JPH05299928A - Primary radiator in common use for circularly polarized wave and linearly polarized wave - Google Patents

Primary radiator in common use for circularly polarized wave and linearly polarized wave

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Publication number
JPH05299928A
JPH05299928A JP10102792A JP10102792A JPH05299928A JP H05299928 A JPH05299928 A JP H05299928A JP 10102792 A JP10102792 A JP 10102792A JP 10102792 A JP10102792 A JP 10102792A JP H05299928 A JPH05299928 A JP H05299928A
Authority
JP
Japan
Prior art keywords
circular waveguide
polarized wave
primary radiator
ferrite rod
polarization
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
JP10102792A
Other languages
Japanese (ja)
Inventor
Akio Seki
昭男 関
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 JP10102792A priority Critical patent/JPH05299928A/en
Publication of JPH05299928A publication Critical patent/JPH05299928A/en
Pending legal-status Critical Current

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  • Waveguide Aerials (AREA)

Abstract

PURPOSE:To receive a polarized wave without deterioration in the reception sensitivity even when a deviation takes place between horizontal and vertical directions being reference directions of the primary radiator and a polarized wave front of a horizontally or vertically polarized wave made incident in the primary radiator. CONSTITUTION:The primary radiator consists of a circular waveguide 2 having an aperture 1 introducing an electromagnetic wave at one end and having a termination face 3 at other end, a ferrite rod 4 with a 1st exciting coil 5 wound around whose lengthwise direction is formed in parallel with a guide axis toward the aperture 1 of the circular waveguide 2 and arranged in the center of the circular waveguide 2, four sets of 2nd-5th exciting coils (6, 7 and others are not shown) provided to an outer circumference of the circular waveguide 2 with the ferrite rod 4 located thereto at an equal interval vertically, and a probe 8 inserted in the inside of the circular waveguide 2 from the side face of the circular waveguide 2 between the ferrite rod 4 and the termination face 3 at an angle bisecting the angle formed by the adjacent exciting coils among the four exciting coils.

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、円偏波を使用している
衛星放送(BS)と、直線偏波(水平偏波及び垂直偏
波)を使用している通信衛星(CS)とを、共に受信可
能とした円偏波及び直線偏波共用一次放射器に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention provides a satellite broadcasting (BS) using circular polarization and a communication satellite (CS) using linear polarization (horizontal polarization and vertical polarization). , And a primary radiator for both circularly polarized waves and linearly polarized waves that can be received together.

【0002】[0002]

【従来の技術】従来の円偏波及び直線偏波共用一次放射
器は、図3に示すように、円形導波管22の開口部21
側に、90度位相差板23を長手方向が管軸と平行とな
るようにして配置し、フェライトポラライザー24を円
形導波管22の終端面27側に配置し、円形導波管22
の開口部21側からみた90度位相差板23の取付角度
が、円形導波管22に導入される水平偏波、あるいは垂
直偏波の電界と平行となる向きにし、フェライトポララ
イザー24と終端面27の間の円形導波管22の側面に
信号出力用のプローブ26を設けて円形導波管22の内
部に挿入し、水平偏波、あるいは垂直偏波を受信する場
合、フェライトポラライザー24に電流を流すことによ
り水平偏波、あるいは垂直偏波の電界の向きを相対的に
回転させて、受信希望の偏波をプローブ26に結合させ
て電気信号に変換し、円偏波を受信する場合、90度位
相差板23をY軸と平行な向きとし、左旋円偏波を90
度位相差板23で直線偏波に変換し、フェライトポララ
イザー24に電流を流すことにより同直線偏波の電界の
向きを回転させて、プローブ26に結合させて電気信号
に変換し、同電気信号を取り出して円偏波及び直線偏波
が受信できるようにしていた。右旋円偏波を受ける場合
は、90度位相差板23の向きを変えて、X軸と平行な
向きとする必要があり、従って、一台の一次放射器で左
旋円偏波及び右旋円偏波用に共用して使用することはで
きなかった。
2. Description of the Related Art A conventional primary radiator for both circularly polarized waves and linearly polarized waves has an opening 21 of a circular waveguide 22 as shown in FIG.
On the side, the 90-degree phase difference plate 23 is arranged so that the longitudinal direction is parallel to the tube axis, and the ferrite polarizer 24 is arranged on the end face 27 side of the circular waveguide 22.
The angle of attachment of the 90-degree phase difference plate 23 as viewed from the side of the opening 21 is set to be parallel to the electric field of the horizontal polarization or the vertical polarization introduced into the circular waveguide 22, and the ferrite polarizer 24 and the termination surface. When a probe 26 for signal output is provided on the side surface of the circular waveguide 22 between the two and is inserted into the circular waveguide 22 to receive horizontal polarization or vertical polarization, a current is passed through the ferrite polarizer 24. When the circularly polarized wave is received by rotating the electric field direction of the horizontal polarized wave or the vertical polarized wave by rotating the electric field, coupling the polarized wave desired to be received with the probe 26 and converting it into an electric signal. The 90-degree phase plate 23 is oriented parallel to the Y-axis, and the left-hand circularly polarized wave is
Degree phase difference plate 23 converts the linearly polarized wave, and the electric current is passed through the ferrite polarizer 24 to rotate the direction of the electric field of the linearly polarized wave, which is coupled to the probe 26 and converted into an electric signal. Was taken out so that circular polarization and linear polarization could be received. When receiving a right-handed circularly polarized wave, it is necessary to change the direction of the 90-degree phase difference plate 23 so that it is parallel to the X-axis. Therefore, a single primary radiator makes a left-handed circularly polarized wave and a right-handed circularly polarized wave. It could not be used commonly for circular polarization.

【0003】円形導波管22の開口部21側からみた9
0度位相差板23の取付角度が、水平偏波、あるいは垂
直偏波の偏波面に対してずれた場合、水平偏波及び垂直
偏波は90度位相差板23に対して、各々垂直方向成分
と水平方向成分とを有する伝播状態となるため、垂直方
向成分と水平方向成分間に位相差が発生し、水平偏波、
あるいは垂直偏波は、90度位相差板23を通り抜けた
ところでは楕円偏波となり、受信感度が低下するといっ
た問題があった。通信衛星は打ち上げられている位置が
各々異なり、地上に到達する水平偏波、あるいは垂直偏
波の偏波面は、各衛星毎に水平方向、あるいは垂直方向
から若干のずれが発生し、さらに、一台のアンテナで複
数の衛星の直線偏波を受信する場合は、アクチュエータ
でアンテナを各々の衛星の方向に向けるため、アンテナ
に取り付けられている一次放射器の基準となる水平方向
及び垂直方向も傾きが生ずるため、一次放射器に入射さ
れる水平偏波、あるいは垂直偏波の偏波面との間にずれ
が発生し、受信感度を低下させるといった問題点があっ
た。
9 viewed from the side of the opening 21 of the circular waveguide 22
When the mounting angle of the 0-degree phase difference plate 23 is deviated from the plane of polarization of the horizontal polarization or the vertical polarization, the horizontal polarization and the vertical polarization are respectively perpendicular to the 90-degree phase difference plate 23. Since there is a propagation state having a component and a horizontal component, a phase difference occurs between the vertical component and the horizontal component, and horizontal polarization,
Alternatively, the vertically polarized wave becomes an elliptically polarized wave when passing through the 90-degree phase difference plate 23, and there is a problem that the reception sensitivity is reduced. Communication satellites are launched at different positions, and the polarization plane of horizontal polarization or vertical polarization that reaches the ground is slightly deviated from the horizontal or vertical direction for each satellite. When receiving linearly polarized waves of multiple satellites with a single antenna, the actuators direct the antennas toward the respective satellites, so the horizontal and vertical directions that are the reference of the primary radiator attached to the antenna are also tilted. Therefore, there is a problem in that a deviation occurs between the polarization plane of the horizontally polarized wave or the vertically polarized wave that is incident on the primary radiator, which lowers the reception sensitivity.

【0004】[0004]

【発明が解決しようとする課題】本発明は、90度位相
差板23を削除してフェライト棒を使用することによ
り、任意の角度で一次放射器に水平偏波、あるいは垂直
偏波が入射された場合でも、受信感度を低下させること
なく、受信できるようにし、また、円偏波(左旋及び右
旋円偏波)が入射された場合でも直線偏波に変換して受
信可能とした円偏波及び直線偏波共用一次放射器を提供
することを目的とする。
According to the present invention, by removing the 90-degree phase difference plate 23 and using a ferrite rod, horizontal polarization or vertical polarization is incident on the primary radiator at an arbitrary angle. In this case, the reception can be performed without lowering the reception sensitivity, and even if circularly polarized waves (left-handed and right-handed circularly polarized waves) are incident, they can be converted to linearly polarized waves and received. An object is to provide a primary radiator for both wave and linear polarization.

【0005】[0005]

【課題を解決するための手段】図1は、本発明の一実施
例を示す、円偏波及び直線偏波共用一次放射器の一部切
欠き斜視図であり、同図に示すように、一端に電磁波を
導入する開口部1を設け、他端に終端面3を設けた円形
導波管2と、同円形導波管2の開口部1側に長手方向が
管軸と平行となるようにして同円形導波管2の中心部に
配置した、周囲に第1励磁コイル5を巻き付けたフェラ
イト棒4と、同フェライト棒4が位置する前記円形導波
管2の外部円周部に垂直に等間隔にして設けた4個の第
2〜第5励磁コイル(6及び7、その他は図示せず)
と、前記円形導波管の開口部からみた取付角度が、前記
4個の励磁コイルの内、隣接した励磁コイル間が成す角
度を2分する角度で、前記フェライト棒4と前記終端面
3間の前記円形導波管2の側面より内部に挿入したプロ
ーブ8とで構成したものである。
FIG. 1 is a partially cutaway perspective view of a primary radiator for circular polarization and linear polarization, showing an embodiment of the present invention. As shown in FIG. A circular waveguide 2 having an opening 1 for introducing an electromagnetic wave at one end and a terminating surface 3 at the other end, and the longitudinal direction on the side of the opening 1 of the circular waveguide 2 is parallel to the tube axis. The ferrite rod 4 having the first exciting coil 5 wound around it and arranged at the center of the circular waveguide 2 is perpendicular to the outer circumferential portion of the circular waveguide 2 where the ferrite rod 4 is located. Four second to fifth exciting coils (6 and 7, other not shown) provided at even intervals
And the mounting angle viewed from the opening of the circular waveguide is an angle that bisects the angle formed by the adjacent exciting coils among the four exciting coils, and between the ferrite rod 4 and the terminal surface 3. The probe 8 inserted inside the circular waveguide 2 from the side.

【0006】[0006]

【作用】励磁コイル5に直流電流を流すことにより、フ
ェライト棒4に軸方向に沿った直流磁界を加えて、円形
導波管2に導入された水平偏波及び垂直偏波の偏波面を
相対的に回転させて、受信希望の方を選択してプローブ
8に結合させて電気信号に変換し、フェライト棒4が位
置する円形導波管2の外部円周部に垂直に等間隔にして
設けた4個の励磁コイル(6及び7、その他は図示せ
ず)の内、対向する2個、例えば、励磁コイル6及び7
に直流電流を流すことにより、フェライト棒4にY軸方
向の直流磁界を加えて、円形導波管2に導入された円偏
波を直線偏波に変換し、前記円偏波と逆旋の円偏波を受
信する場合は、励磁コイル6及び7以外の対向する励磁
コイル(図示せず)に直流電流を流すことにより、フェ
ライト棒4にX軸方向の直流磁界を加えて、円形導波管
2に導入された円偏波を直線偏波に変換し、同直線偏波
をプローブに結合させて電気信号に変換し、同プローブ
を介して信号を取り出せるようにしており、任意の角度
で一次放射器に入射された水平偏波、及び垂直偏波を受
信感度を低下させることなく、受信できるようにし、ま
た、円偏波(左旋及び右旋円偏波)が入射された場合で
も直線偏波に変換して受信できるようにしている。
By applying a DC current to the exciting coil 5, a DC magnetic field along the axial direction is applied to the ferrite rod 4 so that the polarization planes of the horizontal polarization and the vertical polarization introduced into the circular waveguide 2 are made relative to each other. The desired signal to be received and coupled to the probe 8 to convert it into an electric signal, which is provided at equal intervals vertically on the outer circumference of the circular waveguide 2 where the ferrite rods 4 are located. Of the four exciting coils (6 and 7, others not shown), two facing each other, for example, exciting coils 6 and 7
By applying a DC current to the ferrite rod 4, a DC magnetic field in the Y-axis direction is applied to convert the circularly polarized wave introduced into the circular waveguide 2 into a linearly polarized wave. When circularly polarized waves are received, a DC magnetic field in the X-axis direction is applied to the ferrite rod 4 by applying a DC current to the opposing exciting coils (not shown) other than the exciting coils 6 and 7, and the circular waveguide The circularly polarized wave introduced into the tube 2 is converted into a linearly polarized wave, the linearly polarized wave is coupled with a probe to be converted into an electric signal, and the signal can be taken out through the probe, at an arbitrary angle. It enables horizontal polarization and vertical polarization incident on the primary radiator to be received without deteriorating the receiving sensitivity, and linear even when circular polarization (left-handed and right-handed circularly polarized) is incident. It is converted to polarized waves so that it can be received.

【0007】[0007]

【実施例】図1は、本発明の一実施例を示す、円偏波及
び直線偏波共用一次放射器の一部切欠き斜視図であり、
同図において、円形導波管の管軸から上部方向に向かう
軸をY軸とし、左方向に向かう軸をX軸とし、各々反対
方向に向かう軸を−Y軸と−X軸(図示せず)とする
(以下、図2及び図3において同じ)。円形導波管2の
一端を電磁波を効率的に導入できるようにホーン形状の
開口部1とし、他端に導入された電磁波を反射させる終
端面3を設けている。4はフェライト棒であり、円形導
波管2の開口部1側にフェライト棒4の長手方向が管軸
と平行となるようにして同円形導波管2の中心部に配置
し、フェライト棒4の周囲に励磁コイル5を巻き付け、
円形導波管2の内壁で励磁コイル5を挟持せしめてフェ
ライト棒4を円形導波管2の内部の所定の位置に保持す
るようにしている。フェライト棒4を金属管(図示せ
ず)の中に入れ、同金属管の周囲に励磁コイル5を巻付
け、同金属管の両端に円形導波管2との整合用のセラミ
ック片(図示せず)を取り付けた構造としても良い。
DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a partially cutaway perspective view of a primary radiator for both circular polarization and linear polarization, showing an embodiment of the present invention.
In the figure, an axis extending upward from the tube axis of the circular waveguide is defined as a Y-axis, an axis extending leftward is defined as an X-axis, and opposite axes are defined as -Y-axis and -X-axis (not shown). ) (Hereinafter the same in FIGS. 2 and 3). One end of the circular waveguide 2 is formed as a horn-shaped opening 1 so that an electromagnetic wave can be efficiently introduced, and a terminal surface 3 for reflecting the introduced electromagnetic wave is provided at the other end. Reference numeral 4 denotes a ferrite rod, which is arranged at the center of the circular waveguide 2 so that the longitudinal direction of the ferrite rod 4 is parallel to the tube axis on the side of the opening 1 of the circular waveguide 2. Wrap the excitation coil 5 around the
The exciting coil 5 is sandwiched between the inner walls of the circular waveguide 2 so that the ferrite rod 4 is held at a predetermined position inside the circular waveguide 2. The ferrite rod 4 is put in a metal tube (not shown), an exciting coil 5 is wound around the metal tube, and ceramic pieces (not shown) for matching with the circular waveguide 2 are provided at both ends of the metal tube. No) may be attached.

【0008】円形導波管2内に設けられた励磁コイル5
の引き出し線9は、円形導波管2の側面に設けられた開
口(図示せず)を通して、円形導波管2の外部に引き出
して直流電源と接続して、励磁コイル5に直流電流を流
して、所定の直流磁界をフェライト棒4の長手方向に加
えることができるようにしている。8はプローブであ
り、フェライト棒4と終端面3間の円形導波管2の側面
より、円形導波管2の内部に挿入している。円形導波管
2内に導入されたCSの水平偏波及び垂直偏波の電界分
布は、互いに直交したTE11モードの直線偏波であ
り、CSを受信するときには、導入された水平偏波ある
いは垂直偏波に対して希望する方を選択し、励磁コイル
5に流れる電流を制御することにより、フェライト棒4
で相対的に導入された水平偏波、あるいは垂直偏波の電
界の位相角を回転させて、プローブ8に希望する偏波を
結合させて、最大の信号が取り出せるようにする。従っ
て、従来例と異なり位相差板を使用していないため、任
意の角度で一次放射器に水平偏波あるいは垂直偏波が入
射された場合でも、励磁コイル5に流す電流を制御する
ことにより、フェライト棒4で入射された電磁波の電界
の位相角を制御することができるため、プローブ8から
希望する偏波の信号を取り出すことができる。
Exciting coil 5 provided in the circular waveguide 2
Through the opening (not shown) provided on the side surface of the circular waveguide 2, and is connected to the DC power source by connecting to the DC power source so that a DC current flows through the exciting coil 5. Thus, a predetermined DC magnetic field can be applied in the longitudinal direction of the ferrite rod 4. Reference numeral 8 denotes a probe, which is inserted into the circular waveguide 2 from the side surface of the circular waveguide 2 between the ferrite rod 4 and the termination surface 3. The electric field distributions of the horizontal polarization and the vertical polarization of CS introduced in the circular waveguide 2 are linear polarizations of TE11 mode orthogonal to each other, and when the CS is received, the horizontal polarization or the vertical polarization introduced. By selecting the desired one for the polarized wave and controlling the current flowing through the exciting coil 5, the ferrite rod 4
By rotating the phase angle of the electric field of the horizontally polarized wave or the vertically polarized wave which is relatively introduced by (1), the desired polarized wave is coupled to the probe 8 so that the maximum signal can be extracted. Therefore, unlike the conventional example, since the phase difference plate is not used, even if the horizontally polarized wave or the vertically polarized wave is incident on the primary radiator at an arbitrary angle, by controlling the current flowing through the exciting coil 5, Since the phase angle of the electric field of the electromagnetic wave incident on the ferrite rod 4 can be controlled, a desired polarized wave signal can be extracted from the probe 8.

【0009】図2は、図1の円偏波及び直線偏波共用一
次放射器の正面図である。フェライト棒4が位置する円
形導波管2の外部円周部に、垂直に等間隔にして4個の
励磁コイル(6、7、11及び12)を設けている。励
磁コイル(6、7、11及び12)は各々鉄心等(図示
せず)を使用して、同鉄心の周囲に励磁コイル(6、
7、11及び12)を各々巻き付けた構造としており、
円形導波管2の外部円周部の対向した位置に取り付けら
れている励磁コイル6及び7は、フェライト棒4に対し
てY軸方向の直流磁界が加えられるようにしており、同
様に、励磁コイル11及び12は、フェライト棒4に対
してX軸方向の直流磁界が加えられるようにしている。
プローブ8は、隣接した励磁コイル7と11が成す角度
を2分する角度で、フェライト棒4と終端面3間の前記
円形導波管2の側面より、円形導波管2の内部に挿入し
ている。
FIG. 2 is a front view of the circular polarization and linear polarization primary radiator of FIG. Four exciting coils (6, 7, 11, and 12) are provided vertically equidistantly on the outer circumferential portion of the circular waveguide 2 where the ferrite rods 4 are located. Each of the exciting coils (6, 7, 11 and 12) uses an iron core or the like (not shown), and the exciting coil (6, 6,
7, 11 and 12) are respectively wound,
The exciting coils 6 and 7 attached to the outer circumferential portion of the circular waveguide 2 facing each other are arranged so that a direct-current magnetic field in the Y-axis direction is applied to the ferrite rod 4, and the exciting coils 6 and 7 are similarly excited. The coils 11 and 12 are adapted to apply a DC magnetic field in the X-axis direction to the ferrite rod 4.
The probe 8 is inserted into the circular waveguide 2 from the side surface of the circular waveguide 2 between the ferrite rod 4 and the termination surface 3 at an angle that bisects the angle formed by the adjacent excitation coils 7 and 11. ing.

【0010】円偏波は、2つの直交する直線偏波の振幅
が等しく位相が90度ずれている状態であり、BSの円
偏波の電界が−X軸と−Y軸を2分する角度で円形導波
管2内に導入されたとする。円偏波が左旋円偏波である
場合は、−X軸方向の直線偏波に対して、−Y軸方向の
直線偏波が90度位相が進んでいる状態であり、励磁コ
イル6及び7に電流を流してフェライト棒4にY軸方向
の磁界をかけることにより、−X軸方向の直線偏波に対
して、−Y軸方向の直線偏波の位相速度を遅らすことが
でき、フェライト棒4を通り過ぎたところで−X軸方向
の直線偏波と−Y軸方向の直線偏波との位相が合致する
ように、励磁コイル6及び7に流す電流を制御すれば、
−X軸と−Y軸を2分する向きに電界を有する直線偏波
に変換することができるため、プローブ8に同直線偏波
を結合させて、プローブ8を介して左旋円偏波の信号を
取り出すことができる。10は直流電源の入力端子であ
り、励磁コイル6の一端は入力端子10の一端に接続
し、励磁コイル6の他端は励磁コイル7の一端に接続
し、励磁コイル7の他端は入力端子10の他端に接続し
てあり、入力端子10の両端に直流電源を接続して、励
磁コイル6及び7に直流電流を流して、所定の直流磁界
をフェライト棒4に加えることができるようにしてい
る。
The circularly polarized wave is a state in which the amplitudes of two orthogonal linearly polarized waves are equal and their phases are deviated from each other by 90 degrees, and the electric field of the circularly polarized wave of BS bisects the -X axis and the -Y axis. Is introduced into the circular waveguide 2. When the circularly polarized wave is the left-handed circularly polarized wave, the linearly polarized wave in the −Y-axis direction is 90 degrees in phase ahead of the linearly polarized wave in the −X-axis direction, and the excitation coils 6 and 7 are provided. By applying a current to the ferrite rod 4 to apply a magnetic field in the Y-axis direction, the phase velocity of the linearly polarized wave in the -Y-axis direction can be delayed with respect to the linearly polarized wave in the -X-axis direction. If the currents flowing through the exciting coils 6 and 7 are controlled so that the phases of the linearly polarized wave in the -X axis direction and the linearly polarized wave in the -Y axis direction are matched when passing through 4,
Since it can be converted into a linearly polarized wave having an electric field in a direction that bisects the −X axis and the −Y axis, the same linearly polarized wave is coupled to the probe 8 and a signal of a left-handed circularly polarized wave is passed through the probe 8. Can be taken out. Reference numeral 10 is an input terminal of the DC power supply, one end of the exciting coil 6 is connected to one end of the input terminal 10, the other end of the exciting coil 6 is connected to one end of the exciting coil 7, and the other end of the exciting coil 7 is an input terminal. 10 is connected to the other end of the input terminal 10, and a DC power source is connected to both ends of the input terminal 10 so that a DC current can flow through the exciting coils 6 and 7 so that a predetermined DC magnetic field can be applied to the ferrite rod 4. ing.

【0011】円偏波が右旋円偏波である場合は、−Y軸
方向の直線偏波に対して、−X軸方向の直線偏波が90
度位相が進んでいる状態であり、励磁コイル11及び1
2に電流を流してフェライト棒4にX軸方向の磁界をか
けることにより、−Y軸方向の直線偏波に対して、−X
軸方向の直線偏波の位相速度を遅らすことができ、フェ
ライト棒4を通り過ぎたところで−X軸方向の直線偏波
と−Y軸方向の直線偏波との位相が合致するように、励
磁コイル11及び12に流す電流を制御すれば、−X軸
と−Y軸を2分する向きに電界を有する直線偏波に変換
することができるため、プローブ8に同直線偏波を結合
させて、プローブ8を介して右旋円偏波の信号を取り出
すことができる。13は直流電源の入力端子であり、励
磁コイル11の一端は入力端子13の一端に接続し、励
磁コイル11の他端は励磁コイル12の一端に接続し、
励磁コイル12の他端は入力端子13の他端に接続して
あり、入力端子13の両端に直流電源を接続して、励磁
コイル11及び12に直流電流を流して、所定の直流磁
界をフェライト棒4に加えることができるようにしてい
る。従って、従来例と異なり、左旋及び右旋円偏波を同
一の一次放射器で受信することができる。円偏波の内、
左旋円偏波のみを受ける場合は、励磁コイル11及び1
2は省略しても良く、また、右旋円偏波のみを受ける場
合は、励磁コイル6及び7は省略しても良い。
When the circularly polarized wave is a right-handed circularly polarized wave, the linearly polarized wave in the -Y-axis direction is 90 times that in the -Y-axis direction.
Excitation coils 11 and 1
By applying a current to the ferrite rod 4 and applying a magnetic field in the X-axis direction to the ferrite rod 4, the linear polarization in the -Y-axis direction becomes -X.
The phase velocity of the linearly polarized wave in the axial direction can be delayed, and when passing through the ferrite rod 4, the exciting coil is set so that the phase of the linearly polarized wave in the −X axis direction and the linearly polarized wave in the −Y axis direction match. By controlling the currents flowing through 11 and 12, it is possible to convert into a linearly polarized wave having an electric field in a direction that bisects the -X axis and the -Y axis. Therefore, by coupling the linearly polarized wave to the probe 8, A right-handed circularly polarized signal can be taken out via the probe 8. Reference numeral 13 is an input terminal of the DC power supply, one end of the exciting coil 11 is connected to one end of the input terminal 13, and the other end of the exciting coil 11 is connected to one end of the exciting coil 12.
The other end of the exciting coil 12 is connected to the other end of the input terminal 13, a DC power source is connected to both ends of the input terminal 13, and a DC current is caused to flow through the exciting coils 11 and 12 to generate a predetermined DC magnetic field. It is possible to add it to the rod 4. Therefore, unlike the conventional example, left-handed and right-handed circularly polarized waves can be received by the same primary radiator. Of the circular polarization,
When receiving only left-handed circularly polarized waves, exciting coils 11 and 1
2 may be omitted, or the excitation coils 6 and 7 may be omitted when only right-handed circularly polarized waves are received.

【0012】[0012]

【発明の効果】以上説明したように、本発明によれば、
フェライト棒に軸方向に沿って直流磁界を加えることに
より、水平偏波及び垂直偏波の偏波面を相対的に回転さ
せて、受信希望の方を選択してプローブに結合させて電
気信号に変換し、フェライト棒に直径方向の直流磁界を
加えることにより、円偏波を直線偏波に変換し、同直線
偏波をプローブに結合させて電気信号に変換し、同プロ
ーブを介して信号を取り出せるようにしており、従来例
と異なり、90度位相差板を使用していないため、一次
放射器の基準となる水平方向及び垂直方向といった方向
性を無くすことができ、一次放射器に任意の角度で水平
偏波、あるいは垂直偏波が入射された場合でも、感度を
低下させることなく受信可能とした、円偏波及び直線偏
波共用一次放射器を提供することができる。
As described above, according to the present invention,
By applying a DC magnetic field to the ferrite rod along the axial direction, the polarization planes of horizontal polarization and vertical polarization are relatively rotated, and the desired reception is selected and coupled to the probe to convert it to an electrical signal. Then, by applying a DC magnetic field in the diameter direction to the ferrite rod, the circularly polarized wave is converted into a linearly polarized wave, the linearly polarized wave is coupled to the probe, converted into an electric signal, and the signal can be taken out through the probe. Unlike the conventional example, since the 90-degree phase difference plate is not used, it is possible to eliminate the directivity such as the horizontal direction and the vertical direction, which are the reference of the primary radiator, and the primary radiator can have an arbitrary angle. It is possible to provide a primary radiator for both circularly polarized waves and linearly polarized waves that can be received without lowering the sensitivity even when horizontally polarized wave or vertically polarized wave is incident.

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

【図1】本発明の一実施例を示す、円偏波及び直線偏波
共用一次放射器の一部切欠き斜視図である。
FIG. 1 is a partially cutaway perspective view of a primary radiator for both circular polarization and linear polarization, showing an embodiment of the present invention.

【図2】同上の円偏波及び直線偏波共用一次放射器の正
面図である。
FIG. 2 is a front view of the primary radiator for circular polarization and linear polarization, which is the same as the above.

【図3】従来例を示す、円偏波及び直線偏波共用一次放
射器の一部切欠き斜視図である。
FIG. 3 is a partially cutaway perspective view of a primary radiator for both circular polarization and linear polarization, showing a conventional example.

【符号の説明】[Explanation of symbols]

1 開口部 2 円形導波管 3 終端面 4 フェライト棒 5 励磁コイル 6 励磁コイル 7 励磁コイル 8 プローブ 9 引き出し線 10 入力端子 11 励磁コイル 12 励磁コイル 13 入力端子 21 開口部 22 円形導波管 23 位相差板 24 フェライトポラライザー 26 プローブ 27 終端面 1 Opening 2 Circular Waveguide 3 End Surface 4 Ferrite Rod 5 Excitation Coil 6 Excitation Coil 7 Excitation Coil 8 Probe 9 Leader Wire 10 Input Terminal 11 Excitation Coil 12 Excitation Coil 13 Input Terminal 21 Opening 22 Circular Waveguide 23rd Position Phase difference plate 24 Ferrite polarizer 26 Probe 27 End surface

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 一端に電磁波を導入する開口部を設け、
他端に終端面を設けた円形導波管と、同円形導波管の開
口部側に長手方向が管軸と平行となるようにして同円形
導波管の中心部に配置した、周囲に第1励磁コイルを巻
き付けたフェライト棒と、同フェライト棒が位置する前
記円形導波管の外部円周部に垂直に等間隔にして設けた
4個の第2〜第5励磁コイルと、前記円形導波管の開口
部からみた取付角度が、前記4個の励磁コイルの内、隣
接した励磁コイル間が成す角度を2分する角度で、前記
フェライト棒と前記終端面間の前記円形導波管の側面よ
り内部に挿入したプローブとからなることを特徴とする
円偏波及び直線偏波共用一次放射器。
1. An opening for introducing an electromagnetic wave is provided at one end,
A circular waveguide with a terminating surface at the other end and the circular waveguide at the center of the circular waveguide with the longitudinal direction parallel to the tube axis on the opening side of the circular waveguide. A ferrite rod around which the first excitation coil is wound, four second to fifth excitation coils provided at equal intervals vertically on the outer circumferential portion of the circular waveguide where the ferrite rod is located, and the circular shape. The mounting angle viewed from the opening of the waveguide is an angle that bisects the angle formed between the adjacent exciting coils of the four exciting coils, and the circular waveguide between the ferrite rod and the end face. A primary radiator for both circularly polarized waves and linearly polarized waves, characterized in that it comprises a probe inserted inside from the side surface of.
JP10102792A 1992-04-21 1992-04-21 Primary radiator in common use for circularly polarized wave and linearly polarized wave Pending JPH05299928A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10102792A JPH05299928A (en) 1992-04-21 1992-04-21 Primary radiator in common use for circularly polarized wave and linearly polarized wave

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10102792A JPH05299928A (en) 1992-04-21 1992-04-21 Primary radiator in common use for circularly polarized wave and linearly polarized wave

Publications (1)

Publication Number Publication Date
JPH05299928A true JPH05299928A (en) 1993-11-12

Family

ID=14289711

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10102792A Pending JPH05299928A (en) 1992-04-21 1992-04-21 Primary radiator in common use for circularly polarized wave and linearly polarized wave

Country Status (1)

Country Link
JP (1) JPH05299928A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0865035A (en) * 1994-08-25 1996-03-08 Matsushita Electric Ind Co Ltd Satellite reception converter

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0865035A (en) * 1994-08-25 1996-03-08 Matsushita Electric Ind Co Ltd Satellite reception converter

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