JPS5913500A - Transmitter/receiver of ultrasonic wave - Google Patents

Transmitter/receiver of ultrasonic wave

Info

Publication number
JPS5913500A
JPS5913500A JP12131082A JP12131082A JPS5913500A JP S5913500 A JPS5913500 A JP S5913500A JP 12131082 A JP12131082 A JP 12131082A JP 12131082 A JP12131082 A JP 12131082A JP S5913500 A JPS5913500 A JP S5913500A
Authority
JP
Japan
Prior art keywords
ultrasonic waves
piezo
electric element
piezoelectric body
directivity
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.)
Pending
Application number
JP12131082A
Other languages
Japanese (ja)
Inventor
Tadashi Kojima
正 小島
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.)
Nihon Dempa Kogyo Co Ltd
Original Assignee
Nihon Dempa Kogyo 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 Nihon Dempa Kogyo Co Ltd filed Critical Nihon Dempa Kogyo Co Ltd
Priority to JP12131082A priority Critical patent/JPS5913500A/en
Publication of JPS5913500A publication Critical patent/JPS5913500A/en
Pending legal-status Critical Current

Links

Classifications

    • BPERFORMING OPERATIONS; TRANSPORTING
    • B06GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06BMETHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B1/00Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
    • B06B1/02Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy
    • B06B1/06Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with piezoelectric effect or with electrostriction
    • B06B1/0607Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with piezoelectric effect or with electrostriction using multiple elements
    • B06B1/0622Methods or apparatus for generating mechanical vibrations of infrasonic, sonic, or ultrasonic frequency making use of electrical energy operating with piezoelectric effect or with electrostriction using multiple elements on one surface
    • B06B1/0637Spherical array

Abstract

PURPOSE:To obtain an ultrasonic wave transmitter/receiver having flat frequency characteristics in a wide frequency range and non-directivity by forming a piezo-electric element like a hemisphere and preventing the generation of a resonance point at the specific frequency. CONSTITUTION:A hemispherical piezo-electric element 11 consists of piezoelectric crystal such as zircon, lead titanate PZT, lithium niobate and rock crystal. An AC signal is applied to the 1st and 2nd electrodes 12, 13 to project ultrasonic waves to the sperical surface side through lead wires 14, 15 or ultrasonic waves are received, converted into an electric signals and outputted from the lead wires 14, 15. Being formed like a hemisphere, the piezo-electric element 11 has no resonance point at the specific frequency and flat frequency characteristics can be obtained in a wide frequency range. Even if the diameter of the piezo-electric element 11 is larger than the wave length of the used ultrasonic waves, the ultrasonic waves can be transmitted/received at about the same sensitivity in the whole directions of the spherical surface and almost non-directivity can be obtained.

Description

【発明の詳細な説明】 本発明は超音波送受波器に係り、特に周波数特性および
指向特性の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic transducer, and particularly to improvements in frequency characteristics and directivity characteristics.

たとえば超音波の音場測定、・4ワー測定等は超音波送
受波器1.所謂ハイドロホンを用いて行なう。一般にこ
の種の送受波器はl MHz乃至15 MHzの広い周
波数における周波数特性が平坦でかつ無指向性であるこ
とが望ましい。
For example, ultrasonic sound field measurements, 4-wah measurements, etc. are performed using the ultrasonic transducer 1. This is done using a so-called hydrophone. Generally, it is desirable for this type of transducer to have flat frequency characteristics over a wide frequency range of 1 MHz to 15 MHz and to be omnidirectional.

第1図(1) (b)は従来の超音波送受波器の一例を
示す側面図および平面図で図中1は円板状に成形したジ
ルコン、チタン酸鉛(PZT ) 、ニオブ酸リチウム
(LiNb0. ) 、水晶等の圧電体である。そして
この圧電体10表裏板面にそれぞれ電極2,3を設け、
この電極2,3ヘリード線4.5を介して所宇周波数の
交流信号を与えて励振し、超音波を得るようKしている
Figure 1 (1) (b) is a side view and a plan view showing an example of a conventional ultrasonic transducer. In the figure, 1 is made of zircon, lead titanate (PZT), lithium niobate ( It is a piezoelectric material such as LiNb0.) or crystal. Then, electrodes 2 and 3 are provided on the front and back surfaces of the piezoelectric body 10, respectively.
An alternating current signal of a certain frequency is applied to the electrodes 2 and 3 via lead wires 4.5 to excite them, so as to obtain ultrasonic waves.

ところでこの種の超音波送受波器では、たとえばI M
Hz〜15 MHzのように広い周波数範囲で周波数特
性が平坦でかつこの範囲で無指向性であるととが望まし
い。しかしながら第1図に示すような円板状の超音波送
受波器では極く、限定された周波数範囲では平坦な周波
数特性を示すこともあるが広い周波数範囲で平坦な周波
数特性を得ることは困難である。また指向性に関して、
無指向性にするだめには、たとえば周波数10 MHz
で水中における波長は約0.15 rranとなるので
圧電体の直径を0.15m+++以下にする必要がある
。しかし々から、このような寸法は振動子の製造技術上
は不可能であり、まだ圧電体1の直径と厚みの比が5以
下になると多数の径方向の振動モードが発生する問題が
ある。
By the way, in this type of ultrasonic transducer, for example, I M
It is desirable that the frequency characteristics be flat in a wide frequency range such as Hz to 15 MHz and non-directional in this range. However, with a disc-shaped ultrasonic transducer as shown in Figure 1, it is difficult to obtain flat frequency characteristics over a wide frequency range, although it may exhibit flat frequency characteristics in a limited frequency range. It is. Regarding directivity,
To make it omnidirectional, for example, the frequency is 10 MHz.
Since the wavelength in water is approximately 0.15 rran, the diameter of the piezoelectric body must be 0.15 m+++ or less. However, such dimensions are not possible in terms of vibrator manufacturing technology, and there is still a problem that a large number of radial vibration modes will occur if the diameter-to-thickness ratio of the piezoelectric body 1 is less than 5.

本発明は上記の事情に鑑みてなされたもので特定の周波
数に共振点を生じないようにすることによって、広い周
波数範囲で平坦な周波数特性を得られ、しかも無指向性
を得られる超音波送受波器を提供することを目的とする
ものである。
The present invention has been made in view of the above circumstances, and by preventing resonance points from occurring at specific frequencies, it is possible to obtain flat frequency characteristics over a wide frequency range, and also to obtain omnidirectionality. The purpose is to provide wave equipment.

以下本発明の一実施例を第2図(a) (b)に示す側
断面図および底面図を参照して詳細に説明する。
An embodiment of the present invention will be described in detail below with reference to side sectional views and bottom views shown in FIGS. 2(a) and 2(b).

図中11は半球状に成形したノルコン、チタン酸鉛(P
ZT) 、 = オブ酸リチウム(1,lNb0.) 
l水晶等の圧電結晶からなる圧電体である。そしてこの
圧電体11の球面部に第1の電極12を設け、また底面
部に第2の電極13を設け、これら第1、第2の電極1
2.13を相互に電気的に絶縁するとともにそれぞれリ
ード線14.15を介して外部へ導出して送受波器を構
成する。
In the figure, 11 is Norcon, lead titanate (P) formed into a hemispherical shape.
ZT), = lithium oxide (1, lNb0.)
It is a piezoelectric body made of piezoelectric crystal such as l-quartz. A first electrode 12 is provided on the spherical surface of the piezoelectric body 11, and a second electrode 13 is provided on the bottom surface of the piezoelectric body 11.
2 and 13 are electrically insulated from each other and led out to the outside via lead wires 14 and 15, respectively, to constitute a transducer.

なお、圧電体11の底面部の直径は、たとえば最高周波
数15 MHz程度で使用する場合は、1謔程度にすれ
ばよい。
Note that the diameter of the bottom surface of the piezoelectric body 11 may be approximately 1 cm when used at a maximum frequency of approximately 15 MHz, for example.

なお第1、第2の電極12.13は相互に絶縁した状態
であればその一部が底面部あるいは球面部へ延出しても
よい。
Note that a portion of the first and second electrodes 12 and 13 may extend to the bottom surface or the spherical surface as long as they are insulated from each other.

このような構成であればリード線14.15を介して上
記第1、第2の電極12.13へ交流信号を与えて上記
球面側へ超音波を放射し、あるいは超音波を受信して電
気信号に変換し、上記リード線14.15から出力する
ことができる。そして圧電体11を半球状にしているの
で特定の周波数に共振点を持たないようにでき、広い周
波数範囲で平坦な周波数特性を得ることができる。まだ
圧電体11の直径が使用する超音波の波長よりも大きい
場合にも、球面の全ての方向に対して略同−感度で超音
波の送受波が可能であり略無指向性を得ることができる
With such a configuration, an alternating current signal is given to the first and second electrodes 12.13 through the lead wires 14.15 to emit ultrasonic waves to the spherical surface side, or to receive the ultrasonic waves and generate electricity. It can be converted into a signal and output from the lead wires 14 and 15. Since the piezoelectric body 11 has a hemispherical shape, it can be prevented from having a resonance point at a specific frequency, and flat frequency characteristics can be obtained over a wide frequency range. Even if the diameter of the piezoelectric body 11 is larger than the wavelength of the ultrasonic waves used, it is possible to transmit and receive ultrasonic waves with approximately the same sensitivity in all directions of the spherical surface, and it is possible to obtain approximately omnidirectionality. can.

第3図、第4図は周波数特性および指向特性を示す図で
上記実施例の送受波器を曲線A1第1図に示すような従
来の送受波器を曲数Bで示してbる。この図から明らか
なように上記実施例の送受波器では周波数特性も人込範
囲で略平坦であり、また無指向性が得られる。
FIGS. 3 and 4 are diagrams showing frequency characteristics and directivity characteristics, and the transducer of the above embodiment is indicated by curve A1, and the conventional transducer as shown in FIG. 1 is indicated by the number of curves B. As is clear from this figure, the frequency characteristics of the transducer of the above embodiment are approximately flat in the crowded range, and omnidirectionality can be obtained.

なお本発明は上記実施例に限定されるものではなく、た
とえば第5図(a) (b) K示す側断面図および底
面図のように多数の平面からなる多角形によって球面に
近似させた圧電体11を用いるようにしてもよい。この
ようにすれば圧電体11の球面の加工を容易に行なうこ
とができる。また第6図(、) (b)に示す側断面図
および側面図のように球形の圧電体11の表面を略2分
してそれぞれ相互に絶縁して電極12.13を設け、リ
ード線14.15を介して導出するようにしてもよめ。
It should be noted that the present invention is not limited to the above-mentioned embodiments, and, for example, piezoelectrics that are approximated to a spherical surface by a polygon consisting of a large number of planes as shown in the side sectional view and bottom view shown in FIGS. The body 11 may also be used. In this way, the spherical surface of the piezoelectric body 11 can be easily processed. Further, as shown in the side cross-sectional view and side view shown in FIG. You can also derive it via .15.

このようにすれば送受波器の全周の任意の方向に対して
略均等な感度を得られ良好な指向性を得ることができる
In this way, substantially uniform sensitivity can be obtained in any direction around the entire circumference of the transducer, and good directivity can be obtained.

以上詳述したように本発明は、半球体の圧電体の球面お
よび底面にそれぞれ電極を設けて超音波を送受するよう
にしたので広い周波数範囲で平坦な周波数特性を得られ
、しかも無指向性の超音波送受波器を提供することがで
きる。
As described in detail above, the present invention provides electrodes on the spherical surface and the bottom surface of a hemispherical piezoelectric material to transmit and receive ultrasonic waves, so that it is possible to obtain flat frequency characteristics over a wide frequency range, and also to have non-directional properties. Ultrasonic transducer can be provided.

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

第1図(IL) (b)は従来の超音波送受波器の一例
を示す側面図および平面図、第2図(、) (b)は本
発明の一実施例を示す側断面図および底面図、第3図、
第4図は上記実施例および従来の超音波送受波器の周波
数特性および指向性を比較して示す図、第5図(、) 
(b)および第6図(、) (b)は本発明の各別の他
の実施例を示す図である。 11・・・圧電体、12.13・・・電極、14.15
・・・リード線。 出願人代理人  弁理士 鈴 江 武 彦第1図 (b) 第3図 第5図 <8) (b) \ 第6図 (a) (b)
FIG. 1 (IL) (b) is a side view and a plan view showing an example of a conventional ultrasonic transducer, and FIG. 2 (IL) (b) is a side sectional view and bottom view showing an example of the present invention. Figure, Figure 3,
Fig. 4 is a diagram comparing the frequency characteristics and directivity of the above embodiment and the conventional ultrasonic transducer, and Fig. 5 (,)
6(b) and FIG. 6(b) are views showing other embodiments of the present invention. 11... Piezoelectric body, 12.13... Electrode, 14.15
···Lead. Applicant's representative Patent attorney Takehiko Suzue Figure 1 (b) Figure 3 Figure 5 <8) (b) \ Figure 6 (a) (b)

Claims (1)

【特許請求の範囲】 1)半球体に形成した圧電体と、この圧電体の球面部に
形成した第1の電極と、この圧電体の底面部に形成した
第2の電極とを具備する超音波送受波器。 2)圧電体の球面部を多数の平面からなる多角形にした
ことを特徴とする特許請求の範囲第1項記載の超音波送
受波器。 3)圧電体を球形に成形し表面を2分して相互に絶縁し
た第1、第2の電極を設けたことを特徴とする特許請求
の範囲第1項記載の超音波送受波器。
[Claims] 1) A superstructure comprising a piezoelectric body formed into a hemispherical shape, a first electrode formed on the spherical surface of the piezoelectric body, and a second electrode formed on the bottom surface of the piezoelectric body. Sound wave transducer. 2) The ultrasonic transducer according to claim 1, characterized in that the spherical portion of the piezoelectric body has a polygonal shape consisting of many planes. 3) The ultrasonic transducer according to claim 1, characterized in that the piezoelectric body is formed into a spherical shape and the surface thereof is divided into two to provide mutually insulated first and second electrodes.
JP12131082A 1982-07-14 1982-07-14 Transmitter/receiver of ultrasonic wave Pending JPS5913500A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12131082A JPS5913500A (en) 1982-07-14 1982-07-14 Transmitter/receiver of ultrasonic wave

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12131082A JPS5913500A (en) 1982-07-14 1982-07-14 Transmitter/receiver of ultrasonic wave

Publications (1)

Publication Number Publication Date
JPS5913500A true JPS5913500A (en) 1984-01-24

Family

ID=14808074

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12131082A Pending JPS5913500A (en) 1982-07-14 1982-07-14 Transmitter/receiver of ultrasonic wave

Country Status (1)

Country Link
JP (1) JPS5913500A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0242898A (en) * 1988-08-02 1990-02-13 Furuno Electric Co Ltd Ultrasonic oscillator
KR100937361B1 (en) 2007-03-12 2010-01-20 주식회사 제닉슨 3-D Semi-sphere shaped ultrasonic sensor
GB2474103A (en) * 2009-09-15 2011-04-06 Oceanscan Ltd Scanning apparatus and method
CN105606141A (en) * 2016-02-29 2016-05-25 汉得利(常州)电子股份有限公司 Omnibearing spherical ultrasonic sensor
JP2016202053A (en) * 2015-04-21 2016-12-08 多賀電気株式会社 Ultrasonic generator

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5619989B2 (en) * 1972-07-08 1981-05-11

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5619989B2 (en) * 1972-07-08 1981-05-11

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0242898A (en) * 1988-08-02 1990-02-13 Furuno Electric Co Ltd Ultrasonic oscillator
KR100937361B1 (en) 2007-03-12 2010-01-20 주식회사 제닉슨 3-D Semi-sphere shaped ultrasonic sensor
GB2474103A (en) * 2009-09-15 2011-04-06 Oceanscan Ltd Scanning apparatus and method
GB2474103B (en) * 2009-09-15 2012-05-23 Oceanscan Ltd Scanning apparatus and method
JP2016202053A (en) * 2015-04-21 2016-12-08 多賀電気株式会社 Ultrasonic generator
CN105606141A (en) * 2016-02-29 2016-05-25 汉得利(常州)电子股份有限公司 Omnibearing spherical ultrasonic sensor

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