JPS6017164B2 - horn antenna - Google Patents
horn antennaInfo
- Publication number
- JPS6017164B2 JPS6017164B2 JP12537077A JP12537077A JPS6017164B2 JP S6017164 B2 JPS6017164 B2 JP S6017164B2 JP 12537077 A JP12537077 A JP 12537077A JP 12537077 A JP12537077 A JP 12537077A JP S6017164 B2 JPS6017164 B2 JP S6017164B2
- Authority
- JP
- Japan
- Prior art keywords
- waveguide
- mode
- horn antenna
- horn
- straight circular
- 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
- H01Q13/00—Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave
- H01Q13/02—Waveguide horns
Description
【発明の詳細な説明】
この発明はマイクロ波帯またはミリ波帯で用いられる電
磁ホーンで、円形導波管の基本モードであるTE,.モ
ードと高次モードを用いて励振される複モードホーンア
ンテナに関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnetic horn used in the microwave band or millimeter wave band, which is capable of controlling the fundamental modes of a circular waveguide, TE, . The present invention relates to a multimode horn antenna that is excited using modes and higher-order modes.
従来このような複モードホーンアンテナとしては第1図
に示すように円錐ホーン1、直線円形導波管2、テーパ
導波管4が給電導波管3に接続され直線円形導波管部分
の内部にアイリス5が設けられている形式があった。し
かし、このような構成で複モードホーンアンテナとして
必要な高次モードの発生量と位相を得ることは狭い周波
数帯域内では可能でも、広い周波数帯域中に渡って良好
な性能を得ることには困難があった。また周波数特性の
比較的良好なものを実現しようとする場合、円錐ホーン
1の関口径、あるいは開き角に制約が生じ、ホーンアン
テナとして必要な利得を実現することが困難になるとい
うことや、発生する高次モ−ドの調整が困難になるとい
う欠点があった。この発明はこれらの欠点を除去するた
めに、円錐ホーン1と2つの径の異なる直線円形導波賀
2a,2bと2つのテーパ導波管4a,4bと給電導波
管3および金属帯6で構成され、2つの直線円形導波管
の一方あるいは両方の部分の内部に金属帯6を管軸方向
に複数個設けたことを特徴とし、ホーンの開口径、開き
角を所要の利得が得られるように設定すると共に、広い
周波数帯域に渡って必要な高次モードを発生させ、円偏
波を使用する場合には交差偏波成分の少ないまた直線偏
波を使用するときにはE面とH面のビーム中のそろった
良好な放射パターンを得ることを目的とするもので、以
下図面について詳細に説明する。Conventionally, such a multi-mode horn antenna has a conical horn 1, a straight circular waveguide 2, and a tapered waveguide 4 connected to a feeding waveguide 3, as shown in FIG. There was a model in which iris 5 was provided. However, although it is possible to obtain the generation amount and phase of higher-order modes necessary for a multimode horn antenna within a narrow frequency band with this configuration, it is difficult to obtain good performance over a wide frequency band. was there. In addition, when trying to achieve relatively good frequency characteristics, there are restrictions on the diameter or opening angle of the conical horn 1, which makes it difficult to achieve the necessary gain as a horn antenna. The disadvantage is that it is difficult to adjust the higher-order modes. In order to eliminate these drawbacks, this invention consists of a conical horn 1, two linear circular waveguides 2a, 2b with different diameters, two tapered waveguides 4a, 4b, a feeding waveguide 3, and a metal band 6. The feature is that a plurality of metal bands 6 are provided inside one or both of the two linear circular waveguides in the tube axis direction, and the aperture diameter and opening angle of the horn can be adjusted to obtain the required gain. At the same time, it generates the necessary higher-order modes over a wide frequency band, and when using circularly polarized waves, there are few cross-polarized components, and when using linearly polarized waves, it generates E-plane and H-plane beams. The purpose is to obtain a uniform and good radiation pattern, and the drawings will be explained in detail below.
第2図はこの発明の実施例であって直線円形導波管2a
,2bの内部にはそれぞれ断面が矩形状の金属帯6a,
6b,6c,6dが設けられている。給電導波管3より
基本モードであるTE,.モードが入射すると一部はテ
ーパ導波管4a,4bと直線円形導波管2a,2bの接
合面で高次モードに変換される。さらに金属帯6a,6
b,6c,6dの個所でも、高次モードが発生する。複
モードホ−ンアンテナはアンテナを基本モードであるT
E,.モードで励振した場合に発生する交差偏波成分を
、高次モードで励振した場合に発生する交差偏波成分で
打ち消すようにTE,.モードと高次モードを組み合せ
て励振するようにしたものである。複モードホーンアン
テナとして良好な特性を得ることが可能な高次モードの
条件は、この高次モードの交差偏波成分の電力パターン
、位相パターンの形が、広い角度範囲に渡って、TE,
.モードの交差偏波成分の電力パターン、位相パターン
の形に類似していることである。したがって、このよう
な高次モードとしてはTM,.モードやTEMモードな
どがある。これらの高次モード‘ま高次モードが伝播可
能な円形導波管の内部の不連続部によって発生する。こ
の場合、アンテナを構成している各部が機械的に回転対
称であれば、円形導波管の径を大きくするに従ってTM
,.モ−ド、TE,2モードの順に発生する。複モード
ホーンアンテナとして良好な特性を得るために必要な条
件はTE,.モードの交差偏波成分災TE,.とTM,
.モードの交差偏波成分※TM,.とTE,2モードの
交差偏波成分※TE,2の和が零になることである。FIG. 2 shows an embodiment of the present invention, in which a straight circular waveguide 2a
, 2b have metal bands 6a, each having a rectangular cross section.
6b, 6c, and 6d are provided. From the feeding waveguide 3, the fundamental mode TE, . When the mode is incident, a part of the mode is converted into a higher-order mode at the interface between the tapered waveguides 4a and 4b and the straight circular waveguides 2a and 2b. Furthermore, metal bands 6a, 6
Higher-order modes also occur at locations b, 6c, and 6d. A multimode horn antenna uses the antenna as the fundamental mode T.
E. TE, . It is designed to excite by combining modes and higher-order modes. The conditions for the higher-order mode that make it possible to obtain good characteristics as a multi-mode horn antenna are such that the power pattern and phase pattern of the cross-polarized components of this higher-order mode are such that the shape of the power pattern and the phase pattern are TE,
.. The shape of the power pattern and phase pattern of the cross-polarized components of the mode are similar. Therefore, such higher-order modes include TM, . mode, TEM mode, etc. These higher order modes are generated by discontinuities within the circular waveguide through which they can propagate. In this case, if the parts constituting the antenna are mechanically rotationally symmetric, as the diameter of the circular waveguide increases, the TM
、. Mode, TE, and 2 modes occur in this order. The conditions necessary to obtain good characteristics as a multimode horn antenna are TE, . Mode cross-polarization component damage TE, . and TM,
.. Cross polarization component of mode *TM, . and TE, the cross polarization component of two modes*TE,2 becomes zero.
すなわち次式で表わされる。×TE,.十※TM,.十
×TE2=0 ‘1}また、広い周波数帯
域に渡って良好な特性を得るためには、次の条件も成り
立たなければならない。まくXTEu+XTMu+XT
E・2)=。That is, it is expressed by the following equation. ×TE,. 10*TM,. 10×TE2=0′1} Furthermore, in order to obtain good characteristics over a wide frequency band, the following conditions must also be satisfied. MakuXTEu+XTMu+XT
E・2)=.
‘21上式でfは周波数を表わす。複モードホーン
アンテナでは、各個所から発生する高次モードの合計が
、上記式‘1’、式■を満足するようにしなければなら
ない。'21 In the above equation, f represents the frequency. In a multi-mode horn antenna, the sum of higher-order modes generated from each location must satisfy the above equations '1' and (2).
したがってこの発明では、直線円形導波管2bの径をT
M,.モードが伝播しTE,2モードが伝播しない寸法
とし、かつ、第2図に示すように直線円形導波管2aの
径を、上記直線円形導波管2aの径より大きくしTE,
2モードが伝播する寸法とすることによって、テーパ導
波管4bと直線円形導波管2bの接合面、金属帯6c,
6dおよび直線円形導波管2bとテーパ導波管4aの接
合面においてはTM,.モードのみ発生するので、TM
,.モ−ドとTE,2モードの発生量、位相を個々に調
整することが可能であり、それらの組み合せを適当に選
ぶことによって、広い周波数帯城に渡ってTE,.モー
ドの交差偏波成分を打ち消すことができるので、円偏波
を使用する場合には交差偏波成分の少ない、また直線偏
波を使用する場合にはE面とH面のビーム中のそろった
良好な放射パターンを得ることができる。Therefore, in this invention, the diameter of the straight circular waveguide 2b is set to T
M,. The diameter of the straight circular waveguide 2a is set to be larger than the diameter of the straight circular waveguide 2a, as shown in FIG.
By setting the dimensions such that two modes propagate, the joint surface of the tapered waveguide 4b and the straight circular waveguide 2b, the metal band 6c,
6d and the joint surface between the straight circular waveguide 2b and the tapered waveguide 4a, TM, . Since only mode occurs, TM
、. It is possible to individually adjust the generation amount and phase of the two modes, TE, and TE, and by appropriately selecting a combination of them, TE, . Since cross-polarization components of modes can be canceled, when using circularly polarized waves, there are fewer cross-polarized components, and when using linearly polarized waves, the E-plane and H-plane beams are aligned. A good radiation pattern can be obtained.
なお、上記説明は2つの直線円形導波管2a,2bの両
方に金属帯6a,6b,6c,6dを設けた場合につい
て行なったが、第2図bに示すように一方の直線円形導
波管2aのみに金属帯6a,6bを設けても同様の効果
が得られる。The above explanation was given for the case where the metal bands 6a, 6b, 6c, and 6d were provided on both of the two straight circular waveguides 2a and 2b, but as shown in FIG. A similar effect can be obtained even if the metal bands 6a, 6b are provided only on the tube 2a.
さらに第2図cに示すようにテーパ導波管4aのかわり
にステップ7を用いても同様の効果が得られる。以上の
ようにこの発明によって所定の利得をもち、かつ円偏波
では交差偏波成分の少ない、また直線偏波ではE面とH
面のビーム中のそろった良好な放射パターンを得ること
ができるので、ホーンアンテナとしては勿論、パラボラ
アンテナやカセグレンアンテナの一次放射器としても有
効である。Further, as shown in FIG. 2c, the same effect can be obtained by using step 7 instead of the tapered waveguide 4a. As described above, this invention has a predetermined gain, and has few cross-polarized components in circularly polarized waves, and in linearly polarized waves, it is possible to
Since it is possible to obtain a uniform and good radiation pattern in a plane beam, it is effective not only as a horn antenna but also as a primary radiator for a parabolic antenna or a Cassegrain antenna.
図面の簡単な試験
第1図は従来の複モードホーンァンテナの構成図、第2
図はこの発明による複モードホーンアンテナの一実施例
を示す図である。Simple test of drawings Figure 1 is a configuration diagram of a conventional multi-mode horn antenna, Figure 2 is a diagram of the configuration of a conventional multi-mode horn antenna.
The figure shows an embodiment of a multi-mode horn antenna according to the present invention.
図中、1‘ま円錐ホーン、2は直線円形導波管、3は給
電導波管、4はテーパ導波管、5はアイリス、6は金属
帯、7はステップである。なお図中、同一あるいは相当
部分には同一符号を付してある。第1図
第2図In the figure, 1' is a conical horn, 2 is a linear circular waveguide, 3 is a feeding waveguide, 4 is a tapered waveguide, 5 is an iris, 6 is a metal band, and 7 is a step. In the drawings, the same or corresponding parts are denoted by the same reference numerals. Figure 1 Figure 2
Claims (1)
ンテナにおいて、上記ホーンアンテナを、給電側から見
たとき給電導波管、テーパ導波管又はステツプTE_1
_1モードが伝播しTE_1_2モードが伝播しない径
を有する直線円形導波管、テーパ導波管又はステツプ上
記直線円形導波管の径より大きくTE_1_2モードが
伝播する径を有する直線円形導波管、円錐ホーンが順次
接続された管軸に対して回転対称な構造とし、上記2個
の直線円形導波管の一方あるいは両方の内壁に、上記管
軸に対して回転対称な金属帯を管軸方向に複数個設けた
ことを特徴とするホーンアンテナ。1 In a horn antenna used in the microwave band or millimeter wave band, when the horn antenna is viewed from the feeding side, it is a feeding waveguide, a tapered waveguide, or a step TE_1.
A straight circular waveguide, tapered waveguide or step having a diameter in which the _1 mode propagates and the TE_1_2 mode does not propagate.A straight circular waveguide, a cone, which has a diameter larger than the diameter of the above straight circular waveguide and in which the TE_1_2 mode propagates. The structure is rotationally symmetrical with respect to the tube axis to which the horns are sequentially connected, and a metal band rotationally symmetrical with respect to the tube axis is placed on the inner wall of one or both of the two linear circular waveguides in the tube axis direction. A horn antenna characterized by having a plurality of horn antennas.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12537077A JPS6017164B2 (en) | 1977-10-19 | 1977-10-19 | horn antenna |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP12537077A JPS6017164B2 (en) | 1977-10-19 | 1977-10-19 | horn antenna |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5458336A JPS5458336A (en) | 1979-05-11 |
JPS6017164B2 true JPS6017164B2 (en) | 1985-05-01 |
Family
ID=14908442
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP12537077A Expired JPS6017164B2 (en) | 1977-10-19 | 1977-10-19 | horn antenna |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6017164B2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5216433A (en) * | 1991-11-15 | 1993-06-01 | Hughes Aircraft Company | Polarimetric antenna |
-
1977
- 1977-10-19 JP JP12537077A patent/JPS6017164B2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS5458336A (en) | 1979-05-11 |
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