This application is a 371 of PCT/FR02/02090 dated 18 Jun. 2002.
The invention relates to the field of antennas, and more specifically the field of wire-plate antennas.
Wire-plate antennas are known that consist, as represented in
The feed for such an antenna is typically realized by a coaxial line 150 which passes through the ground plane 140, an inner conductor 152 of which is connected to the metal top part 120 and an outer conductor 154 of which is connected to the ground plane 140. The particular aspect of such an antenna is that of having a wire 160 connecting the capacitive top part 120 and the ground plane 140, forming an active metal return to ground.
The return-to-ground wire 160 gives rise to a “parallel” resonance at a frequency less than that of a “fundamental” frequency of a patch.
This parallel resonance is due to an exchange of energy between the self inductance L and the capacitance C of a resonator formed by the return-to-ground wire (inductive effect λ) and the capacitive top part.
A resonant frequency is then obtained, thus giving a range of matching of the antenna, of the type:
The physical parameters affecting this frequency are the permittivity of the dielectric substrate εr, its height (distance between the top part and the ground plane), the radius of the feed line 150, the radius of the return-to-ground wire 140, the distance between the feed line 150 and the return-to-ground wire 160, and the dimensions of the top part 120 and of the ground plane 140.
This large number of parameters multiplies by as much the number of possible configurations, enabling the antennas to be optimized to meet performance specifications.
The wire-plate antenna radiation arises mainly from the return wires 160 and exhibits the typical characteristics of radiation from a monopole perpendicular to the ground plane, the characteristic radiation being an omnidirectional azimuth radiation with respect to the ground plane and almost zero perpendicular to this plane.
Thus, such an antenna exhibits a radiation pattern having a lobe with rotational symmetry, with maximum radiation directed approximately parallel to the ground plane and a minimum radiation in the axis of the feed and return wires. In accordance with the typical radiation of a monopole perpendicular to the ground plane. It is to be noted that in the case of finite ground planes, the effects of diffraction through the breaks in the ground plane 140 introduce distortions of the radiation pattern and a backward radiation.
The operation of a wire-plate antenna is therefore very different from the operation of another type of antenna known as a “resonant antenna”. This is because, the resonance referred to for these “resonant antennas” is an electromagnetic type resonance (resonant modes) and not an electric type resonance as is the case for wire-plate antennas. This is because, in wire-plate antennas, the resonant elements are localized, similar to electrical components.
Operation by electrical resonance and the use of structures like electrical components results in wire-plate antennas having a dimension much smaller than the wavelength, and in any case having dimensions smaller than the smallest dimensions of “resonant antennas”.
The operation of wire-plate antennas is therefore very different from electromagnetic resonance operation that governs the antennas referred to as “resonant antennas”.
The operation of wire-plate antennas distinguishes them in particular from “microstrip” or “microslot” antennas known to those skilled in the art.
Despite the existence of many possibilities in choosing physical parameters to best adapt the known antenna to performance specifications, in practise it is desirable to have an antenna that is still more easily configurable, at its construction stage, in accordance with the multiband, multifunction behavior desired.
This aim is achieved according to the invention by virtue of an antenna of the type comprising:
These cutout-slots generate different capacitances leading to different resonant frequencies of the wire-plate antenna in accordance with the previously mentioned formula.
Preserving the wire-plate radiation (that is to say omnidirectional azimuth) also distinguishes this antenna from those encountered in literature for which antennas it is the cutout-slot in the surface that radiates with a maximum in the axis perpendicular to this surface and not a very weak radiation in this direction as is the case for a wire-plate antenna and especially in the invention.
Advantageously, the first surface has a cutout-slot of very small width with respect to its length and to the main wavelength picked up (preferably a tenth of this length). There may be several cutout-slots, for example greater than two in number.
According to advantageous but non-limiting arrangements:
Other features, aims and advantages of the invention will become apparent from reading the detailed description that follows, made with reference to the accompanying figures in which:
The antenna of
It has a top part 120 that is defined by a series of rectilinear segments of any shape (polyhedron, circular, etc.).
However, in this case, the capacitive top part 120 has a cutout-slot 122 that extends along the edges of this capacitive top part, thus forming a boundary between an edge region 124 of the top part and a central region 126 of the top part 120.
This cutout-slot is of a form that comes back round on itself, but is interrupted on a short stretch of the edge of the top part, such that it describes the general shape of a C. More specifically, the C that it describes is made up of a series of rectilinear portions, each parallel to a corresponding rectilinear edge of the capacitive top part, and the cutout-slot must not be closed up in order to keep a strip of metal exciting the outer antenna.
The antenna has a ground wire 160 and a feed line 150 that extend transversely to the antenna, and that make contact with the top part 120 at its part that is enclosed by the C-shape cutout-slot.
Adopting such a cutout-slot or slot 122 generates two capacitive effects: one at the top part edge 124 (outer part of the slot), and the other at the inner part 126 of the top part.
The addition of such a cutout-slot 122 typically creates an additional resonance of the antenna at a neighboring wavelength of λf/2, where λf corresponds to the total length of the slot.
Thus, the present antenna generates two resonances: one at the wavelength λ corresponding to that of the wire-plate antenna having the region 126 inside the cutout-slot 122 as the capacitive top part, and the other resonance being at a smaller wavelength λf/2 generated by the presence of the cutout-slot 122.
This antenna exhibits a wire-plate type radiation at these two resonant frequencies.
More specifically, the presence of the cutout-slot 122 introduces new physical parameters that affect the electromagnetic behavior, that is to say the width of the cutout-slot 122 measured parallel to the plane of the capacitive top part and transversely to the cutout-slot 122, the position of the cutout-slot 122 on the top part, the position of the cutout-slot 122 with respect to the feed wire 150 and with respect to the return wire 160, and the length of the cutout-slot.
These physical parameters then supplement the physical parameters that normally affect the behavior of antennas, and multiply the number of possible configurations of the antenna enabling the antenna to be better adapted to the use envisaged, in particular by the dual resonance.
As will be seen later, the slot resonates (enabling the antenna to be matched) but does not radiate significantly since the radiation remains that of a wire-plate.
In the embodiment of
In the embodiment of
This second antenna with resonant cutout-slot also has a C-shape cutout-slot, this C being in this case perfectly symmetrical with respect to a plane that is transverse and median to the square top part. This C-shaped cutout-slot has a total length of around λf/2.
The cutout-slot 122 runs along the edges of the capacitive top part 120 maintaining a constant distance from the edges. Thus, it defines a square internally and a strip 124 of constant width externally.
The ground wire 160 and the feed wire 150 are both placed substantially at the center of the inner square 126 in a plane of symmetry of the cutout-slot 122, transverse to the antenna.
Such an antenna has a resonance at the wavelength λ, and also has a resonance approximately at the wavelength λf/2 which is specifically due to the cutout-slot 122. The antenna therefore has two resonances.
The ground wire 160 and the feed wire 150 are in this case placed on a median plane forming a plane of symmetry of the cutout-slot 122 in order to maintain good symmetry in the diagram.
As shown in
More specifically, as represented in
As illustrated in
As illustrated in
A slight dissymmetry is observed on the elevation radiation pattern of the second resonance, and this is due to the dissymmetry of the slot with respect to an axis that is orthogonal to the wires 150 and 160 (more specifically with respect to a plane that is perpendicular to the plane of the wires, perpendicular to the antenna and median to the square formed by the upper plate 120).
Such a dissymmetry may be corrected for example by adopting, in place of the previously proposed cutout-slot 122 one or more pairs of cutout-slots.
Thus,
Each of these C-shaped cutout-slots is formed by three rectilinear branches, each parallel with a side of the square formed by the plate 120. Thus, the two cutout-slots 122 are perfectly symmetrical one with the other, each also being symmetrical with respect to itself such that an upper plate 120 is obtained that is physically symmetrical with respect to two planes that are transverse and median to the square.
The feed wire 150 and the return wire 160 can be placed in one of these median planes and an electrical behavior can be obtained that is symmetrical with respect to the plane of these two wires.
In other words, cutting out on the top part 120 two cutout-slots 122 of the same dimensions results in making the radiation pattern symmetrical while maintaining two operating frequency bands.
A first operating band corresponds appreciably to the wavelength λ of an antenna the capacitive top part of which would be formed by the inner region 126 enclosed by the cutout-slots 122, and the other operating frequency corresponds to a resonance close to λf/2 (half the abovementioned frequency) due to the cutout-slots 122 of same dimensions.
According to one variant, two (or more) cutout-slots are adopted having similar but not equal dimensions and/or having similar but not equal positionings. In this variant, two (or more) resonance peaks are obtained in addition to the wire-plate resonance. These two peaks are close to each other but not equal and they partially overlap, thereby generating in practice a widened frequency band that is additional to the effective operating frequency of the inner region 126.
According to yet another variant, two or more cutout-slots are adopted that extend one with respect to the other and that have dimensions that are sufficiently different to obtain two or more clearly different resonances which are additional with respect to the wire-plate resonance.
Radiation patterns similar to those of known antennas are obtained, but several different frequency bands.
The purpose of the cutout-slots is to create several overlapped wire-plate antennas, each wire-plate antenna formed substantially of the regions bounded by the cutout-slot and of the ground return, collective or otherwise, of the antenna.
The cutout-slots do not change the mode of radiation of each wire-plate antenna considered, which mode remains omnidirectional in azimuth since the slots are not sites for electromagnetic resonance at the frequencies considered.
The various antennas described previously have similar polarizations at their various resonant frequencies.
The various antennas proposed here supply, in addition to the advantages of the conventional wire-plate antenna, the advantage of exhibiting one or more new resonances, while being of a similar size to known antennas.
These antennas can be used to produce, for example, a matched aerial; they advantageously form multi-band antennas (for example for transmission and reception), for example with peaks that are close together in frequency, or even widened band antennas by having peaks that are sufficiently tightly close to one another.
These antennas enable the use of several frequency bands for mobile telephony, for example: GSM, DCS, DECT, or for use inside buildings (indoor use).
The various frequency bands obtained can be used for uplink or downlink paths, for example for transmission and reception in ARGOS tags. Such antennas can also be used for AMPS-PCS 1900 applications.
Number | Date | Country | Kind |
---|---|---|---|
01 07940 | Jun 2002 | FR | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/FR02/02090 | 6/18/2002 | WO | 00 | 12/18/2003 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO02/103843 | 12/27/2002 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
4771291 | Lo et al. | Sep 1988 | A |
6014105 | Davis et al. | Jan 2000 | A |
6133879 | Grangeat et al. | Oct 2000 | A |
6195048 | Chiba et al. | Feb 2001 | B1 |
6348892 | Annamaa et al. | Feb 2002 | B1 |
6529168 | Mikkola et al. | Mar 2003 | B1 |
6624788 | Boyle | Sep 2003 | B1 |
6646610 | Troelsen | Nov 2003 | B1 |
6759991 | Boyle | Jul 2004 | B1 |
20020003499 | Ngounou | Jan 2002 | A1 |
Number | Date | Country |
---|---|---|
WO 0036700 | Jun 2000 | WO |
Number | Date | Country | |
---|---|---|---|
20040164916 A1 | Aug 2004 | US |