ece eee f311 pm and fm sept 3 -11 2014

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    Topic # 5: Phase & Frequency Modulation

    T1. B.P. Lathi, Modern Digital and Analog Communication Systems, 3rd

    Edition, Oxford University Press, 1998: OR 4thEdition 2010 Chapter 5

    T2. Simon Haykin & Michael Moher: Communication Systems; John Wiely, 4th

    Edition OR 5thEdition, 2010, 5/e. : Chapter 4

    Sept 311, 2014

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Introduction

    Amplitude modulation Process of varying a carrier signals amplitude according to message

    signal

    Phase Modulation Can we vary of the phase of a carrier according to message signal ?

    Frequency Modulation

    Can we vary of the frequency of a carrier according to message signal ?

    Is it for fancy or any benefits over AM exist ? Noise immunity over AM at the cost of increased BW

    Constancy of the transmitted signal envelop.2

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Instantaneous Frequency

    3

    ()

    = w

    c

    Given instantaneous frequency, the

    angle function is then

    And the instantaneous Frequency is

    (t) is the generalized angle

    and is a function of t.

    The generalized angle for a conventionalSinusoid A cos( wct + o) is

    Instantaneous Frequency

    (t) = wct + o

    o

    Dt

    ()

    = wi(t)

    ois the accumulated phase upto t = 0.

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Phase Modulation

    4

    Instantaneous frequency varies linearly with derivative of the message signal

    The instantaneous frequency is

    PM Signal

    Phase varies linearly with message signal

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Example.

    5

    In an angle modulating system, for themodulating signal m(t) shown in figure,

    the constant kp = 10p. Carrier frequency

    fc= 100 MHz. Find the frequency

    excursion when PM is used. Sketch PM

    wave

    PM Case:

    Slope of m(t) = 2 / 10-4= (+/-)20,000

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Frequency Modulation

    FM Signal

    The phase varies with respect to the integral of the message signal.

    Instantaneous Frequency varies linearly with message signal

    The Phase is

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Example.

    7

    In an angle modulating system, for the

    modulating signal m(t) shown in figure,

    the constant kf = 2pX 105and Carrier

    frequency fc= 100 MHz. Find the

    frequency excursion when FM is used.

    Sketch FM wave The instantaneous frequency increases

    linearly from 99.9 to 100.1 MHz over ahalf cycle and decreases from 100.1 to

    99.9 MHz, over the rest of the half cycle

    of m(t).

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    Characteristics of PM & FM signals

    8

    1. Constancy of Transmitter Power

    The amplitude of the PM & FM

    waves is constant, irrespective of

    the deviation factors km& kf

    Hence, the transmitted power is

    constant.

    2. Non linearity of the modulationprocess

    If m(t) = m1(t) + m2(t);

    s1(t)= ( + pm1(t))

    s2(t)= ( + pm2(t))

    s(t)= ( + p(m1(t) + m2(t)))

    Clearly s(t) s1(t) + s2(t)

    For Phase Modulation

    Same applies to FM Also.

    Compare this with DSB-SC

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    Characteristics of PM & FM signals

    3. Immunity of angle modulation tononlinearities of the system.

    9

    Even with Higher order nonlinearities.

    Check for DSB-SC Case

    for non linearity of type

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    Bandwidth of Frequency Modulated Waves

    10

    For the FM Signal

    Let

    That is, the FM signal is like several

    DSB-SC signals with modulating

    signals a(t), a2(t), a3(t) an(t).

    Hence, the spectrum consists of un

    modulated carrier plus spectra of

    {an(t) , n= 1,2,3}, centered at wc.

    Expanding in power series

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    Bandwidth of Frequency Modulated Waves

    11

    If M(w) is band limited to B Hz, A(w)

    is also band limited to B Hz

    Spectrum of a2(t) is A(w)*A(w) and is

    band limited to 2B. Similarly, an(t) will

    be band limited to nB.

    Clearly, the theoretical bandwidth of

    Frequency Modulated signal is infinite

    Since, from FT properties,

    However, for practical signals withbounded | a(t)|, |kf a(t)| will remain finite.

    For large n 0

    Hence, many of the higher order

    terms of FM(t)

    Based on Bandwidth we have

    1. Narrowband FM and

    2. Wideband FM

    vanish and power remains in finitebandwidth. BW is finite for practical

    Signals

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    Narrowband Frequency Modulation

    12

    This has similarities toAM signal with

    Carrier.

    If |kfa(t) |

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    Narrowband Phase Modulation

    13

    If |kpm(t) |

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    Wideband Frequency Modulation

    14

    If |kfa(t) |

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    BW - Wideband Angle Modulation

    15

    Each cell has a constant amplitude m(tk) and duration 1/2B

    The FM Spectrum of one burst is then

    The FM BW

    The FM Spectrum of () is then sum

    of the spectra of short burst of sinusoids

    of duration (1/2B) and freq.

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    Example.

    17

    Step 1: Find the essential

    bandwidth of the given waveform

    Consider only upto third harmonic.

    Estimate BFMfor the

    modulating signal m(t) seefigure. Use kf = 2pX 10

    5.

    In this case the amplitude of harmonics decay rapidly.

    Third harmonic is 11% and 5this only 4% of the

    fundamental..

    B = 3 X (104/ 2 ) = 15 KHz.

    Step 2: Find the frequency deviation, based on kfand peak amplitude of the modulating waveform

    The bandwidth of the FM signal is then

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    Example.

    18

    Estimate BPMfor the modulating

    signal m(t) see figure. Use kp = 5p.

    What if amplitude of m(t) is doubled ?

    Doubling the amplitude of m(t) changes its peak

    value and not the BW. Hence for FM signal

    The bandwidth of the FM signal is then

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    Single Tone Frequency Modulation

    20

    Bessel Function of the first kind and nth order.

    Jn(b)

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    Single Tone Frequency Modulation

    21

    n = 0 : Themodulated

    signal has a

    carrier

    component.

    n 0 : It also has

    infinite number of

    sidebands

    The strength of nthsideband at w= wc+ nwm is Jn(b)

    Carsons formula

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    Demodulation of FM Signals.

    23

    The instantaneous frequency

    of the FM signal is

    Can a simple network with

    transfer function H() = j

    produce an output proportionalto instantaneous frequency?

    A circuit with transfer function

    as H(w) = jw, is a

    differentiator in time domain.

    wc+ kf m(t) > 0 for all t

    Dw= kf mp< wc,

    What if A is not constant ? Use band pass Limiting

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    Practical FM Demodulation Circuits

    25

    A tuned circuit (tuned to wc) , followed by

    an envelope detector can then be used.

    Frequency response of a tuned circuit is

    almost linear around the tuned frequency.

    Hence, it acts like a slope detector

    Linearity zone is increased by a

    balanced discriminator.

    Zero Crossing Detectors: Rate of zero

    crossings is the measure of instantaneous

    frequency.

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Interference & Angle Modulated systems

    27

    I cos (wc

    +w

    )t

    Assume an unmodulated Carrier at

    frequency wc is being transmitted.

    the received signal is

    If the demodulator is a Phase Detector, the output i

    Its like a single tone with

    amplitude, scaled by A, the

    carrier amplitude.

    If the demodulator is an FM detector, It will produc

    output from the Instantaneous Frequency:

    the output is

    Its again like a single tone with amplitude, scaled

    by A, the carrier amplitude and the frequency of

    the interferer

    In both cases, for A >> I, effect of

    interference is negligible.

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Interference due to Channel Noise

    29

    The channel noise acts as an interference

    White noise has a constant power spectral

    density: Implies Interference amplitude ,I,

    is constant for all w

    Voice signals have low PSD higher

    frequencies.

    Effect of Noise interference is high for

    higher frequencies,.

    Noise Amplitude in Phase Demodulated

    output = (I/ 2 A) and is independent of

    the interferer frequency

    The Phase detector Output is

    The FM Detector Output is

    Noise Amplitude in Frequency

    Demodulated output = (Iw

    /2 A)

    SNR of FM output suffers !!

    Consequences ?

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Remedy: Pre Emphasis & De Emphasis

    30

    Pre Emphasis: : Amplify the higher

    frequencies of m(t) before modulation

    De Emphasis:After demodulation, apply

    an inverse operation to the pre emphasis.

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    SNR Performance of Angle Modulated Systems

    Phase Modulation ( Small noise Case)Frequency Modulation ( Small noise Case)

    31

    is Baseband SNR

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    ELECTRICAL ELECTRONICS COMMUNICATION INSTRUMENTATION

    Problem # 2

    34

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    Problem # 3

    35

    Composite N = (final deviation / initial deviation)

    = 75000/10 = 7500 : N = N1 * N2

    For carrier : (L1 - 100Khz * N1 ) * N2 = 98.1 MHz. :

    The local Oscillator frequency L1 is constrained

    by 10MHz L1 11 MHz

    Case1:If N1 = 100 then N2 = 75,

    ( L110Mhz) * 75 = 98.1 MHz. :

    L1= 11.308 MHz.

    Does not work !!

    X N1 BPF X N2

    L1

    Case2: If N1 = 125 then N2 = 60,

    (12.5 MHz - L1 ) * 60 = 98.1 MHz. :

    L1= 10.865 MHz.May be this will work

    Case3: If N1 = 75 & N2 = 100,

    ( L1 - 7.5 MHz) * 100 = 98.1 MHz. :

    L1= 8.48 Mhz MHz.

    Does not work !!

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    Problem # 3

    X N1 BPF X N2L1