JPH04575Y2 - - Google Patents

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Publication number
JPH04575Y2
JPH04575Y2 JP8846884U JP8846884U JPH04575Y2 JP H04575 Y2 JPH04575 Y2 JP H04575Y2 JP 8846884 U JP8846884 U JP 8846884U JP 8846884 U JP8846884 U JP 8846884U JP H04575 Y2 JPH04575 Y2 JP H04575Y2
Authority
JP
Japan
Prior art keywords
reflector
sub
focal point
main
primary radiator
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
Application number
JP8846884U
Other languages
Japanese (ja)
Other versions
JPS615010U (en
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 filed Critical
Priority to JP8846884U priority Critical patent/JPS615010U/en
Publication of JPS615010U publication Critical patent/JPS615010U/en
Application granted granted Critical
Publication of JPH04575Y2 publication Critical patent/JPH04575Y2/ja
Granted legal-status Critical Current

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Description

【考案の詳細な説明】 〔考案の技術分野〕 この考案はマイクロ波中継回線等に用いられる
アンテナ装置の改良に関するものである。
[Detailed Description of the Invention] [Technical Field of the Invention] This invention relates to an improvement of an antenna device used in a microwave relay line or the like.

〔従来の技術〕[Conventional technology]

従来、アンテナ装置には、第1図に示すよう
に、位相中心F0を有する一次放射器1、一次放
射器の位相中心F0を共有し、さらに、焦点F1
有する第一副反射鏡2、焦点F1を共有し、さら
に焦点F2を有する第ニ副反射鏡3および焦点F2
を共有する回転放物面鏡からなる主反射鏡4より
構成されているものがある。
Conventionally, as shown in FIG. 1, an antenna device includes a primary radiator 1 having a phase center F 0 , a first sub-reflector sharing the phase center F 0 of the primary radiator, and further having a focal point F 1 . 2. A second sub-reflector 3 that shares the focal point F 1 and further has a focal point F 2 and the focal point F 2
Some mirrors are composed of a main reflecting mirror 4 that is a parabolic mirror of revolution that shares the same characteristics.

図中、M1,M2,Mは、一次放射器1の中心軸
に沿つて、放射される光線5が各鏡面に順に当る
点である。
In the figure, M 1 , M 2 , and M are points along the central axis of the primary radiator 1 at which the emitted light ray 5 hits each mirror surface in turn.

このアンテナは第1図の構成図から明らかなよ
うに、幾何光学的に設計されているために、幾何
光学が成立する周波数領域やD/λ(D:鏡面の
開口径、λ:自由空間波長)が非常に大きいアン
テナでは、広帯域にわたつて開口能率が一定とな
る。しかしながら開口径が10λ以下の小口径の副
反射鏡を有するアンテナでは、電波が波動的な広
がりを有するため、第一副反射鏡1と第ニ副反射
鏡2の共通の焦点であるF1はもはや共焦点とは
なり得ず、第一副反射鏡1の焦点は、見かけ上、 M2F1′<M2F1 (1) が成立するF1′となり、この焦点F1′から図中点
線で示す電波6が放射されるように見える。この
ため、図中、第一副反射鏡2を照射する電波のう
ち点線で囲まれる部分の電波6は、上記第一副反
射鏡2で反射されて、第ニ副反射鏡3の全面を照
射するが、第一副反射鏡2を照射する電波のうち
点線の外側を通る電波は、反射されて第ニ副反射
鏡3の方向へ進むが全てスピルオーバ成分とな
り、広角放射特性の劣化や、開口能率の低下をも
たらすという欠点があつた。
As is clear from the configuration diagram in Figure 1, this antenna is designed based on geometric optics, so the frequency range where geometric optics holds true is D/λ (D: mirror aperture diameter, λ: free space wavelength). ) is very large, the aperture efficiency remains constant over a wide band. However, in an antenna that has a small-diameter sub-reflector with an aperture diameter of 10λ or less, the radio waves have a wave-like spread, so F 1 , which is the common focal point of the first sub-reflector 1 and the second sub-reflector 2, is It can no longer be confocal, and the focal point of the first sub-reflector 1 is apparently F 1 ', where M 2 F 1 '< M 2 F 1 (1) holds, and from this focal point F 1 ', the Radio waves 6 indicated by the dotted line appear to be emitted. Therefore, in the figure, among the radio waves irradiating the first sub-reflector 2, the radio waves 6 in the portion surrounded by the dotted line are reflected by the first sub-reflector 2 and irradiate the entire surface of the second sub-reflector 3. However, among the radio waves that irradiate the first sub-reflector 2, the radio waves that pass outside the dotted line are reflected and travel toward the second sub-reflector 3, but they all become spillover components, causing deterioration of wide-angle radiation characteristics and aperture The drawback was that it resulted in a decrease in efficiency.

又、第ニ副反射鏡3で反射した電波6は、主反
射鏡へ向うかスネルの法則により、第ニ副反射鏡
3の見かけ上の焦点F2′で絞られ、幾何光学的に
決定された主反射鏡の領域より、狭い部分を照射
するため、主反射鏡を有効に利用しないことにな
り、開口能率の低下をもたらすという欠点があつ
た。
Also, the radio wave 6 reflected by the second sub-reflector 3 is focused on the apparent focal point F 2 ' of the second sub-reflector 3, determined by geometric optics, according to Snell's law, whether it heads toward the main reflector or not. Since a narrower area is irradiated than the area of the main reflecting mirror, the main reflecting mirror is not used effectively, resulting in a reduction in aperture efficiency.

〔考案の概要〕[Summary of the idea]

この考案は、これらの欠点を解決するため、第
一副反射鏡2および第ニ副反射鏡3の焦点が共焦
点とならないように鏡面系を構成したものであ
り、以下図面に従つて詳細に説明する。
In order to solve these drawbacks, this invention has a mirror system configured so that the focal points of the first sub-reflector 2 and the second sub-reflector 3 do not become confocal, and will be described in detail below according to the drawings. explain.

〔考案の実施例〕[Example of idea]

第2図は、この考案の一実施例を示すもので、
1は一次放射器となる円錐ホーン、2は回転二次
曲面鏡からなる第一副反射鏡、3は回転二次曲面
鏡からなる第ニ副反射鏡、4は回転放物面鏡から
なる主反射鏡である。
Figure 2 shows an example of this invention.
1 is a conical horn serving as a primary radiator, 2 is a first sub-reflector consisting of a rotating quadratic curved mirror, 3 is a second sub-reflector consisting of a rotating quadratic curved mirror, and 4 is a main sub-reflector consisting of a rotating parabolic mirror. It is a reflective mirror.

F0,F1′は第一副反射鏡2の焦点であり、F0
円錐ホーンの位相中心でもある。さらに、F1
F2は第ニ副反射鏡の焦点で、F2は主反射鏡4の
焦点でもある。第2図において、幾何光学的に考
えた場合、円錐ホーン1の中心軸に沿つて放射さ
れる光線5が、それぞれの反射鏡に当たる点を順
にM1,M2,Mとするとき、F0,F1,F1′,F2
M1,M2,Mが同一平面内にあり、しかも
12→,F1′M2→が同一線上にあるものとする。
F 0 and F 1 ' are the focal points of the first sub-reflector 2, and F 0 is also the phase center of the conical horn. Furthermore, F 1 ,
F 2 is the focus of the second sub-reflector, and F 2 is also the focus of the main reflector 4. In FIG. 2, when considered from the perspective of geometrical optics, when the points at which the light ray 5 emitted along the central axis of the conical horn 1 hits each reflecting mirror are M 1 , M 2 , and M in order, then F 0 , F 1 , F 1 ′, F 2 ,
It is assumed that M 1 , M 2 , and M are on the same plane, and that F 1 M 2 → and F 1 'M 2 → are on the same line.

このアンテナの第一副反射鏡2の形状は円錐ホ
ーン1の位相中心F0から放射された電波6が電
波の波動性を考慮して、等価的に、第ニ副反射鏡
3の焦点F1から放射されるように決定されてい
る。
The shape of the first sub-reflector 2 of this antenna is such that the radio wave 6 radiated from the phase center F 0 of the conical horn 1 is equivalently focused at the focal point F 1 of the second sub-reflector 3 in consideration of the wave nature of the radio wave. It is determined that the radiation will be emitted from

すなわち、上記第一副反射鏡2の焦点F1′は、
第(2)式を満足するように決定されている。
That is, the focal point F 1 ' of the first sub-reflector 2 is
It is determined to satisfy equation (2).

1′M2―>F12― (2) 以上のように構成されたアンテナ装置におい
て、円錐ホーン1の位相中心F0から放射された
電波6は、第一副反射鏡2を経由して、効率よく
第ニ副反射鏡3を照射するため、上記第ニ副反射
鏡3からのスピルオーバ成分はほとんどなくなり
アンテナの低サイドローブ化や高能率化を図るこ
とができる。又、円錐ホーン1の位相中心F0
ら放射された電波6は、等価的に第ニ副反射鏡3
の焦点F1から放射されるため、スネルの法則に
より反射後上記第ニ副反射鏡3および主反射鏡4
の共焦点F2で絞られる。従つて、主反射鏡4を
効率よく照射することができ、アンテナの高能率
化を図ることができる。
F 1 'M 2 -> F 1 M 2 - (2) In the antenna device configured as above, the radio wave 6 radiated from the phase center F 0 of the conical horn 1 passes through the first sub-reflector 2. As a result, the second sub-reflector 3 is efficiently irradiated, so that the spillover component from the second sub-reflector 3 is almost eliminated, making it possible to achieve low side lobes and high efficiency of the antenna. Furthermore, the radio wave 6 radiated from the phase center F 0 of the conical horn 1 is equivalently transmitted to the second sub-reflector 3.
Since it is radiated from the focal point F 1 of
focused at confocal F2 . Therefore, the main reflecting mirror 4 can be efficiently irradiated, and the efficiency of the antenna can be increased.

なお、以上の説明では、一次放射器に円錐ホー
ン1を使用したが、本考案はこれに限らず、中心
軸をもついかなる一次放射器であつてもよい。
In the above description, the conical horn 1 is used as the primary radiator, but the present invention is not limited to this, and any primary radiator having a central axis may be used.

又、以上は主反射鏡4が下向きの場合を説明し
たが、上向きの場合でも本考案を適用することが
できる。
Moreover, although the case where the main reflecting mirror 4 is facing downward has been described above, the present invention can be applied even when the main reflecting mirror 4 is facing upward.

〔考案の効果〕[Effect of idea]

以上のように、この考案によれば、副反射鏡か
らのスピルオーバ成分が低減でき、しかも主反射
鏡を効率よく照射するため、高能率、低サイドロ
ーブのアンテナが実現できるという利点を有す
る。
As described above, this invention has the advantage that spillover components from the sub-reflector can be reduced and the main reflector can be efficiently irradiated, making it possible to realize an antenna with high efficiency and low side lobes.

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

第1図は従来のアンテナ装置の構成図、第2図
はこの考案の実施例を示すアンテナ装置の構成図
である。 図中、1は一次放射器、2は第一副反射鏡、3
は第ニ副反射鏡、4は主反射鏡、5は光線、6は
電波である。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てある。
FIG. 1 is a block diagram of a conventional antenna device, and FIG. 2 is a block diagram of an antenna device showing an embodiment of this invention. In the figure, 1 is the primary radiator, 2 is the first sub-reflector, and 3
is a second sub-reflector, 4 is a main reflector, 5 is a light beam, and 6 is a radio wave. It should be noted that the same or corresponding parts in the figures are indicated by the same reference numerals.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 一次放射器と主反射鏡の間に2枚の副反射鏡を
配し、主反射鏡に近い副反射鏡によつて、電波が
主反射鏡の焦点に絞られるように構成されたアン
テナ装置において、一次放射器に近い副反射鏡を
R1、他方の副反射鏡をR2、一次放射器の位相中
心に一致する副反射鏡R1の一方の焦点をF0、他
方の焦点をF1′、副反射鏡R2の主反射鏡との共焦
点をF2、他方の焦点をF1として幾何光学的に考
えたとき、一次放射器の中心軸に沿つて放射され
る光線が2枚の副反射鏡R1,R2に当る点を順に
M1,M2、主反射鏡Rに当る点をMとすると、
F0,F1,F1′,F2,M1,M2,Mが同一面内にあ
り、且つF12→とF1′M2→が同一線上にあつて
1′M2―>F12―なることを特徴とするアンテナ
装置。
In an antenna device configured such that two sub-reflectors are arranged between a primary radiator and a main reflector, and the sub-reflector near the main reflector focuses radio waves on the focal point of the main reflector. , a secondary reflector close to the primary radiator
R 1 , the other sub-reflector R 2 , one focal point of the sub-reflector R 1 that coincides with the phase center of the primary radiator is F 0 , the other focal point is F 1 ′, the main reflection of the sub-reflector R 2 When considering geometric optics with the confocal point with the mirror as F 2 and the other focal point as F 1 , the light rays emitted along the central axis of the primary radiator are reflected on the two sub-reflectors R 1 and R 2. Correct points in order
M 1 , M 2 , and if the point corresponding to the main reflecting mirror R is M, then
F 0 , F 1 , F 1 ′, F 2 , M 1 , M 2 , M are in the same plane, and F 1 M 2 → and F 1 ′M 2 → are on the same line, and F 1 ′M 2 -> F 1 M 2 - An antenna device characterized by the following.
JP8846884U 1984-06-14 1984-06-14 antenna device Granted JPS615010U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8846884U JPS615010U (en) 1984-06-14 1984-06-14 antenna device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8846884U JPS615010U (en) 1984-06-14 1984-06-14 antenna device

Publications (2)

Publication Number Publication Date
JPS615010U JPS615010U (en) 1986-01-13
JPH04575Y2 true JPH04575Y2 (en) 1992-01-09

Family

ID=30641635

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8846884U Granted JPS615010U (en) 1984-06-14 1984-06-14 antenna device

Country Status (1)

Country Link
JP (1) JPS615010U (en)

Also Published As

Publication number Publication date
JPS615010U (en) 1986-01-13

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