JPH03154406A - Antenna system - Google Patents

Antenna system

Info

Publication number
JPH03154406A
JPH03154406A JP29330189A JP29330189A JPH03154406A JP H03154406 A JPH03154406 A JP H03154406A JP 29330189 A JP29330189 A JP 29330189A JP 29330189 A JP29330189 A JP 29330189A JP H03154406 A JPH03154406 A JP H03154406A
Authority
JP
Japan
Prior art keywords
dielectric
metal
face
linearly polarized
dielectric plate
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
JP29330189A
Other languages
Japanese (ja)
Inventor
Norio Miyahara
典夫 宮原
Takashi Hirukoi
蛭子井 貴
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP29330189A priority Critical patent/JPH03154406A/en
Publication of JPH03154406A publication Critical patent/JPH03154406A/en
Pending legal-status Critical Current

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  • Variable-Direction Aerials And Aerial Arrays (AREA)

Abstract

PURPOSE:To facilitate the adjustment of a direction of a radiation beam and the polarized wave face of a linearly polarized wave by adopting the constitution such that a rotary shaft of a rotating parabolic face is place perpendicularly and a tilt angle of a dielectric plate and a rotating angle are adjusted. CONSTITUTION:A metallic grating 3 formed by arranging lots of metallic strips with a narrower width than the wavelength of an operating frequency is provided to the inner face of a dielectric body 2 shaped as a rotating parabolic face. A dielectric plate 4 one side of which a metallic film 8 is provided and other side of which a metallic grating 5 formed hy arranging lots of metallic strips with a narrower width than the wavelength of an operating frequency is provided is placed in an inner space of the dielectric body 2. Furthermore, a primary radiator 1 radiating a radio wave of linearly polarized wave from the inner direction of the dielectric body 2 to the outside is provided and the rotating shaft of the rotating parabolic face of the dielectric body 2 is made almost perpendicular. Then the tilt angle and the rotating angle of the dielectric plate 4 are adjusted. Thus, the volume of the antenna system occupied in space is reduced, and the radiating beam direction of the antenna system and the polarized face of the linearly polarized wave are easily adjusted.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は衛星通信用の簡易地球局に用いられる小型の
直線偏波用のアンテナ装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a small linearly polarized antenna device used in a simple earth station for satellite communication.

〔従来の技術〕[Conventional technology]

第5図は例えば三菱電機技報Vo1.58.No、9.
1984に示された従来のアンテナ装置を示す概略構成
図であり、図において、工は円偏波の電波を放射する一
次放射器、10は電波を反射させる反射鏡、7は電波を
受信する受信機、11は受信周波数を低周波数に変換す
るダウンコンバータ、8は受信機7とダウンコンバータ
11とを接続する同軸ケーブル、12は方向調整用治具
、14は円偏波を発生する円偏波発生器である。第6図
は例えば昭和60年度電子情報通信学会全国大会(講演
番号S6−2)に示された従来のアンテナ装置を示す概
略構成図であり、図において、20は円偏波励振用素子
アンテナ、21は給電回路、11はダウンコンバータ、
7は受信機、8は同軸ケーブルである。
FIG. 5 shows, for example, Mitsubishi Electric Technical Report Vol. 1.58. No, 9.
1 is a schematic configuration diagram showing a conventional antenna device shown in 1984. In the figure, numeral 1 is a primary radiator that emits circularly polarized radio waves, 10 is a reflector that reflects radio waves, and 7 is a receiver that receives radio waves. 11 is a down converter that converts the received frequency to a low frequency; 8 is a coaxial cable that connects the receiver 7 and the down converter 11; 12 is a direction adjustment jig; 14 is a circularly polarized wave that generates circularly polarized waves. It is a generator. FIG. 6 is a schematic configuration diagram showing a conventional antenna device shown, for example, at the 1985 IEICE national conference (lecture number S6-2). In the figure, 20 is an element antenna for circularly polarized wave excitation; 21 is a power supply circuit, 11 is a down converter,
7 is a receiver, and 8 is a coaxial cable.

次に動作について説明する。送信を例にとって説明する
。第5図において、受信機7と接続された一次放射器1
により放射された円偏波を有する球面波の電波は反射鏡
10により反射されて平面波の電波に変換され、反射鏡
10の鏡軸方向に放射される。方向調整用治具12によ
り、反射鏡10の鏡軸と衛星13の方向とを一致させる
Next, the operation will be explained. This will be explained using transmission as an example. In FIG. 5, a primary radiator 1 connected to a receiver 7
The circularly polarized spherical radio waves radiated by the reflector 10 are reflected by the reflector 10, converted into plane wave radio waves, and radiated in the mirror axis direction of the reflector 10. A direction adjustment jig 12 is used to align the mirror axis of the reflecting mirror 10 with the direction of the satellite 13.

また、第6図において、同軸ケーブル8により受信機7
と接続された給電回路2工により各円偏波励振用素子ア
ンテナ20に電力が供給される。
In addition, in FIG. 6, the receiver 7 is connected to the coaxial cable 8.
Power is supplied to each circularly polarized wave excitation element antenna 20 by two feeder circuits connected to the two.

各円偏波励振用素子アンテナ20に給電される振幅分布
は一様であり、位相分布は、給電回路21の線路長を調
整して、放射ビームの方向に直角の面内で位相が揃うよ
うに設定される。
The amplitude distribution fed to each circularly polarized wave excitation element antenna 20 is uniform, and the phase distribution is adjusted by adjusting the line length of the feeding circuit 21 so that the phases are aligned in a plane perpendicular to the direction of the radiation beam. is set to

上記第5図及び第6図に示した従来のアンテナ装置は円
偏波アンテナである。しかし、第5図において円偏波発
生器14を取り外すことにより直線偏波アンテナになる
こと、また、第6図において円偏波励振用素子を直線偏
波励振用素子に変更することにより直線偏波アンテナに
なることは容易に類推できる。ここでは上記第5図及び
第6図を直線偏波アンテナの従来例として説明すること
とする。
The conventional antenna device shown in FIGS. 5 and 6 above is a circularly polarized antenna. However, by removing the circularly polarized wave generator 14 in Fig. 5, it becomes a linearly polarized antenna, and in Fig. 6, by changing the circularly polarized wave excitation element to a linearly polarized wave excitation element, It is easy to infer that it becomes a wave antenna. Here, the above-mentioned FIGS. 5 and 6 will be explained as conventional examples of linearly polarized antennas.

C発明が解決しようとする課題〕 従来のアンテナ装置は以上のように構成されているので
、第5図の従来例においては、アンテナ装置の空間に占
める体積が大きくなり、例えば、アンテナ装置を屋外に
設置する場合、風圧に十分耐える必要があるので、設置
するための工事が繁雑なものになり、また、設置される
アンテナ装置の周囲の景観と調和せず、美観を損ねる問
題点があった。
C Problems to be Solved by the Invention] Since the conventional antenna device is configured as described above, in the conventional example shown in FIG. 5, the volume occupied by the antenna device in the space is large. When installing antenna equipment, it is necessary to withstand sufficient wind pressure, so the installation work becomes complicated, and there is also the problem that it does not harmonize with the surrounding scenery of the antenna equipment to be installed, spoiling its aesthetic appearance. .

また、第6図の従来例においては、平板状の構造を有し
、住宅の屋根や壁等に取り付けられるので、アンテナ装
置の周囲の景観と調和し美観を損ねず、また、アンテナ
装置空間に占める体積は小さく、簡単に設置できる。し
かし、アンテナ装置の放射ビーム方向及び直線偏波面は
、それぞれ、給電回路21の線路長の設定及び直線偏波
励振用素子アンテナの配置により決まっており、一方、
住宅の屋根や壁は必ずしも衛星13の方向を向いておら
ず、アンテナ装置を住宅の屋根や壁等に取り付けた後で
、アンテナ装置の放射ビーム方向を衛星13の方向と一
致させたり、アンテナ装置の直線偏波の偏波面を衛星1
3の偏波面と一致するように調整するのは繁雑であると
いう問題点があった。
In addition, the conventional example shown in Fig. 6 has a flat plate-like structure and can be attached to the roof or wall of a house, so it harmonizes with the surrounding landscape of the antenna device and does not spoil the aesthetic appearance. It occupies a small volume and is easy to install. However, the radiation beam direction and linear polarization plane of the antenna device are determined by the line length setting of the feeder circuit 21 and the arrangement of the linear polarization excitation element antenna, respectively;
The roof or wall of a house does not necessarily face the direction of the satellite 13, so after installing the antenna device on the roof or wall of the house, the direction of the radiation beam of the antenna device should match the direction of the satellite 13, or the direction of the antenna device Satellite 1
There was a problem in that it was complicated to adjust the polarization plane to match the polarization plane of No. 3.

この発明は上記のような課題を解消するためになされた
もので、アンテナ装置の空間に占める体積を小さ(して
美観を損なわないようにできるとともに、アンテナ装置
の放射ビーム方向及び直線偏波の偏波面の調整が容易に
できるアンテナ装置を得ることを目的とする。
This invention was made to solve the above-mentioned problems, and it is possible to reduce the volume occupied by the antenna device (so that the aesthetic appearance is not impaired), and also to change the radiation beam direction and linear polarization of the antenna device. An object of the present invention is to obtain an antenna device whose polarization plane can be easily adjusted.

〔課題を解決するための手段〕[Means to solve the problem]

この発明に係るアンテナ装置は、回転放物面の形状を有
する誘電体2の内面に、使用周波数の波長に比べて幅の
狭い金属帯を多数並べた金属格子3を設け、かつ上記誘
電体2の内部空間に、一方の面に金属膜6と他方の面に
使用周波数の波長に比べて幅の狭い金属帯を多数並べた
金属格子5とを備えた誘電体板4を設け、上記誘電体2
の内方から外方に向かって直線偏波の電波を放射する一
次放射器1を備え、上記誘電体2の回転放物面の回転軸
がほぼ垂直となるように設置すると共に、上記誘電体板
4の傾き角と回転角とを調整できる構成を有したことを
特徴とするものである。
The antenna device according to the present invention includes a metal lattice 3 in which a large number of metal bands having a width narrower than the wavelength of the frequency used is arranged on the inner surface of a dielectric body 2 having a shape of a paraboloid of rotation, and the dielectric body 2 A dielectric plate 4 having a metal film 6 on one surface and a metal grid 5 in which a large number of metal strips having a width narrower than the wavelength of the frequency used is arranged on the other surface is provided in the internal space of the dielectric material. 2
It is equipped with a primary radiator 1 that radiates linearly polarized radio waves from the inside to the outside of the dielectric body, and is installed so that the axis of rotation of the paraboloid of revolution of the dielectric body 2 is substantially perpendicular to the dielectric body. This device is characterized by having a configuration in which the inclination angle and rotation angle of the plate 4 can be adjusted.

〔作用〕[Effect]

この発明におけるアンテナ装置は、上記−次放射器1よ
り放射されたほぼ球面状の直線偏波の電波が、回転放物
面の形状を有する上記誘電体2の内面においてほぼ平面
状の電波に変換されて反射され、さらに上記誘電体板4
において、直線偏波の偏波面が上記−次放射器1におけ
る偏波面と90”異なる平面波に変換されて反射され、
空間に放射される。
In the antenna device of the present invention, substantially spherical linearly polarized radio waves emitted from the -order radiator 1 are converted into substantially planar radio waves on the inner surface of the dielectric body 2 having a paraboloid of revolution shape. The dielectric plate 4
, the polarization plane of the linearly polarized wave is converted into a plane wave that is 90" different from the polarization plane in the -order radiator 1 and reflected,
radiated into space.

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

以下、この発明の一実施例を図について説明する。第1
図において、1はバッチアンテナから構成される一次放
射器、2は誘電体、3は誘電体2の内面に設けた金属格
子、4は誘電体板、5は誘電体板4の一方面に設けた金
属格子、6は誘電体板4の他方面に設けた金属膜、11
は一次放射器1と一体構造で構成された受信機の一部で
あるダウンコンバータ、12はアンテナ装置の放射ビー
ム方向及び偏波面を調整するための方向調整用冶具であ
る。
An embodiment of the present invention will be described below with reference to the drawings. 1st
In the figure, 1 is a primary radiator composed of a batch antenna, 2 is a dielectric, 3 is a metal grid provided on the inner surface of the dielectric 2, 4 is a dielectric plate, and 5 is provided on one side of the dielectric plate 4. a metal grid 6, a metal film provided on the other side of the dielectric plate 4, 11
12 is a down converter which is a part of the receiver integrally constructed with the primary radiator 1, and 12 is a direction adjustment jig for adjusting the radiation beam direction and polarization plane of the antenna device.

送信を例にとり説明する。第1図において、−次放射器
1は、はぼ球面状の直線偏波の電波を、回転放物面の形
状を有する誘電体2の内面に向かって放射する。誘電体
2の内面には、使用周波数の波長に比べて幅の狭い金属
帯を多数並べた金属格子3が設けてあり、その金属格子
3の帯の伸びる方向を、−次放射器1により放射された
電波の偏波面と一致するように誘電体2を設定する。す
ると、−次放射器lにより放射された電波は、金属格子
3により、偏波面が変化しないほぼ平面状の電波に変換
されて反射し、誘電体板4に向かう。
This will be explained using transmission as an example. In FIG. 1, a -order radiator 1 radiates linearly polarized radio waves having a spherical shape toward the inner surface of a dielectric body 2 having a paraboloid of revolution shape. A metal lattice 3 is provided on the inner surface of the dielectric 2. A metal lattice 3 is provided in which a large number of metal bands whose width is narrower than the wavelength of the frequency used is arranged. The dielectric 2 is set so that the plane of polarization of the radio waves coincides with that of the radio waves. Then, the radio waves emitted by the -order radiator l are converted by the metal grating 3 into substantially planar radio waves whose plane of polarization does not change, are reflected, and are directed toward the dielectric plate 4 .

第2図において、誘電体板4は一次放射器1と同一の平
面上に設けられており、誘電体板4の誘電体2に面する
側には、使用周波数の波長に比べて幅の狭い金属帯を多
数並べた金属格子5が設けてあり、その反射面側には金
属膜6が設けられている。金属格子5のパターンの伸び
ている方向は一次放射器1の放射する直線偏波の方向と
、はぼ45″の角度をなすように設定しである。誘電体
板4の厚さは174波長の電気長に設定する。金属格子
3により反射された電波は金属格子5に入射する。第3
図に示すように、金属格子5に入射した電波を、金属格
子5の金属帯の伸びる方向の成分Haと、これに直交す
る成分Ebとに分解する。Haの成分の電波は金属格子
5上で逆相の電波として反射する。一方、Ebの成分の
電波は金属格子5を透過して上記金属膜6において逆相
の電波として反射し再び金属格子5に向かう。誘電体板
4の厚さは174波長の電気長になっているので、金属
格子5に戻ってきた電波の位相は金属格子5に入射した
ときの位相と同相になる。この結果、金属格子5に対し
反射波の偏波方向は入射波の偏波方向と90″異なる。
In FIG. 2, the dielectric plate 4 is provided on the same plane as the primary radiator 1, and the side of the dielectric plate 4 facing the dielectric 2 has a narrow width compared to the wavelength of the frequency used. A metal grid 5 in which a large number of metal strips are arranged is provided, and a metal film 6 is provided on the reflective surface side of the metal grid 5. The extending direction of the pattern of the metal grating 5 is set to form an angle of approximately 45'' with the direction of the linearly polarized wave emitted by the primary radiator 1.The thickness of the dielectric plate 4 is 174 wavelengths. The electrical length is set to .The radio wave reflected by the metal grid 3 enters the metal grid 5.The third
As shown in the figure, the radio wave incident on the metal grid 5 is decomposed into a component Ha in the direction in which the metal strips of the metal grid 5 extend, and a component Eb perpendicular to this. The radio wave of the Ha component is reflected on the metal grid 5 as a radio wave with an opposite phase. On the other hand, the Eb component radio wave passes through the metal grating 5, is reflected at the metal film 6 as a radio wave with an opposite phase, and heads toward the metal grating 5 again. Since the thickness of the dielectric plate 4 is an electrical length of 174 wavelengths, the phase of the radio wave returning to the metal grating 5 is the same as the phase when it is incident on the metal grating 5. As a result, the polarization direction of the reflected wave with respect to the metal grating 5 differs from the polarization direction of the incident wave by 90''.

即ち、金属格子5により直線偏波の偏波面が一次放射器
1における偏波面と90゜異なる平面波に変換されて反
射され、再び誘電体2へ向かう。第4図に示すように、
−次放射器1における偏波面と90’異なる平面波は誘
電体2の内面に設けられた金属格子3に対し透過して空
間に放射される。
That is, the plane of polarization of the linearly polarized wave is converted by the metal grating 5 into a plane wave whose polarization plane differs by 90 degrees from the plane of polarization in the primary radiator 1, and is reflected back toward the dielectric 2. As shown in Figure 4,
A plane wave whose polarization plane differs by 90' from the plane of polarization in the -order radiator 1 is transmitted through the metal grating 3 provided on the inner surface of the dielectric body 2 and radiated into space.

アンテナ装置の回転放物面の形状を存する誘電体2の回
転軸がほぼ垂直となるように設置されるため、アンテナ
装置の空間に占める体積が小さく、風圧に耐えやすいた
め設置のための工事が容易になり、アンテナ装置の設置
される周囲の景観と調和するので美観を損ねない。次に
、アンテナ装置の放射ビーム方向は、誘電体板4の傾き
角を変化することにより容易に調整できる。また、放射
ビームの偏波方向は、同一平面上に構成された一次放射
器1及び誘電体板3の回転角を変化することにより容易
に調整で′きる。
Since the antenna device is installed so that the axis of rotation of the dielectric 2, which has the shape of a paraboloid of revolution, is almost vertical, the volume occupied by the antenna device is small and it can easily withstand wind pressure, so construction work for installation is unnecessary. It is easy to install, and it harmonizes with the surrounding landscape in which the antenna device is installed, so it does not spoil the aesthetics. Next, the radiation beam direction of the antenna device can be easily adjusted by changing the inclination angle of the dielectric plate 4. Further, the polarization direction of the radiation beam can be easily adjusted by changing the rotation angle of the primary radiator 1 and the dielectric plate 3, which are arranged on the same plane.

なお、上記実施例では受信機の一部であるダウンコンバ
ータを誘電体板に取り付けたが、受信機の全体あるいは
送信機の一部又は全部、送受信機の一部又は全部を誘電
体板に取り付けてもよい。
In the above embodiment, the down converter, which is part of the receiver, was attached to the dielectric plate, but the entire receiver, part or all of the transmitter, or part or all of the transceiver may be attached to the dielectric plate. You can.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によれば、回転放物面の形状を
有する誘電体の内面に、使用周波数の波長に比べて幅の
狭い金属帯を多数並べた金属格子を設け、かつ上記誘電
体の内部に、一方の面に金属膜と他方の面に使用周波数
の波長に比べて幅の狭い金属帯を多数並べた金属格子を
設けた誘電体板、及び直線偏波の電波を放射する一次放
射器を設けた構成とし、上記回転放物面の回転軸がほぼ
垂直となるように設置すると共に、上記誘電体板の傾き
角と回転角とを調整できる構成としたので、アンテナ装
置の空間に占める体積を小さくなり、設置が容易であり
美観を損なわないようにできるとともに、アンテナ装置
の放射ビーム方向及び直線偏波の偏波面の調整が容易に
できるという効果が得られる。
As described above, according to the present invention, a metal lattice in which a large number of metal bands having a width narrower than the wavelength of a frequency used is provided on the inner surface of a dielectric having a paraboloid of rotation shape, and the dielectric Inside, there is a dielectric plate with a metal film on one side and a metal lattice with a large number of metal strips narrower than the wavelength of the frequency used on the other side, and a primary plate that emits linearly polarized radio waves. The configuration includes a radiator, which is installed so that the axis of rotation of the paraboloid of rotation is almost vertical, and the tilt angle and rotation angle of the dielectric plate can be adjusted, thereby reducing the space of the antenna device. This has the advantage that the volume occupied by the antenna device can be reduced, the installation is easy, and the aesthetic appearance is not spoiled, and the direction of the radiation beam of the antenna device and the plane of polarization of linearly polarized waves can be easily adjusted.

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

第1図は、この発明の一実施例によるアンテナ装置を示
す概略構成図及びアンテナ装置姓中≠#における金属格
子3を真上から見た透視図、第2図は、誘電体板4上に
構成された一次放射器1、金属格子5、反射膜6、受信
機7及び方向調整用治具12を説明するための図、第3
図は、金属格子5における入射波と反射波の偏波方向の
変化を説明するための図、第4図は、金属格子2と金属
格子5の位置関係を説明するための図、第5図及び第6
図は従来のアンテナ装置を示す概略構成図である。 1・・・−次放射器、2・・・誘電体、3・・・金属格
子、4・・・誘電体板、5・・・金属格子、6・・・金
属膜。
FIG. 1 is a schematic configuration diagram showing an antenna device according to an embodiment of the present invention, and a perspective view of the metal grid 3 seen from directly above when the antenna device name is ≠ #. FIG. A third diagram for explaining the configured primary radiator 1, metal grating 5, reflective film 6, receiver 7, and direction adjustment jig 12.
4 is a diagram for explaining the change in the polarization direction of an incident wave and a reflected wave in the metal grating 5, FIG. 4 is a diagram for explaining the positional relationship between the metal grating 2 and the metal grating 5, and FIG. and the sixth
The figure is a schematic configuration diagram showing a conventional antenna device. 1...-order radiator, 2... dielectric, 3... metal lattice, 4... dielectric plate, 5... metal lattice, 6... metal film.

Claims (1)

【特許請求の範囲】[Claims]  回転放物面の形状を有する誘電体の内面に、使用周波
数の波長に比べて幅の狭い金属帯を並べた金属格子を設
け、かつ上記誘電体の内部空間に、一方の面に金属膜と
他方の面に使用周波数の波長に比べて幅の狭い金属帯を
多数並べた金属格子とを備えた誘電体板を設け、上記誘
電体の内方から外方に向かって直線偏波の電波を放射す
る一次放射器を備え、上記誘電体の回転放射面の回転軸
がほぼ垂直となるように設置すると共に、上記誘電体板
の傾き角と回転角とを調整できる構成を有したことを特
徴とするアンテナ装置。
A metal lattice in which metal bands having a width narrower than the wavelength of the frequency used is arranged on the inner surface of a dielectric body having the shape of a paraboloid of rotation, and a metal film and a metal film on one surface are provided in the internal space of the dielectric body. A dielectric plate is provided on the other surface with a metal grid in which a large number of metal strips having a width narrower than the wavelength of the frequency used is arranged, and linearly polarized radio waves are emitted from the inside of the dielectric to the outside. It is characterized by comprising a primary radiator that emits radiation, installed so that the axis of rotation of the rotating radiation surface of the dielectric is substantially perpendicular, and having a configuration in which the inclination angle and rotation angle of the dielectric plate can be adjusted. antenna device.
JP29330189A 1989-11-10 1989-11-10 Antenna system Pending JPH03154406A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29330189A JPH03154406A (en) 1989-11-10 1989-11-10 Antenna system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29330189A JPH03154406A (en) 1989-11-10 1989-11-10 Antenna system

Publications (1)

Publication Number Publication Date
JPH03154406A true JPH03154406A (en) 1991-07-02

Family

ID=17793059

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29330189A Pending JPH03154406A (en) 1989-11-10 1989-11-10 Antenna system

Country Status (1)

Country Link
JP (1) JPH03154406A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2018109837A1 (en) * 2016-12-13 2018-06-21 三菱電機株式会社 Reflection mirror antenna device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2018109837A1 (en) * 2016-12-13 2018-06-21 三菱電機株式会社 Reflection mirror antenna device
US10797401B2 (en) 2016-12-13 2020-10-06 Mitsubishi Electric Corporation Reflection mirror antenna device

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