Lecture 6
Scanning Systems
Across Track Multispectral Scanner (MSS)
This form of
imaging is used in Landsat series of satellite. The scanning system (Fig.5.6)
employs a single detector per band of the multispectral signal. It has an
electrical motor, to the axel of which is attached a solid metal cylinder whose
free end is cut at 45 degrees to the axis of its rotation and highly polished
to act as a scanning mirror. The field of view (FOV) is restricted by an
aperture so that the mirror will receive signals in almost nadir view from 2000
ground resolution cells that makes one scan line. The signal received by the
rotating scanning mirror from a ground resolution cell (corresponding to GIFOV)
is a white one and contains spectral information in different bands. This white
beam is reflected by the mirror in the flight direction (parallel to the
ground) and is allowed to pass through a monochromator/spectroscope which
splits the composite beam into its color components. The detectors with their
designed apertures
are so placed that they now receive the spectral information from the ground
resolution cells in the Specified bandwidths of various color components of the
white signal
The dwell time of the scanner is compared by the formula
Dwell Time = (Scan rate per line)/(Number of ground
resolution cells per line).
The Spatial Resolution of the scanner
=ground resolution of the scanner
=GIFOV x Attitude of the scanner
Along track
multispectral
Scanner/
Push Broom Scanner
In
this type of scanner, the scan direction is along the track (direction of
night) and hence the name along track scanner (Fig.5.7). It is also called push
broom scanner because the detectors are analogous to the bristles of a push
broom sweeping a path on the floor.
Development of
charge-coupled device (CCD) has contributed to the successful design of the
along track scanner. In this the sensor elements consist of an array of silicon
photodiodes arranged in a line. There are as many silicon photodiodes as there
are ground resolution cells (corresponding to IFOV) accommodated within the
restricted FOV of the sensor optics. Each silicon photodiode, in turn, is
coupled to a tiny charge storage cell in an array of integrated circuit MOS
(metal oxide semiconductor) device forming a char e coupled device (CCD) (Fig.5
3). When light from a ground resolution cell strikes a photodiode in the array,
it generates a small current proportional to the intensity of light falling on
it and the current charges the storage cell placed behind the diode. The
charged cells form part of an electronic shift register which can be activated
to read out the charge stored in the cells in a sequential fashion. The output
signals are correlated with the shift pulses, and digitized to reconstitute the
image.
The spatial resolution of the sensor = ground resolution cell
=GIFOV x altitude of the scanner
The dwell time for the long track scanner is given by
Dwell time = (ground resolution cell dimension)/ (velocity of
sensor platform)
Side Viewing /Side Looking Scanner
The across
track and along track scanners described above are used in passive remote
sensing in
visible, infrared and microwave regions of the electromagnetic spectrum. These
scanners always receive signals in the nadir view. However if the user demands
(on payment basis) to observe a dynamic scene frequently, then there is
provision in SPOT and IRS satellites to steer the cameras to look off-nadir
at the required scene, some days before to some days after the normal nadir
viewing date (fig 5.9).
But scanners
of active remote sensing, like the scanners used 'for radar remote sensing, in
their normal mode of scanning look to the sides and not to the nadir for
technical reasons which will be described later. Therefore such scanners are
called side looking airborne radar (SLAR). The most sought after
sophisticatedly designed synthetic aperture radar (SAR) belongs to
the side looking scanner system.
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