The present application claims priority under 35 U.S.C. §119(a) of European Patent Application No. 11000921.4 filed Feb. 4, 2011, the disclosure of which is expressly incorporated by reference herein in its entirety.
1. Field of the Invention
The embodiments of the invention relate to an antenna array having a WAIM layer for impedance matching for large skew angles. In particular, the antenna array includes an antenna baseplate having a plurality of antenna elements arranged in a regular grid and a dielectric wide angle impedance match (WAIM) layer arranged in front of the antenna elements for impedance matching for large skew angles.
2. Discussion of Background Information
One phenomenon that is often observed in the transmission behavior of an antenna array while the main beam is being electronically scanned is the difference in the transmission level depending on the direction to which the antenna is skewed. Normally, an antenna has a defined polarization alignment, for example vertical or horizontal polarization. In order to explain this phenomenon, it is sufficient to electronically skew the main beam of an antenna array in an imaginary form along two planes (vertical & horizontal). If the vector of the emitted electrical field strength is within the skew plane, defined as being formed from the skew direction and normal to the antenna, the term transverse magnetic polarization (TM) is used. If the vector of the electrical field strength is at right angles to this plane, the term transverse electrical (TE) is used. All other possible polarization states can be broken down into these two polarization components. In principle, conventional antenna arrays (as well as other structures of a related type such as dielectric or frequency-selective radomes) have a tendency to form a poorer transmission level in TE than in TM as the skew angle increases.
A so-called wide angle impedance match (WAIM) layer, which is arranged in front of the antenna elements, can counteract this effect. With respect to the two polarization cases of TE and TM, the WAIM layer acts analogously to an equivalent line model of the antenna as a parallel-connected capacitance, whose relative susceptance (with respect to the characteristic impedance) varies with the skew angle θ. For the case of TE polarization, this change takes place with the factor 1/cos(θ), but with the factor cos(θ) for the case of TM polarization, provided that the dielectric constant of the WAIM layer is sufficiently high, and the thickness of the WAIM layer is sufficiently thin. If the WAIM layer is suitably designed, the described reciprocity of the factors now leads to the transmission levels of the antenna being matched to one another, between TE and TM polarization, during skewing. This applies to all possible skew angles within a technical sensible range from, for example, θ=0° to θ=60°. This matching then results in the normally desired broad individual polar diagrams of antenna elements of an antenna array in all the important section levels.
The solutions used until now have been based essentially on the theoretical works by Magill & Wheeler (E. Magill and H. Wheeler, “Wide-angle impedance matching of a planar array antenna by a dielectric sheet,” IEEE Transactions on Antennas and Propagation, Vol. 14, No. 1, pages 49-53, 1966), the disclosure of which is expressly incorporated by reference herein in its entirety. A WAIM layer carries out the purpose of transmission matching between TE and TM polarization only if it is kept at a short but well-defined distance from the antenna elements in the antenna array.
The standard solution for production of the necessary physical separation is the use of RF foam materials, as described, e.g., in U.S. Pat. No. 7,580,003 B1, the disclosure of which is expressly incorporated by reference herein in its entirety. While the availability of foams such as these does not represent a problem, a range of disadvantages occur in the course of use of such foams:
U.S. Pat. No. 3,605,098, the disclosure of which is expressly incorporated by reference herein in its entirety, describes an antenna array in which there is a separate WAIM element in front of each antenna element. A WAIM element such as this in each case includes a WAIM layer parallel to the plane of the antenna elements, as well as spacers on which the WAIM layer is arranged.
MCGRATH D T: “Accelerated periodic hybrid finite element method analysis for integrated array element and radome design, PHASED ARRAY SYSTEMS AND TECHNOLOGY, 2000. PROCEEDINGS. 2000 IEEE INTERNATIONAL CONFERENCE ON DANA POINT, CA, USA 21-25 MAY 2000, PISCATAWAY, NJ, USA, IEEE, US, 21 May 2000 (21 May 2000), pages 319-322, XP010504600, DOI: DO1: 10.1109/PAST.2000.858965, ISBN: 978-0-7803-6345-8 describes an antenna array having waveguide antenna elements, with the waveguide antenna elements having dielectric filling elements in order to specifically vary the radiation characteristics of the antenna. The dielectric filling elements project out of the antenna. A WAIM layer is arranged on these projecting dielectric filling elements. The disclosure of this document is expressly incorporated by reference herein in its entirety
Embodiments of the invention provides an antenna array with a WAIM layer that avoids the disadvantages that occur when using foams as an intermediate layer between the antenna elements and the WAIM layer.
Accordingly, the WAIM layer is a monolithic layer that covers all the antenna elements and has spacers machined out of its material in a regular grid. The grid of the spacers corresponding to the grid of the antenna elements.
According to embodiments of the invention, spacers are machined in a regular grid from the material of the WAIM layer. The spacers and the WAIM layer are therefore integrally (monolithically) connected to one another, with the grid of the spacers corresponding to the grid of the antenna elements. By way of example, the grid may be square, rectangular or hexagonal. In particular, the spacers may be in the form of columns with a round cross section. The WAIM layer is advantageously attached to the antenna baseplate on the spacers by mechanical connection (e.g., screws), with the numbers of such spacers where a connection is provided being dependent on the specific requirements. In particular, there is therefore no need to provide a connection on each spacer.
Therefore, according to embodiments, only the material of the WAIM layer, in which the spacers have already been integrated, is used, rather than the known multilayer structure of WAIM layer/adhesive film/foam, which comprise different materials. The spacers provide an air-filled or vacuum-filled separator between the WAIM layer and the antenna elements. The described disadvantages resulting from the previously used foams may be completely avoided. Furthermore, there is no need for complex adhesive-bonding processes for connection of the WAIM layer to a foam separator.
The spacers provide the WAIM layer with the required mechanical robustness. The layer is therefore insensitive to vibration, shock etc., and is therefore also suitable for robust application scenarios.
Since the grid in which the spacers are arranged corresponds to the grid of the antenna elements, the natural periodicity of the antenna array is not disturbed. As a result, no Bragg reflections can occur on the antenna surface within the frequency range for which the antenna array is designed. No losses need be accepted in the radar back-scattering cross section. Provided that there are no more stringent requirements for the radar back-scattering cross section (RCS), embodiments are alternatively also possible in which the grid of the spacers and the grid of the antenna elements do not correspond. This modified grid must, however, still be oriented with the grid of the antenna elements. For this purpose, the grid of the spacers is derived from the grid of the antenna elements such that there is a corresponding spacer only for every n-th antenna element (and there are no further spacers apart from these). This therefore represents a defined thinning out of the original grid of the spacers. In other words, the fundamental grid structure is maintained, but the grid size (grid constant) is changed by the factor n. In this case, n is a natural number greater than 1.
The described form of the WAIM layer may be achieved in particular by mechanical machining techniques, for example, milling out. Corresponding to its function as a WAIM layer, the material should have as high a dielectric constant as possible and a low loss angle, and its layer thickness should be as thin as possible. Dielectric materials such as these are commercially available as semi-finished products.
One suitable material for the WAIM layer is, for example, the dielectric material (product)“C-Stock AK” from Cuming Microwave Corporation, which is available with a customer-specific dielectric constant and in various semi-finished product sizes. Materials such as these can easily be processed using mechanical devices or processes (for example milling).
In order to provide more mechanical robustness, additional stiffening structures in the form of ribs may be formed from the material of the WAIM layer. In order to prevent these from having any negative effects on the transmission level of the antenna during electronic skewing, these structures must also follow the periodicity in the arrangement of the antenna elements. The ribs are designed such that they each connect two adjacent spacers.
The WAIM layer need not necessarily be planar. It may also have a one-dimensionally or two-dimensionally curved surface, for use with curved antenna arrays which are conformal with a structure.
The WAIM layer may be extended to form a multilayer WAIM block, by connection to further dielectric layers.
Embodiments of the invention are directed to an antenna array that includes a plurality of antenna elements, an antenna baseplate on which the plurality of antenna elements are arranged in a regular grid, and a dielectric wide angle impedance match (WAIM) layer structured and arranged in front of the antenna elements to match impedance for large skew angles. The WAIM layer includes a monolithic material layer from which spacers are machined in a regular grid that corresponds to the grid of the antenna elements.
According to embodiments, the grid of the antenna elements may be one of square, rectangular or hexagonal.
In accordance with other embodiments, the grid of the spacers may not be the same as the grid of the antenna elements. The grid of the spacers may be derived from the grid of the antenna elements such that there is a corresponding spacer only for every n-th antenna element, where n=2, 3, 4, . . . .
According to still other embodiments, reinforcing ribs can be machined from the WAIM layer so that each reinforcing rib connects two adjacent spacers.
In accordance with still other embodiments, the plurality of spacers can be attached to the antenna baseplate by mechanical connectors. The mechanical connectors may be arranged in a grid that corresponds to the grid of the spacers. The grid of the mechanical connectors may not be the same as the grid of the spacers. The grid of the mechanical connectors can be derived from the grid of the spacers so that a corresponding mechanical connector is provided only for every n-th spacer, where n=2, 3, 4, . . . .
According to other embodiments, the spacers can have a round cross-section.
Embodiments of the instant invention are directed to a method for forming an antenna array. The method includes arranging a plurality of antenna elements on an antenna backplate in an antenna element grid, forming a dielectric wide angle impedance match (WAIM) layer by forming a plurality of spacers from a monolithic material layer, the plurality of spacers being arranged in a regular grid corresponding to the antenna element grid, and positioning the WAIM layer in front of the antenna elements to match impedance for large skew angles.
In accordance with embodiments, the grid formed by the plurality of antenna elements may be one of square, rectangular or hexagonal.
According to other embodiments of the invention, the grid of the spacers may not be the same as the grid of the antenna elements. The grid of the spacers can be derived from the grid of the antenna elements such that there is a corresponding spacer only for every nth antenna element, where n=2, 3, 4, . . . .
In accordance with still other embodiments, the method can also include machining reinforcing ribs in the WAIM layer so that each reinforcing rib connects two adjacent spacers.
According to further embodiments, the method can also include attaching the plurality of spacers to the antenna baseplate with mechanical connectors. The mechanical connectors can be arranged in a grid that corresponds to the grid of the spacers. The grid of the mechanical connectors may not be the same as the grid of the spacers. The grid of the mechanical connectors can be derived from the grid of the spacers so that a corresponding mechanical connector is provided only for every n-th spacer, where n=2, 3, 4, . . . .
In accordance with still yet other embodiments of the present invention, the spacers may be formed to have a round cross-section.
Other exemplary embodiments and advantages of the present invention may be ascertained by reviewing the present disclosure and the accompanying drawing.
The present invention is further described in the detailed description which follows, in reference to the noted plurality of drawings by way of non-limiting examples of exemplary embodiments of the present invention, in which like reference numerals represent similar parts throughout the several views of the drawings, and wherein:
The particulars shown herein are by way of example and for purposes of illustrative discussion of the embodiments of the present invention only and are presented in the cause of providing what is believed to be the most useful and readily understood description of the principles and conceptual aspects of the present invention. In this regard, no attempt is made to show structural details of the present invention in more detail than is necessary for the fundamental understanding of the present invention, the description taken with the drawings making apparent to those skilled in the art how the several forms of the present invention may be embodied in practice.
As illustrated spacers A are arranged in a regular grid to be positioned in the intermediate spaces between individual antenna elements SE and to abut antenna baseplate P, which is formed by a metallic material.
WAIM layer W is attached to metallic antenna baseplate P of the antenna array by a multiplicity of screws S (
The number and position of the individual screws are chosen depending on the antenna robustness requirements. In particular, there is no need to provide a screw on every spacer.
However, in order to influence the antenna polar diagram as little as possible, the same grid as the grid predetermined by the antenna elements is chosen for the arrangement of the screws.
However, if the number of screws required is chosen to be less than the number of spacers A, the arrangement of the screws S is still oriented with the grid of the antenna elements SE. The arrangement of screws S will then be thinned out such that a screw is provided only for every n-th spacer (n=2, 3, 4 . . . ).
With regard to possible reductions in the radar back-scattering cross section (RCS), it is preferable to fit them from the rear, but attachment from the front face has advantages in terms of accessibility, of course.
In
It is noted that the foregoing examples have been provided merely for the purpose of explanation and are in no way to be construed as limiting of the present invention. While the present invention has been described with reference to an exemplary embodiment, it is understood that the words which have been used herein are words of description and illustration, rather than words of limitation. Changes may be made, within the purview of the appended claims, as presently stated and as amended, without departing from the scope and spirit of the present invention in its aspects. Although the present invention has been described herein with reference to particular means, materials and embodiments, the present invention is not intended to be limited to the particulars disclosed herein; rather, the present invention extends to all functionally equivalent structures, methods and uses, such as are within the scope of the appended claims.
Number | Date | Country | Kind |
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11000921 | Feb 2011 | EP | regional |
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Daniel T. McGrath, “Accelerated Periodic Hybrid Finite Element Method Analysis for Integrated Array Element and Radome Design”, Proceedings, International Conference on Phased Array Systems and Technology, XP010504600; ISBN: 978-0-7803-6345-8; pp. 319-322, May 21, 2000. |
S.Sajuyigbe et al., “Wide angle impedance matching metamaterials for waveguide-fed phased-array antennas,” IET Microwaves, Antennas & Propagation, Vo.. 4, Iss.8, XP-002639838, pp. 1063-1072, May 14, 2010. |
E.Magill et al., “Wide-angle impedance matching of a planner array antenna by a dielectric shhet”, IEEE Transactions on Antennas and Propagation, vol. 14, No. 1, pp. 49-53, 1966 |
Number | Date | Country | |
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20120200474 A1 | Aug 2012 | US |