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How does InSAR work?
Gareth Funning
University of California, Riverside
Outline
• Basics of SAR and InSAR
• Application to earthquakes, and other examples
• Limitations
• The future
InSAR
Interferometric
Synthetic
Aperture
Radar
pretend you have a big radar
antenna
use wave interference
emit microwaves, measure echoes
SAR: how it works
1. Satellite emits radar pulse
2. Radar is backscattered
3. Amplitude and phase of echo
recorded at the satellite
flight direction
5 km
flight direction
flight direction
synthetic
aperture
(5 km instead
of 10 m!)
resolution 20 m
instead of 5 km!
• SAR imaging uses amplitude (intensity)
of backscattered echoes
• Radar sees through clouds—all-
weather imaging is possible
• Don’t need illumination by the Sun—
can image day and night
• Surface roughness and slopes control
the strength of the backscatter
• Applications: ship tracks, ice tracking,
oil slicks, land-use changes, planetary
JPL
Kilauea caldera, Hawaii
JPL
Slopes facing toward
satellite have bright
backscatter
Slopes facing away
from satellite show
dark backscatter
and/or shadowing
Flightdirection
Look direction
Kilauea caldera, Hawaii
JPL
Areas of vegetation are
“rough” and have
bright backscatter
Sedimentary drainages are
comparatively smooth and
have less backscatter
What about the phase?
~780 km
~6 cm
Phase is a function of the distance
from the satellite to the ground.
ERS-1
Pass 1 Pass 2
InSAR: How it works
Pass 1: pre-movement Pass 2: post-movement
phase shift due to
ground motion
phase=1 phase=2
InSAR: How it works
phase shift varies with
distance from the fault
InSAR: How it works
Image A - 12 August 1999
Image B - 16 September 1999
Interferogram =
Phase A - Phase B
Remove phase from
topography
satellite positions
earth curvature
Tim Wright
amplitude phase
(0) 0 mm range change
(-1) 28 mm range decrease
(-2) 57 mm range decrease
(-10) 283 mm range decrease
(-20) 567 mm range decrease
17 August 1999, Izmit earthquake (Turkey)
Tim Wright
A’
A
17 August 1999, Izmit earthquake (Turkey)
Tim Wright
10 km
2008 Wells, Nevada
Each cycle of
blue => yellow => red
= 28 mm of displacement
(half of the radar wavelength)
away from the satellite
data model data – model
Weston et al., 2012
Strike: 172°
Dip: 38°
Rake: –95°
Mw: 6.06
“wrapped” “unwrapped”
50 km
Original unwrapped data
Downsampling
Optimization
Slip model
-1.3
1.3
Disp (m)
0
Schmidt and Burgmann (2003)
Pritchard and Simons (2004) Wdowinski et al (2006)
Los Angeles
time span = 1 day
July 1992–March 1993 February 1993–March 1993
Snow!Atmosphere!
Decorrelation
• Changes in radar scattering properties of pixels
• Vegetation, snow, flooding, the passing of time…
• Longer radar wavelengths less susceptible
Atmospheric “noise”
• Refraction of microwaves by water vapor
• “Static” part can resemble topography
• “Turbulent” part can resemble deformation
Sentinel
12 (and then 6) day repeat in same orbit
mean post event wait => 3 days
ascending + descending => mean wait < 3 days
SENTINEL-1A and -1B
European Space Agency
Launch Q2 2014, 2016
ALOS-2 by Japanese Aerospace Exploration Agency
14-day repeat in same orbit
23 cm wavelength – less decorrelation
Launched Summer 2014

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Presentation on the background theory of InSAR

  • 1. How does InSAR work? Gareth Funning University of California, Riverside
  • 2. Outline • Basics of SAR and InSAR • Application to earthquakes, and other examples • Limitations • The future
  • 3. InSAR Interferometric Synthetic Aperture Radar pretend you have a big radar antenna use wave interference emit microwaves, measure echoes
  • 4. SAR: how it works 1. Satellite emits radar pulse 2. Radar is backscattered 3. Amplitude and phase of echo recorded at the satellite
  • 7. flight direction synthetic aperture (5 km instead of 10 m!) resolution 20 m instead of 5 km!
  • 8. • SAR imaging uses amplitude (intensity) of backscattered echoes • Radar sees through clouds—all- weather imaging is possible • Don’t need illumination by the Sun— can image day and night • Surface roughness and slopes control the strength of the backscatter • Applications: ship tracks, ice tracking, oil slicks, land-use changes, planetary JPL
  • 9. Kilauea caldera, Hawaii JPL Slopes facing toward satellite have bright backscatter Slopes facing away from satellite show dark backscatter and/or shadowing Flightdirection Look direction
  • 10. Kilauea caldera, Hawaii JPL Areas of vegetation are “rough” and have bright backscatter Sedimentary drainages are comparatively smooth and have less backscatter
  • 11. What about the phase? ~780 km ~6 cm Phase is a function of the distance from the satellite to the ground. ERS-1
  • 12. Pass 1 Pass 2 InSAR: How it works
  • 13. Pass 1: pre-movement Pass 2: post-movement phase shift due to ground motion phase=1 phase=2 InSAR: How it works
  • 14. phase shift varies with distance from the fault InSAR: How it works
  • 15. Image A - 12 August 1999 Image B - 16 September 1999 Interferogram = Phase A - Phase B Remove phase from topography satellite positions earth curvature Tim Wright amplitude phase
  • 16. (0) 0 mm range change (-1) 28 mm range decrease (-2) 57 mm range decrease (-10) 283 mm range decrease (-20) 567 mm range decrease 17 August 1999, Izmit earthquake (Turkey) Tim Wright
  • 17. A’ A 17 August 1999, Izmit earthquake (Turkey) Tim Wright
  • 18. 10 km 2008 Wells, Nevada Each cycle of blue => yellow => red = 28 mm of displacement (half of the radar wavelength) away from the satellite
  • 19. data model data – model Weston et al., 2012 Strike: 172° Dip: 38° Rake: –95° Mw: 6.06
  • 21. 50 km Original unwrapped data Downsampling Optimization Slip model -1.3 1.3 Disp (m) 0
  • 22. Schmidt and Burgmann (2003) Pritchard and Simons (2004) Wdowinski et al (2006)
  • 24. July 1992–March 1993 February 1993–March 1993 Snow!Atmosphere!
  • 25. Decorrelation • Changes in radar scattering properties of pixels • Vegetation, snow, flooding, the passing of time… • Longer radar wavelengths less susceptible Atmospheric “noise” • Refraction of microwaves by water vapor • “Static” part can resemble topography • “Turbulent” part can resemble deformation
  • 26. Sentinel 12 (and then 6) day repeat in same orbit mean post event wait => 3 days ascending + descending => mean wait < 3 days SENTINEL-1A and -1B European Space Agency Launch Q2 2014, 2016
  • 27. ALOS-2 by Japanese Aerospace Exploration Agency 14-day repeat in same orbit 23 cm wavelength – less decorrelation Launched Summer 2014