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Cassini Radar
Exploring Titan
Contents
● Introduction
● Cassini Radar system
● BIDR product overview
● Surface of Titan
● Conclusion
Introduction
● Cassini spacecraft launched 1997
● Saturn orbiter 2004-07-01
●
Hugyens on Titan 2005-01-14
● Multiple missions
– Saturn, heliosphere, testing relativity
– Icy moons, Saturn's rings, etc.
– Enceladus jets and subsurface ocean
● 10+ years of orbiting Saturn
– 2017 Solstice (dunes moving at equinox season)
The Cassini Radar System
High-Gain
Antenna (HGA)
The Cassini Radar System
● Wavelength is 13.78 GHz (Ku-band)
● Synthetic Aperture Radar Imager
– 0.35 to 1.7 km
● Altimeter
– 24 to 27 km horizontal
– 90 to 150 m vertical
● Radiometer
– Passive
– 7 to 310 km
Mastrogiuseppe (2014)
Modes of operation
● Imaging:
– Timing pulses at many incidence angles
● Altimeter:
– Single focus pulse timing
● Backscatter:
– Returned intensity gives surface properties
● Radiometer:
– Emitted noise from Titan atmosphere (calib)
Types of RADAR modes
From Thesis of Lauren Wye (2011)
Synthetic Aperture Radar
● Doppler-Shifted (DS) signal frequency
– Relative motion of HGA & Titan surface
● “Focusing” uses two DS states of object
– Higher frequency if moving closer
– Lower frequency if moving apart
– Illumination of target point isolated
● Synthetic Aperture
– “Virtual length” of antenna
– Relative velocity displacement
The monostatic radar equation
If Tx and Rx are collocated (same fixed antenna), then:
Pt
total transmitted power (48.084 W),
Gt
on-axis antenna gain (50.7 dB),
Ar
effective aperture area of the receiving antenna (4.43 m2
)
R distance (range) between the radar and the target
Ps
= Pr
− Pn
Ps
received echo signal power
Pr
total received power
Pn
mean noise power
From Wye (2011)
With the effective antenna
aperture Ar = λ2Gt / 4π
Transmitted power, interception
● PtGt is the Transmitted energy
– Isotropic spherical wave
– Spherical spreading loss (1 / 4πR2)
– Attenuation sphere has radius R
● Interception on target surface by σ
– Energy absorption
– Energy isotropically re-radiated
– Spherical spreading loss (1 / 4πR2)
● Reception by the Antenna
From Wye (2011)
Radar Cross-Section (σ)
● Inherent property of the target, units are m2
● Reflectivity
– dielectric properties
● Directivity
– physical structure (size, shape)
– at scales relative to the illuminating wavelength
● Other parameters
– illuminating wavelength
– viewing geometry
– polarization configuration
Proper characterization of the RCS’s response
to incidence and azimuth angle variation
helps to eliminate the viewing geometry dependence
From Wye (2011)
Pulses
● N ~ 50 for SAR
● Interpulse separation
– Not possible at high incidence angle
– Impacts noise modeling → uncertainty
From Wye (2011)
Noise
● Mean noise power level
– receiver electronics thermal noise (mostly, Prec)
– received target radiation thermal noise (less, Pa)
● System noise power
– Psys = Prec + Pa
● The ideal receiver system
– large front-end gain
– receiver thermal noise power unaffected by any back-end gain changes
– In this scenario, Prec constant for a particular receiver bandwidth
– need to calculate the noise power once for each receiver filter
● Not the case in Cassini RADAR
BIDR products in PDS
● SAR image from a single Titan pass
● Raw processing a “formidable undertaking”
● PDS raster format
– IMG data file in binary format
– LBL metadata file in text format
– Imports in ISIS directly
Integrated Software
for Imagers & Spectrometers
● isis.astrogeology.usgs.gov
“Manipulate imagery collected by current and past NASA and
International planetary missions sent throughout our Solar System”
● Works in Linux & Mac
● Command Line Interface
pds2isis from=BIDR*.IMG to=out.cub
● Display, mosaick GUI
Ligeia Mare
Kraken Mare
Northern Lakes
Punga
Mare
T91
Kraken Mare
Small lakes
Kraken Mare
Mývatn Lacus
Oneida Lacus
Waikare Lacus
T91 Fly-By ISIS-GRASS
BIDR scales (F&D)
Kraken Mare main Peninsula
Ligeia Mare
Mechanical erosion
(Not chemical)
Black et al (2012)
Ligeia Mare Island
Mare characteristics (not only from BIDR)
● Strong specular reflection, no waves
- 1mm rms (Zebker et al., 2014)
● Extremely transparent (Mastrogiuseppe, 2014)
- Suspended particles < 0.1%
- 160 m maximum depth
Dissolution/Precipitation play? (personal thought)
Sub Equatorial Dunes
13% of Titan
Matured features
1.3km width
2.7km crest spacing
Hydrocarbon chains
>1m/s saltation
Equinox weather
Savage et al, (2014)
T95 Fly-By
ISIS-GRASS
Craters
● Wood et al. (2010)
– 5 confirmed craters, 44 potential (+ E Xanadu)
● Neish et al (2012)
– 5 confirmed > 20km diameter studied
– Eolian infill ? (see Forsberg-Taylor, 2004)
● Giliam & Jurdy (2014)
– Connection crater<>subsurface water
Menrva
(20.1°N 87.2°W)
Various Geological Features
● Lopes et al. . (2012)
– Hot cross bun from faults (38.5N, 203W)
● Stofan et al. (2008)
– South pole complex surface morphology (T39)
● Wood (2011)
– Caldera/Maar volcanism at the poles (?)
● More features recorded here:
https://en.wikipedia.org/wiki/List_of_geological_features_on_Titan
Maar: phreatovolcanism, explosive, often making lakes on Earth
Arcūs, Faculae, Fluctūs, Flumina, Insulae, Labyrinthi,
Large ring features, Maculae, Montes, Planitia, etc.
Conclusions
● SAR imaging on Cassini probe
● BIDR products explore surface of Titan
● Methane & Ethane circulation
● Eolian, evaporative, rain processes
● Seas, lakes, dunes, geomorphology
● Strange, fascinating World at 92 Kelvin
Thank you
Credit for half of the images:
NASA
clicops.org
& collaborators

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Cassini Radar Reveals Titan's Icy Surface

  • 2. Contents ● Introduction ● Cassini Radar system ● BIDR product overview ● Surface of Titan ● Conclusion
  • 3. Introduction ● Cassini spacecraft launched 1997 ● Saturn orbiter 2004-07-01 ● Hugyens on Titan 2005-01-14 ● Multiple missions – Saturn, heliosphere, testing relativity – Icy moons, Saturn's rings, etc. – Enceladus jets and subsurface ocean ● 10+ years of orbiting Saturn – 2017 Solstice (dunes moving at equinox season)
  • 4. The Cassini Radar System High-Gain Antenna (HGA)
  • 5. The Cassini Radar System ● Wavelength is 13.78 GHz (Ku-band) ● Synthetic Aperture Radar Imager – 0.35 to 1.7 km ● Altimeter – 24 to 27 km horizontal – 90 to 150 m vertical ● Radiometer – Passive – 7 to 310 km Mastrogiuseppe (2014)
  • 6. Modes of operation ● Imaging: – Timing pulses at many incidence angles ● Altimeter: – Single focus pulse timing ● Backscatter: – Returned intensity gives surface properties ● Radiometer: – Emitted noise from Titan atmosphere (calib)
  • 7. Types of RADAR modes From Thesis of Lauren Wye (2011)
  • 8. Synthetic Aperture Radar ● Doppler-Shifted (DS) signal frequency – Relative motion of HGA & Titan surface ● “Focusing” uses two DS states of object – Higher frequency if moving closer – Lower frequency if moving apart – Illumination of target point isolated ● Synthetic Aperture – “Virtual length” of antenna – Relative velocity displacement
  • 9. The monostatic radar equation If Tx and Rx are collocated (same fixed antenna), then: Pt total transmitted power (48.084 W), Gt on-axis antenna gain (50.7 dB), Ar effective aperture area of the receiving antenna (4.43 m2 ) R distance (range) between the radar and the target Ps = Pr − Pn Ps received echo signal power Pr total received power Pn mean noise power From Wye (2011) With the effective antenna aperture Ar = λ2Gt / 4π
  • 10. Transmitted power, interception ● PtGt is the Transmitted energy – Isotropic spherical wave – Spherical spreading loss (1 / 4πR2) – Attenuation sphere has radius R ● Interception on target surface by σ – Energy absorption – Energy isotropically re-radiated – Spherical spreading loss (1 / 4πR2) ● Reception by the Antenna From Wye (2011)
  • 11. Radar Cross-Section (σ) ● Inherent property of the target, units are m2 ● Reflectivity – dielectric properties ● Directivity – physical structure (size, shape) – at scales relative to the illuminating wavelength ● Other parameters – illuminating wavelength – viewing geometry – polarization configuration Proper characterization of the RCS’s response to incidence and azimuth angle variation helps to eliminate the viewing geometry dependence From Wye (2011)
  • 12. Pulses ● N ~ 50 for SAR ● Interpulse separation – Not possible at high incidence angle – Impacts noise modeling → uncertainty From Wye (2011)
  • 13. Noise ● Mean noise power level – receiver electronics thermal noise (mostly, Prec) – received target radiation thermal noise (less, Pa) ● System noise power – Psys = Prec + Pa ● The ideal receiver system – large front-end gain – receiver thermal noise power unaffected by any back-end gain changes – In this scenario, Prec constant for a particular receiver bandwidth – need to calculate the noise power once for each receiver filter ● Not the case in Cassini RADAR
  • 14. BIDR products in PDS ● SAR image from a single Titan pass ● Raw processing a “formidable undertaking” ● PDS raster format – IMG data file in binary format – LBL metadata file in text format – Imports in ISIS directly
  • 15. Integrated Software for Imagers & Spectrometers ● isis.astrogeology.usgs.gov “Manipulate imagery collected by current and past NASA and International planetary missions sent throughout our Solar System” ● Works in Linux & Mac ● Command Line Interface pds2isis from=BIDR*.IMG to=out.cub ● Display, mosaick GUI
  • 17. T91 Kraken Mare Small lakes Kraken Mare Mývatn Lacus Oneida Lacus Waikare Lacus T91 Fly-By ISIS-GRASS
  • 18. BIDR scales (F&D) Kraken Mare main Peninsula
  • 19. Ligeia Mare Mechanical erosion (Not chemical) Black et al (2012)
  • 20. Ligeia Mare Island Mare characteristics (not only from BIDR) ● Strong specular reflection, no waves - 1mm rms (Zebker et al., 2014) ● Extremely transparent (Mastrogiuseppe, 2014) - Suspended particles < 0.1% - 160 m maximum depth Dissolution/Precipitation play? (personal thought)
  • 21. Sub Equatorial Dunes 13% of Titan Matured features 1.3km width 2.7km crest spacing Hydrocarbon chains >1m/s saltation Equinox weather Savage et al, (2014) T95 Fly-By ISIS-GRASS
  • 22. Craters ● Wood et al. (2010) – 5 confirmed craters, 44 potential (+ E Xanadu) ● Neish et al (2012) – 5 confirmed > 20km diameter studied – Eolian infill ? (see Forsberg-Taylor, 2004) ● Giliam & Jurdy (2014) – Connection crater<>subsurface water Menrva (20.1°N 87.2°W)
  • 23. Various Geological Features ● Lopes et al. . (2012) – Hot cross bun from faults (38.5N, 203W) ● Stofan et al. (2008) – South pole complex surface morphology (T39) ● Wood (2011) – Caldera/Maar volcanism at the poles (?) ● More features recorded here: https://en.wikipedia.org/wiki/List_of_geological_features_on_Titan Maar: phreatovolcanism, explosive, often making lakes on Earth Arcūs, Faculae, Fluctūs, Flumina, Insulae, Labyrinthi, Large ring features, Maculae, Montes, Planitia, etc.
  • 24. Conclusions ● SAR imaging on Cassini probe ● BIDR products explore surface of Titan ● Methane & Ethane circulation ● Eolian, evaporative, rain processes ● Seas, lakes, dunes, geomorphology ● Strange, fascinating World at 92 Kelvin
  • 25. Thank you Credit for half of the images: NASA clicops.org & collaborators