Y) = 0.27 bit/sym.

∴ [H(X) – H(X/Y)] . rs

= (1 – 0.27) x 1000

∴ R = 730 bits/sec.

2. A transmitter produces three symbols ABC which are related with joint probability shown.

p(i) i

p(j/i) j

A B C

9/27 A

i

A 0 5

4

5

1

16/27 B B 2

1

2

1 0

2/27 C C 2

1

5

2

10

1

Calculate H(XY)

Solution:

By definition we have

H(XY) = H(X) + H(Y/X) -----(1)

Where, H(X) = ∑−i

symbol/bits)i(plog)i(p -----(2)

and H(Y/X) = ∑∑−ji

symbol/bits)i/j(plog)ij(p -----(3)

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From equation (2) calculate H(X)

∴ H(X) = 1.257 bits/sym.

• To compute H(Y/X), first construct the p(ij) matrix using, p(ij) = p(i), p(j/i)

p(i, j) j

A B C

i

A 0 15

4

15

1

B 27

8

27

8 0

C 27

1

135

4

135

1

• ∴ From equation (3), calculate H(Y/X) and verify, it is

H(Y/X) = 0.934 bits / sym.

• Using equation (1) calculate H(XY)

∴ H(XY) = H(X) + H(Y/X)

= 1.25 + 0.934

2.5 Capacity of a Discrete Memory less Channel (DMC):

• Capacity of noisy DMC

Is Defined as –

The maximum possible rate of information transmission over the channel.

In equation form –

[ ]t)x(P

DMaxC = -----(1)

i.e., maximized over a set of input probabilities P(x) for the discrete

Definition of Dt?

Dt: Ave. rate of information transmission over the channel defined as

Dt [ ] sr)y/x(H)x(H −∆ bits / sec. -----(2)

∴ Eqn. (1) becomes

[ ]{ }s)x(P

r)y/x(H)x(HMaxC −= -----(3)

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• What type of channel is this? • Write the channel matrix

• Do you notice something special in this channel? • What is H(x) for this channel?

Say P(x=0) = P & P(x=1) = Q = (1 – P) H(x) = – P log P – Q log Q = – P log P – (1 – P) log (1 – P)

• What is H(y/x)? H(y/x) = – [p log p + q logq]

DISCRETE CHANNELS WITH MEMORY:

In such channels occurrence of error during a particular symbol interval does not influence the occurrence of errors during succeeding symbol intervals – No Inter-symbol Influence This will not be so in practical channels – Errors do not occur as independent events but tend to occur as bursts. Such channels are said to have Memory. Examples: – Telephone channels that are affected by switching transients and dropouts – Microwave radio links that are subjected to fading In these channels, impulse noise occasionally dominates the Gaussian noise and errors occur in infrequent long bursts. Because of the complex physical phenomena involved, detailed characterization of channels with memory is very difficult. GILBERT model is a model that has been moderately successful in characterizing error bursts in such channels. Here the channel is modeled as a discrete memoryless BSC, where the probability of error is a time varying parameter. The changes in probability of error are modeled by a Markoff process shown in the Fig 1 below.

P(Y/X) Y

0 ? 1

X 0 p q p

1 o q p

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The error generating mechanism in the channel occupies one of three states. Transition from one state to another is modeled by a discrete, stationary Mark off process. For example, when the channel is in State 2 bit error probability during a bit interval is 10-2 and the channel stays in this state during the succeeding bit interval with a probability of 0.998. However, the channel may go to state 1wherein the bit error probability is 0.5. Since the system stays in this state with probability of 0.99, errors tend to occur in bursts (or groups). State 3 represents a low bit error rate, and errors in this state are produced by Gaussian noise. Errors very rarely occur in bursts while the channel is in this state. Other details of the model are shown in Fig 1. The maximum rate at which data can be sent over the channel can be computed for each state of the channel using the BSC model of the channel corresponding to each of the three states. Other characteristic parameters of the channel such as the mean time between error bursts and mean duration of the error bursts can be calculated from the model.

2. LOGARITHMIC INEQUALITIES:

Fig 2 shows the graphs of two functions y1 = x - 1 and y2 = ln x .The first function is

a linear measure and the second function is your logarithmic measure. Observe that the log function always lies below the linear function , except at x = 1. Further the straight line is a tangent to the log function at x = 1.This is true only for the natural logarithms. For example, y2 = log2x is equal to y1 = x - 1 at two points. Viz. at x = 1 and at x = 2 .In between these two values y1 > y2 .You should keep this point in mind when using the inequalities that are obtained. From the graphs shown, it follows that, y1 ≤ y2; equality holds good if and only if x = 1.In other words:

…… (2.1) Multiplying equation (2.1) throughout by ‘-1’ and ln x ≤ (x-1), equality iffy x = 1

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noting that -ln x = ln (1/x), we obtain another inequality as below. ……..…… (2.2) This property of the logarithmic function will be used in establishing the extremal property of the Entropy function (i.e. Maxima or minima property). As an additional property, let {p1, p2, p3,…..pn } and {q1, q2, q3,…..qn } be any two sets of probabilities

such that pi ≥ 0 , qj ≥ 0 ; ∀ i,j and ∑∑∑∑∑∑∑∑========

====n

1jj

n

1ii qp . Then we have:

====

∑∑∑∑∑∑∑∑======== i

in

1ii2

i

i2

n

1ii p

qln.p.elog

pq

log.p

Now using Eq (2.1), it follows that:

n,...2,1i,1pq

.p.elogpq

log.pn

1i i

ii2

i

i2

n

1ii ====∀∀∀∀

−−−−≤≤≤≤

∑∑∑∑∑∑∑∑========

[[[[ ]]]] [[[[ ]]]],pq.elogn

1ii

n

1ii2 ∑∑∑∑∑∑∑∑

========−−−−≤≤≤≤

This, then implies

∑∑∑∑==== i

i2

n

1ii p

qlog.p ≤ 0

That is,

≤≤≤≤

∑∑∑∑∑∑∑∑======== i

2

n

1ii

i2

n

1ii q

1log.p

p1

log.p equality iffy pi = qi ∀∀∀∀ i=1, 2, 3...n .......... (2.3)

This inequality will be used later in arriving at a measure for code efficiency 3. PROPERTIES OF ENTROPY:

We shall now investigate the properties of entropy function 1. The entropy function is continuous in each and every independent variable ,pk in the

interval (0,1) This property follows since each pk is continuous in the interval (0, 1) and that the logarithm of a continuous function is continuous by itself.

2. The entropy function is a symmetrical function of its arguments; i.e. H (pk, 1- pk) = H (1- pk, pk) ∀ k =1, 2, 3...q.

That is to say that the value of the function remains same irrespective of the locations (positions) of the probabilities. In other words, as long as the probabilities of the set are same, it does not matter in which order they are arranged. Thus the sources S1, S2 and S3

with probabilities:

(((( )))),x1x1

ln −−−−≥≥≥≥

equality iffy x = 1

Page 254: Unit -I Amplitude Modulation - WordPress.com · 2016-09-19 · Angle modulation AM DSB-SC SSB VSB FM PM . Communication Systems Continuous-Wave Modulation 3 2.1 Introduction Figure

66

P1 = {p1, p2, p3, p4}, P2 = {p3, p2, p4, p1} and P3 = {p4, p1, p3, p2} with 1p4

1kk ====∑∑∑∑

==== all have

same entropy, i.e. H (S1) = H (S2) = H (S3)

3. Extremal property: Consider a zero memory information source with a q-symbol alphabet S ={s1 , s2 , s3 ,….. ,sq } with associated probabilities P = {p1 , p2 , p3 ,….. ,pq }.

Then we have for the entropy of the source (as you have studied earlier):

∑∑∑∑========

q

1k kk p

1log.p)S(H

Consider log q –H(S). We have:

log q –H(S) = log q - ∑∑∑∑====

q

1k kk p

1log.p

= ∑∑∑∑ ∑∑∑∑−−−−==== ====

q

1k

q

1k kkk p

1log.pqlog.p

= ∑∑∑∑ ∑∑∑∑−−−−==== ====

q

1k

q

1k kkk p

1ln.pqln.pelog

= )p1

lnqln(p.elogk

q

1kk∑∑∑∑ −−−−

====

= )pqln(p.elogq

1kkk∑∑∑∑

====

Invoking the inequality in Eq (2.2), we have:

log q –H(S) ≥ )pq1

1(p.elogq

1k kk∑∑∑∑ −−−−

==== Equality iffy q p k = 1, ∀∀∀∀ k =1, 2, 3…q.

−−−−∑∑∑∑ ∑∑∑∑==== ====

q

1k

q

1kk q

1pelog Equality iffy p k = 1/q, ∀ k =1, 2, 3…q.

Since 1q1

pq

1k

q

1kk ====∑∑∑∑ ∑∑∑∑====

==== ====, it follows that log q –H(S) ≥ 0

Or in other words H(S) ≤ log q …………………. (2.4) The equality holds good iffy p k = 1/q,∀∀∀∀ k =1, 2, 3…q. Thus “for a zero memory information source, with a q-symbol alphabet, the Entropy becomes a maximum if and only if all the source symbols are equally probable” .From Eq (2.4) it follows that: H(S) max = log q … iffy p k = 1/q,∀ k =1, 2, 3 … q ………………….. (2.5) Particular case- Zero memory binary sources: