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Through-Wall Imaging With UWB Radar System - KEMT FEI TUKE

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2.5 <strong>Radar</strong> <strong>Imaging</strong> Methods Overview 18<br />

30,29,31,131,39,151,44,92]. Most of them present methods for computing dinwall.<br />

Even if it looks like a simple task, it is a very complex problem that mostly requires<br />

huge computational power. In Section 4.1 we introduce an efficient, precise and<br />

fast method how to compute TOA for through the wall scenario.<br />

Very simple, fast, but not too precise approximation for compensation of the<br />

wall effect is presented in [31]. Here, the time of flight of the wave inside a wall is<br />

given by:<br />

tinwall = dinwall<br />

vw<br />

(2.5.3)<br />

where vw is the velocity of the signal inside the wall. The approximation of the<br />

velocity inside the wall is related to the wall permittivity and permeability given<br />

by:<br />

vw ≈<br />

1<br />

√ µwεw<br />

=<br />

1<br />

√ µaεaµrwεrw<br />

=<br />

c<br />

√ µrwεrw<br />

(2.5.4)<br />

where µw and εw are the permeability and permittivity of the wall, µa and εa<br />

are the permeability and permittivity of the air, and µrw and εrw are the relative<br />

permeability and permittivity of the wall. For non-magnetic materials such as<br />

concrete or brick wall, the relative permeability µrw = 1. Hence the velocity in<br />

non-magnetic wall is given by:<br />

and time in the wall by:<br />

vw = c<br />

√ εrw<br />

√ εrwdinwall<br />

(2.5.5)<br />

tinwall =<br />

. (2.5.6)<br />

c<br />

<strong>With</strong> the assumption that the wave mostly penetrates perpendicularly to the wall,<br />

the approximation of dinwall can be given by:<br />

dinwall ≈ Dw<br />

(2.5.7)<br />

where Dw is thickness of the wall. Time delay caused by through-wall penetration<br />

is then expressed as comparison to through the air propagation:<br />

tdelay = Dw<br />

vw<br />

− Dw<br />

c<br />

= Dw<br />

c (√ εrw − 1) . (2.5.8)<br />

All impulse responses BP n should be shifted by tdelay before SAR imaging is applied.<br />

Including tdelay into the migration (2.5.2) partly compensates effect of the<br />

wall:<br />

I(xT , zT ) = 1<br />

N<br />

N�<br />

BP n (X, k = (T OAn + tdelay)). (2.5.9)<br />

n=1<br />

The example of migrated image with and without simple wall compensation is<br />

shown in [31]. In general, the targets in compensated image are better focused as<br />

well as the positions of objects behind the wall are closer to the real positions.

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