JPS6018016B2 - direction finder antenna device - Google Patents

direction finder antenna device

Info

Publication number
JPS6018016B2
JPS6018016B2 JP13448580A JP13448580A JPS6018016B2 JP S6018016 B2 JPS6018016 B2 JP S6018016B2 JP 13448580 A JP13448580 A JP 13448580A JP 13448580 A JP13448580 A JP 13448580A JP S6018016 B2 JPS6018016 B2 JP S6018016B2
Authority
JP
Japan
Prior art keywords
output
outputs
antenna
antennas
sum
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
JP13448580A
Other languages
Japanese (ja)
Other versions
JPS5760271A (en
Inventor
憲三 森
彪 保田
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.)
Taiyo Musen Co Ltd
Original Assignee
Taiyo Musen 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 Taiyo Musen Co Ltd filed Critical Taiyo Musen Co Ltd
Priority to JP13448580A priority Critical patent/JPS6018016B2/en
Priority to GB8114590A priority patent/GB2085231A/en
Priority to DE19818115150 priority patent/DE8115150U1/en
Priority to DE19813120229 priority patent/DE3120229A1/en
Priority to FR8110530A priority patent/FR2491217A1/en
Publication of JPS5760271A publication Critical patent/JPS5760271A/en
Publication of JPS6018016B2 publication Critical patent/JPS6018016B2/en
Expired 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
    • G01S3/04Details
    • G01S3/12Means for determining sense of direction, e.g. by combining signals from directional antenna or goniometer search coil with those from non-directional antenna
    • 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
    • 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
    • H01Q21/20Arrays of individually energised antenna units similarly polarised and spaced apart the units being spaced along or adjacent to a curvilinear path
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q25/00Antennas or antenna systems providing at least two radiating patterns
    • H01Q25/02Antennas or antenna systems providing at least two radiating patterns providing sum and difference patterns

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】 例えば互に直交するように配陣したアドコツク空中線の
出力を90度の位相差を有する2つの低周波でそれぞれ
平衡変調して合成し、更にその合成出力に無指向性の垂
直空中線の出力をセンス出力として適当な位相で合成す
ることにより、電波の到来方向を測定することができる
Detailed Description of the Invention For example, the outputs of Adkotsuk antennas arranged orthogonally to each other are balanced modulated using two low frequencies having a phase difference of 90 degrees, and combined, and the combined output is non-directional. By combining the outputs of the vertical antennas as a sense output with an appropriate phase, the direction of arrival of the radio waves can be measured.

本発明はこのような方向探知機において、センス決定用
の垂直空中線を設ける必要が無いようにすると共に指向
性出力とセンス出力との間の安定な位相関係を容易に保
持し得る空中線装置を提供するものである。かつセンス
決定用の無指向性空中線を必要としないから、水平偏波
の電波に対しでもその到来方向を容易に測定することが
できる。第1図は本発明の実施例で、互に直交する2本
の水平線X,Y上にそれぞれ1対の垂直空中線Ve,V
wおよびVn,Vsを2の間隔で配直してある。
The present invention provides an antenna device in such a direction finder that eliminates the need to provide a vertical antenna for sense determination and that can easily maintain a stable phase relationship between the directional output and the sense output. It is something to do. Moreover, since an omnidirectional antenna for sense determination is not required, the direction of arrival of horizontally polarized radio waves can be easily measured. FIG. 1 shows an embodiment of the present invention, in which a pair of vertical antennas Ve, V are placed on two mutually orthogonal horizontal lines X, Y, respectively.
w, Vn, and Vs are rearranged at intervals of 2.

空中線Vn.Vsの出力端子Tn,Tsにそれぞれ2つ
の2次巻線を有する変成器Mm,Msを接続して、各変
成器における1つ宛の2次巻線を出力端子0aまたは0
bの間にそれぞれ同一極性および逆極性で直列に接続し
てある。従って端子0aから空中線Vn,Vsの出力の
和が、また端子○bから差が送出される。なお図示して
ないが空中線Ve,Vwの出力端子Te,Tw‘こも全
く同様の回路を接続してある。このような空中線装置に
角8の方向から Eosinwtの電波が到釆するとき、その波長を入、
空中線の実効高を日とすると、端子Tn,Tsの出力E
n●ESはEn=EHOSinくのt‐峯ICOS8)
ES=地。
Aerial Vn. Transformers Mm and Ms each having two secondary windings are connected to the output terminals Tn and Ts of Vs, and the secondary winding of each transformer is connected to the output terminal 0a or 0.
b are connected in series with the same polarity and opposite polarity, respectively. Therefore, the sum of the outputs of the antennas Vn and Vs is sent from the terminal 0a, and the difference is sent from the terminal ○b. Although not shown, the output terminals Te and Tw' of the antennas Ve and Vw are also connected to the same circuit. When Eosinwt radio waves arrive at such an antenna device from the direction of corner 8, the wavelength is input,
If the effective height of the antenna is day, the output E of terminals Tn and Ts is
n●ES is En=EHOSinkunot-MineICOS8)
ES=Earth.

Sin(のt十竿IC。S8)で与えられる。It is given by Sin('s t 10 IC.S8).

従って端子○aから得られる和の出力E(n+s)はE
(n+S)=細。
Therefore, the sum output E(n+s) obtained from terminal ○a is E
(n+S)=thin.

COS(空C。M)Sinのt であり、また端子○bから得られる差の出力E(n−s
)はE(n−S)=岬。
t of COS (empty C.M) Sin, and the difference output E (n-s
) is E(n-S) = cape.

Sin(竿IC。小COSのt で与えられる。Sin (rod IC. Small COS t is given by

同様にして端子Te,Twの出力の和E(e+w)およ
び差E(e−w)はB(e+W)=畑。
Similarly, the sum E(e+w) and the difference E(ew) of the outputs of terminals Te and Tw are B(e+W)=field.

COS(等Sin8)Sinwt E(e−W)=細OSin(竿ISina)COSのt
である。
COS (equal Sin8) Sinwt E (e-W) = fine OSin (rod ISina) COS t
It is.

すなわち2ml/^〈1とすると、出力E(n+s)お
よびB(e+w)の和を得ることにより、各空中線出力
の総和E(n+s+c十w)として、8(n十s十e+
w)三仏m。
In other words, if 2ml/^<1, then by obtaining the sum of the outputs E(n+s) and B(e+w), the total of each antenna output E(n+s+c+w) is 8(n + s + e+
w) Three Buddhas m.

sinのtが得られる。t of sin is obtained.

この出力は電波の到来方向のこ無関係であるから、これ
を無指向性のセンス出力として用いることができる。ま
た前記差の出力E(n−s)およびE(e−w)はE(
n−S)三畑。
Since this output is independent of the direction in which the radio waves arrive, it can be used as an omnidirectional sense output. Also, the difference outputs E(n-s) and E(ew) are E(
n-S) Mihata.

努C。Sa,Sinのt E(e−W)=畑。Tsutomu C. Sa, Sin's t E (e-W) = field.

竿Sinひ.Sm■t であって、これらはcosoおよびsin8の指向性を
有する。
Rod Sinhi. Sm*t, which have coso and sin8 directionality.

従ってこの指向性出力および前記センス出力を用いて、
無指向性のセンス空中線を必要とすることなく、電波の
到釆方向を測定することができる。かつ同一空中線の出
力によって指向性および無指向性の出力を得るから、そ
れらの位相関係が安定に保たれる。また第2図は水平偏
波の電波到来方向を測定する場合の実施例で、水平ダィ
ボール空中線比,Hsを水平面内の直線Y上に距離2を
もって平行に配置し、直線Yと直交する水平な直線X上
に同様の距離をもって水平ダィポール空中線He,Hw
を平行に配置してある。
Therefore, using this directional output and the sense output,
The arrival direction of radio waves can be measured without requiring an omnidirectional sense antenna. In addition, since directional and non-directional outputs are obtained from the output of the same antenna, the phase relationship between them is kept stable. Fig. 2 shows an example of measuring the arrival direction of horizontally polarized radio waves, in which the horizontal die-ball antenna ratio, Hs, is placed parallel to a straight line Y in the horizontal plane with a distance of 2, and the horizontal Horizontal dipole antennas He, Hw at the same distance on the straight line
are arranged in parallel.

上記空中線Hn,Hsの出力端子Tn,Tsにそれぞれ
変成器MM,M他およびMsa,Msbを接続して、出
力端子仇の間に変成器Mha,Msaの2次巻線を同一
極性で直列に接続し、出力端子0bの闇に変成器Mnb
.Msbの2次巻線を逆犠牲で直列に接続してある。従
って端子oaから空中線Hn,瓜の出力の和が、また端
子0bから差が送出される。なお図示してないが空中線
He,Hwの出力端子Te,Twにも全く同様の回路を
接続してある。このような空中線装魔において、空中線
Hh,聡の出力En,EsはそれぞれEneHE。
Transformers MM, M, etc. and Msa, Msb are connected to the output terminals Tn, Ts of the antennas Hn, Hs, respectively, and the secondary windings of the transformers Mha, Msa are connected in series with the same polarity between the output terminals. Connect the transformer Mnb to the output terminal 0b
.. The secondary windings of Msb are connected in series with reverse sacrifice. Therefore, the sum of the outputs of the antenna Hn and the melon is sent from the terminal oa, and the difference is sent from the terminal 0b. Although not shown, completely similar circuits are also connected to the output terminals Te and Tw of the antennas He and Hw. In such an antenna device, the outputs En and Es of the antenna Hh and Satoshi are each EneHE.

CosO.Smひ (■t−等IC。CosO. Smhi (■t-etc. IC.

S。)Es=HE。S. )Es=HE.

Cos8.Sin(のt+等ICOS8) で与えられる。Cos8. Sin (t+ etc. ICOS8) is given by

従って端子○aから得られる和のタ出力E(n+s)は
E(n十s)=力由。
Therefore, the sum output E(n+s) obtained from terminal ○a is E(n+s)=force.

cosひ.COS等C。coshi. COS etc.C.

S8)Sinのtであり、また端子○bから得られる差
の出力E0(n−s)はE(n−s)=が由。
S8) is t of Sin, and the difference output E0(n-s) obtained from terminal ○b is because E(n-s)=.

cos.sm(学ICOSo)COSのt で与えられる。cos. sm (GakuICOSo) COS's t is given by

すなわち2ml/^<1とする夕と、E(n+s)ニ公
正。
In other words, 2ml/^<1 and E(n+s) is fair.

cosひ.sinのtE(n‐S)=畑。等.C。S2
8.COSのt ひとなる。
coshi. tE(n-S) of sin = field. etc. C. S2
8. COS's t Hitonaru.

同様にして端子Te,Twの出力の和E(e+w)およ
び差E(c−w)はE(e+w)三公正。
Similarly, the sum E(e+w) and the difference E(c-w) of the outputs of terminals Te and Tw are E(e+w).

sino.sinのtE(e…):岬。賀.船ひ夕
,COSのt である。
sino. sin's tE(e...): Misaki. Ga. boat ride
, t of COS.

従って出力E(n−s)とE(e−w)の和をとるとE
(n−S)+E(e−w)=汎峯 0 ICOSの
tとなって無指向性のセンス出力を得ることができる。
Therefore, if we take the sum of the outputs E(n-s) and E(ew), we get E
(n-S)+E(ew)=Honmine 0 It becomes t of ICOS, and a non-directional sense output can be obtained.

また前記出力E(n+s)およびE(c十w)はそれぞ
れcosoおよびsinoの指向性をもっているから、
これらの出力を用いて水平偏波の鰭波到釆方向を水平な
空中線のみによって正確に測定し得る。
Furthermore, since the outputs E(n+s) and E(cw) have coso and sino directivity, respectively,
Using these outputs, the arrival direction of horizontally polarized fin waves can be accurately measured using only a horizontal antenna.

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

第1図、第2図はそれぞれ本発明の実施例における空中
線の平面配置並びに回路を示した図である。 なお図において、Vn,Vs,Ve,Vwは垂直空中線
、Hn,Hs,He.Hw‘ま水平ダィポール空中線で
ある。ぞ/傷 づZ公
FIGS. 1 and 2 are diagrams showing the planar arrangement and circuit of an antenna in an embodiment of the present invention, respectively. In the figure, Vn, Vs, Ve, Vw are vertical antennas, Hn, Hs, He. Hw' is a horizontal dipole antenna. /Kuzu Z-ko

Claims (1)

【特許請求の範囲】 1 互に交叉する複数本の直線上に適当な距離をもつて
それぞれ1対の垂直空中線を配置し、各対における2つ
の空中線出力の差によつてそれぞれ指向性出力を得る回
路と、各空中線出力の総和によつてセンス出力を得る回
路とを設けたことを特徴とする方向探知機の空中線装置
。 2 互に直交する2本の直線上に適当な距離をもつてそ
れぞれ1対の水平空中線を配置し、各対における2つの
空中線出力の和によつてそれぞれ指向性出力を得る回路
と、各対における2つの空中線出力の差を更に合成して
センス出力を得る回路とを設けたことを特徴とする方向
探知機の空中線装置。
[Claims] 1. Pairs of vertical antennas are arranged at appropriate distances on a plurality of straight lines that intersect with each other, and each directional output is determined by the difference between the outputs of the two antennas in each pair. 1. An antenna device for a direction finder, comprising: a circuit for obtaining a sense output from the sum of the outputs of each antenna; and a circuit for obtaining a sense output from the sum of outputs of each antenna. 2. A circuit in which a pair of horizontal antennas are placed at an appropriate distance on two straight lines that are perpendicular to each other, and obtains a directional output from the sum of the outputs of the two antennas in each pair, and An antenna device for a direction finder, comprising a circuit for further synthesizing the difference between two antenna outputs to obtain a sense output.
JP13448580A 1980-09-29 1980-09-29 direction finder antenna device Expired JPS6018016B2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP13448580A JPS6018016B2 (en) 1980-09-29 1980-09-29 direction finder antenna device
GB8114590A GB2085231A (en) 1980-09-29 1981-05-13 Antenna system for direction finder
DE19818115150 DE8115150U1 (en) 1980-09-29 1981-05-21 ANTENNA SYSTEM FOR A SPILL
DE19813120229 DE3120229A1 (en) 1980-09-29 1981-05-21 "ANTENNA SYSTEM FOR A PILOT
FR8110530A FR2491217A1 (en) 1980-09-29 1981-05-27 ANTENNA SYSTEM FOR RADIOGONIOMETERS

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13448580A JPS6018016B2 (en) 1980-09-29 1980-09-29 direction finder antenna device

Publications (2)

Publication Number Publication Date
JPS5760271A JPS5760271A (en) 1982-04-12
JPS6018016B2 true JPS6018016B2 (en) 1985-05-08

Family

ID=15129425

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13448580A Expired JPS6018016B2 (en) 1980-09-29 1980-09-29 direction finder antenna device

Country Status (4)

Country Link
JP (1) JPS6018016B2 (en)
DE (2) DE8115150U1 (en)
FR (1) FR2491217A1 (en)
GB (1) GB2085231A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63129615U (en) * 1987-02-17 1988-08-24
JPH02133921U (en) * 1989-04-13 1990-11-07
JPH0622032U (en) * 1992-08-31 1994-03-22 八千代工業株式会社 Sunroof equipment

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB528514A (en) * 1939-04-28 1940-10-31 Standard Telephones Cables Ltd Improvements in or relating to radio direction finding systems
US2480234A (en) * 1946-05-03 1949-08-30 Leon Ottinger Cathode-ray direction finder
DE1226172B (en) * 1955-05-09 1966-10-06 Kokusai Denshin Denwa Co Ltd Sight direction finder for electromagnetic high frequency oscillations
DE1094822B (en) * 1957-11-07 1960-12-15 Dr Maximilian Waechtler Arrangement for three-dimensional direction finding of a radio transmitter

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63129615U (en) * 1987-02-17 1988-08-24
JPH02133921U (en) * 1989-04-13 1990-11-07
JPH0622032U (en) * 1992-08-31 1994-03-22 八千代工業株式会社 Sunroof equipment

Also Published As

Publication number Publication date
JPS5760271A (en) 1982-04-12
GB2085231A (en) 1982-04-21
FR2491217A1 (en) 1982-04-02
DE3120229A1 (en) 1982-04-29
DE8115150U1 (en) 1984-07-26

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