See-Through-Wall Imaging Using Ultra Wideband Short-Pulse Radar System Yunqiang Yang, Aly E. Fathy The ECE Department, University of Tennessee Knoxville, TN 37996 Abstract: See-Through-Wall imaging radar is a unique application of Ultra Wideband communication that can provide soldiers and law enforcement officers an enhanced situation awareness. We have developed an Ultra-wideband high-resolution short pulse imaging radar system operating around 10 GHz, where two essential considerations were addressed, the effect of penetrating the walls, and the pulse fidelity through the UWB components and antennas of the radar. Modeled and measured wall parameters, and the effect of antenna types on signal fidelity will be discussed here in details. Background Ultra Wideband technology has been the subject of extensive research in recent years due to its potential applications and unique capabilities. Meanwhile, there is a lot of interest and attention on See-Through-Wall application because of current homeland security issues, where extensive work has been performed in the field of short-pulse radar [1, 2]. As the primary advantages of UWB for short-range radar imaging include extremely fine range resolution (theoretically sub-centimeter resolution), high power efficiency (because of low transmit duty cycle), low probability of detection, low interference to legacy systems, and its ability to detect moving or stationary targets [3]. We have developed a radar prototype, which utilizes an instantaneous 3dB bandwidth of 600 MHz and a center frequency of 10 GHz. In this paper, however, we emphasize two essential and special design considerations of the system. First, the electromagnetic wave propagation through walls made of typical building materials, and the pulse fidelity. Walls were examined both theoretically and experimentally and pulse fidelity was investigated in time domain. Evaluation of Wall Materials See-Through-Wall radar requires the ability to detect targets through materials such as concrete, bricks, dry wall, and plywood. Relatively high-density materials like concrete and bricks can result in considerable attenuation of electromagnetic waves, increasing requirements for both radar power and signal processing. Fig. 1 shows the RF attenuation in different types of walls as measured by our team in comparison to Currie, et al [4]. The lines show that most walls, such as dry wall, plywood, and bricks are fairly transparent to radar frequencies, thus making through-the-wall imaging possible. If radar signal must penetrate concrete block, a practical operational frequency is about 3 GHz, and the usable frequency range is no greater than approximately 10 GHz, as is one of the reasons the system operates at 10 GHz center frequency. The other reason is that, despite the fact that attenuation through materials is greater, the antennas and components are smaller than at lower frequency, resulting in a more compact system. 0-7803-8883-6/05/$20.00 @2005 IEEE 334 We also measured the insertion transfer function through wall slabs. Fig.2 shows the experimental configuration, where the transmit and receive antennas are positioned on line of sight, and transmission coefficients were measured with and without the presence of wall slabs between antennas, using 85 IOC Vector Network Analyzer. The insertion transfer function is defined as the ratio of such two transmission coefficients. An Advanced Design System (ADS) model was developed to simulate this experiment, shown in Fig.3. In the ADS model, wall slabs and free space paths were represented by transmission-lines. The parameters of transmission line, such as dielectric constant and loss tangent are adjusted according to the wall materials, i.e. when simulation matches measurement. Fig.4 plots the insertion transfer functions versus frequency for drywall slabs with different thickness, where we can see that the measured results match the simulation very well. The simple ADS model will help us to take the wall effect into account. See-Thru-Wall Radar Prototype The UWB radar system consists of four basic blocks: antennas, transceiver, data acquisition, and imaging post processing, where the radar sends out UWB short pulse signal, and receives echo retumed from targets. I/Q channel information are extracted from echo signal, then digitized and saved for image processing. Computers are used for user interface, and application programs for imaging processing. The developed system utilizes a 1-18 GHz UWB double-ridge hom antenna for transmission, and a 16-element antipodal Vivaldi [5] sub-array for reception, the system is shown in Fig. 5. While, the developed antenna is part of a 16x16 synthetic-aperture receive antenna. The radar operates at a center frequency of 10 GHz and has an instantaneous 10dB bandwidth of 1 GHz. Off-the-shelf UWB equipments and components were purchased for the experimental investigation. Pulse Fidelity through Radar System The image of the target behind walls is recovered based on the efficient transmission and reception of pulse signal. The distortion of pulse signal will translate into the distortion of images of targets. Therefore it is necessary to understand how pulse distortion is generated and how the pulse fidelity can be preserved in our system. There are several factors, which could possibly cause pulse distortion, changing timedomain pulse shape in other words. The first cause could be due to the imperfect UWB performance of off-the shelf components. The second cause can occur due to the transmit and receive antennas, since the intensity of radiated/received electromagnetic field varies proportionally with the derivative of the antenna current in transmit, and the integral of the current in reception. Experimental measurements were carried out to investigate the pulse distortion through components and antennas. The output of the pulser is up-converted to 10GHz through a mixer, and then connected to an UWB antenna through an UWB amplifier. Receive and transmit antennas are positioned for line-of-sight free-space transmission. On the receiving end, instead of I/Q demodulation, we just simply down-converted the modulated pulse signal. The pulser output and recovered down-converted pulse are both hooked up to a Tektronix sampling oscilloscope and compared. Different transmit/receive antenna pair were used, and the effect of antenna on pulse distortion was examined. Fig. 335 6 shows the shape of recovered pulse, compared to the original one, after transmitting through components and antennas. The comparison indicates that the pulse fidelity is best preserved when using two identical UWB antennas for transmission and reception. Use of different antennas can cause slight distortion, unless both have very wide bands. Conclusion An ultra wideband short-range radar has been developed and is based on SAR principles. The developed radar was used to evaluate various wall materials, and study pulse signal fidelity through the system. It was concluded that at 3 GHz, brick walls can be penetrated, and systems can be operable up to 10 GHz, other wall materials would allow operation to much higher frequencies. Our system even though it utilizes Vivaldi antenna for reception and UWB hom antenna for transmission does not distort the signal quality. Acknowledgements The authors would like to thank Dr. Mongi A. Abidi of University of Tennessee, Knoxville for his support in this work. Reference: [I] J. Taylor, Ed. Introduction to Ultra-wideband Radar Systems. Boca Raton, FL: CRC, 1995. [2] Ultra-Wideband, Short-Pulse Electromagnetics 1, 2, 3 and 4, New York: Plenum, 1993, 1994, 1997, and 1999 [3] 1.1. Immoreeve and D.V. Fedotov, "Ultra wideband radar systems: Advantages and disadvantages", in Proc. IEEE Ultra Wideband Systems and Technologies Conf, Baltimore, MD, May 2002, pp.201-205. [4] N.C. Currie, D.D. Ferris, and al, "New law enforcement application of millimeter wave radar", SPIE Vol. 3066, pp2-10, 1997 [5] E.Ehud Gazit, "Improved design of the Vivaldi antenna," Proc. Inst. Elect. Eng., pt. H, vol. 135, no. 2, pp. 89-92, Apr. 1988. Free 9er, Thbckss, Lc -. II SWab s II _ N litt Tra., Frs,Sj;pLeU0h L_ldt Ticks,ssU_s-L sb LlietcD,akM C ebpsi t: L TsTargont. pr2 FMSp.oePAl h Lsoti, 2b TMd-sssss L _as Lr sl b D.Clab,o Cn.n.sl epsl Loss Th5ssI eps2 AVA Figure 2: Experimental Setup 336 ' lReseasa .~~~ . e N* umM d ~~._* . Figure 3: ADS Model - ....... s-Shrutedrest I 1 _ -4-- fM endsZ1 -0 -0: !2-0.' .Oh . _lb Skuaedardt -02- ---1 ----------- 4---4 --- -1: 0 2 4 6 8 10 12 14 1 10 2 4 6 0 10 12 14 16 18 2 (a) 1/2 inch Slab (b): 5/8 inch Slab Figure 4: Insertion Transfer Function versus Frequency for Drywall, Dielectric Constant=2.4@lO GHz. T. s-kc (a) Transmitter Structure (b) Receiver Structure Figure 5: Transmitter and Receiver Diagram (a) Spiral/Spiral (b) Horn/Hom (c) Vivaldi/Hom (d) Spiral/Hom Figure 6: Original and Recovered Pulse after transmission. (Red lines on top is original pulse waveform, and green lines on bottom are recovered) 337
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