JPS6181003A - Array antenna - Google Patents

Array antenna

Info

Publication number
JPS6181003A
JPS6181003A JP20351384A JP20351384A JPS6181003A JP S6181003 A JPS6181003 A JP S6181003A JP 20351384 A JP20351384 A JP 20351384A JP 20351384 A JP20351384 A JP 20351384A JP S6181003 A JPS6181003 A JP S6181003A
Authority
JP
Japan
Prior art keywords
array antenna
maximum phase
antenna
phase
maximum
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.)
Granted
Application number
JP20351384A
Other languages
Japanese (ja)
Other versions
JPH0473644B2 (en
Inventor
Koichi Kitajima
北島 耕一
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 JP20351384A priority Critical patent/JPS6181003A/en
Publication of JPS6181003A publication Critical patent/JPS6181003A/en
Publication of JPH0473644B2 publication Critical patent/JPH0473644B2/ja
Granted 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
    • H01Q21/22Antenna units of the array energised non-uniformly in amplitude or phase, e.g. tapered array or binomial array

Landscapes

  • Variable-Direction Aerials And Aerial Arrays (AREA)

Abstract

PURPOSE:To obtain an array antenna of good electric characteristics without degrading the antenna efficiency by setting the excitation phase distribution of element antennas to a polygonal line and making the radiation pattern asymmetrical. CONSTITUTION:Phase adjusters 3a-3n connected to element antennas 1a-1n are used to adjust a phase phiX of input signals of element antennas 1a-1n on a basis of the center of the array antenna. If a position P of a maximum phase quantity is smaller than 0.3, the value which a maximum phase quantity phiM can take is <=15 deg., and the improvement factor of the side lobe level is about maximum 4dB, and therefore, the array antenna is not suitable for practical use experimentally. If the position P of the maximum phase quantity is larger than 0.7, the improvement factor of the side lobe level is degraded and the gain is reduced according as the position P of the maximum phase quantity is made larger, and therefore, the array antenna is not suitable for practical use experimentally. Thus, the range of the position P of the maximum phase quantity is limited to 0.4<=P<=0.7.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は複数の素子アンテナを有す6アレーアンテナ
に関するものである、 〔従来技術〕 第1図は従来のアレーアンテナを示す図でアシ。
[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to a six-array antenna having a plurality of element antennas. [Prior Art] Fig. 1 is a diagram showing a conventional array antenna.

第1図において、  (1a)〜(1n)は素子アンテ
ナ。
In FIG. 1, (1a) to (1n) are element antennas.

(2)は電力分配器でおる。(2) is handled by a power divider.

従来この種のアンテナにおいては、放射パターンの形灰
において素子アンテナ(1a)〜(1n)の振幅を電力
分配器(2)により設定し位相は等位相とする。このた
め、地面や海面等か二の反射の影響ケ少な(するために
上記アレーアンテナのサイドローブレベルな低減すせる
:う、素子アンテナ(1a)〜(1n)の振幅を設定す
るとアンテナの効工が低下する(例えば、サイドローブ
レベル−30dBの効工は約85チであり、−4DdB
の効工は約70%となる)という欠点があつ念。
Conventionally, in this type of antenna, the amplitudes of the element antennas (1a) to (1n) are set by the power divider (2) and the phases are made equal in the shape of the radiation pattern. For this reason, the influence of reflections from the ground, sea surface, etc. is small (in order to reduce the side lobe level of the array antenna described above), setting the amplitude of the element antennas (1a) to (1n) will reduce the effect of the antenna. (For example, the effect of a sidelobe level of -30 dB is approximately 85 cm, which is -4 D dB.
However, there is a drawback that the effectiveness of this method is approximately 70%.

〔発明の概要〕[Summary of the invention]

この発明はこのような従来の問題点を改善するためにな
づハたものであり、放射パターンを非対称化して片側の
サイドローブレベルを低減させるような位相を素子アン
テナに設定することによりアンテナ効率を低下すせるこ
となく電気特性の良好なアレーアンテナを提供するもの
である。
This invention was developed to improve these conventional problems, and improves antenna efficiency by setting a phase in the element antenna that makes the radiation pattern asymmetric and reduces the side lobe level on one side. The present invention provides an array antenna with good electrical characteristics without deteriorating the electrical characteristics.

〔発明の実施例〕[Embodiments of the invention]

第2図はこの発明の一実施例を示す図であり。 FIG. 2 is a diagram showing an embodiment of the present invention.

第2図において+  (1a)〜(1n)は素子アンテ
ナ。
In FIG. 2, + (1a) to (1n) are element antennas.

(2)は電力分配器、  (3a)〜(3n)は位相調
整器である。
(2) is a power divider, and (3a) to (3n) are phase adjusters.

第3図(A)は、上記素子アンテナ(1a) 〜(In
)に与える励振振幅であシ、第3図の)は励振位相であ
る。
FIG. 3(A) shows the element antennas (1a) to (In
) in FIG. 3 is the excitation phase.

ただし、素子アンテナのアレーアンテナに対する位置は
アレーアンテナ長で正規化しである。
However, the position of the element antenna with respect to the array antenna is normalized by the array antenna length.

第3図(J3)に示すように、素子アンテナ(1a)〜
(1n)の入力信号の位相φ(x)を上記素子アンテナ
(1a)〜(1n)に接続される位相調整器(5a)〜
(3n)を、甲いて、 fllえはアレーアンテナの中
心を基泡として、第(1)式のように調=hEする〇た
だし、(6Ml−を最大位相量、Pは最大位相量φMの
位W、Xはアレーアンテナ上の位置でおる。
As shown in Figure 3 (J3), element antennas (1a) to
The phase adjuster (5a) to which the phase φ(x) of the input signal of (1n) is connected to the element antennas (1a) to (1n)
(3n), with the center of the array antenna as the base bubble, tune = hE as shown in equation (1)〇However, (6Ml- is the maximum phase amount, P is the maximum phase amount φM) Positions W and X are the positions on the array antenna.

こねより、アレーアンテナの放射/くターンE (u)
は、第12)式で表わすれる。
Radiation of array antenna/kuturn E (u)
is expressed by equation 12).

+ま ただし、A(x)は素子アンテナの励掻去幅、u=2π
地θ/λ(λは使用波長)でおる。
+ However, A(x) is the excitation and removal width of the element antenna, u = 2π
The ground is θ/λ (λ is the wavelength used).

第4図は、この発明による一実施例におりて。FIG. 4 shows an embodiment according to the present invention.

素子アンテナ(1a)〜(1n)の励振振幅A (x)
を邸(x’+で与えた場合のサイドローブレベルが従米
の等位相分布を与えた場合に比牧し、3dB 以上改善
吏れる励振位相φ(x)の最大位相量φMと最大位相量
の位iPの関係を示すものであり第(31式%式% 算(31式において、最大位相量の位置Pのぐ囲がP 
(0,3の場合は第(21式の計算結果から最大位相量
φ基のとりうる値け15°以下と小すぐかつサイドロー
ブレベルの改善度は最大で4 dB 8度と小言い念め
経験上実用に適づない。また、最大位相量の位[Pの範
囲がP〉07の場合は最大位相量の位cpを大き(する
に従ってサイドローブレベルの改善度は低下しかつ利得
も低下するため経験上実用に適さな論。上記理由により
第(3)式における最大位相量の位ET’ Pのとりう
る範囲は0.3≦P≦07に限定すれる。
Excitation amplitude A (x) of element antennas (1a) to (1n)
The maximum phase amount φM of the excitation phase φ(x) and the maximum phase amount of which the sidelobe level when given by It shows the relationship between the position P and the position P of the maximum phase amount.
(In the case of 0, 3, the calculation result of Equation 21 shows that the possible value of the maximum phase amount φ base is 15 degrees or less, and the sidelobe level improvement is at most 4 dB 8 degrees. From experience, it is not suitable for practical use.Also, if the range of the maximum phase amount [P is P>07, increase the maximum phase amount cp (as the degree of improvement in the sidelobe level decreases and the gain also decreases). Therefore, it is a theory suitable for practical use based on experience.For the above reason, the possible range of the maximum phase amount ET'P in equation (3) is limited to 0.3≦P≦07.

第5図は第(3)式に基づき最大位相量φMを35’。In FIG. 5, the maximum phase amount φM is 35' based on equation (3).

最大位相量の位置Pを0.575の励蚤位相φ(x)を
与えfc場合と従来の等位相分布を与えfC場合の放射
パターンの比較を示すもめで、aけこの発明による実施
例の放射パターン、bは従来の放射パターンである。
This is a discussion to compare the radiation patterns of the case where the position P of the maximum phase amount is given an excitation phase φ(x) of 0.575 and fc and the conventional case where an equal phase distribution is given and fC. Radiation pattern b is a conventional radiation pattern.

上記方法Vcz flば、第5図に示すように、地面や
海面等からの反射の影響を受ける側のサイドローブレベ
ルをアンテナの効二を低下すぜることなく太幅に改善で
き良好な電気性能ケ得ることができるO 々お、上記説明では第2図に示す直線状に配列されたア
レーアンテナにつ込て述べたが1面状に配列さf′Lf
c場合についても同様に実施可能である。
If the above method Vcz fl is used, as shown in Fig. 5, the sidelobe level on the side affected by reflection from the ground, sea surface, etc. can be greatly improved without reducing the effectiveness of the antenna. Performance can be obtained.In the above explanation, we have focused on the linearly arranged array antenna shown in Fig. 2, but when the array antenna is arranged in one plane,
The same implementation is possible for case c.

また、実施例では素子アンテナ(1)と電力分配器12
)との間に位相調整器(3)を挿入する場合について述
べたが、素子アンテナと電力分配器との間の線路の長さ
を変えることによっても実施可能である。
In addition, in the embodiment, the element antenna (1) and the power divider 12
), but this can also be implemented by changing the length of the line between the element antenna and the power divider.

〔発明の効果〕   ・ 以上説明したように、この発明によれば素子アンテナの
励振位相分布を折れ線状に設定し放射ノ〈ターンを非対
称化することにより、アンテナ効率を低下;せることな
(電気特性の良好なアレーアンテナが実現できるという
効果がある。
[Effects of the Invention] - As explained above, according to the present invention, by setting the excitation phase distribution of the element antenna in a polygonal manner and making the radiation turn asymmetrical, antenna efficiency can be prevented from decreasing (electrical This has the effect of realizing an array antenna with good characteristics.

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

第1図は従来のアレーアンテナの構成図、算2図はこの
発明による7レーアンテナの一実施例の構成図、第3図
(A)はこの発明のアレーアンテナtこおける励振キ幅
を示す図、第3財1 (B)はこの発明のアレー了ンテ
ナにおける1かノ振位相を示す図、第4図はこの発明の
アレーアンテナにおける励振位相の最大位相量と最大位
相量の位rの関係を示す図。 第5図はこの発明によるアレーアンテナと従来のアレー
アンテナの指向特性の比較牙でおる。 図中、  (Ia)〜Nn)h素子アンテナ、(2)は
電力分配器、  (3a)〜(3n)は位相=X器であ
る。 なお1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。
Fig. 1 is a block diagram of a conventional array antenna, Fig. 2 is a block diagram of an embodiment of a 7-ray antenna according to the present invention, and Fig. 3 (A) shows the excitation amplitude in the array antenna according to the present invention. Figure 3, Part 1 (B) is a diagram showing the oscillation phase of 1 or more in the array antenna of the present invention, and Figure 4 is a diagram showing the maximum phase amount of the excitation phase and the position r of the maximum phase amount in the array antenna of the present invention. Diagram showing relationships. FIG. 5 compares the directivity characteristics of the array antenna according to the present invention and the conventional array antenna. In the figure, (Ia) to Nn) are h-element antennas, (2) is a power divider, and (3a) to (3n) are phase=X devices. Note that in FIG. 1, the same or corresponding parts are designated by the same reference numerals.

Claims (2)

【特許請求の範囲】[Claims] (1)複数の素子アンテナと各素子アンテナへ電力を分
配する電力分配器とを備えたアレーアンテナにおいて、
上記各素子アンテナそれぞれに放射パターンを非対称化
し、かつその放射パターンの片側のサイドローブレベル
を低減させる励振位相φ_M(x+1)/(1−p)(
−1≦x≦−p)、−φ_M/p(−p≦x≦p)、φ
_M(x−1)/(1−p)(p≦x≦1) 〔ただし、xはアレーアンテナ長で正規化したアンテナ
上の距離、φ_Mは最大位相量、pは最大位相量の位置
。〕 を設定する位相調整手段を設けたことを特徴とするアレ
ーアンテナ。
(1) In an array antenna equipped with a plurality of element antennas and a power divider that distributes power to each element antenna,
An excitation phase φ_M (x+1)/(1-p)(
−1≦x≦−p), −φ_M/p(−p≦x≦p), φ
_M(x-1)/(1-p) (p≦x≦1) [where x is the distance on the antenna normalized by the array antenna length, φ_M is the maximum phase amount, and p is the position of the maximum phase amount. ] An array antenna characterized by being provided with phase adjustment means for setting.
(2)上記励振位相において、最大位相量φMの範囲を
35P−5≦φ_M≦210P−50(0.3≦P≦0
.7)とすることを特徴とする特許請求範囲第(1)項
記載のアレーアンテナ。
(2) In the above excitation phase, the range of the maximum phase amount φM is 35P-5≦φ_M≦210P-50 (0.3≦P≦0
.. 7) The array antenna according to claim (1), characterized in that:
JP20351384A 1984-09-28 1984-09-28 Array antenna Granted JPS6181003A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20351384A JPS6181003A (en) 1984-09-28 1984-09-28 Array antenna

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20351384A JPS6181003A (en) 1984-09-28 1984-09-28 Array antenna

Publications (2)

Publication Number Publication Date
JPS6181003A true JPS6181003A (en) 1986-04-24
JPH0473644B2 JPH0473644B2 (en) 1992-11-24

Family

ID=16475394

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20351384A Granted JPS6181003A (en) 1984-09-28 1984-09-28 Array antenna

Country Status (1)

Country Link
JP (1) JPS6181003A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60197001A (en) * 1984-03-21 1985-10-05 Mitsubishi Electric Corp Array antenna

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60197001A (en) * 1984-03-21 1985-10-05 Mitsubishi Electric Corp Array antenna

Also Published As

Publication number Publication date
JPH0473644B2 (en) 1992-11-24

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