Synthetic Aperture Radar and Sonar SAR and SAS

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Synthetic Aperture Radar and Sonar SAR and SAS Sverre Holm DEPARTMENT OF INFORMATICS 1

SAR Resolution Real aperture beamwidth: θ λ/d Size of footprint: L F θ R= R λ/d Size of synthetic aperture = footprint: L s L F Beamwidth of synthetic aperture:θ s =(1/2) λ/l s =(1/2) λ/(rλ/d)=d/(2r) Ground resolution: ΔX s = Rθ s =D/2 DEPARTMENT OF INFORMATICS 2

SAR Resolution Ground resolution: ΔX s =Rθ s =D/2 Note: The smaller the real antenna, the better the resolution Resolution is independent of range Why? A small D causes the synthetic aperture to be larger But, small D means energy is spread over larger area, so SNR suffers Range resolution: ΔX r =ct/2=c/2b - as in any pulsed system DEPARTMENT OF INFORMATICS 3

SAR Doppler Interpretation Doppler equation: f D =2 v/c f 0 sinθ Max Dopplershift: f D =2 v/c f 0 sinθ/2 2 v/c f 0 θ/2 =v/c c/λ λ/d=v/d Doppler bandwidth: B D =2 f D Time resolution: t m =1/B D =D/2v Equivalent azimuth resolution: X a =v t m =D/2 QED! Same result as found from aperture-resolution considerations http://www2.jpl.nasa.gov/basics/bsf12-1.html DEPARTMENT OF INFORMATICS 4

SAR Doppler - Sampling Doppler shift is in the range +/- f D Proper complex sampling with PRF>2f D =2v/D Max movement of aperture per pulse: x=v T=v/PRF=D/2 Gough & Hawkins, IEEE JOE, Jan 1997 claim that there should be no more than D/4 between pulses Element beamwidth/doppler bandwidth is not easily defined:»d/4 null-to-null sinc bw»d/2 3dB. A question of acceptable level of azimuth ambiguity DEPARTMENT OF INFORMATICS 5

Satellite SAR: ERS-1 (1991-2000) Satellite the simplest SAR Real aperture: D=10 m Frequency: 5.3 GHz Wavelength: λ=5.66 cm Height: R=850 km Real aperture beamwidth: θ=λ/d=0.33º Real aperture azimuth resolution = synthetic aperture: L s =λ/d R=4850 m SAR resolution: D/2=5 m B=19 MHz => Range res 8m Velocity: v=7 km/sec <http://www.sso.admin.ch/themes/02-earth_observation/english/ e_03_esa_missions_in_orbit.htm> DEPARTMENT OF INFORMATICS 6

ERS-1 SAR image of west coast of Norway, 22 June 1996. http://marsais.nersc.no/product_wind.html DEPARTMENT OF INFORMATICS 7

Focused unfocused SAR Small synthetic aperture => straight lines of constant delay => no focusing required Nearfield-farfield limit: R f =L s2 /(4 λ) Largest unfocused synthetic aperture for R=R f =>L s =2(Rλ) 0.5 ERS-1: L s =439 m < 4850 m Focusing is required in order to obtain full resolution DEPARTMENT OF INFORMATICS 8

Sampling considerations Fast enough for Doppler no grating lobes: PRF>2v/D Simple radar, only one pulse in medium at a time 1/PRF > 2R/c i.e. 2v/D < PRF < c/2r Swath width < R such as in satellite SAR => Several pulses in medium at a time No sampling while tx No sampling during subsatellite echo DEPARTMENT OF INFORMATICS 9

SAR coverage DEPARTMENT OF INFORMATICS 10

Aircraft SAR Real aperture: D=1 m Frequency: 5.3 GHz Wavelength: λ=5.7 cm Height: R=10 km Real aperture beamwidth: θ=λ/d=3.3º Real aperture azimuth resolution = Synthetic aperture: L s =λ/d R=570 m SAR resolution: D/2=0.5 m v=720 km/hr = 200 m/s (Some guesses) DEPARTMENT OF INFORMATICS 11

Synthetic aperture sonar: Hugin Height: R = typ 20 m, speed: v = typ 2 m/s FFI & Kongsberg Maritime DEPARTMENT OF INFORMATICS 12

Real aperture synthetic aperture Tx element Rx element Tx element Rx element SAR Tx element Rx element SAS like seismics Real aperture all rx/tx combinations DEPARTMENT OF INFORMATICS 13

Hugin Edgetech: Rx: 6 x 20 cm (6 x 17λ) Tx: 1 rx element f = 125 khz, λ= 1.2 cm Bandwidth B=15 khz Synthetic aperture: L s =λ/d R=(0.012/0.2) 20 =1.2m SAR resolution: 10 cm Range resolution: 5 cm Sensotek: Rx: 1.5 m, 96 elements Tx: effectively 1.5λx1.5λ (larger defocused aperture to increase power) f=60-120, typ 90 khz, λ= 1.67 cm Bandwidth, typ. B=30 khz Synthetic aperture: L s =λ/d R=(1/1.5) 20 13m SAR resolution: 1.25 cm Range resolution: 2.5 cm DEPARTMENT OF INFORMATICS 14

SAR vs SAS Criterion for not creating increased sidelobe level: position known to λ/16 Satellite ERS-1, λ=5.7 cm L s = 4850 m, v = 7 km/s => 0.7 sec Must know position within 3.5 mm over 0.7 sec Aircraft SAR, λ=5.7 cm L s = 570 m, v = 200 m/s => 2.85 sec Must know position within 3.5 mm over 2.85 sec Sonar Hugin: Edgetech λ=1.2 cm, L s = 1,2 m, v = 2 m/s => 0.6 sec Must know position within 0.75 mm over 0.6 sec Sensotek λ=1.7 cm, L s = 13 m, v = 2 m/s => 6.5 sec Must know position within 1 mm over 6.5 sec! DEPARTMENT OF INFORMATICS 15

SAR vs SAS: c=3 10 8 vs 1500 m/s Motion compensation: much more severe for sonar as it takes much longer to travel one synthetic aperture => accurate navigation and micronavigation (sub λ accuracy) More severe range ambiguity problem for sonar than radar. Harder to achieve good mapping rate => multielement rx arrays which also can be used for DPCA (displaced phasecenter antenna) micronavigation Noise: SAR thermal/electronic noise, SAS noisy medium Medium: Sonar multipath, refraction, instability, attenuation; Radar much more stable, only spherical spreading loss Same range resolution for smaller bandwidth in SAS than SAR: ΔX r =c/2b DEPARTMENT OF INFORMATICS 16

Interferometry Compare two images at slightly different aspects Requires image with amplitude and phase Dual-pass: Satellite SAR Single-pass, requires two imaging systems Aircraft SAR, SAS Ellery Creek floodplain, http://www.csr.utexas.edu/rs/research/aussie/finke_flood.html DEPARTMENT OF INFORMATICS 17

Imaging modes Strip-map ( standard mode ) Spotlight mode (figure) Squint mode http://www.terrasar.de/en/prod/img_prod/hs/index.php DEPARTMENT OF INFORMATICS 18

Literature A. Currie: Synthetic aperture radar, August 1991. Electronics & Communication Engineering Journal. Cutrona, L.J., Comparison of sonar system performance achievable using synthetic-aperture techniques with the performance achievable by more conventional means, J. Acoust. Soc. Amer., Vol.58, No.2, pp336-348, Aug. 1975. H D Griffiths: Synthetic aperture imaging with sonar and radar: A comparison, World Congress on Ultrasonics, Paris 2003. M.P. Hayes and P.T. Gough, Synthetic aperture sonar: A maturing discipline, Proc 7. Eur. Conf Underwater Acoustics, Netherlands, July, 2004 DEPARTMENT OF INFORMATICS 19