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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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)