1- INTRODUCTION
SPOT-1
followed by
the two
synchronous
was launched in February 1986 and
SPOT-2 in January 1990. Each one of
satellites circles the Earth in a
orbit (altitude 832 km) and repeats
its coverage every 26 days. SPOT-1 and SPOT-2
carry an identical push-broom sensor system.
This sensor system includes two identical
optical instruments, the HRV1 and HRV2 (High
Visible Resolution). SPOT's sensor produces
images in two modes; the panchromatic mode (P)
with a single spectral band (0.51 um to 0.73 um)
and a ground resolution of 10 m and the
multispectral mode (XS) with three spectral
bands (between 0.5 um to 0.84 um) and a ground
resolution of 20 m.
The reflected radiation picked up by the
optical instrument, for each spectral band, is
measured by an array of detectors (6000 for the
^P' mode, 3000 for each of the spectral bands of
the ^"XS' mode) which forms .rows of the image
perpendicular to the satellite track (60 km on
the ground). The scenes dimension parallel to
the satellite .track is achieved by movement of
the satellite along its orbit. Each SPOT scene
covers 60 km by 60 km.
in front of the HRV
modification of the look
an across-track angle with the
reach +27 degrees. So, it is
images of the same ground
look angles from different
a stereoscopic pair from any two
situated
allows
making
A mirror
instrument
direction
vertical that can
possible to record
area at different
orbits forming
of such images.
SPOT stereoscopic
used to extract 3-dimensional
information by using conventional
photogrammetric methods. In the first method, a
stereomodel was formed by an analytical relative
orientation. Model coordinates, then, were
fitted into ground coordinates using
3-dimensional affine and polynomials
transformations. In the second method of
stereoscopic analysis, ground coordinates, in
three dimensions, of check points are computed
by space intersection. In this case, the
exterior orientation elements of each image is
determined, first, by space resection and then
used to orient left and right rays through image
In this
pair Was
investigation a
points to intersect in the ground position of
any point. A variable number of ground control
points is used to determine the transformation
and orientation parameters in each case. A
special polynomial was used to correct computed
heights derived from the second method.
Residuals and their root mean squares in a
number of check points were determined and
analysed.
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2- THE MATHEMATICAL MODELS
Conventional photogrammetrical mathematical
models were used in this investigation to
perform stereoscopic analysis of the SPOT data.
There are two well known analytical methods for
extracting 3-dimensional ground coordinates from
a stereo pair of images. In the first method, a
stereomodel is formed and ,then, computed model
coordinates are transformed into ground
coordinates by a mathematical model for absolute
orientation. There are a number of ways to solve
the problem of relative orientation ,coplanirity
equation, analytically. In this investigation,
the method of fixing the left hand image is
adopted and, accordingly, the relative
orientation mathematical model can be written
as:
{x y z)Le]| 0 -Bz By
Bz O0 -Bx
-By Bx O0
X
ER sly
z
r
where (x y z)L and (x y z)r are the image
coordinates of any point at the left and right
images respectively and Bx is an arbitrary scale
factor for the formed stereomodel. The five
orientation parameters are; the base component
in Y-direction ’By’, the base component in
Z-direction ’Bz’ and the three rotation elements
which define the orthogonal rotation matrix 'R'.
For images collected by scanners, the relative
orientation parameters may change along the
track direction and polynomials may be
considered to represent these changes. In this
study, changes .in the base components 'By' and
?Bz* are taken into consideration and
represented by polynomials.
after
orientation
coordinates
overlapping
computed.
coordinates
coordinates are:
determining the relative
elements, 3-dimensional model
of any image point in the
area between the two images can be
The mathematical models used for model
transformation into ground
(i) The three-dimensional transformation in the
form:-
E = al + a2.Xm + a3.Ym + a4.Zm,
N - bil * b2.Xm + b3.Ym + b4.Zm, and
Haz clat:c2.Xm + cS: ¥Ynitocd.Zm
(ii) The three-dimensional second order
polynomials in the form:-
E = al + a2.%m * a3.Ym t ad.Zm t a5.Xm**2 +
a6.Ym**2 t a7.Xm.Ym,
N = bi + b2.Xm | bs5.Ym 4 b4.7m t b5.Xmt**2 *
b6.Ym**2 + b7.Xm.Ym and
H = cl t c2.YXm | c5.Ym * cd.7m t c5.Xm**2 +
c6.Ym**2 * c7»Xm.Ym.
(E,N,H), (Xm,Ym,Zm) are, respectively, the
ground and model coordinates of any reference
point and the remaining elements are the
transformation parameters or cxonstants. This
method, some times, is called ’the two steps
orientation’
where