JPH0149201B2 - - Google Patents

Info

Publication number
JPH0149201B2
JPH0149201B2 JP3177184A JP3177184A JPH0149201B2 JP H0149201 B2 JPH0149201 B2 JP H0149201B2 JP 3177184 A JP3177184 A JP 3177184A JP 3177184 A JP3177184 A JP 3177184A JP H0149201 B2 JPH0149201 B2 JP H0149201B2
Authority
JP
Japan
Prior art keywords
circularly polarized
polarized wave
waveguide
polarized waves
polarizer
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
Application number
JP3177184A
Other languages
Japanese (ja)
Other versions
JPS60176302A (en
Inventor
Hisashi Abe
Morio Higa
Tatsuhiro Noguchi
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP3177184A priority Critical patent/JPS60176302A/en
Publication of JPS60176302A publication Critical patent/JPS60176302A/en
Publication of JPH0149201B2 publication Critical patent/JPH0149201B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/165Auxiliary devices for rotating the plane of polarisation
    • H01P1/17Auxiliary devices for rotating the plane of polarisation for producing a continuously rotating polarisation, e.g. circular polarisation

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は、マイクロ波帯およびミリ波帯で使
用される偏分波器の改良に関するもので、更に詳
しく言えば、互いに直交する直線偏波を同一軸方
向に分波する偏分波器に関するものである。
Detailed Description of the Invention [Technical Field of the Invention] The present invention relates to an improvement in polarization demultiplexers used in microwave bands and millimeter wave bands. This relates to a polarization demultiplexer that demultiplexes waves in the same axial direction.

〔従来技術〕[Prior art]

従来このような偏分波器としては、第1図に示
すように円形主導波管1、直交副導波管2、共軸
副導波管3、結合窓4、短絡棒5で構成されるも
のがあつた。また他の従来例としては、第2図に
示すように円形主導波管1、2つの直交する副導
波管2a,2b、結合窓4、短絡棒5で構成され
るものがあつた。
Conventionally, such a polarization splitter is composed of a circular main waveguide 1, an orthogonal sub-waveguide 2, a coaxial sub-waveguide 3, a coupling window 4, and a shorting rod 5, as shown in FIG. Something was warm. Another conventional example includes a circular main waveguide 1, two orthogonal sub waveguides 2a and 2b, a coupling window 4, and a shorting bar 5, as shown in FIG.

いずれの偏分波器も、少なくとも1つの副導波
管は主導波管軸に直交するように配置する必要が
あり、このため、偏分波器の断面寸法が大きくな
るという欠点があつた。
In any polarization splitter, at least one sub-waveguide must be arranged perpendicular to the main waveguide axis, which has the disadvantage that the cross-sectional size of the polarization splitter becomes large.

特に、マルチビームアンテナ等においては、第
3図に示すように複数個のホーンアンテナ6をな
らべて配置し、このホーンアンテナ6に互いに直
交する直線偏波を分波する分波器7を接続する必
要がある。ところで、従来の偏分波器では主導波
管に直交するように副導波管を構成するため、こ
の副導波管が隣接する分波器7と干渉しあう欠点
があつた。
In particular, in a multi-beam antenna, a plurality of horn antennas 6 are arranged side by side as shown in FIG. There is a need. By the way, in the conventional polarization splitter, since the sub-waveguide is configured to be orthogonal to the main waveguide, this sub-waveguide has a drawback that it interferes with the adjacent splitter 7.

また、干渉を避けようとする場合には、ホーン
アンテナ6の配列位置が制限されるため、所望の
方向にビームを放射することができない等の欠点
があつた。
Furthermore, when trying to avoid interference, the array position of the horn antenna 6 is restricted, resulting in drawbacks such as the inability to radiate a beam in a desired direction.

〔発明の概要〕[Summary of the invention]

この発明は、かかる欠点を改善する目的でなさ
れたもので、空間において直線偏波を円偏波に変
換する円偏波発生器と右旋、左旋の2つの円偏波
を電波の進行方向に2つの直線偏波に分離する隔
壁偏波器とを組み合わせて構成することにより、
互いに直交する2つの直線偏波を容易に分離する
ことができ、隣接する分波器との干渉を避けるこ
とができる偏分波器を提案するものである。
This invention was made with the aim of improving such drawbacks, and includes a circularly polarized wave generator that converts linearly polarized waves into circularly polarized waves in space, and two circularly polarized waves, right-handed and left-handed, in the direction of propagation of radio waves. By configuring it in combination with a bulkhead polarizer that separates into two linearly polarized waves,
The present invention proposes a polarization splitter that can easily separate two mutually orthogonal linearly polarized waves and avoid interference with adjacent splitters.

〔発明の実施例〕[Embodiments of the invention]

まずこの発明の動作原理について簡単に説明す
る。円偏波発生器を2台用いることにより、1台
の円偏波発生器で直線偏波を右旋あるいは左旋円
偏波に変換し、もう1台の円偏波発生器で、右旋
あるいは左旋円偏波を直線偏波に変換する。従つ
て、一方の円偏波発生器つまり、円偏波を直線偏
波に変換する側において、円偏波の進行方向と同
一方向に、右旋あるいは左旋円偏波を直線偏波に
分離することができれば、互いに直交する2つの
直線偏波を同一方向に分波することができる。
First, the operating principle of this invention will be briefly explained. By using two circularly polarized wave generators, one circularly polarized wave generator converts linearly polarized waves into right-handed or left-handed circularly polarized waves, and the other circularly polarized wave generator converts them into right-handed or left-handed circularly polarized waves. Convert left-handed circularly polarized waves to linearly polarized waves. Therefore, one circularly polarized wave generator, that is, the side that converts circularly polarized waves into linearly polarized waves, separates right-handed or left-handed circularly polarized waves into linearly polarized waves in the same direction as the traveling direction of the circularly polarized waves. If possible, two mutually orthogonal linearly polarized waves can be split in the same direction.

この発明では、2台の円偏波発生器として、空
間において直線偏波を円偏波に変換するメアンダ
ライン(Meander−Line)あるいはグリツド
(Grid)などのストリツプ線路型の円偏波発生
器、および正方形導波管の断面を面積の等しい2
つの長方形断面に分割するように設けられたテー
パ状の金属板を有し、右旋と左旋の2つの円偏波
をそれぞれ上記2つの長方形断面に直線偏波とし
て分離する隔壁偏波器を用いる例について示す。
以下図面を用いて詳細に説明する。
In this invention, the two circularly polarized wave generators include a strip line type circularly polarized wave generator such as a meander-line or grid type that converts linearly polarized waves into circularly polarized waves in space; and the cross section of a square waveguide is 2 with equal area
A bulkhead polarizer is used, which has a tapered metal plate that is divided into two rectangular cross sections, and separates two circularly polarized waves, right-handed and left-handed, into the two rectangular sections as linearly polarized waves. An example will be shown.
This will be explained in detail below using the drawings.

第4図はこの発明の一実施例を示す偏分波器の
概略構造を示す図であり、図において、8はスト
リツプ線路型の円偏波発生器、9は変換導波管、
10は隔壁偏波器、11は金属板、12a,12
bは金属板11で分波される直線偏波をとり出す
変換器である。
FIG. 4 is a diagram showing a schematic structure of a polarization splitter showing an embodiment of the present invention. In the figure, 8 is a strip line type circularly polarized wave generator, 9 is a conversion waveguide,
10 is a partition wall polarizer, 11 is a metal plate, 12a, 12
b is a converter that extracts linearly polarized waves separated by the metal plate 11;

第4図に示すようにストリツプ線路型の円偏波
発生器8を配置するものとする。まず、円偏波発
生器8の左側から実線の矢印で示す直線偏波EV
が入射する場合について考える。直線偏波EV
EVに対して±45゜の傾きを有し、互いに直交する
2つの直線偏波ECとELに分解することができる。
ところで、ストリツプ線路の定数を適当に選ぶこ
とにより、ストリツプ線路に平行な偏波ECは線
路を透過する時に、45゜の位相遅れとなり、また
線路方向に直交する偏波ELは線路を透過すると
きに45゜の進み位相となり、従つて、直線偏波EV
はストリツプ線路を透過することにより、第4図
に実線で示される右旋円偏波(RHCP)に変換さ
れる。同様な原理により、点線で示される直線偏
波EHは円偏波発生器8を透過することにより点
線で示される左旋円偏波(LHCP)に変換され
る。右旋、左旋の円偏波RHCP,LHCPは、変換
導波管9を伝ぱんし隔壁偏波器10に達する。
As shown in FIG. 4, a strip line type circularly polarized wave generator 8 is arranged. First, from the left side of the circularly polarized wave generator 8, the linearly polarized wave E V shown by the solid arrow
Consider the case where is incident. The linearly polarized wave E V is
It has an inclination of ±45° with respect to E V and can be decomposed into two mutually orthogonal linearly polarized waves E C and E L.
By the way, by choosing the constants of the strip line appropriately, the polarized wave E C parallel to the strip line will have a phase delay of 45 degrees when it passes through the line, and the polarized wave E L perpendicular to the line direction will pass through the line. Therefore, the linearly polarized wave E V
is converted into right-handed circularly polarized wave (RHCP) as shown by the solid line in FIG. 4 by passing through the strip line. By the same principle, the linearly polarized wave E H shown by the dotted line is transmitted through the circularly polarized wave generator 8 and converted into a left-handed circularly polarized wave (LHCP) shown by the dotted line. The right-handed and left-handed circularly polarized waves RHCP and LHCP propagate through the conversion waveguide 9 and reach the bulkhead polarizer 10 .

ここで隔壁偏波器10の動作について簡単に説
明する。第5図、第6図は隔壁偏波器10の動作
を示すための概略図であり、a,b,cはそれぞ
れ、入口、中間、端部における電界のふるまいを
示す図である。
Here, the operation of the partition wall polarizer 10 will be briefly explained. 5 and 6 are schematic diagrams showing the operation of the partition wall polarizer 10, and a, b, and c are diagrams showing the behavior of the electric field at the entrance, middle, and end, respectively.

まず第4図で示される隔壁偏波器10に実線で
示される右旋円偏波が入射する場合を考える。
First, consider the case where a right-handed circularly polarized wave shown by a solid line is incident on the partition wall polarizer 10 shown in FIG.

右旋円偏波RHCPは、第4図に示すように振幅
が等しく位相が90゜異なる2つの互いに直交する
直線偏波AとBに分解することができる。RHCP
の場合は偏波Bは偏波Aに対して90゜の遅れ位相
となる。
As shown in FIG. 4, the right-handed circularly polarized wave RHCP can be decomposed into two mutually orthogonal linearly polarized waves A and B, which have the same amplitude and a 90° phase difference. RHCP
In this case, polarized wave B has a phase delay of 90° with respect to polarized wave A.

従つて第4図の実線で示される右旋円偏波
RHCPは第5図aの偏波Aと偏波Aに対して90゜
位相の遅れた第6図aで示す偏波Bに分解され
る。
Therefore, the right-handed circularly polarized wave shown by the solid line in Figure 4
RHCP is decomposed into polarized wave A shown in FIG. 5a and polarized wave B shown in FIG. 6a, which is delayed in phase by 90 degrees with respect to polarized wave A.

ところで、偏波Aは第5図bの状態に進むと、
金属板11の効果によつて位相遅れが生じる。金
属板11の形状を適当に選ぶことにより、隔壁偏
波器10における偏波Aを偏波Bに対して90゜の
位相遅れとすることができる。
By the way, when the polarized wave A advances to the state shown in Figure 5b,
The effect of the metal plate 11 causes a phase delay. By appropriately selecting the shape of the metal plate 11, the polarized wave A in the partition wall polarizer 10 can be delayed in phase by 90 degrees with respect to the polarized wave B.

従つて、第4図の金属板11により分割される
右旋円偏波RHCPの電界は第5図cと第6図cの
電界を同相で重ね合わせたものとなり、第7図に
示すように右側の長方形導波管に全電力が分波さ
れることになる。従つて第4図に実線で示す直線
偏波EVを同図の右側の変換器12aで取り出す
ことができる。同様な動作原理により、左旋円偏
波LHCPは左側の長方形導波管に全電力が分波さ
れるため、第4図に点線で示す直線偏波EHは左
側の変換器12bで取り出すことができる。
Therefore, the electric field of the right-handed circularly polarized wave RHCP divided by the metal plate 11 in FIG. 4 is the same phase superposition of the electric fields in FIG. 5 c and FIG. 6 c, as shown in FIG. 7. All the power will be split into the rectangular waveguide on the right. Therefore, the linearly polarized wave E V shown by the solid line in FIG. 4 can be extracted by the converter 12a on the right side of the figure. According to the same principle of operation, the left-handed circularly polarized wave LHCP has its entire power split into the rectangular waveguide on the left, so the linearly polarized wave E H shown by the dotted line in Figure 4 can be extracted by the left converter 12b. can.

以上説明した通り、第4図のように偏分波器を
構成することにより、空間において、互いに直交
する直線偏波を容易に導波管の管軸方向に分波す
ることができる。
As explained above, by configuring the polarization demultiplexer as shown in FIG. 4, mutually orthogonal linearly polarized waves can be easily demultiplexed in the direction of the tube axis of the waveguide in space.

〔発明の効果〕〔Effect of the invention〕

この発明は以上説明したとおり、空間で直線偏
波を円偏波に変換する円偏波発生器、隔壁偏波器
により偏分波器を構成することにより、従来の偏
分波器の如く、主導波管に副導波管を直交させる
ような構造とする必要がないため、偏分波器の断
面寸法を主導波管の断面寸法と同一あるいはそれ
以下とすることができる。このためホーンアンテ
ナを多数個ならべて配置するマルチビームアンテ
ナ等において絶大なる効果を期待することができ
る。
As explained above, this invention comprises a circularly polarized wave generator that converts linearly polarized waves into circularly polarized waves in space, and a partition wall polarizer, so that, like a conventional polarized beam splitter, Since there is no need for a structure in which the sub-waveguide is orthogonal to the main waveguide, the cross-sectional dimension of the polarization splitter can be made equal to or smaller than that of the main waveguide. Therefore, great effects can be expected in multi-beam antennas, etc. in which a large number of horn antennas are arranged side by side.

【図面の簡単な説明】[Brief explanation of drawings]

第1図、第2図は従来の偏分波器の概略構造
図、第3図は偏分波器の使用例を示す図、第4図
はこの発明の一実施例を示す概略構造図、第5図
〜第8図はこの発明で使用する隔壁偏波器の動作
原理を示す図であり、1は円形導波管、2は直交
副導波管、3は共軸副導波管、4は結合窓、5は
短絡棒、6はホーンアンテナ、7は分波器、8は
円偏波発生器、9は変換導波管、10は隔壁偏波
器、11は金属板、12は変換器である。なお、
図中同一符号は同一または相当部分を示すものと
する。
1 and 2 are schematic structural diagrams of a conventional polarization splitter, FIG. 3 is a diagram showing an example of the use of a polarization splitter, and FIG. 4 is a schematic structural diagram showing an embodiment of the present invention. 5 to 8 are diagrams showing the operating principle of the partition wall polarizer used in the present invention, in which 1 is a circular waveguide, 2 is an orthogonal sub-waveguide, 3 is a coaxial sub-waveguide, 4 is a coupling window, 5 is a shorting rod, 6 is a horn antenna, 7 is a splitter, 8 is a circularly polarized wave generator, 9 is a conversion waveguide, 10 is a bulkhead polarizer, 11 is a metal plate, 12 is It is a converter. In addition,
The same reference numerals in the figures indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】 1 正方形導波管の断面を面積の等しい2つの長
方形断面に分割するように設けられたテーパ状の
金属板を有し、右旋と左旋の2つの円偏波をそれ
ぞれ上記2つの長方形断面に直線偏波として分離
する隔壁偏波器、この隔壁偏波器より分波された
直線偏波を取り出す変換器、上記隔壁偏波器と空
間との間に設ける上記正方形導波管と同一断面寸
法あるいは、テーパ状に正方形または円形にひろ
がる変換導波管、空間において、直線偏波を円偏
波に変換する円偏波発生器とを備え、空間で互い
に直交する2つの直線偏波を円偏波発生器、変換
導波管、隔壁偏波器により、上記正方形導波管の
管軸方向に分波することを特徴とする偏分波器。 2 空間において直線偏波を円偏波に変換する円
偏波発生器として、メアンダライン(Meander
−Line)、あるいはグリツド(Grid)などのスト
リツプ線路型の円偏波発生器を用いることを特徴
とする特許請求の範囲第1項記載の偏分波器。
[Claims] 1. A tapered metal plate is provided to divide the cross section of a square waveguide into two rectangular cross sections with equal areas, and each waveguide receives two circularly polarized waves, right-handed and left-handed. A partition wall polarizer that separates the linearly polarized wave into the two rectangular cross sections, a converter that takes out the linearly polarized wave split from the partition wall polarizer, and the square guide provided between the partition wall polarizer and the space. It is equipped with a conversion waveguide that has the same cross-sectional dimensions as the wave tube or extends in a square or circular shape in a tapered shape, and a circularly polarized wave generator that converts linearly polarized waves into circularly polarized waves. A polarization demultiplexer characterized in that linearly polarized waves are demultiplexed in the tube axis direction of the square waveguide using a circularly polarized wave generator, a conversion waveguide, and a partition wall polarizer. 2 Meander line is a circularly polarized wave generator that converts linearly polarized waves into circularly polarized waves in space.
2. The polarization demultiplexer according to claim 1, characterized in that a strip line type circularly polarized wave generator such as a line or a grid is used.
JP3177184A 1984-02-22 1984-02-22 Polarizer Granted JPS60176302A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3177184A JPS60176302A (en) 1984-02-22 1984-02-22 Polarizer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3177184A JPS60176302A (en) 1984-02-22 1984-02-22 Polarizer

Publications (2)

Publication Number Publication Date
JPS60176302A JPS60176302A (en) 1985-09-10
JPH0149201B2 true JPH0149201B2 (en) 1989-10-24

Family

ID=12340310

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3177184A Granted JPS60176302A (en) 1984-02-22 1984-02-22 Polarizer

Country Status (1)

Country Link
JP (1) JPS60176302A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10798790B2 (en) 2012-03-14 2020-10-06 Microwave Materials Technologies, Inc. Enhanced microwave system utilizing tilted launchers

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB8619680D0 (en) * 1986-08-13 1986-09-24 Collins J L F C Flat plate array
JPS63187828A (en) * 1987-01-30 1988-08-03 Nippon Telegr & Teleph Corp <Ntt> Radio communication system commonly using polarized wave
DE69115783T2 (en) * 1990-07-26 1996-07-25 Loral Space Systems Inc Dual band antenna with multiple use of the frequency bands
JPH05283902A (en) * 1992-03-31 1993-10-29 Sony Corp Circular polarized wave generator and circular polarized wave receiving antenna
JP3650007B2 (en) 1999-11-22 2005-05-18 シャープ株式会社 Polarization separator
GB9928095D0 (en) * 1999-11-26 2000-01-26 Cambridge Ind Ltd Dual circular polarity waveguide system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10798790B2 (en) 2012-03-14 2020-10-06 Microwave Materials Technologies, Inc. Enhanced microwave system utilizing tilted launchers

Also Published As

Publication number Publication date
JPS60176302A (en) 1985-09-10

Similar Documents

Publication Publication Date Title
EP0355898B1 (en) A planar array antenna, comprising coplanar waveguide printed feed lines cooperating with apertures in a ground plane
US3389394A (en) Multiple frequency antenna
EP0457500B1 (en) Dual linear and dual circular polarization antenna
US4975712A (en) Two-dimensional scanning antenna
US9728863B2 (en) Power splitter comprising a tee coupler in the e-plane, radiating array and antenna comprising such a radiating array
US6304226B1 (en) Folded cavity-backed slot antenna
EP2330681A1 (en) Compact OMT device
US6137450A (en) Dual-linearly polarized multi-mode rectangular horn for array antennas
US11367935B2 (en) Microwave circular polarizer
JP2001237602A (en) Converter for receiving satellite double frequency band
US8089415B1 (en) Multiband radar feed system and method
US20030067367A1 (en) Dual-band electromagnetic coupler
JPH0149201B2 (en)
US9748623B1 (en) Curved filter high density microwave feed network
US3680142A (en) Circularly polarized antenna
JPH0149202B2 (en)
EP0564266B1 (en) Circular polarization apparatus for micro wave antenna
US4797643A (en) Coaxial hybrid coupler and crossing element
US4749970A (en) Compact orthomode transducer
JPS625524B2 (en)
Fonseca et al. Compact orthomode power divider for high-efficiency dual-polarisation rectangular horn antennas
Zhang An integrated coaxial circular-polarised OMJ/OMT for dual-band feed applications
US2685029A (en) Compact wide band antenna system
JPS61102802A (en) Polarized multiplexer
JPS59226505A (en) Resonance waveguide opening manifold