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    7 Communication Systems

    . . . transmitting messages, and possibly information . . .

    Transformationof source (message) signalx(t)into transmit signal

    y(t)matchedto transmission channel (frequency range, propagation

    and attenuation characteristics etc.)

    Mechanisms

    Modulation process of embedding information-bearing signal

    x(t)into y(t)

    Demodulation process of extracting information-bearing sig-

    nal

    Multiplexing combination of independent source signals into

    a composite signal suitable for transmission over a common

    channel

    Distinguish

    Analog vs. digital message signals

    analog time continuous + continuum of values digital time-discrete+ quantized values

    Analog vs. digital transmission

    Transmit signal varies continuously with message signal

    Finiteset of transmit signals to represent information This chapter

    Analog transmission of analog message signals

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    Outline

    7.1 Amplitude Modulation

    7.2 Frequency Modulation7.3 Analog-Pulse Amplitude Modulation

    7.4 Multiplexing

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    7.1 Amplitude Modulation

    Amplitude modulation (AM):Amplitudeofsinusoidal carrier signal

    c(t)is varied in proportion to a message signal x(t)

    AM is oldest and most simple technique for wireless transmission

    and multiplexing.

    Used for longwave, mediumwave, and shortwave radio and broad-

    casting, for analog television, for frequency multiplexing for analog

    telephone transmission, etc.

    7.1.1 Modulation

    Distinguish

    Double-sideband AM

    AM with/suppressed carrier

    Quadrature AM

    Single-sideband AM

    Vestigial-sideband AM

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    Double-sideband AM suppressed carrier

    Generation of AM wave

    y(t) =x(t)c(t) =x(t)

    2crmscos(ct + c)with carrier signal

    c(t) =

    2crmscos(ct + c)

    Notation

    x(t): message signal, modulating signal

    y(t): modulated signal c(t): carrier signal, carrier wave crms: root mean square value of sinusoidal carrier c: carrier frequency c: carrier phase

    Illustration 2crmscos(ct + c)

    x(t) y(t)

    y(t)x(t)

    t t

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    Frequency domain

    Spectrum of carrier waveC(j) =

    2crms (

    c)ejc + (+ c)e

    jc Multiplication property of Fourier transformY(j) =

    crms2

    X(j( c))ejc +X(j(+ c))ejc

    Replications of original spectrum centered aroundc

    double representation of modulation signal

    Bandwidthof message signal M bandwidth of modulatedsignal2

    M x(t)recoverable fromy(t)only ifc> M

    0

    0

    2crms

    2crms

    cc

    c c c+ M

    X(j)

    C(j)

    Y(j)

    1

    c M

    sidebandsidebandUpper

    sidebandsideband

    UpperLower Lower

    MM

    crms2

    0

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    Double-sideband AM with carrier

    Add carrier wave to transmit signal

    Simple demodulation possible

    Less power efficient, since carrier does not contain informa-tion

    Modulated signal

    y(t) = (A + x(t))

    2crmscos(ct + c)

    with

    DC component A Modulation indexm=

    max{|x(t)|}A

    Illustration

    Phase reversals

    m >1

    m= 1

    m

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    Efficiency factor

    = average power of message signal

    average total power

    = m2S21 + m2S2

    with degree of saturation

    S=

    average power of message signal

    max{|x(t)|} Frequency domain

    Superposition of message signal part and carrier waveY(j) =

    crms2

    X(j( c))ejc + X(j(+ c))ejc

    +

    2Acrms

    ( c)ejc + (+ c)ejc

    0

    X(j)

    1

    0c c

    Y(j)

    2Acrms

    2Acrms

    Uppersidebandsideband sideband

    Lower Lower Uppersideband

    crms2

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    Quadrature AM

    Feature

    2

    doubled-sideband AM using orthogonal carrier waves

    cos(ct)and sin(ct)

    Twoindependentmessage signals occupy same transmis-sion bandwidth (multiplexing)

    Bandwidth-conservation scheme

    Time-domain description (c= 0)

    y(t) =

    2crms(x1(t)cos(ct) x2(t)sin(ct))

    Block diagram

    2crmssin(ct)

    2crmscos(ct)

    y(t)

    x2(t)

    x1(t)

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    Frequency domain

    Spectrum of modulated signalY(j) =

    crms

    2 X1(j( c)) + X1(j(+c))+j

    X2(j( c))X2(j(+ c))

    Spectrum ofY(j) not symmetric about c no doublerepresentation

    Bandwidthof modulated signal2Mequals sum of the band-

    widths of the modulation signals nobandwidth expansion Illustration for real-valued spectra X1(j)andX2(j)

    Im{Y(j)}

    c

    c

    Re{Y(j)}

    X2(j)

    X1(j)

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    Single-sideband AM

    Observation from double-sideband AM

    Redundant representation of message signal in upper and

    lower sideband

    Twice the signal bandwidth M is required

    Therefore

    No information lost if one sideband is suppressed!single-sideband AM

    Frequency-domain description

    2crms

    0

    X(j)

    1

    0c c

    Y(j)

    Upper sideband

    Lower sideband

    0c c

    Y(j)

    2crms

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    Spectrum (c= 0)

    Upper sidebandY(j) =

    2crms1

    2

    (sign(

    c) + 1) X(j(

    c))

    12

    (sign(+ c) 1) X(j(+ c))

    Lower sidebandY(j) =

    2crms

    12

    (sign(+ c) + 1) X(j(+ c))

    1

    2

    (sign(

    c)

    1) X(j(

    c))

    Remark:

    We note that from the convolution property of the Fourier transform

    andF{1/t} = jsign()we have the Fourier pair1

    x(t) 1

    tF jX(j)sign().

    The left-hand side operation is called Hilbert transform, and is de-fined as

    H{x(t)} = 1

    x(t) 1t

    = 1

    x()

    t d

    and thus

    H{x(t)} = F1{jX(j)sign()}

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    Single-sideband signal

    Upper sidebandy(t) =

    F1

    {Y(j)

    }= 2crms

    12

    (x(t) +jH{x(t)}) e+jct

    +1

    2(x(t)jH{x(t)}) ejct

    y(t) =

    2crms(x(t)cos(ct)H{x(t)}sin(ct))

    Lower sidebandy(t) =

    2crms(x(t)cos(ct) + H{x(t)}sin(ct))

    Block diagram

    x(t)

    2crmssin(ct)

    2crmscos(ct)y(t)

    H{}

    Observe

    Single-sideband AM is QAM withx2(t) = H{x1(t)}

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    Illustration for real-valued spectrumX(j)

    Im

    F{cos(ct)}

    F{sin(ct)}

    Re

    +

    Y(j)

    Im

    Re

    Y(j)

    Im

    Re

    =

    Im

    Re

    ++

    Im

    =

    Re

    Im Im

    ReRe

    Im

    Re

    X(j)

    F{H{x(t)}} = jsign()X(j)

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    Implementation of exact Hilbert-transform filter impossible

    For DC-free message signals soft-Hilbert filter possible

    Method by Weaver

    0

    X(j)

    1

    uo ou

    y(t)

    2crmscos(2t)

    2crmssin(2t)

    2cos(1t)

    2sin(1t)x(t)

    Lowpass

    Lowpass

    1

    1

    1= o+u

    2

    ou2

    1

    Lowpass

    1= o+ u2

    2=c 1

    + : upper sideband

    : lower sideband

    Lowpass filter with finite edge steepnessLampe, Schober: Signals and Communications

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    Vestigial-sideband AM

    Single-sideband modulation not applicable when message signal

    contains significant low-frequency components, e.g., for televi-

    sion signals

    Compromise between double- and single-sideband AM

    Vestigial-sideband AM One sideband is passed almost completely Onlyvestigeof other sideband is retained

    Sideband-shaping filtersymmetric about c

    Illustration

    c

    Y(j)

    c+ Mc M

    X(j)

    MM

    cc

    Bandwidth-expansion factor (roll-off factor) [0, 1]

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    7.1.2 Demodulation

    Assumption: No overlap (c> M), transmitted signaly(t)is also

    received signal (no noise, distortion etc.)

    Distinguish

    Synchronous demodulation

    Asynchronous demodulation

    Synchronous Demodulation

    Demodulation of high-frequency signal into low-frequency signal

    with locally generated carrier wave

    c(t) =

    2

    crmscos(ct +

    c)

    Carrier frequency offset: c= c c Carrier phase offset: c=c c

    Subsequent lowpass filtering with cutoff frequency co

    Transmitter-receiver structure for general QAM

    w2(t)

    w1(t)

    y(t)

    2crmssin(ct + c)

    2crmscos(ct + c)

    x2(t)

    x1(t)

    v2(t)

    v1(t)co

    Lowpass

    co

    Lowpass

    2crms sin(ct + c)

    2

    crmscos(ct +

    c)

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    Signals after multiplication with carrier

    w1(t) = 2x1(t)cos(ct + c)cos(ct +

    c)

    2x2(t)sin(ct + c)cos(

    ct +

    c)

    = x1(t) [cos(ct + c) +cos((c+ c)t + c+c)]+x2(t) [sin(ct + c) sin((c+c)t + c+ c)]

    w2(t) = 2x2(t)sin(ct + c)sin(ct +

    c)

    2x1(t)cos(ct + c)sin(ct + c)= x2(t) [cos(ct + c) cos((c+ c)t +c+ c)]x1(t) [sin(ct + c) +sin((c+c)t + c+ c)]

    Signals after lowpass filtering with

    M< oc 2c M

    v1(t) = x1(t)cos(ct + c) + x2(t)sin(ct + c)

    v2(t) = x2(t)cos(ct + c) x1(t)sin(ct + c)

    Convenient combination to complex demodulated signal

    v1(t) +jv2(t) = x1(t) [cos(ct + c) jsin(ct + c)]+jx2(t) [cos(ct + c) jsin(ct + c)]

    v1(t) +jv2(t) = (x1(t) +jx2(t))ej(ct+c)

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    Double-sideband AM:x1(t) =x(t), x2(t) 0 Only real part used

    v(t) =v1(t) =x(t)cos(ct + c)

    Forv(t) = x(t)c= 0andc=k , k ZZ

    Synchronous carriers required!

    In case of AM with carrier: highpass to suppress carrier

    QAM

    v1(t) = x1(t)cos(ct + c) + x2(t)sin(ct + c)

    v2(t) = x2(t)cos(ct + c) x1(t)sin(ct + c) c= 0 andc =k , k ZZ: Coupling of signals

    c= 0 andc=k , k ZZ: Separation of signals Single-sided AM: x1(t) =x(t), x2(t) = H{x(t)} Only real part used

    v(t) = v1(t) =Re

    (x(t)jH{x(t)})ej(ct+c)

    = x(t)cos(ct + c)

    H{x(t)

    }sin(ct + c)

    c= 0, phase offset:v(t) =x(t)cos(c)H{x(t)}sin(c)

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    Frequency offset

    Lowpass|W(j)|

    c> c

    Upper sideband |Y(j)|

    cc

    Lowpass|W(j)

    |

    c< c

    Lower sideband

    |W(j)|Lowpass

    c> c

    |Y(j)|

    cc

    Lowpass|W(j)

    |

    c< c

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    Asynchronous Demodulation

    No demodulation with carrier wave no need for synchroniza-tion

    Evaluation ofenvelopeof received signal envelope detector Only applicable for Double-sideband AMwithcarrier andm 1

    y(t)

    t

    2crms(A + x(t))

    How to get rid of carrier wave?

    For non-overlapping sidebands

    H{y(t)} = H{(A +x(t)) 2crmscos(ct + c)}= (A + x(t)) 2crmssin(ct + c)

    cos2(ct +c) +sin2(ct + c) = 1

    env{y(t)} = 12y2(t) + H2{y(t)}

    Envelopeenv{y(t)} = crms|A + x(t)|

    m1= crms(A + x(t))

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    Envelope detector

    Hv(t): Bandpass filter to suppress DC component and highfrequencies|| > M

    Non-overlapping sidebands andm 1 v(t) =x(t)

    ()/2

    ()2

    y(t) Hv(j) v(t)

    ()2

    H{}

    Practical implementation

    v(t)v(t)

    y(t)

    y(t) v(t) v(t)

    ttt

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    7.2 Frequency Modulation

    Belongs to class ofangle modulation techniques

    Representation of message in phaseof carrier wave

    Average power= maximum power

    zero dynamic of envelope efficient power amplification

    Higher quality than amplitude modulation

    higher power efficiency than amplitude modulation Requires higher bandwidth than amplitude modulation

    trade-off between power and bandwidth efficiency Angle-modulated signal

    y(t) =

    2crmscos(ct + (t))

    with information bearing phase (t)

    Instantaneous frequency

    i(t) =c+d(t)

    dt

    Types of angle modulation

    Phase modulation (PM)

    (t) =kpx(t)

    Frequency modulation (FM)

    i(t) c=kfx(t)(x(t): modulating signal)

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    Frequency modulation

    Modulated signal

    y(t) = 2crmscosct +

    t

    (i() c) d

    with

    i(t) c=kfx(t)

    Phase signal

    (t) =kft

    x() d

    Maximum frequency deviation

    =kfmax{|x(t)|}

    kf issystem parameter Usually max{|x(t)|}adjusted through limiter is sys-

    tem parameter

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    Example:

    Cosine message signal

    x(t) =Acos(Mt) =kfA

    i(t) c= cos(Mt) (t) = Msin(Mt)

    FM signal

    y(t) = 2crmscosct +Msin(Mt)(= PM signal with x(t) =Asin(Mt) andkp=kf/A)

    t

    t

    t

    y(t)

    y(t)

    x(t)

    PM

    FM

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    Spectrum of FM signals for cosine signal x(t)

    y(t) =

    2crmscosct +

    Msin(Mt)

    = crms2

    y(t)ejct + (y(t)ejct)

    with

    y(t) =ejM

    sin(Mt)

    y(t)periodic with period 2/M

    Fourier series description ofyt)

    y(t) =

    k=Jk

    M

    ejkMt

    with Bessel function of the first kind,nth order

    Jk(u) = 1

    2

    ej(usin(v)kv) dv

    Spectrum ofy(t)

    Y(j) = 2

    k=Jk

    M

    ( kM)

    Spectrum of FM signal

    Y(j) =crms

    2[Y(j( c)) + Y(j( c))]

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    Illustration

    0 2 4 6 8 10 12 14 160.5

    0

    0.5

    1

    6 4 2 0 2 4 60.4

    0.2

    0

    0.2

    0.4

    u

    J0(u)

    J1(u) J2(u)

    Y(j)

    /M= 5

    /M

    J0(5)

    J1(5)

    J2(5)J2(5)

    Interpretation:

    Discrete spectrum LargerM density decreases Larger for fixedM bandwidth increases /M 1:

    J0(/M) = 1, J1(/M) (/M)/2,Jk(/M) 0 fork >1

    Spectrum ofnarrowbandFM similar to double-sideband

    AM with carrier

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    15 10 5 0 5 10 150

    0.2

    0.4

    0.6

    0.8

    15 10 5 0 5 10 150

    0.05

    0.1

    0.15

    0.2

    0.25

    0.3

    15 10 5 0 5 10 150

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    15 10 5 0 5 10 150

    0.05

    0.1

    0.15

    0.2

    0.25

    0.3

    15 10 5 0 5 10 150

    0.1

    0.2

    0.3

    0.4

    0.5

    15 10 5 0 5 10 150

    0.1

    0.2

    0.3

    0.4

    15 10 5 0 5 10 15

    0

    0.1

    0.2

    0.3

    0.4

    15 10 5 0 5 10 15

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    M

    for

    =

    2

    (5kHz)

    forM

    =

    2

    (1kHz)

    = 2 (5kHz)

    M= 20

    M= 10

    M= 2.5

    M= 5

    M= 5

    M= 3.8

    M= 2.4

    M= 1

    M= 2 (1 kHz)

    /(2(1kHZ))/(2(1kHZ))

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    Estimation of bandwidth of FM signal for cosine message signal

    Strictly speaking: infinite bandwidth

    Approximation by Carson

    How many discrete spectral components are required to re-tainp (100%) of the total modulated signal power?Parseval:

    J20(u) + 2

    Kk=1

    J2k(u) p

    Bandwidth limited toB = 2KM

    causes loss of(1p) (100%) in signal powerCarsons approximation of bandwidth of FM signal

    B =

    2(+ M) forp= 0.9

    2(+ 2M) forp= 0.99

    Note: bandwidth measured in Hz (as usual)Bf=B/(2)[Hz]

    Carsons approximation is also applicable to non-cosine message

    signals.

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    Demodulation

    Ideal angle modulation track angle of modulated signal

    v(t) = v1(t) +jv

    2(t) =

    |v(t)

    |ej(t)

    v(t) = d

    dt(arg{v(t)}) = d

    dt

    tan1

    v2(t)

    v1(t)

    = kfx(t)

    Lowpass

    Lowpass

    arg{}

    v1(kT)

    v2(kT)

    2crms

    cos(ct)

    2

    crmssin(ct)

    y(t)

    T

    + v(kT)

    FM-AM conversion

    v(t) = d

    dt

    y(t)

    2crms

    = (c+ kfx(t)) sin(ct + (t))

    and AM envelope detector (c =kfmax{|x(t)|})

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    7.3 Analog Pulse-Amplitude Modulation

    Analog transmission of discrete-time sample valuesof message sig-

    nal

    Amplitude of the pulse carrier is modulated in accordance with in-

    stantaneous sample values of the message signal.

    Pulse-Amplitude Modulation (PAM)

    Lowpass anti-aliasing filtering of message signal band limitation to || M Sampling signal at rate T = 2/s,s>2M

    Modulation of impulses h(t)

    x(nT)x(t)

    Mx(t)

    Lowpass

    h(t) y(t)

    PAM signal

    y(t) =

    n=x(nT)h(t nT))

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    Example:

    Rectangular pulse of durationT0

    h(t) =rect

    t T0/2T0

    y(t) =

    n=x(nT)rect

    t T0/2 nT

    T0

    T

    x(t)

    T0

    y(t)

    t

    Sampling-and-hold operation with sampling period T and holddurationT0

    Express PAM signal

    y(t) =

    x(t)

    k=

    (t kT) h(t)

    Spectrum of PAM signal

    Y(j) = 1

    T

    k=

    X(j( ns))H(j)

    whereH(j) = F{h(t)}

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    Effect of pulse shape

    E.g. h(t) =recttT0/2T0

    F H(j) =T0sincT02 ejT0/2

    ss

    (Xj)

    MM

    sincT0

    2

    2

    T02

    T0

    Frequency distortion

    Shorter pulse duration

    less distortion

    Demodulation of PAM signal

    Lowpass filter with cutoff frequencyM< co s M Compensate for distortion due to pulse shape

    Hr(j)y(t) v(t)

    E.g. for rectangular pulse shape

    Hr(j) =

    1

    T0sinc(T0/(2))ej(TdT0) , || M

    0,

    |

    | (s

    M)

    dont care, else

    v(t) =x(t Td)(delay Td for causal filter)

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    7.4 Multiplexing

    Combination of independent message signals into a composite signal

    suitable for transmission over a common channel

    General structure

    xI(t)

    Channel

    v1(t)

    v2(t)

    vI(t)Demultiplexer

    ......

    x1(t)

    x2(t)

    Multiplexer

    Basic types of multiplexing

    1. Frequency-division multiplexing (FDM)

    Individual signals are separated by allocating them to differ-

    ent frequency bands.

    Used with sinusoidal carrier-wave modulation

    Examples:

    Wired telephony and telegraphy Radio and TV broadcasting 1st generation (analog) cellular phone systems as the US

    Advanced Mobile Phone Service (AMPS), the UK Total

    Access Communications System (TACS), the German C-Netz

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    2. Time-division multiplexing (TDM)

    Individual signals are separated by allocating them to differ-

    ent time slots within a sampling interval.

    Used with (digital) pulse modulation Examples:

    Digital Enhanced Cordless Telecommunications (DECT) 2nd generation digital cellular phone systems as Global

    System for Mobile Communications (GSM), Digital-American

    Mobile Phone Service (D-AMPS), and Personal Digital

    Cellular (PDC)

    3. Code-division multiplexing (CDM)

    Individual signals are separated by assignment of different

    codes to them.

    Used with digital pulse modulation

    Examples:

    3rd generation mobile communication standards CDMA2000,

    Universal Mobile Telecommunications System (UMTS)

    4. Space-division multiplexing (SDM)

    Individual signals are separated spatially.

    Based on directed antennas

    Examples:

    GSM, UMTS

    If the message signals correspond to different user which access the

    same transmission medium, the above techniques are also referred

    to asmultiple-accesstechniques (FDMA, TDMA, CDMA, SDMA).

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    Illustration

    Tim

    e

    Frequency

    SDMCDM

    Frequency

    Tim

    e

    TDM

    Tim

    e

    Frequency

    Power

    Power

    Pow

    er

    FDM

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    7.4.1 Frequency-Division Multiplexing

    Multiplexing

    Lowpass filtering of message signal no interference with othersignals sharing the common channel

    Modulation

    Shift the frequency ranges of signals so as to occupy mutuallyexclusive frequency intervals

    Most widely used: single-sideband AM

    Bandpass filter restrict the band of each modulated wave to itsprescribed range

    Summation forms input to common channel

    Modulator

    Modulator

    Modulator

    ... ...

    Bandpass

    Bandpass

    Bandpass

    x1(t) Lowpass

    x2(t) Lowpass

    xI(t) Lowpass

    supply

    Carrier

    ... ...

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    Demultiplexing received signal

    Bandpass filtering to extract the modulated signals correspond-

    ing to their specific frequency range

    Demodulation to recover the original signal

    Lowpass filtering to reduce interference and noise

    Carrier

    ...

    supply

    Demod.

    Demod.

    Demod.

    vI(t)

    ...

    v2(t)

    v1(t)

    ...

    Lowpass

    Lowpass

    Lowpass

    ...

    Bandpass

    Bandpass

    Bandpass

    To allow for a coexistence of different communication systems and

    standards over the entire usable frequency range, the allocation of

    frequencies for different purposes is controlled by several national

    and international standards and regulation bodies.

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    7.4.2 Time-Division Multiplexing

    TDM is based on the sampling theorem.

    Transmission of oneband-limitedmessage signal engages trans-mission channel for only a fraction of the sampling interval.

    Time interval between adjacent samples is cleared for use by

    other message signals.

    Multiplexing

    Lowpass filtering to restrict bandwidth to || M Commutator

    Takes narrow samples of each of the Imessage signals atrate1/T > /M

    Sequentially interleavesIsamples inside sampling intervalT Pulse modulation

    ......

    LowpassxI(t)

    Lowpassx2(t)

    Lowpassx1(t)

    Commutator

    modulatorPulse-

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    Demultiplexing

    Pulse demodulator produces narrow samples

    Decommutator distributes samples

    Lowpass filtering to reconstruct message signal

    Decommutator

    Pulse-demodulator ...

    Lowpass

    Lowpass

    Lowpass v1(t)

    v2(t)

    vI(t)

    ...

    Timing synchronization between commutator and decommutator

    critical

    Appropriate choice of pulse shape and pulse demodulation to avoid

    intersymbol interference

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