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JP3454892B2 - Radio source location method and device - Google Patents
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JP3454892B2 - Radio source location method and device - Google Patents

Radio source location method and device

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Publication number
JP3454892B2
JP3454892B2 JP31906793A JP31906793A JP3454892B2 JP 3454892 B2 JP3454892 B2 JP 3454892B2 JP 31906793 A JP31906793 A JP 31906793A JP 31906793 A JP31906793 A JP 31906793A JP 3454892 B2 JP3454892 B2 JP 3454892B2
Authority
JP
Japan
Prior art keywords
cross
correlation function
radio wave
phase difference
received
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 - Fee Related
Application number
JP31906793A
Other languages
Japanese (ja)
Other versions
JPH07146352A (en
Inventor
宏幸 美齊津
義明 小林
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.)
Tokyo Electric Power Co Holdings Inc
Original Assignee
Tokyo Electric Power Co Inc
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 Tokyo Electric Power Co Inc filed Critical Tokyo Electric Power Co Inc
Priority to JP31906793A priority Critical patent/JP3454892B2/en
Publication of JPH07146352A publication Critical patent/JPH07146352A/en
Application granted granted Critical
Publication of JP3454892B2 publication Critical patent/JP3454892B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Position Fixing By Use Of Radio Waves (AREA)

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は電波発生源の位置標定を
行う電波源位置標定方法および装置に関し、特に、連続
波を放射する電波源でも高い精度で標定できるようにし
た電波源位置標定方法および装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a radio wave source position locating method and apparatus for locating a radio wave source, and particularly to a radio wave source position locating method capable of locating a continuous wave radiating source with high accuracy. And equipment.

【0002】[0002]

【従来の技術】現在、電力会社における発電所や変電所
等の電力設備構内の連絡手段として、保安用移動無線,
ページャ,小電力コードレス電話システム等といった電
波を利用した通信機器が必要不可欠なものになってい
る。
2. Description of the Related Art At present, as a means of communication in power facilities such as power plants and substations in electric power companies, mobile radio for security,
Communication equipment using radio waves such as pagers and small power cordless telephone systems has become indispensable.

【0003】一方、電力設備構内において、巡視・作業
状態を正確に把握したり、電力設備の状態を把握するた
め、各巡視員・作業員の正確な位置検出や、発生電波雑
音による設備診断の必要性が高まっている。このため、
電気設備構内の電波環境を把握するために、上記通信機
器の電波の発生源の位置標定を行ったり、雑音電波の発
生源の位置標定を行っている。
On the other hand, in the premises of a power facility, in order to accurately ascertain the patrol / working state and to grasp the state of the power facility, accurate position detection of each patrol / worker and facility diagnosis by radio noise are performed. The need is growing. For this reason,
In order to grasp the radio wave environment in the electric equipment premises, the position of the radio wave source of the communication device is located, or the position of the noise radio wave source is located.

【0004】従来、電波源の位置標定を行う場合には、
例えば、図5に示すような標定装置が用いられている。
この電波源位置標定装置は、有限な平面領域11に位置
する電波源10から放射される信号を受信する4台のア
ンテナ121 〜124 と、各アンテナ121 〜124
それぞれ接続された4台の受信器131 〜134 と、こ
れら受信器131 ,132 と受信器133 ,134 の組
み合わせに対してそれぞれ接続された2台の到達時間差
検出回路141 ,142 と、2台の到達時間差検出回路
141 ,142 からの時間差信号を入力して所定の演算
を行う演算回路(MP)15より構成されている。
Conventionally, when locating a radio wave source,
For example, an orientation device as shown in FIG. 5 is used.
This radio wave source position locating device was connected to four antennas 12 1 to 12 4 for receiving signals radiated from the radio wave source 10 located in a finite plane area 11 and to the respective antennas 12 1 to 12 4 . Four receivers 13 1 to 13 4 and two arrival time difference detection circuits 14 1 and 14 2 respectively connected to the combinations of the receivers 13 1 and 13 2 and the receivers 13 3 and 13 4. It is composed of an arithmetic circuit (MP) 15 which receives the time difference signals from the two arrival time difference detection circuits 14 1 and 14 2 and performs a predetermined calculation.

【0005】上記構成の標定装置を用いて電波源位置を
標定する場合には、電波源10から放射された電波を受
信器131 〜134 のアンテナ121 〜124 でそれぞ
れ受信し、到達時間差検出回路141 でアンテナ121
とアンテナ122 から取り込んだ受信信号の波形を、ま
た、到達時間差検出回路142 でアンテナ123 とアン
テナ124 から取り込んだ受信信号の波形をそれぞれ比
較し、電波源10からそれぞれのアンテナ121 〜12
4 への信号の到達時間差を検出することによって行って
いる。すなわち、電波源10からの電波が連続波の場合
には、図6に示すように、また、電波源10からの電波
が不連続波の場合には、図7に示すように、2つの信号
の到達時間差Δtを測定することにより電波源の位置を
標定している。
In the case of locating the position of the radio wave source using the locating device having the above-mentioned configuration, the radio waves radiated from the radio wave source 10 are received by the antennas 12 1 to 12 4 of the receivers 13 1 to 13 4 and reach them. antenna 12 1 by the time difference detection circuit 14 1
And the waveform of the received signal received from the antenna 12 2 and the waveform of the received signal received from the antenna 12 3 and the antenna 12 4 by the arrival time difference detection circuit 14 2 are respectively compared, and each antenna 12 1 from the radio wave source 10 is compared. ~ 12
This is done by detecting the difference in the arrival time of the signal to 4 . That is, when the radio wave from the radio wave source 10 is a continuous wave, as shown in FIG. 6, and when the radio wave from the radio wave source 10 is a discontinuous wave, as shown in FIG. The position of the radio wave source is located by measuring the arrival time difference Δt.

【0006】[0006]

【発明が解決しようとする課題】しかし、従来の電波源
位置標定装置によると、電波源が放射する電波が連続波
の場合、到達時間差のΔtとΔt+n×1/f(n=
1,2,3・・)の判別ができないため、測定精度にn
×1/fの不確定性が生じ、電波源の位置標定の精度を
低下させるばかりでなく、標定不可能となることもあ
る。
However, according to the conventional radio wave source position locating device, when the radio wave emitted from the radio wave source is a continuous wave, the arrival time difference Δt and Δt + n × 1 / f (n =
1, 2, 3, ...) cannot be discriminated.
Uncertainty of x1 / f may occur, which not only lowers the accuracy of location determination of the radio wave source but also makes location impossible.

【0007】従って、本発明の目的は連続波を放射する
電波源でも高い精度で標定することができる電波源位置
標定方法および装置を提供することである。
Therefore, an object of the present invention is to provide a radio wave source position locating method and apparatus capable of locating a radio wave source radiating a continuous wave with high accuracy.

【0008】[0008]

【課題を解決するための手段】本発明は上記問題点に鑑
み、連続波を放射する電波源でも高い精度で標定できる
ようにするため、有限の平面領域に位置する電波源から
連続波として放射される信号を少なくとも2つの位置で
受信して受信信号間の位相差を相互相関関数として測定
によって求め、平面領域の複数のから放射されたと仮
定した仮想信号を少なくとも2つの位置で受信したと仮
定したときの仮想受信信号間の位相差を相互相関関数と
して演算によって求め、測定に基づく相互相関関数と複
数のに対応する演算に基づく相互相関関数とを比較し
測定に基づく相互相関関数に最も近似した相互相関
関数を複数の点に対応する演算に基づく相互相関関数
ら選択し、選択された相互相関関数に対応したを電波
源の位置として標定するようにした電波源位置標定方法
を提供するものである。
The present invention SUMMARY OF THE INVENTION In view of the above problems, because the to be orientation with high precision even in radio sources for emitting a continuous wave, the radio wave source located on a finite planar area
It receives the signal emitted as a continuous wave at least two at a position determined by measuring the phase difference between the received signals as a cross-correlation function, even a virtual signal is assumed to have been emitted from a plurality of points of the plane area small without 2 The cross-correlation function is the phase difference between the virtual received signals, assuming that they are received at one position.
Then , the measurement-based cross-correlation function is compared with the calculation-based cross-correlation function corresponding to a plurality of points , and the cross-correlation closest to the measurement-based cross-correlation function is calculated.
The function or cross-correlation function <br/> et select based on a corresponding operation to a plurality of points, the radio source position location method to be orientation points corresponding to the cross-correlation function selected as the location of the radio source It is provided.

【0009】また、上記目的を達成する本発明の電波源
位置標定装置は、有限な平面領域に位置する電波源から
連続波として放射される信号を少なくとも2つの位置で
受信する少なくとも2つの受信手段と、少なくとも2つ
の受信手段によって受信した受信信号間の位相差を相互
相関関数として測定する位相差測定手段と、平面領域の
複数のから放射されたと仮定した仮想信号を少なくと
も2つの位置で受信したと仮定したときの仮想受信信号
間の位相差を相互相関関数として演算によって求め、測
定に基づく相互相関関数と複数のに対応する演算に基
づく相互相関関数とを比較して測定に基づく相互相関
関数に最も近似した相互相関関数を複数の点に対応する
演算に基づく相互相関関数から選択し、選択した相互相
関関数に対応したを電波源の位置として標定するよう
に構成されている。
Further, a radio wave source position locating device of the present invention which achieves the above-mentioned object is provided from a radio wave source located in a finite plane area.
Interacting with the at least two receiving means for receiving the signals radiated at least two at the position, the phase difference between the received signals received by at least two receiving means as a continuous wave
A phase difference measuring means for measuring as a correlation function, and a phase difference between virtual received signals when virtual signals assumed to be emitted from a plurality of points in a plane area are received at at least two positions as a cross-correlation function. determined by calculation, by comparing the cross-correlation function based on operation corresponding to the cross-correlation function and a plurality of points based on the measurement, the cross-correlation based on the measurement
The cross-correlation function that most closely approximates the function corresponds to multiple points
Select from the cross-correlation function based on the operation and select the cross phase
It is configured to locate the point corresponding to the function as the position of the radio wave source.

【0010】上記受信手段は、電波源から放射される信
号を受信するアンテナと、アンテナで受信した受信信号
を所定のレベルまで増幅する低雑音増幅器と、増幅した
受信信号の振幅を一定にするリミッタと、振幅が一定な
受信信号のレベルを所定のレベルに減衰調整する可変抵
抗減衰器と、少なくとも2つの受信手段間の受信動作中
に生じる移相が一定となるように校正する移相器より構
成されている。また、アンテナは水平面内又は垂直面内
無指向性,或いは有限な平面領域の方向に広い指向性を
有している。
The receiving means comprises an antenna for receiving a signal radiated from a radio wave source, a low noise amplifier for amplifying the received signal received by the antenna to a predetermined level, and a limiter for keeping the amplitude of the amplified received signal constant. A variable resistance attenuator that attenuates and adjusts the level of a received signal whose amplitude is constant to a predetermined level, and a phase shifter that calibrates the phase shift that occurs during the receiving operation between at least two receiving means to be constant. It is configured. Further, the antenna has an omnidirectionality in a horizontal plane or a vertical plane, or has a wide directivity in the direction of a finite plane area.

【0011】上記演算手段は、有限な平面領域を座標と
して入力する座標入力部と、座標上の各点を電波源と仮
定したときに少なくとも2つの受信手段が受信すると想
定される仮想受信信号の位相を各点について演算する位
相演算部と、少なくとも2つの受信手段が受信すると想
定される仮想受信信号の位相差から相互相関関数を各
ついて演算する位相差演算部と、位相差測定手段によ
って測定された測定に基づく位相差を相互相関関数とし
入力する測定位相差入力部と、位相差演算部で演算さ
れた演算に基づく相互相関関数と測定位相差入力部より
入力した測定に基づく相互相関関数とを比較する比較回
路と、比較回路の比較結果において、測定に基づく相互
相関関数に最も近似した相互相関関数座標上の各点に
対応する演算に基づく相互相関関数から選択し、選択し
相互相関関数に対応した座標上の点を電波源の位置と
して標定する電波源標定回路と、標定結果を表示する表
示部より構成されている。
It is assumed that the above-mentioned calculation means is received by at least two receiving means assuming that a coordinate input section for inputting a finite plane area as coordinates and each point on the coordinates as a radio wave source.
The phase calculation unit that calculates the phase of the virtual received signal that is determined for each point, and the concept that at least two receiving means receive the signal.
Each point of the cross-correlation function from the phase difference of the virtual reception signal constant
A phase difference calculator for calculating with the the phase difference based on the measurement measured by the phase difference measuring means and cross-correlation function
Of the measured phase difference input section, the comparison circuit for comparing the cross-correlation function based on the calculation calculated by the phase difference calculation section and the cross-correlation function based on the measurement input from the measured phase difference input section, In the comparison result, the measurement-based mutual
The cross-correlation function that best approximates the correlation function at each point on the coordinate
It consists of a radio source localization circuit that selects from the cross-correlation function based on the corresponding calculation, and locates the point on the coordinates corresponding to the selected cross-correlation function as the position of the radio source, and a display unit that displays the localization result. .

【0012】[0012]

【実施例】以下、本発明の電波源位置標定方法および装
置について添付図面を参照しながら詳細に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The radio wave source position locating method and apparatus of the present invention will be described in detail below with reference to the accompanying drawings.

【0013】図1には、本発明の一実施例の電波源位置
標定装置のブロック図が示されている。この電波源位置
標定装置は、有限な平面領域11に位置する電波源10
から放射される信号を受信する4台のアンテナ121
124 と、各アンテナ121〜124 にそれぞれ接続さ
れた4台の受信器131 〜134 と、受信器131 〜1
4 にそれぞれ接続され、受信信号をそれぞれ3つの出
力に分配する信号分配器161 〜164 と、各受信器1
1 〜134 の組み合わせより成る2つの受信信号の相
互相関関数を位相差信号 1,2 〜M 3,4 として出力するミ
キサ171 〜176 と、ミキサ出力 1,2 〜M 3,4 を演
算して電波源の位置を標定する演算回路(MP)15よ
り構成されている。
FIG. 1 is a block diagram of a radio wave source position locating device according to an embodiment of the present invention. This radio wave source position locator includes a radio wave source 10 located in a finite plane area 11.
4 antennas 12 1 to receive signals radiated from
12 4 , four receivers 13 1 to 13 4 respectively connected to the antennas 12 1 to 12 4 , and receivers 13 1 to 1
Signal distributors 16 1 to 16 4 respectively connected to 3 4 and distributing received signals to three outputs, and each receiver 1
Mixers 17 1 to 17 6 for outputting a cross-correlation function of two reception signals composed of a combination of 3 1 to 13 4 as phase difference signals M 1,2 to M 3,4 and mixer outputs M 1,2 to M 3 , 4 to locate the position of the radio wave source.

【0014】受信器13(131 〜134 )は、図2に
示されているように、アンテナ12(121 〜124
で受信した受信信号を所定のレベルまで増幅する低雑音
増幅器18と、増幅した受信信号の振幅を一定にするリ
ミッタ19と、振幅が一定な受信信号のレベルを所定の
レベルに減衰して調整する可変抵抗減衰器20と、アン
テナ12から可変抵抗減衰器20までに至る経路の違い
や周囲環境の変化によって生じる各受信器13の移相量
を一定にする移相器21より構成されている。
The receiver 13 (13 1 to 13 4 ) has an antenna 12 (12 1 to 12 4 ) as shown in FIG.
The low noise amplifier 18 that amplifies the received signal received at 1. to a predetermined level, the limiter 19 that makes the amplitude of the amplified received signal constant, and the level of the received signal whose amplitude is constant is attenuated and adjusted to a predetermined level. The variable resistance attenuator 20 and the phase shifter 21 that keeps the phase shift amount of each receiver 13 constant due to the difference in the path from the antenna 12 to the variable resistance attenuator 20 and the change in the surrounding environment are configured.

【0015】アンテナ12(121 〜124 )として、
水平面内又は垂直面内無指向性,或いは有限な平面領域
11の方向に広い指向性を有したものを使用している。
As the antenna 12 (12 1 to 12 4 ),
An omnidirectional pattern in the horizontal plane or the vertical plane, or a wide directional pattern in the direction of the finite plane region 11 is used.

【0016】演算回路15は、図3に示されているよう
に有限な平面領域11を座標として入力する座標入力部
22と、座標上の各点を電波源と仮定したとき、そこか
ら放射される信号を各アンテナ121 〜124 で受信し
たときの仮想受信信号の位相を各点について演算する位
相演算部23と、各点の仮想受信信号のアンテナ間の位
相差から相互相関関数IMを演算する位相差演算部24
と、ミキサ17から出力される位相差信号 1,2 〜M 3,4
を入力する測定位相差入力部25と、位相差演算部24
で演算された演算に基づく位相差から求めた相互相関関
数IMと測定位相差入力部25より入力した測定に基づ
く位相差信号M 1,2 〜M 3,4 を比較する比較回路26と、
比較回路26の比較結果において、測定に基づく位相差
信号M 1,2 〜M 3,4 に最も近似したを演算に基づく複数
位置の位相差から求めた相互相関関数IMから選択し、
選択した位相差から求めた相互相関関数IMに対応した
座標上の点を電波源の位置として標定する電波源標定回
路27と、標定結果を表示する表示部28より構成され
ている。
As shown in FIG. 3, the arithmetic circuit 15 has a coordinate input section 22 for inputting a finite plane area 11 as coordinates, and when each point on the coordinates is assumed to be a radio wave source, it is radiated from it. Phase calculation unit 23 that calculates the phase of the virtual received signal when each of the antennas 12 1 to 12 4 is received by each antenna 12 1 to 12, and the cross-correlation function IM from the phase difference between the antennas of the virtual received signal of each point. Phase difference calculator 24 for calculating
And the phase difference signals M 1,2 to M 3,4 output from the mixer 17
And a phase difference calculator 24 for inputting the measured phase difference
The cross-correlation relation calculated from the phase difference based on the calculation
A comparator circuit 26 for comparing the number IM and the phase difference signals M 1,2 to M 3,4 based on the measurement input from the measurement phase difference input unit 25 ;
In the comparison result of the comparison circuit 26, the phase difference based on the measurement
A value that is most approximate to the signals M 1,2 to M 3,4 is selected from the cross-correlation function IM obtained from the phase differences at a plurality of positions based on the calculation,
A radio source locating circuit 27 for locating a point on the coordinate corresponding to the cross-correlation function IM obtained from the selected phase difference as the position of the radio source, and a display unit 28 for displaying the orientation result.

【0017】以下、上記標定装置を用いた本発明の電波
源位置標定方法を説明する。まず、電波源10が存在し
ていると考慮する有限な広さの平面領域11を座標とし
て演算回路15の座標入力部22から入力する。すなわ
ち、図4に示すように、平面領域11のX軸の座標値n
とY軸の座標値mを入力することにより、平面領域11
をn×m個の点から成る座標として表す。
The radio source position locating method of the present invention using the above locator will be described below. First, a plane area 11 having a finite width, which is considered to exist the radio wave source 10, is input as coordinates from the coordinate input unit 22 of the arithmetic circuit 15. That is, as shown in FIG. 4, the coordinate value n of the X-axis of the plane area 11
And the coordinate value m of the Y axis are input, the plane area 11
Is represented as a coordinate composed of n × m points.

【0018】座標入力部22からの入力が完了すると、
座標入力部22から平面領域11の座標を表す座標信号
が位相演算部23に出力される。位相演算部23はこの
座標信号を入力して、座標上のn×m個の各点を電波源
と仮定したとき、そこから放射されている信号を各アン
テナ121 〜124 で受信したときの仮想受信信号の位
相を各点について演算する。この演算結果は位相差演算
部24に出力され、位相演算部24は各アンテナ12
1 〜124 で受信した各点の仮想受信信号間の位相差
ら相互相関関数IMを演算する。すなわち、この演算結
果によって座標上の各点について以下のアンテナで受信
した6通りの仮想的な位相差から相互相関関数IMが得
られる。 (1) アンテナ121 とアンテナ122 (2) アンテナ121 とアンテナ123 (3) アンテナ121 とアンテナ124 (4) アンテナ122 とアンテナ123 (5) アンテナ122 とアンテナ124 (6) アンテナ123 とアンテナ124
When the input from the coordinate input section 22 is completed,
A coordinate signal representing the coordinates of the plane area 11 is output from the coordinate input unit 22 to the phase calculation unit 23. When the phase calculation unit 23 inputs this coordinate signal and assumes n × m points on the coordinate as radio wave sources, when signals radiated from the points are received by the respective antennas 12 1 to 12 4. The phase of the virtual received signal of is calculated for each point. This calculation result is output to the phase difference calculation unit 24, and the phase difference calculation unit 24 causes each antenna 12
Is it the phase difference between the virtual received signals at each point received at 1 to 12 4 ?
To calculate the cross-correlation function IM . That is, the cross-correlation function IM is obtained from the six types of virtual phase differences received by the following antennas for each point on the coordinate according to this calculation result. (1) Antenna 12 1 and Antenna 12 2 (2) Antenna 12 1 and Antenna 12 3 (3) Antenna 12 1 and Antenna 12 4 (4) Antenna 12 2 and Antenna 12 3 (5) Antenna 12 2 and Antenna 12 4 (6) Antenna 12 3 and antenna 12 4

【0019】一方、平面領域11に存在する電波源10
からの放射電波S0は、解析信号を用いて以下のように
表すことができる。 S0=P・exp{j(ωt+φ0)} (1) (1) 式において、Pは振幅,ωは2πf,fは周波数,
φ0は初期位相である。
On the other hand, the radio wave source 10 existing in the plane area 11
The radiated radio wave S0 from can be expressed as follows using an analysis signal. S0 = P · exp {j (ωt + φ0)} (1) In the equation (1), P is the amplitude, ω is 2πf, f is the frequency,
φ0 is the initial phase.

【0020】電波源10から放射された信号は、受信器
131 〜134 のアンテナ121 〜124 でそれぞれ受
信される。それぞれの受信器131 〜134 で受信され
た信号Siは、以下のように表すことができる。 (2) 式において、riは電波源10から各アンテナ12
1 〜124 までの距離,φiはκ・ri,κはω/c,
cは光速である。
The signal emitted from the radio wave source 10, are received respectively by antennas 12 1 to 12 4 of the receiver 131-134. The signal Si received by each of the receivers 13 1 to 13 4 can be expressed as follows. In the equation (2), ri is from the radio wave source 10 to each antenna 12
Distance from 1 to 12 4 , φi is κ · ri, κ is ω / c,
c is the speed of light.

【0021】受信器131 〜134 では、アンテナ12
1 〜124 で受信した受信信号を低雑音増幅器18で所
定のレベルまで増幅し、次いで、リミッタ19で受信信
号の振幅を一定にし、更に、可変抵抗減衰器20で受信
信号のレベルを所定のレベルに減衰し、最後に、移相器
21でアンテナ12から可変抵抗減衰器20までに至る
経路の違いや周囲環境の変化によって生じる各受信器1
3の移相量を一定にした後、出力する。
In the receivers 13 1 to 13 4 , the antenna 12
The low noise amplifier 18 amplifies the received signal received at 1 to 12 4 to a predetermined level, then the limiter 19 makes the amplitude of the received signal constant, and the variable resistance attenuator 20 further sets the received signal level to a predetermined level. Each of the receivers 1 is attenuated to a level and finally caused by a difference in the path from the antenna 12 to the variable resistance attenuator 20 in the phase shifter 21 and a change in the surrounding environment.
After the phase shift amount of 3 is made constant, it is output.

【0022】受信器131 〜134 から出力された受信
信号は、信号分配器161 〜164でそれぞれ3つの受
信信号として出力され、ミキサ171 〜176 にそれぞ
れ入力する。ミキサ171 〜176 に入力する入力信号
SCiは、以下のように表すことができる。 SCi=exp{j(ωt+φ0+φi)} (i=1〜4) (3) ミキサ171 〜176 への入力は、以下のアンテナで受
信した6通りの受信信号である。 (1) アンテナ121 とアンテナ122 (2) アンテナ121 とアンテナ123 (3) アンテナ121 とアンテナ124 (4) アンテナ122 とアンテナ123 (5) アンテナ122 とアンテナ124 (6) アンテナ123 とアンテナ124
The reception signals output from the receivers 13 1 to 13 4 are output as three reception signals by the signal distributors 16 1 to 16 4 and input to the mixers 17 1 to 17 6 , respectively. The input signal SCi input to the mixers 17 1 to 17 6 can be expressed as follows. SCi = exp {j (ωt + φ0 + φi)} (i = 1 to 4) (3) The inputs to the mixers 17 1 to 17 6 are six types of received signals received by the following antennas. (1) Antenna 12 1 and Antenna 12 2 (2) Antenna 12 1 and Antenna 12 3 (3) Antenna 12 1 and Antenna 12 4 (4) Antenna 12 2 and Antenna 12 3 (5) Antenna 12 2 and Antenna 12 4 (6) Antenna 12 3 and antenna 12 4

【0023】ミキサ171 〜176 は、入力した2つの
受信信号の位相差に比例した相互相関関数を位相差信号
1,2 〜M 3,4 として出力する。ミキサ171 〜176
らの出力信号Mk,lは、以下のように表すことができ
る。 Mk,l=SCk・SCl* =exp{j(φk−φl)} (k=1〜3,l=k+1〜4) (4) (4) 式において、*は複素共役を表す。また、ミキサ出
力Mk,lはそれぞれのアンテナ121 〜124 で受信
した信号の位相差φk−φlの値のcosineに比例
する。
The mixers 17 1 to 17 6 form the cross-correlation function proportional to the phase difference between the two input received signals by the phase difference signal.
Output as M 1,2 to M 3,4 . The output signals Mk, l from the mixers 17 1 to 17 6 can be expressed as follows. Mk, l = SCk.SCl * = exp {j (φk-φl)} (k = 1 to 3, l = k + 1 to 4) (4) In the formula (4), * represents a complex conjugate. The mixer output Mk, l is proportional to the cosine of the value of the phase difference φk−φl of the signals received by the respective antennas 12 1 to 12 4 .

【0024】ミキサ171 〜176 から出力された位相
差信号 1,2 〜M 3,4 は、演算回路15に入力され、演算
回路15では、比較回路26において前述した位相差演
24で演算して求めた仮想的な位相差から(4)式
を用いて演算した相互相関関数IMと、測定位相差入力
部25から入力した測定に基づく位相差信号M 1,2 〜M
3,4 との差ΔMを平面領域11上のあらゆる点,或いは
選択された所定の点に関して計算し、更に、電波源標定
回路27においてΔMが最小となる平面領域11の座標
上の点から捜し出してその点を電波源10として標定
し、最後に、標定結果を表示部28に表示する。
The phase difference signal M 1, 2 ~M 3, 4 which are outputted from the mixer 17 1-17 6 is input to the arithmetic circuit 15, the arithmetic circuit 15, a phase difference calculation section 24 described above in the comparison circuit 26 Equation (4) from the virtual phase difference calculated by
A cross-correlation function IM computed using a phase difference signal M 1, 2 ~M based on measurements input from the measured phase difference input section 25
The difference ΔM between 3 and 4 is calculated with respect to all points on the plane area 11 or selected predetermined points, and further, it is searched for from the point on the coordinates of the plane area 11 where ΔM becomes the minimum in the radio wave source locating circuit 27. The point is located as the radio wave source 10, and finally, the result of the orientation is displayed on the display unit 28.

【0025】上記した電波源位置標定方法において、電
波源10の標定精度は演算器15における入力信号M
k,lのA/D変換ステップ数に依存するため、このス
テップ数を多くして1つのステップを小さくすれば精度
を向上させることができ、分解能を1波長よりも小さい
値にすることができる。理論的にはA/D変換のステッ
プ数を無限に多くすれば、分解能は限り無く0に近づく
ことになるため、非常に分解能の良い電波源の位置標定
が期待できる。
In the above-mentioned radio wave source position locating method, the accuracy of locating the radio wave source 10 depends on the input signal M in the calculator 15.
Since it depends on the number of A / D conversion steps of k and l, the accuracy can be improved by increasing the number of steps and reducing one step, and the resolution can be set to a value smaller than one wavelength. . Theoretically, if the number of A / D conversion steps is increased infinitely, the resolution will approach 0 as much as possible, so that the location of the radio wave source with very good resolution can be expected.

【0026】以上説明した実施例では、アンテナおよび
受信器が4台の場合について述べたが、アンテナおよび
受信器の台数は少なくとも2台以上あれば良く、また多
い方が効果が大きくなり、実質的には6台以上が望まし
い。
In the above-described embodiments, the case where the number of antennas and receivers is four has been described. However, the number of antennas and receivers should be at least two or more, and the larger the number, the greater the effect and the substantial effect. It is desirable to have 6 or more units.

【0027】[0027]

【発明の効果】以上説明したように、本発明の電波源位
置標定方法および装置によると、有限の平面領域に位置
する電波源から連続波として放射される信号を少なくと
も2つの位置で受信して受信信号間の位相差を相互相関
関数として測定によって求め、平面領域の複数のから
放射されたと仮定した仮想信号を少なくとも2つの位置
で受信したと仮定したときの仮想受信信号間の位相差を
相互相関関数として演算によって求め、測定に基づく
互相関関数と複数のに対応する演算に基づく相互相関
関数とを比較して測定に基づく相互相関関数に最も近
似した相互相関関数を複数の点に対応する演算に基づく
相互相関関数から選択し、選択された相互相関関数に対
応したを電波源の位置として標定するようにしたた
め、連続波を放射する電波源でも高い精度で標定できる
ようにすることができる。
As described above, according to the radio wave source position locating method and apparatus of the present invention, a signal radiated as a continuous wave from a radio wave source located in a finite plane area is received at at least two positions. Cross-correlate phase difference between received signals
Determined by measurement as a function of the phase difference between the virtual reception signal, assuming that received on has been assumed the two even less without a virtual signal position radiation from a plurality of points of the plane area
Calculated as a cross-correlation function and phase based on measurement
Cross-correlation based on cross-correlation function and operation corresponding to multiple points
By comparing the function, based on the cross-correlation function that best approximates the cross-correlation function based on the measurement operation corresponding to a plurality of points
Select from the cross-correlation function, because you to locating the points corresponding to the cross-correlation function is selected as the position of the radio source, it is possible to allow orientation with high precision even in radio sources that emit continuous wave.

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

【図1】本発明の一実施例を示すブロック図。FIG. 1 is a block diagram showing an embodiment of the present invention.

【図2】一実施例に係る受信器の内部構成を示す回路
図。
FIG. 2 is a circuit diagram showing an internal configuration of a receiver according to an embodiment.

【図3】一実施例に係る演算回路の内部構成を示すブロ
ック図。
FIG. 3 is a block diagram showing an internal configuration of an arithmetic circuit according to an embodiment.

【図4】一実施例に係る平面領域を示す説明図。FIG. 4 is an explanatory diagram showing a plane area according to an embodiment.

【図5】従来の電波源位置標定装置を示すブロック図。FIG. 5 is a block diagram showing a conventional radio wave source position locating device.

【図6】従来の電波源位置標定方法を示す説明図。FIG. 6 is an explanatory view showing a conventional radio wave source position locating method.

【図7】従来の電波源位置標定方法を示す説明図。FIG. 7 is an explanatory diagram showing a conventional radio wave source position locating method.

【符号の説明】[Explanation of symbols]

10 電波源 11 平面領域 12(12〜12) アンテナ 13(13〜13) 受信器 14 到達時間差検出回路 15 演算回路 16〜16 信号分配器 17〜17 ミキサ 18 低雑音増幅器 19 リミッタ 20 可変抵抗減衰器 21 移相器 22 座標入力部 23 位相演算部 24 位相差演算部 25 測定位相差入力部 26 比較回路 27 電波源標定回路 28 表示部10 radio wave source 11 plane area 12 (12 1 to 12 4 ) antenna 13 (13 1 to 13 4 ) receiver 14 arrival time difference detection circuit 15 arithmetic circuit 16 1 to 16 4 signal distributor 17 1 to 17 6 mixer 18 low noise Amplifier 19 Limiter 20 Variable resistance attenuator 21 Phase shifter 22 Coordinate input section 23 Phase calculation section 24 Phase difference calculation section 25 Measurement phase difference input section 26 Comparison circuit 27 Radio wave source localization circuit 28 Display section

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平5−264712(JP,A) 特開 昭61−162765(JP,A) 特開 昭56−98011(JP,A) 特開 昭57−119271(JP,A) 特開 昭63−284481(JP,A) 特開 平5−288823(JP,A) (58)調査した分野(Int.Cl.7,DB名) G01S 5/00 - 5/14 ─────────────────────────────────────────────────── ─── Continuation of the front page (56) Reference JP-A-5-264712 (JP, A) JP-A-61-162765 (JP, A) JP-A-56-98011 (JP, A) JP-A-57- 119271 (JP, A) JP 63-284481 (JP, A) JP 5-288823 (JP, A) (58) Fields investigated (Int.Cl. 7 , DB name) G01S 5/00-5 /14

Claims (5)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 有限の平面領域に位置する電波源から連
続波として放射される信号を少なくともつの位置で受
信してすべての組み合わせの受信信号間の位相差をそれ
ぞれ相互相関関数として測定によって求め、 前記平面領域の複数の点から放射されたと仮定した仮想
信号を前記少なくともつの位置で受信したと仮定した
ときのすべての組み合わせの仮想受信信号間の位相差を
それぞれ相互相関関数として前記複数の点の各点につい
演算によって求め、 前記測定に基づく相互相関関数と前記複数の点に対応す
る前記演算に基づく相互相関関数とを比較して、前記測
定に基づく相互相関関数に最も近似した相互相関関数を
前記複数の点に対応する前記演算に基づく相互相関関数
から選択し、 選択された前記相互相関関数に対応した前記点を前記電
波源の位置として標定することを特徴とする連続波電波
源位置標定方法。
1. A signal radiated as a continuous wave from a radio wave source located in a finite plane area is received at at least four positions and the phase difference between the received signals of all combinations is calculated.
Phase differences between virtual reception signals of all combinations when virtual signals assumed to be emitted from a plurality of points in the planar area are received at the at least four positions, which are obtained by measurement as cross-correlation functions. To
For each of the above-mentioned points as a cross-correlation function,
The cross-correlation function based on the measurement is compared with the cross-correlation function based on the calculation corresponding to the plurality of points, and the cross-correlation function that is the closest to the cross-correlation function based on the measurement is calculated. A method for locating a continuous wave radio wave source, characterized by selecting from the cross-correlation function based on the calculation corresponding to the point, and locating the point corresponding to the selected cross-correlation function as the position of the radio wave source.
【請求項2】 有限な平面領域に位置する電波源から連
続波として放射される信号を少なくともつの位置で受
信する少なくともつの受信手段と、 前記少なくともつの受信手段によって受信したすべて
の組み合わせの受信信号間の位相差をそれぞれ相互相関
関数として測定する位相差測定手段と、 前記平面領域の複数の点から放射されたと仮定した仮想
信号を前記少なくともつの位置で受信したと仮定した
ときのすべての組み合わせの仮想受信信号間の位相差を
それぞれ相互相関関数として前記複数の点の各点につい
演算によって求め、前記測定に基づく相互相関関数と
前記複数の点に対応する前記演算に基づく相互相関関数
とを比較して、前記測定に基づく相互相関関数に最も近
似した相互相関関数を前記複数の点に対応する前記演算
に基づく相互相関関数から選択し、選択した前記相互相
関関数に対応した前記点を前記電波源の位置として標定
する演算手段とを備えることを特徴とする連続波電波源
位置標定装置。
Wherein at least four receiving means for receiving at least four positions signal emitted as a continuous wave from a radio wave source located on finite planar region, all received by the at least four receiving means
It is assumed that the phase difference measuring means for measuring the phase difference between the received signals of the combination of 1 and 2, respectively, and the virtual signals assumed to be radiated from the plurality of points in the plane area are received at the at least four positions. The phase difference between the virtual received signals of all combinations when
For each of the above-mentioned points as a cross-correlation function,
The cross-correlation function based on the measurement is compared with the cross-correlation function based on the calculation corresponding to the plurality of points, and the cross-correlation function most approximate to the cross-correlation function based on the measurement is calculated. select from the cross-correlation function based on the operation that corresponds to the point of continuous wave radio source, characterized in that the point corresponding to the cross-correlation function selected and a calculation means for locating the position of the radio sources Position locator.
【請求項3】 前記受信手段は、前記電波源から放射さ
れる信号を受信するアンテナと、前記アンテナで受信し
た受信信号を所定のレベルまで増幅する低雑音増幅器
と、増幅した受信信号の振幅を一定にするリミッタと、
振幅が一定な受信信号のレベルを所定のレベルに減衰調
整する可変抵抗減衰器と、前記少なくともつの受信手
段間の受信動作中に生じる移相が一定となるように校正
する移相器より構成されている請求項2の連続波電波源
位置標定装置。
3. The receiving means includes an antenna for receiving a signal radiated from the radio wave source, a low noise amplifier for amplifying a received signal received by the antenna to a predetermined level, and an amplitude of the amplified received signal. A limiter that keeps it constant,
A variable resistance attenuator that attenuates and adjusts the level of a received signal whose amplitude is constant to a predetermined level, and a phase shifter that calibrates so that the phase shift generated during the receiving operation between the at least four receiving means is constant. The continuous wave radio wave source position locating device according to claim 2.
【請求項4】 前記アンテナは、水平面内又は垂直面内
無指向性,或いは前記有限な平面領域の方向に広い指向
性を有する構成の請求項3の連続波電波源位置標定装
置。
4. The continuous wave radio wave source position locating device according to claim 3, wherein the antenna has a non-directivity in a horizontal plane or a vertical plane, or has a wide directivity in the direction of the finite plane region.
【請求項5】 前記演算手段は、前記有限な平面領域を
座標として入力する座標入力部と、前記座標上の各点を
前記電波源と仮定したときに前記少なくともつの受信
手段が受信すると想定されるすべての組み合わせの前記
仮想受信信号の位相をそれぞれ前記各点について演算す
る位相演算部と、前記少なくともつの受信手段が受信
すると想定されるすべての組み合わせの前記仮想受信信
号の位相差から相互相関関数をそれぞれ前記各点につい
て演算する位相差演算部と、前記位相差測定手段によっ
て測定された前記測定に基づく位相差を相互相関関数と
して入力する測定位相差入力部と、前記位相差演算部で
演算された前記演算に基づく相互相関関数と前記測定位
相差入力部より入力した前記測定に基づく相互相関関数
とを比較する比較回路と、前記比較回路の比較結果にお
いて、前記測定に基づく相互相関関数に最も近似した相
互相関関数を前記座標上の各点に対応する前記演算に基
づく相互相関関数から選択し、選択した前記相互相関関
数に対応した前記座標上の前記点を前記電波源の位置と
して標定する電波源標定回路と、標定結果を表示する表
示部より構成されている請求項2の連続波電波源位置標
定装置。
5. The calculation means is assumed to be received by the at least four reception means when a coordinate input section for inputting the finite plane area as coordinates and each point on the coordinates as the radio wave source. cross the phase of the virtual reception signals of all the combinations are from the phase difference of a phase calculator for calculating for each point, the virtual reception signal of the all at least four receiving means are supposed to receive a combination a phase difference calculator for calculating the correlation function respectively the points, the measured phase difference input unit for inputting a phase difference based on the measurement measured by the phase difference measuring means as a cross-correlation function, the phase difference computation unit A comparison circuit for comparing the cross-correlation function based on the calculation calculated in step 1 and the cross-correlation function based on the measurement input from the measurement phase difference input unit. Path and the comparison result of the comparison circuit, a cross-correlation function most approximate to the cross-correlation function based on the measurement is selected from the cross-correlation function based on the calculation corresponding to each point on the coordinate, and the selected cross-correlation function is selected. 3. The continuous wave radio wave source position locating device according to claim 2, further comprising a radio wave source locating circuit for locating the point on the coordinates corresponding to a correlation function as a position of the radio wave source, and a display section for displaying a locating result.
JP31906793A 1993-11-25 1993-11-25 Radio source location method and device Expired - Fee Related JP3454892B2 (en)

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JPH07146352A JPH07146352A (en) 1995-06-06
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