PATCH ANTENNA

Abstract: A patch antenna comprises a radiating element and a ground plane with a dielectric therebetween, one or both of the radiating element and the ground plane comprising means defining current paths in a pattern which approximates to a preferred excitation mode of a patch radiating element of uniform and continuous section.

Description: PATCH ANTENNA This invention relates to patch antennas, particularly (but not exclusively) for microwave or near-microwave applications. The invention has particular utility in the provision of antennas for attachment to, or formed on or built into, the windows of buildings, or the windows or non-metallic body panels of vehicles. For convenience, the invention is described and claimed in terms of a transmitting antenna. However, since an antenna is intrinsically a functionally reversible device, the invention relates equally to antennas for use in a transmitting mode, a receiving mode, or both, and the claims are to be interpreted as extending to all such antennas. Figure 1 of the accompanying drawings shows a conventional patch antenna, consisting of a conducting radiating element or "patch" 10 separated from a conducting ground plane 12 by a dielectric layer 14. The patch is a piece of foil or other sheet-like conductive material adhered or printed on to the surface of the dielectric, and is of continuous and uniform section (thickness) in its plane. It will be appreciated that the term "plane" is here used figuratively; the antenna, if conforming to a curved surface, such as a body panel or rear window of a vehicle, will not be strictly planar in the geometrical sense. The radiating element is fed either by a physical connection to a suitable conductor or is electromagnetically coupled to a microstrip line. In such antennas, transmission is effected via fringing fields between the radiating element 10 and the ground plane 12. These fields depend on the distribution of the currents flowing in the radiating element and the ground plane. The current distribution is in accordance with one of several modes which are determined by the shape and size of the patch. It is not possible to configure the antenna always to operate in the desired mode across its full operating range, with the result that the radiation pattern of the antenna is adversely affected. The performance of the antenna, in particular bandwidth and gain for example, then may be reduced compared to its performance in the preferred mode. The present invention, at least in its preferred embodiments, is directed to alleviating this problem. Some preferred embodiments also provide an antenna with a useful degree of transparency which can be attached to or incorporated in a vehicle windscreen or other window. The invention provides in one aspect a patch antenna comprising a radiating element and a ground plane with a dielectric therebetween, one or both of the radiating element and the ground plane comprising means defining current paths in a pattern which approximates to a preferred excitation mode of a patch radiating element of uniform and continuous section. In another aspect the invention provides the use, in a least one of a radiating element and a ground plane of a patch antenna, of means defining current paths in a pattern approximating to a preferred excitation mode of a patch radiating element of uniform and continuous section, whereby to constrain the antenna to operate simulating the preferred excitation mode. In a third aspect the invention provides a method of transmitting or receiving radio frequency energy comprising transmitting or receiving said energy via a patch antenna in which at least one of a radiating element and a ground plane thereof comprises means defining current paths approximating to the current pattern present in a patch radiating element of uniform and continuous section when operating in a preferred excitation mode, said pattern constraining the antenna to simulate the preferred excitation mode. Preferably, there are means for permitting minor currents to flow between the current paths, to enable the current distribution to conform to that of the preferred excitation mode. The means defining the current paths preferably are a plurality of spaced discrete conductors. Preferably, the discrete conductors are intersected by further discrete spaced conductors to form a grid pattern, the further conductors permitting the said flow of minor currents. The conductors preferably intersect substantially orthogonally. The pattern may approximate to an excitation mode of a circular or annular patch. Thus, it may be the TM 01 , TM n , TM 21 , TM 10 , or TM 12 mode of such a patch. Other possible modes (without limitation) are TM 3 , and TM 41 . Alternatively, the pattern may occupy a substantially rectangular or square shape. Thus (without limitation) the pattern may approximate to the TM 10 , TM n , TM 21 , TM 01 or TM 12 mode for a uniform square or rectangular patch. Alternatively, the conductors of the square or rectangular pattern may be substantially parallel to a diagonal thereof. Means may be provided for stimulating circularly-polarised emission from the radiating element. Thus the radiating element may comprise at least one notch or projection whereby it is adapted to emit circularly-polarised signals. Opposite corners of a square shape pattern may be absent whereby the radiating element is adapted to emit circularly-polarised signals. Preferably, there is a solid dielectric disposed between the radiating element and the ground plane. In one preferred form of the invention, the radiating element and the ground plane both comprise a said conductor pattern, and the dielectric is transparent. Preferably the patterns of the radiating element and the ground plane are identical. One or both of radiating element and the ground plane may be printed on or otherwise carried by a glass or other transparent substrate. The invention also comprises a window glass or other optically transparent substrate or a vehicle body part comprising an antenna as set forth above. The invention will now be described merely by way of example with reference to the accompanying drawings, wherein: Figure 1 (as already discussed) shows a conventional patch antenna; Figures 2a, 2b, 3a, 3b, 4a and 4b show conductor patterns for circular patch antennas according to the invention; Figure 5 shows a composite patch antenna according to the invention; and Figures 6a, 6b and 6c show conductor patterns for rectangular patch antennas according to the invention; Figure 7 shows another form of antenna according to the invention. Referring to figure 2a, when a solid continuous circular patch antenna is operating in its TM n mode, the currents in the patch follow a pattern of paths as shown in the figure. According to this embodiment of the invention, to force this mode of oscillation, a patch antenna is manufactured by providing conductors in this pattern on a substrate by any suitable known technique such as etching or photolithography. Preferably at the same time an intersecting conductor pattern as shown in figure 2b is also provided, concentric with that of figure 2a. The individual elements of this pattern each intersect the conductors of figure 2a orthogonally, and permit cross-flows of current between the elements of the figure 2a pattern so that the current distribution matches that of the TM n mode. It will be appreciated that the intersecting pattern need not be as shown in figure 2b. The precise pattern is unimportant, provided that it offers adequate opportunities for cross-flow between the elements of the figure 2a pattern, but does not give rise to an arrangement of alternative current paths such that the patch will support an additional and undesired excitation mode. Figures 3 a and 4a illustrate conductor element patterns designed to operate respectively in the TM 21 and TM 0] excitation modes for a circular patch antenna, and figures 3b and 4b are suitable current-balancing interconnecting patterns, which again intersect the elements of the figure 3a and 4a patterns orthogonally. Such a gridded patch works in a different way to a conventional solid conductor patch. At the resonant frequency of a solid patch, the surface currents produce radiation via electric fields at the edge. The currents are relatively high at the edge of the solid patch and therefore the main radiation comes from the edge. Simulations of the gridded patches show that the currents are not as high at the edges, but being concentrated in the conductors, are locally higher than the diffuse currents in a solid patch. The overall current is substantially the same as the solid patch, but the radiation comes from the relatively high local currents on the grid. Consequently the beamwidth is wider than the solid patch as the effective aperture appears smaller, due to tapering of the field distribution. As the number of lines increases the fringing fields are forced to the edges as they become shorted by the proximity of adjacent lines. The mode-constraining conductor pattern for a particular application is chosen according to the established principles for a solid continuous patch antenna. Thus the TM,, mode produces a directional pattern in which the gain is greatest normal to the plane of the patch. This mode is therefore suitable for a horizontally-oriented patch intended for receiving and transmitting signals from and to satellites, for example in satellite-based communication systems, or GPS systems. The TM 01 mode produces a directional pattern in which the gain is greatest in directions near-parallel to the plane of the patch. A horizontally-disposed patch thus can be used to replace a conventional upright rod antenna for mobile telephone communications, or for receiving broadcast signals. The TM 21 mode produces a pattern in which the sensitivity of the antenna is greatest at an angle of about 35° to the plane of the patch. The TM 31 and TM 41 modes (which are not illustrated, but are known per se) produce patterns where the gain of the antenna is greatest at about 45° and 55° respectively to the plane of the patch. A horizontal patch antenna operated in one of these modes may offer a cost effective solution with adequate performance for both vertically-directed and horizontally-directed signals. However, in general, if both vertical and horizontal sensitivity is required it is likely that a better result will be obtained by using separate TM n and TM 01 antennas. A compact solution is to arrange one of the patches (eg. the TM 01 patch) as an annulus around but electrically separate from the other (eg. the TM U patch), as shown in figure 5. The intersecting connectors equivalent to figures 2b and 4b are omitted from the drawing for clarity, but are present. Alternatively the patches may be disposed side by side over a common ground plane. Another compact solution is to stack the radiating elements concentrically on top of but insulated from each other above a common ground plane. This technique is known for solid patch antennas, and so is not illustrated. In some circumstances eg. when one patch is very small, it may be advantageous to make only one of the antennas of figure 5 gridded, the other (for example the inner one), being solid. Similarly only one of a pair of stacked or side-by-side antennas could be gridded. Figures 6a, 6b and 6c show some conductor patterns suitable for square or rectangular patches. The dotted lines are the mode-defining conductors and the solid lines represent conductors for minor balancing currents to flow between the mode- defining conductors. Each mode radiates a different beam shape, eg. the TM 0 , mode radiates a single beam perpendicular to the plane of the patch while the TM π , mode radiates a null in that plane. Hence one mode might be suitable for satellite communication while the other is suitable for ground based communications. The size and spacing of the mode-defining conductors of the grid has an effect on the antenna gain, and on cross-polarisation performance. Measurements were made on a TM n pattern circular patch antenna according to the invention and a TM 10 square patch antenna also according to the invention. It was found that a spacing of the conductor elements to provide 20 lines/wavelength at the resonant frequency of the antenna gave a reduction in gain compared to an otherwise identical solid patch antenna of 2dB. Increasing the element density to 40 lines/wavelength reduced the loss to less than 0.5dB. We believe that as the grid line pitch gets finer the patch will behave increasingly like a solid patch with transmission from the fringing fields. Thus subject to considerations of cost, ease of manufacture and (where relevant) transparency, the lines of the pattern should be of a fine pitch as practicable, consistent with permitting only the preferred mode of excitation. Other tests have indicated that narrow conductors produce lower cross-polarisation than wide ones, but that for the same thickness for each conductor, wider conductors produce higher gain. It is believed that this is because more metal is present. A further advantage which has been identified is that a gridded patch can be made smaller than a solid one for a given resonant frequency. For example, a circular solid patch operating in the TM n mode and resonant at 1.49 GHz had a diameter of 38mm. A circular gridded patch operating in the same mode and resonating at the same frequency had a diameter of only 30mm. In both cases the patches were mounted on Duroid (a PTFE-based dielectric material) of thickness 0.787mm and dielectric constant 2.33 above an identical ground plane. This reduction in size can be of assistance where the visual impact of the antenna has to be minimised, and/ or in portable equipment where space is limited. The reduction in size is believed to be attained because in the gridded construction the current pattern is more accurately constrained to its desired mode. In a solid patch imperfections or variations in the material may lend to distortions. The improved cross- polarisation performance of the gridded patch is perhaps also indicative of this. The conductor patterns of figures 2 and 3 are for disc-like patches. Annular gridded patches may be employed in place of solid annular patches simply by leaving the conductor patterns unprinted in a circular central region, but with an interconnection between the conductors around the inner edge of the annulus. Alternatively a combination solid and gridded patch may be produced by printing a solid circular panel of conductive material in the centre of the conductor pattern (or vice versa), provided that the remaining patterned area is sufficient to force the patch to adopt the required excitation mode. A circular patch with a solid centre was found to have better gain, cross polarisation and front to back ratio compared to a patch with an open centre when operated in the TM 0 , mode. In the embodiments so far described the radiating patch is a grid, and the ground plane is solid. However the ground plane may be gridded instead, or both patch and ground plane may be gridded. Thus, if the antenna is to be attached to or forms part of a window, the ground plane may be formed as a grid or mesh so that it has a useful degree of transparency. We have found that for the circular mode patterns, a ground plane pattern in the form of a square mesh produces good (ie. low) cross-polarisation. A suitable transparent dielectric for use between the ground plane and the radiating element is a material such as polymethylmethacrylate (Perspex * ). Alternatively if the radiating element and ground plane can be adequately supported on thin sheets of transparent insulating material, arranged parallel to but spaced from each other, air may be employed as the dielectric between them. However the preferred method of providing an antenna according to the invention on a window is to print the radiating element and the ground plane directly on to opposite sides of the glass, or (particularly if the window is of laminated construction), to incorporate one or both of them within it. Conventional techniques for incorporating antennas or heating elements within glass for road vehicle or aircraft applications may be employed for this purpose. A gridded patch whether printed on to glass or other substrate or incorporated within it is expected to be more tolerant of differential thermal expansion between itself and the substrate than is a solid patch. An antenna employing a gridded patch and a gridded ground plane is likely to have a better bandwidth than a comparable gridded patch with a solid ground plane. It also has a degree of optical transparency. On the other hand an antenna with a solid ground plane is likely to have better cross-polarisation performance than one with a gridded ground plane. Both are likely to have superior cross-polarisation performance (perhaps 8dB or more) compared to a conventional antenna with a solid patch and a solid ground plane. The invention may be applied to patch antennas other than of circular or annular shape, where it is required to force the antenna to operate only in a preferred excitation mode. For example, suitable conductor patterns may be employed for elliptical patches, or for square or rectangular patches. Figure 7 shows a square patch in which the conductor pattern is a series of lines parallel to a diagonal of the patch, the conductors for the adjusting currents extending parallel to the other diagonal. The two sets of conductors intersect orthogonally; if the patch were rectangular rather than square or elliptical rather than circular the intersection may not be orthogonal, but the required excitation mode would still be imposed. The figure 7 patch is configured to produce a circularly polarised signal; two opposite corners of the patch are removed, and this (as known per se) introduces perturbations in to the current pattern such that a circularly polarised signal is transmitted. Other known techniques for stimulating circularly polarised transmission from a patch antenna may be employed, for example cut-outs or the addition of a perturbation segment, as appropriate to the shape of the patch. Thus, for circular patches, circular polarisation may be induced by feeding two signals of λ/4 phase difference to the radiating element pattern at two points τ/2 (90°) apart. Alternatively a cut-out or perturbation segment may be provided so as to provide two modes excited in equal amplitude and 90° out of phase at the centre frequency from a single current input. Each feature disclosed in this specification (which term includes the claims) and/or shown in the drawings may be incorporated in the invention independently of other disclosed and/or illustrated features. The text of the abstract filed herewith is repeated here as part of the specification. A patch antenna comprises a radiating element and a ground plane with a dielectric therebetween, one or both of the radiating element and the ground plane comprising means defining current paths in a pattern which approximates to a preferred excitation mode of a patch radiating element of uniform and continuous section.

Claims: CLAIMS: 1. A patch antenna comprising a radiating element and a ground plane with a dielectric therebetween, one or both of the radiating element and the ground plane comprising means defining current paths in a pattern which approximates to a preferred excitation mode of a patch radiating element of uniform and continuous section. 2. In a patch antenna, the use, in a least one of a radiating element and a ground plane, of means defining current paths in a pattern approximating to a preferred excitation mode of a patch radiating element of uniform and continuous section, whereby to constrain the antenna to operate simulating the preferred excitation mode. 3. An antenna as claimed in Claim 1, or 2 comprising means for permitting minor currents to flow between the current paths. 4. An antenna as claimed in Claim 1, 2 or 3, wherein the means defining the current paths comprises a plurality of spaced discrete conductors. 5. An antenna as claimed in Claims 3 and 4, wherein the discrete conductors are intersected by further discrete spaced conductors to form a grid pattern, the further conductors permitting the said flow of minor currents. 6. An antenna as claimed in Claim 5, wherein the conductors intersect substantially orthogonally. 7. An antenna as claimed in any preceding claim comprising means for stimulating circularly-polarised emission from the radiating element. 8. An antenna as claimed in any preceding claim, wherein the pattern approximates to an excitation mode of a circular or annular patch. 9. An antenna as claimed in Claim 8, wherein the pattern is the TM 0 , or the TM,, or the TM 21 mode for a uniform circular patch. 10. An antenna as claimed in any of Claims 1 to 7 wherein the pattern approximates to an excitation mode of a square or rectangular patch. 11. An antenna as claimed in Claim 10 wherein the pattern is the TM, 0 , TM,, or TM 2 , mode for a uniform square or rectangular patch. 12. An antenna as claimed in Claim 10, wherein the pattern occupies a substantially rectangular or square shape, and the conductors of the pattern are substantially parallel to a diagonal thereof. 13. An antenna as claimed in Claims 7 and 10, of square shape and wherein opposite corners of the square shape are absent whereby the radiating element is adapted to emit circularly-polarised signals. 14. An antenna as claimed in Claims 7 and 8 wherein the radiating element comprises at least one notch or projection whereby it is adapted to emit circularly-polarised signals. 15. An antenna as claimed in any preceding claim, wherein a solid dielectric is disposed between the radiating element and the ground plane. 16. An antenna as claimed in Claim 15, wherein the radiating element and the ground plane both comprise a said conductor pattern, and the dielectric is transparent. 17. An antenna as claimed in any preceding claim, wherein the ground plane comprises a said conductor pattern and is printed on or is otherwise carried by a glass or other transparent substrate. 18. A patch antenna as claimed in any preceding claim comprising at least two radiating elements, one or more of which comprises a said means defining current paths, the radiating elements being stacked, side by side, or concentric. 19. A patch antenna substantially as herein described and/or as shown in the accompanying drawings. 20. A window glass or other optically transparent substrate or a vehicle body part comprising an antenna as claimed in any preceding claim. 21. A method of transmitting or receiving radio frequency energy comprising transmitting or receiving said energy via a patch antenna in which at least one of a radiating element and a ground plane thereof comprises means defining current paths approximating to the current pattern present in a patch radiating element of uniform and continuous section when operating in a preferred excitation mode, said pattern constraining the antenna to simulate the preferred excitation mode. 22. A method of transmitting or receiving radio frequency energy substantially as herein described.

Inventors: CLASEN GISELA, LANGLEY RICHARD JONATHAN, CLASEN, GISELA, LANGLEY, RICHARD, JONATHAN
Applicants: CLASEN GISELA, HARADA IND EUROP LIMITED, LANGLEY RICHARD JONATHAN, CLASEN, GISELA, HARADA INDUSTRIES (EUROPE) LIMITED, LANGLEY, RICHARD, JONATHAN
Application year: 1999
Main classification: H01Q9
IPC codes: H01Q1, H01Q9, H01Q13