JPH04267606A - Primary radiator in common use for vertically and horizontally polarized wave - Google Patents

Primary radiator in common use for vertically and horizontally polarized wave

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Publication number
JPH04267606A
JPH04267606A JP4922391A JP4922391A JPH04267606A JP H04267606 A JPH04267606 A JP H04267606A JP 4922391 A JP4922391 A JP 4922391A JP 4922391 A JP4922391 A JP 4922391A JP H04267606 A JPH04267606 A JP H04267606A
Authority
JP
Japan
Prior art keywords
linearly polarized
waveguide
phase circuit
probe
output means
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.)
Pending
Application number
JP4922391A
Other languages
Japanese (ja)
Inventor
Katsuaki Kaminakada
上中田 勝明
Shoichi Furukawa
昌一 古川
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.)
Fujitsu General Ltd
Original Assignee
Fujitsu General 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 Fujitsu General Ltd filed Critical Fujitsu General Ltd
Priority to JP4922391A priority Critical patent/JPH04267606A/en
Publication of JPH04267606A publication Critical patent/JPH04267606A/en
Pending legal-status Critical Current

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  • Waveguide Aerials (AREA)

Abstract

PURPOSE:To facilitate the handling and to attain excellent external appearance by using a waveguide bonded to a circularly waveguide from a same direction with respect to the vertical and horizontal polarized wave common use primary radiator employing a circular waveguide so as to extract a vertically and a horizontally polarized wave signal. CONSTITUTION:One end of a circular waveguide 2 is formed to be a horn aperture 1 able to introduce a vertical and horizontal linearly polarized wave signal, the other end is formed to be a termination face 5, a square waveguide 7 as an output means of a linearly polarized wave signal is bonded to the opening 1 and a phase circuit 4 is provided to the termination face 5 and a square waveguide 9 as an output means of the other linearly polarized wave signal is bonded in the mmddle of the same phase circuit 4 and the same phase circuit 4 delays the phase of the other linearly polarized wave signal to extract an output while the guide axis direction of the square waveguides 7,9 is made identical. A probe may be used in place of the square waveguide.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は、垂直偏波及び水平偏波
で送信されてくる通信衛星(CS)の電波を受信する垂
直及び水平偏波共用一次放射器に関する。通信衛星の電
波は、円偏波を使用している衛星放送の電波と異なり、
直線偏波方式が採用されており、同じ帯域内でより多く
のチャンネルが伝送できるようにするため、垂直偏波及
び水平偏波の電波が使用されている。従って、一台のパ
ラボラアンテナで垂直偏波及び水平偏波の電波を受信す
るため、垂直及び水平偏波共用一次放射器が使用され、
同垂直及び水平偏波共用一次放射器から垂直偏波信号と
水平偏波信号とを取り出し、各々のCSコンバータに入
力して通信衛星(CS)からの電波を受信するようにし
ている。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a primary radiator for both vertical and horizontal polarization, which receives communication satellite (CS) radio waves transmitted in vertical and horizontal polarization. Communication satellite radio waves differ from satellite broadcasting radio waves, which use circularly polarized waves.
Linear polarization is used, and vertically and horizontally polarized radio waves are used to allow more channels to be transmitted within the same band. Therefore, in order to receive vertically polarized and horizontally polarized radio waves with one parabolic antenna, a primary radiator for both vertical and horizontal polarization is used.
A vertically polarized signal and a horizontally polarized signal are taken out from the vertically and horizontally polarized primary radiator and input to each CS converter to receive radio waves from a communication satellite (CS).

【0002】0002

【従来の技術】従来の垂直及び水平偏波共用一次放射器
は、図13に示すように円形導波管2の一端を垂直及び
水平直線偏波の信号を導入し得るホーン形の開口1とし
、他端を終端面5とし、開口1側に水平偏波信号の出力
手段として方形導波管24を下方に向かって接合し、終
端面5側に垂直偏波信号の出力手段として方形導波管2
5を水平方向に接合して、各々直角に交差する電界とな
っている垂直偏波信号と水平偏波信号を各々の方形導波
管で取り出すようにして、各々CSコンバータに信号を
入力して通信衛星からの電波を受信するようにしていた
2. Description of the Related Art A conventional primary radiator for vertically and horizontally polarized waves has one end of a circular waveguide 2 as a horn-shaped opening 1 capable of introducing vertically and horizontally linearly polarized signals, as shown in FIG. , the other end is the termination surface 5, a rectangular waveguide 24 is connected downward to the aperture 1 side as an output means for a horizontally polarized signal, and a rectangular waveguide is connected to the termination surface 5 side as an output means for a vertically polarized signal. tube 2
5 are connected in the horizontal direction, and the vertically polarized signal and the horizontally polarized signal, which have electric fields crossing at right angles, are taken out by each rectangular waveguide, and the signals are input to the CS converter. It was designed to receive radio waves from communication satellites.

【0003】0003

【発明が解決しようとする課題】従って、方形導波管2
4と方形導波管25の管軸方向は直角に交差する向きで
円形導波管2に接合されており、さらに、方形導波管2
4と方形導波管25の先端には各々CSコンバータが取
り付けられ、同CSコンバータからの出力ケーブルも、
また直角に交差する方向で引き出されるため、取り扱い
がしにくく、見映えが悪いといった問題点があった。本
発明は、二つの方形導波管の管軸方向を略同一方向にし
て円形導波管に接合することにより、取り扱いやすく、
また、外観上も見映えの良い垂直及び水平偏波共用一次
放射器を提供することを目的とする。
[Problem to be Solved by the Invention] Therefore, the rectangular waveguide 2
4 and the rectangular waveguide 25 are joined to the circular waveguide 2 with their tube axes intersecting at right angles, and the rectangular waveguide 2
4 and the tip of the rectangular waveguide 25 are each equipped with a CS converter, and the output cable from the CS converter is also
In addition, since they are pulled out at right angles, they are difficult to handle and have a poor appearance. The present invention is easy to handle by joining two rectangular waveguides to a circular waveguide with their tube axes in substantially the same direction.
Another object of the present invention is to provide a primary radiator for both vertical and horizontal polarization that has a good appearance.

【0004】0004

【課題を解決するための手段】図1は、本発明の垂直及
び水平偏波共用一次放射器の原理説明図であり、同図に
示すように、円形導波管2の一端を垂直及び水平の直線
偏波の信号を導入し得るホーン形の開口1とし、他端を
終端面5とし、開口1側に一方の直線偏波信号の第1出
力手段として方形導波管7を接合し、終端面5側に位相
回路4を設けて同位相回路4の中間に他方の直線偏波信
号の第2出力手段として第2方形導波管9を接合し、前
記位相回路4で他方の直線偏波信号の位相を遅延させる
ことにより、前記第1方形導波管と第2方形導波管の管
軸方向を略同一方向に接合して出力を取り出すようにし
ている。
[Means for Solving the Problems] FIG. 1 is a diagram explaining the principle of a primary radiator for both vertical and horizontal polarization according to the present invention. As shown in the figure, one end of a circular waveguide 2 is A horn-shaped aperture 1 capable of introducing a linearly polarized signal, the other end is a termination surface 5, and a rectangular waveguide 7 is connected to the aperture 1 side as a first output means for one linearly polarized signal, A phase circuit 4 is provided on the termination surface 5 side, and a second rectangular waveguide 9 is connected between the same phase circuits 4 as a second output means for the other linearly polarized signal. By delaying the phase of the wave signal, the tube axes of the first rectangular waveguide and the second rectangular waveguide are joined in substantially the same direction, and output is extracted.

【0005】[0005]

【作用】本発明は上記した構成により、垂直偏波の電波
と水平偏波の電波を受信するようにしており、円形導波
管2の一端のホーン形の開口1に導入される水平偏波の
電界は、図5に示すように、水平方向をX軸とし、垂直
方向をY軸とすると、X軸方向のベクトル成分Ehx 
、Y軸方向のベクトル成分Ehy を有し、Ehx と
Ehy を合成した電界Ehとして示すことができ、同
様に、円形導波管2の一端のホーン形の開口1に導入さ
れる垂直偏波の電界は、X軸方向のベクトル成分Evx
 、Y軸方向のベクトル成分Evy を有し、Evx 
とEvy を合成した電界Evとして示すことができる
[Operation] With the above-described configuration, the present invention receives vertically polarized radio waves and horizontally polarized radio waves, and horizontally polarized waves are introduced into the horn-shaped opening 1 at one end of the circular waveguide 2. As shown in Figure 5, if the horizontal direction is the X-axis and the vertical direction is the Y-axis, the electric field in the X-axis direction is the vector component Ehx
, has a vector component Ehy in the Y-axis direction, and can be expressed as an electric field Eh that is a combination of Ehx and Ehy. Similarly, the vertically polarized wave introduced into the horn-shaped aperture 1 at one end of the circular waveguide 2 The electric field is a vector component Evx in the X-axis direction.
, has a vector component Evy in the Y-axis direction, and Evx
and Evy can be expressed as a combined electric field Ev.

【0006】従って、円形導波管2の一端のホーン形の
開口1に導入される水平偏波と垂直偏波の電界は、図5
に示すように、各々直角に交差する電界となっているた
め、図2に示すように円形導波管2の内部の方形導波管
7と方形導波管9の接合箇所間に位相回路4a を設け
て、垂直偏波の電界のX軸方向のベクトル成分Evx 
を約90度遅延させ、円形導波管2の終端面5に設けた
位相回路4b で更に前記ベクトル成分Evx を約9
0度遅延させるようにし、位相回路4a 及び4b を
合わせて図1に示すように円形導波管2の終端面5に設
けるようにすれば、前記ベクトル成分Evx を180
度遅延させることができ、図5に点線で示すようなX軸
方向のベクトル成分としてEvx ′を有する電界Ev
′が得られるため、方形導波管7と方形導波管9の管軸
方向を略同一方向にして円形導波管2に接合するように
しても、方形導波管7から水平偏波の信号を取り出すこ
とができ、方形導波管9から垂直偏波の信号を取り出す
ことができる。
Therefore, the electric fields of the horizontally polarized wave and the vertically polarized wave introduced into the horn-shaped opening 1 at one end of the circular waveguide 2 are as shown in FIG.
As shown in FIG. 2, since the electric fields intersect at right angles, a phase circuit 4a is installed between the junction of the rectangular waveguide 7 and the rectangular waveguide 9 inside the circular waveguide 2, as shown in FIG. and the vector component Evx in the X-axis direction of the vertically polarized electric field
is delayed by about 90 degrees, and a phase circuit 4b provided on the terminal surface 5 of the circular waveguide 2 further delays the vector component Evx by about 90 degrees.
If the delay is 0 degrees and the phase circuits 4a and 4b are provided together at the end face 5 of the circular waveguide 2 as shown in FIG.
The electric field Ev has Evx′ as a vector component in the X-axis direction as shown by the dotted line in FIG.
' is obtained, so even if the rectangular waveguide 7 and the rectangular waveguide 9 are connected to the circular waveguide 2 with their tube axes in substantially the same direction, the horizontally polarized wave from the rectangular waveguide 7 is A signal can be extracted, and a vertically polarized signal can be extracted from the rectangular waveguide 9.

【0007】同様にして、方形導波管7から垂直偏波の
信号を取り出すようにし、図5に示す水平偏波の電界の
X軸方向のベクトル成分Ehx を位相回路4で180
度遅延させることにより、方形導波管9から水平偏波の
信号を取り出すようにしても、方形導波管7と方形導波
管9の管軸方向を略同一方向とすることができる。従っ
て、円形導波管に二つの方形導波管の管軸方向を略同一
方向にして接合することができるため、外観上の見映え
もよくすることができ、二つの方形導波管の先端に各々
CSコンバータを接合する場合、略同位置にCSコンバ
ータを配置できるため、各々のCSコンバータの外箱を
共通にすることも可能となり、取り扱いをしやすくする
ことができる。
Similarly, a vertically polarized signal is taken out from the rectangular waveguide 7, and the vector component Ehx in the X-axis direction of the horizontally polarized electric field shown in FIG.
Even if a horizontally polarized signal is extracted from the rectangular waveguide 9 by delaying the rectangular waveguide 9, the tube axes of the rectangular waveguide 7 and the rectangular waveguide 9 can be made substantially the same direction. Therefore, since it is possible to join two rectangular waveguides to a circular waveguide with their tube axes in the same direction, the appearance can be improved, and the tips of the two rectangular waveguides can be When the CS converters are joined to each other, the CS converters can be placed at substantially the same position, so it is possible to use the same outer box for each CS converter, which makes handling easier.

【0008】図2において用いられている位相回路4a
は導波管に通常使用される配置となっており説明を省略
するが、終端面5に設けた位相回路4b の作用につい
て以下に説明する。図3は、本発明の円偏波/直線偏波
変換器の原理説明用の等価構成図であり、入出力手段と
してプローブ10を用い、同プローブ10と円形導波管
2の終端面5迄の長さをLとし、プローブ10に電流I
を流して電波を励振させたとすると、円形導波管2の開
口に向かう電磁界Eは、プローブ10から直接開口に向
かう電磁界成分Ea と、プローブ10から出て終端面
5で反射して開口に向かう電磁界成分Eb との合成で
表される。従って、E=Ea +Eb ・・・・・■
Phase circuit 4a used in FIG.
Although the arrangement is generally used in waveguides and the explanation thereof will be omitted, the operation of the phase circuit 4b provided on the termination surface 5 will be explained below. FIG. 3 is an equivalent configuration diagram for explaining the principle of the circularly polarized wave/linearly polarized wave converter of the present invention. Let the length of the probe 10 be L, and the current I to the probe 10
When a radio wave is excited by excitation of a radio wave, the electromagnetic field E directed toward the aperture of the circular waveguide 2 consists of an electromagnetic field component Ea directed from the probe 10 directly toward the aperture, and an electromagnetic field component Ea that exits the probe 10 and is reflected by the end surface 5 to form the aperture. It is expressed as a combination with the electromagnetic field component Eb directed toward . Therefore, E=Ea +Eb...■


0009】円形導波管の終端面をZ=0とし、管軸方向
にZ軸をとり、 A=円形導波管内の電波の振幅定数 β=円形導波管内の電波の波数 とすると、Ea は次式で示される。 Ea =A・exp[j{ωt−β(Z−L)}]・・
・・・■ Eb は図3のように、終端面5より右方にLだけ離れ
た位置でプローブ11に電流−Iを流して電波を励振さ
せたものと等価となり、次式で示される。 Eb =−A・exp[j{ωt−β(Z+L)}]・
・・・・■ 従って、Eは■、■、■の各式から次式で示される。   E=A・exp[j{ωt−β(Z−L)}]  
    −A・exp[j{ωt−β(Z+L)}] 
   =A・exp[j{ωt−βZ}] ・[exp
{jβL}−exp {−jβL}]     =j2
A・SIN(βL) ・exp[j{ωt−βZ}] 
・・・・・■従って、プローブ10で電磁波を励振させ
た場合、円形導波管2中に発生する電磁波の位相は、■
式によれば終端面5からの距離Zと波数βで変化するこ
とを示している。
[
[0009] Let Z = 0 at the end surface of the circular waveguide, take the Z axis in the direction of the tube axis, and let A = amplitude constant of the radio wave in the circular waveguide β = wave number of the radio wave in the circular waveguide, then Ea is It is shown by the following formula. Ea =A・exp[j{ωt−β(Z−L)}]・・
As shown in FIG. 3, Eb is equivalent to excitation of a radio wave by passing a current -I through the probe 11 at a position a distance L to the right from the end surface 5, and is expressed by the following equation. Eb =-A・exp[j{ωt-β(Z+L)}]・
...■ Therefore, E is expressed by the following formula from the formulas ■, ■, and ■. E=A・exp[j{ωt−β(Z−L)}]
−A・exp[j{ωt−β(Z+L)}]
=A・exp[j{ωt−βZ}]・[exp
{jβL}−exp {−jβL}] =j2
A・SIN(βL)・exp[j{ωt−βZ}]
...■ Therefore, when electromagnetic waves are excited by the probe 10, the phase of the electromagnetic waves generated in the circular waveguide 2 is:
According to the formula, it is shown that it changes depending on the distance Z from the termination surface 5 and the wave number β.

【0010】図4は本発明の円偏波/直線偏波変換器の
原理説明図であり、円形導波管2の内部にプローブ10
と、管内波長が異なり直交した2つの電磁波のモードを
有し、管軸方向の長さLb の位相回路4b を設けて
いる。プローブ10で電磁波を励振させ、同電磁波の位
相回路4b 中を伝播する直交した2つのモードの電磁
波の電界を各々Ex 及びEy とし、管内波長が異な
るため各々に生ずる波数をβx 及びβy とすると、
位相回路4b の開口部での電界Ex とEy の位相
差は■式から、(βx −βy )Lb となる。 (βx −βy )Lb =π/2・・・・・■位相回
路4b を■式が成り立つように構成すれば、位相回路
4b で90度位相を変えることができる。従って、円
形導波管2の終端面5に一体とし、管軸方向の長さが略
4a +4b の長さになるようにして設けた位相回路
で180度位相を遅延させることが可能となり、同位相
回路の中間から位相を180度遅延させた信号を取り出
すことができる。
FIG. 4 is a diagram illustrating the principle of the circularly polarized wave/linearly polarized wave converter of the present invention, in which a probe 10 is placed inside the circular waveguide 2.
A phase circuit 4b having a length Lb in the tube axis direction and having two orthogonal electromagnetic wave modes with different tube wavelengths is provided. When an electromagnetic wave is excited by the probe 10, and the electric fields of two orthogonal modes of electromagnetic waves propagating in the phase circuit 4b of the same electromagnetic wave are respectively Ex and Ey, and the wave numbers generated in each mode are βx and βy because the tube wavelengths are different, then
The phase difference between the electric fields Ex and Ey at the opening of the phase circuit 4b is (βx −βy)Lb from equation (2). (βx −βy)Lb =π/2... If the phase circuit 4b is configured so that the formula (2) holds, the phase can be changed by 90 degrees with the phase circuit 4b. Therefore, it is possible to delay the phase by 180 degrees with a phase circuit that is integrated with the end face 5 of the circular waveguide 2 and whose length in the tube axis direction is approximately 4a + 4b. A signal whose phase is delayed by 180 degrees can be extracted from the middle of the phase circuit.

【0011】[0011]

【実施例】図6は、本発明の垂直及び水平偏波共用一次
放射器の一実施例を示す一部切欠き斜視図であり、円形
導波管2の一端を垂直及び水平の直線偏波の信号を導入
し得るホーン形の開口1とし、他端を終端面5とし、開
口1側に水平偏波信号の出力手段としてプローブ15を
円形導波管2の外部側面から内部に挿入して、固定具1
4で円形導波管2の側壁に固定するようにし、終端面5
側に垂直偏波信号の出力手段として同様にプローブ17
を円形導波管2の外部側面から内部に挿入して、固定具
16で円形導波管2の側壁に固定するようにしている。 19は切欠き線であり、円形導波管2を破断させた状態
を示しており、円形導波管2の終端面5に金属塊12及
び13からなる位相回路を設けて、プローブ15で水平
偏波信号を取り出してCSコンバータに信号を入力する
ようにし、垂直偏波信号は金属塊12及び13からなる
位相回路で垂直偏波信号の位相を遅延させて、前記プロ
ーブ15と略同一方向にして前記位相回路の中間に設け
たプローブ17で垂直偏波信号を取り出してCSコンバ
ータに信号を入力するようにしている。
[Embodiment] FIG. 6 is a partially cutaway perspective view showing an embodiment of the primary radiator for vertically and horizontally polarized waves of the present invention. A horn-shaped aperture 1 capable of introducing a signal of , fixture 1
4 to be fixed to the side wall of the circular waveguide 2, and the terminal surface 5
Similarly, a probe 17 is provided on the side as a means for outputting a vertically polarized signal.
is inserted into the inside of the circular waveguide 2 from the external side, and is fixed to the side wall of the circular waveguide 2 with a fixture 16. 19 is a notch line, which shows the state in which the circular waveguide 2 is broken, and a phase circuit consisting of metal lumps 12 and 13 is provided on the terminal surface 5 of the circular waveguide 2, and the probe 15 is used to horizontally The polarized signal is extracted and input to the CS converter, and the phase of the vertically polarized signal is delayed by a phase circuit made up of metal blocks 12 and 13, so that the vertically polarized signal is in substantially the same direction as the probe 15. A probe 17 provided in the middle of the phase circuit extracts a vertically polarized signal and inputs the signal to the CS converter.

【0012】3は金属板であり、プローブ15と、金属
塊12及び13からなる位相回路との間に水平偏波信号
の電界と略平行となるようにして取り付け、水平偏波信
号が位相回路に進行しないように水平偏波信号を短絡し
て、水平偏波信号と垂直偏波信号の分離をよくしている
。図7は図6の正面図であり、水平偏波は水平方向に電
界を有する信号として、垂直偏波は垂直方向に電界を有
する信号として円形導波管2に導入され、水平偏波の信
号は同信号の電界方向と平行して設けられたプローブ1
5で信号が取り出される。
Reference numeral 3 denotes a metal plate, which is attached between the probe 15 and the phase circuit consisting of metal blocks 12 and 13 so as to be substantially parallel to the electric field of the horizontally polarized signal, so that the horizontally polarized signal is connected to the phase circuit. The horizontally polarized signal is short-circuited to prevent the horizontally polarized signal from moving forward, thereby improving the separation of the horizontally polarized signal and the vertically polarized signal. FIG. 7 is a front view of FIG. 6, in which the horizontally polarized wave is introduced into the circular waveguide 2 as a signal having an electric field in the horizontal direction, and the vertically polarized wave is introduced into the circular waveguide 2 as a signal having an electric field in the vertical direction. is the probe 1 installed parallel to the electric field direction of the same signal.
5, the signal is taken out.

【0013】さらに、水平偏波の信号は円形導波管2の
直径と同じ幅にして円形導波管2の内部に取り付けられ
た金属板3により反射させて、位相回路に進行しないよ
うにし、位相回路として使用する略カマボコ形の金属塊
12及び13は円形導波管2の内部表面の円弧が平面と
なるようにして、円形導波管2の対向する円弧に取り付
けられて、金属塊12及び13の各々の中心を結んだ中
心線20は金属板3と略45度の角度を成すように配置
している。
Furthermore, the horizontally polarized signal is made to have the same width as the diameter of the circular waveguide 2 and is reflected by a metal plate 3 installed inside the circular waveguide 2 so as not to proceed to the phase circuit. The substantially semicylindrical metal blocks 12 and 13 used as a phase circuit are attached to opposing arcs of the circular waveguide 2 so that the arcs of the inner surface of the circular waveguide 2 are flat. and 13 are arranged so that a center line 20 connecting the centers of each of the metal plates 3 and 13 forms an angle of approximately 45 degrees with the metal plate 3.

【0014】中心線20の方向をX軸とし、中心線20
と直交する方向をY軸とすると、円形導波管2に導入さ
れる垂直偏波の電界Evのベクトルは図5のように表す
ことができる。金属塊12及び13で構成された位相回
路中を垂直偏波の信号が進行すると、金属塊12及び1
3により垂直偏波の電界のベクトル成分Evy よりベ
クトル成分Evx の方が波長が短くなるため、ベクト
ル成分Evx の位相を遅延させることができ、図6に
示すように金属塊12及び13の左端からプローブ17
迄の位相回路でベクトル成分Evx を略90度位相を
遅延させ、プローブ17から終端面5迄の位相回路でベ
クトル成分Evx を略90度位相を遅延させるように
してあり、従ってプローブ17の位置でベクトル成分E
vx を180度位相を遅延させて図5の点線で示すよ
うな電界Ev′とすることができる。従って、電界Ev
′は前記水平偏波の信号と同じ向きの電界方向となって
おり、プローブ15と同様にして設けられたプローブ1
7で垂直偏波の信号を取り出すことができる。
[0014] The direction of the center line 20 is taken as the X axis, and the center line 20
The vector of the vertically polarized electric field Ev introduced into the circular waveguide 2 can be expressed as shown in FIG. When a vertically polarized signal travels through the phase circuit made up of metal blocks 12 and 13, metal blocks 12 and 1
3, the vector component Evx has a shorter wavelength than the vector component Evy of the vertically polarized electric field, so the phase of the vector component Evx can be delayed, and as shown in FIG. probe 17
The phase circuit up to this point delays the phase of the vector component Evx by approximately 90 degrees, and the phase circuit from the probe 17 to the termination surface 5 delays the phase of the vector component Evx by approximately 90 degrees. Vector component E
By delaying the phase of vx by 180 degrees, the electric field Ev' can be obtained as shown by the dotted line in FIG. Therefore, the electric field Ev
' is the electric field direction in the same direction as the horizontally polarized signal, and the probe 1 provided in the same manner as the probe 15
7, a vertically polarized signal can be extracted.

【0015】図8は、本発明の垂直及び水平偏波共用一
次放射器のその他の実施例を示す一部切欠き斜視図で、
図9は図8の正面図であり、前記実施例図6及び図7と
の相違は信号の出力手段としてプローブを使用する代わ
りに円形導波管2の側面に方形導波管を接合したもので
ある。開口1側に水平偏波信号の出力手段としてスリッ
ト6を介して方形導波管7を接合し、金属塊12及び1
3からなる位相回路の略中間にスリット8を介して方形
導波管9を方形導波管7と管軸を略同一方向にして接合
するようにしている。スリットの形状は円形導波管2の
管軸方向と平行になるように長辺を設け、開口面が水平
偏波信号の電界と平行な向きに配置している。スリット
8の管軸方向の取付位置は、スリット8の開口の中心が
図6のプローブ17と同じ位置となるようにして、18
0度位相を遅延させた垂直偏波の信号を取り出せるよう
にし、スリット6の管軸方向の取付位置は、スリット6
の開口の中心が図6のプローブ15と略同位置となるよ
うにすれば良い。なお、図10は図8を破断線n−mで
破断させた縦断面図であり、スリット8の開口上に金属
塊13が重ならないように配置している。
FIG. 8 is a partially cutaway perspective view showing another embodiment of the primary radiator for both vertical and horizontal polarization according to the present invention.
9 is a front view of FIG. 8, and the difference from the embodiments shown in FIGS. 6 and 7 is that instead of using a probe as a signal output means, a rectangular waveguide is joined to the side surface of the circular waveguide 2. It is. A rectangular waveguide 7 is connected to the aperture 1 side via a slit 6 as an output means for a horizontally polarized signal, and metal blocks 12 and 1
A rectangular waveguide 9 is connected to the rectangular waveguide 7 through a slit 8 approximately in the middle of the phase circuit consisting of the rectangular waveguide 7 with its tube axis in approximately the same direction. The shape of the slit is such that the long side is parallel to the tube axis direction of the circular waveguide 2, and the opening surface is arranged in a direction parallel to the electric field of the horizontally polarized signal. The mounting position of the slit 8 in the tube axis direction is such that the center of the opening of the slit 8 is at the same position as the probe 17 in FIG.
A vertically polarized signal with a 0 degree phase delay can be extracted, and the mounting position of the slit 6 in the tube axis direction is
The center of the opening may be located approximately at the same position as the probe 15 in FIG. Note that FIG. 10 is a longitudinal cross-sectional view of FIG. 8 taken along the breaking line nm, and the metal lump 13 is arranged so as not to overlap the opening of the slit 8.

【0016】図11は、本発明の垂直及び水平偏波共用
一次放射器のその他の実施例を示す一部切欠き斜視図で
、図12は図11の正面図であり、前記実施例図8及び
図9との相違は位相回路として金属塊12及び13を使
用する代わりに誘電体板18を使用するようにしたもの
である。誘電体板18の板厚の中心線23と図9におけ
る金属塊12及び13の中心線20とが合致するように
誘電体板18を配置しており、誘電体板18の短辺方向
の両端は円形導波管2の内壁で挟持されて固定されるよ
うにしている。誘電体板18の長辺方向の長さは、垂直
偏波の信号の位相を180度位相を遅延させることがで
きる長さとしている。その他の構成は前記実施例図8及
び図9の場合と同様である。
FIG. 11 is a partially cutaway perspective view showing another embodiment of the vertically and horizontally polarized primary radiator of the present invention, and FIG. 12 is a front view of FIG. 11, and FIG. The difference from FIG. 9 is that a dielectric plate 18 is used as a phase circuit instead of metal blocks 12 and 13. The dielectric plate 18 is arranged so that the center line 23 of the plate thickness of the dielectric plate 18 matches the center line 20 of the metal lumps 12 and 13 in FIG. 9, and both ends of the dielectric plate 18 in the short side direction are clamped and fixed between the inner walls of the circular waveguide 2. The length of the dielectric plate 18 in the long side direction is such that the phase of the vertically polarized signal can be delayed by 180 degrees. The other configurations are the same as those in the embodiments shown in FIGS. 8 and 9.

【0017】[0017]

【発明の効果】以上説明したように、本発明によれば垂
直及び水平偏波の信号電界を同一方向にすることができ
、二つの方形導波管を使用して出力を取り出す場合でも
管軸方向を略同一方向にして円形導波管に接合すること
ができ、取り扱いやすく、また、外観上も見映えの良い
垂直及び水平偏波共用一次放射器を提供することができ
る。
As explained above, according to the present invention, it is possible to make the signal electric fields of vertically and horizontally polarized waves in the same direction, and even when output is extracted using two rectangular waveguides, the tube axis remains unchanged. It is possible to provide a primary radiator for vertically and horizontally polarized waves that can be joined to a circular waveguide with substantially the same direction, is easy to handle, and has a good appearance.

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

【図1】本発明の垂直及び水平偏波共用一次放射器の基
本構成図である。
FIG. 1 is a basic configuration diagram of a primary radiator for both vertical and horizontal polarization according to the present invention.

【図2】本発明の垂直及び水平偏波共用一次放射器の原
理説明図である。
FIG. 2 is a diagram illustrating the principle of a primary radiator for both vertical and horizontal polarization according to the present invention.

【図3】本発明の垂直及び水平偏波共用一次放射器の原
理説明用の等価構成図である。
FIG. 3 is an equivalent configuration diagram for explaining the principle of a primary radiator for both vertical and horizontal polarization according to the present invention.

【図4】本発明の垂直及び水平偏波共用一次放射器に用
いる位相回路の説明図である。
FIG. 4 is an explanatory diagram of a phase circuit used in the vertically and horizontally polarized primary radiator of the present invention.

【図5】水平偏波、及び垂直偏波の電界のベクトル図で
ある。
FIG. 5 is a vector diagram of electric fields of horizontally polarized waves and vertically polarized waves.

【図6】本発明の垂直及び水平偏波共用一次放射器の一
実施例を示す一部切欠き斜視図である。
FIG. 6 is a partially cutaway perspective view showing an embodiment of a primary radiator for both vertical and horizontal polarization according to the present invention.

【図7】図6の正面図である。FIG. 7 is a front view of FIG. 6;

【図8】本発明の垂直及び水平偏波共用一次放射器のそ
の他の実施例を示す一部切欠き斜視図である。
FIG. 8 is a partially cutaway perspective view showing another embodiment of the primary radiator for both vertical and horizontal polarization according to the present invention.

【図9】図8の正面図である。FIG. 9 is a front view of FIG. 8;

【図10】図8を破断線n−mで破断させた縦断面図で
ある。
10 is a vertical cross-sectional view taken along the breaking line nm in FIG. 8; FIG.

【図11】本発明の垂直及び水平偏波共用一次放射器の
その他の実施例を示す一部切欠き斜視図である。
FIG. 11 is a partially cutaway perspective view showing another embodiment of the primary radiator for both vertical and horizontal polarization according to the present invention.

【図12】図10の正面図である。FIG. 12 is a front view of FIG. 10;

【図13】従来例の垂直及び水平偏波共用一次放射器を
示す斜視図である。
FIG. 13 is a perspective view showing a conventional primary radiator for both vertical and horizontal polarization.

【符号の説明】[Explanation of symbols]

1  開口 2  円形導波管 3  金属板 4  位相回路 4a  位相回路 4b  位相回路 5  終端面 6  スリット 7  方形導波管 8  スリット 9  方形導波管 10  プローブ 11  プローブ 12  金属塊 13  金属塊 14  固定具 15  プローブ 16  固定具 17  プローブ 18  誘電体板 19  切欠き線 20  中心線 21  X軸 22  Y軸 23  中心線 24  方形導波管 25  方形導波管 1 Opening 2 Circular waveguide 3 Metal plate 4 Phase circuit 4a Phase circuit 4b Phase circuit 5 End surface 6 Slit 7 Square waveguide 8 Slit 9 Square waveguide 10 Probe 11 Probe 12 Metal lump 13 Metal lump 14 Fixing tool 15 Probe 16 Fixing tool 17 Probe 18 Dielectric plate 19 Notch line 20 Center line 21 X-axis 22 Y-axis 23 Center line 24 Square waveguide 25 Square waveguide

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】  一端を垂直及び水平の直線偏波の信号
を導入し得る開口とし、他端を終端面とし、開口側に一
方の直線偏波信号の第1出力手段として第1方形導波管
を接合し、終端面側に位相回路を設けて同位相回路の中
間に他方の直線偏波信号の第2出力手段として第2方形
導波管を接合した円形導波管において、前記位相回路で
他方の直線偏波信号の位相を遅延させることにより、前
記第1方形導波管と第2方形導波管の管軸方向を略同一
方向に接合せしめるようにしたことを特徴とする垂直及
び水平偏波共用一次放射器。
Claim 1: One end is an aperture capable of introducing vertical and horizontal linearly polarized signals, the other end is an end surface, and a first rectangular waveguide is provided on the aperture side as a first output means for one of the linearly polarized signals. In a circular waveguide in which the tubes are joined together, a phase circuit is provided on the end face side, and a second rectangular waveguide is joined in the middle of the same phase circuit as a second output means for the other linearly polarized signal, the phase circuit By delaying the phase of the other linearly polarized wave signal, the first rectangular waveguide and the second rectangular waveguide are joined in substantially the same direction with their tube axes. Horizontal polarization shared primary radiator.
【請求項2】  一端を垂直及び水平の直線偏波の信号
を導入し得る開口とし、他端を終端面とし、開口側に一
方の直線偏波信号の第1出力手段として第1プローブを
設け、終端面側に位相回路を設けて同位相回路の中間に
他方の直線偏波信号の第2出力手段として第2プローブ
を設けた円形導波管において、前記位相回路で他方の直
線偏波信号の位相を遅延させることにより、前記第1プ
ローブと第2プローブを略同一方向にして相互に異なる
直線偏波信号と結合せしめるようにしたことを特徴とす
る垂直及び水平偏波共用一次放射器。
2. One end is an opening capable of introducing vertical and horizontal linearly polarized signals, the other end is a termination surface, and a first probe is provided on the opening side as a first output means for one of the linearly polarized signals. , in a circular waveguide in which a phase circuit is provided on the termination surface side and a second probe is provided in the middle of the same phase circuit as a second output means for the other linearly polarized signal, the phase circuit outputs the other linearly polarized signal. 1. A primary radiator for both vertical and horizontal polarization, characterized in that the first probe and the second probe are made to be in substantially the same direction and coupled with mutually different linearly polarized signals by delaying the phase of the probe.
【請求項3】  前記第1出力手段と前記位相回路間に
同第1出力手段で出力せしめる直線偏波信号の電界と略
平行となるようにして、短絡用の金属板を前記円形導波
管の内部に取り付けたことを特徴とする請求項1又は2
記載の垂直及び水平偏波共用一次放射器。
3. A short-circuiting metal plate is connected to the circular waveguide between the first output means and the phase circuit so that the electric field is substantially parallel to the electric field of the linearly polarized signal outputted by the first output means. Claim 1 or 2 characterized in that it is attached inside the
The vertically and horizontally polarized primary radiator described.
JP4922391A 1991-02-21 1991-02-21 Primary radiator in common use for vertically and horizontally polarized wave Pending JPH04267606A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4922391A JPH04267606A (en) 1991-02-21 1991-02-21 Primary radiator in common use for vertically and horizontally polarized wave

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4922391A JPH04267606A (en) 1991-02-21 1991-02-21 Primary radiator in common use for vertically and horizontally polarized wave

Publications (1)

Publication Number Publication Date
JPH04267606A true JPH04267606A (en) 1992-09-24

Family

ID=12824936

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4922391A Pending JPH04267606A (en) 1991-02-21 1991-02-21 Primary radiator in common use for vertically and horizontally polarized wave

Country Status (1)

Country Link
JP (1) JPH04267606A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54114155A (en) * 1978-02-27 1979-09-06 Nec Corp Polarizer device
JPH0229001A (en) * 1988-07-18 1990-01-31 Nec Corp Polarization coupler

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS54114155A (en) * 1978-02-27 1979-09-06 Nec Corp Polarizer device
JPH0229001A (en) * 1988-07-18 1990-01-31 Nec Corp Polarization coupler

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