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JPH0138270B2 - - Google Patents
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JPH0138270B2 - - Google Patents

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Publication number
JPH0138270B2
JPH0138270B2 JP57225908A JP22590882A JPH0138270B2 JP H0138270 B2 JPH0138270 B2 JP H0138270B2 JP 57225908 A JP57225908 A JP 57225908A JP 22590882 A JP22590882 A JP 22590882A JP H0138270 B2 JPH0138270 B2 JP H0138270B2
Authority
JP
Japan
Prior art keywords
signal
delay time
value
time difference
estimated value
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
JP57225908A
Other languages
Japanese (ja)
Other versions
JPS59116562A (en
Inventor
Masao Igarashi
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.)
Oki Electric Industry Co Ltd
Original Assignee
Oki Electric Industry 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 Oki Electric Industry Co Ltd filed Critical Oki Electric Industry Co Ltd
Priority to JP57225908A priority Critical patent/JPS59116562A/en
Publication of JPS59116562A publication Critical patent/JPS59116562A/en
Publication of JPH0138270B2 publication Critical patent/JPH0138270B2/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
    • G01S3/80Direction-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 ultrasonic, sonic or infrasonic waves
    • G01S3/802Systems for determining direction or deviation from predetermined direction
    • G01S3/808Systems for determining direction or deviation from predetermined direction using transducers spaced apart and measuring phase or time difference between signals therefrom, i.e. path-difference systems

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
  • Radar Systems Or Details Thereof (AREA)

Description

【発明の詳細な説明】 (技術分野) 本発明は、雑音を含む狭帯域信号を空間的に配
列された複数の素子からなるアレーで受信し、該
アレーの2素子の出力信号間の位相差を推定する
ことにより、該信号のアレーに対する入射角を求
める信号入射角の推定方法に関する。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention receives a narrowband signal containing noise with an array consisting of a plurality of spatially arranged elements, and detects the phase difference between the output signals of two elements of the array. The present invention relates to a method for estimating the angle of incidence of a signal by estimating the angle of incidence of the signal onto an array.

(背景技術) 2つの素子からなるアレーを用いて、該アレー
の2素子の出力信号間の位相差を推定することに
より、該アレー上の基準軸に対する信号入射角を
推定する信号入射角測定装置は、ソーナー、音響
測位装置あるいはレーダにおいて広く用いられて
いる。よく知られているように受信信号が狭帯域
信号である場合、前記信号入射角の推定において
グローテイング・ローブによる曖昧さを避けるた
めには、前記アレーの素子の配列間隔を該狭帯域
信号の波長の1/2以下にとらなければならないと
いう制約がある。一方、該受信信号には一般に雑
音が付加されるから、前記信号入射角の推定値に
は推定誤差が生じ、該誤差は例えば文献「五十
嵐、似鳥;“平面受波器アレーを用いたSSBL音
響測位方式”、電子通信学会論文誌、Vol.J65−
A、No.3」で示されているように、前記素子の配
列間隔長に反比例する。このような理由のために
従来は前記両者を考慮して、前記アレーの2素子
の配列間隔を信号波長の1/2にとるか、あるいは
アレーの各素子に指向性を持たせて該アレーの視
野角に制限を加えることによりサイド・ローブに
よる曖昧さを避け、これによつて前記素子の配列
間隔を1/2以上にとる方法が用いられてきた。
(Background Art) A signal incidence angle measurement device that uses an array consisting of two elements and estimates the signal incidence angle with respect to a reference axis on the array by estimating the phase difference between the output signals of the two elements of the array. is widely used in sonar, acoustic positioning equipment or radar. As is well known, when the received signal is a narrowband signal, in order to avoid ambiguity due to growing lobes in estimating the angle of incidence of the signal, the arrangement spacing of the elements of the array should be adjusted to match the narrowband signal. There is a restriction that it must be less than 1/2 of the wavelength. On the other hand, since noise is generally added to the received signal, an estimation error occurs in the estimated value of the signal incidence angle. “Positioning Method”, Transactions of the Institute of Electronics and Communication Engineers, Vol.J65−
As shown in "A, No. 3", it is inversely proportional to the length of the arrangement interval of the elements. For these reasons, conventionally, taking both of the above into consideration, the spacing between the two elements of the array is set to 1/2 of the signal wavelength, or each element of the array is made to have directivity. A method has been used in which ambiguity due to side lobes is avoided by limiting the viewing angle, thereby increasing the arrangement interval of the elements to 1/2 or more.

従つてこのような従来の方法では、信号入射角
を推定するためのアレーの視野角を広くとろうと
すると、素子の配列間隔を信号波長の1/2以下に
しなければならず、このため受信信号の信号対雑
音比が低くなるに伴つて十分な精度が得られなく
なり、また該アレー素子の配列間隔を信号波長の
1/2以上にとる場合には、該アレーの視野角が制
約を受けるという欠点がある。
Therefore, in such conventional methods, in order to widen the viewing angle of the array for estimating the signal incidence angle, the array spacing of the elements must be set to 1/2 or less of the signal wavelength. As the signal-to-noise ratio decreases, sufficient accuracy cannot be obtained, and when the array elements are arranged at intervals of 1/2 or more of the signal wavelength, the viewing angle of the array is restricted. There are drawbacks.

(発明の課題) 本発明はこれらの欠点を除去するために、信号
波長の1/2以下の間隔で配列された2つの素子に
該間隔より長い間隔で配列された他の素子を付加
したアレーを用い、信号入射角の推定時における
広い視野角と高い推定精度の同時実現を目的とす
るものであり、以下詳細に説明する。
(Problems to be solved by the invention) In order to eliminate these drawbacks, the present invention provides an array in which two elements arranged at an interval of 1/2 or less of the signal wavelength are added with another element arranged at an interval longer than the interval. The purpose of this method is to simultaneously achieve a wide viewing angle and high estimation accuracy when estimating the signal incidence angle, and will be described in detail below.

(発明の構成および作用) 第1図は本発明の第1の実施例のアレーの説明
図であつて、11はアレーの第1の素子、12はア
レーの第2の素子、13はアレーの第3の素子で
ある。本実施例では該アレーは直線アレーとし、
各素子11,12,13はX軸上に配列され、素子
1と12の間隔はd1、素子11と13の間隔はd2
あり、狭帯域信号源は十分遠方にある。この狭帯
域信号源から素子11,12,13に入射される入
射信号は、中心周波数f0、波長λ0、周期T0(=
1/f0)、X軸に対して入射角θを有する信号で
ある。該信号の中心周波数の波長をλ0とすると、
前記各素子の間隔d1、d2はd1≦λ0/2、d2>λ0
2に選ばれる。
(Structure and operation of the invention) FIG. 1 is an explanatory diagram of an array according to a first embodiment of the invention, in which 1 1 is the first element of the array, 1 2 is the second element of the array, and 1 3 is the second element of the array. is the third element of the array. In this example, the array is a linear array,
Each element 1 1 , 1 2 , 1 3 is arranged on the X axis, the spacing between elements 1 1 and 1 2 is d 1 , and the spacing between elements 1 1 and 1 3 is d 2 , and the narrowband signal source is sufficient. It's far away. The incident signal input from this narrow band signal source to the elements 1 1 , 1 2 , 1 3 has a center frequency f 0 , a wavelength λ 0 , and a period T 0 (=
1/f 0 ), which is a signal having an incident angle θ with respect to the X-axis. Letting the wavelength of the center frequency of the signal be λ 0 ,
The spacing d 1 and d 2 between each element is d 1 ≦λ 0 /2, d 20 /
Selected as number 2.

第2図は本発明の信号入射角推定方法による第
1の実施例を示す構成図である。21,22,23
は素子11,12,13の出力信号を入力している
増幅器、31,32,33は増幅器21,22,23
出力信号を入力している帯域フイルタ(BPF)
である。41は帯域フイルタ31,32の出力信号
を入力し、出力値φ^1を出力す位相差推定器
(PHD)である。42は帯域フイルタ31,33の信
号を入力し、出力値φ^2を出力する位相差推定器
(PHD)である。51は位相差推定器41の出力値
φ^1と、定数−(d2/d12πf0)とを掛算して疎推定
値τ〓2を得る掛算器(×)である。52は位相差推
定器42の出力値φ^2と、定数−(1/2πf0)とを掛算
して時間遅延差μ^2を得る掛算器(×)である。
FIG. 2 is a block diagram showing a first embodiment of the signal incidence angle estimation method of the present invention. 2 1 , 2 2 , 2 3
are amplifiers to which the output signals of elements 1 1 , 1 2 , and 1 3 are input, and 3 1 , 3 2 , and 3 3 are bandpass filters (BPF) to which the output signals of amplifiers 2 1 , 2 2 , and 2 3 are input. )
It is. 4 1 is a phase difference estimator (PHD) which inputs the output signals of band filters 3 1 and 3 2 and outputs an output value φ^ 1 . 4 2 is a phase difference estimator (PHD) which inputs the signals of band filters 3 1 and 3 3 and outputs an output value φ^ 2 . 5 1 is a multiplier (x) that multiplies the output value φ^ 1 of the phase difference estimator 4 1 by a constant −(d 2 /d 1 2πf 0 ) to obtain a sparse estimated value τ〓 2 . 5 2 is a multiplier (x) that multiplies the output value φ^ 2 of the phase difference estimator 4 2 by a constant -(1/2πf 0 ) to obtain a time delay difference μ^ 2 .

1,62はレジスタ(REG)であり、それぞれ
定数1/2πf0、−(d2/d12πf0)を掛算器51,52
入力している。7は可変遅延時間差発生器であ
り、第5図を参照して以下で詳細に説明するが、
2乗算出器10から予測誤差e(n)を入力し、
整数nを変化させて予測誤差e(n)に対応する
遅延時間差nT0を逐次求めて加算器8に入力する
と共に、予測誤差e(n)が最小値を示すか否か
を調べてこれが最小値を示すときはそのときの遅
延時間差nT0を遅延時間差n^T0として加算器8に
入力する。8は加算器(Σ)であり、掛算器52
から時間遅延差μ2と遅延時間差nT0(但し、n=
−[2d2/λ]…、−1、0、±1、…、[2d2/λ]、
[2d2/λ]は2d2/λを超えない最大の正の整数
である。)とを入力し、それらの加算結果である
遅延時間差の予測値τ2(n)を出力している。9
は加算器(Σ)であり、加算器8から予測値τ2
(n)、掛算器51から疎推定値τ2を入力している。
10は2乗算出器(SQR)であり、加算器9の
出力信号を入力し、予測誤差e(n)を出力して
いる。
6 1 and 6 2 are registers (REG), which input constants 1/2πf 0 and −(d 2 /d 1 2πf 0 ) to multipliers 5 1 and 5 2 , respectively. 7 is a variable delay time difference generator, which will be explained in detail below with reference to FIG.
Input the prediction error e(n) from the square calculator 10,
By varying the integer n, the delay time difference nT 0 corresponding to the prediction error e(n) is successively determined and input to the adder 8, and at the same time, it is checked whether the prediction error e(n) shows the minimum value and this is the minimum value. When indicating a value, the delay time difference nT 0 at that time is input to the adder 8 as the delay time difference n^T 0 . 8 is an adder (Σ), and multiplier 5 2
, the time delay difference μ 2 and the delay time difference nT 0 (where n=
−[2d 2 /λ]…, −1, 0, ±1,…, [2d 2 /λ],
[2d 2 /λ] is the largest positive integer not exceeding 2d 2 /λ. ), and outputs a predicted value of delay time difference τ 2 (n) which is the result of their addition. 9
is an adder (Σ), and the predicted value τ 2 from adder 8 is
(n), the sparse estimated value τ 2 is input from the multiplier 5 1 .
10 is a square calculator (SQR) which inputs the output signal of the adder 9 and outputs the prediction error e(n).

11は角度変換器であり、掛算器8からの予測
値τ2(n^)を入力し、その角度変換値である入射角
θの推定値θ^を出力端子12を介して外部に出力
している。前記アレーの各素子11,12,13
受信された各信号は、前記各増幅器21,22,2
で適当なレベルまで増幅され、各帯域フイルタ
1,32,33で必要としない帯域成分を除去さ
れた後、前記位相差推定器41,42に入力され
る。該位相差推定器41では、前記第1の素子の
出力信号に対する前記第2の素子の出力信号の位
相差(第2の素子の位相差)φ1の推定値φ^1(但し
|φ^1|≦π)を求め、位相差推定器42では、前
記第1の素子の出力信号に対する前記第3の素子
の出力信号の位相差(第3の素子の位相差)φの
推定値φ^2(但し|φ^2|≦π)を求める。該第1の
素子11と第2の素子12との配列間隔d1は信号波
長の1/2以下にとられているから、該第1の素子
1の出力信号に対する第2の素子12の出力信号
の時間遅延差の推定値は、前記第2の素子の位相
差の推定値φ^1から直接−φ^1/2π0(但し0は信

の中心周波数)で求められるのに対して、該第1
の素子11と第3の素子13との配列間隔d2は信号
波長の1/2以上にとられているから、該第1の素
子11の出力信号に対する第3の素子13の出力信
号の遅延時間差の推定値は、前記第3の素子の位
相差の推定値φ^2から直接求めることはできない。
しかし、前記第2の素子の時間遅延差の推定値−
φ^1/2π0を用いて、該第3の素子の時間遅延差を (d2/d1)(−φ^1/2π0)=−d2φ^1/d10 のように推定することは可能である。前記レジス
タ61は定数 −d2/d10 を記憶し、該レジスタ61の出力値と前記位相差
推定器41の出力値φ^1は前記掛算器51で掛け合わ
され、前記第3の素子の遅延時間差の疎推定値 τ〓2△ =−d2φ^1/d12πf0 が求められる。一方、前記レジスタ62は定数 −1/2π0 を記憶し、該レジスタ62の出力と前記位相差推
定器42の出力値φ^2は前記掛算器52で掛け合わさ
れ、該位相差φ^2(但し|φ^2|≦π)に対応する時
間遅延差 μ^2△ =−φ^2/2π0 が求められる。前記可変遅延時間差発生器7は、
信号中心周波数の周期T0△ =1/0の整数倍の
nT0;n=0、±1、…、±[2d2/λ0](但し
[2d2/λ0]は2d2/λ0を越えない最大の正の整数)
を出力し、前記加算器8は該可変遅延時間差発生
器7の出力nT0と前記掛算器52の出力μ^2との和、
すなわち第2の素子の遅延時間差の予測値 τ2(n)△ =μ^2+nT0 を算出して、前記加算器9は前記加算器8の出力
τ2(n)と前記掛算器51の出力τ〓2との差τ〓2(n
)−
τ〓2を算出し、前記2乗値算出器10は該算出値の
2乗すなわち予測誤差 e(n)△ ={τ2(n)−τ〓22 が求められる。前記可変遅延時間差発生器7は、
該予測誤差e(n)を最小とする整数n^に対応す
る遅延時間差値n^T0を出力する。角度変換器11
は、該時間差値n^T0に対応する遅延時間差の予測
値 τ2(n^)△ =μ^2+n^T0 を前記第1の素子11の出力信号に対する第3の
素子の出力信号の遅延時間差の真の推定値とし
て、該推定値τ2(n^)を信号入射角θの推定値θ^に θ^=cos-1{c・τ2(n^)/d2} の関係式に従つて変換し、該推定値θ^を前記出力
端子12に出力する。第5図は可変遅延時間差発
生器7の詳細を示すブロツク図である。第5図に
おいて、13はカウンタであり、アドレス発生器
14にカウントm(=1、2、…m)を入力する。
アドレス発生器14は遅延時間差記憶器15のデ
ータを読出すためのアドレスAmを発生する。遅
延時間差記憶器15はアドレスAmにより、遅延
時間差nT0を出力する。
Reference numeral 11 denotes an angle converter, which inputs the predicted value τ 2 (n^) from the multiplier 8 and outputs the estimated value θ^ of the incident angle θ, which is the angle conversion value, to the outside via an output terminal 12. ing. Each signal received by each element 1 1 , 1 2 , 1 3 of the array is transmitted to each of the amplifiers 2 1 , 2 2 , 2
3 to an appropriate level, and after removing unnecessary band components by band filters 3 1 , 3 2 , 3 3 , the signals are input to the phase difference estimators 4 1 , 4 2 . In the phase difference estimator 4 1 , an estimated value φ^ 1 of the phase difference (phase difference of the second element) φ 1 between the output signal of the second element and the output signal of the first element (where |φ ^ 1 |≦π), and the phase difference estimator 4 2 calculates the estimated value of the phase difference (phase difference of the third element) between the output signal of the third element and the output signal of the first element. Find φ^ 2 (where |φ^ 2 |≦π). Since the arrangement interval d 1 between the first element 1 1 and the second element 1 2 is set to 1/2 or less of the signal wavelength, the second element The estimated value of the time delay difference between the output signals of 1 and 2 can be obtained directly from the estimated value of the phase difference of the second element φ^ 1 by −φ^ 1 /2π 0 (where 0 is the center frequency of the signal). For the first
Since the arrangement interval d 2 between the element 1 1 and the third element 1 3 is set to more than 1/2 of the signal wavelength, the output signal of the third element 1 3 with respect to the output signal of the first element 1 1 is The estimated value of the delay time difference of the output signals cannot be directly obtained from the estimated value φ^ 2 of the phase difference of the third element.
However, the estimated time delay difference of the second element -
Using φ^ 1 / 2π 0 , the time delay difference of the third element is expressed as (d 2 / d 1 ) (−φ^ 1 / 2π 0 ) = −d 2 φ^ 1 / d 10 It is possible to estimate The register 6 1 stores a constant −d 2 /d 10 , and the output value of the register 6 1 and the output value φ^ 1 of the phase difference estimator 4 1 are multiplied by the multiplier 5 1 , and the A sparse estimate of the delay time difference of the third element τ〓 2 △ = −d 2 φ^ 1 /d 1 2πf 0 is obtained. On the other hand, the register 6 2 stores a constant -1/2π 0 , and the output of the register 6 2 and the output value φ^ 2 of the phase difference estimator 4 2 are multiplied by the multiplier 5 2 to calculate the phase difference. A time delay difference μ^ 2 △ = −φ^ 2 /2π 0 corresponding to φ^ 2 (where |φ^ 2 |≦π) is obtained. The variable delay time difference generator 7 is
Period of signal center frequency T 0 △ = integer multiple of 1/0
nT 0 ; n=0, ±1,..., ±[2d 20 ] (However, [2d 20 ] is the largest positive integer that does not exceed 2d 20 )
The adder 8 outputs the sum of the output nT 0 of the variable delay time difference generator 7 and the output μ^2 of the multiplier 52,
That is, the predicted value τ 2 (n)△ = μ^ 2 + nT 0 of the delay time difference of the second element is calculated, and the adder 9 calculates the output τ 2 (n) of the adder 8 and the multiplier 5 1 The difference between the output τ〓 2 and the output τ〓 2 (n
)−
τ〓 2 is calculated, and the square value calculator 10 calculates the square of the calculated value, that is, the prediction error e(n)Δ={τ 2 (n)−τ〓 2 } 2 . The variable delay time difference generator 7 is
A delay time difference value n^T 0 corresponding to the integer n^ that minimizes the prediction error e(n) is output. Angle converter 11
is the predicted value of delay time difference τ 2 (n^)△ = μ^ 2 + n^T 0 corresponding to the time difference value n^T 0 , and the output of the third element with respect to the output signal of the first element 1 1 . As the true estimated value of the signal delay time difference, the estimated value τ 2 (n^) is converted into the estimated value θ^ of the signal incidence angle θ as θ^=cos -1 {c・τ 2 (n^)/d 2 } The estimated value θ^ is output to the output terminal 12. FIG. 5 is a block diagram showing details of the variable delay time difference generator 7. In FIG. 5, 13 is a counter, which inputs a count m (=1, 2, . . . m) to the address generator 14.
Address generator 14 generates address Am for reading data from delay time difference memory 15. The delay time difference memory 15 outputs the delay time difference nT 0 based on the address Am.

16は最小予測誤差Mine(m)と予測誤差e
(n)とを比較する比較器、17は最小値記憶器で
あり、遅延時間差記憶器15から遅延時間差
nT0、2乗乗算器10から予測誤差e(n)及び
比較器16から比較結果を入力し、最小予測誤差
Mine(m)及びこれに対応する遅延時間差n^T0
出力する。
16 is the minimum prediction error Mine (m) and prediction error e
(n), 17 is a minimum value memory, and the delay time difference is stored in the delay time difference memory 15.
nT 0 , the prediction error e(n) from the square multiplier 10 and the comparison result from the comparator 16 are input, and the minimum prediction error is
Output Mine(m) and the corresponding delay time difference n^T 0 .

18は出力切換器であり、最小値記憶器17か
ら遅延時間差n^T0、及び遅延時間差記憶器15か
ら遅延時間差nT0を入力し、遅延時間差nT0(最
終的にn^T0)を出力し、これを加算器8に入力す
る。
18 is an output switch which inputs the delay time difference n^T 0 from the minimum value storage 17 and the delay time difference nT 0 from the delay time difference storage 15, and outputs the delay time difference nT 0 (finally n^T 0 ). This is output and inputted to the adder 8.

可変遅延時間発生器7の動作において、アドレ
ス発生器14はカウンタ13から出力される整数
m=1、2、…mに応じて予め定めたアドレス
Amを発生する。遅延時間差記憶器15は遅延時
間差nT0(但し、n=−[2d2/λ]…、−1、0、
±1、…、[2d2/λ]、[2d2/λ]は2d2/λを超
えない最大の正の整数である。)を記憶しており、
これがアドレスAmにより読出される。読出され
た遅延時間差nT0は、出力切換器18を介して加
算器8に入力される。
In the operation of the variable delay time generator 7, the address generator 14 generates a predetermined address according to the integer m=1, 2,...m output from the counter 13.
Generate Am. The delay time difference memory 15 stores the delay time difference nT 0 (where n=-[2d 2 /λ]..., -1, 0,
±1, ..., [2d 2 /λ], [2d 2 /λ] are the largest positive integers not exceeding 2d 2 /λ. ),
This is read by address Am. The read delay time difference nT 0 is input to the adder 8 via the output switch 18.

最小値記憶器17は、m=1のときに、予測誤
差e(n)を最小予測誤差Mine(m)として、ま
た遅延時間差nT0を遅延時間差n^T0として記憶す
る。
The minimum value storage unit 17 stores the prediction error e(n) as the minimum prediction error Mine(m) and the delay time difference nT 0 as the delay time difference n^T 0 when m=1.

m>2のときに、遅延時間差記憶器15のアド
レスAmに記憶されている遅延時間差nT0に対応
する予測誤差e(n)と、最小値記憶器17に記
憶されている最小予測誤差Mine(m)とを比較器
16により比較して最小予測誤差Mine(m)>予
測誤差e(n)であれば、この予測誤差e(n)を
最小予測誤差Mine(m)として、また遅延時間差
n^T0を遅延時間差n^T0として記憶を更新する。
When m>2, the prediction error e(n) corresponding to the delay time difference nT 0 stored at the address Am of the delay time difference storage 15 and the minimum prediction error Mine ( m) by the comparator 16, and if the minimum prediction error Mine (m) > prediction error e (n), this prediction error e (n) is set as the minimum prediction error Mine (m), and the delay time difference
The memory is updated with n^T 0 as the delay time difference n^T 0 .

このような処理を全てのmについて繰り返すこ
とにより、最小値記憶器17には最終的に全ての
mについての最小予測誤差Mine(m)及び遅延時
間差n^T0が残るので、この最小値の遅延時間差
n^T0が出力切換器18を介して出力される。
By repeating this process for all m, the minimum prediction error Mine(m) and delay time difference n^T 0 for all m will finally remain in the minimum value storage 17, so this minimum value delay time difference
n^T 0 is output via the output switch 18.

以上説明したように、本発明の第1の実施例で
は、配列間隔が信号の波長の1/2以下である第2
の素子の遅延時間差の推定値から、配列間隔が信
号波長の1/2以上である第3の素子の遅延時間差
のおおよその値すなわち疎推定値τ〓2を求め、該第
3の素子の位相差の推定値φ^2と整数値nから求
めたT0周期で離散的に変化できる該第3の素子
の遅延時間差の予測値τ2(n)との2乗誤差を最
小とするような該整数n^に対応する予測値 τ2(n^)=−φ^2/2π0+n^T0 を第1の素子の遅延時間差の真の推定値とするか
ら、信号入射角の任意値に対してサイド・ローブ
による曖昧さを避けることとができ、また信号入
射角の推定精度は、前記整数値n^の推定に誤差が
なければ信号波長の1/2以上の配列間隔の2つの
素子で推定した場合と同等であり、従つて前記従
来の方法に存在した信号入射角の推定時の視野
角、及び精度上の欠点を改善できるという利点が
ある。
As explained above, in the first embodiment of the present invention, the second
From the estimated value of the delay time difference of the elements of A method that minimizes the square error between the estimated value of the phase difference φ^ 2 and the predicted value τ 2 (n) of the delay time difference of the third element, which can vary discretely in the T 0 period obtained from the integer value n. Since the predicted value τ 2 (n^) = −φ^ 2 /2π 0 + n^T 0 corresponding to the integer n^ is the true estimate of the delay time difference of the first element, any value of the signal incidence angle If there is no error in estimating the integer value n^, the accuracy of estimating the angle of incidence of the signal is as follows: This method is equivalent to the estimation using the element, and therefore has the advantage that the disadvantages in terms of viewing angle and accuracy when estimating the signal incidence angle, which existed in the conventional method, can be improved.

第3図は本発明の第2の実施例のアレーの説明
図であつて、14はアレーの第4の素子である。
本実施例では、アレーの第1の素子11と第2の
素子12はX軸上に間隔d1で配列され、該アレー
の第3の素子13と第4の素子14は該X軸と平行
なX′軸上に間隔d2で配列されているものとし、
配列間隔値d1、d2は第1の実施例と同様にとると
する。
FIG. 3 is an explanatory diagram of an array according to a second embodiment of the present invention, and 1 4 is the fourth element of the array.
In this example, the first element 1 1 and the second element 1 2 of the array are arranged on the X-axis with a spacing d 1 , and the third element 1 3 and the fourth element 1 4 of the array are Assume that they are arranged at an interval d 2 on the X' axis parallel to the X axis,
It is assumed that the array interval values d 1 and d 2 are taken in the same manner as in the first embodiment.

第4図は本発明の第2の実施例の構造図であつ
て、24は第4の増幅図、34は第4の帯域フイル
タである。本実施例の場合は、前記位相差推定器
1は第1の実施例と同様に、前記第1の素子11
の出力信号に対する第2の素子12の出力信号の
位相差を推定するのに対して、位相差推定器42
は、前記第3の素子13の出力信号に対する第4
の素子14の出力信号の位相差を推定する。前記
各々の位相差の推定値をφ^1、φ^2とおけば、以下
第1の実施例と同様の方法によつて、前記第3の
素子の出力信号に対する第4の素子の出力信号の
遅延時間差の真の推定値τ2(n^)を求めることがで
き、信号入射角の推定値θ^が求まるので、第2の
実施例であつても第1の実施例と同様の効果を得
ることができる。
FIG. 4 is a structural diagram of the second embodiment of the present invention, where 2 4 is a fourth amplification diagram and 3 4 is a fourth bandpass filter. In the case of this embodiment, the phase difference estimator 4 1 is connected to the first element 1 1 as in the first embodiment.
The phase difference estimator 4 2 estimates the phase difference of the output signal of the second element 1 2 with respect to the output signal of the second element 1 2 .
is the fourth element for the output signal of the third element 13
Estimate the phase difference between the output signals of elements 1 and 4 . If the estimated values of the respective phase differences are set as φ^ 1 and φ^ 2 , the output signal of the fourth element relative to the output signal of the third element can be calculated by using the same method as in the first embodiment. Since the true estimated value τ 2 (n^) of the delay time difference of and the estimated value θ^ of the signal incidence angle can be determined, the second embodiment has the same effect as the first embodiment. can be obtained.

(発明の効果) 本発明は、配列間隔が信号波長の1/2以下の2
つの素子と配列間隔が信号波長の1/2以上の他の
素子を用い、該各素子の出力信号の位相差の推定
値の組合せから該信号入射角の推定値を求めてい
るので、サイド・ローブによる曖昧さがなく、か
つ信号波長の1/2以上の配列間隔の素子で推定し
たのと同等の推定精度が得られるという利点があ
り、高い信号入射角の推定精度を必要とするソー
ナー、音響測定装置あるいはレーダの信号入射角
測定装置に利用することができる。
(Effects of the Invention) The present invention provides two
Since the estimated value of the signal incidence angle is obtained from the combination of the estimated value of the phase difference of the output signal of each element, the side It has the advantage that there is no ambiguity caused by lobes, and that it can obtain estimation accuracy equivalent to that obtained using elements with an arrangement spacing of 1/2 or more of the signal wavelength.Sonar, which requires high estimation accuracy of the signal incidence angle, It can be used in an acoustic measuring device or a radar signal incident angle measuring device.

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

第1図は本発明の第1の実施例を示すアレーの
説明図、第2図は本発明の第1の実施例を示す構
成図、第3図は本発明の第2の実施例を示すアレ
ーの説明図、第4図は本発明の第2の実施例を示
す構成図、第5図は第2図に示す可変時間差発生
器のブロツク図である。 11,12,13,14;アレー素子、21,22
3,24;増幅器、31,32,33,34;帯域フ
イルタ、41,42:位相差推定器、51,52;掛
算器、61,62;レジスタ、7;可変遅延時間差
発生器、8;加算器、9;加算器、10;2乗算
出器、11;角度変換器、12;出力端子。
Fig. 1 is an explanatory diagram of an array showing a first embodiment of the present invention, Fig. 2 is a configuration diagram showing the first embodiment of the invention, and Fig. 3 shows a second embodiment of the invention. FIG. 4 is an explanatory diagram of the array, FIG. 4 is a block diagram showing a second embodiment of the present invention, and FIG. 5 is a block diagram of the variable time difference generator shown in FIG. 1 1 , 1 2 , 1 3 , 1 4 ; array element, 2 1 , 2 2 ,
2 3 , 2 4 ; Amplifier, 3 1 , 3 2 , 3 3 , 3 4 ; Bandpass filter, 4 1 , 4 2 : Phase difference estimator, 5 1 , 5 2 ; Multiplier, 6 1 , 6 2 ; Register , 7; variable delay time difference generator; 8; adder; 9; adder; 10; square calculator; 11; angle converter; 12; output terminal.

Claims (1)

【特許請求の範囲】 1 空間上に配列された複数の素子の出力信号間
の位相差から入射信号の入射角を推定する信号入
射角推定方法において、 第1、第2及び第3の素子を一直線上に配置す
ると共に、 前記第2の素子を前記第1の素子から前記入射
信号の波長(λ)のλ/2以下となる位置に配列
し、 前記第3の素子を前記第1の素子から前記入射
信号の波長のλ/2以上となる位置に配置し、 前記第1の素子の出力信号と前記第2の素子の
出力信号との間の第1の位相差の推定値(φ^1)、
及び前記第1の素子の出力信号と前記第3の素子
の出力信号との間の第2の位相差の推定値(φ^2
を求める第1の処理と、 前記第1の位相差の推定値(φ^1)と、前記第
1及び第2の素子の配列間隔(d1)と、前記第1
及び第3の素子の配列間隔(d2)とに基づき、前
記第1の素子の出力信号に対する前記第2の素子
の出力信号の遅延時間差の疎推定値(τ〓2)を求め
る第2の処理と、 前記第2の位相差の推定値(φ^2)に対応する
時間遅延差(μ^2)と、前記入射信号の中心周波数
の周期(T0)を整数n(但し、n=−[2d2/λ]
…、−1、0、±1、…、[2d2/λ]、[2d2/λ]
は2d2/λを超えない最大の正の整数である。)に
より乗算した値(nT0)とを加算して前記第2の
素子の遅延時間差の予測値(τ2(n))を求める第
3の処理と、 前記疎推定値(τ〓2)と前記第2の素子の遅延時
間差の予測値との間の予測誤差(e(n))を求め
る第4の処理と、 前記整数を逐次変更して前記第3及び第4の処
理を反復的に実行し、最小値を示す前記予測誤差
(e(n))を求める第5の処理と、 前記第5の処理により前記最小値の前記予測誤
差(e(n))に対応する前記遅延時間差の予測値
から前記入射信号の入射角の推定値(θ^)を求め
て、該推定値を前記第1の素子の出力信号に対す
る前記第3の素子の遅延時間差の真の推定値とし
て出力する第6の処理と を有することを特徴とする信号入射角推定方法。 2 空間上に配列された複数の素子の出力信号間
の位相差から入射信号の入射角を推定する信号入
射角推定方法において、 第1及び第2の素子を前記入射信号の波長の1/
2以下の間隔で第1の直線上に配置し、 第3及び第4の素子を前記第1及び第2の素子
の配列と並行させ、かつ前記入射信号の波長の1/
2以上の間隔で第2の直線上に配置し、 前記第1の素子の出力信号と前記第2の素子の
出力信号との間の第1の位相差の推定値(φ^1)、
及び前記第3の素子の出力信号と前記第4の素子
の出力信号との間の第2の位相差の推定値(φ^2
を求める第1の処理と、 前記第1の位相差の推定値(φ^1)と、前記第
1及び第2の素子の配列間隔(d1)と、前記第3
及び第4の素子の配列間隔(d2)とに基づき、前
記第1の素子の出力信号に対する前記第2の素子
の出力信号の遅延時間差の疎推定値(τ〓2)を求め
る第2の処理と、 前記第2の位相差の推定値(φ^2)に対応する
時間遅延差(μ^2)と、前記入射信号の中心周波数
の周期(T0)を整数n(但し、n=−[2d2/λ]
…、−1、0、±1、…、[2d2/λ]、[2d2/λ]
は2d2/λを超えない最大の正の整数である。)に
より乗算した値(nT0)とを加算して前記第2の
素子の遅延時間差の予測値(τ2(n))を求める第
3の処理と、 前記疎推定値(τ〓2)、と前記第2の素子の遅延
時間差の予測値との間の予測誤差(e(n))を求
める第4の処理と、 前記整数を逐次変更して前記第3及び第4の処
理を反復的に実行し、最小値を示す前記予測誤差
(e(n))を求める第5の処理と、 前記第5の処理により前記最小値の前記予測誤
差(e(n))に対応する前記遅延時間差の予測値
から前記入射信号の入射角の推定値(θ^)を求め
て、該推定値を前記第1の素子の出力信号に対す
る前記第4の素子の遅延時間差の真の推定値とし
て出力する第6の処理と を有する信号入射角推定方法。
[Claims] 1. A signal incidence angle estimation method for estimating the incidence angle of an incident signal from the phase difference between the output signals of a plurality of elements arranged in space, wherein the first, second, and third elements are The second element is arranged in a straight line, and the second element is arranged at a position that is less than or equal to λ/2 of the wavelength (λ) of the incident signal from the first element, and the third element is arranged in a position that is less than or equal to λ/2 of the wavelength (λ) of the incident signal. is placed at a position where the wavelength is λ/2 or more of the wavelength of the incident signal from 1 ),
and an estimated value of a second phase difference (φ^ 2 ) between the output signal of the first element and the output signal of the third element.
the estimated value of the first phase difference (φ^ 1 ), the arrangement interval (d 1 ) of the first and second elements, and the first
and a sparse estimation value (τ〓 2 ) of the delay time difference between the output signal of the second element and the output signal of the first element based on the arrangement interval (d 2 ) of the third element. processing, the time delay difference (μ^ 2 ) corresponding to the estimated value of the second phase difference (φ^ 2 ), and the period ( T0 ) of the center frequency of the incident signal as an integer n (where n= −[2d 2 /λ]
..., -1, 0, ±1, ..., [2d 2 /λ], [2d 2 /λ]
is the largest positive integer not exceeding 2d 2 /λ. ) and the predicted value (τ 2 (n)) of the delay time difference of the second element by adding the value (nT 0 ) multiplied by a fourth process of calculating a prediction error (e(n)) between the predicted value of the delay time difference of the second element; and repeating the third and fourth processes by sequentially changing the integer. a fifth process for calculating the prediction error (e(n)) having the minimum value; and a fifth process for calculating the delay time difference corresponding to the prediction error (e(n)) having the minimum value by the fifth process. A second step that calculates an estimated value (θ^) of the angle of incidence of the incident signal from the predicted value and outputs the estimated value as a true estimated value of the delay time difference of the third element with respect to the output signal of the first element. 6. A method for estimating an angle of incidence of a signal, comprising the steps of 2. In a signal incidence angle estimation method for estimating the incidence angle of an incident signal from the phase difference between the output signals of a plurality of elements arranged in space, the first and second elements are set at 1/1 of the wavelength of the incident signal.
The third and fourth elements are arranged on the first straight line with an interval of 2 or less, and the third and fourth elements are parallel to the arrangement of the first and second elements, and the wavelength of the incident signal is 1/1/2.
an estimated value (φ^ 1 ) of a first phase difference between the output signal of the first element and the output signal of the second element, arranged on a second straight line with an interval of 2 or more;
and an estimated value (φ^ 2 ) of a second phase difference between the output signal of the third element and the output signal of the fourth element.
a first process for determining the first phase difference estimate (φ^ 1 ), an arrangement interval (d 1 ) between the first and second elements, and the third
and a sparse estimation value (τ〓 2 ) of the delay time difference between the output signal of the second element and the output signal of the first element based on the array interval (d 2 ) of the fourth element. processing, the time delay difference (μ^ 2 ) corresponding to the estimated value of the second phase difference (φ^ 2 ), and the period ( T0 ) of the center frequency of the incident signal as an integer n (where n= −[2d 2 /λ]
..., -1, 0, ±1, ..., [2d 2 /λ], [2d 2 /λ]
is the largest positive integer not exceeding 2d 2 /λ. ) to obtain a predicted value (τ 2 ( n )) of the delay time difference of the second element; and the sparse estimated value (τ〓 2 ); and a predicted value of the delay time difference of the second element. a fifth process to obtain the prediction error (e(n)) having the minimum value; and a fifth process to calculate the delay time difference corresponding to the prediction error (e(n)) having the minimum value by the fifth process. An estimated value (θ^) of the angle of incidence of the incident signal is obtained from the predicted value of , and the estimated value is output as a true estimated value of the delay time difference of the fourth element with respect to the output signal of the first element. A signal incidence angle estimation method comprising a sixth process.
JP57225908A 1982-12-24 1982-12-24 Estimating system of signal incident angle Granted JPS59116562A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57225908A JPS59116562A (en) 1982-12-24 1982-12-24 Estimating system of signal incident angle

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57225908A JPS59116562A (en) 1982-12-24 1982-12-24 Estimating system of signal incident angle

Publications (2)

Publication Number Publication Date
JPS59116562A JPS59116562A (en) 1984-07-05
JPH0138270B2 true JPH0138270B2 (en) 1989-08-11

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Country Link
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JP2007127503A (en) * 2005-11-02 2007-05-24 Nippon Soken Inc Object position detection device
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JP5063416B2 (en) * 2008-02-29 2012-10-31 三菱電機株式会社 Angle measuring device
US10416269B2 (en) * 2017-04-20 2019-09-17 Raytheon Company Disambiguated direction finding
US10422847B2 (en) * 2017-04-20 2019-09-24 Raytheon Company Interferometric time delay of arrival
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