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    14-Feb-2012
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Radar Course III
43. Texture and image analysis
42. Temporal averaging
12. Synthetic Aperture Radar (SAR)
34. Space, time and processing constraints
15. Slant range / ground range
8. Side-looking radars
19. Shadow
10. Real Aperture Radar: Range resolution
11. Real Aperture Radar: Azimuth resolution
9. Real Aperture Radar (RAR)
7. Radar principles
38. Radar image interpretation
35. The radar equation
36. Parameters affecting radar backscatter
16. Optical vs. microwave image geometry
25. Method
18. Layover
32. Landers Earthquake in South California
23. Introduction
27. Interferogramme of Naples (Italy)
29. Interferogramme and DEM of Gennargentu (Italy)
2. Independence of clouds coverage
40. Image interpretation: Speckle
41. Image interpretation: Speckle filters
39. Image interpretation: Tone
20. Geometric effects for image interpretation
22. Geocoding: Geometry
17. Foreshortening
26. First ERS-1/ERS-2 tandem interferogramme
6. Electromagnetic spectrum
30. Differential interferometry
45. Data reduction: 16 to 8 bit, blockaverage vs incrementing
4. Control of imaging geometry
3. Control of emitted electromagnetic radiation
24. Concept
28. Coherence image of Bonn area (Germany)
44. Classification of ERS-1 SAR images with Neural Networks
37. Bragg scattering
5. Access to different parameters compared to optical systems
13. SAR processing
33. SAR interferometric products
21. SAR image geocoding
14. ERS SAR geometric configuration
31. The Bonn experiment
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Side-looking radars

Most imaging radars used for remote sensing are side-looking airborne radars (SLARs). The antenna points to the side with a beam that is wide vertically and narrow horizontally. The image is produced by motion of the aircraft past the area being covered.

A short pulse is transmitted from the airborne radar, when the pulse strikes a target of some kind, a signal returns to the aircraft. The time delay
associated with this received signal, as with other pulse radars, gives the distance between target and radar.

When a single pulse is transmitted, the return signal can be displayed on an oscilloscope; however, this does not allow the production of an image. Hence,
in the imaging radar, the signal return is used to modulate the intensity of the beam on the oscilloscope, rather than to display it vertically in proportion to the signal strength.

Thus, a single intensity-modulated line appears on the oscilloscope, and is transferred by a lens to a film. The film is in the form of a strip that moves synchronously with the motion of the aircraft, so that as the aircraft moves forward the film also moves.

When the aircraft has moved one beamwidth forward, the return signals come from a different strip on the ground. These signals intensity-modulate the line on
the cathode-ray tube and produce a different image on a line on the film adjacent to the original line. As the aircarft moves forward, a series of these
lines is imaged onto the film, and the result is a two-dimensional picture of the radar return from the surface.

The speed of the film is adjusted so that the scales of the image in the directions perpendicular to and along the flight track are maintained as nearly
identical to each other as possible. Because the cross-track dimension in the image is determined by a time measurement, and the time measurement is
associated with the direct distance (slant range) from the radar to the point on the surface, the map is distorted somewhat by the difference between the
slant range and the horizontal distance, or ground range.

In some radar systems, this distortion is removed by making the sweep on the cathode-ray tube nonlinear, so that the points are mapped in their proper
ground range relationship. This, however, only applies exactly if the points all lie in a plane surface, and this modification can result in excessive distortion in mountainous areas.

Side-looking airborne radars normally are divided into two groups: the real-aperture systems that depend on the beamwidth determined by the actual
antenna, and the synthetic aperture systems that depend upon signal processing to achieve a much narrower beamwidth in the along-track direction than that
attainable with the real antenna.
The customary nomenclature used is "SLAR" for the real-aperture system and "SAR" for the synthetic aperture system, although the latter is also a
side-looking airborne (or spaceborne) radar.


Keywords: ESA European Space Agency - Agence spatiale europeenne, observation de la terre, earth observation, satellite remote sensing, teledetection, geophysique, altimetrie, radar, chimique atmospherique, geophysics, altimetry, radar, atmospheric chemistry