ch5-radar+target+and+clutter

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<레이다 공학> 교수 [email protected] 항공전자 및 정보통신 공학부 한국항공대학교

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radar target and clutter

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  • [email protected]

  • Korea Aerospace Univ. (Prof. Kwag)

    Lecture 5 : Targets and Clutter

    Objective

    - Radar Cross Section - Target Fluctuation - Clutter - Clutter

    - RCS Definition and Fundamentals - RCS Fluctuation - Target Fluctuation Models - RCS of Fundamental Shapes - RCS of Complex Objects - Interfering Signals-Noise - Radar Clutter Model - Surface Clutter Characteristics - Volume Clutter Characteristics - Moving Clutter - Doppler Spectrum - Reference

    2

  • Korea Aerospace Univ. (Prof. Kwag) 3

    Part I : Radar Target

  • Korea Aerospace Univ. (Prof. Kwag)

    5.1 RCS Definition and Fundamentals

    4

    RCS Definition - Target RCS (Radar Cross Section) is defined as the ratio of its effective isotropically reflected power to the incident power density

    areaUnitpowerIncident

    anglesolidUnitpowerReflected 4

    - RCS measures the targets reflection of signals in the direction of the radar receiving antenna

    backscatter, which is the only reflected energy from the target to the radar

    24 T

    TTtgt

    R

    GPP

    )(

    targetbyreflectedtgt

    wattsradartheofdirectionthein

    thepowereffectivetheP

    222 4

    1

    44

    1

    RR

    TT

    R

    tgtRR

    GP

    RPP

    rBackscatte

    24 T

    TTtgt

    R

    GPP

  • Korea Aerospace Univ. (Prof. Kwag)

    5.1 RCS Definition and Fundamentals

    5

    Mode of Radar Cross Section

    < Mode of Radar Cross Section >

  • Korea Aerospace Univ. (Prof. Kwag)

    5.1 RCS Definition and Fundamentals

    6

    RCS Dependence on Shape and Angle

    < RCS Dependence on Shape & Orientation >

  • Korea Aerospace Univ. (Prof. Kwag)

    5.1 RCS Definition and Fundamentals

    7

    RCS Components

    )(

    :

    :

    :

    metersquareunitGA

    radartheofdirectiontheintargettheofgainG

    radartheofpolizationtheattargettheoftyreflectivi

    targettheofareaA

    tgttgttgt

    tgt

    tgt

    tgt

    Target Field Zone

    .

    2 2

    antradartheofaxisthetonormalextentlinerstarget'Dwhere

    DR

    distancefieldFar

    FF

  • Korea Aerospace Univ. (Prof. Kwag)

    5.2 RCS Fluctuation

    8

    RCS Fluctuation - Amplitude fluctuation : scintillation = variations in received echo power - Phase fluctuation : glint = wave fronts echoing from the target

    Fluctuation speed - slow fluctuation : time constant is greater than dwell time, vary from scan to scan - rapid fluctuation : varies from pulse to pulse

    < Slow and Rapid Fluctuations >

  • Korea Aerospace Univ. (Prof. Kwag)

    5.2 RCS Fluctuation

    9

    Fluctuation Mechanism - Fluctuation of extended target (single far field target)

    total RCS is the vector sum of the all small elemental scatterers

    RCS depends on the targets aspect angle

    different angles cause different summations

    reflectionnozero

    negativesumvector

    < Fluctuations of a Single Extended Scatterer >

  • Korea Aerospace Univ. (Prof. Kwag)

    5.2 RCS Fluctuation

    10

    - Fluctuation of array of scatterers vs. aspect depends on the aspect angle from which a complex target of many

    scatterers is viewed

    (EX) aircraft target RCS

    : summation of many individual scattering center on target

    )(....... 2 termpowerRCSTotal n21 RCSRCSRCS

    - Fluctuation of complex targets as a function of freq. depends on the viewing a target at different frequencies

    Notes

    spacing of the scatterers and the wave length

    determines the amount of fluctuation for a given freq.

    The wider the spacing, the greater the RCS fluctuation with small freq. change

  • Korea Aerospace Univ. (Prof. Kwag)

    5.2 RCS Fluctuation

    11

    - RCS Dependence Angle and Frequency of 3 GHz

    < Aspect Dependence of RCS for Complex Target >

    < Frequency Dependence of RCS >

  • Korea Aerospace Univ. (Prof. Kwag)

    5.2 RCS Fluctuation

    12

    - Fluctuation from multi-path

    < Target Fluctuation Caused by Multipath>

    from signal path : d-d, d-r, r-d, r-r

    As the range changes, the sum of four signals changes

    * Note : RCS varies from zero to 16 times.

  • Korea Aerospace Univ. (Prof. Kwag)

    5.3 Target Fluctuation Models

    13

    Marcum / Swerling Models [Ref]

    - Marcum : A Statistical Theory of Detection by Pulsed Radar IRE Tr. Vol. IT-6, PP.59-267, Apr, 1960

    - Swerling : Probability of Detection for Fluctuating Targets IRE Tr. Vol. IT-6, PP.269-308, Apr, 1960

    Swerling case 0 and case 5 - non fluctuating target - modeled as single isotropic scatterers - targets size

  • Korea Aerospace Univ. (Prof. Kwag)

    5.3 Target Fluctuation Models

    14

    Swerling case 1 - slowly fluctuating target (large fluctuation, scan to scan) - modeled as several scatterers, equal RCS - little aspect change over a look (Ex) Aircraft target without pulse-to-pulse freq. agility

    Swerling case 2 - rapidly fluctuating target, large fluctuation - modeled as case 1 - aspect angle is rapidly changing - complex target for pulse-to-pulse freq. Agility

  • Korea Aerospace Univ. (Prof. Kwag)

    5.3 Target Fluctuation Models

    15

    Swerling case 3 - slowly fluctuation target, small fluctuation - modeled as one prominent scatterer with several scatterers (ex.missile)

    - aspect angle changes are small(scan to scan) over a look Swerling case 4

    - same as case 3 - rapidly fluctuating target - rapid aspect angle changes or from radar freq. change agility

  • Korea Aerospace Univ. (Prof. Kwag)

    5.3 Target Fluctuation Models

    16

    RCS Case Changes through Target Argumentation

    Small Target

    (case 1&2 model)

    Large Single RCS Scatterer Target case 3 & 4 model

  • Korea Aerospace Univ. (Prof. Kwag)

    5.4 RCS of Fundamental Shapes

    17

    Sphere RCS vs. Frequency - If wavelength = circumference, resonance case : circumference = 0.5 10 times wavelength

    RCS varies from 0.3 3.5 times optical cross section

    called MIE region

    - wavelength >> circumference, RCS ratio = (kr) power of 4 called Rayleigh scattering region

  • Korea Aerospace Univ. (Prof. Kwag)

    5.4 RCS of Fundamental Shapes

    18

    RCS of Fundamental Shapes

    RCS of Fundamental Shapes

    (Adapted from Barton)

  • Korea Aerospace Univ. (Prof. Kwag) 19

    (a) Sphere RCS

    sigma = pi.d2 /4 (equation. 4.8)

    where d = spheres diameter

    Cylinder RCS

    Flat plate RCS

    cLdffreqoftermsinRCScylinderconductingfor

    Ldcylinderfosectioncrossradarbroadsidepeak

    dLAareacylinder

    lengthncecircumferethe

    CYL

    CYL

    2

    2

    .

    &

    22222 44 cAfAFP

    RCS of Fundamental Shape-I

  • Korea Aerospace Univ. (Prof. Kwag) 20

    RSP Lab Hankuk Aviation Univ.

    dwhenoccursofvaluepeak 2

    88.0 2

    aircraftanoffuselagewingaofonintersectifromRCShighaccidently

    .argumentortargetforusedso,plate.thethanwidermuchlobeRCSpeak

    triangularforaCR

    &,

    ,)3(4 22

    224

    .

    .

    A

    lobemainwide

    arriveditwhichfromdirectiontheinpowerreflectwhichdevice

    LL

    principlereflectorCorner

    reflection%100

    RCS of Fundamental Shape-II

  • Korea Aerospace Univ. (Prof. Kwag) 21

    Luneburg Lens Principle

  • Korea Aerospace Univ. (Prof. Kwag)

    5.4 RCS of Fundamental Shapes

    22

    Triangular Corner Reflector RCS

  • Korea Aerospace Univ. (Prof. Kwag)

    5.5 RCS of Complex Objects

    23

    RCS of Complex Object

    < T-33A Aircraft >

  • Korea Aerospace Univ. (Prof. Kwag)

    5.5 RCS of Complex Objects

    24

    < T-33A Aircraft at 425MHz >

    < T-33A Aircraft at 3.0 GHz >

  • Korea Aerospace Univ. (Prof. Kwag)

    5.5 RCS of Complex Objects

    25

    Hypothetical RCS Data

  • Korea Aerospace Univ. (Prof. Kwag) 26

    Part II : Radar Clutter

  • Korea Aerospace Univ. (Prof. Kwag)

    5.6 Radar Clutter Model

    27

    Definition - Clutter is a term used to describe, any object that generate unwanted radar returns that may interfere within normal

    radar operation

    - Classified into two categories surface clutter : trees, vegetation, ground terrain,

    see surface (see clutter)

    volume clutter : chaff, rain, birds, insects

    - Note clutter signal is much higher than the receiver noise level

    SCR(Signal to Clutter Ratio)

  • Korea Aerospace Univ. (Prof. Kwag)

    5.7 Radar Clutter Model

    28

    Radar Clutter Type

    SEA

    desert

    stormDustfarmland

    AnglesChaffvegetated

    Insectssnowwoods

    Birdsrainmountains

    vehiclesMovingWeatherLand

  • Korea Aerospace Univ. (Prof. Kwag)

    5.6 Radar Clutter Model

    29

    Radar Clutter Characteristics

    Weibull),Normal-Log,us(homogeneoondistributiSpatial

    Rician),(RayleighnfluctuatioAmplitude

    velocity)(radilshiftdopplerAverage

    Gaussian) (e.g.widthandshapeSpectrum

    )mmormm(tyReflectivi 3222

  • Korea Aerospace Univ. (Prof. Kwag)

    5.6 Radar Clutter Model

    30

    Reflectivity

    length

    volume

    area

    Lextentlinear

    sectionsscroradar

    m

    m

    caseDcorridorchaffNarrow

    Volumevcellresolution

    sectionsscroradar

    m

    m

    caseDclutterVolume

    Aareacellresolution

    sectionsscroradar

    m

    m

    caseDclutterSurface

    ctivityRefleClutter

    11

    2

    1

    33

    2

    3

    0

    2

    20

    )1(

    )3(

    )2(

  • Korea Aerospace Univ. (Prof. Kwag)

    5.6 Radar Clutter Model

    31

    Clutter Environmental Characteristics

  • Korea Aerospace Univ. (Prof. Kwag)

    5.6 Radar Clutter Model

    32

    Clutter Doppler Characteristics - Clutter bandwidth

    < Summary of Standard Ceviations of the Clutter Spectrum >

  • Korea Aerospace Univ. (Prof. Kwag)

    5.6 Radar Clutter Model

    33

    Clutter Spectrum Characteristics - Response of a double canceller MTI to ground, rain and chaff clutter

  • Korea Aerospace Univ. (Prof. Kwag)

    5.7 Surface Clutter Characteristics

    34

    Surface Clutter

    ondistributiAmplitude

    onpolarizatiBeam

    velocityMean

    spreadVelocity

    angleGrazing

    tyreflectivideterminesstateSeaSea

    spreadSpectrl

    ondistributiAmplitude

    angleGrazing

    ctivityRefleLand

    sticscharactericlutterArea

    )(

  • Korea Aerospace Univ. (Prof. Kwag)

    5.7 Surface Clutter Characteristics

    35

    Radar Equation for Surface Clutter

    gdBC

    cRA

    sec

    23

    RcSCR

    R

    GPclutterfromreceivedPower

    R

    GPfromradarbyreceivedPower

    dB

    gt

    AC

    ct

    tt

    3

    0

    43

    22

    c

    43

    22

    t

    cos2)(

    )4(S

    )4(Starget

  • Korea Aerospace Univ. (Prof. Kwag)

    5.7 Surface Clutter Characteristics

    36

    Clutter Region - low grazing angle region

    < Example of Clutter Regions >

    heightsurfaceRMShwherehanglecritical

    heightRMShwhereh

    EEC :4

    sin:

    :8

    sin

    - plateau region : the scattering is by facets smaller than the wavelength - high grazing angle region : specular scattering, with diffuse clutter components disappearing. angle90o as specular mirror, clutter coefficient is larger for

    smooth terrain and seas than for rough

  • Korea Aerospace Univ. (Prof. Kwag)

    5.7 Surface Clutter Characteristics

    37

    Rough Surface Definition

    grms

    grms

    g

    hphasedifferencepath

    hncedisabypathsmooththanlongerispathrough

    hifsmooth

    sin22

    .sin2tan ""

    2sin

    4

    < Rough Surface Definition >

  • Korea Aerospace Univ. (Prof. Kwag)

    5.7 Surface Clutter Characteristics

    38

    Sea clutter

    velocitylengthperiodheightwave

    wavehighzerostepsSSStateSea

    ctn

    SS

    C

    g

    g

    ,,,

    )~(8~0:)(

    tan

    )2(tanexplog10

    )log(sin10log10)1(664

    0

    0

    2

    2

    0

    2

    0

    Land clutter

    mountainfordesertforA

    uB

    ctnA Cg

    g

    14~29:

    tan

    )(tanexplog10)log(sin10log10 0

    02

    2

    02

    0

  • Korea Aerospace Univ. (Prof. Kwag)

    5.7 Surface Clutter Characteristics

    39

    Rayleigh Distribution - First sea & land clutter empirically, composed of many

    small scatterers with in the resolution cell (not spiky)

    Log-normal Distribution - Fits

    Some low angle land clutter

    High resolution samples of sea clutter

    )(:2

    clutter.RMSthe tonormalizedvariable:

    0)2exp(2

    )(

    22

    0

    2

    0

    2

    2

    0

    meanxofvalueaveragex

    tindependenxwhere

    xforxxx

    xxP

    xlnofdeviationstandard:

    :x

    variable:

    02

    lnlnexp)2()(

    m

    2

    2

    5.0

    xofvaluemedian

    tindependenxwhere

    xforxx

    xxP m

  • Korea Aerospace Univ. (Prof. Kwag)

    5.7 Surface Clutter Characteristics

    40

    K-distribution - For sea clutter

    parametershapev

    parameterscaleb

    ordervthkindthirdtheoffunctionBesseleK

    powerclutterxwhere

    bKvbxvbxP

    v

    v

    :

    :

    ,modifid:

    :

    2)(2)( 1

    Weibull distribution - first low angle clutter in 0.5~5.0 for 1~10GHz

    tioncrosscluttermeanx

    parametershapeb

    normalizedrbackscatteclutterwhere

    foraa

    bP

    bb

    sec:

    :

    :

    0exp)(

    1

    11

    1

    11

  • Korea Aerospace Univ. (Prof. Kwag)

    5.7 Surface Clutter Characteristics

    41

    Clutter Doppler Sea & Land - Sea clutter doppler

    .,3

    36.0,65.0

    10101.0

    101.0

    14.0

    freqpowerhalffnwhere)ff(1

    1P(f)

    ondistributispectral

    secondpermetersifknotsinareWandifisB

    speedwindWdeviationstandard

    CnC

    SV

    SSBV

    SV

    - Land clutter doppler

    ionapproximatGaussian)ff(11fP

    terrainvegetatedforb

    terrainvegetatedforaaW

    terrainvegetatedfor

    ddistributeGaussianspectrumstandard

    Wf

    3C

    bSV

    SC

    )(

    28.1

    007.0

    )0272.0exp(33.1

  • Korea Aerospace Univ. (Prof. Kwag)

    5.8 Volume Clutter Characteristics

    42

    Volume Clutter (weather, chaff, insect & birds) - Weather clutter

    modeled as a very simple elemental scatterers

    raindrops modeled as a sphere, co-polarized

    dropthiofdiameterDwheretyreflectiviDZ

    cellresolutiontheofvolumeVwhereV

    RCSTotal

    scatterersthitheofRCSwheremm

    RCStheofsummation

    ii

    II

    ii

    ;

    )(

    6

    32

    - Chaff

    215.0 Chaff

    cluttervolumegeneratedlyartificial

  • Korea Aerospace Univ. (Prof. Kwag)

    5.8 Volume Clutter Characteristics

    43

    - Angel clutter (birds, insects, dust)

    s)nsects(dBmiorbirdsindividualofRCSwhere

    W

    bi

    bibi

    :

    log8.546

    cRV

    resolutionvolume

    eaW2

    8

  • Korea Aerospace Univ. (Prof. Kwag)

    5.11 Reference

    [1] Radar Cross-Section by E. F. Long, J. F. Shaeffer, and M. T. Tuley,

    Artech House, 1985

    [2] Radar Reflectivity of Land and Sea by M. W. Long, Artech House, 1983

    [3] Handbook of Radar Scattering Statistics for Terrain by F. T. Ulaby and

    M. C Dobson, Artech House, 1989

    [4] Airborne Early Warning Radar by W.C. Morchin, Artech House, 1990

    [5] Radar System Analysis by D. K. Barton, Artech House, 1976

    [6] The Scattering of Electromagnetic Waves from Rough Surfaces by P. Beckmann

    and A. Spizzichino, Artech House 1987

    [7] Introduction to Radar System by I. Katz in M. I. Skolink, McGraw-Hill, 1980

    44