JPH0244223Y2 - - Google Patents

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Publication number
JPH0244223Y2
JPH0244223Y2 JP14441084U JP14441084U JPH0244223Y2 JP H0244223 Y2 JPH0244223 Y2 JP H0244223Y2 JP 14441084 U JP14441084 U JP 14441084U JP 14441084 U JP14441084 U JP 14441084U JP H0244223 Y2 JPH0244223 Y2 JP H0244223Y2
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JP
Japan
Prior art keywords
ultrasonic waves
transducers
αmax
azimuth
mask
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
JP14441084U
Other languages
Japanese (ja)
Other versions
JPS6160181U (en
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 filed Critical
Priority to JP14441084U priority Critical patent/JPH0244223Y2/ja
Publication of JPS6160181U publication Critical patent/JPS6160181U/ja
Application granted granted Critical
Publication of JPH0244223Y2 publication Critical patent/JPH0244223Y2/ja
Expired legal-status Critical Current

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  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)

Description

【考案の詳細な説明】 〔技術分野〕 本考案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2図乃至第5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、他方をアン
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2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3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2
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4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5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 sinα≒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。
2 to 5 are views showing a conventional example, in which the upper surface 6 which is the detection surface of two vibrators 1a and 1b having cylindrical sensor bodies 8a and 8b.
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 the other is connected to the amplifier 2a, 2b with a cable, 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 respectively, and when ultrasonic waves are incident from the front direction as shown by the solid line arrow in Figure 2, the outputs V 01 and V 02 of the amplifiers 2a and 2b are As shown in FIG. 3, the waveforms have the same phase. Next, from the direction tilted by α degrees from the front direction, the second
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. 4, and a phase difference (φα) occurs. here,
As shown in the top view of FIG. 5a, vibrators 1a and 1b
Let the distance between the centers of oscillators 1a and 1 be l 0 .
b are in contact. ), and the difference in the distance traveled by the ultrasonic waves is Δl, then the azimuth α is sinα≈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).
If the wavelength of the ultrasonic wave is λ, then the condition Δl<|λ/2| must be satisfied.

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)′
becomes sin(αmax′)≒|λ/2l 0 |. That is, when detecting the orientation as described above, the wavelength (λ) of the ultrasonic wave and the transducers 1a, 1b
The maximum detectable azimuth (αmax') is determined by the distance l 0 between the centers of Therefore, the maximum detectable azimuth (αmax') is limited.

〔考案の目的〕[Purpose of invention]

本考案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
の拡角化を計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 was devised in view of the above-mentioned problems, and its purpose is to provide an ultrasonic azimuth sensor capable of widening the maximum detectable azimuth angle.

〔考案の開示〕[Disclosure of invention]

第1図は本考案の実施例を示す図であり、マス
ク3を除いては従来例と同様の構成である。マス
ク3は振動子1a,1bの上面6a,6bを覆
い、振動子1a,1bとの接触部と同じ点で接触
し、半径を小さくした検出孔3a,3bを両振動
子1a,1bごとに上面6a,6b上に設け、
夫々検出孔3a,3bの中心の距離をl1としてあ
る。
FIG. 1 is a diagram showing an embodiment of the present invention, and except for the mask 3, the structure is the same as that of the conventional example. The mask 3 covers the upper surfaces 6a, 6b of the transducers 1a, 1b, makes contact with the transducers 1a, 1b at the same point, and provides detection holes 3a, 3b with a small radius on each of the transducers 1a, 1b. Provided on the upper surfaces 6a and 6b,
The distance between the centers of the detection holes 3a and 3b is defined as l1 .

上述のマスク3の構造により本実施例の最大検
出可能方位角(αmax′)は sin(αmax)≒|λ/2l1| で示され、ここで、l1<l0であるから αmax>αmax′ となり(ただしαmax′はマスク3のないときの最
大検出可能方位角である。)最大検出可能方位角
(αmax)の拡角化が実現できる。
Due to the structure of the mask 3 described above, the maximum detectable azimuth (αmax') of this embodiment is expressed as sin(αmax)≒|λ/2l 1 |, where, since l 1 <l 0 , αmax>αmax (However, αmax' is the maximum detectable azimuth when there is no mask 3.) The maximum detectable azimuth (αmax) can be expanded.

例えば超音波の周波数(f)をf=25kHzとする
と、波長(λ)はλ=13.3〔m/m〕となり、マ
スク3の孔3a,3bの中心間の距離l1をl1=8
〔m/m〕、振動子1a,1bの中心間の距離l0
l0=16〔m/m〕とすると、最大検出可能方位角
(αmax)とマスク3なしの最大検出可能方位角
(αmax′)とは αmax=56゜、αmax′=24゜ となる。なお、検出方位は第1図に示すように上
方向に限定されることはない。
For example, if the frequency (f) of the ultrasonic wave is f = 25 kHz, the wavelength (λ) is λ = 13.3 [m/m], and the distance l 1 between the centers of holes 3a and 3b of the mask 3 is l 1 = 8.
[m/m], the distance l 0 between the centers of vibrators 1a and 1b is
When l 0 =16 [m/m], the maximum detectable azimuth (αmax) and the maximum detectable azimuth (αmax') without the mask 3 are αmax=56° and αmax'=24°. Note that the detection direction is not limited to the upward direction as shown in FIG.

〔考案の効果〕[Effect of idea]

本考案は振動子の検出面を覆い超音波を遮蔽す
るマスクとを有すると共に前記マスクに振動子の
中心間の距離より短かい中心間の距離で振動子の
外径より小さい径の2個の検出孔を各振動子の検
出面に対応するマスクに穿設しているため、最大
検出可能方位角の決定に際する振動子の中心間の
距離を実質上短かくできるので従来振動子の中心
間の距離にて決定されていた最大検出可能方位角
を広くすることができるという効果を有する。
The present invention has a mask that covers the detection surface of the transducer and blocks ultrasonic waves, and the mask includes two pieces having a center-to-center distance shorter than the center-to-center distance of the transducer and a diameter smaller than the outer diameter of the transducer. Since the detection hole is drilled in the mask corresponding to the detection surface of each transducer, the distance between the centers of the transducers when determining the maximum detectable azimuth can be substantially shortened. This has the effect of widening the maximum detectable azimuth, which had been determined based on the distance between the two.

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

第1図aは本考案の実施例を示す上面図、同図
bは側面図、第2図は従来例の概略構成図、第3
図〜第5図は同上の動作説明図である。 1a,1bは振動子、3はマスク、3a,3b
は検出孔、6a,6bは上面である。
Fig. 1a is a top view showing an embodiment of the present invention, Fig. 1b is a side view, Fig. 2 is a schematic configuration diagram of a conventional example, and Fig. 3 is a top view showing an embodiment of the present invention.
5 to 5 are explanatory views of the same operation as above. 1a, 1b are vibrators, 3 are masks, 3a, 3b
is the detection hole, and 6a and 6b are the upper surfaces.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 同一平面内に検出面を配設し入射して来る超音
波を電気信号に変換する2個の振動子と、振動子
の検出面を覆い超音波を遮蔽するマスクを有すと
共に、振動子の中心間の距離より短かい中心間の
距離で振動子の外径より小さい径の2個の検出孔
を各振動子の検出面に対応するマスクに穿設し、
前記振動子にて検出した信号間の位相差を比較
し、超音波の入射して来た方位を検出して成る超
音波方位センサ。
It has two transducers with detection surfaces disposed in the same plane and converts incoming ultrasonic waves into electrical signals, and a mask that covers the detection surfaces of the transducers to shield the ultrasonic waves. Two detection holes with a center-to-center distance shorter than the center-to-center distance and a diameter smaller than the outer diameter of the transducer are drilled in the mask corresponding to the detection surface of each transducer,
An ultrasonic azimuth sensor that compares the phase difference between signals detected by the vibrator and detects the direction in which the ultrasonic waves are incident.
JP14441084U 1984-09-25 1984-09-25 Expired JPH0244223Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14441084U JPH0244223Y2 (en) 1984-09-25 1984-09-25

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14441084U JPH0244223Y2 (en) 1984-09-25 1984-09-25

Publications (2)

Publication Number Publication Date
JPS6160181U JPS6160181U (en) 1986-04-23
JPH0244223Y2 true JPH0244223Y2 (en) 1990-11-22

Family

ID=30702686

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14441084U Expired JPH0244223Y2 (en) 1984-09-25 1984-09-25

Country Status (1)

Country Link
JP (1) JPH0244223Y2 (en)

Also Published As

Publication number Publication date
JPS6160181U (en) 1986-04-23

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