Through-Wall Imaging With UWB Radar System - KEMT FEI TUKE
Through-Wall Imaging With UWB Radar System - KEMT FEI TUKE
Through-Wall Imaging With UWB Radar System - KEMT FEI TUKE
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4.4 Measurements of the Practical Scenarios 81<br />
differ depending on the chosen interpretation method. Subfigure a) e.g. Fig.<br />
A.0.1 a) shows the photo of object behind the wall. Subfigure b) e.g. Fig. A.0.1<br />
b) shows 1D cross-range plot mostly at position X = 1 m what corresponds to the<br />
object position and X = 0.3 m what corresponds to the position where object is<br />
absent. Subfigure c) e.g. Fig. A.0.1 c) shows 2D image of the scanned environment<br />
including the target, the front and the rear wall. After migration the image consists<br />
from positive and negative values. Dividing values into the both positive and<br />
negative do not have any physical interpretation in image. Therefore, an absolute<br />
value from Hilbert transform is imaged here in order to be closer to the ”energy”<br />
representation. Subfigure d) e.g. Fig. A.0.1 d) shows the same 2D image as in c).<br />
However, only a zoomed region where the object occurs is imaged. The colormap<br />
is also changed in order to enhance the target visibility. Subfigure e) e.g. Fig.<br />
A.0.1 e) shows 3D image of scanned environment including the target, the front<br />
and the rear wall. The third dimension represents the ”magnitude” of the image.<br />
Both, the positive and the negative values are imaged. Colormap differs from the<br />
one used in subfigures c). Subfigure f) e.g. Fig. A.0.1 f) shows the same 3D image<br />
as in c). However, only a zoomed region where the object occurs is imaged. Such<br />
representation helps to concentrate on the object especially when the front wall<br />
dominates in the migrated image.<br />
From the Figures in Appendix A it can be seen that the most visible objects<br />
behind the brick wall are the metallic ones with the flat surface placed in parallel<br />
with the scanning direction. The metallic fire extinguisher with rounded surface<br />
is also clearly visible. However, a small sphere covered with aluminum foil with<br />
diameter only 20 cm is almost invisible behind a such wall. Subfigures A.0.7<br />
b), d), and f) can help to find the position of the sphere. Even if the wooden<br />
cupboard is the biggest object that was scanned, the wood and glass are not<br />
a good reflectors for electromagnetic waves at such frequencies. Therefore, the<br />
magnitudes of cupboard in both directions are similar with much smaller objects<br />
but the metallic ones, sometimes even smaller. A clear watter is not the best<br />
conductor for direct current, however even the small aquarium filled with clear<br />
watter is a good reflector for electromagnetic waves at the used frequencies. The<br />
dimensions of the objects in scanning - X direction can be estimated with relatively<br />
good precision. However, dimensions of the objects in looking - Z direction can be<br />
estimated very difficultly from the migrated images. It is because of a most of the<br />
energy reflected from the front surface of the object and only hardly penetrate into<br />
the object, reflect from the rear surface and penetrate back to the receive antenna<br />
through the object and the wall. Such handicap can be eliminated by scanning of<br />
the objects from at least two sides.<br />
Based on the previous analysis, the most of the objects in the room could<br />
be imaged with the <strong>UWB</strong> radar device through the brick wall. The methods for<br />
image representation should be chosen according to the scanned objects and also