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Polarization

VHF Capability and RCS Measurements from Long Cylinders
P.S.P. Wei (The Boeing Company),A.W. Reed (The Boeing Company), C.N. Ericksen (The Boeing Company), November 2002

In order to better understand the capability and limitation of the radar in the VHF band, we present the results from RCS measurements on simple calibration objects of sizes from small to large. Though the uncertainty for measuring a small object is usually well behaved to within +0.2 dB, the greatest difficulty for a large object is the lack of knowledge on the distribution of the incident field. Some qualitative ideas may be obtained from fieldprobes along a few directions. Yet, a thorough investigation of the field in 3-D as a function of the frequency and polarization is generally beyond time and budget constraints. For the special cases of long and thin cylinders at broadside, we find that the difference in HH-VV is very sensitive to ka, which allows us to distinguish them apart.

Wide-Band Dual Polarized Probes for High Precision Near Field Measurements
L.J. Foged (SATIMO),L. Duchesne (SATIMO), L. Roux (Alcatel Space Industries), Ph. Garreau (SATIMO), November 2002

High precision near field measurement systems in dual polarization have stringent requirements on the probe performance in terms of radiation pattern shape, on-axis and off-axis polarization purity and port-to-port isolation. In general, these specific requirements can be fulfilled using single polarized probes for narrow frequency bands (about 10% relative bandwidth) and using mechanical rotation for polarization diversity. Consequently, several sealed probes and complicated procedures are necessary to cover the operational frequency band of most common antenna applications leading to inefficient and time-consuming measurement procedures. SATIMO has developed high precision wide-band, dual polarized near field probes covering the frequency range from L to Ka-band to overcome this problem. Two different probe technologies have been applied, each particularly well suited for the appropriate low (L to X-band) and high (X to Ka-band) frequency range. The low frequency probe design is based on a compact corrugated horn with capacitive orthogonal excitations. The high frequency probe design consists of an axially symmetric corrugated horn, a square to circular wave-guide transition, and a wide-band, high isolation ortho-mode junction (OMJ) exciting the orthogonal polarizations. Probes in C-band and Ku-band have been delivered to and tested by ALCATEL SPACE INDUSTRIES in their planar near field antenna test range in Toulouse. The C-band probes have operational bandwidths of 25% covering the entire commonly used transmit and receive frequency bands for C-band communication satellites. The Ku-band probes have operational bandwidths of 40% covering the entire commonly used transmit and receive frequency bands for Ku-band communication satellites.

Ultra-Wide Band and Ultra-Wide Angle (UWB/A) SAR Antenna Design and Analysis With Measured Results
J.S. Gwynne (Mission Research Corporation),G.R. Salo (Mission Research Corporation), November 2002

Ultra-Wide Band (UWB) antenna descriptors have been used to design an optimal Log Periodic Dipole Array (LPDA) antenna for the Army Research Laboratory’s (ARL) BoomSAR. Although dispersive in nature, the LPDA design offers improvements over existing antennas with broader beamwidth, higher efficiency, and improved off-boresight polarization performance. In the UWB/A SAR application, it is important that the antenna polarimetric spectral response remains coherent and uniform over the aspect angles used in the image formation process. This paper describes the process by which these goals were achieved and presents measured results from the BoomSAR of trihedrals and cylinders that validate the approach.

How to Choose an Antenna Range Configuration
D. Gray (Nearfield Systems, Inc.), November 2002

Choosing the proper antenna range configuration is important in making accurate measurements and verifying antenna performance. This paper will describe the steps involved so the antenna engineer can select and specify the best antenna range configuration for a given antenna. It will describe the factors involved in choosing between near-field systems versus far-field systems, and the different scan types involved. It will explain the advantages of each type of antenna range and how the choices are affected by such factors as aperture size, frequency range, gain, beamwidth, polarization, field of view, sidelobe levels, and backlobe characterization desires. This paper will help the antenna engineer identify, understand, and evaluate the applicable characteristics and will help him in specifying the proper antenna range for testing the antenna.

Outdoor Broadband RCS Measurements of Model Scale Aircraft
J.R. Rasmusson (Swedish Defence Research Agency),J. Rahm (Swedish Defence Research Agency), N. Gustafsson (Swedish Defence Research Agency), November 2002

In real life, most radar targets are located outdoors. Here we present results from outdoor broadband RCS measurements at the X-, Ka- and W-band of “Holger”, a metallized model-scale aircraft with cavities. RCS vs. angle data in the wing plane (0° elevation) were recorded at discrete frequencies (9, 35 and 94 GHz) in both horizontal (HH) and vertical (VV) polarizations. ISAR data at 7-13, 32-38 and 92-97 GHz were acquired. Results from a 104.1 m ground range and a 162.7 m free space range will be compared.

Portable Dechirp-On-Receive Radar
S.E. Gordon (Sensor Concepts Inc.),M.L. Sanders (Sensor Concepts Inc.), November 2002

Sensor Concepts Inc. has prototyped a fast, lightweight, dechirp-on-receive radar called the SCI-Lr to provide the capability of a range instrumentation radar in a highly portable package. The small weight, size and power requirements of the SCI-Lr allow a variety of new deployment options for the user including in a small general aviation aircraft or on a mountaintop that is accessible only by four wheel drive. Pulse rates up to 20 KHz enables investigation of high Doppler bandwidth phenomenon such as ground vehicle microdoppler features. The dual integration from dechirp-on-receive matched filtering in fast time and Doppler processing in slow time provides high sensitivity with low output power. Planned enhancements of waveform bandwidth up to 2 GHz , frequency operation between .2 and 18 GHz and pulseto- pulse polarization switching will provide high information content for target discrimination. The flexibility provided by the hardware is augmented by software tools to examine data in near real time to monitor data quality and sufficiency. A variety of applications are being investigated including RCS measurement, SAR and ISAR imaging, Ground Moving Target Indication, and signature collection for ATC.

Simultaneous Axis Motion Applications in Antenna and Radome Measurements
J.F. Aubin (ORBIT/FR, Inc.),C.J. Arnold (ORBIT/FR, Inc.), K. Flood (ORBIT/FR, Inc.), November 2002

This paper describes the use of simultaneous axis motion for various antenna, RCS, and radome applications, and the use of off the shelf hardware to support the corresponding measurement requirements. This is particularly relevant to polarization, low reflectivity target characterization, and radome measurements. Specific motion profiles required to accomplish various classes of tests are discussed, along with the implications on the mode of operation of the measurement system in order to achieve the most efficient collection of the required data. These simultaneous axis motion requirements may typically be user defined from the available set of axes composing the positioning system. Evaluation of the speed and real time tracking capability of the multiple axes are examined as they relate to the accuracy of the measurements that are required.

Ground Vehicle Tracking Performance of Low-Cost 3.5 GHz Ground Wave Radar
T. Ustun (The Ohio State University),E.R. Walton (The Ohio State University), November 2001

This paper will discuss the design and performance of a small step-frequency homodyne monopulse radar. The radar is designed to sit on the ground and penetrate weedy foliage to observe moving vehicles. It operates with horizontal polarization near 3.3 GHz with approximately 500 MHz bandwidth. Only 8 dBm power is needed. We will show the results of tests done with a corner reflector and with a walking human. Tracking performance in both range and azimuth will be shown.

Error Analysis of Circular-Polarization Components Synthesized From Linearly Polarized Measurements
P.N. Betjes (Nearfield Systems, Inc., Europe), November 2001

A usual way of performing pattern-measurements on circularly polarized antennas is by measuring the linear components of the field and mathematically converting those to the left-hand and right-hand circular components. These synthesized circular components are sensitive for a number of factors: The exact orthogonality of the measured linear components, the measurement-accuracy of both phase and amplitude of the measured linear components, the polarization-pureness (or the accuracy of the description of the polarization-characteristics) of the probe, etc. This paper analyzes these factors, using a computer-model. An indication on the requirements to be imposed on the measurement-equipment is provided.

A Truck-Based Multifrequency SAR Platform
G. Rubin (System Planning Corporation),B. Noviello (System Planning Corporation), E. Sager (System Planning Corporation), R. Reynolds (System Planning Corporation), G. Easley (System Planning Corporation), J. Zimmerman (System Planning Corporation), November 2001

The growing need for a mobile radar system able to conduct measurements away from fixed radar ranges has prompted System Planning Corporation (SPC) to develop a mobile MkV radar system. Planned helicopter-based SAR measurements generated a requirement for a ground-based platform to verify functionality of X-band and VHF/UHF data collection and processing systems. Accordingly, SPC developed TruckSAR, a DGPS-equipped mobile testbed to collect side-looking and normal-incidence SAR data. Interleaved step chirp data were collected at 9.0-9.3 GHz (HH polarization) and 150-450 MHz (HH, VV, HV, and VH polarization). The system is self-contained and is proving useful for applications beyond ground and foliage penetration SAR investigations. This paper describes the TruckSAR hardware and data analysis systems. Results of measurements are presented, along with observations of challenges in data interpretation. Promising extensions of this mobile ground-based radar are also discussed.

Broadband, Dual Linearly-Polarized Antenna With Controllable Beamwidth
P.A. Diaz (ElectroScience Laboratory),C-C Chen (ElectroScience Laboratory), W.D. Burnside (ElectroScience Laboratory), November 2001

The OSU/ESL has been developing a broadband, dual-polarized dielectric horn antenna (DHA). This antenna has some attractive characteristics such as dual-polarization, good antenna isolation and stable beamwidth. By adjusting the geometry, the beamwidth of the E- and H-plane patterns can also be controlled independently. Critical design issues that affect the DHA performance include launch structure, lateral-wave elimination and dielectric constant will be addressed. A design example will be provided with a prototype DHA antenna constructed and tested for 2~14 GHz frequency range with a 110o beamwidth in both Eand H-planes. The antenna isolation was found to be greater than 30 dB for this prototype. The new DHA antenna could have wide applications in which broadband, dual-polarization operation, independent E- and H-plane beamwidths are desired.

Broadband Dielectric Probe for Near Field Measurements
C-C Chen (ElectroScience Laboratory),P.A. Diez (ElectroScience Laboratory), W.D. Burnside (ElectroScience Laboratory), November 2001

A novel broadband dielectric rod probe design that has the characteristics of broad bandwidth; symmetric probe pattern; low RCS; low antenna clutter and dual polarization operation is discussed. The RCS level reduces the interaction between the probe and antenna under test (AUT). The lower antenna clutter level improves the sensitivity in detecting responses from wide angles with greater time delays. During the transmission mode, the rod is excited with a broadband microwave launcher from one end. The radiation then occurs at the other terminal of the rod. Measurement results of the far-field patterns, RCS and reflection coefficient for a prototype rod probe (DRP) are presented.

Experimental Studies With Comparisons to Computational Model for Automobile Antennas
Y. Kim (ElectroScience Laboratory),E.K. Walton (ElectroScience Laboratory), November 2001

A series of experimental and theoretical tests designed to develop techniques for reliable computational modeling of automobile antenna performance is presented. The results from the experimental measurements are compared with the results of computational techniques to verify their accuracy and reliability. The Electromagnetic Surface Patch (ESP5) code, a theoretical Method of Moment (MoM) general-purpose code developed at the Ohio State University, is used for computational modeling. We progress from the simple geometry of a single square plate and a monopole, to the more complex structure of a small copper-coated plastic model of an automobile. The computational simulation and measurements are configured with both a monopole antenna mounted at the center of the automobile roof and a backlite heater grid FM antenna. The input impedance, pattern, and polarization are all measured. Comparisons between the results of the computational simulations are presented, as well as the procedures used to measure the antenna characteristics and compare the experimental data with the measured data.

Advanced Compact Antenna Test Range Quiet Zone Characterization and Extension Techniques
B. Buralli (ALCATEL SPACE INDUSTRIES),C. Bouvin (ALCATEL SPACE INDUSTRIES), C. Nardini (ALCATEL SPACE INDUSTRIES), G. Forma (ALCATEL SPACE INDUSTRIES), H. Garcia (ALCATEL SPACE INDUSTRIES), M. Vacarella (ALCATEL SPACE INDUSTRIES), November 2001

Telecommunication satellites capacity growth has lead to a new generation of antennas , larger in size and with extremely sharp performance in terms of gain , cross polarization and coverage isolation (frequency re-use). In order to test such kind of antennas (the largest one is a Ku-band 3.6 m diameter and 6 m focal length reflector antenna) Alcatel Space Industries has implemented several innovations in its Compact Antenna Test Range (CATR): - a powerful and flexible machine has been invested , which provides 6 degrees of freedom (the machine has been called “6DOF Table”) in a wide range of motion to any satellite, allowing to bring any antenna of this satellite into the quiet zone - thanks to this new machine a series of accurate scanner probing has been performed , not only in the central plane of the quiet zone , but also on an eight meter range along the Angle Of Arrival (AOA) of the CATR - the quiet zone has been extended by one meter in height thanks to defocusing techniques; this extension has been modeled with GRASP 8 and tested using the vertical degree of freedom of the “6DOF Table” and a very accurate scanner. - In addition , the Cross polarization of the quiet zone has been tested with high dynamic ranges, using very high purity gridded horns . An average Cross polarization isolation better than 55 dB has been evidenced.

Accurate Gain Calibration With Corrugated Horns
L.G.T. Van de Coevering (March Microwave Systems B.V.),S.C. van Someren (March Microwave Systems B.V.), V.J. Vokurka (March Microwave Systems B.V.), November 2001

A method is presented for calculating the gain of corrugated conical horns. It is based on basic symmetry conditions of circular or conical waveguide mode fields. This formulation allows to derive the radiation pattern over a complete sphere form two principal polarization patterns (E- and H-plane patterns). This method can be applied for both theoretical or experimental patterns, respectively. The theory has been verified experimentally with measurements carried out on two different ranges. The results agreed within 0.05 dB or less in all situations.

Quasi-Optical Waveguide Modeling Method for Scattering Matrix Measurements in the Near Millimeter and Submillimeter Wave Regions
V.K. Kiseliov (National Academy of Sciences of Ukraine),P.K.. Nesterov (National Academy of Sciences of Ukraine), T.M. Kushta (National Academy of Sciences of Ukraine), November 2001

Earlier (AMTA'97, AMTA'98), we have proposed a new low-cost laboratory method named the quasi-optical waveguide modeling (QWM) method to study power and amplitude-phase scattering characteristics of objects, in particular the RCS of targets or their scale models, in the near millimeter (NMM) and submillimeter (SMM) wave regions. A specific feature of this technique in that an investigated object (or its scale model) is mounted inside a quasi-optical waveguide structure in the form of a hollow dielectric waveguide (HDW), in which the scattering characteristics of the waveguide dominant HE11 mode are determined. These characteristics are related to the wanted scattering characteristics of the test object in free space by definite relationships. At the same time the HDW serves several functions: it forms a quasiplane incident wave within the scattering area where test object is placed, performs the low-loss and low-distortion transmission of the scattered wave carrying information of the object being tested to the receiver, effectively filters the unwanted modes arising at the scattering on the test object, and insulates the measurement area from the ambient conditions containing parasitic sources. In this paper we consider the possibility of using the QWM method to study polarization backward scattering characteristics of physical objects, in particular the complex elements of the scattering matrix with relative phase (SMR). A quasi-optical polarimetric micro-compact range (PMCR) based on the circular HDW and quasi-optical devices has been developed and built. The measurement results of the SMR and backward scattering patterns of a reference object as a square metallic cylinder obtained in the PMCR for the different linear polarization basic sets at the 4-mm wave band are presented. The comparison between the experimental results for the reference object and the theoretical data calculated by the geometrical theory of diffraction have shown a good agreement, and demonstrated the possibilities of the QWM method, and its good perspectives for backward scattering polarization characteristics modeling in the NMM and SMM wave regions.

Application of the NIST 18 Term Error Model to Cylindrical Near-Field Antenna Measurements
A.C. Newell,D. Lee, November 2000

This paper describes error analysis and measurement techniques that have been developed specifically for cylindrical near-field measurements. A combination of analysis and computer simulation is used to show the comparison between planar and cylindrical probe correction. Error estimates are derived for both the pattern and probe polarization terms. The analysis is also extended to estimate the effect of position errors. The cylindrical measurement geometry is very useful for evaluating the effect of room scattering from very wide angles since scans can cover 360 degrees in azimuth. Using a broad beam AUT and scanning over a large y-range provides almost full spherical coverage. Comparison with planar measurements with similar accuracy is presented.

Dielectrically-Loaded Horns for Use as Antenna Measurement Range Illuminators
K.J. Greene,C. Granet, November 2000

The design of hybrid-mode dielectrically-loaded horns [1][2] for antenna test range illumination is described. These horns have a wide operating bandwidth of 5:1 or greater and were designed to replace conventional corrugated- or smooth-walled illumination horns that, typically, have a bandwidth of 2:1or less. Dielectrically-loaded horns have the radiation characteristics desirable for test range illumination: principal plane pattern symmetry, reasonably low cross-polarization and low sidelobes, low reflection coefficient and relatively constant beamwidth. At CSIRO we have developed software and manufacturing techniques to design and make these horns accurately. Measured results, that show close agreement with predicted values, are presented for a horn made for the frequency range, 7 to 40 GHz.

Raytheon 23' x 22' 50GHz Pulse System
T. Speicher,A. Puzella, J.K. Mulcahey, November 2000

Nearfield Systems, Inc. in Carson, California delivered a vertical 23' by 22' (7.0m x 6.7m) near-field test range to Raytheon Electronic Systems in Sudbury, Massachusetts. This planar and cylindrical measurement system is capable of characterizing antennas of various physical sizes in continuous wave or in pulse mode from 800MHz to 50GHz. The near-field measurements are computer controlled and capable of multiple frequency, multiple beam and multiple polarization in AUT transmit or receive modes. The precision robotic system uses a Data Acquisition Controller running NSI software to provide four-axes for probe positioning and three-axes for antenna positioning. The RF subsystem is based on the HP 8530A microwave receiver, HP 83630B RF source, HP 83621A LO source and HP 85309A LO/IF Distribution Unit. The test range was evaluated using the NIST 18- term error analysis on a 45GHz 54" diameter left-hand circular polarized reflector antenna.

Ground Bounce Reduction Using a Tapered Resistive Sheet Fence
Y. Kim,E.K. Walton, November 2000

One problem in a RCS ground bounce range is that the direct signal can be interfered with by the ground reflected signal. The undesired ground bounce signal will cause errors in the RCS measurement. This paper presents a study of ground bounce reduction using a tapered and stepped resistive sheet fence. In order to show that the proposed R-card fence technique can reduce the ground reflected signal significantly, both experimental and theoretical studies are performed. The resistance of the R-card varies based on a Kaiser-Bessel taper function. The experimentall results with and without the R-card fence show that the ground reflected signal can be attenuated by about 20dB. Both vertical and horizontal polarization cases are considered. This paper also the results of a simulation using NEC-BSC (Numerical Electromagnetic Code - Basic Scattering Code, developed at The Ohio State University ElectroScience Laboratory). Comparison of the results between measurements and simulations will be shown in this paper.







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