JPS6080780A - Antenna device for measuring azimuth - Google Patents
Antenna device for measuring azimuthInfo
- Publication number
- JPS6080780A JPS6080780A JP18853883A JP18853883A JPS6080780A JP S6080780 A JPS6080780 A JP S6080780A JP 18853883 A JP18853883 A JP 18853883A JP 18853883 A JP18853883 A JP 18853883A JP S6080780 A JPS6080780 A JP S6080780A
- Authority
- JP
- Japan
- Prior art keywords
- antennas
- output
- antenna
- sum
- transformer
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO 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
- G01S3/00—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic or electromagnetic waves, or particle emission, not having a directional significance, are being received
- G01S3/02—Direction-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
- G01S3/14—Systems for determining direction or deviation from predetermined direction
- G01S3/52—Systems 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
- G01S3/54—Systems 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
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- 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)
Abstract
Description
【発明の詳細な説明】
本発明は電波の到来方向、即ち無線方位を測定する無線
方向探知装置(以下、方探と略す)に用いるアンテナ装
置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an antenna device used in a radio direction finding device (hereinafter abbreviated as direction finding) that measures the arrival direction of radio waves, that is, the radio direction.
従来のアトコックアンテナを用いた方探は、アンテナ素
子を多重素子としてもアンテナ口径を1波長以上にする
ことは不6」能であった。これに反し、ドツプラ方探や
ウーレンウエバ方探は、アンテナ口径を1波長以上任意
の口径とすることができ、このため広開口面化による測
定精度の向上。In a conventional directional search using an Atcock antenna, it was impossible to increase the antenna diameter to more than one wavelength even if the antenna element was a multiplex element. On the other hand, with Doppler square probes and Uhlen-Weber square probes, the antenna aperture can be set to any diameter of one wavelength or more, which improves measurement accuracy by widening the aperture surface.
偏波面変動による誤差の改善、 i<+1+定方位変動
の安定化、近接擾乱物体の影響の軽沢などが得られる特
徴を有している。It has the characteristics of improving errors caused by polarization plane fluctuations, stabilizing i<+1+ constant azimuth fluctuations, and reducing the effects of nearby disturbing objects.
本発明における2本のアンテナを1対とした大口径アン
テナ装置は、上記広開口面化と同等の特徴を得ることが
でき、且つ、このアンテナ装置を用いることにより、ド
ツプラ方探やウーレンウエバ方探の如き復雑な構成を必
要とすることなく、従来のゴニオメータ方探の既製技術
を利用して簡易な構成で高性能な方探を得ることができ
る。The large-diameter antenna device of the present invention, which has a pair of two antennas, can obtain the same characteristics as the above-mentioned wide aperture area, and by using this antenna device, it can be used for Doppler direction finding and Uhlen-Weber direction finding. It is possible to obtain a high-performance direction finder with a simple structure by using the ready-made technology of the conventional goniometer direction finder without requiring a complicated structure such as the above.
第1図はこの原理を示しだもので、間隔Sの1対のアン
テナ1,2を設け、その出力に変成器3旧を接続し、そ
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、丑たこの変成器の一次側の中点からは、2本のア
ンテナの和(位相和)出力がとシ出されるようになって
いる。Figure 1 shows this principle. A pair of antennas 1 and 2 with a spacing S is provided, a transformer 3 is connected to the output of the antenna, and the secondary output is connected to the phase difference between the two antennas. A voltage corresponding to the sum (phase sum) of the two antennas is output from the midpoint of the primary side of the transformer.
令弟1図の如き方向より電波が到来し7たとし、アンテ
ナ1,2を口径りなる円周上に沿っ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の弼に比例し、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)によって決まる第2図の如き位相差出力が得ら
れる。Assuming that radio waves arrive from the direction shown in Figure 1, and antennas 1 and 2 are rotated along the circumference of the aperture, the difference output terminal of the transformer 301 has two antennas. A phase difference output as shown in Fig. 2 is obtained, which is proportional to the angle θ between the center of It will be done.
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.
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トコックアンテナの指πS
同行性sl++ (>・弼θ)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KGって回転させた場
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。Figure 3 shows the well-known Atcock antenna finger πS concurrency sl++ (>・弼θ) using 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 two antennas with a spacing S are rotated by KG on the circumference will have 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って定まり、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、
これはアトコンクアンテナの出力の位相が到来方向の正
反によって1800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, and the phase differs by 180° depending on whether the two directions are the same or the opposite direction.
This is similar to the fact that the phase of the output of an atconch antenna differs by 1800 degrees depending on the direction of arrival.
ドツプラ方探では到来方向によって周波数変化や位相変
化の正負が決まる方位成分そのものを利用しているので
、センス決定を必要としないが、本発明では方位成分を
電圧として取出しているので別にセンス決定が必要とな
る。この場合アンテナの口径が1波長以上と々るため、
例えば口径の中心にセンスアンテナを設けてこれを利用
するとしても、センスの不確定が生じ使用できない。そ
こで回転する2本のアンテナにおいて方位成分と同時に
センス用の和出力を取出すようにすれば、そのアンテナ
の回転位置における方位成分とセンス成分が得られるの
で、センスの不確定性は解決される。Doppler direction searching uses the azimuth component itself, which determines whether the frequency change or phase change is positive or negative depending on the direction of arrival, and therefore does not require sense determination. However, in the present invention, the azimuth component is extracted as a voltage, so no separate sense determination is required. It becomes necessary. In this case, since the diameter of the antenna is more than one wavelength,
For example, even if a sense antenna is provided at the center of the aperture and used, the sense becomes uncertain and cannot be used. Therefore, if the sum output for sensing is extracted at the same time as the azimuth component from the two rotating antennas, the azimuth component and the sense component at the rotational position of the antennas can be obtained, and the sense uncertainty can be resolved.
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900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、i5[:l:S/λを
パラメータとした2本のアンチπS
すの位相和特性cos (T−cosθ)を示したもの
で、S/λは第3図と対比させて示しである。図のよう
KSがλに比し少さいときは和特性はほぼ円に近いか、
Sが05λに近ずくに従って楕円状となり、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
ができる。Since the sum output of two antennas is nothing but the vector sum of their respective antenna outputs, the sum output always has a phase difference of 900 degrees from the difference output as shown in Figure 4, so the phase of this sum output is The figure shows the phase sum characteristic cos (T-cosθ) of two anti-πS with i5[:l:S/λ as a parameter, and S/λ is compared with Fig. 3. This is an indication. As shown in the figure, when KS is small compared to λ, the sum characteristic is almost circular, or
As S approaches 05λ, it becomes elliptical, and S = 0
.. When the angle is 5λ, a figure-8 characteristic occurs in which the output is zero in the 0 degree and 180 degree directions. When S becomes 0.5λ or more, S becomes exactly 0.
Since there is a direction of 5λ, the output becomes zero at this point. Since this direction occurs in each quadrant, it becomes a four-lobed output characteristic in which the output becomes zero in a specific direction determined by S/λ (S =
(See characteristics of 0.75λ and 1λ). However, as mentioned above, the phase of the sum characteristic does not change, just like the phase of a single vertical antenna, regardless of these characteristics and regardless of the direction of arrival, 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図の特性をそのま捷用い、且つ、和出力の90度位
相変換損失を無視し、1:1で(成したときを示したも
のである。Sが0.5λ以上になっ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, using the characteristics of Figures 3 and 5 as they are, ignoring the 90 degree phase conversion loss of the sum output, and 1:1 (achieved). If S is 0.5λ or more, a complex sense waveform will result, but 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. I understand that.
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って決捷り、またアンテナの口径
りはアンテナ素子数nによって決る。今、仮りにSを0
.72とし最高測定周波数を30■叙とすると、n−1
2本でDは約27m、n=18本でDは約40λとなる
。丑た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
.5 m 、 n=18本ではDは約2.4 mとなる
。一方ドツプラ方探の場合Sは最大0.5λ以内04λ
程度であるから同一素子数の場合、ドツプラアンテナよ
りもアンテナの口径を大きくとれることがわかる。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シアンテナ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υ差と和の出力をとり出すよう
にする。第8図はこの切換によっ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
検波しフィ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
同様フィ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。寸だ到来方位のテジタル表示も既知
の手段により実施できる。Figure 7 shows an example in which n antennas are arranged at equal intervals on the circumference (hereinafter referred to as equal interval arrangement), and the antenna element spacing S
is determined by the highest measurement frequency, and the aperture of the antenna is determined by the number of antenna elements n. Now, suppose S is 0
.. 72 and the highest measured frequency is 30cm, then n-1
With two lines, D is approximately 27m, and with n=18 lines, D is approximately 40λ. Dipole antennas are used in the VHF and UHF bands, but at 500MHz, D is approximately 1 with n-12 antennas.
.. 5 m, with n=18 lines, D is approximately 2.4 m. On the other hand, in the case of Doppler square search, S is within 0.5λ at most 04λ
It can be seen that the diameter of the antenna can be larger than that of a Doppler antenna when the number of elements is the same. The antennas are switched by a switching element provided in the antenna switching device 401, and antennas 1, 2, 2, and 3 are switched by a switching pulse.
, 3 and 4, etc., two antennas are switched at the same time, and one output converter outputs the υ difference and the sum. Figure 8 shows an example of the signal waveform of the difference output obtained by this switching, and after amplifying this output,
If detected and shaped by a filter, a waveform like the dotted line in the figure can be obtained. The sum output also becomes a step-like wave as shown in FIG. 9, but it is similarly shaped by a filter. 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 exact direction of arrival can also be carried out by known means.
このように本発明によれば、ドツプラ方探の如く2台の
受信機を使用して測定電波の周波数変調成分の打消しや
、方位成分検出などの復雑な手法を用いることなく、1
台の受信機を用いて機器を構成することができる。また
ドツプラ方探(例えばドツプラ効果による周波数偏位を
とシ出す方式のような場合)の如くアンテナの切換周期
を速くする必要がなく、従来と同様500−1000回
転/回転度で充分であるから、測定帯域幅による制限や
帯域内における方位変化も少なく、測定も容易である。As described above, according to the present invention, it is possible to obtain one signal without using complicated techniques such as canceling the frequency modulation component of the measurement radio wave or detecting the azimuth component using two receivers as in Doppler direction finding.
The device can be configured using several receivers. In addition, there is no need to increase the switching frequency of the antenna as in Doppler square search (for example, in the case of a method that extracts frequency deviation due to the Doppler effect), and 500-1000 rotations/rotation degree is sufficient as in the conventional case. , there are few restrictions due to measurement bandwidth and azimuth changes within the band, and measurement is easy.
等間隔配置では多くのアンテナ素子が配列されるため、
広帯域の場合ようなには、使用してい々いアンテナから
の再輻射が方位測定に影響を与えることがある。これは
ドツプラ方探の場合も同様であるが、このため使用しな
いアンテナは測定周波数によりアンテナ基部を接地捷た
は開放し、またインピーダンスを挿入するなどしてその
影響を少なくすることも必要となる。Since many antenna elements are arranged at equal intervals,
In some cases, such as in the case of broadband, re-radiation from the antenna may affect orientation measurements during use. This is the same in the case of Doppler direction finding, but for this reason, it is necessary to reduce the influence of unused antennas by ungrounding or opening the base of the antenna depending on the measurement frequency, and by inserting impedance. .
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−ヒ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。On the other hand, the method of symmetrically arranging m sets of two antennas (hereinafter referred to as the symmetrical arrangement method) arranges the antennas in pairs symmetrically around the circumference, as shown in Figure 10. ,
The number of antennas in a set may be at least four, but it is usually eight or an integral multiple of eight.
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。例えは8組のアンテナのとき、
最高測定周波数が30MH2でもアンテナ口径を100
?n、 Kまだ500MI(zのときでもアンテナ口
径を20m程度にすることができる。従って大口径アン
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。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 there are 8 sets of antennas,
Even if the highest measurement frequency is 30MH2, the antenna diameter is 100.
? Even when n, K is still 500 MI (z), the antenna diameter can be set to about 20 m. Therefore, the characteristics of a large diameter antenna can be further demonstrated, and the influence of other antennas not in use can 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。得られた鼓形は第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, 3 and 4, and 5 and 6, are switched in sequence at the same time. Although the obtained hourglass shape has a step-like shape as in FIG. 9, it can be processed and measured in the same manner as in the case of equally spaced antennas, including the sense output.
本発明によるアンテナ装置を用いた方位測定の感度は、
基本的には間隔Sのアトコックアンテナとほぼ同様であ
るが、ゴニオメータを用いたアトコックアンテナに比し
ゴニオメータの損失がなく(通常6〜10dB程度の損
失を伴なう)、アンテナ切換回路の損失(通常1〜2
dB )が伺加される程度であるから、精度のみならず
感度のよい方位測定を行なうことができる。The sensitivity of direction measurement using the antenna device according to the present invention is
Basically, it is almost the same as the Atcock antenna with the spacing S, but compared to the Atcock antenna using a goniometer, there is no goniometer loss (usually accompanied by a loss of about 6 to 10 dB), and the antenna switching circuit is Loss (usually 1-2
dB), it is possible to perform direction measurements not only with high accuracy but also with high sensitivity.
本発明は指向特性を有するアンテナを広囲口面に対称配
置し、擾乱物体などの影響による誤差の改善率を向上さ
せ、指向特性が対称性を有するときはそのアンテナ位置
における垂直成分を取出して指向特性に単向性を持たせ
ることを特徴としたアンテナ装置であるが、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
越しプこ間隔の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 improves the improvement rate of errors caused by the influence of disturbing objects by symmetrically arranging antennas with directional characteristics on a wide aperture surface, and when the directional characteristics have symmetry, the vertical component at the antenna position is extracted. Although the antenna device is characterized by having unidirectional directivity, the present invention is not limited to the above-mentioned two embodiments, and various modifications can be made without departing from the gist of the present invention. can be carried out. For example, in FIG. 7, in the low measurement frequency band, antenna elements 1 and 3, 3 and 5, 5 and 7
...or 1 and 3, 2 and 4, 3 and 5, etc. Switch two antennas with skipped spacing as a set, double the antenna spacing to improve sensitivity, and use antennas 1 and 3. It is also possible to return to the combination of antennas 1 and 2 at frequencies where the spacing is approximately 0.7λ.
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図はこの原理によって得られる位相差出力N
1第3図は2本のアンテナの位相差出力の特性即ちアト
コックアンテナの指向毛性を示したもの、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。寸だ第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、50トアンテナ素子、601・・
アンテナ接続ケーブル。
特許出願人
図面の浄店(内容に変更なし)
牛 1 回
/172 口
回転角度e
木 3 図
オ 7 口
180゜
季8k オ9図
S=0.25入
第10図
800
手続補正書(自発)
昭和58年//月25日
特許庁長官 殿
1、事件の表示
η寺願昭 58−/88S3B
2、発明の名称
方位測定用アンテナ装置□
3 補正をする者
事件との関係 特許出願人
〒141東京部品川区上大崎2−10−45明細書・図
面
56 補正の内容
明細書・図面の浄書(内容に変更なし)6、添付書類の
目録
(1) 補正用明細書 1通
(2) 補正用図 面 1通
手 続 補 正 1(自発)
昭和5?年/I月29日
特許庁長官 殿
1 事件の表示
特願昭5B −/g/353B
2、発明の名称
方位測定用アンテナ装置
3、 補正をする者
事件との関係 特許出願人
〒141 東京部品用区上大崎2〜10−45明細1
5 補正の内容
別紙の通り
6、 添付書類の目録
(1) 補正内容書
補 正 内 容 書The drawings show examples, FIG. 1 is an explanatory diagram showing the principle of the invention, and FIG. 2 shows the phase difference output N obtained by this principle.
1 Figure 3 shows the characteristics of the phase difference output of the two antennas, that is, the directivity of the Atcock antenna. Figure 4 is a vector diagram showing the phase difference and sum of the two antennas. Figure 5 shows the phase difference output characteristics of the two antennas. The phase sum characteristic diagram of the same two antennas, Figure 6 is similar to Figures 3 and 5.
The composition (sense) characteristics of the difference between the figures and the sum output are shown by each S/λ, and Fig. 7 is a schematic diagram of the configuration of the equally spaced arrangement method, which is one of the embodiments of the present invention. Evenly spaced arrangement of figures −
FIG. 9 is a diagram showing the difference output obtained by switching the antenna, and FIG. 9 is a diagram showing the sum output of the same antenna. Figure 10 is a schematic diagram of the symmetrical arrangement of another embodiment. 1-16. n...Antenna, 301...Transformer, 401
・・Antenna switcher, 50 antenna elements, 601・・
antenna connection cable. Purification of the patent applicant's drawing (no change in content) Cow 1 time/172 Mouth rotation angle e Tree 3 Figure O 7 Mouth 180° Season 8k O9 Figure S = 0.25 entered Figure 10 800 Procedural amendment (voluntary ) Director General of the Japan Patent Office, July 25, 1982 1. Indication of the case η Temple Gansho 58-/88S3B 2. Name of the invention Antenna device for measuring direction□ 3. Relationship with the person making the amendment Patent applicant: 141 2-10-45 Kamiosaki, Honbunagawa-ku, Tokyo Specification/Drawings 56 Contents of amendments Reprint of the specification/drawings (no change in content) 6, List of attached documents (1) Specification for amendment 1 copy (2) 1 drawing for correction Procedure Correction 1 (voluntary) Showa 5? Director General of the Japan Patent Office, January 29, 2013 1. Indication of the case Patent application 1973-/g/353B 2. Name of the invention Antenna device for direction measurement 3. Relationship with the amended person case Patent applicant address: 141 Tokyo Parts 2-10-45 Kami-Osaki 2-10-45 details 1 5 Contents of the amendment As shown in the attached sheet 6 List of attached documents (1) Amendment to the content of the amendment Contents
Claims (1)
群のうちの相隣れる2本のアンテナまたは飛び越した間
隔の2本のアンテナを組として循環状に順次に切換えな
がら1つの変成器の1次側に接続し、この変成器の2次
側よシ前記2本のアンテナ間の位相差電圧を取り出した
出力によって方位測定を行ない、前記変成器の中点より
和出力を取り出した出力によってセンス決定を行なうこ
とを特徴とする方位測定用アンテナ装置。 2、特許請求の範囲第1項の方位測定用アンテナ装置で
あり、広帯域にわたる周波数について方位測定を行なう
ものであって、ある周波数帯では前記相隣れる2本のア
ンテナを組とし、他の周波数帯では飛ひ越した間隔の2
本のアンテナを組として前記切換えを行なうことを特徴
とする方位測定用アンテナ装置。 3 間隔配置した2本のアンテナを組にして円周上に対
称的に複数組配置し、この各組を循環状に順次に切換え
ながら変成器の1次側に接続し、この変成器の2次側よ
り前記2本のアンテナ間の位相差電圧を取シ出した出力
によって方位測定を行ない、前記変成器の中点より和出
力を取り出した出力によってセンス決定を行なうことを
特徴とする方位測定用アンテナ装置。[Scope of Claims] ■ A group of antennas in which a plurality of antennas are arranged at equal intervals on the circumference, and two adjacent antennas or two antennas with skipped intervals are sequentially switched in a circular manner as a set. Connected to the primary side of one transformer, the output of the phase difference voltage between the two antennas is taken out from the secondary side of this transformer, and the direction is measured, and the sum output is calculated from the midpoint of the transformer. An antenna device for azimuth measurement, characterized in that a sense determination is made based on an output extracted from the azimuth. 2. The antenna device for measuring direction according to claim 1, which measures direction over a wide range of frequencies, in which the two adjacent antennas are set as a set in a certain frequency band, and in other frequencies. In the belt, 2 with skipped intervals
An antenna device for azimuth measurement, characterized in that the switching is performed using a set of book antennas. 3 A plurality of sets of two antennas arranged at intervals are arranged symmetrically on the circumference, and each set is connected to the primary side of the transformer while being sequentially switched in a circular manner. Direction measurement is performed using an output obtained by extracting a phase difference voltage between the two antennas from the next side, and sense determination is performed using an output obtained by extracting a sum output from the midpoint of the transformer. antenna device.
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 true JPS6080780A (en) | 1985-05-08 |
| JPH0260147B2 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) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02231589A (en) * | 1989-03-03 | 1990-09-13 | Koden Electron Co Ltd | Wide frequency band type direction finding device |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4933916A (en) * | 1972-07-29 | 1974-03-28 |
-
1983
- 1983-10-11 JP JP18853883A patent/JPS6080780A/en active Granted
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4933916A (en) * | 1972-07-29 | 1974-03-28 |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02231589A (en) * | 1989-03-03 | 1990-09-13 | Koden Electron Co Ltd | Wide frequency band type direction finding device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0260147B2 (en) | 1990-12-14 |
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