SAR Training Course, MCST, Kalkara, Malta, November SAR Maritime Applications. History and Basics

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SAR Maritime Applications History and Basics Martin Gade Uni Hamburg, Institut für Meereskunde

SAR Maritime Applications Thursday, 13 Nov.: 1 - History & Basics Introduction Radar/SAR History Basics Scatterometer 2 - Wind and Waves SAR Wind Fields Storms, Tropical Cyclones Ocean Surface Waves Oceanic Internal Waves Marine Surface Films Rain Friday, 14 Nov.: 3 - Currents and Objects Surface Currents Sea Bottom Topography Ship Detection Oil Pollution Monitoring Sea Ice Intertidal Flats 4 - Exercises NEST 5: Calibration, Georeferencing, Wind Fields, Oil Pollution, Radar Contrast, Statistics Martin Gade - SAR Maritime Applications - 1 - Basics & History 2

SAR History Martin Gade - SAR Maritime Applications - 1 - Basics & History 3

Radar History 1864 J.C. Maxwell: EM Field, Maxwell Equations 1885-88 H. Hertz: classical experiments with radio waves (455 MHz) 1900s C. Hülsmeyer: first monostatic pulse radar 1919 R.A. Watson-Watt: patent for radio detection of objects 1922 S.G. Marconi: radio detection of targets A.H. Taylor & L.C. Young: detection of wooden ship on Potomac river 1930s 1940s 1950s after radar rediscovered in frame of pre-wwii armament operational military radar to detect bigger ships and aircraft (bombers) independent research in Germany, U.K., U.S., Italy, USSR, France, Japan, Netherlands microwave magnetron (higher frequencies = smaller antennas) military applications during WWII and shortly after Doppler radar Synthetic Aperture Radar (SAR) invented at Goodyear Aircraft Corporation Pulse compression Phased array antenna Growing civil and scientific applications Digital signal processing Martin Gade - SAR Maritime Applications - 1 - Basics & History 4

Radar Basics Band Designation Nominal Frequency Range Specific Frequency Range (ITU) HF Absorption of EM Waves in the Atmosphere 3-30 MHz VHF 30-300 MHz 138-144 MHz 216-225 MHz UHF 300-1000 MHz 420 450 MHz 850 942 MHz L 1 2 GHz 1215 1400 MHz S 2 4 GHz 2300 2500 MHz 2700 3700 MHz C 4 8 GHz 5250 5925 MHz X 8 12 GHz 8500 10680 MHz Ku 12 18 GHz 13.4 14.0 GHz 15.7 17.7 GHz K 18 27 GHz 24.05 24.25 GHz Ka 27 40 GHz 33.4 36 GHz V 40 75 GHz 59 64 GHz W 75 110 GHz 76 81 GHz 92 100 GHz mm 110 300 GHz 126 142 GHz 144 149 GHz 231 235 GHz 238 248 GHz [Skolnik, 2001] Martin Gade - SAR Maritime Applications - 1 - Basics & History 5

SAR History 1951 C. Wiley (Goodyear): Postulation of Doppler beam-sharpening concept 1952 Beam-sharpening concept demonstrated at U Illinois 1957 First SAR imagery (U Michigan; optical correlator) 1964 Analog electronic SAR correlation (U Michigan) 1969 Digital electronic SAR correlation (Hughes, Goodyear, Westinghouse) 1972 Real-time digital SAR demonstrated; motion compensation (aircraft systems) 1978 Spaceborne SAR aboard SEASAT (analog downlink, optical processing, non-real time) 1981 Shuttle Imaging Radar (SIR) -A (optical processing on ground, non-real time) 1984 SIR-B (digital downlink, digital processing, non-real time) 1986 Spaceborne SAR real-time processing (JPL) 1987 Soviet 1870 SAR 1990 Magellan SAR imagery of Venus > 1990 More spaceborne SAR sensors in orbit Martin Gade - SAR Maritime Applications - 1 - Basics & History 6

Spaceborne SAR History Absorption of EM Waves in the Atmosphere Year Satellite Band Incid.Angle Polarization 1978 SEASAT (USA) L (1.3 GHz) 23 HH 1981 SIR-A (USA) L (1.3 GHz) 50 HH 1984 SIR-B (USA) L (1.3 GHz) 15-65 HH 1991 ERS-1 (Europe) C (5.3 GHz) 23 VV 1991 ALMAZ-1 (USSR) S (3.0 GHz) 30-60 HH 1992 JERS-1 (Japan) L (1.3 GHz) 39 HH 1994 SIR-C/X-SAR (USA, Germany) L (1.3 GHz), C (5.3 GHz), X (9.6 GHz) 15-55 1995 ERS-2 (Europe) C (5.3 GHz) 23 VV 1995 Radarsat-1 (Canada) C (5.3 GHz) 20-50 HH HH, HV, VV, VH (SIR-C), VV (X-SAR) 2000 SRTM (USA, Germany) C (5.3 GHz), X (9.6 GHz) 54 HH, VV (C), VV (X) 2002 ENVISAT (Europe) C (5.3 GHz) 15-45 HH, HV, VV, VH 2006 ALOS-1 (Japan) L (1.3 GHz) 8-60 HH, HV, VV, VH 2007 TerraSAR-X (Germany) X (9.7 GHz) 15-60 HH, HV, VV, VH 2007 Radarsat-2 (Canada) C (5.3 GHz) 10-60 HH, HV, VV, VH 2007-10 COSMO-SkyMed 1-4 (Italy) X (9.6 GHz) 20-59 HH, HV, VV, VH 2010 TanDEM-X (Germany) X (9.7 GHz) 15-60 HH, HV, VV, VH 2014 ALOS-2 (Japan) L (1.3 GHz) 8-70 HH, HV, VV, VH 2014 Sentinel-1A (Europe) C (5.4 GHz) 20-45 HH-HV, VV-VH Martin Gade - SAR Maritime Applications - 1 - Basics & History 7

Spaceborne SARs Seasat (1978) ERS-1/2 (1991/1995) SIR-C/X-SAR (1994) RADARSAT-1 (1995) ENVISAT (2002) ALOS-1 (2006) TerraSAR/TanDEM-X (2007/10) RADARSAT-2 (2007) ALOS-2 (2014) Cosmo Skymed 1-4 (2007-10) Sentinel-1A (2014) more SARs on, e.g., Indian, Chinese, German, Russian satellites Martin Gade - SAR Maritime Applications - 1 - Basics & History 8

SAR History Take-Home Messages SAR ~ 60 years 1978 Seasat >1991 continuous spaceborne SAR Martin Gade - SAR Maritime Applications - 1 - Basics & History 9

Some Basics Martin Gade - SAR Maritime Applications - 1 - Basics & History 10

Basics Absorption / Transmission / Scattering a b ink milk ink milk [Petty, 2006] Martin Gade - SAR Maritime Applications - 1 - Basics & History 11

Basics Absorption of e/m waves in the atmosphere [Kappas, 1994] Martin Gade - SAR Maritime Applications - 1 - Basics & History 12

Microwave Basics Complex dielectric constant of pure and sea water (32.45 ) Real part (permittivity), ε w Imaginary part (loss factor), ε w [Jackson & Apel, 2004] Complex dielectric constant, ε c = ε - iε : response to electromagnetic field Loss tangent, tan δ = ε /ε : good (tan δ>>1) or poor (tan δ<<1) conductor Martin Gade - SAR Maritime Applications - 1 - Basics & History 13

Microwave Basics Penetration depth into water (1) Plane wave propagation in lossy media, along direction ζ : e iκζ = e βζ+iαζ with attenuation coefficient β: β = 2π I ε λ 0 Penetration depth δ = 1/β: depth, at which power is reduced by e -2. [Swift, 1980] Martin Gade - SAR Maritime Applications - 1 - Basics & History 14

Microwave Basics Penetration depth into water (2) Penetration depth depends on dielectric properties of sea water and radar wavelength, f R = 1.43 GHz Dielectric properties depend on salinity and temperature [Swift, 1980] Martin Gade - SAR Maritime Applications - 1 - Basics & History 15

Microwave Basics Surface scattering mechanisms INCIDENT WAVE REFLECTED WAVE SMOOTH SURFACE BACK SCATTERED COMPONENT SLIGHTLY ROUGH SURFACE ROUGH SURFACE [Barale & Gade, 2008] Martin Gade - SAR Maritime Applications - 1 - Basics & History 16

Wind-Wave Tank of the University of Hamburg UHH s Wind-Wave Tank Size: 24 m 1 m 1.5 m Water depth: 0.5 m (freshwater) Wind: 2 20 m/s Rain: up to 160 mm/h @ 12.5 14.8 m Martin Gade - SAR Maritime Applications - 1 - Basics & History 17

Wind-Roughened Water Surface Martin Gade - SAR Maritime Applications - 1 - Basics & History 18

Microwave Basics Radar backscattering at the sea surface (a) (b) (c) specular Bragg edges & shadowing [Robinson, 2003] Martin Gade - SAR Maritime Applications - 1 - Basics & History 19

Microwave Basics Bragg Scattering [Jackson & Apel, 2004] k B = 2k r sin θ = 4π sin θ λ r Martin Gade - SAR Maritime Applications - 1 - Basics & History 20

Microwave Basics Bragg Scattering L : 1.25 GHz S : 2.40 GHz C : 5.30 GHz X : 10.0 GHz K u : 15.0 GHz k B = 2k r sin θ = 4π sin θ λ r Martin Gade - SAR Maritime Applications - 1 - Basics & History 21

Microwave Basics Bragg Scattering σ 0 = 8πk e 4 cos 4 θ 0 b pp (θ 0 ) 2 Ψ k B + Ψ( k B ) k e : electromagnetic wavenumber θ 0 : nominal incidence angle (20.. 70 ) Ψ(k) : waveheight spectrum Bragg wavenumber k B = 2k e sin θ 0 Polarization coefficients b HH = ε cos θ 0 + ε 2 ; b VV = ε2 1+sin2 θ 0 ε cos θ 0 + ε 2 [Wright, 1968] Martin Gade - SAR Maritime Applications - 1 - Basics & History 22

Geophysical Model Functions Dependence between radar cross section and wind speed and direction σ 0 = A(f, p, θ) U γ(f,p,θ) 1 + B(f, p, θ) cos χ + C f, p, θ cos2χ with f : radar frequency p : radar polarization θ : incidence angle U : wind speed (usually at 10m height) χ : azimuth angle Martin Gade - SAR Maritime Applications - 1 - Basics & History 23

Geophysical Model Functions Measuring wind speed and direction [Robinson, 2003] Martin Gade - SAR Maritime Applications - 1 - Basics & History 24

Geophysical Model Functions Measuring wind speed and direction [Jackson and Apel, 2004] Martin Gade - SAR Maritime Applications - 1 - Basics & History 25

Excursion: Scatterometer Martin Gade - SAR Maritime Applications - 1 - Basics & History 26

Scatterometer Scatterometers aboard satellites ERS-1/2 (1991 / 1995) Seasat (1978) QuikScat (1999) MetOp-A/B (2006 / 2012) Oceansat-2 (2009) Martin Gade - SAR Maritime Applications - 1 - Basics & History 27

Scatterometer One single day of Oceansat-2 NRCS (HH) Martin Gade - SAR Maritime Applications - 1 - Basics & History 28

Scatterometer One single day of Oceansat-2 NRCS (VV) Martin Gade - SAR Maritime Applications - 1 - Basics & History 29

Scatterometer Measurement principle [Robinson, 2003] Martin Gade - SAR Maritime Applications - 1 - Basics & History 30

Scatterometer Measurement principle [Robinson, 2003] Martin Gade - SAR Maritime Applications - 1 - Basics & History 31

Scatterometer Measurement principle, ERS Scat [Robinson, 2003] Martin Gade - SAR Maritime Applications - 1 - Basics & History 32

Scatterometer Measurement principle, ASCAT (MetOp) [Eumetsat] Martin Gade - SAR Maritime Applications - 1 - Basics & History 33

Scatterometer Measurement principle, Seawinds (QuikScat, OSCAT) [Robinson, 2003] Martin Gade - SAR Maritime Applications - 1 - Basics & History 34

Scatterometer One single orbit of Oceansat-2 winds Martin Gade - SAR Maritime Applications - 1 - Basics & History 35

Scatterometer One single day of Oceansat-2 winds (descending) Martin Gade - SAR Maritime Applications - 1 - Basics & History 36

back to Radar & SAR Martin Gade - SAR Maritime Applications - 1 - Basics & History 37

Radar Backscattering from the Sea Surface Tilt and hydrodynamic modulation [Robinson, 2003] Martin Gade - SAR Maritime Applications - 1 - Basics & History 38

Ocean Waves Orbital motion of long ocean waves [NOAA] [Jackson & Apel, 2004] Martin Gade - SAR Maritime Applications - 1 - Basics & History 39

Radar Backscattering from the Sea Surface Tilt and hydrodynamic modulation [Jackson & Apel, 2004] Martin Gade - SAR Maritime Applications - 1 - Basics & History 40

Three-Scale Model [Plant, 2002] Martin Gade - SAR Maritime Applications - 1 - Basics & History 41

Radar Doppler Spectra Scatterometer experiments with upwind looking antenna dashed, circles: VV dashed-dotted, crosses: HH solid, pluses: acoustic [Plant et al., 2004] Martin Gade - SAR Maritime Applications - 1 - Basics & History 42

Radar Doppler Spectra Scatterometer experiments with downwind looking antenna dashed, circles: VV dashed-dotted, crosses: HH solid, pluses: acoustic [Plant et al., 2004] Martin Gade - SAR Maritime Applications - 1 - Basics & History 43

SAR Definitions [Robinson, 2003] Martin Gade - SAR Maritime Applications - 1 - Basics & History 44

SAR Artifacts Foreshortening [ESA] Martin Gade - SAR Maritime Applications - 1 - Basics & History 45

SAR Artifacts Azimuthal shift ( Ship-off-the-Wake Effect ) [Mallas & Graber, 2013] Martin Gade - SAR Maritime Applications - 1 - Basics & History 46

SAR Artifacts Velocity bunching [Robinson, 2003] Propagation direction of the ocean waves is important! [Jackson and Apel, 2004] Martin Gade - SAR Maritime Applications - 1 - Basics & History 47

Ocean Features on SAR Imagery Feature Scale Derived Measurement Imaging Mechanism Wind Speed Range [m s -1 ] Characteristics and Considerations Surface Waves 100-600 m wavelength Wavelength Propagation direction Wave height Tilt Hydrodynamic Velocity Bunching 3 40 Azimuth-traveling waves may be nonlinear without correction. Other limiting factors include wavelength, wave height and fetch. Internal Waves 0.3-3 km wavelength Wavelength Direction Amplitude Mixed layer depth Convergence/Divergence Surfactants 2 10 Curvilinear packets with multiple waves, decreasing wavelength from front to back. Sensitive to wind conditions, wave crest orientation to platform. Internal Tides 10-20 km Wavelength Direction Interaction of centimeter Waves/Currents/Surfactants 3 7 Currents and Fronts 1-100 km Location Shear Strain Velocity Shear/Convergence Convergence Wind stress Surfactants 3-10 3-10 3-10 3 7 Sensitive to wind conditions. Often multiple mechanisms present simultaneously. Eddies 1-200 km diameter Location and source Diameter Velocity Shear Strain Shear/Convergence Wind Stress Surfactants 3-10 3-10 3 7 Sensitive to wind conditions. Often multiple mechanisms present simultaneously. Shallow Water Bathymetry 5-50 m depth Location/change detection Current velocity Depth Convergence 3-12 Sensitive to wind, current properties, depth. [Jackson & Apel, 2004] Martin Gade - SAR Maritime Applications - 1 - Basics & History 48

Air-Sea Interactions on SAR Imagery Feature Scale Derived Measurement Imaging Mechanism Wind Speed Range [m s -1 ] Characteristics and Considerations Surface Winds > 1km grid Wind speed Wind direction Wind stress Indirectly via windrows, models, or sensors 3 25 For mesoscale, coastal variability. Requires good calibration. Roll Vortices 1-5 km wavelength Boundary Layer: Stratification Wind stress 3 15 Long axis/crests parallel to wind direction. Gravity Waves 2-10 km wavelength Height Turbulence spectrum Drag coefficient Wind stress 3 15 Long axis/crests perpendicular to wind direction, often associated with topography Rain Cells 2-40 km diameter Rain rate Wind stress Rain damping 3-15 Appearance sensitive to frequency, rain rate, wind speed. [Jackson & Apel, 2004] Martin Gade - SAR Maritime Applications - 1 - Basics & History 49

Surface Films on SAR Imagery Feature Scale Derived Measurement Imaging Mechanism Wind Speed Range [m s -1 ] Characteristics and Considerations Biogenic Surfactants > 100m² area Areal extent Convergence 2 8 Both forms have signatures similar to low wind, cold thermal water masses, etc. Mineral Oils > 100m² area Areal extent Seeps Ship discharge Run-off 3 15 Wind speed, combination of L- and C-/Xbands may enable discrimination of each form. [Jackson & Apel, 2004] Martin Gade - SAR Maritime Applications - 1 - Basics & History 50

Some Basics Take-Home Messages Radar backscattering from water surface Bragg scattering surface roughness important GMF: wind-speed dependence Martin Gade - SAR Maritime Applications - 1 - Basics & History 51

Martin Gade - SAR Maritime Applications - 1 - Basics & History 52

to be continued Martin Gade - SAR Maritime Applications - 1 - Basics & History 53