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Transcript of ECEN5633 Radar Theory Lecture #17 10 March 2015 Dr. George Scheets n Read 12.2 n Problems 11.5, 8,...
ECEN5633 Radar TheoryECEN5633 Radar TheoryLecture #17 10 March 2015Lecture #17 10 March 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen5633www.okstate.edu/elec-eng/scheets/ecen5633
ECEN5633 Radar TheoryECEN5633 Radar TheoryLecture #17 10 March 2015Lecture #17 10 March 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen5633www.okstate.edu/elec-eng/scheets/ecen5633 Read 12.2Read 12.2 Problems 11.5, 8, & 12.5Problems 11.5, 8, & 12.5 Corrected quizzes due 1 week after returnCorrected quizzes due 1 week after return
Live: 12 MarchLive: 12 March Exam #2, 31 March 2014 (Exam #2, 31 March 2014 (<< 4 April DL) 4 April DL)
ECEN5633 Radar TheoryECEN5633 Radar TheoryLecture #18 12 March 2015Lecture #18 12 March 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen5633www.okstate.edu/elec-eng/scheets/ecen5633
ECEN5633 Radar TheoryECEN5633 Radar TheoryLecture #18 12 March 2015Lecture #18 12 March 2015Dr. George ScheetsDr. George Scheetswww.okstate.edu/elec-eng/scheets/ecen5633www.okstate.edu/elec-eng/scheets/ecen5633
Read 13.1 & 2Read 13.1 & 2 Problems 12.7, 8, & Web 3Problems 12.7, 8, & Web 3 Corrected quizzes due 1 week after returnCorrected quizzes due 1 week after return
Live: 12 MarchLive: 12 March Exam #2, 31 March 2014 (Exam #2, 31 March 2014 (<< 4 April DL) 4 April DL)
Coherent Detection (PLL), Single Pulse, Fixed Pr
Coherent Detection (PLL), Single Pulse, Fixed Pr
Noise PDFGaussianMean = 0
Variance = kTºsysWn
Echo PDFGaussian
Mean = Pr0.5
Variance = kTºsysWn
r (volts)Matched Filter
Outputat Optimum Time
γ
Coherent Detection (PLL)M Pulse Integration
Fixed Pr
Coherent Detection (PLL)M Pulse Integration
Fixed Pr
Noise PDFGaussianMean = 0
Variance = MkTºsysW n
Signal PDFGaussian
Mean = MPr0.5
Variance = MkTºsysW n
r (volts)Matched Filter
Outputat Optimum Timeγ
Coherent Detection, Single PulseRCS Exponential PDF
Coherent Detection, Single PulseRCS Exponential PDF
Noise PDFGaussianMean = 0
Variance = kTºsysW n
Echo PDFGaussian☺Rayleigh
Mean = Pr0.5
Variance = Var(sig) + Var(noise)= 0.2734Pr
+ kTºsysW n
r (volts)Matched Filter
Outputat Optimum Time
γ
Coherent DetectionM Pulse Integration
RCS Exponential PDF
Coherent DetectionM Pulse Integration
RCS Exponential PDF
Noise PDFGaussianMean = 0
Variance = MkTºsysW n
Signal PDFGaussian
Mean = MPr0.5
Variance = MkTºsysW n
+ MPr0.2734
r (volts)Matched Filter
Outputat Optimum Timeγ
Variance of MFD voltage (Rayleigh) PDF
Integral Result Integral Result
Stephen O. RiceStephen O. Rice
Born 1907Born 1907 Died 1986Died 1986 Bell Labs 1930 – 1972Bell Labs 1930 – 1972 IEEE FellowIEEE Fellow Paper "Mathematical Analysis of Paper "Mathematical Analysis of
Random Noise" discusses Rice PDFRandom Noise" discusses Rice PDF
Source: http://www.ieeeghn.org/wiki/index.php/Stephen_Rice
Friedrich BesselFriedrich Bessel Born 1784Born 1784 Died 1846Died 1846 German MathematicianGerman Mathematician In 1820's, while studyingIn 1820's, while studying
"many body" gravitational"many body" gravitational systems, generalized systems, generalized solutions forsolutions for
Rice PDFRice PDF
x
Starts to look somewhat Gaussian when v/σ2 > 2
Coherent DetectionCoherent Detection Previous Equations are IdealPrevious Equations are Ideal
Require instantaneous phase lock to echoRequire instantaneous phase lock to echo Won't happen in realityWon't happen in reality
Will effectively lose part of echo pulse…Will effectively lose part of echo pulse…• … … Till PLL or Phase-Frequency detector locksTill PLL or Phase-Frequency detector locks
Lock can be obtained on Doppler Shifted echoesLock can be obtained on Doppler Shifted echoes Could use bank of PLL's, free running at different freqsCould use bank of PLL's, free running at different freqs
Coherent Detection not used a lotCoherent Detection not used a lot But equations give feel as to processBut equations give feel as to process
Have somewhat easily digestible derivations Have somewhat easily digestible derivations
Non Coherent Radar DetectionNon Coherent Radar Detection Fixed PFixed Prr & Random Noise & Random Noise
Single Range Bin Single Range Bin Noise has Rayleigh DistributionNoise has Rayleigh Distribution
Mean = 1.253 Mean = 1.253 σσnn
Variance = 0.4292Variance = 0.4292 σ σnn22
σσnn22 = kTº = kTºsyssysWWnn (if calculations off front end) (if calculations off front end)
Signal + Noise has Ricean DistributionSignal + Noise has Ricean Distribution≈ Gaussian if ≈ Gaussian if αα//σσnn
22 = P = Prr0.50.5//σσnn
22 > 5 > 5 Mean = PMean = Prr
0.50.5
Variance = kTºVariance = kTºsyssysWWnn
Noncoherent (Quadrature) Detection, Single Pulse, Fixed Pr
Noncoherent (Quadrature) Detection, Single Pulse, Fixed Pr
Noise PDFRayleigh
Mean = 1.253(kTºsysWn)0.5
Variance = 0.4292kTºsysWn
Echo PDF≈ GaussianMean = Pr
0.5
Variance = kTºsysWn
r (volts)Matched Filter
Outputat Optimum Time
γ
Ex) P(Hit | Coherent) = 0.3253 & P(Hit | Noncoherent) = 0.1692
Noncoherent Detection, M Pulse Integration(Envelope Detection, fixed Pr)
Noncoherent Detection, M Pulse Integration(Envelope Detection, fixed Pr)
Sample envelope M times, sum resultsSample envelope M times, sum resultsMake decision based on sumMake decision based on sumNoise and Signal PDF's approximately GaussianNoise and Signal PDF's approximately Gaussian
P(Hit) = P(Hit) = Q[0.6551QQ[0.6551Q-1-1[P(FA)] + 1.253M[P(FA)] + 1.253M0.50.5 – (M*SNR) – (M*SNR)0.50.5]]
Noncoherent (Quadrature) DetectionM Pulse Integration
Fixed Pr
Noncoherent (Quadrature) DetectionM Pulse Integration
Fixed Pr
Noise PDF≈ Gaussian
Mean = M1.253(kTºsysWn)0.5
Variance = M0.4292kTºsysWn
Signal PDFGaussian
Mean = MPr0.5
Variance = MkTºsysWn
r (volts)Matched Filter
Outputat Optimum Timeγ
Ex) P(Hit | Coherent) = Q(-8.848) & P(Hit | Noncoherent) = Q(-6.523)
CommentComment Noncoherent Integration GainNoncoherent Integration Gain
Sometimes stated as MSometimes stated as M0.5 0.5
P(Hit) ≈ Q[ QP(Hit) ≈ Q[ Q-1-1[P(FA)] – (M[P(FA)] – (M0.50.5*SNR)*SNR)0.50.5 ] ] "Noncoherent Integration Gain, and it's Approximation" "Noncoherent Integration Gain, and it's Approximation"
Mark Richards, GaTech, May 2013Mark Richards, GaTech, May 2013 Has an example where gain is MHas an example where gain is M0.83330.8333
P(Hit) ≈ Q[ QP(Hit) ≈ Q[ Q-1-1[P(FA)] – (M[P(FA)] – (M0.8330.833*SNR)*SNR)0.50.5 ] ] EX) P(Hit) ≈ Q[4.753 – 10EX) P(Hit) ≈ Q[4.753 – 100.8330.833*18.5) *18.5) 0.50.5
= Q[4.753 – 11.22] = Q[-6.469]= Q[4.753 – 11.22] = Q[-6.469] Safer to say gain is MSafer to say gain is Maa; 0.5 < a < 1.0; 0.5 < a < 1.0
Radar P(Hit), Fixed PrRadar P(Hit), Fixed Pr
Single Pulse, CoherentSingle Pulse, Coherent P(Hit) = Q[ Q P(Hit) = Q[ Q-1-1[P(FA)] – SNR[P(FA)] – SNR0.50.5]] Equation 12.19 in textEquation 12.19 in text
M Pulse Integration, CoherentM Pulse Integration, Coherent P(Hit) = Q[ Q P(Hit) = Q[ Q-1-1[P(FA)] – (M*SNR)[P(FA)] – (M*SNR)0.50.5 ] ] See equation 13.3 in textSee equation 13.3 in text
Radar P(Hit), Exponential PrRadar P(Hit), Exponential Pr
Single Pulse, CoherentSingle Pulse, CoherentNoise is GaussianNoise is GaussianSignal (echo) Voltage is RayleighSignal (echo) Voltage is Rayleigh Evaluate 2nd Order PDF f(n,s) or f(n)☺f(s)Evaluate 2nd Order PDF f(n,s) or f(n)☺f(s)
M Pulse Integration, CoherentM Pulse Integration, CoherentP(Hit) ≈ Q{[QP(Hit) ≈ Q{[Q-1-1[P(FA)][P(FA)]σσnn
– (M*P– (M*Psignal_1signal_1))0.50.5 ]/ ]/σσsumsum}} where where σσsum sum = (= (σσ22
nn + + σσ22ss))0.50.5
σσ22nn = noise power = noise power
σσ22s s = variance of noise free signal (echo) voltage= variance of noise free signal (echo) voltage
= 0.2734*M*P = 0.2734*M*Psignal_1signal_1
Radar P(Hit), Fixed PrRadar P(Hit), Fixed Pr Single Pulse, NoncoherentSingle Pulse, Noncoherent
Noise is Rayleigh DistributedNoise is Rayleigh DistributedSignal is Ricean Distributed → GaussianSignal is Ricean Distributed → GaussianP(Hit) ≈ Q[P(Hit) ≈ Q[γγ//σσnn – SNR – SNR0.50.5]]
where where γγ = {ln[1/P(FA)]2 = {ln[1/P(FA)]2σσnn22}}0.50.5
Equation 12.49 in TextEquation 12.49 in Text M Pulse Integration, NoncoherentM Pulse Integration, Noncoherent
P(Hit) ≈ Q[ QP(Hit) ≈ Q[ Q-1-1[P(FA)] – (M[P(FA)] – (MaaSNR)SNR)0.50.5 ] ]
P(Hit) ≈ Q[ 0.655QP(Hit) ≈ Q[ 0.655Q-1-1[P(FA)] +1.253M[P(FA)] +1.253M0.50.5 - (M*SNR)- (M*SNR)0.50.5 ] ]
Noncoherent DetectionFluctuating Pr
Noncoherent DetectionFluctuating Pr
Will not be derived in classWill not be derived in class Text has calculations for several casesText has calculations for several cases Below is PDF of SignalBelow is PDF of Signal
Sum of S.I. Gaussian noise & Rayleigh echoSum of S.I. Gaussian noise & Rayleigh echo
Need PDF of I sumNeed PDF of I sum22 added to another SI Q sum added to another SI Q sum22, then take , then take square root.square root.
Peter SwerlingPeter Swerling
Born 1929Born 1929 Died 2000Died 2000 PhD in Math at UCLAPhD in Math at UCLA Worked at RANDWorked at RAND
Entrepreneur (founded 2 consulting companies)Entrepreneur (founded 2 consulting companies) Developed & analyzed Swerling Target Models Developed & analyzed Swerling Target Models
in 1950's while at RANDin 1950's while at RAND
SwerlingModel
Performance
M = 10Noncoherent Integration
P(FA) = 10-9
SwerlingModel
Performance
M = 10Noncoherent Integration
P(FA) = 10-9
Source: Merrill Skolnik's Introduction to Radar Systems, 3rd Edition
Receiver Phase Locked LoopReceiver Phase Locked Loop
XActive
Low PassFilter
VoltageControlledOscillator
cosωct(from antenna)
sin((ωvcot +θ) -sin((ωvco -ωc)t+θ)
VCO set to free run at ≈ ωc
VCO output frequency = ωc + K * input voltage
LPF withnegative gain.
2 sinα cosβ = sin(α-β) + sin(α+β)
PPI with clutterPPI with clutter
Source: www.radartutorial.eu