JPS6022844B2 - array antenna - Google Patents

array antenna

Info

Publication number
JPS6022844B2
JPS6022844B2 JP1032678A JP1032678A JPS6022844B2 JP S6022844 B2 JPS6022844 B2 JP S6022844B2 JP 1032678 A JP1032678 A JP 1032678A JP 1032678 A JP1032678 A JP 1032678A JP S6022844 B2 JPS6022844 B2 JP S6022844B2
Authority
JP
Japan
Prior art keywords
distribution
array antenna
antenna
shape
amplitude
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
JP1032678A
Other languages
Japanese (ja)
Other versions
JPS54103657A (en
Inventor
清司 真野
誠 小野
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 JP1032678A priority Critical patent/JPS6022844B2/en
Publication of JPS54103657A publication Critical patent/JPS54103657A/en
Publication of JPS6022844B2 publication Critical patent/JPS6022844B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q21/00Antenna arrays or systems
    • H01Q21/06Arrays of individually energised antenna units similarly polarised and spaced apart

Landscapes

  • Variable-Direction Aerials And Aerial Arrays (AREA)

Description

【発明の詳細な説明】 この発明は多くの素子アンテナを配列して成るアレイア
ンテナにおいて、各素子アンテナは同一の励振振幅をも
ちながら、アレイアンテナとしてはその放射パターンが
低サイドロープであるアレイアンテナに関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides an array antenna in which many element antennas are arranged, each element antenna having the same excitation amplitude, and the radiation pattern of the array antenna being a low side lobe. It is related to.

従来のこの種アレイアンテナは複数個の素子アンテナを
直線状あるいは円形状に配列し、各素子アンテナの励振
振幅に重みをつけることによりアレイアンテナ全体とし
ての励振振幅分布を例えばドルフチェビシェフ分布やテ
ーラ分布などの低サイドローブ化振幅分布にし、放射パ
ターンの低サイドローブ化を実現してきた。
Conventional array antennas of this type have a plurality of element antennas arranged in a linear or circular shape, and by weighting the excitation amplitude of each element antenna, the excitation amplitude distribution of the entire array antenna can be adjusted to, for example, the Dolph-Chebyshev distribution or the Taylor distribution. We have achieved a low sidelobe radiation pattern by creating a low sidelobe amplitude distribution such as .

このため、各素子アンテナに所望の励振振幅を与えるた
めの不等分配の給電回路系を構成する必要があり、その
設計および製作が複雑であり、コスト高になる欠点を有
していた。アレイアンテナのように多くの素子アンテナ
を配列して構成する場合には各素子アンテナへ、いかに
効率よく電力を分配供給するかは電気性能上、また配列
構造上も重要であり、このためにはその回路構成はでき
るだけ単純である方が優れているといえる。第1図は従
来のアレイアンテナの説明図で、複数個の素子アンテナ
1はその外周配列形状が円周2に沿ってほぼ円形状とな
るように配列され、アレイアンテナ3を構成している。
For this reason, it is necessary to construct a feeding circuit system with unequal distribution in order to give a desired excitation amplitude to each element antenna, which has the disadvantage that its design and manufacture are complicated and the cost is high. When arranging many element antennas like an array antenna, it is important to efficiently distribute and supply power to each element antenna from the viewpoint of electrical performance and arrangement structure. It can be said that it is better if the circuit configuration is as simple as possible. FIG. 1 is an explanatory diagram of a conventional array antenna, in which a plurality of element antennas 1 are arranged so that their outer periphery is substantially circular along a circumference 2, forming an array antenna 3.

このため、もし、各素子アンテナ1の励振振幅が均一で
あれば円形関口アンテナとほぼ同じ約一17dBのサイ
ドローブレベルとなり、このレベルをさらに下げるため
には各素子アンテナ1の励振振幅に重みをつけてアレイ
アンテナ3全体の励振振幅分布を低サイドローブ化分布
変えなければならない。この発明は従釆の欠点を除去す
るために各素子アンテナへ電力は均一に分配して分配回
路をもっとも単純にしながら、複数個の素子アンテナの
外周配列形状を低サイドローブ化振幅分布形状に合わせ
て低サイドローブ化を可能ならしめたもので、以下図面
について詳細に説明する。
Therefore, if the excitation amplitude of each element antenna 1 is uniform, the side lobe level will be approximately 17 dB, which is almost the same as that of a circular Sekiguchi antenna.In order to further reduce this level, the excitation amplitude of each element antenna 1 must be weighted. In addition, the excitation amplitude distribution of the entire array antenna 3 must be changed to a low sidelobe distribution. In order to eliminate the drawbacks of the secondary structure, this invention distributes power uniformly to each element antenna to simplify the distribution circuit, and at the same time adjusts the outer circumferential arrangement shape of the multiple element antennas to a low sidelobe amplitude distribution shape. This makes it possible to reduce side lobes, and the drawings will be described in detail below.

第2図はこの発明の実施例であり、複数個の素子アンテ
ナ1はその外周配列形状がいわゆるテーラ分布4にほぼ
一致するように配列され、アレイアンテナ5を構成して
いる。
FIG. 2 shows an embodiment of the present invention, in which a plurality of element antennas 1 are arranged so that their outer circumferential arrangement shape approximately corresponds to a so-called Taylor distribution 4, forming an array antenna 5.

各素子アンテナ1は同一の振幅で励振されるように電力
が供給分配されている。なお、6は基本の配列鼠である
。このように構成されているから、その効果としては基
本配列軸6を含む平面内の放射パターンのサイドロープ
は上記テーラ分布4によって決まる低い放射レベルとな
る。これは基本配列軸6の上に投影された等価的な線状
アレイアンテナの1個の素子アンテナの振幅が、第2図
の基本配列軸6に直交する方向に配列された素子アンテ
ナの数に比例した振幅に等しく、したがって、その等価
的線状アレイアンテナの振幅分布4にほぼ等しくなるた
めである。しかも、第2図においては各素子アンテナ1
への給電電力の分配が均一であるため、その分配回路の
構成が不等分配に比べて、はるかに単純になる。つまり
、分配回路の設計・製作が容易で、コストが安く、かつ
、所期の電気性能の得られやすいアレイアンテナを提供
する。第3図はこの発明の他の実施例であるが、この場
合、素子アンテナ1の外周配列形状線7は第2図におけ
るようなテーラ分布4にそのまま合致していない。しか
し、基本配列軸8の上に投影された等価的な線状アレイ
アンテナの振幅分布は、ある所望のテーラ分布になるよ
うに、基本配列軸8に直交する方向に配列されている素
子アンテナ1の数が選ばれている。このように外周配列
形状線7をテーラ分布曲線そのものに合致させなくとも
等価的にテーラ分布を実現している。第8図の例ではア
レイアンテナ9は全体として基本配列軸8に関してほぼ
対称な構造としている。なお、この実施例においても、
当然、各素子アンテナ1の励振振幅は同一であり、アレ
イアンテナ9への電力分配回路は等分配回路になってい
る。なお、以上は低サイドロープ化振幅分布としてテー
ラ分布を用いる場合について説明したが、この発明はこ
れに限らず、ドルフテェビシェフ分布、余弦(cosi
雌)分布、変形テーラ分布、COSme−on−ped
esね1分布などあらゆる低サイドローブ化振幅分布を
用いて実施することができる。
Power is distributed so that each element antenna 1 is excited with the same amplitude. Note that 6 is the basic array mouse. With this configuration, the effect is that the side lobes of the radiation pattern in the plane containing the basic arrangement axis 6 have a low radiation level determined by the Taylor distribution 4 described above. This means that the amplitude of one element antenna of an equivalent linear array antenna projected onto the basic arrangement axis 6 is equal to the number of element antennas arranged in the direction orthogonal to the basic arrangement axis 6 in FIG. This is because it is equal to the proportional amplitude and therefore approximately equal to the amplitude distribution 4 of its equivalent linear array antenna. Moreover, in Fig. 2, each element antenna 1
Since the distribution of the power supplied to the terminals is uniform, the configuration of the distribution circuit is much simpler than that in the case of unequal distribution. In other words, the present invention provides an array antenna whose distribution circuit is easy to design and manufacture, whose cost is low, and whose desired electrical performance is easily obtained. FIG. 3 shows another embodiment of the present invention, but in this case, the outer circumference array shape line 7 of the element antenna 1 does not match the Taylor distribution 4 as shown in FIG. However, the element antennas 1 are arranged in a direction orthogonal to the basic arrangement axis 8 so that the amplitude distribution of the equivalent linear array antenna projected onto the basic arrangement axis 8 becomes a certain desired Taylor distribution. The number of has been selected. In this way, the Taylor distribution is equivalently realized even if the outer circumferential array shape line 7 does not match the Taylor distribution curve itself. In the example shown in FIG. 8, the array antenna 9 as a whole has a substantially symmetrical structure with respect to the basic array axis 8. In addition, also in this example,
Naturally, the excitation amplitude of each element antenna 1 is the same, and the power distribution circuit to the array antenna 9 is an equal distribution circuit. Although the case where the Taylor distribution is used as the low siderope amplitude distribution has been described above, the present invention is not limited to this, and the Dorftebyshev distribution, the cosine (cosine) distribution, etc.
female) distribution, modified Taylor distribution, COSme-on-ped
It can be implemented using any low sidelobe amplitude distribution, such as the esne1 distribution.

なお、前述の原理説明からも明らかなように、この発明
は外周素子配列形状が等価的に低サイドロープ化振幅分
布の形状に合えばよいのであるから、実施例のような外
周配列形状に限定されるものではなく、構成のしやすさ
などを考慮して種々の形状をとりうるものである。また
、これまで送信について説明したが、受信についても同
様に実施できることは当然であり、さらに、アレイアン
テナとしては平面状、曲面状に配列されたもの、あるい
は、可変移相器などによって電子的ビーム走査を行なう
いわゆるフェィズドアレィアンテナを用いて実施するこ
ともできる。以上のようにこの発明に係るアレイアンテ
ナでは、配列する素子アンテナの外周配列形状を低サイ
ドローブ化振幅分布の形状に合わせることによって電力
分配回路構成の容易な均一分配で、かつ、低サイドロー
ブ特性をもたすことができるから、これをレーダ用アン
テナなどとして用いた場合にその効果に著しく大きい。
Note that, as is clear from the above explanation of the principle, the present invention is limited to the outer peripheral element array shape as in the embodiment, since it is sufficient that the outer peripheral element array shape equivalently matches the shape of the low siderope amplitude distribution. Rather, it can take various shapes in consideration of ease of construction. Furthermore, although we have explained transmission so far, it goes without saying that reception can also be carried out in the same way; It can also be implemented using a so-called phased array antenna that performs scanning. As described above, in the array antenna according to the present invention, by matching the outer circumferential arrangement shape of the arrayed element antennas to the shape of the low sidelobe amplitude distribution, the power distribution circuit configuration can easily achieve uniform distribution and have low sidelobe characteristics. Therefore, when used as a radar antenna, the effect is extremely large.

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

第1図は従釆のアレイアンテナの説明図、第2図はこの
発明の一実施例の説明図、第3図はこの発明の他の実施
例の説明図である。 図中、1は素子アンテナ、2は円周、4はテーラ分布で
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。多1図 多z図 多3図
FIG. 1 is an explanatory diagram of a subordinate array antenna, FIG. 2 is an explanatory diagram of one embodiment of the invention, and FIG. 3 is an explanatory diagram of another embodiment of the invention. In the figure, 1 is an element antenna, 2 is a circumference, and 4 is a Taylor distribution. In the drawings, the same or corresponding parts are denoted by the same reference numerals. Many 1 drawings Many z drawings Many 3 drawings

Claims (1)

【特許請求の範囲】[Claims] 1 複数個の素子アンテナを等間隔に、かつ平面状ある
いは曲面状に配列して成るアレイアンテナにおいて、外
周素子配列によつて決まる上記アレイアンテナの外周形
状が低サイドローブ化振幅分布の形状に対応して決めら
れていることを特徴とするアレイアンテナ。
1 In an array antenna consisting of a plurality of element antennas arranged at regular intervals in a planar or curved shape, the outer circumferential shape of the array antenna determined by the outer circumferential element arrangement corresponds to the shape of the low sidelobe amplitude distribution. An array antenna characterized by:
JP1032678A 1978-02-01 1978-02-01 array antenna Expired JPS6022844B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1032678A JPS6022844B2 (en) 1978-02-01 1978-02-01 array antenna

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1032678A JPS6022844B2 (en) 1978-02-01 1978-02-01 array antenna

Publications (2)

Publication Number Publication Date
JPS54103657A JPS54103657A (en) 1979-08-15
JPS6022844B2 true JPS6022844B2 (en) 1985-06-04

Family

ID=11747086

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1032678A Expired JPS6022844B2 (en) 1978-02-01 1978-02-01 array antenna

Country Status (1)

Country Link
JP (1) JPS6022844B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6398696U (en) * 1986-12-18 1988-06-25
JPH0557893U (en) * 1992-01-07 1993-07-30 田淵電機株式会社 Electronic circuit device

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7460077B2 (en) * 2006-12-21 2008-12-02 Raytheon Company Polarization control system and method for an antenna array
GB2532206A (en) * 2014-11-06 2016-05-18 Bluwireless Tech Ltd Antennas
GB2532207A (en) * 2014-11-06 2016-05-18 Bluwireless Tech Ltd Radio frequency communications devices

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6398696U (en) * 1986-12-18 1988-06-25
JPH0557893U (en) * 1992-01-07 1993-07-30 田淵電機株式会社 Electronic circuit device

Also Published As

Publication number Publication date
JPS54103657A (en) 1979-08-15

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