Planetary & Cometary Exploration Cameras on Orbiters and Landers



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tarix05.01.2018
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Planetary & Cometary Exploration

  • Cameras on Orbiters and Landers

  • Nick Hoekzema



Purpose of the camera (I)

  • Navigation, orientation 

    • Solar sensors  orientation with ~ 0.5º accuracy
    • Star trackers to recognize constellations  accuracy up to the `` range
    • Feedback between cameras and gyros/rockets
  • Atmospheric research

    • Usually large FOV and high S/N is more important than high spatial resolution. Usually a few km/pixel is quite sufficient  WAC cameras
    • E.g., weather, cloud, and aerosol studies


Purpose of the camera (II)

  • Surface geology

    • Usually high spatial resolution is more important than high S/N or large FOV  NAC cameras
    • Try to embed NAC image in WAC context image
  • Geochemistry  spectral imaging

  • Surface topography  stereo cameras, laser altimeters

  • Mapping needs:

    • very accurate positional measurements
    • very accurate description of the body
    • Image deformations by optics must be well known


Border conditions (I)

  • Data rate

    • Earth remote sensing: many Gbytes/day if needed
    • Deep space: be happy with a Gbyte/day
  • Weight, how much payload does a camera take?

    • Simple WAC & navigational cameras nowadays: few kg or even few hundred grams
    • Some Earth observers have cameras of hundreds of kg
    • Old fashioned pre CCD era cameras: tens of kg
    • Omega (spectral imager) ~20—25 kg
  • Temperature environment

    • Dark current and response to incident light change with temperature  unstable temperature environment ruins calibration
    • Spectral imagers, IR cameras often need cooling


Border conditions (II)

  • Power consumption

    • Small WAC cameras: few W or even less
    • Old fashioned pre CCD era camera: tens of W
    • Active system like MOLA laser altimeter: tens of W
    • Huge, cooled, IR telescopes: hundreds of W
  • Weathering: CCDs don’t like cosmic rays, fast solar wind protons, etc

  • Dimensions

    • some positional cameras and WACs fit into a matchbox
    • High resolution cameras need a telescope  much larger e.g., MOC ~ 0.5 X 0.5 X 0.9 m
    • Some spy satellites had telescopes of several meters


Lander Stereo Cameras

  • Most landers have stereo cameras

  • Stereo information is needed to manouvre vehicle or manipulators



Past sixties & seventies

  • Extremely high resolution space images

  • from spy satellites. E.g., US Samos

    • Use television system for targeting
    • Register high resolution images on film
    • Drop film in capsule to Earth surface
    • (Panic when capsule lands on wrong spot)
  • Obvious problems when you want to have pictures from planets other than Earth, then use television  quality not so good



Lunar Orbiter

  • 1966-1967

  • Great images (but the reproduction shown here is less than optimal)

  • Although the optics were not impressive, objects of only a few meters are visible…

  • and intensities are extremely well calibrated

  • …because the S/C could be put into low lunar orbit…

  • …and, most of all, because it exposed onto a 70 mm film!



Lunar orbiter (II)

  • Essentially used a normal photo-camera

  • The spacecraft developed and digitized its own films onboard

  • Drawbacks

  • Not used for interplanetary missions such as Viking or Voyager



Vidicon

  • Telescope focuses images on a Vidicon

  • Image is an imprint of variable electrostatic charge on the faceplate of the Vidicon

  • Faceplate is then scanned and neutralized with an electron beam and variations in charge are read in parallel into a seven-track tape recorder

  • They flew on numerous missions (Mariners, Voyagers, etc)

  • They were heavy (Voyager camera system ~40 kg)



VIS: Viking orbiter vidicon cameras as an example

  • But for many over/under exposed pixels, intensities are ~1% reliable

  • Bit slow (i.e., the readout and digitization)

  • Moving parts (shutter, filter wheel)

  • Consume upto 35 watts



Facsimile Viking lander cameras

  • Very different from vidicon principle

  • Intensities from a small solid angle are measured by one or more photodiodes (viking facsimiles had 12)

  • A nodding mirror is used to build an image pixel by pixel

  • Advantage: extremely accurate intensity measurements

  • Drawback: slow, very slow, and contains moving parts



Present

  • And then miniaturization gave birth to the CCD

  • Each pixel stores a charge that is determined by the illumination incident on it

  • End of exposure 

    • charge is transferred to a storage register
    • the CCD is freed up for the next exposure
  • First interplanetary use:

  • 1986 Halley flyby of

    • Giotto CCD from MPAE!
    • Vega


CCD: good and bad

  • Few or no moving parts • Extremely lightweight

  • Fast • Reliable • Small power consumption

  • Can handle large contrasts

  • Measured intensities are not too accurate

    • Originally ~5%
    • Nowadays ~0.5% or better
  • Sensitive to damage from e.g., cosmic rays

  • In short: If time, weight, maintenance, data transfer rates, and transport were no problem then old fashioned facsimile and film cameras would often still be the better choice



Framing cameras

  • Use rectangular CCD to take pictures

  • No Viking-like problems with fast phenomena like these dust-devils

  • Since nowadays CCD may easily have several million pixels…

  • …observing at high spatial resolution usually is less of a problem than…

  • …sending images of a few Mbyte each in a reasonable amount of time

  • Therefore add pixels prior to transmitting the image 

    • Higher S/N ratios
    • Lower spatial resolution
  • This procedure is called macro pixeling



Push broom scanners Examples: MOC (on Mars Global Surveyor) MISR (on Terra) HRSC (on Mars Express) ((Omega (on Mars Express))) compare Sumer (on SOHO)

  • Push broom cameras scan the surface with line CCDs

  • Images are built line after line as the spacecraft moves along its orbit

  • Line CCDs may have many thousands of pixels

  • Biggest problems usually:

    • Data rate
    • Need for accurate correction for S/C movements and vibrations




High resolution MOC image

  • MOC couldn’t quite resolve Pathfinder

  • But the 2005 orbiter camera probably will

  • S/N ratio is pretty awful: ~20--30



Multiple line push broom scanners

  • Examples, MISR and HRSC

  • Several line CCDs are mounted in parallel

  • Each observe in different colors and/or angles  stereo view in color

  • Note the difference in optical depth between 0º and 60º



Stereo Remote Sensing

  • Gives DEMs

  • Very useful for aerosol and other atmospheric studies

  • Useful for separating atmosphere from surface

  • Some stereo cameras fly onboard airplanes are Air Misr and HRSCa

  • Stereo remote sensing of Earth:

    • ATSR-2 onboard ERS
    • POLDER onboard ADEOS
    • MISR onboard TERRA
  • Stereo remote sensing of Mars from 2004 with HRSC on Mars Express



So what about the future? Scanning with a rectangular CCD?

  • In fact a 1000 X 1000 pixel CCD is a set of 1000 line CCDs in parallel

  • You might put a grating in front of it so that a spectrum is projected on the CCD

  • Scan the surface with each of these ‘line CCDs’

  • This is a form of ‘spectral imaging’

  • Largest drawback: the data rate is enormous if done at high resolution

  • Mars Climate observer was to use a simple, low data rate version of this principle (pity it was lost)



Laser altimeters

  • MOLA (Mars Orbiting Laser Altimeter) gave a superb topographic map of Mars

  • However, it also:

    • Probes the atmosphere
    • Measures surface albedos
    • Measures surface roughness
    • Can look at dark surfaces
  • Will be a valuable tool on missions to Mercury, asteroids, Jovian moons, etc



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