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Radar

Productivity improvements for a gated-CW radar
J.B. Wilson (Scientific-Atlanta, Inc.), November 1990

This paper will describe new developments in a gated-CW radar that has been designed to improve the productivity and sensitivity of RCS measurements. Improvements in data acquisition speeds result from the design of a fast synthesizer, a data acquisition co-processor and a pulse modulator. Each of these new products have been specifically designed to take advantage of the high speed capabilities of Scientific-Atlanta’s Model 1795 Microwave Receiver. The RF sub-system has also been designed to permit continuous 2-18 GHz, full polarization data acquisitions. Critical RF components are now mounted at the feed in the chamber, improving the sensitivity and ringdown of the system. Productivity in analysis activities has been improved by the use of a multi-tasking system controller which permits simultaneous use of the system for acquisitions, analysis and plotting.

Monostatic and bistatic polarimetric radar cross section measurements on canonical targets
S. Mishra (Canadian Space Agency),J. Mantz (Canadian Space Agency), November 1990

This paper describes results of extensive polarimetric Radar Cross Section (RCS) measurements on canonical targets. Amplitude and phase of both co- and cross- polar returns are measured for horizontally and vertically polarized transmit signals in order to determine the complete complex scattering matrix. Measurements have been carried out on a variety of targets. Results presented with this summary show data for a metallic and a dielectric disk. Details of measurement and calibration procedure, hardware, and software are also presented.

Radar cross section measurements in a reflecting chamber
E. Walton (The Ohio State University ElectroScience Laboratory),L. Beard (The Ohio State University ElectroScience Laboratory), November 1990

This paper is concerned with the measurement of RCS in a room with conducting walls. The experimental measurement system uses a moving antenna to produce a scan of the target and the clutter. The scattered signal as a function of frequency and position is recorded. New field crossrange processing is then used to map the target zone. Example images will be shown for both two-dimensional and one-dimensional scans. Images from point targets and distributed targets will be presented.

Multipath effects on radar cross section measurements
A.J. Stoyanov (Douglas Taylor Research Center),M.A. Sekellick (Douglas Taylor Research Center), W.H. Schuette (Douglas Taylor Research Center), Y.J. Stoyanov (Douglas Taylor Research Center), November 1990

Accurate radar measurement of complex marine targets from a shore-based radar are difficult to achieve because of the effects of a multipath environment. This paper summarizes multipath effects at low and very low grazing angles. The investigation of scattering from the sea surface and from marine targets is important for radars operating at low elevation angles over a sea surface because severe fading and distortions in measured target radar cross section can occur due to multipath propagation. It can be shown that the lobing structure due to the interference of the direct and reflected signal is still a problem for very low elevation angles even in high sea states, suggesting a limited usefulness for low elevation radar cross section measurement sites. Further it has been observed that in the microwave region at elevation angles smaller than 0.5 degrees, scattering centers located at certain heights above the sea surface may be masked. At higher elevation angles, however, multipath interference is reduced, thus giving a more stable basis for measurement and evaluation.

Correction/calibration of wide-band RCS radar data containing I/Q error
D.E. Pasquan (Texas Instruments Incorporated), November 1990

In-phase and quadrature (I/Q) aberrations in radar receiver data create problems in radars used for radar cross section (RCS) measurements. I/Q errors cause incorrect representations of the target under test. A method for correcting I/Q error and calibrating the measured amplitude to a scattering standard provides a means of obtaining a more accurate representation of the target under test. The RCS measurement instrumentation addressed here uses a wide band receiver with a single quadrature mixer for conversion of radio frequency (RF) to base band (also referred to as video) frequency. In the one-step down conversion, distortions in the I/Q constellation occur, causing I/Q errors. This method quantifies the extent of the I/Q problem by estimating the actual I/Q error from a series of calibration measurements. An algorithm is presented which quantifies parameters of the I/Q distortion, then uses the distortion parameters to remove the I/Q aberrations from the target measurement.

Short term stability performance of pulsed instrumentation radars using TWTAS
J. Allison (Hughes Aircraft Company),J. Paul (Hughes Aircraft Company), R. Santos (Hughes Aircraft Company), November 1990

Pulse-to-pulse amplitude and phase noise can affect the overall measurement accuracy of RCS instrumentation radars. Depending upon the measurement requirements, such noise can limit the overall performance whenever pulse-to-pulse repeatability is required in the signal processing. Radar systems using pulsed TWTAs are subject to high noise due to limitations in the performance of the TWTA modulators and power supplies. A characterization of this additive noise is important to understand the limitations in system performance. Measurements have been made on kilowatt power TWTAs at L and X band as well as 20 watt pulsed TWTAs at S, C, and X/Ku band at various duty cycles and PRFs.

Coherent RF measurements with a long reference path
M.C. Li (Naval Research Laboratory), November 1990

In coherent measurements, one measures the interference of signals from test and reference paths. These techniques are widely used in RF image measurements of antennas and radar cross sections. The success of a coherent measurement depends highly upon the stability of the path length difference between test and reference signals as well as the quality of the reference signal. The stability and quality are hampered when the experiment has to be conducted with a long reference path length, particularly at outdoor ranges. A new measurement scheme, based on the scattering process initiated by two coherent beams, will be presented here are has the advantage over others in reducing the problems associated with the path length difference instability.

The Test and set-up of spaceborne, active SAR antennas
P. Miller (Marconi Space Systems Ltd.),J. Reddy (ESA/ESTEC), November 1990

This paper presents an overview of the test and set-up requirements of active Synthetic Aperture Radar (SAR) antennas. The specific antennas under consideration are those that are intended to be used in the next generation of spaceborne SAR C-Band satellites. These antennas are typically 1m to 2m wide and 10m to 20m long, possessing between 3000 to 12000 radiating elements. The paper considers each unit of the active antenna in turn and identifies which tests are to be carried out where. In considering the test of the whole antenna some initial result of focussing techniques, to allow the antenna to be tested in real time at reduced distance, are presented.

Wideband polarimetric determination of antenna radiation and scattering characteristics by RCS-measurements
E. Heidrich (University Karlsruhe),W. Wiesbeck (University Karlsruhe), November 1990

A novel and very powerful measurement technique is presented which allows the determination of antenna radiation and scattering by radar-cross-section (RCS-_ measurements. The antenna under test is treated as a loaded scatterer using a polarization dependent network model that allows a complete antenna description in terms of scattered, radiated and absorbed waves. A load variation principle is used to determine the network model parameters and all commonly used antenna parameters like gain, antenna polarization, axial ratio, polarization decoupling, input impedance and also structural scattering can be derived from the backscatter measurement without using any additional standard antenna. With the antenna network description it is furthermore possible to examine the antenna behavior for arbitrary excitation or loading on their waveguide or radiation port.

An Overview of parameters determining productivity and sensitivity in RCS measurement facilities
E. Hart (Scientific-Atlanta, Inc.),W.G. Luehrs (Scientific-Atlanta, Inc.), November 1990

A major objective in the design of an RCS measurement facility is to obtain the greatest possible productivity (overall measurement efficiency) while maintaining the accuracy and sensitivity necessary for low radar cross section targets. This paper will present parameters affecting the total throughput rates of an indoor facility including instrumentation, target handling, and band changes-one of the most time consuming activities in the measurement process. Sensitivity and accuracy issues to be discussed include radar capabilities, feeds and feed clustering, compact range, background levels, and diffraction control.

Hughes Aircraft Company's new RCS measurement facility
A.R. Lamb (Hughes Aircraft Company),R.G. Immell (Denmar, Inc.), November 1990

The Hughes Aircraft Company recently completed the design, development, and construction of a new engineering facility that is dedicated to providing state-of-the-art Radar Cross Section Measurements. The facility is located at the Radar Systems Group in El Segundo, California and consists of two secure, tempest shielded anechoic chambers, a secure high bay work area, two large secure storage vaults, a secure tempest computer facility, a secure conference room, and the normal building support facilities. This RCS measurement test facility is the result of Hughes committing the time and money to study the problems which influence user friendly RCS measurement facility design decisions. Both anechoic chambers contain compact ranges and RCS measurement data collection systems. A description of the facility layout, instrumentation, target handling capability, and target access is presented.

The New French anechoic chamber for wide band RCS measurements
J.L. Bonnefoy (CESTA),J. Garat (CESTA), J. Saget (Dassault Electronique), J.P. Behaegal (Dassault Electronique), J.P. Prulhiere (CESTA), November 1990

Among its different facilities, C.E.A. has an indoor range for radar cross section (RCS) measurements over a wide frequency range from 0,1 GHz to 18 GHz. The dimensions of this anechoic chamber, 45m x 13m x 12m and a quiet zone diameter of about 3m, make it one of the largest in Europe. It consists in a parabolic reflector for frequencies higher than 0,8 GHz and a system using inverse synthetic aperture radar (ISAR) techniques for lower frequencies associated with a short pulse coherent radar instrumentation equipment. In addition to performant instrumentation and illumination systems, the main features of this installation dedicated to measure stealth objects, are low residual clutter, discrete target supports, and powerful processing software. The technical solutions adopted are described.

Near-field testing of adaptive radar systems
A.J. Fenn (Massachusetts Institute of Technology), November 1990

Airborne or spaceborne radar systems often require adaptive suppression of interference and clutter. Before the deployment of this adaptive radar, tests must verify how well the system detects targets and suppresses clutter and jammer signals. This paper discusses a recently developed focused near-field testing technique that is suitable for implementation in an anechoic chamber. With this technique, phased-array near-field focusing provides far-field equivalent performance at a range distance of one aperture diameter from the adaptive antenna under test. The performance of a sidelobe-canceller adaptive phased array antenna operating in the presence of near-field clutter and jamming is theoretically investigated. Numerical simulations indicate that near-field and far-field testing can be equivalent.

Scale model aircraft/phased array measurements
M. O'Brien (Loran Randtron Systems),R. Magatagen (Loran Randtron Systems), November 1989

This paper describes the techniques applied to a fully automatic computer controlled, HP8510 based, range gated digital data acquisition system used to provide scale modeled large aperture synthesis, evaluation of aircraft blockage effects, array patterns, element cancellation ratios, as well as providing a large accurate data base for radar simulation exercises.

Financially justifying an antenna/RCS measurement system
J. Swanstrom (Hewlett-Packard Company), November 1989

This paper examines the economic justification process for a new Antenna or Radar Cross-Section (RCS) measurement system, and presents the techniques that can be used to determine the financial feasibility of a new system. Specific examples are given that will allow engineers to customize calculations to fit their company's specific accounting methods and labor rates.

Guided weapons radar testing
R.H. Bryan (Scientific-Atlanta, Inc.), November 1989

An overview of non-destructive real-time testing of missiles is discussed in this paper. This testing has become known as hardware-in-the-loop (HIL) simulation because it involves the actual missile hardware.

Hybrid compact radar range reflector
M.R. Hurst (McDonnell Douglas Missile Systems Company),P.E. Reed (McDonnell Douglas Missile Systems Company), November 1989

A new type of rolled-edge compact range reflector was designed and built by McDonnell Douglas Corporation. To minimize diffraction, the reflector contour was designed such that the surface radius of curvature and all its derivatives are continuous everywhere. This was accomplished by summing a parabolic function and two hyperbolic functions which have appreciable magnitude only in the edge-roll region. The bottom edge was treated using serrations.

Development of a lab-sized antenna test range for millimeter waves
J. Saget (Electronique Serge Dassault), November 1989

In the last few years, the interest in millimeter wave systems, like radars, seekers and radiometers has increased rapidly. Though the size of narrow-beamwidth antennas in the 60-200 GHz range is limited to some 20 inches, an accurate far-field antenna test range would need to be very long. The achievement of precision antenna pattern measurements with a 70' or even longer transmission length requires the use of some power that is hardly available and expensive. A cost-effective and more accurate solution is to use a lab-sized compact range that presents several advantages over the classical so-called far-field anechoic chamber: - Small anechoic enclosure (2.5 x 1.2 x 1.2 meters) meaning low cost structure and very low investissement in absorbing material. No special air-conditioning is needed. This enclosure can be installed in the antenna laboratory or office. Due to the small size of the test range and antennas under test, installation, handling and operation are very easy. For spaceborne applications, where clean environment is requested, a small chamber is easier to keep free of dust than a large one. - The compact range is of the single, front fed, paraboloid reflector type, with serrated edges. The size and shape of the reflector and serrations have been determined by scaling a large compact range of ESD design, with several units of different size in operation. The focal length of 0.8 meter only accounts in the transmission path losses and the standard very low power millimeterwave signal generators are usable to perform precision measurements. The largest dimension of the reflector is 1 meter and this small size allows the use of an accurate machining process, leading to a very high surface accuracy at a reasonable cost. The aluminum alloy foundry used for the reflector is highly temperature stable. - Feeds are standard products, available from several millimeter wave components manufacturers. They are corrugated horns, with low sidelobes, constant and broad beamwidth over the full waveguide band and symmetrical patterns in E and H planes. - The compact range reflector, feeds and test positioner are installed on a single granite slab for mechanical and thermal stability, to avoid defocusing of the compact range. - A micro-positioner or a precision X Y phase probe can be installed at the center of the quiet zone. Due to their small size, these devices can be very accurate and stable. Due to the compactness of this test range, all the test instrumentation can be installed under the rigid floor of the enclosure and the length of the lossy RF (waveguide) connections never exceeds 1 meter.

Millimeter wave compact range measurements
M.J. Lynch (Harris Corporation), November 1989

This paper discusses the configuration and performance of millimeter-wave measurement systems comprised of standard Harris Shaped Compact Ranges, Hewlett Packard (HP) 8510B Network Analyzer, and Millitech frequency extenders designed for use with the network analyzer. Millimeter-wave capabilities have been integrated into the Harris automated measurement system to allow computer controlled millimeter-wave compact range characterizations. This system offers a new measurement alternative for antenna and Radar Cross Section (RCS) measurements. Measured 35 GHz data from the Harris Model 1606 compact range, and 95 GHz data from the Model 1603 compact range are included.

Target diagnostics with high resolution multifrequency radar
R. Harris (METRATEK, Inc.),J. Gray (METRATEK, Inc.), November 1989

This paper describes methodology for performing high resolution target radar cross section (RCS) diagnostic measurements with a new type of portable multifrequency radar. The Model 200 radar system is capable of operating at extremely short ranges, and does not require an anechoic chamber for performing highly sensitive radar cross section measurements. Measurements can be made in conventional low range resolution polar plot modes, in high-range-resolution (HRR) mode, in Inverse Synthetic Aperture (ISAR) mode, and in Synthetic Aperture (SAR) mode. The radar is described and the implications for present and future measurement technology are discussed.







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