1 channel models 2004

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    Channel models

    Propagation channel

    physical medium between antennas

    Radio channel

    propagation channel + transmitter and

    receiver antennas

    Digital channel

    includes the modulation and demodulation

    Radio wave propagation

    In this course we concentrate on radiochannels

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    Radio wave propagation

    BS

    Pt

    Pr1

    Pt

    Pr2

    Radio wave propagation - fading

    Line-of-Sight (LOS)

    Reflection ()

    Scattering (>>object)

    = signalwavelength

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    Too complicated to use in practice

    Other, simpler solutions are used

    Maxwells equations

    Radio wave propagation

    Radio wave propagation

    Usually separated in to three groups

    Path loss

    Shadow fading

    Multipath fading

    Propagation effects

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    Radio wave propagation

    Path loss

    Shadow fading

    Multipath fading

    PrxPtr

    d=vt

    v

    Prx/Ptr

    d=vt

    Very slow

    Slow

    Fast

    Ptr= transmitted powerPrx = received power

    Radio wave propagation

    shadow fading gainsg

    distance dependent

    average path gain

    pg

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    Radio wave propagation

    BS

    Pt

    Pr1

    Pt

    Pr2

    Radio wave propagation

    Mobile unit is distance raway from antenna

    Distance dependence:

    Distance dependent path loss (gp)

    Shadow fading gain (gs) The multipath gain (gm)

    RECEIVED POWER

    rx tx p s mP P g g g = + + +

    in dB scale

    rx tr p s m tr P gP g g g P = =

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    Radio wave propagation

    Radio wave propagation (dB)

    RECEIVED POWER in dB scale (No bars)

    Definition of decibel (dB), dbW and dBm

    1010log

    gain in dB

    = input power

    = output power

    outdB

    in

    dB

    in

    out

    PG

    P

    G

    P

    P

    =

    =

    rx tx p s mP P g g g = + + +

    10

    dBW = decibel-Watt

    10 log1 W

    WdBW

    PowerPower =

    10

    dBm = decibel-milliWatt

    10 log

    1 mW

    mWdBm

    PowerPower =

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    Radio wave propagation

    Separated in to three groups

    Path loss

    Shadow fading

    Multipath fading

    Propagation effects

    Distance power loss

    Average path loss

    10 2log ,

    in dB

    p pg C r =

    2

    2;

    4p tr rx

    Cg C G G

    r

    = =

    2

    2

    4

    rx tr tr rx

    tr p tr

    P P G G

    rC

    P g P r

    =

    = =

    Carrier wavelength =r = propagation distance

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    Shadowing

    Shadowing

    Shadowing

    A terminal moving behind a hill, etc.

    At or above 300 MHz, the amount of diffracted energy is

    low shadows will be distinct

    Signal will fluctuate shadow fading

    Shadowing gain can be estimated

    Included in Geographical Information Systems (GIS)planning tools

    Finer details not known

    maps have resolution of 50-100 m

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    Shadowing

    Path loss

    Shadow fading

    PrxPtr

    d=vt

    v

    Prx/Ptr

    d=vt

    Very slow

    Slow

    Ptr= transmitted powerPrx = received power

    log-normal

    Shadowing

    Shadowing

    A common model log-normal, probability density

    function

    log-standard deviation 8-12 dB

    2

    2

    ( )

    21( )

    2

    i avg

    i

    g g

    i

    i

    p g e

    =

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    Shadowing

    ShadowingA common model log-normal, probabilitydensity function

    Model parametersobained

    empirically.

    dB power normally

    distributed

    Shadowing

    Shadowing

    log-normal

    rx tr p tr

    C

    P g P r= =

    Prx/Ptr

    d=vt

    Very slow

    Slow

    log-normal

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    Shadowing

    Autocorrelation between dB-samples of the signal level

    taken at sample rate 1/T in a mobile moving at speed v,

    given by

    where = correlation of two shadow fading gains,

    X(r) andX(r+D)

    2( )k

    XR k a= /T Da =

    D

    Shadowing

    hb =

    Antenna

    height

    hm =

    Mobile

    height

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    Shadowing

    Okumura-Hata

    Multipath fading

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    Multipath fading

    Multipath fading

    Looking more microscopic model:

    Fast multipath fading dependent on phase differencesbetween wave components

    Shadow fading is slow (wavelengths 10-100 m),multipath fading very rapid (wavelengths 0.5-1 m)

    Multipath fading is narrowband phenomenon, when thedelay of the multipath components < the symbol durationof the transmitted signals

    For wideband signals, the received power fluctuationshave considerably lower amplitude.

    Multipath fading

    Line-of-Sight (LOS)

    Reflection ()

    Scattering (>>object)

    = signalwavelength

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    Effects of multipath fading

    Intersymbol interference

    Multipath model

    Random number of multipathcomponents, each with

    Random amplitude Random phase

    Random Doppler shift

    Random delay

    Each component varies with time

    Model is time-varying impulseresponse

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    Multipath model

    Response of a channel at time ttoimpulse at t-

    Each component varies with time

    Model is time-varying impulse

    response

    Multipath model

    Response of a channel at time tto impulse at t-

    t = time when impulse is observed

    t-= time when impulse was put into the channel

    = how long ago impulse was put into channel

    ( ) ( )1

    , ( ) ( ( ))nN

    j tn n

    n

    c t t e t

    ==

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    Multipath model

    Response of a channel at time tto impulse at t-

    n = changes slowly

    n = changes quickly

    Amplitude fading

    ( ) ( )1

    , ( ) ( ( ))nN

    j t

    n n

    n

    c t t e t

    =

    =

    Multipath fading

    Narrowband signals central limit theorem used

    Received signal hasNcomponents

    Herex(t) andy(t) uncorrelated Gaussian processes

    (N large and incoming components have the same

    statistical properties).

    { } ( )( )1 1 1

    ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( )N N N

    j t

    n n n n

    n n n

    z t t e x t jy t x t jy t x t jy t

    = = =

    = = + = + = +

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    Multipath fading

    Amplitude

    Phase

    2 2( ) ( ) ( )t x t y t = +

    ( )( ) arctan

    ( )

    x tt

    y t =

    Multipath fading

    The joint probability density function

    2-D Gaussian

    Joint probability density function of

    has uniform distribution over the interval

    independent of

    ( ) and (t)t

    2 22

    2( , )

    2

    Marginal distribution of

    p e

    =

    2 2- 2

    2Rayleigh dist

    rp() = e ibu

    tion

    ( )t

    ( )t [0,2 ]

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    Multipath fading

    First two moments of

    Compute the density of the power of

    Then

    [ ] 2

    ( )2

    2 14

    E

    Var

    =

    =

    ( )t

    2( ), (t)= ( )t t

    0

    0

    1( )p e

    =

    2 2

    0 ( ) 2E E = = =

    ll signalcomponents have

    the same energy.

    The Resource Management Problem

    ll signalcomponents have

    the same energy

    If there is a strong

    component

    one can compute( ) ( ) ( )z t x t jy t = + +

    2 2 2( ) 2

    0 2 2

    0

    ( )

    zero-order Bessel function

    amplitude of the dominant, constant signal

    (line-of-sight)

    p I e

    I

    + =

    Nakami-Rice or just Rice distribution

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    Multipath fading time series models

    Jakes model in fading

    Multipath fading Jakes model

    N0 low-frequency oscillators with frequency

    = Doppler shifts

    m=cos(2n/N), n=1,2,...,N0, +

    m are used to generate signals with frequency-shifted from a carrier frequency c using modu-lation methods. The amplitudes are =1 except mwhich is = .

    n chosen so that the probability distribution ofthe resultant phase is close to uniform didtri-

    bution (1/2).N0=8.

    1/ 2

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    Multipath fading time series models

    and others

    Slow correlation in fading

    { }

    [ ] [ ]

    1 2 1

    2 2

    2

    1 2 1

    ( ) ( 1) ( 2) ( ) ( 1),

    ( ) ,

    , , 1.8384,0.8395, 0.9634 , 2.01,

    Sample instanst are with respect to spatial sample interval ,

    0.1 m

    s s s s s

    s e

    T T

    e

    s

    s

    g k a g k a g k e k b e k

    Var e k

    a a b

    k x

    x

    = + +

    =

    = =

    =