JPH0260147B2 - - Google Patents

Info

Publication number
JPH0260147B2
JPH0260147B2 JP58188538A JP18853883A JPH0260147B2 JP H0260147 B2 JPH0260147 B2 JP H0260147B2 JP 58188538 A JP58188538 A JP 58188538A JP 18853883 A JP18853883 A JP 18853883A JP H0260147 B2 JPH0260147 B2 JP H0260147B2
Authority
JP
Japan
Prior art keywords
antenna
antennas
spacing
pair
frequency
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 - Lifetime
Application number
JP58188538A
Other languages
Japanese (ja)
Other versions
JPS6080780A (en
Inventor
Akihiro Yasujima
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.)
Koden Electronics Co Ltd
Original Assignee
Koden Electronics Co Ltd
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 Koden Electronics Co Ltd filed Critical Koden Electronics Co Ltd
Priority to JP18853883A priority Critical patent/JPS6080780A/en
Publication of JPS6080780A publication Critical patent/JPS6080780A/en
Publication of JPH0260147B2 publication Critical patent/JPH0260147B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S3/00Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic or electromagnetic waves, or particle emission, not having a directional significance, are being received
    • G01S3/02Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic or electromagnetic waves, or particle emission, not having a directional significance, are being received using radio waves
    • G01S3/14Systems for determining direction or deviation from predetermined direction
    • G01S3/52Systems for determining direction or deviation from predetermined direction using a receiving antenna moving, or appearing to move, in a cyclic path to produce a Doppler variation of frequency of the received signal
    • G01S3/54Systems for determining direction or deviation from predetermined direction using a receiving antenna moving, or appearing to move, in a cyclic path to produce a Doppler variation of frequency of the received signal the apparent movement of the antenna being produced by coupling the receiver cyclically and sequentially to each of several fixed spaced antennas

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Variable-Direction Aerials And Aerial Arrays (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はアンテナ配置円を大口径化して設置環
境による擾乱誤差を低減する方位測定用アンテナ
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 for azimuth measurement that reduces disturbance errors caused by the installation environment by increasing the diameter of the antenna arrangement circle.

〔従来の技術〕[Conventional technology]

アンテナ配置円を大口径化することにより、方
位測定信号に対する設置環境にある微小擾乱物体
からの再輻射波の影響を少なくして、設置環境誤
差を少なくし得ることは、文献:昭和32年8月コ
ロナ社発行〔無線方位測定機〕§58.Site Error
の項などにより開示されている。
By increasing the diameter of the antenna arrangement circle, it is possible to reduce the influence of re-radiated waves from minute disturbance objects in the installation environment on the direction measurement signal, and to reduce the installation environment error, as shown in the document: 1958 8. Published by Moon Corona Co., Ltd. [Radio Direction Measuring Device] §58.Site Error
This is disclosed in the following sections.

そして、こうした大口径化のアンテナ装置とし
ては、循環切換ドツプラー型位相変調式のもの、
循環切換ウーレンウエバ型振幅変調式のものなど
によるアンテナ装置が周知である。
These large-diameter antenna devices include circular switching Doppler phase modulation type antennas,
2. Description of the Related Art Antenna devices such as those of the circulating switching Uhlenweber type and amplitude modulation type are well known.

また、2つのアンテナやループアンテナの出力
に接続した変成器の1次側中点からセンス決定用
信号を得るようにした構成が上記文献§18.単向
決定用回路諸方式の項第43図などにより開示さ
れている。
In addition, the configuration in which the sense determination signal is obtained from the midpoint of the primary side of the transformer connected to the outputs of two antennas or loop antennas is shown in Figure 43 of the above-mentioned document, §18. Unidirectional determination circuit systems. It has been disclosed by et al.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上記のような従来の大口径化したアンテナ装置
では、アンテナ切換接続構成や方位測定信号の検
出構成の部分、つまり、受信部分や表示部分が比
較的複雑であるため、こうした構成部分を簡便化
した構成により、安価に提供し得るようにした方
位測定用アンテナ装置が期待されているという課
題がある。
In the conventional large-diameter antenna device as described above, the antenna switching connection configuration and direction measurement signal detection configuration, that is, the receiving part and display part, are relatively complex. There is a problem in that there are expectations for an antenna device for azimuth measurement that can be provided at low cost due to its configuration.

〔課題を解決するための手段〕[Means to solve the problem]

本発明は、上記のような アンテナ配置の口径を直径とする円周上に配置
した複数のアンテナのうちから、同時に2つのア
ンテナを選択して順次に切換接続し、2つのアン
テナの各出力の位相差を検出することにより方位
測定用信号を得るとともに、各出力が接続された
変成器の中点からセンス決定用信号を得るように
して方位測定用アンテナ装置であつて、 上記に同時に選択する2つのアンテナの間隔、
つまり、アンテナ間隔を最高測定周波数の波長の
3/4程度に設定してアンテナ対とするとともに、
4対以上のアンテナ対を、各アンテナ対を交叉さ
せずに、上記の円周上に沿つて配置するアンテナ
配置手段と、 各切換接続における各アンテナ対の各出力を1
個の変成器に接続して得られる位相差の信号にも
とづいて上記の方位測定用信号を得る方位測定信
号手段と、 を設けるなどにより、アンテナ配置の口径を大口
径化して、上記の課題を解決し得るようにしたも
のである。
The present invention selects two antennas at the same time from among a plurality of antennas arranged on a circumference whose diameter is the aperture of the antenna arrangement as described above, sequentially switches and connects them, and outputs each output of the two antennas. The antenna device for direction measurement obtains a direction measurement signal by detecting a phase difference, and also obtains a sense determination signal from the midpoint of the transformer to which each output is connected, and simultaneously selects the above. the distance between the two antennas,
In other words, while setting the antenna spacing to about 3/4 of the wavelength of the highest measurement frequency and forming an antenna pair,
Antenna arrangement means for arranging four or more antenna pairs along the circumference without intersecting each antenna pair;
The above problem can be solved by increasing the diameter of the antenna arrangement by providing a direction measurement signal means for obtaining the above direction measurement signal based on the phase difference signal obtained by connecting to the transformer. It was designed to be solvable.

〔実施例〕〔Example〕

以下、図により実施例を説明する。 Examples will be described below with reference to figures.

第1図は本発明の原理的構成を示すもので、図
のように、アンテナ配置の口径Dの円周上に間隔
Sをもつて配置した1対のアンテナ1,2の各出
力は口径Dの中心に設けた変成器301に接続さ
れており、間隔Sをもつ従来のアドコツクアンテ
ナと相似の構成のものを1対だけ口径Dの円周上
に配置した構成になつている。
FIG. 1 shows the basic configuration of the present invention. As shown in the figure, each output of a pair of antennas 1 and 2 arranged with an interval S on the circumference of the antenna diameter D is The antenna is connected to a transformer 301 provided at the center of the antenna, and has a configuration in which only one pair of antennas having a configuration similar to that of a conventional adkotok antenna with a spacing S are arranged on the circumference of an aperture D.

そして、変成器301の二次側出力には2本の
アンテナの位相差に相当する電圧が、またこの変
成器の1次側の中点からは、2本のアンテナの和
(位相和)出力がとり出されるようになつている。
The secondary output of the transformer 301 has a voltage corresponding to the phase difference between the two antennas, and the midpoint of the primary side of this transformer outputs the sum (phase sum) of the two antennas. are being taken out.

今第1図の如き方向より電波が到来したとし、
アンテナ1,2を口径Dなる円周上に沿つて回転
させたとすれば、変成器301の差出力端子に
は、2本のアンテナの中心と電波の到来方向との
なす角度θのcosに比例し、且つ、アンテナの間
隔S(但しSが波長λに比し無視し得る場合)に
よつて決まる第2図の如き位相差出力が得られ
る。
Now suppose that radio waves arrive from the direction shown in Figure 1,
If antennas 1 and 2 are rotated along the circumference with aperture D, the difference output terminal of transformer 301 will have a value proportional to the cos of the angle θ between the center of the two antennas and the direction of arrival of the radio wave. In addition, a phase difference output as shown in FIG. 2 determined by the antenna spacing S (provided that S is negligible compared to the wavelength λ) can be obtained.

これは間隔Sのアンテナをこの口径の中心で回
転させた場合と同等の指向特性で、回転させるア
ンテナの口径の大きさには無関係である。
This is the same directivity characteristic as when an antenna with a spacing S is rotated around the center of this aperture, and is independent of the size of the aperture of the rotated antenna.

つまり、一般的に、電波の発射地点からアンテ
ナ装置の設置地点までの距離に対して口径Dが無
視できる程度に小さいので、実際には、アンテナ
1,2は口径Dの半径1/2Dをもつて回転してい
るが、この半径が無視されて口径Dの中心で回転
しているものと同様にみなされるわけである。
In other words, in general, the aperture D is so small that it can be ignored relative to the distance from the radio wave emission point to the installation point of the antenna device, so antennas 1 and 2 actually have a radius 1/2D of the aperture D. However, this radius is ignored and it is treated as if it were rotating around the center of the aperture D.

したがつて、従来のアドコツクアンテナの出力
と同様のもの方位測定用信号が得られることにな
る。
Therefore, an azimuth measurement signal similar to the output of a conventional adkotok antenna can be obtained.

つまり、第3図はアンテナの間隔Sと波長λの
比S/λをパラメータとした周知のアドコツクア
ンテナの指向特性sin(πS/λ・cosθ)を示したもの であるが、間隔Sの2本のアンテナを円周上に沿
つて回転させた場合の位相差出力も、第3図と全
く同様の指向特性となることは明らかである。
In other words, Fig. 3 shows the directivity characteristic sin (πS/λ・cosθ) of the well-known adkotok antenna with the ratio S/λ of the antenna spacing S and the wavelength λ as a parameter. It is clear that the phase difference output when the book antenna is rotated along the circumference also has the same directivity characteristics as shown in FIG. 3.

この出力電圧の位相は、到来電波の方向とアン
テナの回転方向との関係によつて定まり、この2
つの方向が一致している場合と逆反方向とで位相
が180゜異なるが、これはアドコツクアンテナの出
力の位相が到来方向の正反によつて180゜異なるの
と同様である。
The phase of this output voltage is determined by the relationship between the direction of the arriving radio wave and the rotation direction of the antenna.
The phase differs by 180 degrees when the directions of arrival are the same and when they are in the opposite direction. This is similar to the fact that the phase of the output of an adkotok antenna differs by 180 degrees depending on whether the direction of arrival is opposite.

以上の構成により得られる出力のみではセンス
の不確定性があり、何らかの手段で、センス決定
用の信号を得る必要がある。
There is uncertainty in sensing with only the output obtained by the above configuration, and it is necessary to obtain a signal for sensing determination by some means.

このため、上記の文献により開示されているよ
うに変成器301の1次側の中点からセンス決定
用信号を得る手段を利用することが考えられる。
For this reason, it is conceivable to use means for obtaining a sense determination signal from the midpoint of the primary side of the transformer 301, as disclosed in the above-mentioned literature.

つまり、2本のアンテナの和出力は、それぞれ
のアンテナ出力のベクトル和にほかならないか
ら、第4図に示すように和出力が差出力と必ず90
度の位相差を有するので、この和出力の位相を約
90度変え、差出力と同位相(若しくは反対位相)
として合成すればセンスを決定することができ
る。
In other words, the sum output of two antennas is nothing but the vector sum of their respective antenna outputs, so as shown in Figure 4, the sum output is always equal to the difference output by 90
Since there is a phase difference of approximately
Changed by 90 degrees, same phase as difference output (or opposite phase)
The sense can be determined by synthesizing it as

第5図はS/λをパラメータとした2本のアン
テナの位相和特性cos(πS/λ・cosθ)を示したもの で、S/λは第3図と対比させて示してある。図
のようにSがλに比し小さいときは和特性はほぼ
円に近いが、Sが0.5λに近ずくに従つて楕円状と
なり、S=0.5λのとき0度と180度方向で出力が
零となる8字状特性となる。Sが0.5λ以上になる
とSが丁度0.5λとなる方向があるためこの点で出
力が零となる。この方向は各象限に生じるから結
局S/λで決る特定方向で出力が零になる4葉状
の出力特性となる(図のS=0.75λと1λの特性参
照)。しかし既に述べたように和特性の位相は、
これら特性如何にかかわらず、また到来方向に無
関係に1本の垂直アンテナの位相と同様変化しな
いから、これを利用してセンス決定を行なうこと
ができる。
FIG. 5 shows the phase sum characteristic cos (πS/λ·cos θ) of two antennas with S/λ as a parameter, and S/λ is shown in comparison with FIG. As shown in the figure, when S is small compared to λ, the sum characteristic is almost circular, but as S approaches 0.5λ, it becomes elliptical, and when S = 0.5λ, the output is in the 0 degree and 180 degree directions. It becomes a figure-of-eight characteristic where is zero. When S becomes 0.5λ or more, there is a direction in which S is exactly 0.5λ, so the output becomes zero at this point. Since this direction occurs in each quadrant, the result is a four-lobed output characteristic in which the output becomes zero in a specific direction determined by S/λ (see the characteristics of S=0.75λ and 1λ in the figure). However, as already mentioned, the phase of the sum characteristic is
Regardless of these characteristics or irrespective of the direction of arrival, the signal does not change like the phase of a single vertical antenna, so this can be used to make sense decisions.

第6図はこのセンス合成特性を示したもので、
第3図と第5図の特性をそのまま用い、且つ、和
出力の90度位相変換損失を無視し、1:1で合成
したときを示したものである。Sが0.5λ以上にな
つた場合複雑なセンス波形となるが、本発明によ
るアンテナ間隔の限界に近いS=0.75λのときで
も満足できるセンス波形が得られることがわか
る。
Figure 6 shows this sense synthesis characteristic.
This figure shows the case where the characteristics of FIGS. 3 and 5 are used as they are, and the 90-degree phase conversion loss of the sum output is ignored, and they are combined at a ratio of 1:1. When S becomes 0.5λ or more, the sense waveform becomes complicated, but it can be seen that a satisfactory sense waveform can be obtained even when S=0.75λ, which is close to the limit of the antenna spacing according to the present invention.

以上が本発明による方位測定用アンテナ装置の
原理であるが、実際には1対のアンテナを回転さ
せる代りに、アンテナを円周上に配列し、中心に
設けたアンテナ切換器401により、1対づつア
ンテナを循環状に順次切換え、差と和の出力を得
るようにしている。
The above is the principle of the antenna device for direction measurement according to the present invention, but in reality, instead of rotating a pair of antennas, the antennas are arranged on the circumference, and the antenna switcher 401 provided at the center is used to connect the antennas to one pair. The antennas are sequentially switched in a circular manner to obtain the difference and sum outputs.

第7図はn本のアンテナを円周上に等間隔に配
列した一例で(以下等間隔配置と云う)、アンテ
ナ素子の間隔Sは最高測定周波数によつて決ま
り、またアンテナの口径Dはアンテナ素子数nに
よつて決る。今、仮りにSを0.7λとし最高測定周
波数を30MHzとすると、n=12本でDは約27m、
n=18本でDは約40λとなる。またVHFやUHF
帯ではダイポールアンテナなどを使用するが、
500MHzの場合n=12本でDは約1.6m、n=18本
ではDは約2.4mとなる。
Figure 7 shows an example in which n antennas are arranged at equal intervals on the circumference (hereinafter referred to as equal interval arrangement), where the antenna element spacing S is determined by the highest measurement frequency, and the antenna aperture D is determined by the antenna Determined by the number of elements n. Now, if S is 0.7λ and the highest measurement frequency is 30MHz, then D is approximately 27m with n = 12 lines.
When n=18, D is approximately 40λ. Also VHF and UHF
In the band, dipole antennas are used, but
In the case of 500MHz, when n=12 lines, D is about 1.6 m, and when n=18 lines, D is about 2.4 m.

これを従来の循環切換ドツプラー型の場合のも
のと比較してみると、循環切換ドツプラー型の場
合には、切換接続するアンテナ間の間隔、つま
り、本発明における間隔Sに相当する間隔が最大
0.4〜0.5程度である。
Comparing this with that of the conventional circulating switching Doppler type, it is found that in the case of the circulating switching Doppler type, the distance between the switchingly connected antennas, that is, the distance corresponding to the spacing S in the present invention is the maximum.
It is about 0.4 to 0.5.

これに対して、本発明における間隔Sは0.75λ
程度にできるので、同一のアンテナ数の場合で
も、本発明の方が口径Dを約1.5倍に大きくでき
ることがわかる。
On the other hand, the spacing S in the present invention is 0.75λ
It can be seen that even if the number of antennas is the same, the diameter D can be made approximately 1.5 times larger in the present invention.

また、従来のアドコツクアンテナ型の場合のも
のと比較してみると、アドコツクアンテナ型の場
合には、上記のように口径Dの最大値を3/4λ程
度にできるのが限度であり、、これをアンテナ配
置の円周上で見ると、その1/√2の間隔、つま
り、約0.53λの間隔になる。
Also, when compared with the conventional adkotoku antenna type, in the case of the adkotoku antenna type, the maximum value of the aperture D can be approximately 3/4λ as mentioned above. , if you look at this on the circumference of the antenna arrangement, it will be an interval of 1/√2, that is, an interval of about 0.53λ.

これに対して、本発明の場合には、円周上にお
けるアンテナ間の間隔Sを3/4λ程度にしている
ので、同一アンテナ数の場合でも、アドコツクア
ンテナと同様に4本のアンテナを配置した場合で
も、本発明の方が口径Dを約1.4倍に大きくでき
ることがわかる。
On the other hand, in the case of the present invention, the spacing S between the antennas on the circumference is set to about 3/4λ, so even if the number of antennas is the same, four antennas are arranged like the adkotok antenna. It can be seen that even in this case, the diameter D can be increased by about 1.4 times in the present invention.

アンテナの切換えはアンテナ切換器401に設
けた切換素子により行ない切換パルスによりアン
テナ1と2、2と3、3と4……の如く2本のア
ンテナを同時に切換え、1個の出力変換器により
差と和の出力をとり出すようにする。第8図はこ
の切換えによつて得られた差出力の信号波形の一
例を示したもので、この出力を増幅後、AM検波
しフイルタにより整形すれば図の点線の如き波形
が得られる。また和出力も第9図の如き階段状波
となるが同様フイルタにより整形される。これら
波形はゴニオメータ回転方式における出力波形と
同様であるから、切換周期と同期したCRT円形
掃引信号を変調し到来方向をプロペラ映像やセン
ス映像として表示でき方位測定を行なうことがで
きる。また到来方位のデジタル表示も既知の手段
により実施できる。
Antenna switching is performed by a switching element provided in the antenna switching device 401. Two antennas are switched at the same time, such as antennas 1 and 2, 2 and 3, 3 and 4, etc., using a switching pulse, and a single output converter is used to output the difference. and output the sum. FIG. 8 shows an example of the signal waveform of the difference output obtained by this switching. If this output is amplified, AM detected, and shaped by a filter, a waveform as shown by the dotted line in the figure can be obtained. The sum output also becomes a step-like wave as shown in FIG. 9, which is shaped by a filter in the same way. Since these waveforms are similar to the output waveforms in the goniometer rotation method, the direction of arrival can be displayed as a propeller image or sense image by modulating the CRT circular sweep signal synchronized with the switching cycle, and the direction can be measured. Digital display of the direction of arrival can also be performed by known means.

第7図のように多数のアンテナが配置されてい
るものでは、切換接続によつて使用されていない
アンテナと使用しているアンテナとが比較的近い
位置に配置されるため、使用していないアンテナ
からの再輻射やアンテナ間の干渉などが方位測定
に影響を与えるため、方位測定周波数に対応し
て、アンテナ基部を接地または解放し、あるいは
インピーダンスを挿入するなどにより、この影響
を少なくする手段が、従来のものでも用いられて
いるが、本発明の構成においても、勿論、これと
同様の手段により対処する必要があることは言う
までもない。
When a large number of antennas are arranged as shown in Figure 7, the unused antennas and the used antennas are placed relatively close to each other due to switching connections, so the unused antennas Since re-radiation from antennas and interference between antennas affect direction measurement, there are ways to reduce this effect by grounding or opening the antenna base, or inserting impedance, depending on the direction measurement frequency. , is also used in the conventional system, but it goes without saying that it is necessary to take measures similar to this in the configuration of the present invention as well.

これに反し、2本のアンテナをm組対称的に配
列する方式(以下、対称配置方式と云う)は、第
10図の如く組になるアンテナを円周上に対称的
に配列するもので、組になるアンテナ数は最小4
組でもよいが、通常8組または8組の整数倍とす
る。この対称配置の場合、組になるアンテナの間
隔Sは等間隔配置の場合と同様であるが、アンテ
ナの口径は任意に選定できる特徴がある。例えば
8組のアンテナのとき、最高測定周波数が30MHz
でもアンテナ口径を100mにまた500MHzのときで
もアンテナ口径を20m程度にすることができる。
従つて大口径アンテナによる特徴をより一層発揮
でき、また使用していない他のアンテナの影響も
小さくすることができる。
On the other hand, the method of symmetrically arranging m sets of two antennas (hereinafter referred to as the symmetric arrangement method) arranges the antennas in pairs symmetrically on the circumference as shown in Figure 10. Minimum number of antennas in a set is 4
Although it may be a set, it is usually 8 sets or an integral multiple of 8 sets. In the case of this symmetrical arrangement, the spacing S between the antennas in the set is the same as in the case of equally spaced arrangement, but the diameter of the antennas can be arbitrarily selected. For example, when using 8 sets of antennas, the maximum measurement frequency is 30MHz
However, the antenna diameter can be set to 100 m, or even at 500 MHz, the antenna diameter can be set to about 20 m.
Therefore, the characteristics of the large-diameter antenna can be further exhibited, and the influence of other antennas that are not used can also be reduced.

第10図はアンテナを8組使用した場合である
が、切換えはアンテナ1と2、3と4、5と6の
如く2本同時に順次切換える。得られた波形は第
9図と同様に階段状となるが、センス出力を含め
等間隔配置アンテナの場合と同様に処理し測定を
行なうことができる。
FIG. 10 shows a case where eight sets of antennas are used, and two sets of antennas such as antennas 1 and 2, antennas 3 and 4, and antennas 5 and 6 are switched sequentially at the same time. Although the obtained waveform has a step-like shape as in FIG. 9, it can be processed and measured in the same manner as in the case of evenly spaced antennas, including the sense output.

本発明は上記した2つの実施例のみに限定され
ることなく、本発明の要旨を変更しない範囲で
種々の変形を実施することができる。例えば第7
図において測定周波数の低い周波数帯において、
アンテナ素子1と3、3と5、5と7……または
1と3、2と4、3と5……のように飛越した間
隔の2本を組として切換え、アンテナ間隔を2倍
にして感度を向上させ、1と3のアンテナ間隔が
ほぼ0.7λになる周波数で1と2のアンテナに組合
せをもどす方法も可能である。
The present invention is not limited to the two embodiments described above, and various modifications can be made without departing from the gist of the present invention. For example, the seventh
In the figure, in the frequency band where the measurement frequency is low,
The antenna elements 1 and 3, 3 and 5, 5 and 7... or 1 and 3, 2 and 4, 3 and 5... are switched as a set with skipped spacing, and the antenna spacing is doubled. It is also possible to improve the sensitivity and return the combination to antennas 1 and 2 at a frequency where the distance between antennas 1 and 3 is approximately 0.7λ.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、以上のように、円周上に沿つ
て配置した隣接するアンテナ間のの間隔を最高測
定周波数の波長の3/4程度の間隔に設定してアン
テナ対を4対以上配置し、このアンテナ対を順次
に選択して1つの変成器に切換接続することによ
り、従来のアドコツクアンテナの場合と同様の方
位測定用信号を得ているため、方位測定用の受信
部分や表示部分については従来のアドコツクアン
テナの場合と同様に簡便な構成で済むにもかかわ
らず、アンテナ配置の口径を、従来の循環切換ド
ツプラー型に比べ約1.5倍、また、アドコツクア
ンテナの場合に比べ約1.4倍の大きさにできるの
で、上記の設置環境誤差を少なくし得る、ドツプ
ラー型のように、FM電波の測定に対して音声変
調成分を補正するような複雑な構成が不要になる
ため、装置全体を簡便安価にして提供し得るなど
の特長がある。
According to the present invention, as described above, four or more antenna pairs are arranged by setting the spacing between adjacent antennas arranged along the circumference to be about 3/4 of the wavelength of the highest measurement frequency. However, by sequentially selecting these antenna pairs and switching and connecting them to one transformer, a direction measurement signal similar to that of a conventional adkotok antenna is obtained, so the direction measurement receiving part and display are Although the configuration is as simple as that of a conventional adkotok antenna, the diameter of the antenna arrangement is approximately 1.5 times larger than that of a conventional circulation switching Doppler type, and compared to an adkotok antenna. Since it can be made approximately 1.4 times larger, it can reduce the installation environment error mentioned above, and it eliminates the need for a complicated configuration like the Doppler type, which corrects audio modulation components for FM radio wave measurements. It has the advantage that the entire device can be provided simply and inexpensively.

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

図面は実施例を示し、第1図はこの発明の原理
を示す説明図、第2図はこの原理によつて得られ
る位相差出力図、第3図は2本のアンテナの位相
差出力の特性即ちアドコツクアンテナの指向特性
を示したもの、第4図は2本のアンテナの位相差
と和を示すベクトル図、第5図は同2本のアンテ
ナの位相和特性図、第6図は第3図と第5図の差
と和出力の合成(センス)特性を各S/λにより
示したもの、第7図は本発明の実施例の1つであ
る等間隔配置方式の構成略図、第8図は第7図の
等間隔配置アンテナを切換えて得られた差出力
図、第9図は同アンテナの和出力図である。また
第10図は他の実施例の対称配置方式の構成略図
である。 1〜16,n……アンテナ、301……変成
器、401……アンテナ切換器、501……アン
テナ素子、601……アンテナ接続ケーブル。
The drawings show embodiments, FIG. 1 is an explanatory diagram showing the principle of the invention, FIG. 2 is a diagram of the phase difference output obtained by this principle, and FIG. 3 is the characteristic of the phase difference output of two antennas. In other words, Figure 4 shows the directivity characteristics of the Adkotoku antenna, Figure 4 is a vector diagram showing the phase difference and sum of the two antennas, Figure 5 is the phase sum characteristic diagram of the two antennas, and Figure 6 is the vector diagram showing the phase difference and sum of the two antennas. The difference between FIG. 3 and FIG. 5 and the combination (sense) characteristics of the sum output are shown by each S/λ. FIG. FIG. 8 is a difference output diagram obtained by switching the equally spaced antennas shown in FIG. 7, and FIG. 9 is a sum output diagram of the antennas. Further, FIG. 10 is a schematic diagram of the configuration of a symmetrical arrangement method of another embodiment. 1 to 16, n...Antenna, 301...Transformer, 401...Antenna switcher, 501...Antenna element, 601...Antenna connection cable.

Claims (1)

【特許請求の範囲】 1 アンテナ配置の口径を直径とする円周上に配
置した複数のアンテナのうちから、同時に2つの
アンテナを選択して順次に切換接続し、前記2つ
のアンテナの各出力の位相差を検出することによ
り方位測定用信号を得るとともに、前記各出力が
接続された変成器の中点からセンス決定用信号を
得るようにして方位測定用アンテナ装置であつ
て、 a 前記同時に選択する2つのアンテナの間隔
(以下、アンテナ間隔という)を最高測定周波
数の波長の3/4程度に設定してアンテナ対とす
るとともに、4対以上の前記アンテナ対を、各
アンテナ対を交叉させずに、前記円周上に沿つ
て配置するアンテナ配置手段と、 b 各前記切換接続における各アンテナ対の各出
力を1個の変成器に接続して得られる前記位相
差の信号にもとづいて前記方位測定用信号を得
る方位測定信号手段と を具備することを特徴とするアンテナ装置。 2 特許請求の範囲第1項記載のアンテナ装置で
あつて、 a 前記アンテナ対の各対の間に、前記アンテナ
間隔よりも大きい間隔であつて前記選択を行わ
ない間隔を設けて、前記アンテナを配置した前
記アンテナ配置手段 を具備するもの。 3 特許請求の範囲第1項記載のアンテナ装置で
あつて、 a 各前記アンテナ対の一対のアンテナを前記切
換接続の次順にあたるアンテナ対の一方のアン
テナと共通にして配置した前記アンテナ配置手
段 を具備するもの。 4 アンテナ配置の口径を直径とする円周上に配
置した複数のアンテナのうちから、同時に2つの
アンテナを選択して順次に切換接続し、前記2つ
のアンテナの各出力の位相差を検出することによ
り方位測定用信号を得るとともに、前記各出力が
接続された変成器の中点からセンス決定用信号を
得るようにした方位測定用アンテナ装置であつて
広帯域の周波数について方位測定を行うものにお
いて、 a 前記2つのアンテナ間の間隔(以下、定常の
アンテナ間隔という)を最高測定周波数の波長
の3/4程度に設定して前記円周上に配置する定
常間隔配置手段と、 b 前記定常間隔により配置されたアンテナを適
宜に飛び越して選択した2つのアンテナ間の間
隔(以下、飛越間隔という)が前記広帯域の中
間における周波数の波長の3/4程度になる周波
数(以下、帯域内中間周波数という)を設定す
る帯域内周波数設定手段と、 c 前記帯域内中間周波数より高い周波数の方位
測定に対しては、前記定常間隔による2つのア
ンテナ(以下、定常間隔アンテナ対という)を
選択して前記切換接続を行い、前記帯域内中間
周波数より低い周波数の方位測定に対しては、
前記飛越間隔による2つのアンテナ(以下、飛
越間隔アンテナ対という)を選択して前記切換
接続を行う切換接続選択手段と、 d 4対以上の前記飛越間隔アンテナ対を、各飛
越間隔アンテナ対を交叉させずに、前記円周上
に沿つて配置するアンテナ配置手段と、 e 各前記切換接続における各定常間隔アンテナ
対または各飛越間隔アンテナ対(以下、アンテ
ナ対という)の各出力を1個の変成器に接続し
て得られる前記位相差の信号にもとづいて前記
方位測定用信号を得る方位測定信号手段と を具備することを特徴とするアンテナ装置。 5 特許請求の範囲第4項記載のアンテナ装置で
あつて、 a 各前記定常間隔アンテナ対の一方のアンテナ
を前記切換接続の次順にあたる前記定常間隔ア
ンテナ対の一方のアンテナと共通にして配置
し、または、各前記飛越間隔アンテナ対の一方
のアンテナを前記切換接続の次順にあたる前記
飛越間隔アンテナ対の一方のアンテナと共通に
して配置した前記アンテナ配置手段 を具備するもの。
[Scope of Claims] 1. Two antennas are selected at the same time from among a plurality of antennas arranged on a circumference having a diameter equal to the diameter of the antenna arrangement, and the outputs of each of the two antennas are sequentially switched and connected. An antenna device for direction measurement, which obtains a direction measurement signal by detecting a phase difference, and also obtains a sense determination signal from the midpoint of a transformer to which each of the outputs is connected, wherein a. The spacing between the two antennas (hereinafter referred to as antenna spacing) is set to about 3/4 of the wavelength of the highest measurement frequency to form an antenna pair, and four or more of the antenna pairs are arranged without intersecting each antenna pair. (a) antenna arrangement means disposed along the circumference; (b) determining the orientation based on the phase difference signal obtained by connecting each output of each antenna pair in each of the switching connections to one transformer; An antenna device comprising: azimuth measurement signal means for obtaining a measurement signal. 2. The antenna device according to claim 1, characterized in that: (a) an interval is provided between each pair of the antenna pairs that is larger than the antenna interval and does not perform the selection; The antenna arranging means is provided with the antenna arranging means. 3. The antenna device according to claim 1, further comprising: (a) the antenna arrangement means in which one antenna of each of the antenna pairs is arranged in common with one antenna of the antenna pair that is next in the switching connection order; What to have. 4. Selecting two antennas at the same time from among a plurality of antennas arranged on a circumference whose diameter is the aperture of the antenna arrangement, sequentially switching and connecting them, and detecting the phase difference between the outputs of the two antennas. In an antenna device for measuring a direction, which obtains a signal for direction measurement from the midpoint of the transformer to which each of the outputs is connected, and obtains a signal for sense determination from the midpoint of the transformer to which each of the outputs is connected, the antenna device performs direction measurement over a wide band of frequencies, a) a steady spacing arrangement means for setting the spacing between the two antennas (hereinafter referred to as steady antenna spacing) to approximately 3/4 of the wavelength of the highest measurement frequency and arranging them on the circumference; b. A frequency at which the interval between two antennas selected by appropriately skipping the arranged antennas (hereinafter referred to as skipped interval) is approximately 3/4 of the wavelength of the frequency in the middle of the wide band (hereinafter referred to as in-band intermediate frequency) c. For direction measurement at a frequency higher than the in-band intermediate frequency, two antennas with the constant spacing (hereinafter referred to as a pair of constant spacing antennas) are selected and the switching connection is performed. For direction measurement at a frequency lower than the intermediate frequency within the band,
switching connection selection means for selecting two antennas based on the staggered spacing (hereinafter referred to as staggered spacing antenna pairs) and performing the switching connection; an antenna arranging means arranged along the circumference without causing any interference; an azimuth measurement signal means for obtaining the azimuth measurement signal based on the phase difference signal obtained by being connected to an antenna device. 5. The antenna device according to claim 4, wherein: (a) one antenna of each pair of regularly spaced antennas is arranged in common with one antenna of the pair of regularly spaced antennas that is next in the order of the switching connection. Or, the antenna arrangement means is arranged such that one antenna of each of the interlaced interval antenna pairs is arranged in common with one of the antennas of the interlaced interval antenna pair that is next in the switching connection order.
JP18853883A 1983-10-11 1983-10-11 Antenna device for measuring azimuth Granted JPS6080780A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18853883A JPS6080780A (en) 1983-10-11 1983-10-11 Antenna device for measuring azimuth

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18853883A JPS6080780A (en) 1983-10-11 1983-10-11 Antenna device for measuring azimuth

Publications (2)

Publication Number Publication Date
JPS6080780A JPS6080780A (en) 1985-05-08
JPH0260147B2 true JPH0260147B2 (en) 1990-12-14

Family

ID=16225454

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18853883A Granted JPS6080780A (en) 1983-10-11 1983-10-11 Antenna device for measuring azimuth

Country Status (1)

Country Link
JP (1) JPS6080780A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2787586B2 (en) * 1989-03-03 1998-08-20 株式会社光電製作所 Wireless direction finder

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4933916A (en) * 1972-07-29 1974-03-28

Also Published As

Publication number Publication date
JPS6080780A (en) 1985-05-08

Similar Documents

Publication Publication Date Title
US4328499A (en) Radio direction finding systems
RU2144200C1 (en) Process of direction finding of radio signals and multichannel direction finder
Welsby et al. Multiplicative receiving arrays
US5228006A (en) High resolution beam former apparatus
US4870420A (en) Signal acquisition apparatus and method
Asai et al. Multi-station system for solar wind observations using the interplanetary scintillation method
US2711533A (en) Multi-lobe omnidirectional radio navigation system
US4380010A (en) Phase directional antenna array and phased ring combiner for radio direction finding
GB2064257A (en) Radio direction finders
JPH0260147B2 (en)
US5568394A (en) Interferometry with multipath nulling
JPH0668542B2 (en) Holographic It Crader
US20060012518A1 (en) Method for enhancing the measuring accuracy in an antenna array
JP2544299B2 (en) Beam compression processing method of antenna pattern in radar
JPH0338548B2 (en)
GB2274953A (en) Navigation system incorporating screened two-loop antenna
JPH05299926A (en) Beam compression processing method for antenna pattern
JP2732302B2 (en) Radio direction measurement antenna system
JP2562763B2 (en) Antenna device
Mueller et al. Application of modern DOA algorithms to an Adcock array antenna
JPH0563749B2 (en)
JPS6352346B2 (en)
JPH06118154A (en) Direction detector
JPH0372950B2 (en)
JPS61270904A (en) Direction finder