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

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

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2.2 <strong>Through</strong>-<strong>Wall</strong> <strong>Radar</strong> Basic Model 7<br />

<strong>System</strong><br />

clock<br />

Signal<br />

processing<br />

Clock rate fc<br />

Binary<br />

divider<br />

N-stage<br />

shift register<br />

Σ/ADC/T&H<br />

Σ/ADC/T&H<br />

M-sequence TX<br />

Response<br />

Response<br />

RX1<br />

RX2<br />

Fig. 2.1.2: Block diagram of M-sequence <strong>UWB</strong> radar system.<br />

averaged, and correlated with the transmitted one. In principle, after the correlation,<br />

the output from the M-sequence radar system is the same as the output<br />

from a classic <strong>UWB</strong> pulse radar system. Therefore, the common signal processing<br />

techniques could be used after the data are gathered from radars. An analysis of 2<br />

Dimensional (2D) target positioning accuracy for M-sequence <strong>UWB</strong> radar system<br />

under ideal conditions with the concentration on error caused by sampling with<br />

finite frequency we described in [2].<br />

Two M-sequence <strong>UWB</strong> radars with number of chips M = 511 and clock frequency<br />

fc1 = 4.5 GHz or fc2 = 9 GHz are used for our experiment. One chip<br />

represents time interval between the two nearest impulses in M-sequence. Msequence<br />

generator has N = 7 stages. For more information about M-sequence<br />

<strong>UWB</strong> radar see [43, 116, 118].<br />

2.2 <strong>Through</strong>-<strong>Wall</strong> <strong>Radar</strong> Basic Model<br />

<strong>Through</strong>-wall radar (TWR) basic model specifies all processes which contribute<br />

to the measured data. These processes are caused mainly by the measurement<br />

system, the measurement environment and partly also by measured objects. For<br />

description of this model TWR system with one RX and one TX stationary antenna<br />

is used.<br />

Antenna signal effects would be shown for both, RX and TX antennas. The<br />

electric field which is generated by the TX antenna is called Erad and could be<br />

modeled by [79, 125]:<br />

E rad (r, θ, ϕ, n) = 1<br />

2πrc hT X(θ, ϕ, n) ∗<br />

√<br />

Z0<br />

√<br />

Zc<br />

∆VS(n)<br />

∆n<br />

(2.2.1)

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