Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6312438B2 - - Google Patents
[go: Go Back, main page]

JPS6312438B2 - - Google Patents

Info

Publication number
JPS6312438B2
JPS6312438B2 JP56136077A JP13607781A JPS6312438B2 JP S6312438 B2 JPS6312438 B2 JP S6312438B2 JP 56136077 A JP56136077 A JP 56136077A JP 13607781 A JP13607781 A JP 13607781A JP S6312438 B2 JPS6312438 B2 JP S6312438B2
Authority
JP
Japan
Prior art keywords
housing
piezoelectric material
transducer
piezoelectric materials
acoustic impedance
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
JP56136077A
Other languages
Japanese (ja)
Other versions
JPS5839200A (en
Inventor
Yoshitada Tominaga
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.)
NEC Corp
Original Assignee
Nippon Electric 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP13607781A priority Critical patent/JPS5839200A/en
Publication of JPS5839200A publication Critical patent/JPS5839200A/en
Publication of JPS6312438B2 publication Critical patent/JPS6312438B2/ja
Granted 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
    • B06B1/0633Cylindrical array

Landscapes

  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Transducers For Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】 本発明は超音波の送・受波を行なう送受波器に
関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a transducer for transmitting and receiving ultrasonic waves.

従来、この種の送受波器において、指向性の特
性を得るためには複数個の送受波器を空間的に配
列し、これ等によつて生ずる音波の伝播の経路差
を利用していた。しかし、この方法では、周波数
が低くなり、媒質中の音波の波長が長くなつてく
ると、それに比例して送受波器間の距離を大きく
とる必要があり、構造が大型になるという欠点が
あつた。
Conventionally, in this type of transducer, in order to obtain directional characteristics, a plurality of transducers were spatially arranged and the difference in the propagation path of sound waves caused by these was utilized. However, this method has the disadvantage that as the frequency becomes lower and the wavelength of the sound wave in the medium becomes longer, the distance between the transducer and the transducer must be increased proportionally, resulting in a larger structure. Ta.

また上記の欠点を除くために、圧力傾度型送受
波器を4直角方向に配置し、これらの送受波器の
組合せにより指向性を得る方法が採用されてい
る。しかし、この方法による送受波器の構造はバ
イモルフ形のために複雑になるばかりでなく、筐
体より突出して保持されるために機械的強度が不
十分であるなどの欠点があつた。或はまた、円筒
形振動体の内面に4直角方向に圧電材を配置し、
振動体の変形により伝達される応力によつて誘起
される出力を組合せて指向性を得るものがある
が、この方法においても構造が複雑であり、機械
的強度が不十分であるなどの欠点があつた。
In order to eliminate the above-mentioned drawbacks, a method has been adopted in which pressure gradient type transducers are arranged in four orthogonal directions and directivity is obtained by a combination of these transducers. However, the structure of the transducer obtained by this method is not only complicated due to its bimorph shape, but also has drawbacks such as insufficient mechanical strength because it is held protruding from the housing. Alternatively, piezoelectric materials are arranged in four orthogonal directions on the inner surface of the cylindrical vibrating body,
Some methods obtain directivity by combining the outputs induced by the stress transmitted by the deformation of the vibrating body, but this method also has drawbacks such as a complex structure and insufficient mechanical strength. It was hot.

本発明の目的は、従来の欠点を除去し、板状の
圧電材に媒質の音響インピーダンスにほぼ近いも
のを使用することによつて、送波器と受波器が一
体化され、構造が小型化されるばかりでなく、機
械的強度の向上と、更に単一指向性を得ることの
できる送受波器を提供するにある。
The purpose of the present invention is to eliminate the drawbacks of the conventional method, and by using a plate-shaped piezoelectric material with an acoustic impedance that is close to the acoustic impedance of the medium, the transmitter and receiver are integrated, and the structure is compact. It is an object of the present invention to provide a transducer which not only has improved mechanical strength but also has unidirectionality.

本発明の送受波器は、円筒形、若しくは球形の
筐体と、該筐体の円周上の少なくとも1対向表面
に対として固着された板状の圧電材とによつて構
成され、対向する2つの圧電材を組とし、それぞ
れの入出力を差合成することにより指向性を得る
ようにしたものである。
The transducer of the present invention is constituted by a cylindrical or spherical housing and plate-shaped piezoelectric materials fixed as a pair to at least one opposing surface on the circumference of the housing. Two piezoelectric materials are used as a set, and directivity is obtained by differentially synthesizing the input and output of each.

次に、本発明による実施例について図面を参照
して説明する。
Next, embodiments according to the present invention will be described with reference to the drawings.

第1図は本発明の第1の実施例の構造を斜視図
により示したものである。この図において、1は
円筒形の金属筐体、2−1,2−2,2−3,2
−4は筐体1に接着された媒質の音響インピーダ
ンスに近い板状の圧電材である。第2図は、第1
図の送受波器を上方からみた平面図である。この
平面図において、圧電材2−1〜4の(+),
(−)の表示はそれぞれの圧電材の極性を表わし
ている。極性の反転されたものは、同一のものを
面を逆に接着することによつて得られる。
FIG. 1 is a perspective view showing the structure of a first embodiment of the present invention. In this figure, 1 is a cylindrical metal case, 2-1, 2-2, 2-3, 2
-4 is a plate-shaped piezoelectric material whose acoustic impedance is close to that of the medium bonded to the housing 1. Figure 2 shows the first
FIG. 3 is a plan view of the transducer shown in the figure, viewed from above. In this plan view, (+) of piezoelectric materials 2-1 to 2-4,
The symbol (-) represents the polarity of each piezoelectric material. Those with reversed polarity can be obtained by gluing identical ones with their sides reversed.

このように構成された送受波器の動作につい
て、第3図の原理図を参照して説明する。なお、
この図には、圧電材が対になる一組についてのみ
記されている。そして、送波と受波は丁度現象の
プロセスが逆で動作原理は同じであるから、ここ
には受波についてのみ記述する。いま、図の矢印
に示す方向より音波が到来すると、筐体1は進行
方向の前後に振動する。このため、2つの圧電材
には圧縮、又は膨張の力が作用し、お互に位相の
逆の電圧がそれぞれ誘起する。この両電圧を差合
成すると、この電圧が2倍になつて取りだせる。
この電圧は、音波の到来角度がθの方向にあると
き、cos θに減少する。その結果、いわゆる8の
字形の指向性が得られる。このことから判るよう
に、2つの圧電材を結ぶ直線に直角の方向から音
波が到来した場合には、それぞれの圧電材は同相
の電圧が誘起するから、これ等両方の電圧を差合
成すると、その電圧は0となる。
The operation of the transducer configured in this way will be explained with reference to the principle diagram of FIG. 3. In addition,
In this figure, only one pair of piezoelectric materials is shown. Since the process of transmitting and receiving waves is exactly the opposite and the principle of operation is the same, only wave reception will be described here. Now, when a sound wave arrives from the direction shown by the arrow in the figure, the housing 1 vibrates back and forth in the direction of travel. Therefore, a compression or expansion force acts on the two piezoelectric materials, and voltages having opposite phases are induced in each of the piezoelectric materials. By combining the differences between these two voltages, this voltage can be doubled.
This voltage decreases to cos θ when the angle of arrival of the sound wave is in the direction of θ. As a result, a so-called figure-eight directivity is obtained. As can be seen from this, when a sound wave arrives from a direction perpendicular to a straight line connecting two piezoelectric materials, voltages of the same phase are induced in each piezoelectric material, so when combining both voltages, The voltage becomes 0.

第4図は本発明による第2の実施例の構造を斜
視図により示したものである。この図において、
3はジルコン酸チタン酸鉛系の圧電材で形成され
た筐体であり、媒質の音響インピーダンスより大
きく選定されている。4−1,4−2,4−3,
4−4は高分子圧電材である。これ等圧電材4−
1〜4の極性は第1の実施例と同じに選定され
る。従つて、この受波器も第1の実施例と同じよ
うに動作するので、その点についての詳細な説明
は省略する。ただ、圧電材よりなる筐体3を受波
器として動作させたとき、これに誘起される電圧
と圧電材4−1〜4に誘起される電圧とを和、又
は差合成することによつて、受波の指向性を単一
指向性にすることができる。また、圧電材4−1
〜4は媒質の音響インピーダンスに近いため、到
来した音波の伝播は阻害されず、音波は筐体3に
到達する。また、筐体3のみを送波器として動作
させた場合、送波器は0次の振動モード、いわゆ
る呼吸振動により振動して音波を発生する。この
状態においては、外面の圧電材4−1〜4は媒質
の音響インピーダンスにほぼ近いため、振動の阻
害および音波の伝播の阻害にはならない。
FIG. 4 is a perspective view showing the structure of a second embodiment of the present invention. In this diagram,
3 is a housing made of a piezoelectric material based on lead zirconate titanate, and is selected to have a larger acoustic impedance than the medium. 4-1, 4-2, 4-3,
4-4 is a polymer piezoelectric material. This iso-piezoelectric material 4-
The polarities of 1 to 4 are selected in the same way as in the first embodiment. Therefore, since this receiver also operates in the same manner as in the first embodiment, a detailed explanation thereof will be omitted. However, when the housing 3 made of piezoelectric material is operated as a wave receiver, the voltage induced therein and the voltage induced in the piezoelectric materials 4-1 to 4-4 are summed or differentially combined. , the directivity of received waves can be made unidirectional. In addition, piezoelectric material 4-1
Since ~4 is close to the acoustic impedance of the medium, the propagation of the arriving sound waves is not inhibited and the sound waves reach the housing 3. Further, when only the housing 3 is operated as a wave transmitter, the wave transmitter vibrates in a zero-order vibration mode, so-called respiratory vibration, and generates a sound wave. In this state, the piezoelectric materials 4-1 to 4 on the outer surface have approximately the acoustic impedance of the medium, so they do not impede vibration or propagation of sound waves.

上記第1および第2の実施例においては、筐体
1や圧電材よりなる筐体3は4直角方向について
のみ、板状の圧電材を接着しているが、これは一
平面の全方位の弁別に必要な最少の数として例示
されたものである。本発明においては、これに限
定されることなく、単に指向性を得るため、或は
指向性のビーム数を多数個得るために、それぞれ
4直角方向以下、或はそれ以上の方向に圧電材を
固着してもよいことは言うまでもない。例えば、
球面の筐体を使用し、直交する2平面の計6直角
方向に圧電材を固着すれば、より全方向的な弁別
が可能になる。
In the first and second embodiments described above, the housing 1 and the housing 3 made of piezoelectric material are bonded with plate-shaped piezoelectric materials only in four orthogonal directions; This is an example of the minimum number necessary for discrimination. In the present invention, the piezoelectric material is not limited to this, but in order to simply obtain directivity or to obtain a large number of directional beams, the piezoelectric material is arranged in four or less or more perpendicular directions. Needless to say, it may be fixed. for example,
If a spherical casing is used and piezoelectric materials are fixed in six orthogonal directions, two orthogonal planes, more omnidirectional discrimination becomes possible.

なお、上記の実施例に使用されている圧電材
は、近年、開発がとみに進展し、感度等に関係す
る圧電定数の改善、音響インピーダンスの低減、
或は可撓性の増大等によつて、その性能が向上
し、本発明の送受波器に対する有効な活用が期待
されるようになつた。
The piezoelectric materials used in the above examples have been rapidly developed in recent years, and improvements in piezoelectric constants related to sensitivity, reduction in acoustic impedance, etc.
Alternatively, the performance has been improved due to increased flexibility, etc., and it has come to be expected that the present invention can be effectively utilized in the transducer.

以上の説明により明らかなように、本発明によ
れば板状の圧電材を複数個筐体に固着することに
より、機械的強度が得られ、かつ製造が容易にな
るばかりでなく、更に、筐体部を音響インピーダ
ンスが大きい圧電材とし板状の固着する圧電材を
媒質の音響インピーダンスとほぼ近いものにする
ことによつて、複数の受波器、又はこれらと送波
器が一体化され、構造の小型化が容易になり、或
は単一指向性を容易に得ることができるなど得ら
れる効果は大きい。
As is clear from the above description, according to the present invention, by fixing a plurality of plate-shaped piezoelectric materials to the casing, not only mechanical strength is obtained and manufacturing is easy, but also the casing By making the body part a piezoelectric material with a large acoustic impedance and making the plate-shaped fixed piezoelectric material almost close to the acoustic impedance of the medium, multiple receivers or these and a transmitter can be integrated. The advantages that can be obtained are significant, such as the ability to easily downsize the structure and easily obtain unidirectivity.

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

第1図は本発明による第1の実施例の構造を示
す斜視図、第2図は、第1図の送受波器を上方か
ら見た平面図、第3図は、第1図の送受波器の動
作を説明するための原理図、第4図は本発明によ
る第2の実施例の構造を示す斜視図である。 図において、1は筐体、2−1,2−2,2−
3,2−4,4−1,4−2,4−3,4−4は
板状の圧電材、3は圧電材よりなる筐体である。
FIG. 1 is a perspective view showing the structure of the first embodiment of the present invention, FIG. 2 is a plan view of the transducer shown in FIG. 1 viewed from above, and FIG. 3 is the transducer shown in FIG. FIG. 4 is a perspective view showing the structure of a second embodiment of the present invention. In the figure, 1 is the housing, 2-1, 2-2, 2-
3, 2-4, 4-1, 4-2, 4-3, and 4-4 are plate-shaped piezoelectric materials, and 3 is a housing made of the piezoelectric material.

Claims (1)

【特許請求の範囲】 1 円筒形、若しくは球形の筐体と、該筐体の円
周上の少なくとも1対向表面に対として固着され
た板状の圧電材とによつて構成され、前記対向す
る2つの圧電材の入出力を差合成することを特徴
とする送受波器。 2 特許請求の範囲第1項に記載の送受波器にお
いて、前記筐体が媒質の音響インピーダンスより
大きいインピーダンスを有する圧電材で形成さ
れ、前記板状の圧電材が媒質の音響インピーダン
スにほぼ近いインピーダンスを有することを特徴
とする送受波器。
[Scope of Claims] 1. Consisting of a cylindrical or spherical housing and plate-shaped piezoelectric materials fixed as a pair to at least one opposing surface on the circumference of the housing, A transducer characterized by differentially combining the input and output of two piezoelectric materials. 2. In the transducer according to claim 1, the casing is formed of a piezoelectric material having an impedance larger than the acoustic impedance of the medium, and the plate-shaped piezoelectric material has an impedance substantially close to the acoustic impedance of the medium. A transducer characterized by having.
JP13607781A 1981-09-01 1981-09-01 Transmitter-receiver Granted JPS5839200A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13607781A JPS5839200A (en) 1981-09-01 1981-09-01 Transmitter-receiver

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13607781A JPS5839200A (en) 1981-09-01 1981-09-01 Transmitter-receiver

Publications (2)

Publication Number Publication Date
JPS5839200A JPS5839200A (en) 1983-03-07
JPS6312438B2 true JPS6312438B2 (en) 1988-03-18

Family

ID=15166691

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13607781A Granted JPS5839200A (en) 1981-09-01 1981-09-01 Transmitter-receiver

Country Status (1)

Country Link
JP (1) JPS5839200A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5355417A (en) * 1992-10-21 1994-10-11 The Center For Innovative Technology Active control of aircraft engine inlet noise using compact sound sources and distributed error sensors
JPH07284197A (en) * 1994-04-08 1995-10-27 Nec Corp Dipole radiating type low-frequency underwater sound wave transmitter

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS492524A (en) * 1972-04-20 1974-01-10
JPS55140399A (en) * 1979-04-20 1980-11-01 Hitachi Ltd Cylindrical piezoelectric porcelain vibrator

Also Published As

Publication number Publication date
JPS5839200A (en) 1983-03-07

Similar Documents

Publication Publication Date Title
US3370187A (en) Electromechanical apparatus
JPS61253998A (en) Electromechanical converter
US4044273A (en) Ultrasonic transducer
JP5125652B2 (en) Low frequency vibrator, omnidirectional low frequency underwater acoustic wave transducer and cylindrical radiation type low frequency underwater acoustic transducer using the same
JPH0431480B2 (en)
US4996713A (en) Electroacoustic piezoelectric transducer having a broad operating range
JPH06222783A (en) Acoustic lens
JPS6312438B2 (en)
JP2972741B1 (en) Composite oscillator
JP2671855B2 (en) Underwater acoustic transmitter
US4131874A (en) Inertial balanced dipole hydrophone
US3253674A (en) Ceramic microphone
JPH02309799A (en) Transmitter-receiver
US3704385A (en) Piezoelectric transducer assembly with phase shifting accoustical parts
JPH0453585Y2 (en)
JPH09271098A (en) Electro-acoustic transducer
JPS5824785Y2 (en) Array-shaped ultrasonic probe
JPS62470B2 (en)
JP2581665B2 (en) Ultrasonic probe
JPH0452677B2 (en)
JPS6126397A (en) Ultrasonic transmitter-receiver
JP2005523594A (en) Surface acoustic wave antenna for submarine
JPH11146492A (en) Ultrasonic probe
JPS62136198A (en) Ultrasonic array probe
JPS6313640B2 (en)