1. Field of the Invention
This invention relates to microwave reflector antennas. More particularly, the invention relates to a reflector antenna with vertex region scatter compensation via an RF reflective surface on the boom of the feed assembly, which enhances the reflector antenna signal pattern characteristics.
2. Description of Related Art
Reflector Antenna feed assemblies typically utilize a vertex plate/forward feed hub surface positioned at the proximal end of a boom (feed waveguide) supporting a subreflector proximate a focal point of the reflector dish. The vertex plate typically improves the antenna Voltage Standing Wave Ratio (VSWR), an indicator of Return Loss.
Although an ideal reflector antenna would have a radiation pattern in which the entirety of the signal radiation is directed in a narrow forward beam, significant amounts of the signal radiate in undesired directions, including to the rear of the antenna. For terrestrial microwave communication systems, the sensitivity of the antenna radiation characteristics in the rearward hemisphere is a significant parameter for systems engineers reviewing potential sources of interference. Specifically, extraneous signals received by the antennas, either from adjacent links, or from within the designed link, can severely limit the carrier to noise ratio of the radio system, and thereby ultimately limit the system carrier capacity.
The amount of signal radiation directed forward with respect to an amount also radiating backward in the reflector antenna signal pattern is quantified as the front to back ratio (F/B) of the antenna. The F/B is regulated by international standards, and is specified by for example, the FCC in 47 CFR Ch.1 Part 101.115 in the United States, by ETSI in EN302217-4-1 and EN302217-4-12 in Europe, and by ACMA RALI FX 3 Appendix 11 in Australia.
Microwave parabolic antennas can be designed to meet these stringent regulatory requirements by minimizing the antenna's sensitivity to RF signals in the rear hemisphere. Feed radiation illumination in the direction of the periphery of the main reflector dish together with the geometry of the periphery region determine, via the mechanisms of diffraction and scattering, the radiation pattern characteristics of the antenna in the rear hemisphere and at the border region between front and rear hemispheres. Electromagnetic boundary conditions at the reflector dish rim provide cancellation of the electric field to incident vertical polarisation (H-plane), but provide continuity to the electric field to incident horizontal polarisation (E-plane). Thereby the radiation pattern levels in the horizontal, E-plane, will be higher than the corresponding H-plane in this border region.
The direct feed illumination at the periphery of the reflector known as edge-illumination can be controlled by effective design of the feed radiator. Measures such as the use of RF chokes or corrugations adjacent to the radiating aperture of the feed can effectively reduce the spill-over component, for example as disclosed in commonly owned U.S. Pat. No. 6,919,855, titled “Tuned Perturbation Cone Feed for Reflector Antenna” by Hills.
However, secondary illumination of the periphery of the reflector via scattering of the direct feed illumination from the main reflector particularly from the region adjacent to the reflector vertex can significantly degrade the edge illumination and lead to poor radiation pattern control, particularly in the transition region from front to rear hemispheres and into the rear hemisphere, thus preventing compliance to regulatory specifications.
Competition in the reflector antenna market has focused attention on improving electrical performance and minimization of overall manufacturing and installation costs. Therefore, it is an object of the invention to provide a reflector antenna that overcomes deficiencies in the prior art, including reduction of scattered radiation pattern components at the border region between front and rear hemispheres, and into the rear hemispheres.
The accompanying drawings, which are incorporated in and constitute a part of this specification, illustrate embodiments of the invention, where like reference numbers in the drawing figures refer to the same feature or element and may not be described in detail for every drawing figure in which they appear and, together with a general description of the invention given above, and the detailed description of the embodiments given below, serve to explain the principles of the invention.
a and 14b are charts illustrating a series of predicted E-plane and H-plane feed radiation patterns, respectively, at discrete frequencies across a typical operating band (eg 15 GHz) using the feed illustrated in
a and 15b are charts illustrating a series of predicted E-plane and H-plane feed radiation patterns, respectively, at discrete frequencies across a typical operating band (eg 15 GHz) using the feed illustrated in
c is a chart illustrating the predicted E-plane antenna radiation pattern characteristics from the antenna design illustrated in
a and 16b are charts illustrating a series of predicted E-plane and H-plane feed radiation patterns, respectively, at discrete frequencies across a typical operating band (eg 15 GHz) using the feed of
c is a chart illustrating the predicted E-plane antenna radiation pattern characteristics from the antenna design illustrated in
The inventors have analyzed the electrical performance of conventional deep dish reflector antennas (Focal Length/Diameter, F/D<=0.25), for example as shown in
The inventors have devised a method and apparatus for minimising the E-plane reflection and scatter of undesired feed radiation from the vertex region 10 to the reflector dish periphery 12 thus enabling edge illumination similar to that predicted from the feed design before integration with the reflector antenna 2 and thereby providing design level signal discrimination at the boundary between front and rear hemispheres and improving the F/B.
The addition of a boom disc 18, as shown for example in
The inventors have observed that additional reduction in the scattered component in the direction of the reflector periphery can be achieved by the placement of Radio Frequency (RF) absorbing material 19, as shown for example in
The boom disc 18 may be formed from metal, metalized or other RF reflective material and may be dimensioned and positioned as shown for example in
Dimensions A and B are dependant on the type of feed illumination and are therefore determined by the numerical analysis based thereupon. A number of candidate axial positions can be identified each with separations of, for example, a multiple of one half a wavelength. It will be apparent to one experienced in the art that as the boom disc axial position moves closer to the subreflector 14 that the amplitude of the intercepted component will increase; the optimum position and diameter for reflection cancellation against the reflected components from the vertex region 10 in the direction of edge illumination half angle T, will therefore be dependant on the subreflector 14 configuration.
Once the first position of the boom disc 18 adjacent to the vertex region 10 has been identified, further minima at the requisite illumination half angle T are evident at spacing of multiples of one-half wavelength starting adjacent to the vertex region 10 according to the relation:
B=wavelength×(2N+1)/2,
Where N=integer
Dimension A is typically between 1.0 and 2.5 wavelengths of the desired operating frequency band.
The worse case prediction shown by
As the boom disc 18 axial position moves closer to the sub-reflector 14, a degree of obscuration of the feed radiation will occur which in turn will impact the radiation characteristics of the reflector antenna 2. Furthermore the antenna return loss will also be influenced by the presence and position of the boom disc 18. Therefore in practice, a compromise may be determined by way of numerical and/or experimental analysis such that the boom disc 18 axial position that provides optimum suppression at the boundary and F/B regions also provides the requisite antenna return loss and radiation pattern directivity in the forward hemisphere in view of the priorities assigned to each of the boundary suppression and F/B characteristics.
a thru 16c demonstrate the impact of the boom disc 18 on the E-plane and H-plane feed radiation patterns.
One skilled in the art will recognize that although the boom disc 18 is demonstrated in the exemplary embodiment as generally circular with a uniform periphery edge, the distal boom disc surface planar and normal to the boom longitudinal axis. In alternative embodiments, the boom disc shape and/or distal surface may be modified according to the desired electrical performance parameters, reflector dish and/or subreflector configuration. For example, as shown in
Edge illumination is primarily an issue with so called “deep” reflector dishes 8 using circularly symmetric self supported waveguide feed assemblies 20 where the feed edge-illumination half-angles are >90 degrees, and where stringent regulatory specifications are to be achieved without the need for a conventional RF absorber-lined shield. However, the boom disc 18 may also be used in other reflector dish configurations where specific E-plane suppression of adjacent to on-axis radiation is desired towards the periphery of the reflector dish 8.
As mentioned previously, further suppression of the radiation pattern signal in the border regions between front and rear hemispheres can also be achieved by addition of a RF absorbing material 19 placed between the rear face of the boom disc 18 and the front face of the vertex region 10—see
Additional enhancement can be achieved by use of a dielectric cylinder placed between the rear face of the boom disc and the front face of the vertex, 4. A typical dielectric constant of 2.1, corresponding to readily available PTFE, for example, can be readily designed, either empirically thru optimization on a test range, or by the use of FDTD software. The device is diameter sensitive and is typically between 1 and 5 mm in thickness.
One skilled in the art will appreciate that significant improvements to the electrical performance of the reflector antenna 2 may be achieved by the addition of the boom disc 18 vertex plate scatter compensation feature, with minimal additional manufacturing and/or installation cost.
Where in the foregoing description reference has been made to materials, ratios, integers or components having known equivalents then such equivalents are herein incorporated as if individually set forth.
While the present invention has been illustrated by the description of the embodiments thereof, and while the embodiments have been described in considerable detail, it is not the intention of the applicant to restrict or in any way limit the scope of the appended claims to such detail. Additional advantages and modifications will readily appear to those skilled in the art. Therefore, the invention in its broader aspects is not limited to the specific details, representative apparatus, methods, and illustrative examples shown and described. Accordingly, departures may be made from such details without departure from the spirit or scope of applicant's general inventive concept. Further, it is to be appreciated that improvements and/or modifications may be made thereto without departing from the scope or spirit of the present invention as defined by the following claims.
This application claims the benefit of U.S. Provisional Patent Application No.: 61/286,815, titled “Method and Apparatus for Reflector Antenna with Vertex Region Scatter Compensation” filed Dec. 16, 2009 by Chris Hills, John Curran and Bruce Hughes, hereby incorporated by reference in its entirety.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IB2010/055582 | 12/3/2010 | WO | 00 | 5/24/2012 |
Number | Date | Country | |
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61286815 | Dec 2009 | US |