JPS5820161B2 - antenna device - Google Patents
antenna deviceInfo
- Publication number
- JPS5820161B2 JPS5820161B2 JP11052278A JP11052278A JPS5820161B2 JP S5820161 B2 JPS5820161 B2 JP S5820161B2 JP 11052278 A JP11052278 A JP 11052278A JP 11052278 A JP11052278 A JP 11052278A JP S5820161 B2 JPS5820161 B2 JP S5820161B2
- Authority
- JP
- Japan
- Prior art keywords
- antenna device
- antenna
- aperture
- radio wave
- plate made
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q19/00—Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic
- H01Q19/10—Combinations 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
- H01Q19/12—Combinations 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 wherein the surfaces are concave
- H01Q19/13—Combinations 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 wherein the surfaces are concave the primary radiating source being a single radiating element, e.g. a dipole, a slot, a waveguide termination
- H01Q19/132—Horn reflector antennas; Off-set feeding
Landscapes
- Aerials With Secondary Devices (AREA)
- Waveguide Aerials (AREA)
Description
【発明の詳細な説明】
この発明はマイクロ波以上の高い周波数帯で用いられる
開口面アンテナで、優れた広角放射パターンをもつアン
テナ装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an antenna device that is an aperture antenna used in a high frequency band higher than microwaves and has an excellent wide-angle radiation pattern.
従来の開口面アンテナの一例を第1図に示す。An example of a conventional aperture antenna is shown in FIG.
第1図において1は給電ホーン、2は回転放物面鏡の一
部である反射鏡面、3は円筒形の構造物である。In FIG. 1, 1 is a feeding horn, 2 is a reflecting mirror surface which is a part of a parabolic mirror of revolution, and 3 is a cylindrical structure.
このような構成のアンテナにおいては給電ホーン1から
放射された球面波は反射鏡面2によって反射され平面波
となり、円筒形の構造物3内を通って外部へ放射される
。In the antenna having such a configuration, a spherical wave radiated from the feeding horn 1 is reflected by the reflecting mirror surface 2 to become a plane wave, which passes through the cylindrical structure 3 and is radiated to the outside.
しかしこの場合、開口のエツジP1.P2において回折
現象が生じ、その回折波によって広角放射パターンが劣
下するという欠点があった。However, in this case, the edge of the opening P1. A diffraction phenomenon occurs at P2, and the wide-angle radiation pattern is degraded by the diffracted waves.
すなわち第1図に示すように十分遠方の観測点Sを示す
角度θを定義すれば、θが90°より大なるとき、Sの
放射レベルに寄与する回折波EdはPlからの回折波で
あり、それはPlでの電界強度をEi とすれば次式で
表わされる。In other words, if we define an angle θ indicating a sufficiently distant observation point S as shown in Fig. 1, when θ is greater than 90°, the diffracted wave Ed contributing to the radiation level of S is the diffracted wave from Pl. , which is expressed by the following equation, assuming that the electric field strength at Pl is Ei.
SはPlとSの距離、aは開口の半径、kは波数を示す
。S is the distance between Pl and S, a is the radius of the aperture, and k is the wave number.
ここでD(φ、φ′)は回折係数で、幾何光学的回折理
論によれば次のような形で表わされる。Here, D(φ, φ') is a diffraction coefficient, which is expressed in the following form according to the geometric optical diffraction theory.
複号の(lは偏波がエツジに平行な場合(力は垂直な場
合である。(l is the case where the polarization is parallel to the edge (the force is perpendicular).
この発明はこのような欠点を除去するために、開口の縁
に繰上の各点における電波の進行方向に対して一定の角
度をなす直線の集合で構成される錐状の金属板または金
属板に電波吸収体を設けた構造のしゃへい板を設けたこ
とを特徴とし、その目的は広角放射パターンに寄与する
エツジへの入射レベルを下げることによって回折波を低
減し、:優れた広角放射パターンをもつアンテナ装置を
実現することにあり、以下図面について詳細に説明する
。In order to eliminate such drawbacks, the present invention has developed a conical metal plate or a metal plate consisting of a set of straight lines that form a fixed angle with respect to the direction of propagation of radio waves at each point on the edge of the opening. It is characterized by the provision of a shielding plate with a structure provided with a radio wave absorber, the purpose of which is to reduce diffracted waves by lowering the incident level to the edges that contribute to the wide-angle radiation pattern: to have an excellent wide-angle radiation pattern The purpose is to realize an antenna device, and the drawings will be described in detail below.
第2図はこの発明の実施例で、第1図に示した開口面ア
ンテナの開口の縁に円錐状のしゃへい板4をとりつけた
構造になっている。FIG. 2 shows an embodiment of the present invention, which has a structure in which a conical shielding plate 4 is attached to the edge of the aperture of the aperture antenna shown in FIG.
このような構造になっているので、広角放射パターンに
寄与するのはQtからの回折波Edであり、Qlでの電
界強度をE自とすれば次式で表わされる。With such a structure, it is the diffracted wave Ed from Qt that contributes to the wide-angle radiation pattern, and if the electric field strength at Ql is E, it can be expressed by the following equation.
Qlでの電界Ei1は、Plからの回折波であるのでP
lにおける電界強度Eiより次式で求められる。The electric field Ei1 at Ql is a diffracted wave from Pl, so P
It is determined from the electric field strength Ei at l by the following equation.
ここで01は第2図に示すように電波通路とじゃへい板
のなす角、SlはPlとQlの距離を示す。Here, 01 indicates the angle formed by the radio wave path and the baffle plate as shown in FIG. 2, and Sl indicates the distance between Pl and Ql.
DI(φ、φ′)は次式で表わされる。DI (φ, φ') is expressed by the following equation.
計算の一例として2a−1661!1711 θ1−2
0°、S1=293mm、周波数31GHzの場合につ
いて計算した結果を第3図に示す。As an example of calculation, 2a-1661!1711 θ1-2
FIG. 3 shows the calculation results for the case of 0°, S1=293 mm, and frequency of 31 GHz.
第3図においてたて軸はPlまたはQlからの回折波E
dの相対レベル(dB)、よこ軸は角度θを示す。In Figure 3, the vertical axis is the diffracted wave E from Pl or Ql.
The relative level of d (dB), the horizontal axis shows the angle θ.
この図より広角放射パターンに寄与する回折波のレベル
が顕著に改善できることが分る。It can be seen from this figure that the level of diffracted waves contributing to the wide-angle radiation pattern can be significantly improved.
なお、第3図に於て、実線Aは第1図の従来の場合のP
lから回折波のレベルを示し、破線Bは第2に示す本発
明の実施例のQlからの回折波のレベルを示す。In addition, in FIG. 3, the solid line A indicates P in the conventional case of FIG.
The level of the diffracted wave is shown from Ql, and the broken line B shows the level of the diffracted wave from Ql in the second embodiment of the present invention.
またじゃへい板の内側に電波吸収体を設けることによっ
て第2図に示す開口のエツジP1.P2からの回折波か
じゃへい波の内側で反射され、放射パターンに影響を及
ぼすことを避けることができる。Furthermore, by providing a radio wave absorber inside the baffle plate, the opening edge P1 shown in FIG. It is possible to prevent the diffracted wave from P2 from being reflected inside the deflection wave and affecting the radiation pattern.
なお以上は開口の形状が円形の場合について説明したが
、この発明はこれに限らず任意の形状の開口について使
用してもよい。Although the case where the shape of the aperture is circular has been described above, the present invention is not limited to this and may be used for apertures of any shape.
また以上の説明は開口の波面が平面の場合について行な
ってるが本発明はこれに限らず、第4図に示すように電
磁ホーンのように球面波などを放射する開口面アンテナ
についてもまた任意の形状の波を放射する開口面アンテ
ナについても同様に使用できる。Furthermore, although the above explanation has been made for the case where the wavefront of the aperture is a plane, the present invention is not limited to this, and as shown in FIG. An aperture antenna that emits shaped waves can also be used in the same way.
また開口面アンテナとして単独に使用するだけでなく第
5図に示すようにアンテナの一次放射器系に使用してア
ンテナ全体の広角放射パターンを改良することもできる
。In addition to being used alone as an aperture antenna, it can also be used in the primary radiator system of the antenna, as shown in FIG. 5, to improve the wide-angle radiation pattern of the entire antenna.
またアンテナ形式としてオフセット形式にすることによ
って、しやへい板によるブロッキング等による広角放射
パターンの劣下を避けることができる。Furthermore, by using an offset type antenna, it is possible to avoid deterioration of the wide-angle radiation pattern due to blocking caused by the shield plate.
以上のようにこの発明に係るアンテナ装置においては、
開口の縁に設けた錐状のじゃへい板の効果によって容易
に広角放射パターンの優れたアンテナ装置を実現できる
利点がある。As described above, in the antenna device according to the present invention,
The effect of the conical baffle plate provided at the edge of the opening has the advantage that an antenna device with an excellent wide-angle radiation pattern can be easily realized.
第1図は従来のアンテナ装置の構成を示す断面図、第2
図は本発明の実施例の一つの構成を示す断面図、第3図
は本発明の効果を示す計算結果を示す図、第4図は本発
明の他の実施例の構成を示す断面図、第5図は本発明を
アンテナ装置の構成要素の一つとして用いた場合の断面
図である。
図中1は給電ホーン、2は反射鏡面、3は円筒形のしゃ
へい板、4は本発明のしゃへい板、5は副反射鏡、6は
主反射鏡である。
また第3図の実線Aは第1図に示す従来のアンテナ装置
のエツジP1からの回折波、破線Bは第2図に示す本発
明の実施例の場合のエツジQ1からの回折波のそれぞれ
のレベルを示すものである。
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
しである。Figure 1 is a cross-sectional view showing the configuration of a conventional antenna device;
The figure is a sectional view showing the configuration of one embodiment of the present invention, FIG. 3 is a diagram showing calculation results showing the effects of the present invention, and FIG. 4 is a sectional view showing the configuration of another embodiment of the present invention. FIG. 5 is a sectional view when the present invention is used as one of the components of an antenna device. In the figure, 1 is a feeding horn, 2 is a reflecting mirror surface, 3 is a cylindrical shielding plate, 4 is a shielding plate of the present invention, 5 is a sub-reflector, and 6 is a main reflector. Further, the solid line A in FIG. 3 represents the diffracted wave from the edge P1 of the conventional antenna device shown in FIG. 1, and the broken line B represents the diffracted wave from the edge Q1 in the case of the embodiment of the present invention shown in FIG. This indicates the level. In the drawings, the same or corresponding parts are designated by the same reference numerals.
Claims (1)
面アンテナを有し、上記開口面アンテナの開口に至る電
波の通路が金属板で構成される構造物で覆われている形
式のアンテナ装置において、開口の縁に繰上の各点にお
ける電波の進行方向に対して所定の角度をなす直線の集
合で構成される錐状の金属板で構成されたしゃへい板を
設けたことを特徴とするアンテナ装置。 2 金属板で構成されるじゃへい板の電波通路に近い側
の面に電波吸収体を設けたことを特徴とする特許請求の
範囲第1項記載のアンテナ装置。 3 マイクロ波帯以上の高い周波数帯で用いられるもの
であって、アンテナ系の一部に一次放射器系を有するア
ンテナ装置に於て、上記−次放射器の開口の縁に、線上
の各点における電波の進行方向に対して所定の角度をな
す直線の集合で構成される錐状の金属板で構成されたし
ゃへい板を設けたことを特徴とするアンテナ装置。 4 金属板で構成されるじゃへい板の電波通路に近い側
の面に電波吸収体を設けたことを特徴とする特許請求の
範囲第3項記載のアンテナ装置。 5 アンテナ系として、オフセット形式のアンテナ系と
したことを特徴とする特許請求の範囲第3項記載のアン
テナ装置。[Claims] 1. It has an aperture antenna used in a high frequency band above the microwave band, and a radio wave path leading to the aperture of the aperture antenna is covered with a structure made of a metal plate. In this type of antenna device, a shielding plate made of a cone-shaped metal plate made of a set of straight lines forming a predetermined angle with respect to the direction of propagation of radio waves at each point of the opening is provided on the edge of the opening. Characteristic antenna device. 2. The antenna device according to claim 1, characterized in that a radio wave absorber is provided on the surface of the barrier plate made of a metal plate on the side closer to the radio wave path. 3. In an antenna device that is used in a high frequency band above the microwave band and has a primary radiator system as part of the antenna system, each point on the line is placed at the edge of the aperture of the secondary radiator. An antenna device comprising a shielding plate made of a cone-shaped metal plate made of a set of straight lines forming a predetermined angle with respect to the direction of propagation of radio waves. 4. The antenna device according to claim 3, characterized in that a radio wave absorber is provided on the surface of the barrier plate made of a metal plate on the side closer to the radio wave path. 5. The antenna device according to claim 3, wherein the antenna system is an offset type antenna system.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11052278A JPS5820161B2 (en) | 1978-09-08 | 1978-09-08 | antenna device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11052278A JPS5820161B2 (en) | 1978-09-08 | 1978-09-08 | antenna device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5537076A JPS5537076A (en) | 1980-03-14 |
JPS5820161B2 true JPS5820161B2 (en) | 1983-04-21 |
Family
ID=14537924
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11052278A Expired JPS5820161B2 (en) | 1978-09-08 | 1978-09-08 | antenna device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5820161B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6930647B2 (en) | 2001-05-17 | 2005-08-16 | Hitachi Kokusai Electric Inc. | Semicircular radial antenna |
-
1978
- 1978-09-08 JP JP11052278A patent/JPS5820161B2/en not_active Expired
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6930647B2 (en) | 2001-05-17 | 2005-08-16 | Hitachi Kokusai Electric Inc. | Semicircular radial antenna |
Also Published As
Publication number | Publication date |
---|---|
JPS5537076A (en) | 1980-03-14 |
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