The present invention relates to a method for designing low signature array antennas using a calculation method.
In the future many of the advanced low signature vehicles, such as air planes, missiles, unmanned aerial vehicles (UAV), ships and terrain vehicles, will be equipped with some kind of array antenna. It is of great importance that these array antennas exhibit low passive radar cross section.
It is a known fact that array antennas may cause a very high radar cross section. The total radar cross section of an array antenna is the result of several subcontributions. The most important subcontributions are mirror reflection, edge scattering, scattering, reflections in the feed network, grating lobes, scattering caused by the location of the antenna elements in the aperture and diffuse scattering due to mechanical inaccuracy of manufacture. For hull integrated antennas the antenna behaves electromagnetically different than the surrounding hull and in particular within the frequency band of operation of the antenna. The transition between the antenna and the surrounding hull consists of an impedance transition causing scattering and due to that radar cross section. Accordingly, the material of the surrounding hull may be of great significance.
Prior art array antennas of today are commonly designed based upon given requirements on antenna performance, such as frequency of operation, band width, field of view, lobe widths, side lobe level and polarisation. An example of an array antenna designed based upon such requirements is known from U.S. Pat. No. 6,323,809 disclosing designing of a fragmented array antenna. When designing array antennas in this way the signature reduction is set aside and has to be considered afterwards when mounted in a hull. One way of obtaining signature reduction in this connection is to introduce frequency selective surfaces and space demanding absorbents located around the edges of the array antenna. One disadvantage of frequency selective surfaces is that they perform insufficient with respect to signature reduction for frequencies and polarisation coinciding with the frequency and polarisation of the antenna. Furthermore, if the surface is curved it may be difficult to design and manufacture frequency selective surfaces.
The hulls of future low signature air vehicles will most likely consist of some kind of composite material. Such material does not behave as conducting metals having very good conductivity. Furthermore the conductivity of composites may be anisotropic, i.e. the conductivity varies in different directions. A frequency selective surface usually behaves electromagnetically as a good electric conductor within its suppressed frequency band. If the surrounding material consists of a composite the hull and the frequency selective surface will behave electromagnetically different and due to that be the cause of radar cross section.
The object of the invention is to obtain a method for designing array antennas avoiding the drawbacks of prior art methods discussed above.
The object of the invention is obtained by a method characterized in that electromagnetic antenna and signature characteristics are specified, an iterative optimizing method is performed to design the antenna to fulfil the specified characteristics, the iterative method being interrupted when a design fulfils the specified characteristics, and that the specified characteristics are readjusted in an iterative optimizing method to follow if the specified characteristics not are fulfilled. A main principle of the method is that given requirements on antenna and signature performance are simultaneously fulfilled. For frequencies, polarisation and directions in space in which low signature is required it is, as already indicated above, important that hull integrated antennas behave as the surrounding hull irrespective of the material. This requirement is fulfilled by the method according to the invention.
The following advantages of the method of the invention can be emphasized.
According to a favourable method of the invention an array antenna of fragmented array type is designed. The fragmented array antenna exhibits a great number of degrees of freedom involving many possibilities in the optimizing process. Other antenna elements having a great number of degrees of freedom are also conceivable.
According to another favourable method of the invention the optimizing method involves use of a genetic algorithm. Examples of genetic algorithms are i. a. discussed in B. Thors, H. Steyskal, H. Holter, “Broadband fragmented aperture phased array element optimization using genetic algorithms”, IEEE Transactions on Antennas and Propagation, October 2005, pp. 3280-3287, and J. Michael Johnson and Yahya Rahmat-Samii, “Genetic Algorithms in Engineering Electromagnetics”, IEEE Antennas and Propagation Magazine, Vol. 39, No. 4, August 1997, pp 7-21.
According to still another favourable method of the invention the reflection factor of the antenna is adapted to coincide in amount and phase with the reflection factor of a material surrounding the antenna when mounted. Introducing such a requirement will facilitate the use of arbitrary hull materials.
According to yet another favourable method of the invention a frequency selective surface is located in front of the antenna. By introducing such a frequency selective surface cross section, grating lobes arising at high frequencies can be dealt with. Preferably the frequency selective surface is provided with a periodic pattern having a periodicity being a multiple of the periodicity of the antenna.
The invention will now be described in more detail below with reference to the accompanying drawings in which:
a in side view and
According to the method illustrated in
When the antenna and signature characteristics have been specified, an optimizing process is started, block II. During this step the process tries to find out a design of the antenna that fulfils the specified characteristics i. a. trying to find a design with acceptable low radar cross section often with the side condition that the reflection factor of the array antenna is to coincide with the reflection factor surrounding the array antenna. When using an antenna element to be described below with reference to
If the optimizing process finds a design that fulfils the specified antenna and signature characteristics the optimizing process stops and an antenna design configuration is available as an output of block III.
If the specified antenna and signature characteristics have been set too strictly, it may happen that the optimizing process fails to find a design fulfilling the set requirements. In such a case the set antenna and signature characteristics can be readjusted, block IV, and a new optimizing process can be carried out.
The antenna element shown in
According to a further development of the embodiment shown in
The method is described with reference to fragmented antenna elements above. It is however easy and within the scope of the invention to apply the same method to other array antennas having a large number of degrees of freedom. Furthermore, it has above been proposed that the optimizing method uses genetic algorithms. This does not exclude other suitable algorithms from being used in the general concept of the invention.
Number | Date | Country | Kind |
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06445070.3 | Nov 2006 | EP | regional |