Lec02 Final

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    Analog Digital Communication :

    Asad Abbas

    Assistant Professor Telecom Department

    Air University, E-9, Islamabad

    Lec2_chpater01

    10/29/2009 Lecture 1 2

    Scope of the course ...

    General structure of a communication systems

    FormatterSource

    encoder

    Channel

    encoderModulator

    FormatterSource

    decoder

    Channel

    decoderDemodulator

    Transmitter

    Receiver

    SOURCE

    Info.Transmitter

    Transmitted

    signal

    Received

    signalReceiver

    Received

    info.

    Noise

    ChannelSource User

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    10/29/2009 Lecture 1 3

    Random Variable

    The random variable, X(A) represents a

    functional relationship between random eventand a real number.

    It is designated by X and functional

    dependence upon A is considered as implicit.

    Discrete Random Variable

    If in any finite interval X assumes only finite number of

    distinct values, it is discrete random variable, for example

    tossing of dice, tossing of a coin

    Continuous Random Variable

    If X assumes any value within interval it is continuous, for

    example noise, temperature etc

    10/29/2009 Lecture 1 4

    Distribution

    Cumulative Distribution (CD):

    Fx (x) = P ( X

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    10/29/2009 Lecture 1 5

    Distribution (contd..)

    Probability Density Distribution (PDF)

    px(x) = d/dx (Fx (x))It is rate of change of CD with respect to the random

    variable

    Properties

    ( ) ( )x

    X XF x p x dx=

    10/29/2009 Lecture 1 6

    Ensemble Averages of Random Variable

    Mean =

    Nth moment of PD of a random variable=

    The second central moment is given by

    Second moment of PD of a random variable=

    Mean of a Discreet RV = E{ X } =1

    ( )n

    i

    i

    X xPx x

    =

    =

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    10/29/2009 Lecture 1 9

    Random Process..contd

    The random processes at each a point in time

    is random variable. X(tk) is random variable by observing random

    process at time at t=k.

    The values that X(tk) can take are

    X1(tK)XN(tK)

    The random processes have all the properties

    of random variables, such as mean,

    correlation, variances, etc

    10/29/2009 Lecture 1 10

    Statistical Properties of Random process

    Mean

    Autocorrelation of Random Process X(t)

    It measures of the degree to which two time samples

    of the same random process are related

    It is function of two variables t1= t and t2= t+

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    10/29/2009 Lecture 1 11

    Random process Types

    Stationary Process or Strictly Stationery Process:

    If all of the statistical properties random process donot change with time it is called strictly stationery,that is:

    Random process do not depends on time i.e

    X(A,t) = X(A)

    Its Probability Density Function do not change withtime, i.e

    _

    Mean= E{X(t)} = mx(t)= constant

    Autocorrelation= Rx (t1, t2)= constant

    Nth moment = E{X(t)n} = constant.

    1 2 1 2, ,...... , ,......

    t t t t tk X X tk X X Xp p p p p p

    + + +=

    10/29/2009 Lecture 1 12

    Random Process Types

    Wide ( or Weak) sense stationary (WSS):

    In WSS random process only two statistics (

    mean and autocorrelation) do not change

    with time

    Mean of X(t)= E{X(t)} = mx(t) = Constant

    Rx (t1, t2) = Rx (t1+, t2+) = Rx (t2 t1,0)= Rx ()

    It means Autocorrelation only depends on difference

    between t1 and t2. Thus all pairs of X(t) at times

    separated by t2-t1 have same correlation value

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    10/29/2009 Lecture 1 13

    Random process Types (Contd..)

    Ergodic process:A random process is ergodic if its

    ensemble ( statistical) and time averages are same,that is:

    10/29/2009 Lecture 1 14

    Random Process

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    10/29/2009 Lecture 1 15

    Spectral density

    Energy signals:

    Energy spectral density (ESD):

    Power signals:

    Power spectral density (PSD):

    Random process: Power spectral density (PSD):

    10/29/2009 Lecture 1 16

    Autocorrelation

    Autocorrelation of an energy signal

    Autocorrelation of a power signal

    For a periodic signal:

    Autocorrelation of a random signal

    For a WSS process:

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    10/29/2009 Lecture 1 17

    Properties of an autocorrelation function

    For real-valued (and WSS in case of random

    signals):1. Autocorrelation and spectral density form a Fourier

    transform pair.

    2. Autocorrelation is symmetric around zero.

    3. Its maximum value occurs at the origin.

    4. Its value at the origin is equal to the average power or

    energy.

    10/29/2009 Lecture 1 18

    Power SpectralDensity and

    Autocorrelation of a

    Low Rate Signal

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    10/29/2009 Lecture 1 19

    Power Spectral

    Density and

    Autocorrelation of a

    High rate Signal

    10/29/2009 Lecture 1 20

    Noise

    It is undesired signal interfering with the

    desired signal.

    External Sources

    Atmospheric Noise ( Max Freq range: 30 Mhz)

    lightening

    Solar Noise

    Cosmic Noise

    ( Source is sun and distant stars. Frequency range is 8Mhz-

    1.43 GHz)

    Industrial Noise (Freq Range = 1-600 MHz)

    Ignition, motors, leakage from high voltage line, Fluorescent

    tube

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    10/29/2009 Lecture 1 23

    White Noise

    The Power Spectral Density ( Gn(f) ) of thermal

    noise is same from DC to about 1012 Hz. ThusGn(f) is flat for all frequencies of interest

    [w/Hz]

    Power spectral

    density

    Autocorrelation

    function

    The autocorrelation of White noise is given by inverse Fourier Transform

    of Gn(f)

    10/29/2009 Lecture 1 24

    Signal transmission through linearsystems

    Frequency Transfer Function

    Deterministic signals:

    Random signals:

    Input Output

    Linear system

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    10/29/2009 Lecture 1 25

    Signal transmission - contd

    Ideal distortion less transmission:

    All the frequency components of a signal at input of a linearsystem are amplified (or attenuated ) and delayed by the

    system equally.

    = Group Delay

    10/29/2009 Lecture 1 26

    Frequency and Impulse Responses ofIdeal Filter

    Ideal Lowpass filters: BW = fu - 0 = fu

    Low-pass

    Non-causal!

    fu-fu 0

    1

    2 [2 ( )]u u of sinc f t t=

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    10/29/2009 Lecture 1 27

    Frequency and Impulse responses of

    Ideal Filter

    Band-pass

    fufl-fl-fu

    BW = fu-fl

    High-pass

    Ideal Bandpass filters:

    Filter Bands Pass band

    Transition Band

    Stop Band

    10/29/2009 Lecture 1 28

    Frequency response of a Realizable Filter

    Realizable filters: RC filters

    3 0

    2

    1

    2

    1( )

    1 ( )u

    cut off dB u

    f

    f

    f f f fRC

    H f

    = = = =

    =+

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    10/29/2009 Lecture 1 29

    Frequency Response of Realizable Filter

    R1 = R2 =1 Ohm

    At cut- off frequency = ( ) 3

    ( ) .707

    dBH f dB

    H f

    =

    =

    10/29/2009 Lecture 1 30

    Bandwidth of a Passband signal

    Different definition of bandwidth:

    a) Half-power bandwidth

    b) Noise equivalent bandwidth

    c) Null-to-null bandwidth

    d) Fractional power containment bandwidth

    e) Bounded power spectral density

    f) Absolute bandwidth

    (a)

    (b)

    (c)

    (d)

    (e)50dB

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    10/29/2009 Lecture 1 31

    Bandwidth of signal(contd)

    10/29/2009 Lecture 1 32

    END

    Thank You