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Synthetic Aperture Radar

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1 Synthetic Aperture Radar
Chiba University Signal Processing Synthetic Aperture Radar Josaphat Tetuko Sri Sumantyo, Ph.D Center for Environmental Remote Sensing, Chiba University

2 Contents 1. Introduction of Synthetic Aperture Radar (SAR)
2. SAR Applications (History, Theory, Relationship with Remote Sensing etc) 3. Basic of Electromagnetic waves (Wave, Polarization, Absorption, Scattering etc) 4. Radar Equation and Microwave Scattering (Antenna Pattern) 5. Pulse Compression Technique and Image Production in Range Direction 6. Synthetic Aperture Technique and Image Production in Azimuth Direction 7. Basic of SAR Image Analysis

3 References

4 References

5 Introduction Microwave Sensor Active Sensor SAR and Definition
  SAR (Synthetic Aperture Radar)     Satellite (sensor) itself illuminates microwave, then sensor receives backscattered wave and processes this signal to be an image. Benefit of SAR     All weather     Day and night time monitoring (Active sensor)     High coherency → InSAR applications     Polarization characteristics → Polarimetry Lack of SAR     Analysis of backscattering Microwave Image  very complicated       (Different to the point of view in optical image analysis)     Image distortion (foreshortening, shadowing etc) caused by side looking  Microwave Sensor  Active Sensor  Imaging Radar

6 Introduction SEASAT (1978) SIR-A (1981) SIR-B (1984) SIR-C (1994) Frequency (GHz) 1 1, 5 Polarization HH HH, HV, VH, VV Look angle 20o 50o 20o – 60o Analog data Digital data Central Transmitter/ Receiver Distributed T/R modules Fixed antenna beam Mechanical beam steering Electronic Pictures :

7 Introduction ERS-1 (1991) JERS-1 (1992) Radarsat (1995) Frequency (GHz) 5 (C band) 1.275 (L band) Polarization VV HH Look angle 20o 35o 20o – 60o Pictures :

8 Specification of ALOS-PALSAR
Introduction Specification of ALOS-PALSAR Main Observation Mode High Resolution Mode SCAN SAR Observation Frequency L-band(1.27GHz) Polarization HH,VV,HH&HV,VV&VH HH,VV Ground Resolution 10m 100m Look numbers 2 8 Swap area 70km 250~350km Off Nadir Angle 10~51°

9 Satellite-onboard SAR and flat-ground geometric system
sensor / antenna ①: off-nadir angle   (look angle) ②:depression angle ③:range beam width ④:incidence angle ⑤:azimuth beam width horizontal direction platform direction slant range direction range direction azimuth direction far range near range Ground range target JERS-1 SAR antenna Pi-SAR (NICT/JAXA)

10 Optic sensor and microwave sensor
Optic sensor  :employed wavelength is recognized by human eyes                    Sun light scattering  easy to recognize  Microwave sensor :wavelength is cm order  difficult to recognize                    Mechanism of backscattering  complicated                    Image distortion Mount Fuji : JERS-1 / OPS Mount Fuji : JERS-1 / SAR

11 Microwave characteristics
Wave expression : phase and amplitude Electromagnetic fields vibrate as the function of time when observed in one point in the space Space distribution of electromagnetic fields is the function of space when time is fixed amplitude wavelength electric field electric field time(t) phase:f space (x) Time changing signal can be expressed as space function by using variable of amplitude and phase df wave expression: F(t)=exp[2pift] f : frequency  = f dt

12 Wavelength Domain of Microwave
10GHz GHz 0.2mm mm mm mm cm m Band Wavelength (mm) Frequency(GHz) Ka 7.5 ~ 11.0 40.0 ~ 26.5 K 11.0 ~ 26.7 26.5 ~ 18.0 Ku 16.7 ~ 24.0 18.0 ~ 12.5 X 24.0 ~ 37.5 12.5 ~ 8.0 C 37.5 ~ 75.0 8.0 ~ 4.0 S 75.0 ~ 150 4.0 ~ 2.0 L 150 ~ 300 2.0 ~ 1.0 P 300 ~ 1000 1.0 ~ 0.3 Visible                          Microwave IR NIR                             KaKuX C S L P Wavelength domain of electromagnetics and definition 100 Atm. Pen. % 50 0.2mm mm mm mm cm m wavelength Atmospheric penetration ratio

13 Reflection and Penetration of Microwave
incident wave scattering wave Relationship of scattering and penetration q q ratio of scattered and penetrated wave :  effect of dielectric constant mirror / corner reflection :   effect of surface roughness penetrated wave q`

14 Reflection and Penetration of Microwave
corner reflection water / sea surface : high dielectric constant perfectly scattering / corner reflection black color on SAR image Krakatau volcano complex, Indonesia

15 Reflection and Penetration of Microwave
Effect of earth’s surface :    Rayleigh conditions : h≦l/(8 cos q) → standard of smooth surface         in case of JERS-1: l=0.23m, q=38o           Conditions to satisfy ① : h≦3.65 cm ① smooth surface ② slightly rough surface ③ rough surface Illustration of microwave scattering by earth’s surface

16 Krakatau volcano complex, Indonesia
③ rough surface ① smooth surface ② slightly rough surface Krakatau volcano complex, Indonesia

17 Scattering of microwave : surface scattering and volume scattering
(a) scattering on the boundary surface (different dielectric constant ) (b) scattered wave is reflected to different direction from incident wave          Volume scattering   (a) Penetrated electromagnetic wave is traped in the dielectical material (b) Scattered wave in object on the earth’s surface (i.e. forest)

18 Scattering of microwave : surface and volume scatterings
Scattering Models vegetation (forest) icy river surface scattering surface scattering volume scattering volume scattering surface scattering surface scattering dried sandy area surface scattering volume scattering surface scattering

19 Polarizations Linier polarization Linier polarization
Horizontal polarization Circular Pol. Left handed circular polarization(LHCP)

20 SAR History 1953 Carl Wiley (Good Year Corporation) invented SAR
1960s Civil application : archeology, real aperture interferometry SEASAT (NASA) : 25m resolution, L band 1980s ALMAZ (Soviet), Shuttle Imaging Radar (SIR)(NASA) ERS-1 (ESA), Interferometry, C band 1992 JERS-1 (JAXA), 12.5m resolution, L band RADARSAT (RSI) 1999 SRTM, single pass interferometry, 80% continental coverage 2002 ENVISAT (ESA) 2006 ALOS

21 SARs Specification ERS-1 JERS-1 RADARSAT ENVISAT ALOS Launched date
April 1991 February 1992 November 1995 March 2002 January 2006 Height 785 km 568 km km 799.8 km km Inclination angle 98.5 degrees 97.7 degrees 98.6 degrees 98.55 degrees 98.16 degrees Frequency 5.3 GHz (C band) 1.275 GHz (L band) 5.331 GHz ( C band) 1.27 GHz (L band) Wavelength 5.7 cm 23.5 cm 5.6 cm 23.6 cm Polarization VV HH HH, VV, HH+VV, VV+VH, HH+HV HH, VV, HH+HV, VV+VH, HH+VV+ HV+VH Off-nadir angle 20 degrees 35 degrees degrees degrees degrees Incident angle 23 degrees 38.7 degrees degrees degrees degrees Swap width 100 km 75 km km km km Azimuth resolution 30 m 18 m (3 looks) m m m (2 looks) m (multi looks) Range resolution 18 m m Peak Power 4.8 kW 325 W (1.3 kW spec) 5 kW 1.4 kW 2.3 kW Bandwidth 19 MHz 15 MHz 11.6/17.3/30.0 MHz MHz 14 MHz/28MHz Antenna size 1 x 10 m 2.2 x 12 m 1.5 x 15 m 1.3 x 10 m 3.1 x 8.9 m

22 wave illuminating pattern
Basic Theory of SAR : Antenna wave illuminating pattern L=11.92 m b=2.2 m ‘half value’ JERS-1 SAR antenna b : antenna length in range direction L : antenna length in azimuth direction a : half value in range direction (JERS-1 : 5.3o) b : half value in azimuth direction (JERS-1 : 1.0o)

23 Basic Theory of SAR : Antenna
sensor/antenna L P1 P0 side lobe main lobe b0 1 1/2 y x z b a0 Definition of half value : Po : power in the center of main lobe P1 : power in the peripheral of main lobe The half value is defined by ‘P1 is attenuated to 3 dB (equally 50%) of Po’. 10log10Po/P1=3 dB or P1=0.5P0

24 Basic Theory of SAR : Radar Equation
To realize the relationship between radar received power and characteristic of scatterer. A : effective surface of the receiver’s antenna G : gain : radar cross section or back scatterer surface Pt : transmitted power Ps : scattered power Pr : received power Pr=PsA/4pR2 Ps=PtG/4pR2s Pt antenna R attenuation by spreading of wave = 1/4pR2 PtG/4pR2 Scatterer Pr=Ps A/4pR2=PtGAs/(4pR2)2

25 peak power×pulse width
Pulse radar Pulse power (Transmitted power) || peak power×pulse width sensor / antenna 22 20 1 21 18 2 19 17 20 3 18 16 19 4 17 5 JERS-1 SAR antenna 15 18 16 6 17 14 15 7 propagation of transmitted pulse 16 13 8 14 15 9 12 13 Rn : slant range length at near range Rf : slant range length at far range Time to receive the pulse by antenna : Near range side (start to receive) : 2Rn/C Far range side (end of receiving) : 2Rf/C+τ Continuity time of received pulse : T=(2Rf /C+τ)-2Rn/C 14 10 11 12 13 11 10 11 12 12 Rn tree house Rf concrete building (a)Pulse front wave Transmitted pulse received signal concrete building’s echo Signal intensity house’s echo tree’s echo time Pulse width τ (b)Time flows of transmit & received signal

26 Flowchart of SAR Signal Processing
Start Parameter calculation Doppler center frequency Range compression Corner turn Azimuth compression Output image

27 range compressed image azimuth compressed image
Flowchart of SAR Signal Processing Range JERS-1 satellite Azimuth corner turn North raw data range compressed image North sensor illumination azimuth compressed image rotated image

28 A B A B

29 DR ct q q earth’s surface q Dx

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31 frequency MHz 1282.5 1275.0 Df=15 MHz 1267.5

32 1/Df 1/Df time t t reference signal output signal time
pulse length (t) A B C transmitted pulse received pulse time t t reference signal output signal 1/Df time A B C 1/Df

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35 L b=l/L R P d

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40 Az Az t=0 t=0 R R Az t=0 R

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42 R Az

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55 Multi scattering length 3.910m (a) bridge’s architecture figure 2 1
Akasikaikyo bridge ( length 3.910m (a) bridge’s architecture figure 2 1 (b) SAR image’s signature 1 2 wire sea surface (c) scattering mechanism

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