JPH02237203A - Offset antenna - Google Patents

Offset antenna

Info

Publication number
JPH02237203A
JPH02237203A JP5695189A JP5695189A JPH02237203A JP H02237203 A JPH02237203 A JP H02237203A JP 5695189 A JP5695189 A JP 5695189A JP 5695189 A JP5695189 A JP 5695189A JP H02237203 A JPH02237203 A JP H02237203A
Authority
JP
Japan
Prior art keywords
radome
side plate
deterioration
primary radiator
reflecting mirror
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
JP5695189A
Other languages
Japanese (ja)
Inventor
Toshio Masujima
増島 俊雄
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 JP5695189A priority Critical patent/JPH02237203A/en
Publication of JPH02237203A publication Critical patent/JPH02237203A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain an offset antenna without the deterioration cause of electric and mechanical characteristics at low cost by setting a side board a specified conical enveloping body. CONSTITUTION:The external form of a radome 11 is set to be two semiellipsoidal assembled forms, and the internal face form of the side board 10 is constituted by the conical enveloping body in which the outer peripheral of a main reflecting mirror is composed of a conductor and respective points on the outer periphery of the radome 11 are set to be vertexes. An auxiliary reflecting mirror 2 and a primary radiator 3 are installed in the conical enveloping body, namely, the side board 10. Since the side board 10 can cover a transmission path 8 without cutting or blocking a radio wave radiated from the primary radiator 3, a hole through which the radio wave passes is eliminated in the side board 10, and the deterioration of a side lobe characteristic due to the edge of the hole and the deterioration of mechanical strength around the hole do not exist. Thus, the inexpensive offset antenna without the deterioration cause of the electric/mechanical characteristics can be obtained.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明Iハ主おしてマイクロ波帯通信あるいはレーダ
ー等に用いる開口面アンテナに関するもので.さらに詳
しく言えば円形開口を有するオフセットアンテナの改良
に関するものであるっ〔従来の技術〕 第4図は例えば特公昭53−31345号公報に示され
た従来のオフセットアンテナを示す側面図.第5図は正
面図.第6図は部分斜ネ芹図であり,図において(1)
はF2  を焦点としAAを回転軸とする回転放物面を
前記11転IIIIAA.!:φなる角度をなす平面P
で切断して得られる主反射鏡,(2)はF1とF2  
を共やく焦点とじBBを回転軸きする回転楕円面の一部
の副反射鏡.(3)は例えば円錐ホーンの一次放射器で
1 この一次放射器(3)の放射電波位相中心は副反射
鏡r21の焦点の1つF1  と一致しているっ{4)
は主反射億(1)の(資)囲を覆う円筒形状の側板.(
5)は側板(4)の一部を切1つて構成される穴(6)
は一次放射器(3)と側板(4)の穴(5)を覆う箱体
,(力は側板(4)の副反射境12)の側の開口を覆う
誘電体板のレドーム,(8)は一次放射器(3)から放
射される電波の伝送路1(9)は穴(5)のエソジであ
るっ従来のオフセントアンテナは上記の様に構成され,
これを送信アンテナとして考えた場合,一次放射器(3
)より放射される雷波は伝送路(8)の通り.前記一次
放射器(3)の放射電波位相中心.すなわち焦点F1 
 を中心とする球面波きして放射され,副反射鏡(2)
で反射して焦点F’2  f経由し,主反射鏡(1)で
反射して平面波となり,アンテナの前方に鋭いビームを
形成するっこの一次放射器(3}の開口に雨滴や雪が付
着すると.一次放射器(3)から放射される眠波の根巾
分布が変化するため.本来の鋭いビームが劣化したり,
不要な方向への電波が放射されるので,レドーム+7l
 ld主反射鏡(1),側板(4).箱体(6)ととも
に密閉溝造をなし,この内部に雨や雪が浸入して一次放
射器13)に付着するときを防いでいるっさらにゴ次放
射器(3)から副反射鏡(2),主反射鏡filを経て
アンテナ前方に至る伝送路f8)の途上で電波がブロッ
クされるとおのないように側板(4)の穴(5)は配攬
されており,レドーム(7)も波長と比べて十分薄い誘
電体の薄漠を使田し,レドーム(7)と伝送路(8)と
のなす角を直角でない角度ψとして電波が通過する際の
反射を啄力少なくしているっ上記の様な留意によりオフ
セットアンテナは.本質的にプロツキングの存在するパ
ラボラアンテナやカセグレンアンテナと比べ,プロッキ
ングによるサイドロープ劣化や利得低下がなく.特性良
好なアンテナとして高密度通信や衛星通信に利用されて
いるっ〔発明が解決しようきする課題〕 しかるに.上記従来のオ′7セットアンテナにおいて必
要とされる側・板f41の穴(5)に関して.電気的特
性および機械的強度上2〜3の考慮すべき点がある, まず電気的特性では,穴15)を幾何光学的に考えた唱
合にはその形状は焦点F2  を頂点きし主反射@(1
)の固囲を導線きする円錐と側板(4)との相貫線とす
ればよい訳だが,実際Kは波長が数儒の゛心波であるた
めこの電波がなす円錐は波動的な拡りを有しているから
,穴(5)は上記相貫線より大きくなくてはならない,
)4?に焦点F2  の近傍では十分大きくする必要が
あり.実用にあたっては第6図に示すように穴(5)は
箱体(6)と同等の大きさとするのが通常である.さら
に穴(5)は側板(4)との間にエッジ(9)を形成し
.アンテナとしての不可避的なエッジすなわち主反射鏡
(1)キ副反射鏡(2)の外川の他にエッジ19)を有
することになり,エッジ回折あるいけエッジ散乱によっ
てサイドローブ特性の劣化が増大するので電波吸収体の
装着などが必要になるっつぎに機械的強度の面では1側
板(4)の円筒ンエルとしての連続性を穴(5)が分断
し.さらに側板(5)と箱体16)の接合される箇所は
シェルとしての曲率bその方向が角,変するから,ここ
に面外曲げモーメントが発生するので板厚を厚くしたり
,補強を加えるなどの処置が必要である,またアンテナ
に台風など強風が作用する際.箱体(6)は風の流線を
乱し風荷重を憎加させるので.乱れを少なくするよう風
洞実験などにより影響の少ない形状を模索し.その結果
に基づき各部の強度を向上させる必要があるっ これらはいずれもオフセットアンテナ本来の電気・機械
的特性の劣化を防ぐためになされるものであるわけだが
,その改善には電波吸収体の使用.板厚の増加々ど製作
費の増大と.穴の形状や電波吸収体の装着位置.箱体の
形状選定など実験的要素の犬なる開発手順を円き.結果
として安価かつ特性良好なオフセットアンテナの実現を
困難にしていた、 この発明はかかる課題を解決するためになされたもので
.上記の特性劣化要因のない安価なオフセットアンテナ
を得ることを目的さしていろう〔課題を解決するための
手段〕 この発明に関わるオフセットアンテナは.レドームの外
周形状を2つの半倒円形の集合形状とし.側板の内面形
状を主反射鏡の外周を導線きしレドームの外周上の各点
を頂点とする錐体の包絡体で構成し.この包絡体すなわ
ち側板内に副反射境お一次放射器を包含するものである
, 〔作用〕 この発明においては,川0板が一次放射器から放射され
る電波を分断あるいはプロツキングすることなく伝送路
を覆うこ々がで久るから.4則板に電波を通過させる穴
が不要で穴のエッジに起因するサイドローブ特性劣化や
穴固辺の機械的強度の劣化がない。さらに副反射鐘.一
次放射器と穴を覆う箱体をこの発明の側板は兼ねるから
.オフセットアンテナを構成する部品の数を少なくする
う〔実施例〕 第1図はこの発明の一実施例を示す側面図.第2図は正
面図であり.図において(1)は主反射鏡,(2)1は
副反射鏡.(3)は一次放射器.(8)は伝送路でこれ
らは上記従米装置と同じである.,01は側板,ロDは
レドームであろう側板fll,:レドーム旧)の形状ハ
以下のように定める。主反射鏡(1)の外周を導線とし
レドームOBの外局上の一点を頂点とする錐体は楕円形
であり一義的に定オる。レドーム[lIの外周上で頂点
を移動していくと,それに対応して錐体が順次定オるが
,レドームaI1の外周を頂点が一周するとこれら帷体
の集合として色絡体が形成される。この包絡体の形状は
.レドームロ9の外固形状と.主反射鐘(1)とレドー
ムanとの相対位置が定まれば主反射鐘fi+に対して
一義的に定まる。従ってL/ ト− ムQηの外ll形
状をアンテナの開口面に投影した際,すなわち第2図の
ごさく回転輸AAの方向から見た際,開口中心0より上
部は反射鏡(11の外周形状すなわち半径rの半円おし
.開口中心Oより下部はその内部に副反射鏡(2)々一
次放射器(3)が包含されるように.延長寸法flとし
て短半径r 長半径R=r+lの半嘴円にレドームQl
1の外周形状とその位置を定めるっ上記のようにレドー
ム■9の外周形状を定めると前記包絡体は一義的に定ま
り,これを内面形状とする側板Illの形状が定まるっ
この側板(110面は.!=0すなわち側板α1が円筒
の場合以外は畏開可能曲而ではないが.第3図に示すよ
うに主反射鏡(1)おレドームt+ 11の各々の外周
を等分し,各点の1川の実長から三角形の累積形状きし
て数値的に近似展開可能であるっ上記のように構成され
たオフセットアンテナにおいて 一次放射器(3)から
副反射@(2),主反射鎖(1)へ枚射される電波は従
来装置と同様に伝送路(8)を伝搬しアンテナ前方に鋭
いビームを形成するが,この電波がなす円錐は側板^■
に包含されており.従来装喧に存在した穴や穴によるエ
ッジは不要であり.側板(I■が伝送路(8)を分断あ
るいはプロツキングするこさがないつつまり゜電気特性
の劣化要因のエツ′)はアンテナとしての不可避的なエ
ッジすなわち主反射儒m.!:副反射@(2)の外局の
みであり.電波の波動的なふるまいによるサイドローブ
劣化は情小限のものになろうまた機械的には,この側板
(11の各微小部分け哨円錐シェルであって周に沿って
連続かつ滑らかであるから.従来装置の側板(4)の円
筒シェルと同じガウス曲率0のシェルに近似であって,
強度一ヒの性状はほぼ同じであるうえ従来装置と異なり
穴がないからシェルの連続性が保たれるので.シェルの
強度を最大限に発揮でき補強措置は不要であるっそして
従来装置の箱体(6)をこの発明の側板(11は兼ねる
から,箱体(6)が不要であって部品点数が減少する.
!:サもに風の流線は円滑なものK々り風荷重も増加し
ないっこの側板11〔は上記で述べたようK@}直的に
近似[拒開するときが可能であり,その製造は板金加工
でできるので極めて安価にオフセソトアンテナが構成で
きるっ従って特性劣化要因のないオフセソトアンテナが
極めて安価に実現できるっ〔発明の効果〕 この発明は以上説明した通り.オフセットアンテナの側
板をある定められた錐体の包絡体とすることにより,電
気的機械的特性の劣化要因のないオフセットアンテナを
安価に実現できるきいう効果がある,
[Detailed Description of the Invention] [Industrial Field of Application] This invention relates primarily to an aperture antenna used for microwave band communication or radar. More specifically, it relates to the improvement of an offset antenna having a circular aperture. [Prior Art] Fig. 4 is a side view showing a conventional offset antenna disclosed in, for example, Japanese Patent Publication No. 53-31345. Figure 5 is a front view. Figure 6 is a partial oblique view, and in the figure (1)
is a paraboloid of revolution with F2 as the focal point and AA as the rotation axis. ! :Plane P forming an angle of φ
The main reflecting mirror obtained by cutting at (2) is F1 and F2
A sub-reflector that is a part of an ellipsoid of revolution that focuses both BB and BB as the axis of rotation. (3) is, for example, a primary radiator of a conical horn.1 The phase center of the radiated radio waves of this primary radiator (3) coincides with one of the focal points F1 of the sub-reflector r21. {4)
is a cylindrical side plate that covers the main reflector. (
5) is a hole (6) made by cutting a part of the side plate (4).
is a box body that covers the primary radiator (3) and the hole (5) in the side plate (4), a radome made of a dielectric plate that covers the opening on the side of the side plate (the force is the sub-reflection boundary 12 of the side plate (4)), (8) The transmission path 1 (9) of the radio waves radiated from the primary radiator (3) is a hole (5). The conventional offset antenna is configured as above,
When considering this as a transmitting antenna, the primary radiator (3
) The lightning waves radiated from the line follow the transmission path (8). The phase center of the radiated radio wave of the primary radiator (3). That is, the focal point F1
is emitted as a spherical wave centered at the sub-reflector (2)
When raindrops or snow adhere to the aperture of this primary radiator (3), it is reflected by the main reflector (1) and forms a sharp beam in front of the antenna. .Because the root width distribution of the sleep wave emitted from the primary radiator (3) changes.The original sharp beam may deteriorate,
Since radio waves are emitted in unnecessary directions, the radome +7L
ld main reflecting mirror (1), side plate (4). Together with the box body (6), a sealed groove structure is formed to prevent rain and snow from entering the interior and adhering to the primary radiator 13). The holes (5) in the side plate (4) are arranged so that the radio waves will not be blocked on the way to the transmission line f8) that passes through the main reflector fil and reaches the front of the antenna, and the radome (7) is also The dielectric material is sufficiently thin compared to the radome (7) and the transmission line (8) are made at an angle ψ which is not a right angle to reduce the reflection force when the radio waves pass through. With the above considerations in mind, offset antennas. Compared to parabolic antennas and Cassegrain antennas that inherently have blocking, there is no side rope deterioration or gain reduction due to blocking. As an antenna with good characteristics, it is used in high-density communications and satellite communications [a problem that the invention aims to solve]. Regarding the hole (5) in the side plate f41 required in the conventional O'7 set antenna mentioned above. There are a few points to consider in terms of electrical properties and mechanical strength. Firstly, in terms of electrical properties, when considering the hole 15) from a geometric optics perspective, its shape has a focal point F2 at its apex and a main reflection. @(1
) can be used as a line of mutual penetration between the cone that carries the conductor and the side plate (4), but in reality K is a heart wave with a wavelength of several degrees, so the cone formed by this radio wave is a wave expansion. The hole (5) must be larger than the above-mentioned intersecting line.
)4? It is necessary to make it sufficiently large near the focal point F2. In practical use, the hole (5) is usually the same size as the box (6), as shown in Figure 6. Furthermore, the hole (5) forms an edge (9) between it and the side plate (4). In addition to the edges of the main reflector (1) and sub-reflector (2), the antenna has an unavoidable edge (edge 19), which increases the deterioration of the sidelobe characteristics due to edge diffraction or edge scattering. Therefore, it is necessary to install a radio wave absorber.Secondly, in terms of mechanical strength, the hole (5) breaks up the continuity of the first side plate (4) as a cylindrical well. Furthermore, since the curvature b as a shell changes its direction at an angle, an out-of-plane bending moment is generated here at the point where the side plate (5) and the box body 16) are joined, so the plate thickness is increased or reinforcement is added. Such measures may be necessary, or when strong winds such as typhoons act on the antenna. The box body (6) disturbs the flow lines of the wind and adds to the wind load. In order to reduce turbulence, we searched for a shape with less impact through wind tunnel experiments. Based on the results, it is necessary to improve the strength of each part. All of these are done to prevent deterioration of the original electrical and mechanical characteristics of the offset antenna, but to improve this, it is necessary to use radio wave absorbers. As the plate thickness increases, manufacturing costs increase. The shape of the hole and the mounting position of the radio wave absorber. The development procedure for experimental elements, such as selecting the shape of the box, was thoroughly explained. As a result, it has become difficult to realize an offset antenna that is inexpensive and has good characteristics.This invention was made to solve this problem. The objective is to obtain an inexpensive offset antenna that does not have the above characteristics deterioration factors [Means for solving the problem] The offset antenna according to the present invention is as follows. The outer circumferential shape of the radome is a collection of two semi-inverted circles. The inner surface of the side plate is composed of a pyramidal envelope whose vertices are each point on the radome's outer periphery, with the outer periphery of the main reflecting mirror being the conducting wire. This envelope, that is, the side plate contains the sub-reflection boundary and the primary radiator. [Function] In this invention, the zero plate allows the radio waves emitted from the primary radiator to be connected to the transmission path without dividing or blocking. The things that cover it will be there for a long time. There is no need for holes in the four-rule plate for passing radio waves, and there is no deterioration in side lobe characteristics caused by the edges of the holes or deterioration in mechanical strength around the holes. In addition, there is a secondary reflective bell. The side plate of this invention also serves as the primary radiator and the box that covers the hole. [Embodiment] Fig. 1 is a side view showing an embodiment of the present invention. Figure 2 is a front view. In the figure, (1) is the main reflector, and (2) 1 is the sub-reflector. (3) is the primary radiator. (8) is the transmission line, and these are the same as the conventional device described above. , 01 is the side plate, and D is the radome. A cone with the outer periphery of the main reflecting mirror (1) as a conducting wire and a point on the outer center of the radome OB as its apex is elliptical and uniquely defined. As you move the apex on the outer circumference of the radome [lI, cones are formed one after another, but as the apex goes around the outer circumference of the radome a1, a chromatic body is formed as a collection of these cones. . The shape of this envelope is. The external solid shape of Radomero 9. Once the relative position between the main reflective bell (1) and the radome an is determined, it is uniquely determined with respect to the main reflective bell fi+. Therefore, when the outer 11 shape of the L/tome Qη is projected onto the aperture surface of the antenna, that is, when viewed from the direction of rotational transport AA in Fig. 2, the area above the aperture center 0 is the reflector (the outer periphery of The shape is a semicircle with a radius r.The area below the aperture center O contains the sub-reflector (2) and the primary radiator (3).The extended dimension fl is the short radius r, the long radius R= Radome Ql on half beak circle of r+l
When the outer circumferential shape of the radome (1) and its position is determined as described above, the envelope is uniquely defined, and the shape of the side plate Ill with this as the inner shape is determined. !=0, that is, it is not possible to open it unless the side plate α1 is cylindrical.As shown in Fig. It can be approximated numerically by calculating the cumulative shape of a triangle from the actual length of one river at a point.In the offset antenna configured as above, the primary radiator (3) causes the sub-reflection @(2), and the main reflection. The radio waves emitted to the chain (1) propagate through the transmission path (8) as in the conventional device and form a sharp beam in front of the antenna, but the cone formed by these radio waves is located on the side plate ^■
It is included in There is no need for holes or edges created by holes that existed in conventional mountings. The side plate (I) has no tendency to cut or block the transmission line (8), which is a cause of deterioration of electrical characteristics). ! : Secondary reflection @(2) only external station. Sidelobe deterioration due to the wave-like behavior of radio waves is extremely limited.Also, mechanically, this side plate (11 minute portions) is a conical shell and is continuous and smooth along the circumference. .It is approximated to a shell with a Gaussian curvature of 0, which is the same as the cylindrical shell of the side plate (4) of the conventional device,
The strength and properties are almost the same, and unlike conventional equipment, there are no holes, so the continuity of the shell is maintained. The strength of the shell can be maximized and no reinforcing measures are required.The box body (6) of the conventional device also serves as the side plate (11) of this invention, so the box body (6) is unnecessary and the number of parts is reduced. do.
! : The wind streamlines are smooth, and the wind load does not increase.As stated above, this side plate 11 can be directly approximated, and its manufacture Since it can be made by sheet metal processing, it is possible to construct an off-set antenna at an extremely low cost.Therefore, an off-set antenna with no characteristics deterioration factor can be realized at an extremely low cost.[Effects of the Invention] This invention is as explained above. By making the side plate of the offset antenna a predetermined pyramidal envelope, it is possible to realize an offset antenna at a low cost without any deterioration factors in its electrical and mechanical properties.

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

第1図はこの発明の一実施例を示す側面図.第2図は正
面図,第3図は側板の展開図,第4図は従来のオフセッ
トアンテナを示す側面図,2g5図は正面図,第6図は
部分斜初図である。 図において.CI)は主反射鏡,(2)は副反射鏡,(
3)id一次放射器,(4)は側板,(5)は穴,j6
)は箱体.(7)はレドーム.t8)は伝送路,(9)
はエッジ,(1■は側板旧}はレドームであるっ なお,各図中同一σ号は同一−1たは相当部分を示すっ
Figure 1 is a side view showing one embodiment of this invention. Fig. 2 is a front view, Fig. 3 is a developed view of the side plate, Fig. 4 is a side view showing a conventional offset antenna, Fig. 2g5 is a front view, and Fig. 6 is a partial oblique view. In the figure. CI) is the main reflector, (2) is the sub-reflector, (
3) ID primary radiator, (4) is the side plate, (5) is the hole, j6
) is a box body. (7) is a radome. t8) is the transmission line, (9)
is the edge, (1■ is the old side plate} is the radome. In each figure, the same σ sign indicates the same -1 or equivalent part.

Claims (1)

【特許請求の範囲】[Claims]  回転放物面を平面で切断して得られる主反射鏡と、上
記主反射鏡外周につけた側板と、上記主反射鏡の焦点を
共やく焦点の1つとする回転楕円面の一部の副反射鏡と
、上記副反射鏡の他方の共やく焦点を電波位相中心とす
る一次放射器と、上記側板の開口側を覆うレドームとか
らなるオフセットアンテナにおいて、外周形状が2つの
半楕円の集合形状であるレドームを備えるとともに、上
記主反射鏡の外周を導線とし上記レドームの外周上の各
点を頂点とする錐体の包絡体を内面形状とする側板を備
え、この側板の内部に上記副反射鏡と上記一次放射器を
備えたことを特徴とするオフセットアンテナ。
A main reflecting mirror obtained by cutting a paraboloid of revolution with a plane, a side plate attached to the outer periphery of the main reflecting mirror, and a sub-reflection of a part of the ellipsoid of revolution whose focal point is the focal point of the main reflecting mirror. In an offset antenna consisting of a mirror, a primary radiator whose radio wave phase center is at the focus of the other sub-reflector, and a radome covering the opening side of the side plate, the outer circumferential shape is a collection of two semi-ellipses. A radome is provided, and a side plate is provided, the inner surface of which is a pyramidal envelope with the outer periphery of the main reflecting mirror as a conducting wire and each point on the outer periphery of the radome as the apex. An offset antenna characterized by comprising: and the above primary radiator.
JP5695189A 1989-03-09 1989-03-09 Offset antenna Pending JPH02237203A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5695189A JPH02237203A (en) 1989-03-09 1989-03-09 Offset antenna

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5695189A JPH02237203A (en) 1989-03-09 1989-03-09 Offset antenna

Publications (1)

Publication Number Publication Date
JPH02237203A true JPH02237203A (en) 1990-09-19

Family

ID=13041855

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5695189A Pending JPH02237203A (en) 1989-03-09 1989-03-09 Offset antenna

Country Status (1)

Country Link
JP (1) JPH02237203A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110542800A (en) * 2019-08-12 2019-12-06 中国电子科技集团公司第四十一研究所 design method of adjustable waveguide probe for electrical thickness fitting reflection test

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110542800A (en) * 2019-08-12 2019-12-06 中国电子科技集团公司第四十一研究所 design method of adjustable waveguide probe for electrical thickness fitting reflection test
CN110542800B (en) * 2019-08-12 2021-08-17 中国电子科技集团公司第四十一研究所 Design method of adjustable waveguide probe for electrical thickness fitting reflection test

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