JPH0555808A - Primary radiator to be shared with left-handed and right-handed circularly polarized waves - Google Patents
Primary radiator to be shared with left-handed and right-handed circularly polarized wavesInfo
- Publication number
- JPH0555808A JPH0555808A JP21077491A JP21077491A JPH0555808A JP H0555808 A JPH0555808 A JP H0555808A JP 21077491 A JP21077491 A JP 21077491A JP 21077491 A JP21077491 A JP 21077491A JP H0555808 A JPH0555808 A JP H0555808A
- Authority
- JP
- Japan
- Prior art keywords
- handed
- circularly polarized
- waveguide
- dielectric plate
- lpw
- 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
Links
Landscapes
- Waveguide Switches, Polarizers, And Phase Shifters (AREA)
- Variable-Direction Aerials And Aerial Arrays (AREA)
- Waveguide Aerials (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、一つの衛星放送受信ア
ンテナで、右旋円偏波と左旋円偏波を切り換えて使用で
きる、左旋及び右旋円偏波共用一次放射器に関し、本発
明の動作原理は送信側でも使用することができ、送信側
に使用すれば、右旋円偏波及び左旋円偏波を放射する一
次放射器として使用することができる。衛星放送は、サ
ービスエリア毎に電波の有効利用の面から右旋円偏波と
左旋円偏波が割り当てられており、日本では右旋円偏波
を使用することになっている。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a left-handed and right-handed circularly polarized primary radiator which can be used by switching between right-handed circularly polarized wave and left-handed circularly polarized wave with one satellite broadcast receiving antenna. The principle of operation can be used on the transmitting side as well, and if used on the transmitting side, it can be used as a primary radiator that radiates right-handed circular polarization and left-handed circular polarization. Satellite broadcasting is assigned right-handed circular polarization and left-handed circular polarization in terms of effective use of radio waves for each service area, and in Japan, right-handed circular polarization is used.
【0002】[0002]
【従来の技術】従来の技術では、一つの衛星放送受信ア
ンテナで、右旋円偏波と左旋円偏波を切り換えて使用で
きるものはなかったので、受信しようとするエリア毎
に、別々に受信アンテナを準備する必要があった。2. Description of the Related Art In the prior art, there is no single satellite broadcast receiving antenna that can be used by switching between right-handed circular polarization and left-handed circular polarization. I had to prepare an antenna.
【0003】[0003]
【発明が解決しようとする課題】本発明は、パラボラア
ンテナに左旋及び右旋円偏波共用一次放射器を備えるこ
とにより、右旋円偏波用と左旋円偏波用のアンテナを共
通化することができ、アンテナを標準化して生産管理コ
ストを引き下げることを目的とする。SUMMARY OF THE INVENTION According to the present invention, a parabolic antenna is provided with a left-handed and right-handed circularly polarized wave primary radiator, so that the antennas for right-handed circularly polarized wave and left-handed circularly polarized wave are made common. It is possible to reduce the production control cost by standardizing the antenna.
【0004】[0004]
【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、左旋及び右旋円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、一端を電磁波が
導入し得る開口部1とし、他端に終端面5を設けた円形
導波管2において、同円形導波管2の内部の開口部1側
に同円形導波管2の管軸を中心として回転可能とした誘
電体板3を設け、同誘電体板3の円形導波管2の管軸方
向に沿った長さを円偏波の電磁波を直線偏波の電磁波に
変換できる長さとし、前記円形導波管2の終端面5側の
側面に前記直線偏波の出力手段(図1においては、方形
導波管4)を設けて、前記誘電体板3を回転させて円偏
波の直交する2つの直線偏波の一方の電界と平行となる
ようにして前記出力手段から、前記開口部1に導入され
た左旋円偏波の電磁波から信号を取り出し、前記誘電体
板3を円偏波の直交する2つの直線偏波の他方の電界と
平行となるようにして前記出力手段から、前記開口部1
に導入された右旋円偏波の電磁波から信号を取り出すよ
うにしている。FIG. 1 is a partially cutaway perspective view of a left-handed and right-handed circularly polarized primary radiator showing an embodiment of the present invention. As shown in FIG. In a circular waveguide 2 having one end as an opening 1 through which an electromagnetic wave can be introduced and the other end provided with a terminating surface 5, a tube of the circular waveguide 2 inside the circular waveguide 2 on the side of the opening 1 is provided. A dielectric plate 3 rotatable about an axis is provided, and the length of the dielectric plate 3 along the tube axis direction of the circular waveguide 2 can convert a circularly polarized electromagnetic wave into a linearly polarized electromagnetic wave. The linearly polarized wave output means (the rectangular waveguide 4 in FIG. 1) is provided on the side surface of the circular waveguide 2 on the side of the termination surface 5 and the dielectric plate 3 is rotated to form a circle. The left-handed circularly polarized wave introduced into the opening 1 from the output means so as to be parallel to the electric field of one of the two linearly polarized waves orthogonal to each other. Taking out a signal from a wave from said output means so as to be parallel to the other field of the two linear orthogonal polarized waves of the dielectric plate 3 to circular polarization, the aperture 1
The signal is extracted from the right-handed circularly polarized electromagnetic wave introduced in.
【0005】[0005]
【作用】本発明は上記した構成により、円偏波を直線偏
波に変換しており、図1は、本発明の一実施例を示す、
左旋及び右旋円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、管軸から垂直方向(上部方向)
に向かう軸をY軸とし、管軸から水平方向(左部方向)
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〜図6におい
て同じ)。円形導波管2に導入された左旋円偏波及び右
旋円偏波に対し、誘電体板3を円形導波管2の管軸を中
心として回転させて、円形導波管2の開口部1からみた
誘電体板3の端面の長手方向をX軸と平行にして、右旋
円偏波を直線偏波に変換して円形導波管2の終端面5側
の側面に設けた方形導波管4から信号を出力し、誘電体
板3を回転させて第2図に示すように、円形導波管2の
開口部1からみた誘電体板3の端面の長手方向をY軸と
平行にして、左旋円偏波を直線偏波に変換して方形導波
管4から信号を出力するようにしている。The present invention converts the circular polarized wave into the linear polarized wave by the above-mentioned structure, and FIG. 1 shows an embodiment of the present invention.
FIG. 3 is a partially cutaway perspective view of a left-handed and right-handed circularly polarized primary radiator, in which a vertical direction (upward direction) from the tube axis is shown.
Is the Y-axis, and the horizontal direction from the tube axis (left direction)
The axis toward the X axis is the X axis, and the axis toward the opposite direction is -Y
Axis and -X axis (not shown) (hereinafter the same in FIGS. 2 to 6). The dielectric plate 3 is rotated about the tube axis of the circular waveguide 2 with respect to the left-handed circularly polarized light and the right-handed circularly polarized wave introduced into the circular waveguide 2 to open the opening of the circular waveguide 2. The rectangular guide provided on the side surface of the circular waveguide 2 on the side of the end surface 5 by converting the right-handed circularly polarized wave into a linearly polarized wave with the longitudinal direction of the end surface of the dielectric plate 3 viewed from 1 parallel to the X axis. As shown in FIG. 2, by outputting a signal from the wave guide 4 and rotating the dielectric plate 3, the longitudinal direction of the end face of the dielectric plate 3 viewed from the opening 1 of the circular waveguide 2 is parallel to the Y axis. Then, the left-hand circularly polarized wave is converted into the linearly polarized wave and the signal is output from the rectangular waveguide 4.
【0006】図3は、円偏波の説明図であり、円偏波
は、2つの直交した直線偏波の合成とみなすことがで
き、この2つの直交した直線偏波の振幅が等しく、位相
が90度ずれている場合に円偏波となる。図3に示す円
は、円偏波の電界ベクトルの軌跡を示しており、X軸と
Y軸を2分する向きに電界ベクトルEを有する円偏波が
円形導波管2に導入されたとすると、円偏波はX軸方向
に直線偏波成分Exを有し、Y軸方向に直線偏波成分Eyと
を有する電磁波として表すことができる。X軸方向の直
線偏波の電界が、Y軸方向の直線偏波の電界より位相が
遅れている場合、円偏波の電界ベクトルEは、矢印bの
向きに回転し左旋円偏波となり、Y軸方向の直線偏波の
電界が、X軸方向の直線偏波の電界より位相が遅れてい
る場合、円偏波の電界ベクトルEは、矢印aの向きに回
転し右旋円偏波となる。FIG. 3 is an explanatory diagram of circularly polarized waves, which can be regarded as a combination of two orthogonal linearly polarized waves. The amplitudes of these two orthogonally polarized linearly polarized waves are equal and the phase Are polarized by 90 degrees, circular polarization is obtained. The circle shown in FIG. 3 indicates the locus of the electric field vector of circular polarization, and it is assumed that the circular polarization having the electric field vector E is introduced into the circular waveguide 2 in a direction that bisects the X axis and the Y axis. The circularly polarized wave can be represented as an electromagnetic wave having a linear polarization component Ex in the X axis direction and a linear polarization component Ey in the Y axis direction. When the electric field of the linearly polarized wave in the X-axis direction lags the phase of the electric field of the linearly polarized wave in the Y-axis direction, the electric field vector E of the circularly polarized wave rotates in the direction of arrow b to become a left-handed circularly polarized wave, When the electric field of the linearly polarized wave in the Y-axis direction lags the phase of the electric field of the linearly polarized wave in the X-axis direction, the electric field vector E of the circularly polarized wave rotates in the direction of arrow a and becomes a right-handed circularly polarized wave. Become.
【0007】図4(A)及び(B)は、誘電体板3を使
用した位相器の作用についての説明図であり、円形導波
管2の開口部1からみた正面図である。同位相器に図3
に示す右旋円偏波の電磁波が導入されたとすると、同右
旋円偏波の電磁波のY軸方向の直線偏波の電界は、
(A)図に示すような向きで位相器中を伝播し、X軸方
向の直線偏波の電界は、(B)図に示すような向きで位
相器中を伝播する。誘電体板3は、円形導波管2の開口
部1からみた端面の長手方向をX軸と平行となる向きに
しているため、Y軸方向の直線偏波の位相速度には影響
を与えないが、X軸方向の直線偏波の位相速度を遅くす
ることができる。従って、誘電体板3の円形導波管2の
管軸方向に沿った長さを、Y軸方向の直線偏波の位相よ
りX軸方向の直線偏波の位相が90度遅れる長さとすれ
ば、位相器を電磁波が通り抜けた位置では、位相器に導
入された右旋円偏波の電磁波は直線偏波に変換される。
信号出力手段として方形導波管4を、同方形導波管4の
円形導波管2の管軸方向に向かう中心線が、X軸方向の
電界とY軸方向の電界の合成した電界に対して直角とな
る、Y軸と−X軸を2分する向きにすることにより、同
方形導波管4から変換された前記直線偏波信号を出力す
ることができる。FIGS. 4A and 4B are explanatory views of the operation of the phase shifter using the dielectric plate 3, and are front views seen from the opening 1 of the circular waveguide 2. Figure 3
If the right-handed circularly polarized electromagnetic wave shown in is introduced, the electric field of the right-handed circularly polarized electromagnetic wave of the linearly polarized wave in the Y-axis direction is
The electric field of the linearly polarized wave in the X-axis direction propagates in the phaser in the direction shown in FIG. The dielectric plate 3 does not affect the phase velocity of the linearly polarized wave in the Y-axis direction because the longitudinal direction of the end face of the circular waveguide 2 viewed from the opening 1 is parallel to the X-axis. However, the phase velocity of the linearly polarized wave in the X-axis direction can be reduced. Therefore, if the length of the dielectric plate 3 along the tube axis direction of the circular waveguide 2 is set such that the phase of the linearly polarized wave in the X axis direction is delayed by 90 degrees from the phase of the linearly polarized wave in the Y axis direction. At the position where the electromagnetic wave passes through the phase shifter, the right-handed circularly polarized electromagnetic wave introduced into the phase shifter is converted into the linearly polarized wave.
As the signal output means, the rectangular waveguide 4 is arranged such that the center line of the rectangular waveguide 4 in the tube axis direction of the circular waveguide 2 is the electric field obtained by combining the electric field in the X-axis direction and the electric field in the Y-axis direction. The linearly polarized signal converted from the rectangular waveguide 4 can be output by arranging the Y-axis and the -X-axis that are perpendicular to each other so as to be bisected.
【0008】図5(A)及び(B)は、誘電体板3を使
用した位相器の作用についての説明図であり、円形導波
管2の開口部1からみた正面図である。同位相器に図3
に示す左旋円偏波の電磁波が導入されたとすると、同左
旋円偏波の電磁波のY軸方向の直線偏波の電界は、
(A)図に示すような向きで位相器中を伝播し、X軸方
向の直線偏波の電界は、(B)図に示すような向きで位
相器中を伝播する。誘電体板3は、開口部1からみた端
面の長手方向をY軸と平行となる向きにしているため、
X軸方向の直線偏波の位相速度には影響を与えないが、
Y軸方向の直線偏波の位相速度を遅くすることができ
る。従って、誘電体板3の円形導波管2の管軸方向に沿
った長さを、X軸方向の直線偏波の位相よりY軸方向の
直線偏波の位相が90度遅れる長さとすれば、位相器を
電磁波が通り抜けた位置では、位相器に導入された左旋
円偏波の電磁波は直線偏波に変換される。信号出力手段
として方形導波管4を、同方形導波管4の円形導波管2
の管軸方向に向かう中心線が、X軸方向の電界とY軸方
向の電界の合成した電界に対して直角となる、Y軸と−
X軸を2分する向きにすることにより、同方形導波管4
から変換された前記直線偏波信号を出力することができ
る。従って、方形導波管4からの出力をBSコンバータ
に入力することにより、右旋円偏波と左旋円偏波の衛星
放送を受信することが可能となり、右旋円偏波用と左旋
円偏波用のアンテナを共通化することができ、アンテナ
を標準化して生産管理コストを引き下げることができ
る。FIGS. 5A and 5B are explanatory views of the operation of the phase shifter using the dielectric plate 3, and are front views seen from the opening 1 of the circular waveguide 2. Figure 3
If the left-handed circularly polarized electromagnetic wave shown in is introduced, the electric field of the left-handed circularly polarized electromagnetic wave of the linearly polarized wave in the Y-axis direction is
The electric field of the linearly polarized wave in the X-axis direction propagates in the phaser in the direction shown in FIG. Since the dielectric plate 3 has the end face viewed from the opening 1 in the longitudinal direction parallel to the Y axis,
Does not affect the phase velocity of linearly polarized waves in the X-axis direction,
It is possible to reduce the phase velocity of the linearly polarized wave in the Y-axis direction. Therefore, if the length of the dielectric plate 3 along the tube axis direction of the circular waveguide 2 is set such that the phase of the linearly polarized wave in the Y axis direction is delayed by 90 degrees from the phase of the linearly polarized wave in the X axis direction. , At the position where the electromagnetic wave passes through the phase shifter, the left-handed circularly polarized electromagnetic wave introduced into the phase shifter is converted into a linear polarized wave. The rectangular waveguide 4 is used as a signal output means, and the circular waveguide 2 of the same rectangular waveguide 4 is used.
The center line extending in the tube axis direction of is perpendicular to the combined electric field of the electric field in the X axis direction and the electric field in the Y axis direction.
By making the X-axis into two directions, the rectangular waveguide 4
It is possible to output the linearly polarized signal converted from Therefore, by inputting the output from the rectangular waveguide 4 to the BS converter, it becomes possible to receive satellite broadcasts of right-handed circularly polarized waves and left-handed circularly polarized waves. The wave antenna can be shared, and the antenna can be standardized to reduce the production management cost.
【0009】[0009]
【実施例】図1は、本発明の一実施例を示す、左旋及び
右旋円偏波共用一次放射器の一部切欠き斜視図であり、
1は、円形導波管2に電磁波を効率良く導くためのホー
ン形状とした開口部であり、5は、円形導波管2に導入
された電磁波を反射させるための終端面5であり、同円
形導波管2の内部の開口部1側に同円形導波管2の管軸
を中心として回転可能とした誘電体板3を設け、前記円
形導波管2の終端面5側の側面に導入した電磁波から信
号を取り出す手段として方形導波管4を設けている。誘
電体板3は90度位相器として使用しており、同誘電体
板3の円形導波管2の管軸方向に沿った長手方向の長さ
を、円形導波管2に導入された円偏波の電磁波が直線偏
波に変換される長さとし、短辺方向の長さは両端が円形
導波管2の内部表面に当たらないような長さとしてい
る。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a partially cutaway perspective view of a left-handed and right-handed circularly polarized primary radiator showing an embodiment of the present invention.
Reference numeral 1 denotes a horn-shaped opening for efficiently guiding an electromagnetic wave to the circular waveguide 2, and reference numeral 5 denotes a termination surface 5 for reflecting the electromagnetic wave introduced into the circular waveguide 2. A dielectric plate 3 which is rotatable around the tube axis of the circular waveguide 2 is provided on the side of the opening 1 inside the circular waveguide 2, and the side surface of the circular waveguide 2 on the side of the termination surface 5 is provided. A rectangular waveguide 4 is provided as a means for extracting a signal from the introduced electromagnetic wave. The dielectric plate 3 is used as a 90-degree phase shifter, and the length of the dielectric plate 3 in the longitudinal direction along the tube axis direction of the circular waveguide 2 is a circle introduced into the circular waveguide 2. The length of the polarized electromagnetic wave is converted into a linear polarized wave, and the length in the short side direction is set such that both ends do not hit the inner surface of the circular waveguide 2.
【0010】6は駆動部であり、例えばモータ等を使用
して、同モータの回転と連動して回転する回転軸7を設
けて誘電体板3の短辺方向の中心に取り付け、円偏波の
直交する2つの直線偏波の各々の成分と平行となるよう
に、誘電体板3を回転させることができるようにしてい
る。あるいは、駆動部6を使用する代わりに、手動で誘
電体板3を回転させるようにしても良い。誘電体板3
は、開口部1からみた誘電体板3の端面の長手方向がX
軸と平行となるようにした状態を示し、方形導波管4
は、同方形導波管4の円形導波管2の管軸方向に向かう
中心線と、−X軸とが約45度の角度をなすようにし
て、円形導波管2の終端面5側の側面に接合している。Reference numeral 6 denotes a drive unit, which is provided with a rotary shaft 7 that rotates in conjunction with the rotation of the motor using, for example, a motor, and is attached to the center of the dielectric plate 3 in the direction of the short side for circular polarization. The dielectric plate 3 can be rotated so as to be parallel to the respective components of the two linearly polarized waves orthogonal to each other. Alternatively, instead of using the drive unit 6, the dielectric plate 3 may be manually rotated. Dielectric plate 3
Is X in the longitudinal direction of the end surface of the dielectric plate 3 as viewed from the opening 1.
The rectangular waveguide 4 is shown to be parallel to the axis.
Is the end surface 5 side of the circular waveguide 2 such that the center line of the isotropic waveguide 4 in the tube axis direction of the circular waveguide 2 and the −X axis form an angle of about 45 degrees. Is joined to the side of.
【0011】図2は、図1の誘電体板3を回転させて、
誘電体板3の開口部1からみた端面の長手方向がY軸と
平行となるようにした状態を示している。図1に示すよ
うに、誘電体板3の開口部1からみた端面の長手方向を
X軸と平行となるようにすることにより、右旋円偏波を
直線偏波に変換して、方形導波管4から前記直線偏波信
号を出力し、図2に示すように、誘電体板3の開口部1
からみた端面の長手方向をY軸と平行となるようにする
ことにより、左旋円偏波を直線偏波に変換して、方形導
波管4から前記直線偏波信号を出力するようにしてい
る。In FIG. 2, the dielectric plate 3 shown in FIG.
The figure shows a state in which the longitudinal direction of the end surface of the dielectric plate 3 as viewed from the opening 1 is parallel to the Y axis. As shown in FIG. 1, by making the longitudinal direction of the end face viewed from the opening 1 of the dielectric plate 3 parallel to the X-axis, the right-handed circularly polarized wave is converted into the linearly polarized wave, and the rectangular wave is guided. The linearly polarized signal is output from the wave tube 4, and the opening 1 of the dielectric plate 3 is opened as shown in FIG.
By making the longitudinal direction of the end face as viewed parallel to the Y axis, the left-hand circularly polarized wave is converted into a linearly polarized wave, and the linearly polarized wave signal is output from the rectangular waveguide 4. ..
【0012】図6(A)は、本発明の他の実施例を示
す、左旋及び右旋円偏波共用一次放射器の一部切欠き斜
視図であり、同図(B)は正面図であり、図1の方形導
波管4を使用する代わりに励振プローブ10を信号出力
手段として用いている。励振プローブ10の取り付け位
置は、誘電体板3と終端面5の間の円形導波管2の側面
に設けており、(B)図に示すように、励振プローブ1
0の円形導波管2の管軸方向に向かう中心線が、X軸と
Y軸を2分する角度とし、誘電体板3で直線偏波に変換
された電磁波を励振プローブ10で電気信号に変換し
て、BSコンバータに電気信号を伝送するようにしてい
る。あるいは、左旋及び右旋円偏波共用一次放射器の正
面図からみた励振プローブ10の取り付け角度は−X軸
と−Y軸を2分する角度にしても、同様に誘電体板3で
直線偏波に変換された電磁波を電気信号に変換して、B
Sコンバータに電気信号を伝送することができる。図1
の実施例において、誘電体板3の短辺方向の端面の形状
を略V字型としているが、位相回路としての整合がとれ
るようであれば、他の形状としても良い。また、回転軸
7としては、金属棒、あるいは絶縁物を被せた金属棒、
又は誘電体材料で固い材質のものであれば使用すること
ができる。なお、図1、図2及び図6における8及び9
は、切欠き線を示す。FIG. 6 (A) is a partially cutaway perspective view of a left-handed and right-handed circularly polarized primary radiator showing another embodiment of the present invention, and FIG. 6 (B) is a front view thereof. The excitation probe 10 is used as a signal output means instead of using the rectangular waveguide 4 of FIG. The mounting position of the excitation probe 10 is provided on the side surface of the circular waveguide 2 between the dielectric plate 3 and the end surface 5, and as shown in FIG.
The center line of the circular waveguide 2 of 0 in the tube axis direction is an angle that bisects the X axis and the Y axis, and the electromagnetic wave converted into the linearly polarized wave by the dielectric plate 3 is converted into an electric signal by the excitation probe 10. The electric signal is converted and transmitted to the BS converter. Alternatively, when the mounting angle of the excitation probe 10 as viewed from the front view of the left-handed and right-handed circularly polarized primary radiators is set to an angle that bisects the -X axis and the -Y axis, the linear displacement is similarly performed by the dielectric plate 3. The electromagnetic wave converted into a wave is converted into an electric signal, and B
An electric signal can be transmitted to the S converter. Figure 1
In the embodiment, the shape of the end surface of the dielectric plate 3 in the short side direction is substantially V-shaped, but other shapes may be used as long as matching can be achieved as a phase circuit. Further, as the rotating shaft 7, a metal rod or a metal rod covered with an insulator,
Alternatively, a hard dielectric material can be used. 8 and 9 in FIGS. 1, 2 and 6
Indicates a notch line.
【0013】[0013]
【発明の効果】以上説明したように、本発明によれば、
左旋円偏波を受信時と、右旋円偏波を受信時とで、誘電
体板3の向きを変えることにより各々の電磁波を受信す
ることが可能な左旋及び右旋円偏波共用一次放射器を提
供することができ、衛星放送受信アンテナに同一次放射
器を備えることにより、左旋円偏波用と右旋円偏波用の
アンテナを共通化することができ、アンテナを標準化し
て生産管理コストを引き下げることができる。As described above, according to the present invention,
Left-handed and right-handed circularly polarized primary radiation capable of receiving respective electromagnetic waves by changing the direction of the dielectric plate 3 when receiving left-handed circularly polarized waves and when receiving right-handed circularly polarized waves Can be provided, and by equipping the satellite broadcast receiving antenna with the same primary radiator, the antennas for left-handed circularly polarized waves and right-handed circularly polarized waves can be shared, and standardized antennas are produced. Management costs can be reduced.
【図1】本発明の一実施例を示す、左旋及び右旋円偏波
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 left-handed and right-handed circularly polarized primary radiator showing an embodiment of the present invention.
【図2】図1に示す左旋及び右旋円偏波共用一次放射器
の誘電体板3を、垂直方向に回転させた状態を示す一部
切欠き斜視図である。2 is a partially cutaway perspective view showing a state in which a dielectric plate 3 of the left-handed and right-handed circularly polarized primary radiator shown in FIG. 1 is rotated in a vertical direction.
【図3】円偏波の説明図である。FIG. 3 is an explanatory diagram of circular polarization.
【図4】(A)及び(B)は、誘電体板3を使用した位
相器の作用についての説明図であり、円形導波管2の開
口部1からみた正面図である。4 (A) and 4 (B) are explanatory views of the action of the phase shifter using the dielectric plate 3, and are front views seen from the opening 1 of the circular waveguide 2.
【図5】(A)及び(B)は、誘電体板3を使用した位
相器の作用についての説明図であり、円形導波管2の開
口部1からみた正面図である。5 (A) and 5 (B) are explanatory views of the action of the phase shifter using the dielectric plate 3, and are front views seen from the opening 1 of the circular waveguide 2.
【図6】(A)は、本発明の他の実施例を示す、左旋及
び右旋円偏波共用一次放射器の一部切欠き斜視図であ
り、(B)は、正面図である。6A is a partially cutaway perspective view of a left-handed and right-handed circularly polarized primary radiator according to another embodiment of the present invention, and FIG. 6B is a front view thereof.
1 開口部 2 円形導波管 3 誘電体板 4 方形導波管 5 終端面 6 駆動部 7 回転軸 8 切欠き線 9 切欠き線 10 励振プローブ 1 Opening 2 Circular Waveguide 3 Dielectric Plate 4 Rectangular Waveguide 5 End Face 6 Drive Part 7 Rotation Axis 8 Notch Line 9 Notch Line 10 Excitation Probe
Claims (2)
他端に終端面を設けた円形導波管において、同円形導波
管の内部の開口部側に同円形導波管の管軸を中心として
回転可能とした誘電体板を設け、同誘電体板の円形導波
管の管軸方向に沿った長さを円偏波の電磁波を直線偏波
の電磁波に変換できる長さとし、前記円形導波管の終端
面側の側面に前記直線偏波の出力手段を設けて、前記誘
電体板を回転させて円偏波の直交する2つの直線偏波の
一方の電界と平行となるようにして前記出力手段から、
前記開口部に導入された左旋円偏波の電磁波から信号を
取り出し、前記誘電体板を円偏波の直交する2つの直線
偏波の他方の電界と平行となるようにして前記出力手段
から、前記開口部に導入された右旋円偏波の電磁波から
信号を取り出すことを特徴とする左旋及び右旋円偏波共
用一次放射器。1. An opening at one end of which electromagnetic waves can be introduced,
In a circular waveguide having a terminating surface at the other end, a dielectric plate that is rotatable around the tube axis of the circular waveguide is provided on the opening side inside the circular waveguide. The length of the plate along the tube axis direction of the circular waveguide is set to a length capable of converting the circularly polarized electromagnetic wave into the linearly polarized electromagnetic wave, and An output means is provided, and the dielectric plate is rotated so as to be parallel to one of the electric fields of two linearly polarized waves orthogonal to each other of circularly polarized waves.
A signal is extracted from the left-handed circularly polarized electromagnetic wave introduced into the opening, and the dielectric plate is made parallel to the other electric field of the two linearly polarized waves orthogonal to each other from the circularly polarized wave. A left-handed and right-handed circularly polarized primary radiator, wherein a signal is taken out from the right-handed circularly polarized electromagnetic wave introduced into the opening.
ローブからなることを特徴とする請求項1記載の左旋及
び右旋円偏波共用一次放射器。2. The left-handed and right-handed circularly-polarized primary radiator according to claim 1, wherein the output means is a rectangular waveguide or an excitation probe.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21077491A JPH0555808A (en) | 1991-08-22 | 1991-08-22 | Primary radiator to be shared with left-handed and right-handed circularly polarized waves |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21077491A JPH0555808A (en) | 1991-08-22 | 1991-08-22 | Primary radiator to be shared with left-handed and right-handed circularly polarized waves |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0555808A true JPH0555808A (en) | 1993-03-05 |
Family
ID=16594924
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP21077491A Pending JPH0555808A (en) | 1991-08-22 | 1991-08-22 | Primary radiator to be shared with left-handed and right-handed circularly polarized waves |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0555808A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9070386B2 (en) | 2012-12-04 | 2015-06-30 | Seagate Technology Llc | Polarization rotator |
CN112713375A (en) * | 2019-10-24 | 2021-04-27 | Vega格里沙贝两合公司 | Waveguide device and antenna |
-
1991
- 1991-08-22 JP JP21077491A patent/JPH0555808A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9070386B2 (en) | 2012-12-04 | 2015-06-30 | Seagate Technology Llc | Polarization rotator |
KR101536980B1 (en) * | 2012-12-04 | 2015-07-16 | 시게이트 테크놀로지 엘엘씨 | Polarization rotator |
US9355662B2 (en) | 2012-12-04 | 2016-05-31 | Seagate Technology Llc | Polarization rotator |
CN112713375A (en) * | 2019-10-24 | 2021-04-27 | Vega格里沙贝两合公司 | Waveguide device and antenna |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JP4027967B2 (en) | Polarization switching / directivity variable antenna | |
US9742069B1 (en) | Integrated single-piece antenna feed | |
JP3195923B2 (en) | Circularly polarized dielectric antenna | |
JP4235251B2 (en) | Polarization switching / directivity variable antenna | |
EP1291965B1 (en) | Antenna | |
JPH01501911A (en) | circular waveguide slot antenna | |
JPH0555808A (en) | Primary radiator to be shared with left-handed and right-handed circularly polarized waves | |
JPH0583004A (en) | Primary radiator in common use for circularly polarized wave and linearly polarized wave | |
JPH0541602A (en) | Primary radiator in common use with circularly polarized wave and linearly polarized wave | |
JPH0529801A (en) | Circularly polarized wave and linear polarized wave and shared primary radiator | |
JPH0555805A (en) | Primary radiator to be shared with circularly polarized wave and linearly polarized wave | |
JPH0555806A (en) | Primary radiator to be shared with circulariy polarized wave and linearly polarized wave | |
Liu et al. | Design of a W-band Omnidirectional Circularly Polarized Antenna by Using OMT | |
JPH06232602A (en) | Primary radiator | |
JPH06132720A (en) | Primary radiator sharing circular polarization and linear polarization waves | |
JPH06232603A (en) | Primary radiator in common use for circularly polarized wave and linearly polarized wave | |
JPH0454002A (en) | Feed horn for both circularly polarized wave and linearly polarized wave | |
JPH04373201A (en) | Primary radiator in common use for circularly polarized wave and linearly polarized wave | |
JPH036685B2 (en) | ||
JPH05206720A (en) | Primary radiator in common use for circularly and linearly polarized waves | |
JPH0541603A (en) | Primary radiator in common use with circularly polarized wave and linearly polarized wave | |
JPH07231201A (en) | Primary radiator | |
JPH06216638A (en) | Feed horn shared by circularly polarized wave and linear polarized wave | |
JPH05327337A (en) | Circularly polarized wave and linearly polarized wave multicoupling primary radiator | |
JPH0555807A (en) | Primary radiator to be shared with circularly polarized wave and linearly polarized wave |