JP2607683B2 - Waveguide circuit - Google Patents

Waveguide circuit

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Publication number
JP2607683B2
JP2607683B2 JP1134396A JP13439689A JP2607683B2 JP 2607683 B2 JP2607683 B2 JP 2607683B2 JP 1134396 A JP1134396 A JP 1134396A JP 13439689 A JP13439689 A JP 13439689A JP 2607683 B2 JP2607683 B2 JP 2607683B2
Authority
JP
Japan
Prior art keywords
waveguide
branch
plane
circuit
electromagnetic 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 - Lifetime
Application number
JP1134396A
Other languages
Japanese (ja)
Other versions
JPH02312302A (en
Inventor
康弘 藤井
博夫 井上
利夫 安彦
活也 塚本
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.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works Ltd
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 Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP1134396A priority Critical patent/JP2607683B2/en
Publication of JPH02312302A publication Critical patent/JPH02312302A/en
Application granted granted Critical
Publication of JP2607683B2 publication Critical patent/JP2607683B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、直交する2つの偏波の電磁波を電力合成す
る導波管回路に関するものであり、例えば直交する2つ
の偏波の電磁波を受信可能な平面アンテナの導波管給電
回路として利用されるものである。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a waveguide circuit for power combining two orthogonally polarized electromagnetic waves, and for example, receives two orthogonally polarized electromagnetic waves. It is used as a waveguide feed circuit for a possible planar antenna.

[従来の技術] 従来、例えば直交する2つの偏波の電磁波を受信する
平面アレイアンテナの給電回路はストリップラインによ
り構成されており、各偏波の電磁波をストリップライン
で合成していた。しかしながら、ストリップラインは伝
送損失が大きく、この損失により平面アレイアンテナの
受信性能が劣化するという問題があった。
[Prior Art] Conventionally, for example, a feeder circuit of a planar array antenna that receives electromagnetic waves of two orthogonal polarizations is configured by a strip line, and the electromagnetic waves of each polarization are combined by the strip line. However, the stripline has a problem that transmission loss is large and the reception performance of the planar array antenna is deteriorated by the loss.

[発明が解決しようとする課題] そこで、平面アレイアンテナの給電回路を導波管回路
で構成することが考えられる。この場合、平面アレイア
ンテナにおける個々のアンテナ素子から出力される各偏
波の電磁波に対応して2系列の導波管による給電回路を
設ける必要がある。このため、給電回路の構成は立体的
に非常に複雑なものとなり、製品コストの上昇を招くと
共に、平面アレイアンテナの平面性をも損なうという問
題があった。
[Problems to be Solved by the Invention] Therefore, it is conceivable to configure a feed circuit of the planar array antenna with a waveguide circuit. In this case, it is necessary to provide a feed circuit using two series of waveguides corresponding to each polarized electromagnetic wave output from each antenna element in the planar array antenna. For this reason, the configuration of the power supply circuit becomes very complicated three-dimensionally, which leads to an increase in product cost and a problem of impairing the flatness of the planar array antenna.

本発明はこのような点に鑑みてなされたものであり、
その目的とするところは、直交する2つの偏波の電磁波
の電力合成を1系列の導波管にて同一平面上で達成でき
る導波管回路を提供することにある。
The present invention has been made in view of such a point,
An object of the present invention is to provide a waveguide circuit capable of achieving power combining of two orthogonally polarized electromagnetic waves on the same plane using a series of waveguides.

[課題を解決するための手段] 本発明に係る導波管回路にあっては、上記の課題を解
決するために、第1図に示すように、方形導波管により
構成される電力合成回路であって、一対の電磁波入力端
A,Bの近傍に入力電磁波の伝搬方向を同一平面内で相対
向する方向に変換するL型ベンド1をそれぞれ備え、前
記平面内を相対向する方向に伝搬される前記一対の電磁
波入力を前記平面内にて直交する伝搬方向の電磁波に電
力合成するT型分岐2を備え、各L型ベンド1から前記
T型分岐2までの距離は導波管の管内波長をλgとする
と、λg/2だけ異なることを特徴とするものである。
[Means for Solving the Problems] In a waveguide circuit according to the present invention, in order to solve the above problems, as shown in FIG. 1, a power combining circuit constituted by a rectangular waveguide And a pair of electromagnetic wave input terminals
A pair of L-shaped bends 1 are provided in the vicinity of A and B for converting the propagation direction of the input electromagnetic wave into opposing directions in the same plane, and the pair of electromagnetic wave inputs propagating in the opposing directions in the plane. A T-branch 2 is provided for combining electric power with electromagnetic waves in orthogonal propagation directions in a plane. The distance from each L-bend 1 to the T-branch 2 is λg / 2, where λg is the waveguide wavelength of the waveguide. Only the difference.

[作用] 本発明にあっては、このように、一対のL型ベンド1
からT型分岐2までの距離がλg/2だけ異なるので、導
波管内を直交する2つの偏波で伝搬される電磁波の電力
合成が各々の偏波について成されるものであり、直交す
る2つの偏波の電磁波の電力合成を1つの導波管回路に
より達成できる。
[Operation] In the present invention, a pair of L-shaped bends 1
Is different from the T-shaped branch 2 by λg / 2, the power of the electromagnetic waves propagated by the two polarizations orthogonal to each other in the waveguide is synthesized for each polarization. Power combining of two polarized electromagnetic waves can be achieved by one waveguide circuit.

[実施例] 第1図は本発明の一実施例に係る導波管回路の斜視図
である。この導波管回路に用いられる方形導波管の基本
モードはTE10モードである。説明の便宜上、第1図にお
いて、実線の矢印で示した偏波をTE10モード、破線の矢
印で示した偏波をTE01モードとする。
FIG. 1 is a perspective view of a waveguide circuit according to one embodiment of the present invention. The fundamental mode of the rectangular waveguide used in the waveguide circuit is a TE 10 mode. For convenience of explanation, in FIG. 1, to the polarization of the TE 10 mode shown by the solid arrows, the polarization indicated by the dashed arrows TE 01 mode.

この導波管回路は、例えば、第4図に示すように、水
平偏波及び垂直偏波の2偏波を受信可能な平面アレイア
ンテナ3の並列給電回路として使用される。第4図に示
す平面アレイアンテナ3における個々のアンテナ素子4
は、実線で示す水平偏波と破線で示す垂直偏波の受信が
可能な導波管開口アンテナよりなる。したがって、第1
図に示す導波管回路において、電磁波入力端A,B,C,Dに
は、実線の矢印で示す偏波と、破線の矢印で示す偏波が
入力される。
This waveguide circuit is used, for example, as shown in FIG. 4, as a parallel feed circuit of a planar array antenna 3 capable of receiving two polarized waves, that is, a horizontally polarized wave and a vertically polarized wave. Individual antenna elements 4 in planar array antenna 3 shown in FIG.
Consists of a waveguide aperture antenna capable of receiving horizontal polarization indicated by a solid line and vertical polarization indicated by a broken line. Therefore, the first
In the waveguide circuit shown in the figure, the polarization indicated by the solid arrow and the polarization indicated by the dashed arrow are input to the electromagnetic wave input terminals A, B, C, and D.

第1図において、電磁波入力端A,Bに設けられたL型
ベンド1は、実線の矢印で示すTE10モードの電磁波に対
しては、第3図(a)に示すように、H面(磁界に平行
な面)のL型ベンド(Hコーナ)として作用する。した
がって、L型ベンドにより電磁波は伝送方向を変えて、
A′面、B′面では図示のように同位相で振動してい
る。このようにして、L型ベンド1により平面アレイア
ンテナの裏面に沿う方向に伝搬方向を変換したTE10モー
ドの電磁波を、T型分岐2により同じくアンテナの裏面
に沿う方向に電力合成する場合には、第2図(b)に示
すようなE面分岐を使用することとなる。ここで、E面
分岐を使用する場合、合成する2つの電磁波(図中、
)はT型分岐2において位相が反転している必要があ
る。そこで、第1図に示す第1のT型分岐2を構成して
いる点Pは、A′面及びB′面から等距離の点よりλg/
4シフトした点としている。このため、A′−P間の距
離とB′−P間の距離とにλg/2の差が生じるので、
A′面とB′面で同位相であったTE10モードの電磁波
は、P点においては逆相となり、第2図(b)に示すE
面分岐により1つの電磁波(図中)に合成される。
In FIG. 1, the L-shaped bend 1 provided at the electromagnetic wave input terminals A and B has an H surface (see FIG. 3A) with respect to a TE 10 mode electromagnetic wave indicated by a solid arrow. It acts as an L-shaped bend (H corner) of a plane parallel to the magnetic field. Therefore, the electromagnetic wave changes its transmission direction due to the L-shaped bend,
The planes A 'and B' vibrate in the same phase as shown. In this manner, when the TE 10 mode electromagnetic wave whose propagation direction is changed in the direction along the back surface of the planar array antenna by the L-shaped bend 1 is power-combined in the direction along the back surface of the antenna by the T-shaped branch 2, In this case, an E-plane branch as shown in FIG. 2B is used. Here, when the E-plane branching is used, two electromagnetic waves to be synthesized (in the figure,
) Requires the phase to be inverted in the T-branch 2. Therefore, the point P constituting the first T-shaped branch 2 shown in FIG. 1 is λg / point from a point equidistant from the A ′ plane and the B ′ plane.
4 points have been shifted. Therefore, a difference of λg / 2 occurs between the distance between A′-P and the distance between B′-P,
A 'plane and B' plane in the electromagnetic wave of the TE 10 mode was in phase becomes a reverse phase in the point P, E shown in FIG. 2 (b)
It is combined into one electromagnetic wave (in the figure) by the surface branch.

一方、破線の矢印で示すTE01モードの電磁波に対して
は、第1図の電磁波入力端A,Bに設けられたL型ベンド
は、第3図(b)に示すように、E面(電界に平行な
面)のL型ベンド(Eコーナ)として作用する。したが
って、L型ベンドにより電磁波は伝送方向を変えて、
A′面、B′面では図示のように逆位相で振動してい
る。このようにして、L型ベンド1により平面アレイア
ンテナの裏面に沿う方向に伝搬方向を変換したTE01モー
ドの電磁波を、T型分岐2により同じくアンテナの裏面
に沿う方向に電力合成する場合には、第2図(a)に示
すようなH面分岐を使用することとなる。ここで、H面
分岐を使用する場合、合成する2つの電磁波(図中、
)はT型分岐において位相が一致している必要があ
る。上述のように、第1図に示す第1のT型分岐2を構
成している点Pは、A′面及びB′面から等距離の点よ
りλg/4シフトした点としている。このため、A′−P
間の距離とB′−P間の距離とにλg/2の差が生じるの
で、A′面とB′面で逆位相であったTE01モードの電磁
波は、P点においては同相となり、第2図(a)に示す
H面分岐により1つの電磁波(図中)に合成される。
On the other hand, for electromagnetic waves in TE 01 mode shown by the dashed arrows, the electromagnetic wave input terminal A of FIG. 1, L-type bends provided in the B, as shown in FIG. 3 (b), E plane ( It acts as an L-shaped bend (E corner) of a plane parallel to the electric field. Therefore, the electromagnetic wave changes its transmission direction due to the L-shaped bend,
The planes A 'and B' vibrate in opposite phases as shown. In this manner, when the TE 01 mode electromagnetic wave whose propagation direction is changed in the direction along the back surface of the planar array antenna by the L-shaped bend 1 is power-combined in the direction along the back surface of the antenna by the T-shaped branch 2, , H-plane branching as shown in FIG. 2 (a) will be used. Here, when the H-plane branch is used, two electromagnetic waves to be synthesized (in the figure,
) Requires that the phases coincide in the T-shaped branch. As described above, the point P forming the first T-shaped branch 2 shown in FIG. 1 is a point shifted by λg / 4 from a point equidistant from the A ′ plane and the B ′ plane. Therefore, A'-P
Since the difference between the lambda] g / 2 to the distance between the distance and B'-P between occurs, the electromagnetic wave of the TE 01 mode which was the opposite phase A 'plane and B' plane, in phase in the point P, the 2A single electromagnetic wave (in the figure) is synthesized by the H-plane branch shown in FIG.

さらに、第1図に示すように、別の1組の電磁波入力
端C,Dから入力されたTE10モード及びTE01モードの電磁
波についても、点Qにおいて電力合成し、点P,Qの対向
する側(内側)の点Rにおいて、第2のT型分岐5を構
成する。このとき、実線で示すTE10モードの電磁波は点
P,Qで逆相となり、破線で示すTE01モードの電磁波は点
P,Qで同相となる。したがって、点P,Qから等距離にある
点RにT型分岐5を構成すれば、TE10モードの電磁波に
対してはE面分岐として、TE01モードの電磁波に対して
はH面分岐として作用し、両モードの電磁波について同
時に電力合成が成される。これにより、第4図に示すよ
うな4素子の平面アレイアンテナについて、直交する2
つの偏波の電磁波の給電回路を1系統の導波管回路で構
成することができる。
Further, as shown in FIG. 1, the power of the TE 10 mode and TE 01 mode electromagnetic waves input from another pair of electromagnetic wave input terminals C and D is combined at the point Q, and the points P and Q are opposed to each other. A second T-shaped branch 5 is formed at a point R on the side (inner side) where the light beam flows. At this time, the TE 10 mode electromagnetic wave shown by the solid line
The phase is reversed at P and Q, and the electromagnetic wave in TE 01 mode indicated by the broken line
P and Q are in phase. Therefore, by forming the T-shaped branch 5 point P, from Q to point R are equidistant, as E-plane branch to electromagnetic waves of TE 10 mode, the H face branch for electromagnetic waves in TE 01 mode Acting, power is simultaneously synthesized for both modes of electromagnetic waves. As a result, for a four-element planar array antenna as shown in FIG.
A power supply circuit for two polarized electromagnetic waves can be constituted by a single-system waveguide circuit.

第5図は本発明の他の実施例の概略構成図である。本
実施例にあっては、第1図に示すような導波管回路を2
組設けて、各導波管回路における第2のT型分岐の対向
する側(内側)の点Sに、第3のT型分岐6を設けたも
のである。この第3のT型分岐6を設ける点Sは、各導
波管回路における第2のT型分岐5から等距離の位置に
ある。このため、点SにおいてTE10モードの電磁波は逆
相、TE01モードの電磁波は同相となり、第3のT型分岐
6はそれぞれE面分岐及びH面分岐として作用し、2つ
のモードの電磁波を同時に電力合成することができる。
これにより、8素子の平面アレイアンテナについて、直
交する2つの偏波の電磁波の給電回路を1系統の導波管
回路で構成することができる。
FIG. 5 is a schematic configuration diagram of another embodiment of the present invention. In this embodiment, a waveguide circuit as shown in FIG.
A third T-shaped branch 6 is provided at a point S on the opposite side (inner side) of the second T-shaped branch in each waveguide circuit. The point S where the third T-branch 6 is provided is located at an equidistant distance from the second T-branch 5 in each waveguide circuit. Therefore, at the point S, the electromagnetic wave in the TE 10 mode is in the opposite phase and the electromagnetic wave in the TE 01 mode is in the same phase, and the third T-shaped branch 6 acts as an E-plane branch and an H-plane branch, respectively, and the electromagnetic waves in the two modes are transmitted. Power can be combined at the same time.
Thus, for an eight-element planar array antenna, a feed circuit for two orthogonally polarized electromagnetic waves can be configured with one system of waveguide circuits.

さらにまた、第5図に示すような導波管回路を2組設
けて、各導波管回路における第3のT型分岐の対向する
側(内側)の中間点に、第4のT型分岐を設ければ、16
素子の平面アレイアンテナ用の導波管給電回路を構成で
きる。以下、同様にして、2n素子(n≧5)の平面アレ
イアンテナ用の導波管給電回路を構成することもでき
る。この場合に必要なT型分岐の個数は(2n−1)個で
ある。
Further, two sets of waveguide circuits as shown in FIG. 5 are provided, and a fourth T-shaped branch is provided at an intermediate point on the opposite side (inside) of the third T-shaped branch in each waveguide circuit. Is provided, 16
A waveguide feed circuit for a planar array antenna of elements can be configured. Hereinafter, similarly, a waveguide feeding circuit for a 2n element (n ≧ 5) planar array antenna can be configured. In this case, the number of T-type branches required is (2 n -1).

[発明の効果] 本発明は方形導波管による電力合成回路であって、一
対の電磁波入力端の近傍に設けたL型ベンドにより入力
電磁波の伝搬方向を同一平面内で相対向する方向とし、
この一対の入力電磁波をT型分岐により前記平面内で直
交する伝搬方向に電力合成し、各L型ベンドからT型分
岐までの距離は導波管内の半波長分異なるようにしたの
で、直交する2つの偏波の電磁波を1系統の方形導波管
により同一平面上で電力合成できるという効果がある。
[Effects of the Invention] The present invention relates to a power combining circuit using a rectangular waveguide, in which an L-shaped bend provided near a pair of electromagnetic wave input terminals causes input electromagnetic waves to propagate in opposite directions in the same plane,
The pair of input electromagnetic waves are power-combined by the T-shaped branch in the direction of propagation orthogonal to each other in the plane, and the distance from each L-bend to the T-shaped branch is made different by a half wavelength in the waveguide. There is an effect that two polarized electromagnetic waves can be combined in power on the same plane by one system of rectangular waveguide.

また、同様の導波管回路をT型分岐により複数段接続
することにより、2n分岐の電力合成回路を構成できると
いう効果がある。
In addition, there is an effect that a 2n- branch power combining circuit can be configured by connecting a plurality of similar waveguide circuits by T-shaped branches.

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

第1図は本発明の一実施例の斜視図、第2図(a),
(b)は同上に用いるT型分岐の動作説明図、第3図
(a),(b)は同上に用いるL型ベンドの動作説明
図、第4図は同上の実施例により給電される平面アレイ
アンテナの斜視図、第5図は本発明の他の実施例の概略
構成図である。 1はL型ベンド、2はT型分岐、A,Bは電磁波入力端で
ある。
FIG. 1 is a perspective view of an embodiment of the present invention, and FIG.
(B) is an explanatory view of the operation of the T-type branch used in the above, FIGS. 3 (a) and 3 (b) are operational explanatory views of the L-type bend used in the above, and FIG. FIG. 5 is a perspective view of an array antenna, and FIG. 5 is a schematic configuration diagram of another embodiment of the present invention. 1 is an L-shaped bend, 2 is a T-shaped branch, and A and B are electromagnetic wave input terminals.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 塚本 活也 大阪府門真市大字門真1048番地 松下電 工株式会社内 (56)参考文献 特開 昭62−58706(JP,A) 実開 昭62−181003(JP,U) 特公 昭34−6816(JP,B1) ──────────────────────────────────────────────────続 き Continuation of the front page (72) Inventor Kuya Tsukamoto 1048 Oaza Kadoma, Kadoma City, Osaka Prefecture Matsushita Electric Works, Ltd. (56) References JP-A-62-58706 (JP, A) 181003 (JP, U) JP34-6816 (JP, B1)

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】方形導波管により構成される電力合成回路
であって、一対の電磁波入力端の近傍に入力電磁場の伝
搬方向を同一平面内で相対向する方向に変換するL型ベ
ンドをそれぞれ備え、前記平面内を相対向する方向に伝
搬される前記一対の電磁波入力を前記平面内にて直交す
る伝搬方向の電磁波に電力合成するT型分岐を備え、各
L型ベンドから前記T型分岐までの距離は導波管内の半
波長分異なることを特徴とする導波管回路。
1. An electric power combining circuit comprising a rectangular waveguide, wherein L-shaped bends for converting a propagation direction of an input electromagnetic field into opposing directions in the same plane are provided near a pair of electromagnetic wave input terminals. A T-branch for power combining the pair of electromagnetic wave inputs propagated in opposite directions in the plane with electromagnetic waves in propagation directions orthogonal to each other in the plane; The waveguide circuit is characterized in that the distance to the waveguide differs by half a wavelength in the waveguide.
【請求項2】請求項1記載の導波管回路を一対備え、各
導波管回路におけるT型分岐から出力される電磁波が前
記平面内で相対向する方向に伝搬されるように各導波管
回路を配置し、各導波管回路から出力される電磁波を前
記平面内にて直交する伝搬方向に電力合成する第2のT
型分岐を備え、第2のT型分岐と各導波管回路のT型分
岐とは等距離に配置されていることを特徴とする導波管
回路。
2. A waveguide circuit comprising a pair of waveguide circuits according to claim 1, wherein each electromagnetic wave output from a T-shaped branch in each waveguide circuit is propagated in opposite directions in said plane. A second T for arranging tube circuits and combining powers of electromagnetic waves output from the respective waveguide circuits in orthogonal propagation directions in the plane.
A waveguide circuit comprising a mold branch, wherein the second T-branch and the T-branch of each waveguide circuit are arranged at an equal distance.
【請求項3】請求項2記載の導波管回路を2n個(nは1
以上の整数)備え、前記2n個の導波管回路から出力され
る電磁波を前記平面内で電力合成するT型分岐を(2n
1)個備えることを特徴とする導波管回路。
Wherein the 2 n a waveguide circuit according to claim 2, wherein (n is 1
(The above integer), and a T-shaped branch (2 n −) for power combining electromagnetic waves output from the 2 n waveguide circuits in the plane.
1) A waveguide circuit comprising:
JP1134396A 1989-05-26 1989-05-26 Waveguide circuit Expired - Lifetime JP2607683B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1134396A JP2607683B2 (en) 1989-05-26 1989-05-26 Waveguide circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1134396A JP2607683B2 (en) 1989-05-26 1989-05-26 Waveguide circuit

Publications (2)

Publication Number Publication Date
JPH02312302A JPH02312302A (en) 1990-12-27
JP2607683B2 true JP2607683B2 (en) 1997-05-07

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JP1134396A Expired - Lifetime JP2607683B2 (en) 1989-05-26 1989-05-26 Waveguide circuit

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4003498B2 (en) 2002-03-25 2007-11-07 三菱電機株式会社 High frequency module and antenna device
JP4709601B2 (en) * 2005-07-19 2011-06-22 日本無線株式会社 Waveguide slot array antenna
JP4980248B2 (en) * 2007-03-29 2012-07-18 三菱電機株式会社 Array antenna device
RU2017108850A (en) * 2014-08-18 2018-09-20 Нек Корпорейшн STRUCTURE FOR TRANSFORMING ELECTRIC FIELD DIRECTIONS AND PLANAR ANTENNA

Also Published As

Publication number Publication date
JPH02312302A (en) 1990-12-27

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