EP0020196B1 - Antenne réseau hyperfréquence du type disque avec son dispositif d'alimentation, et application aux radars d'écartométrie - Google Patents
Antenne réseau hyperfréquence du type disque avec son dispositif d'alimentation, et application aux radars d'écartométrie Download PDFInfo
- Publication number
- EP0020196B1 EP0020196B1 EP80400537A EP80400537A EP0020196B1 EP 0020196 B1 EP0020196 B1 EP 0020196B1 EP 80400537 A EP80400537 A EP 80400537A EP 80400537 A EP80400537 A EP 80400537A EP 0020196 B1 EP0020196 B1 EP 0020196B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- mode
- array antenna
- hand
- guide
- wave
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 230000010287 polarization Effects 0.000 claims description 13
- 230000005540 biological transmission Effects 0.000 claims description 10
- 238000005259 measurement Methods 0.000 claims description 7
- 230000005855 radiation Effects 0.000 claims description 7
- 230000008878 coupling Effects 0.000 claims description 3
- 238000010168 coupling process Methods 0.000 claims description 3
- 238000005859 coupling reaction Methods 0.000 claims description 3
- 238000010586 diagram Methods 0.000 description 4
- 239000003989 dielectric material Substances 0.000 description 2
- 238000005286 illumination Methods 0.000 description 2
- 230000010363 phase shift Effects 0.000 description 2
- 239000000523 sample Substances 0.000 description 2
- 230000005284 excitation Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q25/00—Antennas or antenna systems providing at least two radiating patterns
- H01Q25/02—Antennas or antenna systems providing at least two radiating patterns providing sum and difference patterns
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q21/00—Antenna arrays or systems
- H01Q21/0006—Particular feeding systems
- H01Q21/0012—Radial guide fed arrays
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q21/00—Antenna arrays or systems
- H01Q21/06—Arrays of individually energised antenna units similarly polarised and spaced apart
- H01Q21/20—Arrays of individually energised antenna units similarly polarised and spaced apart the units being spaced along or adjacent to a curvilinear path
Definitions
- the present invention relates to disc type microwave network antennas, more particularly associated with radars performing deviation measurements.
- the disk type array antennas for deviation measurements are known and described for example in American patent US Pat. No. 3,576,579. These antennas comprise a cylindrical cavity of large diameter and small thickness. One of the faces of this cavity is connected in its center to a guide of circular section, the other face is provided with elementary antennas, distributed in concentric circles, and electromagnetically coupled with the interior of the cavity. On transmission, the circular guide is supplied by an electromagnetic wave according to the TM o1 mode which generates a circular radial wave in the cavity.
- the circular guide is supplied by a T-coupler which delivers the TM o1 wave to it and which, upon receipt, on at least two separate channels, the signals Sum ⁇ and Difference A necessary for the development of the deviation signal s.
- Difference A Elevation and A Azimuth There are two ways here Difference A Elevation and A Azimuth.
- the Sum channel of this tee receives the electromagnetic wave TM o1 transmitted to the disk type array antenna.
- This type of embodiment has several disadvantages due to the use of the TM o1 mode for transmission in the Sum channel, this mode allowing neither a wide frequency band nor a high power level.
- This TM 01 mode is generally obtained via the Difference channel of a magic tee connected to the Sum channel of the T-coupler of the antenna.
- this Difference route is difficult to adapt and has a low power handling capacity.
- the device according to the invention aims to remedy these drawbacks by feeding the circular guide connected to the array antenna by an electromagnetic wave according to TE 11 mode which can then come directly from the microwave oscillator.
- the US patent 3,022,506 describes an antenna in which a cylindrical cavity is supplied by a circular guide which receives two TE 11 waves whose relative phase shift adjustment allows, in combination with a network of particular elementary radiating sources formed crossed slots arranged in a circle around the center of the cylindrical cavity, to obtain an antenna with controlled arbitrary polarization.
- This patent also indicates that by supplying the circular guide with two TE 11 modes with rectilinear polarization in quadrature there is obtained a TE 11 mode with circular polarization.
- the invention consists on the one hand, in having perceived that the supply of a network antenna intended to be used in measurements of deviation measurement, was more advantageous in the fundamental mode TE 11 than in the mode usually used until there TM 01 , for reasons of power and frequency band; on the other hand to have produced a network antenna adapted to this new supply mode in which, on transmission, TE mode 11 supplies the sum channel (s) while on reception the sum channel (s) operates in TE 11 mode and the Difference channel in TM oi mode; finally to have properly arranged the elementary radiating sources on the cylindrical cavity to obtain the desired equiphase radiation.
- a disk-type microwave network antenna for carrying out deviation measurements is in accordance with claim 1.
- I (r) translates the attenuation of the current as a function of the radial distance.
- the same TE 11 mode in phase quadrature and in vertical polarization gives a second radial current whose amplitude law is given by the double circle diagram defined by the equation:
- Figure la shows the section of a disk type array antenna. It comprises a cylindrical cavity 3, supplied by a circular guide 4. This cavity has on its periphery a suitable charge 5 which can for example be made of dielectric materials.
- Directive probes 7 are connected on the one hand to suitable loads 6 and on the other hand to elementary antennas 1 by means of phase shifters 2. These elementary antennas 1 can be by way of nonlimiting example of the spiral type or propeller.
- Feeding the antenna according to TE11 mode makes it possible to keep the same arrangement of the prior art of the elementary antennas 1 which then are of the spiral or helix type and therefore do not have axial symmetry and are arranged on concentric circles of center 0, O being the point of intersection of the axis of symmetry of the antenna with the radiating surface of the cylindrical cavity 3.
- This arrangement makes it possible to obtain an equiphase radiation of the elementary antennas if it is carried out in conjunction with an orientation of these elementary antennas 1 made necessary by the use of the TE 11 mode, such that all the antennas located on the same circle are deduced from each other by a rotation about the axis of symmetry of the cylindrical cavity 3.
- this radial orientation of the elementary antennas 1 introduces a phase correction of the form e -i ⁇ which added to the phase modification of the phase shifters 2 of the form e ikr leads to a law of illumination of the disk type array antenna which is a circular symmetry equiphase law radiating a diagram of the same symmetry.
- a significant advantage of the TE 11 mode power supply is the possibility of having a second arrangement of the elementary antennas. allowing a less restrictive choice of the type of elementary antennas.
- the elementary antennas 1 are then arranged in Archimedean spirals, and have an axial symmetry such as for example two crossed dipoles. It is then clear that the law of illumination of the antenna remains unchanged because by being placed on Archimedes spirals, the term of phase e i ⁇ disappears as well as the term e -i ⁇ due to the radial orientation of these antennas elementary 1.
- Couplers can be used to supply the cylindrical cavity 3 of the antenna with TE 11 with circular polarization.
- Figure 2a shows one of them which includes a Tee of the fork type whose structure and operation are known. It is formed of two rectangular section guides 10 and 11 electromagnetically coupled together.
- the guide with rectangular section 10 is connected to a guide with circular section 4.
- This guide with circular section is electromagnetically coupled to a guide with rectangular section 12 by means of a guide, with rectangular section, forming a ring 13.
- this coupler then receives on transmission two waves on the guides 10 and 12.
- An additional advantage therefore lies here in the fact that each guide 10 and 12 receives only half of the power transmitted.
- the guide 11 gives the difference signal ⁇
- the guide 12 the component of the sum signal ⁇ v corresponding to a vertical polarization
- the guide 10 the component of the sum signal ⁇ H corresponding to a horizontal polarization.
- FIG. 2b shows another structure of a coupler usable according to the invention comprising a Te of the fork type. It is formed of a rectangular section guide 10 connected to a circular section guide 40. A rectangular section guide 11 is electromagnetically coupled to the guide 10. The rectangular section guide 11 is such that the plane determined by one of its sections straight is fixed on a plane delimiting the guide 10 and comprising one of the short sides of its straight section, and that the long side of a straight section of the guide 11 is orthogonal to the plane delimiting the guide 10 and comprising the large side of the section rectangular.
- a polarizer 20, for example consisting of an approximately diamond-shaped blade cut out of a dielectric material is fixed in the circular section guide 40 so that the plane of this polarizer 20 makes an angle of n / 4 with respect to the plane delimiting the guide with rectangular section 10.
- the guide 10, on reception, delivers the sum signal ⁇ while the perpendicular guide 11 delivers the difference signal ⁇ .
- FIG. 2c shows a third example of a coupler, called a turnstile, which may be of interest in cases where the antenna diagrams must have good symmetry characteristics, the power supply also has these symmetry characteristics. It comprises, in addition to the circular section guide 40, four rectangular section guides 30, 31, 32 and 33 electromagnetically coupled with the circular section guide 40 so that the long side of the straight section of the guides 30, 31, 32 and 33 is parallel to the axis of the circular section guide 4. In addition, each of these rectangular section guides is deduced from the following by a rotation of n / 2 around the axis of the circular section guide 40.
- the section guide circular 40 is connected at one end to a coaxial line 34, and a coupling means 35 ensures the electromagnetic connection.
- each of the four rectangular section guides 30, 31, 32 and 33 receives a wave according to the TE 11 mode of amplitude A o corresponding to a quarter of the total power that the antenna must receive. If A 1 , A 2 , A 3 and A 4 represent the waves applied respectively to the guides 30, 31, 32 and 33, then it can be shown that to obtain a wave with circular polarization, the following conditions must be fulfilled:
- the components of the sum signal ⁇ are then obtained on the four waveguides 30, 31, 32 and 33 and the difference signal A on the coaxial line 34.
- a disk type array antenna has thus been described providing a solution to the power problem of the prior art.
- This antenna is preferably applied to radars performing deviation measurements.
Landscapes
- Variable-Direction Aerials And Aerial Arrays (AREA)
- Radar Systems Or Details Thereof (AREA)
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| FR7911629A FR2456399A1 (fr) | 1979-05-08 | 1979-05-08 | Antenne reseau hyperfrequence du type disque avec son dispositif d'alimentation, et application aux radars d'ecartometrie |
| FR7911629 | 1979-05-08 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| EP0020196A1 EP0020196A1 (fr) | 1980-12-10 |
| EP0020196B1 true EP0020196B1 (fr) | 1986-06-11 |
Family
ID=9225194
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP80400537A Expired EP0020196B1 (fr) | 1979-05-08 | 1980-04-21 | Antenne réseau hyperfréquence du type disque avec son dispositif d'alimentation, et application aux radars d'écartométrie |
Country Status (4)
| Country | Link |
|---|---|
| US (1) | US4322731A (en:Method) |
| EP (1) | EP0020196B1 (en:Method) |
| DE (1) | DE3071638D1 (en:Method) |
| FR (1) | FR2456399A1 (en:Method) |
Families Citing this family (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB8317938D0 (en) * | 1983-07-01 | 1983-08-03 | Emi Ltd | Antenna |
| JPS63500559A (ja) * | 1985-10-03 | 1988-02-25 | ヒユ−ズ・エアクラフト・カンパニ− | 積分モ−ドフィルタを有した非リアクタンス放射線電力分割器/結合器 |
| GB8624984D0 (en) * | 1986-10-17 | 1986-11-19 | Emi Plc Thorn | Antenna |
| US4831331A (en) * | 1987-04-10 | 1989-05-16 | Chevron Research Company | Method and apparatus for interface location determination |
| JPH02189008A (ja) * | 1989-01-18 | 1990-07-25 | Hisamatsu Nakano | 円偏波アンテナ装置 |
| FR2812457B1 (fr) | 2000-07-28 | 2004-05-28 | Thomson Csf | Reflecteur hyperfrequence actif a bi-polarisation, notamment pour antenne a balalyage electronique |
| WO2015058784A1 (en) * | 2013-10-21 | 2015-04-30 | Esa European Space Agency | Very compact tm01 mode extractor |
| FR3049393B1 (fr) * | 2016-03-24 | 2020-05-08 | Centre National D'etudes Spatiales C N E S | Procede d'alimentation d'un guide d'onde radial et dispositif a guide d'onde radial |
Family Cites Families (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3063049A (en) * | 1959-01-02 | 1962-11-06 | Hughes Aircraft Co | Linearly polarized monopulse lobing antenna having cancellation of crosspolarization components in the principal lobe |
| US3022506A (en) * | 1959-03-27 | 1962-02-20 | Hughes Aircraft Co | Arbitrarily polarized slot antenna |
| FR1459373A (fr) * | 1964-11-02 | 1966-04-29 | Hughes Aircraft Co | Système d'antenne |
| US3524151A (en) * | 1968-01-09 | 1970-08-11 | Emerson Electric Co | Phased array transmission lens feed system |
| US3576579A (en) * | 1968-04-19 | 1971-04-27 | Sylvania Electric Prod | Planar radial array with controllable quasi-optical lens |
| US3731235A (en) * | 1971-11-03 | 1973-05-01 | Gte Sylvania Inc | Dual polarized diplexer |
| US3745585A (en) * | 1972-03-29 | 1973-07-10 | Gte Sylvania Inc | Broadband plane antenna with log-periodic reflectors |
-
1979
- 1979-05-08 FR FR7911629A patent/FR2456399A1/fr active Granted
-
1980
- 1980-04-21 EP EP80400537A patent/EP0020196B1/fr not_active Expired
- 1980-04-21 DE DE8080400537T patent/DE3071638D1/de not_active Expired
- 1980-05-02 US US06/146,370 patent/US4322731A/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| DE3071638D1 (en) | 1986-07-17 |
| US4322731A (en) | 1982-03-30 |
| FR2456399A1 (fr) | 1980-12-05 |
| EP0020196A1 (fr) | 1980-12-10 |
| FR2456399B1 (en:Method) | 1983-07-18 |
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