JPS642320B2 - - Google Patents
Info
- Publication number
- JPS642320B2 JPS642320B2 JP18755781A JP18755781A JPS642320B2 JP S642320 B2 JPS642320 B2 JP S642320B2 JP 18755781 A JP18755781 A JP 18755781A JP 18755781 A JP18755781 A JP 18755781A JP S642320 B2 JPS642320 B2 JP S642320B2
- Authority
- JP
- Japan
- Prior art keywords
- piezoelectric element
- diaphragm
- case
- bonded piezoelectric
- thin plate
- 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
Links
- 239000000463 material Substances 0.000 claims description 9
- 230000005540 biological transmission Effects 0.000 description 8
- 230000035945 sensitivity Effects 0.000 description 8
- 230000007423 decrease Effects 0.000 description 5
- 238000010586 diagram Methods 0.000 description 5
- 238000005259 measurement Methods 0.000 description 5
- 239000000919 ceramic Substances 0.000 description 4
- 230000008878 coupling Effects 0.000 description 4
- 238000010168 coupling process Methods 0.000 description 4
- 238000005859 coupling reaction Methods 0.000 description 4
- 239000011358 absorbing material Substances 0.000 description 2
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- 238000005452 bending Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000013013 elastic material Substances 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 230000000149 penetrating effect Effects 0.000 description 1
- 230000001681 protective effect Effects 0.000 description 1
- 239000011347 resin Substances 0.000 description 1
- 229920005989 resin Polymers 0.000 description 1
Classifications
-
- G—PHYSICS
- G10—MUSICAL INSTRUMENTS; ACOUSTICS
- G10K—SOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
- G10K11/00—Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
- G10K11/02—Mechanical acoustic impedances; Impedance matching, e.g. by horns; Acoustic resonators
- G10K11/025—Mechanical acoustic impedances; Impedance matching, e.g. by horns; Acoustic resonators horns for impedance matching
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R17/00—Piezoelectric transducers; Electrostrictive transducers
- H04R17/10—Resonant transducers, i.e. adapted to produce maximum output at a predetermined frequency
Description
【発明の詳細な説明】
本発明は、尖鋭な指向特性を有し、パルス特性
を改善した超音波送受波器に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ultrasonic transducer having sharp directivity characteristics and improved pulse characteristics.
空気中での超音波の送受波器は、圧電セラミク
スの貼り合せ型圧電素子が多く用いられており、
上記貼り合せ型圧電素子の撓み振動の共振点、反
共振点で使用するように作られている。また、媒
体となる空気の機械的インピーダンスは圧電セラ
ミクスのそれと比して著しく小さいため、貼り合
せ型圧電素子を振動板と結合させて機械的インピ
ーダンスの低下を図つている。 Bonded piezoelectric elements made of piezoelectric ceramics are often used as transmitters and receivers for ultrasonic waves in the air.
It is made to be used at the resonance point and anti-resonance point of the bending vibration of the bonded piezoelectric element. Furthermore, since the mechanical impedance of air as a medium is significantly smaller than that of piezoelectric ceramics, the bonded piezoelectric element is coupled to the diaphragm to reduce the mechanical impedance.
従来の超音波送受波器の構造を第1図に示す。
これは、貼り合せ型圧電素子1の中心部に結合軸
2を貫通固定し、この結合軸2に振動板3を取付
けるとともに、貼り合せ型圧電素子1の振動の節
部を支持台4の先端に弾性接着剤5をもつて固定
したものであつた。6,6′は端子、7は貼り合
せ型圧電素子等を覆うケース、8はケース7の上
部に形成された透孔に取り付けられた保護用メツ
シユ、9,9′は貼り合せ型圧電素子1と端子6,
6′を電気的に接続しているリード線である。 The structure of a conventional ultrasonic transducer is shown in FIG.
This involves penetrating and fixing a coupling shaft 2 to the center of the bonded piezoelectric element 1, attaching a diaphragm 3 to the coupling shaft 2, and directing the vibration nodes of the bonded piezoelectric element 1 to the tip of the support base 4. It was fixed with an elastic adhesive 5. 6 and 6' are terminals, 7 is a case that covers the bonded piezoelectric element, etc., 8 is a protective mesh attached to a through hole formed in the upper part of the case 7, and 9 and 9' are the bonded piezoelectric element 1. and terminal 6,
This is a lead wire that electrically connects 6'.
第2図は、上記構造の超音波送受波器のパルス
特性を示したもので、複数個のパルスで駆動した
ときの送信波形である。圧電セラミクスの機械的
Qが高いことにより、立上り・立下り時間が遅く
2ミリ秒以上にも及ぶものであつた。 FIG. 2 shows the pulse characteristics of the ultrasonic transducer having the above structure, and shows the transmission waveform when driven with a plurality of pulses. Due to the high mechanical Q of piezoelectric ceramics, the rise and fall times were slow, reaching more than 2 milliseconds.
たとえば移動物体の距離測定のとき、このよう
な従来の超音波送受波器を用いると、短い時間間
隔で測定情報を得る必要がある場合、立上り・立
下り時間がきわめて長いために、受信信号がピー
ク値になるまでの時間がかかる。あるいは受信信
号が立下る前に次の信号が受信され混信して、正
確な測定情報が得られなかつた。 For example, when measuring the distance of a moving object, when using such a conventional ultrasonic transducer, it is necessary to obtain measurement information at short time intervals, and the rise and fall times are extremely long, so the received signal is It takes time to reach the peak value. Alternatively, the next signal may be received before the received signal falls, causing interference and making it impossible to obtain accurate measurement information.
また、送受波を単体の素子で行なわせる場合、
送波させてただちに受信可能な状態になるまで、
かなりの時間を要し、その間、測定情報を得るこ
とはできなかつた。 In addition, when transmitting and receiving waves using a single element,
Until it becomes ready to receive after transmitting a wave,
It took a considerable amount of time, during which time no measurement information could be obtained.
さらに測定対象となる物体に対して分解能を上
げようとすると、尖鋭な指向特性が要求される。
尖鋭な指向特性は、公知のように音源の大きさを
増大させ、使用周波数を高くすることにより実現
されるが、使用周波数を高くすると音の減衰は著
しく増大するので、高くすることに限界があり、
音源を大きくする必要がある。 Furthermore, in order to increase the resolution of the object to be measured, sharp directional characteristics are required.
As is well known, sharp directional characteristics can be achieved by increasing the size of the sound source and raising the frequency used, but as the frequency used increases, the attenuation of sound increases significantly, so there is a limit to increasing the frequency. can be,
It is necessary to make the sound source louder.
圧電セラミクスを用いた超音波送受波器に尖鋭
な指向特性を要求すると、振動板、貼り合せ型圧
電素子および貼り合せ型圧電素子を支持する支持
台が著しく大きくなるという欠点があつた。たと
え大きな振動板を用いても、均一なピストン振動
を実現させることはきわめて困難であり、音源を
大きくする割には概して指向特性は尖鋭にならな
かつた。 When an ultrasonic transducer using piezoelectric ceramics is required to have sharp directivity characteristics, there is a drawback that the diaphragm, the bonded piezoelectric element, and the support base that supports the bonded piezoelectric element become significantly large. Even if a large diaphragm was used, it was extremely difficult to achieve uniform piston vibration, and the directional characteristics were generally not as sharp as the sound source was made larger.
一方、ホーンを用いて指向特性を尖鋭にしよう
とする場合、従来の超音波送受器にホーンを付加
して、機械的Qを低下させてパルス特性を改善す
ることは容易に実現できることではなかつた。 On the other hand, when trying to sharpen the directional characteristics by using a horn, it was not easy to add a horn to a conventional ultrasonic transceiver to lower the mechanical Q and improve the pulse characteristics. .
そこで、本発明は、貼り合せ型圧電素子の中心
部に振動板を設け、かつ機械的振動を抑制するよ
うに前記振動板の周囲を弾性ゴム等の弾性材でケ
ースに弾性的に固定するとともに、この前方に開
口部を設けた薄板およびホーンを付加して、尖鋭
な指向特性と良好なパルス特性を有する超音波送
受波器を提供するものである。 Therefore, the present invention provides a diaphragm at the center of a bonded piezoelectric element, and elastically fixes the periphery of the diaphragm to a case with an elastic material such as elastic rubber so as to suppress mechanical vibration. By adding a thin plate with an opening in the front and a horn, an ultrasonic transducer having sharp directional characteristics and good pulse characteristics is provided.
以下、本発明の一実施例を図面にもとづいて説
明する。第3図はこの実施例の断面図である。 Hereinafter, one embodiment of the present invention will be described based on the drawings. FIG. 3 is a sectional view of this embodiment.
貼り合せ型圧電素子11の中心部に配した結合
軸12に金属あるいは樹脂より形成された振動板
13を取り付ける。前記振動板13の周辺部は、
機械的振動を抑制するように円環状に形成された
弾性ゴム等の緩衝材20を介して、円筒状のケー
ス17の内側面に弾性的に固定されている。ケー
ス17の底部には吸音材21が取り付けてある。
振動板13の前方には、結合軸12を通過する直
線を中心にした円状の開口部22と、開口部22
と同心円周上に設けた他の開口部22′を有する
薄板23を設置し、ケース17と薄板23を放物
面ホーン24の喉部に嵌入する。19,19′は
貼り合せ型圧電素子11と端子16,16′を電
気的に接続しているリード線である。 A diaphragm 13 made of metal or resin is attached to a coupling shaft 12 arranged at the center of the bonded piezoelectric element 11. The periphery of the diaphragm 13 is
It is elastically fixed to the inner surface of the cylindrical case 17 via a buffer material 20 such as elastic rubber formed in an annular shape so as to suppress mechanical vibrations. A sound absorbing material 21 is attached to the bottom of the case 17.
In front of the diaphragm 13, there is a circular opening 22 centered on a straight line passing through the coupling shaft 12;
A thin plate 23 having another opening 22' provided on a concentric circumference is installed, and the case 17 and the thin plate 23 are fitted into the throat of the parabolic horn 24. Lead wires 19 and 19' electrically connect the bonded piezoelectric element 11 and the terminals 16 and 16'.
上記薄板23の開口部22,22′は、貼り合
せ型圧電素子11の大きさや振動板13の大き
さ、緩衝材20の内径等により、形状が変化する
が、その代表的な形状を第4図ないし第16図に
示す。いずれの図においても、aは平面図、bは
断面図である。 The shape of the openings 22, 22' of the thin plate 23 changes depending on the size of the bonded piezoelectric element 11, the size of the diaphragm 13, the inner diameter of the cushioning material 20, etc. This is shown in Figures 1 to 16. In both figures, a is a plan view and b is a sectional view.
次に上記本発明の構造による超音波送受波器の
パルス特性を第17図に示す。これから明らかな
パルスの立上り・立下り時間は、0.3ミリ秒以下
を示すようになつた。 Next, FIG. 17 shows the pulse characteristics of the ultrasonic transducer having the structure of the present invention. This clearly shows that the pulse rise and fall times are less than 0.3 milliseconds.
第18図は上記緩衝材20の内径を変化させた
とき、音圧半減角、送波感度および立上り時間の
変化をそれぞれ示している。緩衝材20の内径の
減少に伴ない立上り時間が減少するが、音圧半減
角は少し増大し、送波感度も減少する。さらに内
径を小さくすると、サイドローブも増大してくる
(図示せず)。したがつて緩衝材20の内径は、貼
り合せ型圧電素子11および振動板13の大きさ
や厚さが決まれば、最適値が存在することがわか
る。なお、貼り合せ型圧電素子11の直径は9.1
mm、厚さは約0.6mm、振動板13は底面の直径が
17mm程度のコニカル形、ホーン24の直径は約55
mm、薄板23は第7図のもののときの実験値であ
る。 FIG. 18 shows changes in the half-reduction angle of sound pressure, wave transmission sensitivity, and rise time when the inner diameter of the buffer material 20 is changed. As the inner diameter of the buffer material 20 decreases, the rise time decreases, but the sound pressure half-decrease angle increases slightly and the wave transmission sensitivity also decreases. If the inner diameter is further reduced, the side lobes also increase (not shown). Therefore, it can be seen that the inner diameter of the cushioning material 20 has an optimum value once the sizes and thicknesses of the bonded piezoelectric element 11 and the diaphragm 13 are determined. Note that the diameter of the bonded piezoelectric element 11 is 9.1
mm, the thickness is approximately 0.6 mm, and the diameter of the bottom of the diaphragm 13 is
Conical shape of about 17mm, diameter of horn 24 is about 55mm
mm and thin plate 23 are experimental values for the one shown in FIG.
第19図は、貼り合せ型圧電素子11の直径が
約9.1mmで、厚さを変化させたとき、音圧半減角、
送波感度、立上り時間および駆動周波数(感度最
大になる周波数)の変化をそれぞれ示している。
貼り合せ型圧電素子11の厚さを増大するに伴な
い、駆動周波数が高くなり、音圧半減角が小さく
なるが、送波感度は減少し立上り時間も長くな
る。 FIG. 19 shows that the diameter of the bonded piezoelectric element 11 is approximately 9.1 mm, and when the thickness is changed, the half-reduction angle of the sound pressure,
Changes in transmission sensitivity, rise time, and drive frequency (frequency at which sensitivity is maximized) are shown, respectively.
As the thickness of the bonded piezoelectric element 11 increases, the drive frequency increases and the half-reduction angle of sound pressure decreases, but the wave transmission sensitivity decreases and the rise time also increases.
振動板23の直径を大きくするにつれて送波感
度は増大するが、立上り時間も長くなるので、用
途に応じてその直径を定めればよい。空間的(た
とえば上下左右で)均一な指向性が必要なとき
は、振動板13はコニカル形、ラツパ形、おわん
形等がよい。 As the diameter of the diaphragm 23 increases, the wave transmission sensitivity increases, but the rise time also increases, so the diameter may be determined depending on the application. When spatially uniform directivity (for example, vertically, horizontally, and horizontally) is required, the diaphragm 13 is preferably of a conical shape, a lattice shape, a bowl shape, or the like.
第20図aは、振動板13の前方に薄板23を
設置したときの本発明装置の指向特性を示してい
る。同図bはその設置前の指向特性を示してい
る。これから本発明によればサイドローブが大き
く減少しているのがわかる。空間的にほぼ均一な
指向特性が得られるようになつた。 FIG. 20a shows the directivity characteristics of the device of the present invention when the thin plate 23 is installed in front of the diaphragm 13. Figure b shows the directivity characteristics before installation. It can be seen that according to the present invention, the sidelobes are greatly reduced. It has become possible to obtain spatially almost uniform directional characteristics.
また、ケース17と薄板23を一体化すること
により、一層空間的に均一な指向特性が得られる
ようになつたばかりでなく、特性のばらつきが減
少し、組立てが易になり、量産しやすくなつた。 In addition, by integrating the case 17 and the thin plate 23, it is not only possible to obtain more spatially uniform directivity characteristics, but also the variation in characteristics is reduced, making assembly easier and mass production easier. .
さらに一体形成したケース17と薄板23とを
導電性のものにしてアースに接続すると耐ノイズ
性が向上した。 Furthermore, noise resistance was improved by making the integrally formed case 17 and thin plate 23 conductive and connecting them to ground.
以上のように本発明によれば、尖鋭な指向特性
と良好なパルス特性を有し、短い時間間隔で正確
な測定情報を得ることが可能となつた。したがつ
て本発明の超音波送受波器は、音波を用いた距離
計等、尖鋭な指向特性が要求される超音波応用計
測にはきわめて有用なものである。 As described above, according to the present invention, it has sharp directivity characteristics and good pulse characteristics, and it has become possible to obtain accurate measurement information at short time intervals. Therefore, the ultrasonic transducer of the present invention is extremely useful for ultrasonic applied measurements that require sharp directivity characteristics, such as distance meters using sound waves.
第1図は従来の超音波送受波器の一例を示す断
面図、第2図はそのパルス特性を示す図である。
第3図は本発明の超音波送受波器の一実施例の断
面図、第4図から第16図まではその薄板の代表
例の構造を示し、それらの図aは正面図、同bは
断面図、第17図は本発明の超音波送受波器のパ
ルス特性の一例を示す図、第18図は本発明の超
音波送受波器の緩衝材の内径と音圧半減角、送波
感度、立上り時間との関係を示す図、第19図は
同じく貼り合せ型圧電素子の厚さと音圧半減角、
送波感度、立上り時間、駆動周波数との関係を示
す図、第20図は同じく薄板の効果を示す図であ
る。
11……貼り合せ型圧電素子、13……振動
板、17……ケース、20……緩衝材、21……
吸音材、22,22′……開口部、23……薄板、
24……ホーン。
FIG. 1 is a sectional view showing an example of a conventional ultrasonic transducer, and FIG. 2 is a diagram showing its pulse characteristics.
FIG. 3 is a cross-sectional view of one embodiment of the ultrasonic transducer of the present invention, and FIGS. 4 to 16 show the structure of a typical example of the thin plate thereof, in which figure a is a front view and figure b is a front view. A cross-sectional view, FIG. 17 is a diagram showing an example of the pulse characteristics of the ultrasonic transducer of the present invention, and FIG. 18 is a diagram showing the inner diameter of the buffer material, half-sound pressure angle, and wave transmission sensitivity of the ultrasonic transducer of the present invention. , Figure 19 shows the relationship between the rise time and the thickness of the bonded piezoelectric element and the sound pressure half angle,
FIG. 20, which is a diagram showing the relationship between wave transmission sensitivity, rise time, and drive frequency, is also a diagram showing the effect of a thin plate. 11... Bonded piezoelectric element, 13... Vibration plate, 17... Case, 20... Cushioning material, 21...
Sound absorbing material, 22, 22'... opening, 23... thin plate,
24...Horn.
Claims (1)
子、前記貼り合せ型圧電素子を封入するケース、
前記振動板の周辺部と前記ケースの内側面とに接
触するように取り付けた緩衝材、前記貼り合せ型
圧電素子の前方に設置した開口部を設けた薄板、
および、前記ケースと前記薄板を喉部に封入し固
定するホーンを少なくとも有し、前記緩衝材によ
り前記振動板を前記ケースに弾性的に固定してな
ることを特徴とする超音波送受波器。 2 薄板、ケースおよびホーンを一体形成したこ
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。[Claims] 1. A bonded piezoelectric element having a diaphragm in the center, a case enclosing the bonded piezoelectric element,
a cushioning material attached so as to be in contact with the periphery of the diaphragm and the inner surface of the case; a thin plate with an opening disposed in front of the bonded piezoelectric element;
and an ultrasonic transducer characterized in that it has at least a horn that seals and fixes the case and the thin plate in the throat, and the diaphragm is elastically fixed to the case by the cushioning material. 2. The ultrasonic transducer according to claim 1, characterized in that the thin plate, the case, and the horn are integrally formed.
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18755781A JPS5888999A (en) | 1981-11-20 | 1981-11-20 | Ultrasonic wave transmitter and receiver |
US06/439,549 US4607186A (en) | 1981-11-17 | 1982-11-05 | Ultrasonic transducer with a piezoelectric element |
EP82110290A EP0080100B1 (en) | 1981-11-17 | 1982-11-08 | Ultrasonic transducer |
DE8282110290T DE3272470D1 (en) | 1981-11-17 | 1982-11-08 | Ultrasonic transducer |
CA000415697A CA1202112A (en) | 1981-11-17 | 1982-11-16 | Ultrasonic transducer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18755781A JPS5888999A (en) | 1981-11-20 | 1981-11-20 | Ultrasonic wave transmitter and receiver |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5888999A JPS5888999A (en) | 1983-05-27 |
JPS642320B2 true JPS642320B2 (en) | 1989-01-17 |
Family
ID=16208156
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP18755781A Granted JPS5888999A (en) | 1981-11-17 | 1981-11-20 | Ultrasonic wave transmitter and receiver |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5888999A (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60212097A (en) * | 1984-04-04 | 1985-10-24 | West Electric Co Ltd | Ultrasonic wave transmitter-receiver |
JPH069308U (en) * | 1992-07-08 | 1994-02-04 | 日東工業株式会社 | Air conditioner for electronic equipment cabinet |
-
1981
- 1981-11-20 JP JP18755781A patent/JPS5888999A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS5888999A (en) | 1983-05-27 |
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