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Compact and Spherical Range Design, Application and Evaluation. Walter D. Burnside and Inder J. Gupta The Ohio State University ElectroScience Laboratory 1320 Kinnear Road Columbus, Ohio 43212 (614) 292-5747 and (614) 292-5951. Presented on September 21-22, 2005 for Raytheon (Tucson, AZ).
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Compact and Spherical Range Design, Application and Evaluation Walter D. Burnside and Inder J. Gupta The Ohio State University ElectroScience Laboratory 1320 Kinnear Road Columbus, Ohio 43212 (614) 292-5747 and (614) 292-5951 Presented on September 21-22, 2005 for Raytheon (Tucson, AZ).
Basic Range Design Guidelines (Burnside) Compact Range Reflector Design (Gupta) Absorber Design and Layout (Burnside) Critical Range Evaluation (Gupta) Course Outline First Full Day Second Half Day • R-Card Fences for Outdoor Ranges (Gupta) • Summary of Range Design Issues (Burnside)
Compact Range Reflector Design Inder (Jiti) Gupta ElectroScience Laboratory Electrical & Computer Engineering Dept. The Ohio State University 1320 Kinnear Raod Columbus, OH 43212 Phone: 614-292-5951 Fax: 614-292-7297 Email: gupta.11@osu.edu
Design parameters Feed location Reflector size Focal length Edge treatment Performance comparison Serrated edge Rolled edge reflector Low frequency reflector design Outline
Floor Side wall Near a walkway (corner fed system Subreflector fed system Feed Location
Aperture blockage, feed accessibility and focal length are the main factors. Subreflector fed is the most desired but is also the most expensive Corner fed system also provides good feed accessibility and low aperture blockage. Focal length can be a little large. Feed Location
Reflector Size Minimum reflector size is 20 lmin x 20 lmin, where lmin is the wavelength at the lowest frequency of operation.
To keep the length of the range small, the focal length should be the shortest possible. A small focal length will lead to large taper and high cross-polarization in the quiet zone fields. Conventionally, for a single reflector system (no subreflector), the focal length is selected such that the angle from the feed to the center of the reflector is 25° - 30°. Assuming a 20l x 20l reflector and a 28° feed tilt angle, the focal lengths for various reflectors are Floor-fed ≈ 20l Side wall-fed ≈ 20l Corner – fed ≈ 27.5l Focal Length
Edge treatment is applied to the compact range reflector to reduce the reflector edge diffracted fields in the quiet zone. The two most popular edge treatments are Edge serrations. Rolled edges. Edge Treatment
The whole reflector is a section of a paraboloid. For optimum performance, the serrations should be designed such that the edge diffracted rays do not reach the target zone. One can use ray tracing to design serrations. Serrated Edge Reflectors
The edge diffracted rays lie on a conical surface. The angle between the conical surface and the edge is equal to the angle between the incident ray and the edge. Since the feed location and the edge is known, the conical surface is well defined. In the design of serrations, one makes sure that the conical surface does not intersect the quiet zone. For design purposes, the quiet zone is defined by a rectangle or an ellipse on a vertical plane which passes through the center of the quiet zone and is perpendicular to the desired planar wavefront. We have developed an iterative computer code for the design of serrations. Serrated Edge Reflectors
The computer code is used to design serrations for a 20l x 20l floor-fed reflector. Note that the basic reflector size is 10l x 10l. The focal length of the reflector is 20l. The performance of the reflector is evaluated using physical optics (PO) plus a PTD edge correction. An AEL horn is used to illuminate the reflector. Serrated Edge Reflector
As expected, the performance improves with an increase in the size of serrations. Considering the cost issue, 5l serrations are a good choice. One should add a serration every 1.5l to 2l. Serrated Edge Reflector
The elliptical section is added to the rolled edge such that the slope of the surface is continuous The semi-major axis and the semi-minor axis of the ellipse are selected such that the total size of the reflector does not exceed the desired limit the minimum radius of curvature of the rolled edge is l0/4 where l0 is the wavelength at the lowest frequency of operation. Rolled Edge Reflector
where Rolled Edge Reflector Surface and g is a parametric angle such that 0 ≤ g ≤ gm
Note that gm defines how much of the ellipse is used as the rolled edge. Choice of gm does not affect ae or be. For cost reasons, gm is kept small. Normally 105° ≤ gm ≤ 150° Rolled Edge Reflector Surface
where b(g) is the blending function which varies between [0,1] such that b(0) = 0 and b(gm) = 1. Blended Rolled Edge Reflector
The extended parabola is defined as where xm defines the section of the parabola used in blending. Note that for a given junction height one can select ae, be, xm and gm to satisfy various design constraints. One also has to select the blending function. Blended Rolled Edge Reflector
The blending function is chosen such that its first (n-1) derivatives are zero at the junction. Let us call such a function an nth order blending function. For an nth order blending function, the radius of curvature of the surface and its first n-1 derivatives are continuous across the junction. The higher order blending functions, however, are effective for large rolled edges. A cosine blending function is recommended. Blended Rolled Edge Reflector
Cosine blending is a second order blending function. Thus, the surface curvature and its first derivative are continuous across the junction. The discontinuity in the second derivative of the radius of curvature is given by where One can select ae, be, xm and gm such that = 0. However, one has to meet the other two design constraints; the total height the minimum radius of curvature Blended Rolled Edge Reflector
The two constraints can be defined as and where hmax is the maximum desired height of the reflector surface, h is the total height of the reflector, and Rsh is the radius of curvature of the reflector at the incident shadow boundary. One can select ae, be, xm and gm to minimize 2 under these two constraints. A Lagrange multipliers method can be used for optimization. The function is then defined by where L1 and L2 are the Lagrange multipliers. Blended Rolled Edge Reflector
The function G is not well behaved. One can fix gm and vary ae, be and xm to minimize G. For (105° ≤ gm ≤ 150°), the minimum value of G is approximately the same. Blended Rolled Edge Reflector • For large value of ae, the error term ( 2) increases very rapidly. • For small values of ae the increase in the error term is rather slow. • One should select ae such that it is smaller than its threshold value and then should find be and xm to satisfy the two constraints for a given gm.
The blended rolled edge should be added such that the total surface is smooth and continuous The choice of the rolled edge plane for various points on the reflector rim is important. Blended Rolled Edge Reflector
Let (xav, yav, zav) be the center of the reflector. Define a new coordinate system, such that x = x′ + xav y = y′ + yav z = z′ + zav Next, define a cylindrical coordinate system (r′, f′, z′) such that x′ = r′ cosf′ y′ = r′ sinf′ z′= z For a given f′, the rolled edge is added in the (r′,z′) plane. Blended Rolled Edge Reflector
In the cylindrical coordinate system, the reflector surface is defined as where 0 ≤ f′ ≤ 2p, and 0 ≤ r′ ≤ rj′(f′) . For a given f′, the above equation represents a parabola of focal length F. The vertex of the parabola is at The junction height in the rolled edge plane is One can use the 2-D procedure to add the rolled edge and obtain the rolled edge parameters. Since the height of the junction, rj′′, varies with f′, the rolled edge parameters will vary with f′. The variation, however, is slow. Blended Rolled Edge Reflector
Illustrative Example 10l x 10l floor-fed reflector 20l focal length 5l rolled edge Total reflector is 20l x 20l Blended Rolled Edge Reflector
PO edge correction is used for analysis. The same results hold true for higher frequencies. Blended Rolled Edge Reflector
Focal length = 20ll. A broadband double ridge AEL horn is used as the feed. The test zone is located at 35l from the vertex of the reflector. Performance Comparison
Contour plot of the quiet zone field magnitude. Frequency of operation is 2fl. Performance Comparison Serrated edge reflector Rolled edge reflector
Antenna Measurement Two phase scanned arrays of isotropic elements. One of the antennas is 6ll x6ll, whereas the second antenna is 8ll x 8ll. The amplitude taper of the antenna array is defined by a Kaiser-Bessel function, such that the first sidelobe is more than 40 dB below the main-lobe level. The phase of the array elements is adjusted to scan the beams in the azimuthal plane. Frequency of operation is 2fl. Performance Comparison
Measured and actual pattern of the 6ll x 6ll antenna. Performance Comparison Serrated edge reflector Rolled edge reflector
Measured and actual pattern of the 8ll x 8ll antenna. Performance Comparison Serrated edge reflector Rolled edge reflector
Scattering Measurement Two diagonal flat plates of sizes 4ll x 4ll and 6ll x 6ll, respectively For each rotation angle, the incident fields on the plate are calculated. Next, the equivalent surface currents on the plate are calculated and integrated to obtain the far-zone scattered fields. Frequency of operation is 2fl. Performance Comparison
Measured and actual scattered fields of the 4ll x 4ll plate. Performance Comparison Serrated edge reflector Rolled edge reflector
Measured and actual scattered fields of the 6llx 6ll plate. Performance Comparison Serrated edge reflector Rolled edge reflector
The blended rolled edge reflector performs better for antennas as well as for scattering measurements. The blended rolled edge reflector is, however, costly. The blended rolled edge reflector illuminates the walls, ceiling and floor of the chamber more strongly than the serrated edge reflector, but the impact of this on the measurement accuracy can be made negligible by lining the inside of the chamber with good absorbing material. Performance Comparison
In the previous design, the compact range reflector was designed for a target size of 10lmin or larger, where lmin is the wavelength at the lowest frequency of operation. An important parameter in the selection of a measurement range is the chamber size. For a shperical range, the range size is given by ND2/l, where D is the largest target dimension. N is normally selected between one and four. For a compact range system the range size is approximately 4D. Low Frequency Reflector Design
Range size versus the target size Low Frequency Reflector Design
A 20l x 20l reflector is used to control the edge diffraction in the quiet zone. By properly selecting the rolled edge parameters in a compact range reflector, one can reduce the diffracted fields to very low values. In a blended rolled edge reflector the edge diffracted fields are controlled by extending the parabolic reflector such that the resulting reflected fields are smooth and continuous The concept could be extended to much lower frequencies. Low Frequency Reflector Design
The edge diffracted fields, as expected, decrease with an increase in the rolled edge size. A reflector with total height of 90’ to 100’ should be able to measure a 30’ target at 100 MHz and higher frequencies. The reflector is inefficient in the sense that the potential target zone is less than half of the total size of the reflector. In the case of blended rolled edge reflectors, one can trade the parabolic section with the rolled edge section (up to a certain limit) without any significant degradation in the quiet zone fields. A part of the blended rolled edge can also be used to generate a planar wavefront. Low Frequency Reflector Design
Low Frequency Reflector Size Reflector parameters for various sizes of test zones Minimum frequency = 100 MHz
3-D Reflector 30’ target at 100 MHz Total reflector size 90′ x 90′ Potential target zone 45′ x 45′ Floor-fed system with focal length 84′ Concave rim Cosine blended rolled edge Low Frequency Reflector Design
Front view of the 3-D reflector to measure 30-ft target at 100 MHz and above frequencies Low Frequency Reflector Design
Quiet zone fields of the 3-D reflector at the back end of the target zone. Frequency = 100 MHz. Low Frequency Reflector Design
The compact range reflectors can be designed to measure targets as small as 3l. In other words, the compact range reflectors can be used to measure targets at frequencies as low as 3c/D, where c is the velocity of light and D is the largest dimension of the target. For lower frequencies, one should consider a spherical range. Low Frequency Reflector Design
Conventional reflector design Serrated edge reflector Rolled edge reflector Compared the performance of a rolled edge reflector to a serrated edge reflector Low frequency reflector design. Compact Range Reflector Design (Summary)
W.D. Burnside, M.C. Gilreath and B.M. Kent, “Rolled edge modification of compact range reflector,” AMTA’84, San Diego, CA. W.D. Burnside, A.K. Dominek and R. Barger, “Blended surface concept for a compact range reflector,” AMTA’85, Melbourne, FL. C.W.I. Pistorius and W.D. Burnside, “An improved main reflector design for compact range application,” IEEE Trans. Ant. Prop., vol.35, pp.342-347, March 1987. I.J. Gupta, K.P. Ericksen and W.D. Burnside, “A method to design blended rolled edges for compact range reflectors,” IEEE Trans. Ant. Prop. Vol.38, pp.853-861, June 1990. I.J. Gupta and W.D. Burnside, “Compact range measurement system for electrically small test zones,” IEEE Trans. Ant. Prop., vol. 39, pp. 632-638, May 1991. T.-H. Lee and W.D. Burnside, “Performance trade-off between serrated edge and blended rolled edge compact range reflectors,” IEEE Trans. Ant. Prop., vol. 44, pp. 87-96, January 1996. T.-H. Lee and W.D. Burnside, “Compact range reflector edge treatment impact on antenna and scattering measurements,” IEEE Trans. Ant. Prop., vol. 45, pp. 57-65, January 1997. References