JPS63300608A - Antenna system - Google Patents

Antenna system

Info

Publication number
JPS63300608A
JPS63300608A JP13668587A JP13668587A JPS63300608A JP S63300608 A JPS63300608 A JP S63300608A JP 13668587 A JP13668587 A JP 13668587A JP 13668587 A JP13668587 A JP 13668587A JP S63300608 A JPS63300608 A JP S63300608A
Authority
JP
Japan
Prior art keywords
concave lens
directivity
radome
aperture
equation
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
JP13668587A
Other languages
Japanese (ja)
Inventor
Masato Inoue
正人 井上
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 JP13668587A priority Critical patent/JPS63300608A/en
Publication of JPS63300608A publication Critical patent/JPS63300608A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To attachably/detachably obtain an antenna system whose directivity fre quency characteristic is able to be decreased by assembling a cone taper and a directivity shaping concave lens to a radome incorporatedly and adopting a structure to be screwed to a circular waveguide of a horn antenna main body. CONSTITUTION:Denoting the mechanical size being a difference of path length of an aperture face B without a concave lens 3c as delta and the size of the concave lens 3c as (d), then the phase phi at the aperture ridge face B is retarded by equation I only (inverse of lambdag represents an integration mean value of a guide wavelength). In adding the concave lens 3c to the aperture, a new phase error DELTAphi (equation II) is added when a radio wave is transmitted therethrough, where lambda is a free space wavelength and epsilonv is a specific dielectric constant of the type of material of the concave lens. In mounting the concave lens 3c, the phase lag phi at the aperture ridge end face B with respect to the center is expressed as equations I+II=equation III, and the phase error is further increased with high frequencies in comparison with the equation I. The beam width is wider when the phase error is increased in the directivity of the horn antenna and the frequency characteristic value as to the directivity is decreased before the mounting in mounting the concave lens 3c.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は航空機等に搭載されて電波の送受信用として
用いられるアンテナ装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an antenna device mounted on an aircraft or the like and used for transmitting and receiving radio waves.

[従来の技術J 第12図(、) (b)及び第13図は、例えばM工C
ROWAVE RESEARCHC0RPORATIO
Nのカタログに示された従来のアンテナ装置を示す断面
図であり、第12図(b)は第12図(a)中A−1t
@及びB −B’線で切断したときの断面図であり、(
IJはリッジ4波管部、リッジ萼波管、円形導波管変換
部、円形4波管部、円錐テーパ都(第9図のみ)からな
るホーンアンテナ、(2)/ri該ホーンアンテナ(1
)の円形専政管部に装填された誘電体移相器、(3)は
該ホーンアンテナ(1)の先端に接着により装置された
レドームである。この接着は、航空機等の実機搭載時の
外囲条件からホーンアンテナ(2)の内部を呆護する目
的で内部の気密を呆つべ〈実施されるので十分堅固なも
のである。
[Prior art J Figures 12 (,) (b) and 13 are, for example, M engineering C
ROWAVE RESEARCHHC0RPORATIO
FIG. 12(b) is a sectional view showing a conventional antenna device shown in the catalog of N.
It is a cross-sectional view when cut along @ and B-B' line, (
IJ is a horn antenna consisting of a ridge 4-wave tube section, a ridge calyx wave tube, a circular waveguide conversion section, a circular 4-wave tube section, and a conical taper (FIG. 9 only), (2)/ri the horn antenna (1
) is a dielectric phase shifter loaded in the circular tube section, and (3) is a radome attached to the tip of the horn antenna (1) by adhesive. This adhesion is sufficiently strong because it is carried out to protect the inside of the horn antenna (2) from the surrounding conditions when it is mounted on an actual aircraft such as an aircraft, so as to keep the inside airtight.

次に動作について説明する。ホーンアンテナ(1)のリ
ンジ尋波管部から榴電された電波はりツジ等波管、円形
導波管変換部を辿って円形4波管部に入り、ここに装填
されている誘電体移相器(2)によって円偏波に変換さ
れた後、レドーム(3) 全透過して空間に放射される
Next, the operation will be explained. The radio waves transmitted from the ringed wave tube section of the horn antenna (1) follow the constant wave tube, the circular waveguide conversion section, and enter the circular 4 wave tube section, where the dielectric phase shifter loaded there. After being converted into a circularly polarized wave by the device (2), it is completely transmitted through the radome (3) and radiated into space.

レドーム(3)の材質、厚さ、表面塗装は電波透過特性
を重要視して選択することにより、強度、耐餉性等の機
械特性、耐環境性能が十分ではない場合が生じ得る。
If the material, thickness, and surface coating of the radome (3) are selected with emphasis on radio wave transmission characteristics, mechanical properties such as strength and corrosion resistance, and environmental resistance may not be sufficient.

この場合Fi航室根搭載等の過酷な外囲条件下で使用す
ることにより、レドーム(3)が劣化して交換が必要と
なる可能性がある。しかしなから、レドーム(3)はホ
ーンアンテナ(1)と一体化接着されているため交換作
業が容易ではない。
In this case, the radome (3) may deteriorate and need to be replaced due to use under harsh environmental conditions such as when mounted on a Fi flight. However, since the radome (3) is integrally bonded to the horn antenna (1), replacement work is not easy.

また、ホーンアンテナ(1)の詫口径DI、D2は利得
、指向性等の放射特性のみならず、飢空桜搭載時の空力
抵抗上の要求によって決定されるが、周知のとおり、そ
の指向性りは(よ周波数に比例して鋭くなる傾向を持ち
、広帯域使用に際してはこのことが不都合となる場合も
ある。
In addition, the aperture diameters DI and D2 of the horn antenna (1) are determined not only by the radiation characteristics such as gain and directivity, but also by the requirements for aerodynamic resistance when mounted on Hungry Sakura; This tendency tends to become sharper in proportion to the frequency, and this may be a disadvantage when using a wide band.

L発明が解決しようとする問題点] 従来のアンテナ装置は以上のように構成逼れているので
、レドームの劣化により交換が必要となったときに交換
が容易ではなく、さらに広帯域にれたる指向性要求値を
満たし得ない可能性があるなどの問題点がめった。
[Problems to be Solved by the Invention] Conventional antenna devices have limited configurations as described above, so when the radome needs to be replaced due to deterioration, it is difficult to replace it, and it is not easy to replace it due to the deterioration of the radome. Problems such as the possibility of not being able to meet sexual needs were common.

この発明は上記のような問題点を解消するためになされ
たもので、レドームの着脱が容易にできるとともに、指
向性の同波数特性を小さくできるアンテナ装置をイ4る
ことを目的とする。
This invention was made to solve the above-mentioned problems, and an object of the present invention is to provide an antenna device in which the radome can be easily attached and detached, and the same wave number characteristic of directivity can be reduced.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係るアンテナ装置はレドームVCホーンアン
テナの一口部に相当する円錐テーパ部と、指向性整形用
の凹レンズを一体化して組み込みホーンアンテナ本体の
円形導波管部にネジ込みできる構造としたものである。
The antenna device according to the present invention has a structure in which a conical taper part corresponding to the mouth part of a radome VC horn antenna and a concave lens for directivity shaping can be integrated and screwed into the circular waveguide part of the horn antenna body. It is.

〔作用〕[Effect]

仁の発明によりレドームの着脱は根元のネジ部を締めた
り、ゆるめたりすることにより実施できるので交換作業
が極めて容易にでき、さらに四レンズの効果が周波数が
尚くなるとともに増すことから、指向性の周IjL数依
存性が低減される。
With Jin's invention, the radome can be attached and detached by tightening or loosening the screw at the base, making replacement work extremely easy.Furthermore, since the effectiveness of the four lenses increases as the frequency increases, the directivity can be improved. The dependence on the number of circumferences IjL is reduced.

〔発明の実施例] 以下、この発明の一実施例を図について説明する。第1
図において(3a)dFRP等寥誘電体を材料とする半
球形のレドーム外皮である。(3b)は先端部を円錐テ
ーパ形状とし、根元にネジ加工を施した金属製のマクン
ト部、(3C)はFRB等の誘電体を材料とする凹レン
ズであり、いずれもレドーム外皮(3a)の内面に接着
剤によって固定される。
[Embodiment of the Invention] An embodiment of the present invention will be described below with reference to the drawings. 1st
In the figure, (3a) is a hemispherical radome outer skin made of dFRP isotropic dielectric material. (3b) is a metal lens with a conically tapered tip and a threaded base, and (3C) is a concave lens made of dielectric material such as FRB. It is fixed to the inner surface with adhesive.

第2図において、(la)Vi先端にネジ加工及び0リ
ング渦加工を施したホーンアンテナJ体、(2)u該ホ
ーンアンテナ本体(la)の内部に装填された誘電体移
相器である。
In Fig. 2, (la) Vi is a horn antenna J body with screw processing and O-ring vortex processing applied to the tip, and (2) u is a dielectric phase shifter loaded inside the horn antenna main body (la). .

第3図において、(4)はホーンアンテナ本体(la)
のOリング溝に埋め込まれた気密用の0リングである。
In Figure 3, (4) is the horn antenna body (la)
This is an airtight O-ring embedded in the O-ring groove.

次に動作について説明する口 電波放射のメカニズムは従来の装置と同様であり、ホー
ンアンテナ本体(la)&レドームQのマクント部(3
b)が第3図に示すように嵌合することにより従来の装
置におけるホーンアンテナ(1)と同じ機能を呈する。
The mechanism of mouth radio wave radiation, which will be explained next, is the same as that of the conventional device.
b) is fitted as shown in FIG. 3, thereby exhibiting the same function as the horn antenna (1) in the conventional device.

アンテナの関口には凹レンズが装着されたことになるの
で、この効果を第4図%5図により説明する。第4図は
凹レンズがない場合の開口部での行路長差の機械寸法う
を示し、第5図f′i囲口部に装着した凹レンズの機械
寸ff1dを示す。
Since a concave lens is attached to the entrance of the antenna, this effect will be explained with reference to FIG. 4.5. FIG. 4 shows the mechanical dimensions of the path length difference at the opening when there is no concave lens, and FIG. 5 shows the mechanical dimensions ff1d of the concave lens attached to the surrounding area f'i.

第4図において開口部縁端での位相−は中央を基準に収
ると たけ遅れている。ここでス2はホーンアンテナ内f$面
波伝送部分の管内波長の槓分千均値である。
In FIG. 4, the phase at the edge of the opening lags behind the center. Here, s2 is the average value of the channel wavelength of the f$ surface wave transmission portion within the horn antenna.

次に第5図のように開口部に凹レンズを付加した場合に
はこの部分を電波が透過する際vcvfrたな位相誤差
Δ− 2πd 7111=−スー(Vπ−1)           
          ・・・(2)が加れる。ここでλ
は自由空間波長、 g7は凹レンズを構成する材質の比
誘電率である。
Next, if a concave lens is added to the aperture as shown in Figure 5, when the radio wave passes through this part, the phase error will be vcvfr Δ- 2πd 7111 = - Sue (Vπ-1)
...(2) is added. Here λ
is the free space wavelength, and g7 is the relative permittivity of the material constituting the concave lens.

したがって、凹レンズを装着するとその開口部縁端での
中央に対する位相おくれ−は(1)式と(2)式の和 一== 棋士−にし”(v’lσ°−1)      
      ・・・(3)λ2  λ となり、(1)式に比べて周波数が筒くなると位相誤差
は更に大きくなる。ホーンアンテナの指向性は、その関
口部の位相誤差が大きくなるとビーム幅が広くなる傾向
にあり、結果的に凹レンズを装着することにより指向性
の周Ijt欽特性が装着前より小さくなる。第6図はこ
の幼果を概念的に示したものである。
Therefore, when a concave lens is attached, the phase lag at the edge of the opening with respect to the center is the sum of equations (1) and (2) == ``Shogi player''(v'lσ° - 1)
...(3) λ2 λ, and as the frequency becomes more cylindrical than in equation (1), the phase error becomes even larger. As for the directivity of a horn antenna, the beam width tends to become wider as the phase error of the entrance part becomes larger, and as a result, by installing a concave lens, the circumferential Ijt characteristic of the directivity becomes smaller than before installation. Figure 6 conceptually shows this young fruit.

レドーム(3)ハホーンアンテナ本体(1a)にネジ込
み構造としたことにより着脱は容易となり、双方の電気
的接触は第3図のthJBの当たりによって完全に保た
れる。血Bを完全にl接触させるため向Aにすき間が生
じるがこの部分にけoリング(4)が装置Aされている
ため、これによって気密性は床たれる。
Since the radome (3) is screwed into the main body of the horn antenna (1a), it can be easily attached and detached, and the electrical contact between the two is completely maintained by contacting thJB in FIG. 3. In order to completely contact blood B, a gap is created in direction A, but since an O-ring (4) is placed in this area with device A, airtightness is maintained.

なお、上記実施例ではレドームを楕成スルマクント部元
端の円錐テーパ形状、及び凹レンズ形状が固定のものと
して説明したが、アンテナの指向特性は上記2ケ所の形
状によって左右されるので、零発用の特徴である着脱の
容易性、嵌合部の互換性を利用して第7図(a) (b
) (c)に示すように形状の異なるもの、即ち指向性
の周波数特性の異なるものを何種か準備しておくことに
より下記の利点が生じる。
In addition, in the above embodiment, the radome was explained as having a fixed conical taper shape at the base end of the elliptical surmacund part and a fixed concave lens shape, but since the directivity characteristics of the antenna are influenced by the shapes of the above two places, Figure 7 (a) (b)
) As shown in (c), by preparing several types of beams with different shapes, that is, with different directivity frequency characteristics, the following advantages arise.

準備するレドームを第7図(a) (b) (c)に示
す3種をして考える。
Consider three types of radomes to be prepared as shown in Figures 7(a), (b), and (c).

第7図(a) (b) (C)において(3b(1))
、(3b(2))、(3b(3))II′iそれぞれ先
端の円錐テーパ形状、卸ち関き角θ1、θ2、θ3及び
開口径り、%D2、D、の異なるマクント部、(30(
1))、(3c(2))、(3c(3))t/′iそれ
ぞれその形状(厚さdi s ’12、aa等)が異な
る凹レンズであり上記実施例と同様にいずれもレドーム
外皮(3a)の内面に接着剤によって固定される。マク
ント5(3b(1))、(3b(匈)、(3b(3))
はいずれも根元にネジ加工が施してあり、これによって
レドーム(3(1))、(3(2))、(3(3))は
上記実施例で用いたのと岡じアンテナ本体(la)に着
脱可能となる。
In Figure 7 (a) (b) (C) (3b(1))
, (3b(2)), (3b(3))II'i respectively have different conical taper shapes at the tips, opening angles θ1, θ2, θ3 and opening diameters, %D2, D, ( 30(
1)), (3c(2)), and (3c(3))t/'i are concave lenses with different shapes (thickness dis '12, aa, etc.), and as in the above embodiment, all of them have a radome outer skin. It is fixed to the inner surface of (3a) with adhesive. Makunto 5 (3b(1)), (3b(匈), (3b(3))
The base of each of the radomes (3(1)), (3(2)), and (3(3)) has the same structure as the antenna body (la) used in the above example. ) can be attached and detached.

アンテナ本体(la)にレドーム(3(1))、(3(
2))、(3(3))が装着された状態を第8図(a)
 (b) (c)に示す。
The antenna body (la) has a radome (3(1)), (3(
Figure 8(a) shows the state in which 2)) and (3(3)) are installed.
(b) Shown in (c).

それぞれの関口形状に対応した関口中心部を基準に開口
縁端部の位相おくれm(位相誤差)の周波数特性の傾向
を第9図(a) (b) (c)に示す。
FIGS. 9(a), 9(b), and 9(c) show trends in the frequency characteristics of the phase lag m (phase error) at the edge of the opening based on the center of the exit corresponding to each exit shape.

ホーンアンテナの指向性、利得はrI目口径及び開口面
上の電界分布によって決まるので、第8図(a)(b)
 (c)の関口形状を持つレドーム(3(1))、(3
(2))、(3(3))を共通のホーンアンテナ本体(
la)に装着した際の利得、ビーム幅の周波数特性の傾
向は第1θ図及び第11図に示すようKなる。
The directivity and gain of the horn antenna are determined by the rI eye aperture and the electric field distribution on the aperture surface, so Fig. 8(a)(b)
Radome (3(1)), (3
(2)), (3(3)) to a common horn antenna body (
The tendency of the frequency characteristics of the gain and beam width when installed in the optical system 1a) is K as shown in FIGS. 1θ and 11.

したがって、使用目的に応じてレドーム(3(1))、
(3(2) )、(3(3))、を付けかえることによ
り容易に周波数特性の異なるアンテナ装置を得ることが
できるという効果が生じる。
Therefore, depending on the purpose of use, radome (3(1)),
By replacing (3(2)) and (3(3)), it is possible to easily obtain antenna devices with different frequency characteristics.

〔発明の効果」 以上のように、この発明によれば、レドームにネジ構造
と円錐テーパ構造を併せ持つ金属マクント部を設け、ホ
ーンアンテナ本体に着脱可能としたので交換が容易とな
り装置の呆守性の向上が期待できる。さらにレドームV
Cは騎電体凹レンズも内蔵したので、指向性の8彼数特
性の小さいより広帯域性のアンテナ装置が得られる効果
がある。
[Effects of the Invention] As described above, according to the present invention, the radome is provided with a metal maknt portion having both a threaded structure and a conical taper structure, and is detachable from the horn antenna body, which facilitates replacement and improves the maintainability of the device. can be expected to improve. Furthermore, radome V
Since C also has a built-in chiroelectric concave lens, it has the effect of providing a wider-band antenna device with a smaller 8-helical directivity characteristic.

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

第1図(a)(b) t:tこの完引の一実施例による
アンテナ装置の構成!!素であるレドームの断面図及び
背面図、第2図(a) (b)はこの発明の一実施例に
よるアンテナ装置の構成要素であるホーンアンテナ本体
、誘電体移相器の断面図及び正面図、第3図はこの発明
の一実施例VCよるアンテナ装置の断面図、第4図、第
5図及び第6図は凹レンズの効果を示す説明図、第7図
(a) (b) (c) ld、この発明の他の実施例
によるレドームの断面図、第8 m (a)(b) (
c)はレドーム(3(1)入(3(2))、(3(3月
をホーンアンテナ本体(la)に装着した状態を示す1
m曲図、第9図(、) (b) (C)はレドーム(3
(1)) 、(3(2) 、(3(3) )を共通のホ
ーンアンテナ(la)に装着した場合の関口向上の位相
分布を示す図、第10図、第11図はそれぞれ該3桓の
レドームの利得の周波数特性の差異、ビーム幅の尚波数
特性の差異を示す特性図、第12図及び免13図は従来
のアンテナ装置を示す断面図である。 図において、(la)はホーンアンテナ本体、(2)は
誘電体移相器、(3)はレドーム、(3a)はレドーム
外皮、(3b)はマクント都、(3c)はNレンズ、(
4)は0リングである。 なお、各図中同−符8/fi同−又は相当部分を示す。 代 理 人  大  岩   増  雄きN為)
FIG. 1 (a) (b) t:tThe configuration of the antenna device according to this complete embodiment! ! 2(a) and 2(b) are cross-sectional views and front views of a horn antenna body and a dielectric phase shifter, which are components of an antenna device according to an embodiment of the present invention. , FIG. 3 is a sectional view of an antenna device according to an embodiment of the present invention, FIGS. 4, 5, and 6 are explanatory diagrams showing the effect of a concave lens. FIGS. ) ld, cross-sectional view of a radome according to another embodiment of the invention, No. 8 m (a) (b) (
c) shows the state in which the radome (3 (1) is included (3 (2)), (3 (3) is attached to the horn antenna body (la)
Fig. 9 (,) (b) (C) shows the radome (3
(1)), (3(2), and (3(3))) are attached to a common horn antenna (la). Figures 12 and 13 are cross-sectional views showing the conventional antenna device. In the figure, (la) is a characteristic diagram showing the difference in the frequency characteristics of the gain of the radome and the difference in the wave number characteristics of the beam width. Horn antenna main body, (2) is dielectric phase shifter, (3) is radome, (3a) is radome outer skin, (3b) is Makunto, (3c) is N lens, (
4) is a 0 ring. In each figure, the same reference numerals 8/fi or equivalent parts are indicated. Agent: Masu Oiwa (OkiN Tame)

Claims (1)

【特許請求の範囲】[Claims] 外囲条件からの保護を目的とするレドームをその開口面
に具備したアンテナ装置において、レドーム自体にアン
テナの機能の一部である円錐テーパ部と誘電体レンズ部
を組み込み、根元にネジ加工を施してアンテナ本体に着
脱可能としたことを特徴とするアンテナ装置。
In an antenna device equipped with a radome on its opening surface for the purpose of protection from surrounding conditions, the radome itself incorporates a conical taper part and a dielectric lens part, which are part of the antenna's function, and has a threaded base. An antenna device characterized in that it can be attached to and detached from an antenna body.
JP13668587A 1987-05-29 1987-05-29 Antenna system Pending JPS63300608A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13668587A JPS63300608A (en) 1987-05-29 1987-05-29 Antenna system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13668587A JPS63300608A (en) 1987-05-29 1987-05-29 Antenna system

Publications (1)

Publication Number Publication Date
JPS63300608A true JPS63300608A (en) 1988-12-07

Family

ID=15181079

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13668587A Pending JPS63300608A (en) 1987-05-29 1987-05-29 Antenna system

Country Status (1)

Country Link
JP (1) JPS63300608A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02164104A (en) * 1988-12-19 1990-06-25 Mitsubishi Electric Corp Weather-proof spherical removable radome
JPH0722834A (en) * 1993-06-30 1995-01-24 Murata Mfg Co Ltd Dielectric lens for antenna and its production
JP2002009542A (en) * 2000-06-22 2002-01-11 Nec Corp Antenna system
JP2010166390A (en) * 2009-01-16 2010-07-29 Nikon Corp Imaging device
JP2016036104A (en) * 2014-08-04 2016-03-17 富士通株式会社 Wireless communication module
JP6563159B1 (en) * 2019-03-07 2019-08-21 三菱電機株式会社 Antenna device

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02164104A (en) * 1988-12-19 1990-06-25 Mitsubishi Electric Corp Weather-proof spherical removable radome
JPH0722834A (en) * 1993-06-30 1995-01-24 Murata Mfg Co Ltd Dielectric lens for antenna and its production
JP2002009542A (en) * 2000-06-22 2002-01-11 Nec Corp Antenna system
JP2010166390A (en) * 2009-01-16 2010-07-29 Nikon Corp Imaging device
JP2016036104A (en) * 2014-08-04 2016-03-17 富士通株式会社 Wireless communication module
JP6563159B1 (en) * 2019-03-07 2019-08-21 三菱電機株式会社 Antenna device
WO2020179048A1 (en) * 2019-03-07 2020-09-10 三菱電機株式会社 Antenna device
US11962081B2 (en) 2019-03-07 2024-04-16 Mitsubishi Electric Corporation Antenna device

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