JPS6151802B2 - - Google Patents

Info

Publication number
JPS6151802B2
JPS6151802B2 JP14465780A JP14465780A JPS6151802B2 JP S6151802 B2 JPS6151802 B2 JP S6151802B2 JP 14465780 A JP14465780 A JP 14465780A JP 14465780 A JP14465780 A JP 14465780A JP S6151802 B2 JPS6151802 B2 JP S6151802B2
Authority
JP
Japan
Prior art keywords
reflector
sub
mirror surface
main
waves
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
JP14465780A
Other languages
Japanese (ja)
Other versions
JPS5768905A (en
Inventor
Nobuo Nakajima
Yoshitaro Shimanuki
Shuji Urasaki
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
Nippon Telegraph and Telephone Corp
Original Assignee
Mitsubishi Electric Corp
Nippon Telegraph and Telephone 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, Nippon Telegraph and Telephone Corp filed Critical Mitsubishi Electric Corp
Priority to JP14465780A priority Critical patent/JPS5768905A/en
Publication of JPS5768905A publication Critical patent/JPS5768905A/en
Publication of JPS6151802B2 publication Critical patent/JPS6151802B2/ja
Granted 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
    • H01Q19/191Combinations 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 the primary active element uses one or more deflecting surfaces, e.g. beam waveguide feeds

Landscapes

  • Aerials With Secondary Devices (AREA)

Description

【発明の詳細な説明】 この発明は反射鏡アンテナの広角度方向におけ
るサイドロープレベルの低減を図るようにした反
射鏡アンテナ装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a reflector antenna device designed to reduce the side rope level of a reflector antenna in a wide angle direction.

従来のこの種の反射鏡アンテナ装置は第1図に
示すように、給電ホーン1、副反射鏡A2、副反
射鏡B3および主反射鏡4で構成されていた。副
反射鏡A2,B3は回転2次曲面で、主反射鏡4
は回転放物面である。給電ホーン1の位相中心F
からの電波のうち、ホーン軸に沿う電波は図中、
一点鎖線で示すように各鏡面上の点、A,B,C
を経て空間に放射される。この放射の方向に大部
分の電波が向かい、主ビームを形成するが、一部
は鏡面のエツヂに向かつて回折し、主ビームから
かなり離れた放射方向、すなわち広角度方向に向
かい電波干渉の一因となる。この様子も第1図に
示す。ここでは、副反射鏡A2のエツヂ上の点
A1の場合について示す。この点A1に入射する電
波は点Fから球面波ばかりでなく、副反射鏡B3
のエツヂ上の点B1,B2からの回折波も入射す
る。これらの入射波によつて回折波が生じて広角
放射特性が劣化する欠点があつた。
As shown in FIG. 1, a conventional reflector antenna device of this type includes a feeding horn 1, a sub-reflector A2, a sub-reflector B3, and a main reflector 4. The sub-reflecting mirrors A2 and B3 are rotational quadratic curved surfaces, and the main reflecting mirror 4
is a paraboloid of revolution. Phase center F of feeding horn 1
Among the radio waves from , the radio waves along the horn axis are shown in the figure.
Points A, B, C on each mirror surface as shown by the dashed line
is radiated into space. Most of the radio waves head in the direction of this radiation and form the main beam, but some of them are diffracted towards the edges of the mirror surface and head in the radiation direction that is quite far away from the main beam, i.e. in the wide angle direction, where they eliminate radio wave interference. cause This situation is also shown in FIG. Here, a point on the edge of sub-reflector A2
The case of A1 is shown. The radio waves incident on this point A1 are not only spherical waves from point F, but also from the sub-reflector B3.
Diffracted waves from points B 1 and B 2 on the edge of are also incident. These incident waves generate diffracted waves, which has the disadvantage of deteriorating wide-angle radiation characteristics.

この発明は主反射鏡と給電ホーン側の副反射鏡
とを滑らかな鏡面で連結して一体化することによ
り主、副反射鏡のエツヂ部による回折波を除去し
て広角放射特性を改善するようにした反射鏡アン
テナ装置を提供するものである。以下、図面につ
いて詳細に説明する。
This invention improves wide-angle radiation characteristics by connecting and integrating the main reflecting mirror and the sub-reflecting mirror on the feed horn side with a smooth mirror surface, thereby removing diffracted waves due to the edge portions of the main and sub-reflecting mirrors. The present invention provides a reflector antenna device having the following features. The drawings will be described in detail below.

第2図はこの発明の一実施例を示す図で、図に
おいて、1は給電ホーン、2は副反射鏡A、3は
副反射鏡B、4は主反射鏡、5は給電ホーン1に
続く副反射鏡A2と主反射鏡4との間に設けた接
続鏡面である。ここでも、点Fは給電ホーン1の
位相中心、副反射鏡A2、B3は回転2次曲面で
あるが第1図とは鏡面の種類を違えている。ま
た、主反射鏡4は回転放物面である。接続鏡面5
は次のようにして定める。ここでは図中に示す、
接続鏡面5の断面上の曲線A1D1C1の求め方を示
す。点D1を点A1,C1のほぼ中心の点とする。領
域A1D1に入射する電波は先に述べたように、点
F,B1およびB2からの電波が考えられる。この
場合、反射鏡系のパラメータの選定によつて変化
するが、点Fからの入射波のレベルが一番高いと
考えられるので、図中、点線で示すように、点F
からの入射波が主ビームの近い角度方向に向かう
ように鏡面A1D1を設計できる。また、同様に鏡
面C1D1に関しては点B2からの入射波が主ビーム
近傍に放射するように設計できる。この鏡面設計
において、点C1,D1,A1において、エツヂを形
成することになるが、このエツヂの形状は従来に
比べて急激でなく、ほぼ平坦となつているため、
その回折波は無視できる。これを第3図によつて
説明する。図において、6は回転対称鏡面、7は
平板である。この鏡面6と平板7とでエツヂ
E1,E2を形成し、その角度をとするこれらの
エツヂに平面波が入射した場合のエツヂからの回
折波レベルを第4図に示す。このように、が小
さいと回折波レベルを無視できることがわかる。
FIG. 2 is a diagram showing an embodiment of the present invention. In the figure, 1 is a feed horn, 2 is a sub-reflector A, 3 is a sub-reflector B, 4 is a main reflector, and 5 is a continuation of the feed horn 1. This is a connecting mirror surface provided between the sub-reflector A2 and the main reflector 4. Again, point F is the phase center of the feeding horn 1, and the sub-reflectors A2 and B3 are rotational quadratic curved surfaces, but the types of mirror surfaces are different from those in FIG. Further, the main reflecting mirror 4 is a paraboloid of revolution. Connection mirror surface 5
is determined as follows. Here, shown in the figure,
The method of obtaining the curve A 1 D 1 C 1 on the cross section of the connecting mirror surface 5 will be shown. Let point D 1 be approximately the center of points A 1 and C 1 . As mentioned above, radio waves incident on the area A 1 D 1 are considered to be radio waves from points F, B 1 and B 2 . In this case, the level of the incident wave from point F is considered to be the highest, although it changes depending on the selection of the parameters of the reflecting mirror system, so the level of the incident wave from point F is
The mirror surface A 1 D 1 can be designed so that the incident wave from A 1 D 1 is directed toward an angular direction close to the main beam. Similarly, the mirror surface C 1 D 1 can be designed so that the incident wave from point B 2 is radiated near the main beam. In this mirror design, edges are formed at points C 1 , D 1 , and A 1 , but the shape of these edges is not as sharp as in the past and is almost flat, so
The diffracted waves can be ignored. This will be explained with reference to FIG. In the figure, 6 is a rotationally symmetrical mirror surface, and 7 is a flat plate. This mirror surface 6 and flat plate 7 create an edge
FIG. 4 shows the level of diffracted waves from the edges when a plane wave is incident on these edges forming E 1 and E 2 and having the angles. In this way, it can be seen that when is small, the diffracted wave level can be ignored.

第5図に接続鏡面5の詳細を示す。断面曲線上
における点A1,C1における接線方向から測つた
接続鏡面5の角度acは第4図から許容レベ
ル内になるように決定すればよい。断面曲線上以
外の接続鏡面5も同様の考え方で設計できる。
FIG. 5 shows details of the connecting mirror surface 5. The angles a and c of the connecting mirror surface 5 measured from the tangential direction at points A 1 and C 1 on the cross-sectional curve may be determined from FIG. 4 so as to be within the permissible level. Connecting mirror surfaces 5 other than those on the cross-sectional curve can also be designed using the same concept.

以上のようにこの発明によれば副反射鏡A2、
主反射鏡4の一部エツヂの回折波をほぼ取り除く
ことができ、広角放射特性を改善できる利点があ
る。
As described above, according to the present invention, the sub-reflector A2,
This has the advantage that the diffracted waves on some edges of the main reflecting mirror 4 can be almost eliminated, and the wide-angle radiation characteristics can be improved.

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

第1図は従来の反射鏡アンテナ装置の概略構成
図、第2図はこの発明の一実施例を示す概略構成
図、第3図、第4図、および第5図はこの発明の
動作を説明する図である。 図中、1は給電ホーン、2は副反射鏡、3は副
反射鏡、4は主反射鏡、5は接続鏡面、6は回転
対称鏡面、7は平板である。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てある。
FIG. 1 is a schematic configuration diagram of a conventional reflector antenna device, FIG. 2 is a schematic configuration diagram showing an embodiment of the present invention, and FIGS. 3, 4, and 5 explain the operation of the present invention. This is a diagram. In the figure, 1 is a feeding horn, 2 is a sub-reflector, 3 is a sub-reflector, 4 is a main reflector, 5 is a connecting mirror surface, 6 is a rotationally symmetrical mirror surface, and 7 is a flat plate. Note that the same or corresponding parts in the figures are indicated by the same reference numerals.

Claims (1)

【特許請求の範囲】[Claims] 1 主反射鏡と給電ホーンとの間に2枚の副反射
鏡を設けた反射鏡アンテナ装置において、上記主
反射鏡と給電ホーン側の副反射鏡とを所定形状の
鏡面で連結して上記主反射鏡のエツヂ部と副反射
鏡のエツヂ部とが滑らかになるようにしたことを
特徴とする反射鏡アンテナ装置。
1 In a reflector antenna device in which two sub-reflectors are provided between a main reflector and a feeding horn, the main reflector and the sub-reflector on the side of the feeding horn are connected by a mirror surface of a predetermined shape. A reflector antenna device characterized in that the edge part of the reflector and the edge part of the sub-reflector are smooth.
JP14465780A 1980-10-16 1980-10-16 Antenna device for reflecting mirror Granted JPS5768905A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14465780A JPS5768905A (en) 1980-10-16 1980-10-16 Antenna device for reflecting mirror

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14465780A JPS5768905A (en) 1980-10-16 1980-10-16 Antenna device for reflecting mirror

Publications (2)

Publication Number Publication Date
JPS5768905A JPS5768905A (en) 1982-04-27
JPS6151802B2 true JPS6151802B2 (en) 1986-11-11

Family

ID=15367184

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14465780A Granted JPS5768905A (en) 1980-10-16 1980-10-16 Antenna device for reflecting mirror

Country Status (1)

Country Link
JP (1) JPS5768905A (en)

Also Published As

Publication number Publication date
JPS5768905A (en) 1982-04-27

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