JP2825907B2 - Shaped beam antenna - Google Patents
Shaped beam antennaInfo
- Publication number
- JP2825907B2 JP2825907B2 JP2965790A JP2965790A JP2825907B2 JP 2825907 B2 JP2825907 B2 JP 2825907B2 JP 2965790 A JP2965790 A JP 2965790A JP 2965790 A JP2965790 A JP 2965790A JP 2825907 B2 JP2825907 B2 JP 2825907B2
- Authority
- JP
- Japan
- Prior art keywords
- shaped beam
- reflecting mirror
- distribution
- antenna
- gain
- 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.)
- Expired - Lifetime
Links
Landscapes
- Aerials With Secondary Devices (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は、放送衛星等に搭載され、サービスエリアの
形状に適応した放射パターンを有し、1本のホーンと2
枚の反射鏡とで構成されるアンテナの鏡面を修整する成
形ビームアンテナに関する。DETAILED DESCRIPTION OF THE INVENTION (Industrial application field) The present invention is mounted on a broadcast satellite or the like, has a radiation pattern adapted to the shape of a service area, and has one horn and two horns.
The present invention relates to a shaped beam antenna for modifying a mirror surface of an antenna composed of a plurality of reflectors.
(発明の概要) 本発明は、1本の給電ホーンと2枚の反射鏡とから構
成されるアンテナにおいて、遠方界における利得を拘束
条件として主反射鏡の開口面振幅および位相分布を各々
独立に最適化して、主副反射鏡をそれぞれ鏡面修整する
ことによって、その最適化された開口面分布を実現し、
所要の断面形状の成形ビームを得るようにしたものであ
る。(Summary of the Invention) The present invention provides an antenna composed of one feed horn and two reflectors, and independently controls the aperture amplitude and phase distribution of the main reflector under the condition that the gain in the far field is a constraint. By optimizing and modifying the mirror surfaces of the main and sub reflectors, the optimized aperture distribution is realized,
This is to obtain a shaped beam having a required cross-sectional shape.
(従来の技術) 従来、反射鏡アンテナによって成形ビームを得る技術
としては、例えば“鏡面修整複反射鏡アンテナ、特願昭
63−44208号”に示されているように、仮想マルチホー
ンを使って開口面振幅・位相分布を求め、その開口面分
布を実現するように2枚の反射鏡を修整する方法および "Synthesis of shaped−beam reflector antena patter
ns,J.Bergmann,R.C.Brown,P.J.B. Clarricoats,H.Zhou,IEE Proceedings,Vol.135,Pt.H,N
o.1,February 1988,pp.48−53"に示されているように、
2枚の反射鏡の形状を級数で表しておき、遠方界におけ
る目標利得とアンテナ利得との差の4乗和が最小となる
ように、級数の未定係数を最適化して修整鏡面を求める
方法がある。(Prior art) Conventionally, techniques for obtaining a shaped beam by a reflector antenna include, for example, "mirror-modified double reflector antenna,
No. 63-44208 ”, a method of obtaining an aperture amplitude / phase distribution using a virtual multi-horn and modifying two reflecting mirrors to realize the aperture distribution, and“ Synthesis of shaped-beam reflector antena patter
ns, J. Bergmann, RC Brown, PJB Clarricoats, H. Zhou, IEE Proceedings, Vol. 135, Pt. H, N
o.1, February 1988, pp. 48-53 ",
There is a method in which the shapes of two reflecting mirrors are expressed by a series, and a modified mirror surface is obtained by optimizing the undetermined coefficient of the series so as to minimize the sum of squares of the difference between the target gain and the antenna gain in the far field. is there.
あるいは"A Method for Producing a Shaped contour
Radiation Pattern Using a Single Shaped Reflector
and a Single feel,A,R,Cherrettee,S..W.Lee,R.J.Aco
sta,IEEI Trans.Antennas&Propag.,Vol.37,No.6,June.
1989,pp.698−706"に示されているように、1枚の反射
鏡を使いホーンで与えられる振幅分布に対して、遠方界
における目標利得とアンテナ利得との差の2乗和が最小
となる位相分布を求め、その位相分布を実現するように
反射鏡を修整する方法等がある。Or "A Method for Producing a Shaped contour
Radiation Pattern Using a Single Shaped Reflector
and a Single feel, A, R, Cherrettee, S..W.Lee, RJAco
sta, IEEI Trans.Antennas & Propag., Vol.37, No.6, June.
1989, pp. 698-706 ", the sum of squares of the difference between the target gain and the antenna gain in the far field is minimum for the amplitude distribution given by the horn using one reflector. There is a method of obtaining a phase distribution that satisfies the following condition, and modifying the reflecting mirror so as to realize the phase distribution.
(発明が解決しようとする課題) 従来の仮想マルチホーンを使う方法では、主反射鏡に
急激な段差を生じ、アンテナ製作上または熱歪による放
射パターンの変化等の問題点があった。また、1枚の反
射鏡の鏡面修整では、位相分布のみの制御であるため
に、ビーム成形には限度があった。(Problems to be Solved by the Invention) In the conventional method using the virtual multi-horn, there is a problem that an abrupt step occurs in the main reflecting mirror, and a radiation pattern changes due to antenna fabrication or thermal distortion. Further, in the mirror surface modification of one reflecting mirror, since only the phase distribution is controlled, there is a limit in beam shaping.
本発明は、上述の点に鑑み、従来技術の問題点を有効
に解決し、2枚の反射鏡の鏡面修整が位相のみでなく、
振幅分布も制御されて、所要のサービスエリアの形状に
応じて、より高利得で覆う成形ビームアンテナを得るこ
とおよび主反射鏡面の段差が解消され滑らかな形状を有
する成形ビームアンテナを提供することを目的とする。The present invention has been made in view of the above points, and effectively solves the problems of the related art.
The amplitude distribution is also controlled to obtain a shaped beam antenna that covers with higher gain in accordance with the shape of the required service area, and to provide a shaped beam antenna having a smooth shape by eliminating the steps of the main reflecting mirror surface. Aim.
(課題を解決するための手段) このような目的を達成するために、本発明は、給電ホ
ーンと副反射鏡および主反射鏡とを順次に設けた成形ビ
ームアンテナにおいて、所要の成形ビームの断面形状に
応じて前記主反射鏡および副反射鏡の鏡面の形状を修整
し、前記成形ビームの断面形状に応じた前記主反射鏡上
の振幅分布および位相分布が遠方界における目標利得お
よびアンテナ利得の差の2乗和が最小となる振幅分布お
よび位相分布と等しくなるように鏡面を修整することを
特徴とする。(Means for Solving the Problems) In order to achieve such an object, the present invention relates to a shaped beam antenna having a feed horn, a sub-reflecting mirror, and a main reflecting mirror sequentially provided. The shape of the mirror surface of the main reflecting mirror and the sub-reflecting mirror is modified according to the shape, and the amplitude distribution and the phase distribution on the main reflecting mirror according to the cross-sectional shape of the shaped beam have the target gain and the antenna gain in the far field. The mirror surface is modified so that the sum of squares of the difference becomes equal to the amplitude distribution and the phase distribution that minimize the difference.
(作用) このような技術手段により、本発明は、1本の給電ホ
ーンと2枚の反射鏡とから構成されるアンテナにおける
遠方界における利得を拘束条件として主反射鏡の開口面
振幅、位相分布を各々独立に最適化し、求められた開口
面分布が主幅反射鏡をそれぞれ鏡面修整することによっ
て実現され、所要の断面形状の成形ビームが得られる。(Operation) By such technical means, the present invention provides an aperture plane amplitude and a phase distribution of a main reflector under the condition that a gain in a far field of an antenna composed of one feed horn and two reflectors is a constraint. Are independently optimized, and the obtained aperture distribution is realized by modifying the mirrors of the main width reflecting mirrors, and a shaped beam having a required cross-sectional shape is obtained.
(実施例) 次に、本発明の実施例を図面に基づき、詳細に説明す
る。(Example) Next, an example of the present invention will be described in detail with reference to the drawings.
第1図は東径110度の静止軌道上の衛星から見た日本
地図と利得拘束点である。1は遠方界における利得拘束
点で、2は東径110度の静止軌道から見た日本地図で、
この日本地図2上に利得の拘束点1が重ね書きされ、本
実施例では103点の拘束点が設けられている。Fig. 1 shows a map of Japan and a gain constraint point as viewed from a satellite in a geosynchronous orbit of 110 ° east diameter. 1 is a gain constraint point in the far field, 2 is a map of Japan viewed from a geosynchronous orbit of 110 degrees east,
The constraint point 1 of the gain is overwritten on this Japan map 2, and in this embodiment, 103 constraint points are provided.
第2図は本発明における成形ビームアンテナの一実施
例の概略構成図を示す。成形ビームアンテナ10は、給電
ホーン3、副反射鏡4、主反射鏡5から構成されてい
る。6は給電ホーン3から放射される電波の軌跡であ
る。主反射鏡5の開口面上の位相分布を求めるために、
振幅分布が一様に分布されたと仮定して、遠方界の拘束
点1における目標利得とアンテナ利得との差の2乗和が
最小になるように位相分布を最適化する。この際、位相
の急激な変化を避けるために、位相分布の最適化の過程
において、開口面格子点の隣り同志の位相の差が所要の
値以上にならないたように制限が設けられている。FIG. 2 is a schematic configuration diagram of an embodiment of the shaped beam antenna according to the present invention. The shaped beam antenna 10 includes a feed horn 3, a sub-reflector 4, and a main reflector 5. Reference numeral 6 denotes a locus of a radio wave radiated from the feeding horn 3. In order to obtain the phase distribution on the opening surface of the main reflecting mirror 5,
Assuming that the amplitude distribution is uniformly distributed, the phase distribution is optimized so that the sum of squares of the difference between the target gain and the antenna gain at the far-field constraint point 1 is minimized. At this time, in order to avoid a sudden change in the phase, in the process of optimizing the phase distribution, a limit is set so that the phase difference between adjacent ones of the aperture lattice points does not exceed a required value.
第3図は第2図における主反射鏡開口面において求め
た位相分布図を示す。この位相分布は、本実施例では開
口面格子点の隣り同志の位相差が89度以上にならないよ
うに制限されている。FIG. 3 shows a phase distribution diagram obtained at the opening surface of the main reflecting mirror in FIG. In this embodiment, the phase distribution is restricted so that the phase difference between adjacent aperture lattice points does not exceed 89 degrees.
第4図は同じく主反射鏡開口面の振幅分布図を示す。
主反射鏡5の開口面上の振幅分布を求めるために、上述
のように求められた位相分布を固定して、遠方界の拘束
点1における目標利得とアンテナ利得との差の2乗和
が、最小値になるように振幅分布を最適化する。第4図
の振幅の大きさは相対値で,dB単位で示されている。FIG. 4 shows an amplitude distribution diagram of the aperture surface of the main reflecting mirror.
In order to determine the amplitude distribution on the opening surface of the main reflecting mirror 5, the phase distribution determined as described above is fixed, and the sum of squares of the difference between the target gain and the antenna gain at the far-field constraint point 1 is calculated as , The amplitude distribution is optimized to be the minimum value. The magnitude of the amplitude in FIG. 4 is a relative value and is shown in dB.
第5図は第3図の位相分布と第4図の振幅分布とを組
み合わせて求めた放射パターンを示す。主反射鏡5の開
口面の直径が2.3m(第2図)、周波数が12GHzの場合の
放射パターンがdBi単位の絶対利得で、東径110度の静止
軌道からみた日本地図2の上に重ね書きされている。成
形ビームアンテナ10は、最適化された主反射鏡5の開口
面上の位相分布および振幅分布が1本の給電ホーン3
と、主副反射鏡4,5の鏡面修整とにより実現されてい
る。すなわち、副反射鏡4を修整して、給電ホーン3に
て決定される同心円状の放射ビームを、先に求められた
振幅分布に変換し、次に主反射鏡5の開口面を修整し
て、位相を調整し、先に求められた位相分布を実現する
ものである。FIG. 5 shows a radiation pattern obtained by combining the phase distribution of FIG. 3 and the amplitude distribution of FIG. When the diameter of the opening surface of the main reflector 5 is 2.3m (Fig. 2) and the frequency is 12GHz, the radiation pattern is an absolute gain in dBi unit and is superimposed on the Japanese map 2 viewed from a geosynchronous orbit of 110 ° east diameter. It is written. The shaped beam antenna 10 includes a feed horn 3 having one phase distribution and one amplitude distribution on the aperture surface of the optimized main reflecting mirror 5.
And the surface modification of the main and sub-reflecting mirrors 4 and 5. That is, the sub-reflector 4 is modified to convert the concentric radiation beam determined by the feed horn 3 into the amplitude distribution previously determined, and then the aperture of the main reflector 5 is modified. , The phase is adjusted to realize the phase distribution previously obtained.
(発明の効果) 以上に説明したように、本発明の成形ビームアンテナ
は、1本の給電ホーンと2枚の反射鏡とから構成される
アンテナの遠方界における利得を拘束条件として主反射
鏡の開口面振幅、位相分布を各々独立に最適化し、求め
た開口面分布を2枚の主副反射鏡を鏡面修整することに
よって実現し、所要の断面形状の成形ビームを得ること
により、従来技術の問題点が有効に解決され、従来の鏡
面修整された成形ビームアンテナに比較して、所要の範
囲がより高利得で覆われた放射パターンが得られ、2枚
の反射鏡を鏡面修整し、位相分布のみでなく、振幅分布
も調整して、複雑な形状の成形ビームを得ることおよび
主反射鏡面の段差を解消し滑らかな形状を有する等の効
果を奏する。(Effects of the Invention) As described above, the shaped beam antenna of the present invention uses the main reflector with the gain in the far field of the antenna composed of one feed horn and two reflectors as a constraint. The aperture plane amplitude and phase distribution are independently optimized, and the obtained aperture plane distribution is realized by modifying the surface of the two main and sub-reflecting mirrors to obtain a shaped beam having a required cross-sectional shape. The problem is effectively solved, and a radiation pattern in which the required area is covered with higher gain is obtained as compared with the conventional mirror-shaped shaped beam antenna. By adjusting not only the distribution but also the amplitude distribution, it is possible to obtain a shaped beam having a complicated shape, to eliminate a step on the main reflecting mirror surface, and to obtain a smooth shape.
第1図は東径110度の静止軌道上の衛星から見た日本地
図と利得拘束点、第2図は本発明における成形ビームア
ンテナの一実施例の概略構成図、第3図は第2図におけ
る主反射鏡開口面において求めた位相分布図、第4図は
同じく主反射鏡開口面の振幅分布図、第5図は第3図の
位相分布と第4図の振幅分布とを組み合わせて求めた放
射パターン図である。 1……利得拘束点 2……日本地図 3……給電ホーン 4……副反射鏡 5……主反射鏡 6……電波軌跡 10……成形ビームアンテナ1 is a map of Japan and a gain constraint point as viewed from a satellite in a geosynchronous orbit of 110 ° east diameter, FIG. 2 is a schematic configuration diagram of an embodiment of a shaped beam antenna according to the present invention, and FIG. 3 is FIG. 4, the phase distribution diagram obtained at the main reflecting mirror aperture surface, FIG. 4 is also the amplitude distribution diagram of the main reflecting mirror aperture surface, and FIG. 5 is obtained by combining the phase distribution of FIG. 3 and the amplitude distribution of FIG. FIG. 1 Gain restriction point 2 Map of Japan 3 Feeding horn 4 Sub-reflector 5 Main reflector 6 Radio track 10 Shaped beam antenna
Claims (1)
順次に設けた成形ビームアンテナにおいて、所要の成形
ビームの断面形状に応じて前記主反射鏡および副反射鏡
の鏡面の形状を修整し、前記成形ビームの断面形状に応
じた前記主反射鏡上の振幅分布および位相分布が遠方界
における目標利得およびアンテナ利得の差の2乗和が最
小となる振幅分布および位相分布と等しくなるように鏡
面を修整することを特徴とする成形ビームアンテナ。1. A shaped beam antenna having a power feeding horn, a sub-reflecting mirror and a main reflecting mirror sequentially provided, wherein the shapes of the mirror surfaces of the main reflecting mirror and the sub-reflecting mirror are modified in accordance with the required cross-sectional shape of the shaped beam. The amplitude distribution and the phase distribution on the main reflecting mirror according to the cross-sectional shape of the shaped beam are equal to the amplitude distribution and the phase distribution at which the sum of squares of the difference between the target gain and the antenna gain in the far field is minimized. A shaped beam antenna characterized by modifying the mirror surface.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2965790A JP2825907B2 (en) | 1990-02-13 | 1990-02-13 | Shaped beam antenna |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2965790A JP2825907B2 (en) | 1990-02-13 | 1990-02-13 | Shaped beam antenna |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03235506A JPH03235506A (en) | 1991-10-21 |
| JP2825907B2 true JP2825907B2 (en) | 1998-11-18 |
Family
ID=12282188
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2965790A Expired - Lifetime JP2825907B2 (en) | 1990-02-13 | 1990-02-13 | Shaped beam antenna |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2825907B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2734264B2 (en) * | 1991-11-29 | 1998-03-30 | 日本電気株式会社 | Mirror modified antenna |
| JP3322897B2 (en) * | 1991-11-29 | 2002-09-09 | 株式会社東芝 | Mirror modified antenna |
| WO2020110375A1 (en) * | 2018-11-27 | 2020-06-04 | 三菱電機株式会社 | Antenna device and antenna adjustment method |
-
1990
- 1990-02-13 JP JP2965790A patent/JP2825907B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH03235506A (en) | 1991-10-21 |
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