In: Wagner W., Székely, B. (eds.): ISPRS TC VII Symposium - 100 Years ISPRS, Vienna, Austria, July 5-7, 2010, IAPRS, Vol. XXXVIII, Part 7B
Figure 8. Oblique view aerial image of the DB-Tower
Figure 7. Simulated double bounce reflections overlaid with PS
Therefore, it is reasonable to assume that the PS are caused by
structures on this roof and not by scatterers located at the upper
part of the facade. This assumption is verified by the estimated
height of the PS (see
Figure 2).
It is furthermore possible to assess PS located on double bounce
lines induced by large scale building features (e.g. curb-to-wall
scattering). These are displayed in Figure 7. The PS heights
arranged in five meter classes are overlaid to simplify the
discrimination of PS on and off the double bounce lines. It is
apparent, that the PS densities on the double bounce lines are
not always as high as one may expect due to the strong
backscattering. An example is marked by the red box in Figure
7, where there are hardly any PS resident (PS coloured in light
red). In contrast to that, there are lots of PS on the double
bounce feature marked by the green box. The reason for that
is to be investigated.
As can be seen from the oblique view aerial image in Figure 6
the virtue of the respective façades differ in terms of material
and geometry.
Finally it is remarkable, that there are almost no PS at the
façades visible in Figure 6, which is apparent from
Figure 2 and Figure 5. This is surprising, since there are usually
plenty of PS at building fronts oriented towards the sensor. It is
conceivable, that this is due to the texture of the façades.
However, there are at least some PS located on the skyscraper at
the top of the SAR image (see Figure 1 and
Figure 2), whose façade looks quite similar as can be seen from
the oblique view aerial image displayed in Figure 8.
4. CONCLUSIONS
In theory a SAR simulator can assist the PSI analysis by helping
to determine the exact location of the PS. This is true, if very
precise and detailed 3D building models are available. Although
3D building models are available for many urban areas, they
seldom contain the geometry of the façades. The façade is
mostly represented with an image texture, which is feasible for
visualization purposes, but not for SAR simulation. To simulate
the façade reflection, a 3D model containing the façade
geometry is necessary.
However, the simulation still proofed to be useful. We could
demonstrate that the double bouncing between building and
ground does not cause many PS. Most PS in our test scene are
caused by scatterers located on the building roofs.
Without highly detailed building models, SAR simulation can
only provide very rudimentary assistance for the PSI analysis.
In future work we will augment the 3D model by close range
Photogrammetry in order to represent also pillars, doors,
windows and balconies. In a next step we want to group PS and
match those against facade structures.
ACKNOWLEDGEMENTS
Part of the work was supported by the Research Fellowship for
International Young Scientists of the National Natural Science
Foundation of China (Grant No. 60950110351).
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