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

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4.2 Measurements of the <strong>Wall</strong> Parameters by Reflectometry 56<br />

Z[m]<br />

0.6<br />

0.7<br />

0.8<br />

0.9<br />

1.0<br />

1.1<br />

1.2<br />

Z<br />

X = 1.73 m<br />

Z = 1.0 m<br />

0.5 m<br />

Antennas movement<br />

1.6 m<br />

3 m<br />

0.4 m Brick wall �rw= 3.4<br />

1 m<br />

Metal plate<br />

0.67 m<br />

0.64 m<br />

Fig. 4.1.12: SAR measurement - Scenario 2.<br />

1.6 1.7 1.8 1.9 2.0 2.1 2.2 2.3<br />

a)<br />

X[m]<br />

Z[m]<br />

0.6<br />

0.7<br />

0.8<br />

0.9<br />

1.0<br />

1.1<br />

1.2<br />

X<br />

X = 1.6 m<br />

Z = 1.0 m<br />

1.6 1.7 1.8 1.9 2.0 2.1 2.2 2.3<br />

X[m]<br />

Fig. 4.1.13: Migrated images - Scenario 2. a) Method with simple wall compensation.<br />

b) Proposed method with precise TOA estimation.<br />

4.2 Measurements of the <strong>Wall</strong> Parameters by<br />

Reflectometry<br />

Precise SAR imaging of objects, detection of the moving person behind the wall,<br />

or non-destructive testing of the state or quality of walls constructions in civil<br />

engineering with <strong>UWB</strong> radar requires the knowledge of wall parameters like thickness,<br />

permittivity, and conductivity. Their use in data processing produces more<br />

precise and realistic results, as we have shown in Section 4.1. The more precise the<br />

wall parameters are known the better the complex algorithms for SAR imaging [1]<br />

or detection of moving persons [114] could be enhanced. The measurement of the<br />

wall parameters is challenge in a real environment especially when there is access<br />

only from one side of the wall. In this section, an effective and fast algorithm for<br />

wall parameters estimation that can be used in practice is presented. For that<br />

purpose the magnitudes and the time positions of reflections from inner and outer<br />

interfaces of the wall are extracted from the data. A new scanning method that<br />

b)

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