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JPH0436351B2 - - Google Patents
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JPH0436351B2 - - Google Patents

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Publication number
JPH0436351B2
JPH0436351B2 JP19991684A JP19991684A JPH0436351B2 JP H0436351 B2 JPH0436351 B2 JP H0436351B2 JP 19991684 A JP19991684 A JP 19991684A JP 19991684 A JP19991684 A JP 19991684A JP H0436351 B2 JPH0436351 B2 JP H0436351B2
Authority
JP
Japan
Prior art keywords
azimuth
phase
vibrator
output
midpoint
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
JP19991684A
Other languages
Japanese (ja)
Other versions
JPS6177773A (en
Inventor
Naoya Azuma
Hironobu Inoe
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.)
Panasonic Electric Works Co Ltd
Original Assignee
Matsushita Electric Works 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 Matsushita Electric Works Ltd filed Critical Matsushita Electric Works Ltd
Priority to JP19991684A priority Critical patent/JPS6177773A/en
Publication of JPS6177773A publication Critical patent/JPS6177773A/en
Publication of JPH0436351B2 publication Critical patent/JPH0436351B2/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)

Description

【発明の詳細な説明】 〔技術分野〕 本発明は超音波を利用して方位を検出する超音
波方位センサに関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention relates to an ultrasonic azimuth sensor that detects azimuth using ultrasonic waves.

〔背景技術〕[Background technology]

一般に、この種の超音波方位センサは複数の振
動子を用いて超音波を電気信号に変換し、この信
号間の位相差を検出し、伝搬してきた方位を検出
している。
Generally, this type of ultrasonic azimuth sensor uses a plurality of transducers to convert ultrasonic waves into electrical signals, detects the phase difference between these signals, and detects the propagated azimuth.

第4図乃至第7図は従来例を示す図であり、円
筒状の形状を呈したセンサ本体8a,8bを有し
た2個の振動子1a,1bの検出面である上面6
a,6bを同一平面内となるように配設し、前記
センサ本体8a,8b下部に突設した2本の出力
端子7a,7bの一方を夫々接地し、他方のアン
プ2a,2bに夫々ケーブル5にて接続してあ
る。したがつて、振動子1a,1bの上面6a,
6bに入射された超音波は、振動子1a,1bに
て電気信号に夫々変換され、夫々の電気信号をア
ンプ2a,2bにて増幅される。ここで夫々のア
ンプ2a,2bの出力をV01,V02とし、正面方
向から第4図実線の矢印のように超音波が入射さ
れたとき、アンプ2a,2bの出力V01,V02
第5図に示すように同一の位相の波形となる。次
に、正面方向から角度がα度傾いた方位から第4
図の破線矢印にて示すように超音波が入射された
とき、第6図に示すように出力V02は出力V01
り位相が遅れ、位相差φαが生じる。ここで、第
7図aの上面図に示すように振動子1a,1bの
中心間の距離をl0とし(ただし、振動子1a,1
bは接している。)、超音波の到達する距離の差を
Δlとすると、方位角αは simα≒Δl/l0 となる。ところが位相差φαは±πの範囲内でし
か検出できない(例えば、2/3π進んだ位相と
π/3遅れた位相とが区別できない。)ため、超
音波の波長をλとすると Δl<|λ/2| の条件を満足しなければならない。
4 to 7 are diagrams showing a conventional example, in which an upper surface 6 which is a detection surface of two vibrators 1a and 1b having sensor bodies 8a and 8b having a cylindrical shape is shown.
a, 6b are arranged in the same plane, one of the two output terminals 7a, 7b protruding from the lower part of the sensor bodies 8a, 8b is grounded, and a cable is connected to the other amplifier 2a, 2b, respectively. It is connected at 5. Therefore, the upper surface 6a of the vibrator 1a, 1b,
The ultrasonic waves incident on 6b are converted into electrical signals by transducers 1a and 1b, respectively, and the respective electrical signals are amplified by amplifiers 2a and 2b. Here, the outputs of the amplifiers 2a and 2b are V 01 and V 02 , and when ultrasonic waves are incident from the front direction as shown by the solid arrow in FIG. 4, the outputs of the amplifiers 2a and 2b are V 01 and V 02 . As shown in FIG. 5, the waveforms have the same phase. Next, from the direction tilted by α degrees from the front direction, the fourth
When an ultrasonic wave is incident as indicated by a broken line arrow in the figure, the output V 02 lags behind the output V 01 in phase as shown in FIG. 6, and a phase difference φα occurs. Here, as shown in the top view of FIG.
b are in contact. ), and the difference in the distance traveled by the ultrasonic waves is Δl, then the azimuth α is simα≈Δl/l 0 . However, the phase difference φα can only be detected within the range of ±π (for example, a phase advanced by 2/3π and a phase delayed by π/3 cannot be distinguished), so if the wavelength of the ultrasound is λ, then Δl<|λ /2| must satisfy the following conditions.

したがつて、最大検出可能方位角αmax′は sin(αmax′)≒|λ/2l0| となる。すなわち、上述のように方位を検出する
場合、超音波の波長λ及び振動子1a,1bの中
心間の距離l0で最大検出可能方位角αmax′が決ま
つてしまい、さらに超音波の波長λが一定とする
と、振動子1a,1bの中心間の距離l0によつて
最大検出可能方位角αmax′が限定されてしまうと
いう欠点を有していた。
Therefore, the maximum detectable azimuth αmax′ is sin(αmax′)≒|λ/2l 0 |. That is, when detecting the azimuth as described above, the maximum detectable azimuth angle αmax' is determined by the wavelength λ of the ultrasonic wave and the distance l 0 between the centers of the transducers 1a and 1b, and the wavelength λ of the ultrasonic wave If is constant, the disadvantage is that the maximum detectable azimuth αmax' is limited by the distance l 0 between the centers of the vibrators 1a and 1b.

〔発明の目的〕[Purpose of the invention]

本発明は上述の問題点に鑑みて為されたもの
で、その目的とするところは最大検出可能方位角
の拡角化を図ることのできる超音波方位センサを
提供するにある。
The present invention has been made in view of the above-mentioned problems, and its purpose is to provide an ultrasonic azimuth sensor that can widen the maximum detectable azimuth angle.

〔発明の開示〕[Disclosure of the invention]

第1図乃至第3図は本発明の実施例を示す図で
ある。本実施例では第1図に示すように同半径の
円筒状のセンサ本体8a〜8cを有した振動子1
a〜1cを3個を用い、夫々の振動子1a〜1c
の上面6a〜6cを同一平面内に配設し、振動子
1b,1cを検出すべき方位と垂直方向に振動子
1aを振動子1b,1cの中心b,c間の中点O
を含む水平直線上に中心aが来るように配設して
ある。ここで前記中点Oと振動子1aの中心aを
結ぶ直線が検出すべき方位となる。これら振動子
1a〜1cのセンサ本体8a〜8c下部からは
夫々出力端子7a〜7cが2本づつ突設され、
夫々の出力端子7a〜7cはケーブル5にて次に
述べるアンプ2a〜2cに接続される。第2図は
方位検出回路の概略ブロツク図である。まず、振
動子1a〜1cにて超音波を電気信号に変換され
た出力はアンプ2a〜2cに入力され、夫々増幅
される。ここで、これらアンプ2a〜2cの夫々
の出力電圧をVA,VB,VCとし夫々第3図a〜c
に示す波形となる。次に、アンプ2b,2cの出
力電圧Vb,Vcを1/2位相作成回路3にて検出す べき方位上の位相、すなわち、第1図では中点O
の位置での位相に応じた電圧VBCを作成し、第3
図dに示す波形となる。この電圧VBCとアンプ2
aの出力電圧VAとを方位検出回路4にて比較処
理する。この方位検出回路4の出力V0が方位出
力となる。ここで、方位検出回路4は2つのゲー
トG1〜G3を有し、夫々のゲートG1〜G3はアンプ
2aの出力の半周期の1/3の期間だけ動作する。
1 to 3 are diagrams showing embodiments of the present invention. In this embodiment, as shown in FIG. 1, a vibrator 1 has cylindrical sensor bodies 8a to 8c with the same radius.
Using three pieces of a to 1c, each vibrator 1a to 1c
The upper surfaces 6a to 6c are arranged in the same plane, and the transducer 1a is placed at the midpoint O between the centers b and c of the transducers 1b and 1c in a direction perpendicular to the direction in which the transducers 1b and 1c are to be detected.
They are arranged so that the center a is on a horizontal straight line containing the . Here, the straight line connecting the midpoint O and the center a of the vibrator 1a becomes the direction to be detected. Two output terminals 7a to 7c are protruded from the lower part of the sensor bodies 8a to 8c of these vibrators 1a to 1c, respectively.
The respective output terminals 7a to 7c are connected via cables 5 to amplifiers 2a to 2c, which will be described below. FIG. 2 is a schematic block diagram of the direction detection circuit. First, the outputs of ultrasonic waves converted into electrical signals by the transducers 1a to 1c are input to amplifiers 2a to 2c and amplified, respectively. Here, the output voltages of these amplifiers 2a to 2c are V A , V B , and V C , respectively, as shown in Fig. 3 a to c.
The waveform is shown in . Next, the output voltages Vb and Vc of the amplifiers 2b and 2c are determined by the phase in the direction to be detected by the 1/2 phase generation circuit 3, that is, the midpoint O in FIG.
Create a voltage V BC according to the phase at the position of
The waveform is shown in Figure d. This voltage V BC and amplifier 2
The azimuth detection circuit 4 compares the output voltage V A of the output voltage V A with the output voltage V A of the output voltage V A of the output voltage V A of the output voltage a. The output V 0 of this direction detection circuit 4 becomes the direction output. Here, the azimuth detection circuit 4 has two gates G1 to G3 , and each gate G1 to G3 operates only for a period of ⅓ of the half cycle of the output of the amplifier 2a.

この動作状態は第3図e〜gに示すように、ゲー
トG1はアンプ2aの出力の立上りと同時にオン
し、ゲートG2はゲートG1のオフ、ゲートG3はゲ
ートG2のオフと同時にオンする。このゲートG1
〜G3にて1/2位相作成回路3の出力電圧VBCの立 上りの位置がゲートG1〜G3のどのオン期間に属
するかで位相差φαがアンプ2aの出力電圧VA
半周期πの間のどの範囲内であるかを検出し、位
相が遅れているか進んでいるかを検出できるもの
である。
In this operating state, as shown in Fig. 3e to g, gate G1 is turned on at the same time as the output of amplifier 2a rises, gate G2 is turned on when gate G1 is turned off, and gate G3 is turned on when gate G2 is turned off. Turn on at the same time. This gate G 1
~ G3 , the phase difference φα depends on which on period of the gates G1 to G3 the rising position of the output voltage V BC of the 1/2 phase generation circuit 3 belongs to, and the phase difference φα is a half period of the output voltage V A of the amplifier 2a. It is possible to detect within which range of π the phase is, and to detect whether the phase is behind or ahead.

上述のように、本実施例では3個の振動子1a
〜1cを用いることにより、検出方位と垂直方向
の振動子1b,1cの出力の1/2位相作成回路に て、振動子1aと中点Oの点に中心を有する振動
子があるのと同様の位相検出ができるので実質的
に振動子間の距離を小さくすることができる。し
たがつて、片側の最大検出可能方位角αmaxの拡
角化が実現できる。例えば、前記振動子間の距離
l1を8〔m/m〕とし、超音波の周波数を25KHz
(波長λ=13.3m/m)とすると、 αmax≒sin-113.3/2×8≒56゜ となる。なお上述の条件下でのゲートG2の角度
範囲は約18゜〜37゜の方位となる。
As mentioned above, in this embodiment, three vibrators 1a
By using ~1c, it is the same as having a vibrator whose center is at the midpoint O of the vibrator 1a in the 1/2 phase creation circuit of the output of the vibrators 1b and 1c in the direction perpendicular to the detection direction. Since the phase can be detected, the distance between the vibrators can be substantially reduced. Therefore, it is possible to widen the maximum detectable azimuth αmax on one side. For example, the distance between the vibrators
l 1 is 8 [m/m], and the ultrasonic frequency is 25KHz.
(Wavelength λ = 13.3 m/m), αmax≒sin -1 13.3/2×8≒56°. Note that the angular range of the gate G2 under the above conditions is approximately 18° to 37°.

〔発明の効果〕〔Effect of the invention〕

本発明は上述のように、入射される超音波を電
気信号に変換する少なくとも3つの振動子を備
え、すべての振動子を検出面が同一平面内に含ま
れる状態で配置し、第1及び第2の振動子とを互
いに間隔をおいて配置し、第1及び第2の振動子
の検出面の中心間を結ぶ線上の中点において上記
線に直交する線上に検出面の中心を位置させると
共に、上記中点と検出面の中心との距離を少なく
とも外形寸法未満として第3の振動子を配置し、
上記第1及び第2の振動子の出力を用いて第1及
び第2の振動子の出力の位相の半分の位相を持つ
1/2位相信号を作成し、上記中点位置に検出面の
中心が配置されると仮想される第4の振動子の出
力を求める1/2位相信号作成手段と、上記仮想の
第4の振動子と第3の振動子の出力の位相差から
超音波の行路差を求め、この行路差と上記仮想の
第4の振動子と第3の振動子との中心間の距離か
ら超音波が到来する方位を検出する方位検出手段
とを備えているので、第1及び第2の振動子の中
点位置に中心がある仮想的な第4の振動子と第3
の振動子との間で方位の検出を行い、実質的な振
動子間の距離を外形寸法よりも小さくすることが
でき、このため最大検出可能方位角αmaxを広く
することができる効果を有する。
As described above, the present invention includes at least three transducers that convert incident ultrasonic waves into electrical signals, and all the transducers are arranged so that their detection surfaces are included in the same plane. 2 transducers are arranged at intervals from each other, and the center of the detection surface is located on a line perpendicular to the line at the midpoint on the line connecting the centers of the detection surfaces of the first and second transducers, and , a third vibrator is arranged such that the distance between the midpoint and the center of the detection surface is at least less than the outer dimension;
Using the outputs of the first and second vibrators, create a 1/2 phase signal having a phase that is half the phase of the outputs of the first and second vibrators, and place the center of the detection surface at the midpoint position. 1/2 phase signal generating means for calculating the output of a virtual fourth transducer when the virtual fourth transducer is placed; Since it is equipped with an azimuth detecting means that calculates the difference and detects the azimuth in which the ultrasonic wave arrives from this path difference and the distance between the centers of the virtual fourth and third oscillators, the first and a virtual fourth vibrator whose center is at the midpoint of the second vibrator and a third vibrator.
The azimuth can be detected between the oscillators, and the actual distance between the oscillators can be made smaller than the external dimensions, which has the effect of widening the maximum detectable azimuth angle αmax.

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

第1図aは本発明の実施例の上面図、同図bは
側面図、第2図は同上の要部の概略回路ブロツク
図、第3図は同上の要部の動作説明図、第4図乃
至第6図は従来例の動作説明図、第7図aは従来
例の上面図、同図bは側面図である。1a〜1c
は振動子、6a〜6cは上面、a〜cは中心、O
は中点である。
FIG. 1a is a top view of an embodiment of the present invention, FIG. 1b is a side view, FIG. 2 is a schematic circuit block diagram of the main parts of the same, FIG. 6 to 6 are explanatory diagrams of the operation of the conventional example, FIG. 7a is a top view of the conventional example, and FIG. 7b is a side view. 1a-1c
is the vibrator, 6a to 6c are the top surfaces, a to c are the center, O
is the midpoint.

Claims (1)

【特許請求の範囲】[Claims] 1 入射される超音波を電気信号に変換する少な
くとも3つの振動子を備え、すべての振動子を検
出面が同一平面内に含まれる状態で配置し、第1
及び第2の振動子とを互いに間隔をおいて配置
し、第1及び第2の振動子の検出面の中心間を結
ぶ線上の中点において上記線に直交する線上に検
出面の中心を位置させると共に、上記中点と検出
面の中心との距離を少なくとも外形寸法未満とし
て第3の振動子を配置し、上記第1及び第2の振
動子の出力を用いて第1及び第2の振動子の出力
の位相の半分の位相を持つ1/2位相信号を作成し、
上記中点位置に検出面の中心が配置されると仮想
される第4の振動子の出力を求める1/2位相信号
作成手段と、上記仮想の第4の振動子と第3の振
動子の出力の位相差から超音波の行路差を求め、
この行路差と上記仮想の第4の振動子と第3の振
動子との中心間の距離から超音波が到来する方位
を検出する方位検出手段とを備えて成ることを特
徴とする超音波方位センサ。
1 Equipped with at least three transducers that convert incident ultrasonic waves into electrical signals, all the transducers are arranged so that their detection surfaces are included in the same plane, and the first
and a second vibrator are arranged at a distance from each other, and the center of the detection surface is positioned on a line perpendicular to the line at the midpoint on the line connecting the centers of the detection surfaces of the first and second vibrators. At the same time, a third vibrator is arranged so that the distance between the midpoint and the center of the detection surface is at least less than the outer dimension, and the outputs of the first and second vibrators are used to generate the first and second vibrations. Create a 1/2 phase signal with a phase half that of the child's output,
1/2 phase signal generation means for obtaining an output of a virtual fourth vibrator when the center of the detection surface is placed at the midpoint position; Determine the ultrasonic path difference from the output phase difference,
An ultrasonic azimuth characterized by comprising: azimuth detecting means for detecting the azimuth in which the ultrasonic waves arrive from this path difference and the distance between the centers of the virtual fourth and third oscillators. sensor.
JP19991684A 1984-09-25 1984-09-25 Ultrasonic azimuth sensor Granted JPS6177773A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19991684A JPS6177773A (en) 1984-09-25 1984-09-25 Ultrasonic azimuth sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19991684A JPS6177773A (en) 1984-09-25 1984-09-25 Ultrasonic azimuth sensor

Publications (2)

Publication Number Publication Date
JPS6177773A JPS6177773A (en) 1986-04-21
JPH0436351B2 true JPH0436351B2 (en) 1992-06-15

Family

ID=16415729

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19991684A Granted JPS6177773A (en) 1984-09-25 1984-09-25 Ultrasonic azimuth sensor

Country Status (1)

Country Link
JP (1) JPS6177773A (en)

Also Published As

Publication number Publication date
JPS6177773A (en) 1986-04-21

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