JPS59194513A - Parabolic antenna for circular polarized wave - Google Patents

Parabolic antenna for circular polarized wave

Info

Publication number
JPS59194513A
JPS59194513A JP6868183A JP6868183A JPS59194513A JP S59194513 A JPS59194513 A JP S59194513A JP 6868183 A JP6868183 A JP 6868183A JP 6868183 A JP6868183 A JP 6868183A JP S59194513 A JPS59194513 A JP S59194513A
Authority
JP
Japan
Prior art keywords
polarized wave
wave generator
parabola
circular polarized
circularly polarized
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
JP6868183A
Other languages
Japanese (ja)
Inventor
Shuji Urasaki
修治 浦崎
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 JP6868183A priority Critical patent/JPS59194513A/en
Publication of JPS59194513A publication Critical patent/JPS59194513A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q19/00Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic
    • H01Q19/10Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic using reflecting surfaces
    • H01Q19/18Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic using reflecting surfaces having two or more spaced reflecting surfaces
    • H01Q19/19Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic using reflecting surfaces having two or more spaced reflecting surfaces comprising one main concave reflecting surface associated with an auxiliary reflecting surface
    • H01Q19/195Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic using reflecting surfaces having two or more spaced reflecting surfaces comprising one main concave reflecting surface associated with an auxiliary reflecting surface wherein a reflecting surface acts also as a polarisation filter or a polarising device

Landscapes

  • Aerials With Secondary Devices (AREA)

Abstract

PURPOSE:To omit a circular/angular converter, to obtain an economical antenna and to reduce the quantity of reflected waves from a glid type circular polarized wave generator to a pyramid horn by constituting a parabolic antenna by a parabola, a pyramid horn by constituting a parabolic antenna by a parabola, a pyramid corn, a down converter, an apex matching plate and the glid type circular polarized wave generator. CONSTITUTION:The circular polarized wave parabolic antenna is constituted by the parabola 1, the pyramid horn 14, the down converter 6, the elliptical cone type apex matching plate, and the glid type circular polarized wave generator 10 The terminal of the converter 6 is formed like a square and directly connected to the pyramid horn 14, so that the circular/angular converter can be omitted. Straightly polarized radio waves are radiated from the pyramid horn 14 and converted into circularly polarized waves by the glid type circular polarized wave generator 10 and the converted circular polarized waves are reflected, irradiated to the parabola 1 and then radiated to the space. The center axis of the pyramid horn 14 is made coincide with that of the apex matching plate 15 and the longitudinal direction of an opening of the pyramid horn 14 is made coincide with the apse line direction of the ellipse of the apex matching plate 15. Thus, the quantity of reflected waves from the circular polarized wave generator 10 to the pyramid horn 14 can be reduced.

Description

【発明の詳細な説明】 この発明は一次放射系とパラボラからなる円偏波パラボ
ラアンテナの改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement of a circularly polarized parabolic antenna consisting of a primary radiation system and a parabola.

従来のこの種アンテナは第1図に示すように。A conventional antenna of this type is shown in Figure 1.

パラボラ(1)9円錐ホーン(2)、円偏波発生器(3
)、丸角変換器(4)、矩形導波管(5)、及びダウン
コンバータ(6)で構成されていた。なお人はパラボラ
の中心軸である。ここで9円偏波発生器(3)は4分の
1波長板を円形導波管に挿入したものが一般的である。
Parabola (1) 9-conical horn (2), circularly polarized wave generator (3)
), a round-angle converter (4), a rectangular waveguide (5), and a down-converter (6). Furthermore, people are the central axis of parabola. Here, the nine circularly polarized wave generator (3) is generally one in which a quarter wavelength plate is inserted into a circular waveguide.

また、丸角変換器(4)は矩形導波管(5)の矩形開口
と円偏波発生器(3)の円形開口をなめらかに変換する
ものである。また、ダウンコンバータ(6)は局部発振
器を内蔵しており、中間周波数に変換する。このアンテ
ナの動作を送信の場合で説明する。矩形導波管(5)か
らのTEsoモードの高周波は9円偏波発生器(3)を
構成している円形導波管のTEs1モードに変換され、
4分の1波長板を経た後は円偏波となっており、これが
円錐ホーン(2)に導かれ、パラボラ(1)を照射して
空間に放射される。この照射において。
Further, the round angle converter (4) smoothly converts the rectangular aperture of the rectangular waveguide (5) and the circular aperture of the circularly polarized wave generator (3). Further, the down converter (6) has a built-in local oscillator and converts it to an intermediate frequency. The operation of this antenna will be explained in the case of transmission. The high frequency of the TEso mode from the rectangular waveguide (5) is converted to the TEs1 mode of the circular waveguide constituting the 9 circularly polarized wave generator (3),
After passing through the quarter-wave plate, it becomes a circularly polarized wave, which is guided to the conical horn (2), irradiates the parabola (1), and is radiated into space. In this irradiation.

矩形導波管(5)は電波の進行方向にあるため、ブロッ
キングが発生する。さらに、この矩形導波管(5)はパ
ラボラ(1)で反射して空間に向う際にもブロッキング
となる。なお、この空間に向う際円錐ホーン(2)。
Since the rectangular waveguide (5) is in the direction of propagation of radio waves, blocking occurs. Furthermore, this rectangular waveguide (5) also causes blocking when it is reflected by the parabola (1) and goes into space. In addition, when heading towards this space, use the conical horn (2).

円偏波発生器(3)、丸角変換器(4)もブロッキング
になるが、このブロッキングの位置がパラボラの中心部
分となるために、その量は矩形導波管(5)の場合に比
べて少い。従って、矩形導波管(5)Kよるブロッキン
グが問題となり、これが利得低下、サイドローブレベル
の上昇といった性能劣化をもたらす。
The circularly polarized wave generator (3) and the round angle converter (4) also experience blocking, but since the position of this blocking is at the center of the parabola, the amount of blocking is smaller than in the case of the rectangular waveguide (5). There aren't many. Therefore, blocking due to the rectangular waveguide (5)K becomes a problem, which causes performance deterioration such as a decrease in gain and an increase in sidelobe level.

このため9矩形導波管(5)を省略できる構成として。Therefore, the configuration is such that the nine rectangular waveguides (5) can be omitted.

第2図に示すアンテナがある。−次放射系を構成してい
る円錐ホーン(2)9円偏波発生器(3)、及び丸角変
換器(4)をスティ(7)で支持している。この場合。
There is an antenna shown in FIG. A conical horn (2), a nine-circularly polarized wave generator (3), and a round angle converter (4), which constitute the -order radiation system, are supported by a stay (7). in this case.

第1図の矩形導波管(5)によるブロッキングがステイ
(7)によるブロッキングに置換ゎる。
The blocking by the rectangular waveguide (5) in FIG. 1 is replaced by blocking by the stay (7).

強風時における一次放射系のゆれによる性能劣化を小さ
くするためには、スティ(7)の幅を太くする必要があ
り、そうするとブロッキングが増加することになり、第
1図の場合と同様に性能劣化を生じる欠点があった。
In order to reduce performance deterioration due to fluctuations in the primary radiation system during strong winds, it is necessary to increase the width of the stay (7), which will increase blocking and cause performance deterioration as in the case of Figure 1. There was a drawback that caused

このようなブロッキングの量が少ない形式として、フ頴
ノキングの位置をパラボラの中心部分としたリアフィー
ド(rear −feed )形がある。′従来のリア
フィード形アンテナを第3図に示す。
As a type with a small amount of blocking, there is a rear-feed type in which the position of the punching is placed at the center of the parabola. 'A conventional rear-feed antenna is shown in Figure 3.

円錐ホーン(2)9円偏波発生器(3)、丸角変換器(
4)。
Conical horn (2), 9 circularly polarized wave generator (3), round angle converter (
4).

ダウンコンバータ(6)、金属板(8)、頂点整合板1
91がパラボラ(1)の中心軸A上に突き出すようにパ
ラボラ(1)で支持されており1円錐ホーン(2)から
放射された電波は金属板(8)で反射され、その反射波
がパラボラ(1)を照射して空間に放射される。従って
Down converter (6), metal plate (8), vertex alignment plate 1
The radio wave emitted from the conical horn (2) is reflected by the metal plate (8), and the reflected wave is (1) and is radiated into space. Therefore.

この場合のブロッキングの主たる要因は金属板(8)と
なる。なお、従来このような円偏波アンテナにおいては
円錐ホーン(2)が用いられることが多く。
The main cause of blocking in this case is the metal plate (8). Note that conventionally, a conical horn (2) is often used in such a circularly polarized antenna.

この場合の頂点整合板(9)として9円錐形のものが用
いられている。ここで、安価なアンテナを得るために、
できるだけ部品の少ない形式が必要であり、従来の装置
では十分とは言えなかった。
In this case, a 9-conical plate is used as the vertex matching plate (9). Here, to get a cheap antenna,
A format with as few parts as possible is required, and conventional equipment was not sufficient.

この発明は、この欠点を除去するため、グリッド形円偏
波発生器と角錐ホーンを用いたもので。
This invention uses a grid-type circularly polarized wave generator and a pyramidal horn to eliminate this drawback.

以下1図面によりこの発明の詳細な説明する。The present invention will be explained in detail below with reference to one drawing.

第4図はこの発明の一実施例であり、この発明の円偏波
パラボラアンテナはパラボラf1)、角錐ホー70組ダ
ウンコンバータ(6)、頂点整合板119.およびグリ
ッド形円偏波発生器1101で構成されている。
FIG. 4 shows an embodiment of the present invention, and the circularly polarized parabolic antenna of the present invention includes a parabola f1), a down converter (6) consisting of 70 pyramidal hoes, and an apex matching plate 119. and a grid-shaped circularly polarized wave generator 1101.

ダウンコンバータ(6)の端子は矩形であり、角錐ホー
ン圓と直結でき、丸角変換は不要となる。直線偏波の電
波が角錐ホーン圓から放射され、グリッド形円偏波発生
器flQlで円偏波に変換され、且つ。
The terminal of the down converter (6) is rectangular and can be directly connected to the pyramidal horn circle, eliminating the need for round-corner conversion. A linearly polarized radio wave is radiated from a pyramidal horn circle, and is converted into a circularly polarized wave by a grid-shaped circularly polarized wave generator flQl.

反射され、パラボラ(1)を照射して空間に放射される
It is reflected, irradiates the parabola (1), and is radiated into space.

第5図はグリッド形円偏波発生器の原理説明図である。FIG. 5 is an explanatory diagram of the principle of a grid-type circularly polarized wave generator.

これは厚さtの誘電体板tillの一面の全面に金属箔
02が張られ、他の面には一定巾の金属箔の直線導線U
□□□が一定の間隔で繰返し並べられたものであり、以
後、前者の面を金属箔面、後者の回をグリッド面と称す
ることとする。上記直線導線u3と45°の角をなす直
線偏波の電界圧が垂直入射するものとすると電界圧のう
ち、上記直線導線と平行な成分は、グリッド面で反射さ
れ、垂直な成分は誘電体板Illを透過し、金属箔面で
反射され、再U、 誘11体板t11Jヲ透過し、結局
、 2t(F−r>の位相変化を受は空間に放射される
。・ ここで、εは誘電体板fillの比誘電率、λは波長で
ある。従ってε、tの値を 4πF−−−’  −−−−−一−−−−−〜−−−−
−−+1)λ−2 となるように選べば、グリッド面で反射された電界と金
属箔面で反射された電界とで円偏波が得られる。
This is a dielectric plate till with a thickness t, with a metal foil 02 stretched over the entire surface of one side, and a straight conductor U made of metal foil of a constant width on the other side.
□□□ are arranged repeatedly at regular intervals, and hereinafter, the former surface will be referred to as the metal foil surface and the latter surface as the grid surface. Assuming that the electric field pressure of a linearly polarized wave forming an angle of 45° with the straight conductor u3 is incident perpendicularly to the straight conductor u3, the component parallel to the straight conductor U3 will be reflected by the grid surface, and the perpendicular component will be reflected by the dielectric. It passes through the plate Ill, is reflected by the metal foil surface, passes through the dielectric plate t11J, and is finally radiated into space with a phase change of 2t(F-r>. Here, ε is the dielectric constant of the dielectric plate fill, and λ is the wavelength. Therefore, the values of ε and t are 4πF−−−′ −−−−−−−−−−−−−−−−
--+1) λ-2, circularly polarized waves can be obtained by the electric field reflected by the grid surface and the electric field reflected by the metal foil surface.

従って、この場合にも角錐ホーン+141から放射され
た電波がグリッド形円偏波発生器(111Iで反射され
た形となる。ここで、第3図の場合は円錐ホーン(2)
であるから円錐形の頂点整合板191を用いたが、いま
の場合は角錐ホーン(141であるから楕円錐形の頂点
整合板(15が必要となる。
Therefore, in this case as well, the radio waves emitted from the pyramidal horn +141 are reflected by the grid-shaped circularly polarized wave generator (111I).
Therefore, a conical vertex matching plate 191 was used, but in this case, since it is a pyramidal horn (141), an elliptic conical vertex matching plate (15) is required.

上記楕円錐形頂点整合板f151と角形ホーンQ41の
配置の関係を第6図に示す。即ち、角錐ホーンIの中心
軸と楕円錐形頂点整合板(15の中心軸とを一致′させ
、かつ角錐ホーンQ41の開口の長辺方向と楕円  ゛
錐形頂点整合板(19の楕円の長径方向とが一致するよ
うに配置している。この頂点整合板は角錐ホーン(14
1のVSWRの改善ばかりでなく1円偏波発生器(1[
Iからの放射パターンのコントロールにも寄与する。
FIG. 6 shows the relationship between the arrangement of the elliptical conical apex matching plate f151 and the square horn Q41. That is, the central axis of the pyramidal horn I and the central axis of the elliptical apex matching plate (15) are aligned, and the long side direction of the opening of the pyramidal horn Q41 is aligned with the long axis of the elliptic apex matching plate (19). The apex alignment plate is a pyramidal horn (14
1 circularly polarized wave generator (1[
It also contributes to controlling the radiation pattern from I.

したがって、場合によっては、第6図の楕円錐形頂点整
合板(151を90°回転させ、楕円の短径方向と角錐
ホーン041の開口の長辺方向とを一致させてもよ0゜ 以上のように、この発明に係る円偏波パラボラアンテナ
においては、丸角変換器が不要であるから安価なアンテ
ナが得られ、また楕円錐形頂点整合板を用いることによ
り、グリッド形円偏波発生器から角錐ホーンへの反射波
の量を少なくできる利点がある。
Therefore, in some cases, the elliptical conical apex matching plate (151) shown in FIG. As described above, the circularly polarized parabolic antenna according to the present invention does not require a round angle converter, so an inexpensive antenna can be obtained, and by using an elliptical conical apex matching plate, a grid-shaped circularly polarized wave generator can be obtained. This has the advantage of reducing the amount of reflected waves from the horn to the pyramidal horn.

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

第1図および第2図は従来の円偏波パラボラアンテナの
概略説明図、第3図は従来のリアフィード形円偏波パラ
ボラアンテナを示す図、第4図はこの発明の一実施例の
概略図、第5図はグリッド形円偏波発生器の原理説明図
、第6図は第4図の部分拡大図である。 図中、(1)はパラボラ、(2)は円錐ホーン、(3)
は円偏波発生器、(4)は丸角変換器、(5)は矩形導
波管。 (6)はダウンコンバータ、(7)はステイ、(8)は
金属板。 (9)は頂点整合板、 110+はグリッド形円偏波発
生器。 C11)は誘電体板、0りは金属箔、’ (13は直線
導線、 (141は角錐ホーン、 +151は楕円錐形
頂点整合板である。 なお図中同一あるいは相当部分には同一符号を付して示
しである。 代理人大岩増雄 第 2 図 第3因 第4 固
1 and 2 are schematic illustrations of a conventional circularly polarized parabolic antenna, FIG. 3 is a diagram showing a conventional rear-feed circularly polarized parabolic antenna, and FIG. 4 is a schematic diagram of an embodiment of the present invention. 5 is a diagram explaining the principle of a grid-type circularly polarized wave generator, and FIG. 6 is a partially enlarged view of FIG. 4. In the figure, (1) is a parabola, (2) is a conical horn, and (3)
is a circularly polarized wave generator, (4) is a round angle converter, and (5) is a rectangular waveguide. (6) is a down converter, (7) is a stay, and (8) is a metal plate. (9) is an apex matching plate, and 110+ is a grid-type circularly polarized wave generator. C11) is a dielectric plate; Agent Masuo Oiwa No. 2 Figure 3 Cause No. 4

Claims (1)

【特許請求の範囲】 パラボラの中心軸に沿って角錐ホーンを配置し。 この前方に反射形の円偏波発生器を設けた円偏波パラボ
ラアンテナにおいて、楕円錐形をした頂点整合板の中心
軸を上記、パラボラの中心軸に一致させ、かつ上記頂点
整合板の楕円形の長径方向と上記角錐ホーンの開口の長
辺方向、または短辺方向とが一致するように、上記頂点
整合板を上記反射形の円偏波発生器の表面に配置したこ
とを特徴とする円偏波パラボラアンテナ。
[Claims] A pyramidal horn is arranged along the central axis of the parabola. In this circularly polarized parabolic antenna with a reflective circularly polarized wave generator installed in the front, the central axis of the elliptical cone-shaped apex matching plate is aligned with the central axis of the parabola, and the ellipse of the apex matching plate is aligned with the central axis of the parabola. The apex matching plate is arranged on the surface of the reflective circularly polarized wave generator so that the long axis direction of the shape coincides with the long side direction or the short side direction of the opening of the pyramidal horn. Circularly polarized parabolic antenna.
JP6868183A 1983-04-19 1983-04-19 Parabolic antenna for circular polarized wave Pending JPS59194513A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6868183A JPS59194513A (en) 1983-04-19 1983-04-19 Parabolic antenna for circular polarized wave

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6868183A JPS59194513A (en) 1983-04-19 1983-04-19 Parabolic antenna for circular polarized wave

Publications (1)

Publication Number Publication Date
JPS59194513A true JPS59194513A (en) 1984-11-05

Family

ID=13380709

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6868183A Pending JPS59194513A (en) 1983-04-19 1983-04-19 Parabolic antenna for circular polarized wave

Country Status (1)

Country Link
JP (1) JPS59194513A (en)

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