International Archives of the Photogrammetry, Remote Sensing and Spatial Information Sciences, Vol XXXV, Part B7. Istanbul 2004
motion might reach tens of pixels. Therefore, it is important
to adjust the research area size to the expected maximum
offset, or, if one can model the movement, to provide the
correlation process with the estimated offset value. In the
latter case, the research window may remain small, because
the estimated position of the homologous points in the
secondary image is accurate enough.
2.4 Conversion into latitude and
longitude and geo-coding
Now that we have computed the offsets in line AL and in
columns AC in the reference image, for a given set of points
(usually a regular grid of points), we must convert them into
ALat and ALon on the ground, or their equivalent AX and AY
if we use a map projection. At this stage, we must be careful
not to simply multiply the offset by the average satellite
image pixel size (2.5m in the case of SPOTS THR), because
the pixel size is variable inside the image, in particular in
mountainous areas. To be precise, we proceed the following
way
* Project the reference point on the ground
* Project the secondary point on the ground
* . Deduce by difference the horizontal displacements ALat
and ALon. The difference in altitude is only due to the
local glacier slope.
At this stage, we have converted the initial offset grids, in
pixel unit and in reference image geometry, into offsets in
meter or degrees, in the two directions North and East. A
final transformation, using the geometrical model of the
reference image, allows the geocoding of the two offset grids.
We now have 2 grids of offsets, one in the North/South
direction, and the other in the East/West one, directly
interpretable: they are hopefully null (or almost null) outside
the glaciers and they represent absolute motion on the
glaciers.
From those grids, we can extract profiles of highest velocity
fields, or simply read displacement of reference geographical
points. We may separately consider the two directions, or
compute the total horizontal displacement:
AHorizontal- JAY?-AY?
25 Measurement accuracy
The different errors which might affect the process are
+ Global image geometrical distortion residuals
° Local geometrical residuals, due to local DEM error
+ Local offset computation errors, on the glaciers
themselves.
We can give an upper bound to the first error, computing the
residuals outside the glaciers. Average residual is null (we
refined the image geometrical models in order to minimize
the residuals, by bundle block adjustment, which usually
presents a null residual average), and standard deviation
provides us with an information about the quality of this
process. However, due to the low gain of the images, glaciers
correlate much better than general landscape: the rms error
on the glaciers is expected to be lower than the one outside
the glaciers.
The second error mainly depends on the stereoscopic baseline
between the two acquisitions. The closest the two local
832
acquisition angles, the less sensible the results to relief errors.
Even if an accurate DEM is not available everywhere on the
60km x 60km SPOTS scene, one should try to have a good
DEM at least on the glaciers themselves.
The third error is mainly due the radiometric dissemblance
between the two images, provided the resampling processes
are all performed with an adequate filter, like the apodized
cardinal sine (Carfantan, 2001). This radiometric
dissemblance may be related to surface changes between the
two acquisitions, or may be a consequence of different
acquisition incidence angles. In the case of time interval, one
must not forget that, even if the images are acquired at the
same hour of the day, different sun angles will lead to
different shadows. This is particularly true in mountainous
areas, but in our case, we found it more visible outside the
glaciers than on the glaciers themselves, because glaciers
were not on the areas of steepest slopes in the image.
Quantifying this error is possible: computing the glacier
motion on a given profile (for example on the steepest slope
line), and then on a different one, close to the first one, can
provide a good approximation of the accuracy.
3 TEST CASE: THE ALPS, SUMMER 2003
Glaciers of the Mont Blanc range have been selected for a
first application of the methodology. The two main glaciers
in this area are the “Mer de glace” and the “Argentière”.
They are well known, easily accessible and we have a good
knowledge of their past velocities. A field campaign has
taken place last summer, at about the same time as SPOTS
images were acquired. Ground truth could therefore be
gathered, which allowed us to validate our methodology.
3.1 Images
Four images were acquired by SPOTS (Figure 2) on this
region in the summer 2003, forming the following two pairs:
° 19 July / 19 August: incidence angles -23.6° and -15.2°,
31 days interval
+ . 23 August / 18 September: same local acquisition angle:
16°, 26 days interval ( one SPOTS orbital cycle)
6 42' 6 48' 6 54' Ot 7 06'
16 00' 46 00
45 48
6 42 648 6 54 7 00 7 06
Figure 2: SPOTS image on the Mont Blanc range (detail,
geo-referenced). Lig and Col represent image direction.
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