JPS62224199A - Piezoelectric element for sound wave transmission and reception - Google Patents

Piezoelectric element for sound wave transmission and reception

Info

Publication number
JPS62224199A
JPS62224199A JP6685386A JP6685386A JPS62224199A JP S62224199 A JPS62224199 A JP S62224199A JP 6685386 A JP6685386 A JP 6685386A JP 6685386 A JP6685386 A JP 6685386A JP S62224199 A JPS62224199 A JP S62224199A
Authority
JP
Japan
Prior art keywords
shape
piezoelectric
electrode
plate
rubber 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.)
Pending
Application number
JP6685386A
Other languages
Japanese (ja)
Inventor
Akio Hasegawa
長谷川 秋雄
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.)
Niterra Co Ltd
Original Assignee
NGK Spark Plug 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 NGK Spark Plug Co Ltd filed Critical NGK Spark Plug Co Ltd
Priority to JP6685386A priority Critical patent/JPS62224199A/en
Publication of JPS62224199A publication Critical patent/JPS62224199A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To realize mass production of a piezoelectric element provided with an electrode shape of short shading whose side lobe is suppressed, by forming at least one electrode of a piezoelectric plate to a specific shape. CONSTITUTION:A piezoelectric rubber plate 1 is formed to a waveform being symmetrical in the upper and lower directions, which has a prescribed length size (a) on an X axis, and a width size (b) on a Y axis, being shorter than the size (a), has the maximum width size b-1 in the center part of the length, and also, in which the width size decreases gradually toward both ends in the length direction and both end parts become the minimum width size b-2. The shape of the piezoelectric rubber plate 1 is shaped to the same shape as a window shape which is derived by a Kayser's window function shown in the expression, electrode layers 2, 3 of the same shape as a plane shape of the piezoelectric rubber plate 1 are formed on both its faces, and a polarized area 4 of the electrode layers 2, 3 is made to conform with the plane of the piezoelectric rubber plate 1.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、送受波用圧電素子に係り、ハイドロホーンや
超音波探傷器等の音波送受を利用分野とするものである
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a piezoelectric element for transmitting and receiving waves, and its field of application is the transmission and reception of sound waves such as hydrophones and ultrasonic flaw detectors.

(従来の技術) ハイドロホーンの設計ではビーム中の他にサイドローブ
(side 1obe)も考慮すべき重要なパラメータ
とされている。
(Prior Art) In the design of a hydrohorn, in addition to the beam, side lobes are also important parameters to consider.

第5.6図のように一辺の良さがX釉及びY軸と夫々平
イ〒な2a、21」のh杉板の音波特性は、眉波数・面
積・速度に比例し、X軸上の放射/j向の距離に反比例
し、指向性指数は角度θの増加にしたがって減少した後
にまた増加して極大が現れる。
As shown in Figure 5.6, the sound wave characteristics of 2a and 21" h cedar boards whose sides are flat with the X glaze and the Y axis, respectively, are proportional to the number of eyebrow waves, area, and velocity, and are on the X axis. The directivity index is inversely proportional to the distance in the radial/j direction, and decreases as the angle θ increases, then increases again and reaches a maximum.

これをサイドローブと呼び方形板では20%以上に達し
、これがハイドロホーン等の場合虚探知の原因になって
好ましくない。このサイドローブ抑圧手段としては受渡
のレスポンスを変化する方法(振幅シェージング)と受
渡面積を変える方法(形状シェージング)とがある。
This is called a side lobe and reaches 20% or more in the case of a square plate, which is undesirable in the case of a hydrohorn etc. as it causes false detection. As this sidelobe suppression means, there are a method of changing the transfer response (amplitude shading) and a method of changing the transfer area (shape shading).

後者の形状シェージングはハイドロホーンのサイドロー
ブ抑圧に関するパラメータであり、窓関数でもある。か
かる窓関数w(×〉に付いてはこれまで多くのものが報
告されているが、ケーザーは次(ただし グ 〉0) である。
The latter shape shading is a parameter related to sidelobe suppression of the hydrohorn, and is also a window function. Many such window functions w(×〉) have been reported so far, but Kaeser's is the following (where g〉0).

この窓関数は、主極のビーム幅の広がりが少なく、最適
な窓と言われている。
This window function is said to be the optimal window because the beam width at the main pole is less widened.

(本発明が解決しようとする問題点) 本発明は、前項に述べた、一面を音波送受面して利用す
る圧電板の電極形状に関する従来技術を反映し、実用化
に必須な大量生産を可能にすることを角イ決すべき問題
点とするものである。
(Problems to be Solved by the Present Invention) The present invention reflects the prior art regarding the electrode shape of a piezoelectric plate whose one surface is used as a sound wave transmitting/receiving surface, as described in the previous section, and enables mass production, which is essential for practical use. This is an issue that needs to be resolved.

(問題点を解決するための手段) 本発明は前項に述べた問題点を解決することを目的とす
るもので、X軸上の所定の長さ寸法(a)と、該長さ寸
法(、)より短いY軸上の中寸法(1))を有し、いず
れか一面を音波送受面として利用する圧電板と、該圧電
板の両面に形成した励振電極とからなるものであって、
前記圧電板の少なくとも一つの74極形状を、圧電板の
長さの中央部で最大の中寸法を有すると共に該圧電板の
両端に向かってr巾寸法が漸減する上下対称の波形とし
たことを特徴とし、電極の11q記の波形形状をケーザ
ー窓関数によって求めた窓形状と同形状にしたことをそ
の実施態様例とするものである。
(Means for Solving the Problems) The present invention aims to solve the problems described in the previous section, and it is possible to solve the problems described in the previous section by defining a predetermined length dimension (a) on the X-axis, and a predetermined length dimension (a) on the ) has a shorter medium dimension (1)) on the Y-axis, and consists of a piezoelectric plate, one of which is used as a sound wave transmission and reception surface, and excitation electrodes formed on both sides of the piezoelectric plate,
The shape of at least one 74-pole of the piezoelectric plate is a vertically symmetrical waveform having a maximum medium dimension at the center of the length of the piezoelectric plate and gradually decreasing the r width dimension toward both ends of the piezoelectric plate. An example of its implementation is that the waveform shape of the electrode in 11q is made the same as the window shape determined by the Kaeser window function.

本発明の実施例を次に説明する。Examples of the present invention will now be described.

(実施例) 本発明は、第1.2図に示すように、切断等による整形
が容易な圧電ゴム板その他の圧電板により電極形状1こ
合致する整形を施し、その両面に圧電板の整形平面形状
とするものである同一形状の電極層を形成する第1実施
例と、tjS3.4図に示すように矩形形状などの電極
形状とは無関係な形状の圧電板の一方の而又は両方の部
器こ、上下対称の波形にした電極層を形成する第2実施
例とをもつ。
(Example) As shown in Fig. 1.2, the present invention involves shaping a piezoelectric rubber plate or other piezoelectric plate that is easy to shape by cutting to match the shape of an electrode, and shaping piezoelectric plates on both sides of the plate. In the first embodiment, electrode layers of the same shape are formed in a planar shape, and one or both of the piezoelectric plates have a shape unrelated to the electrode shape, such as a rectangular shape, as shown in Figure tjS3.4. This device has a second embodiment in which an electrode layer is formed in a vertically symmetrical waveform.

第1実施例は#&1図に示すように圧電ゴム板1を、X
軸上の所定の長さ寸法(a)と、該寸法(、)より短い
Y軸上の中寸法(b)を有し、その圧電ゴム板1は長さ
の中央部で最大の中寸法(b−、)を有すると共に、長
さ方向の両端に向かって中寸法が漸減して両端部を最小
の中寸法(b−z)とする上下対称の波形とし、該圧電
ゴム/illの形状を前記したケーザー窓関数によって
求めた窓形状と同形状に整形し、その両面に圧電ゴム板
1の平面形状と同一形状の電極M2.3を形成し、電極
層2.3の分極領域4を圧電ゴム板1の平面に合致させ
たものである。
In the first embodiment, the piezoelectric rubber plate 1 is
The piezoelectric rubber plate 1 has a predetermined length dimension (a) on the axis and a medium dimension (b) on the Y axis that is shorter than the specified length dimension (,), and the piezoelectric rubber plate 1 has the maximum medium dimension (,) at the center of the length. b-, ), and the shape of the piezoelectric rubber/ill is a vertically symmetrical waveform in which the medium dimension gradually decreases toward both ends in the length direction and the minimum medium dimension (b-z) is at both ends, and the shape of the piezoelectric rubber/ill is It is shaped into the same shape as the window shape determined by the above-mentioned Kaeser window function, and electrodes M2.3 having the same planar shape as the piezoelectric rubber plate 1 are formed on both sides of the window shape, and the polarization region 4 of the electrode layer 2.3 is piezoelectrically formed. This is made to match the plane of the rubber plate 1.

圧電ゴム板1に代えて圧電磁器、口・7シエル塩等のゴ
ム以外のピエゾ板を#S1図のように整形して充てるこ
とも充分に可能である。
In place of the piezoelectric rubber plate 1, it is also possible to use a piezo plate other than rubber, such as a piezoelectric ceramic or a 7-shell salt plate, shaped as shown in Figure #S1.

第2実施例は、圧電磁器、圧電ゴム板等の方形圧電板1
1の両刀の面に、第1.2図に示した電極2.3と同形
の電極12.13を形成し、両電極12.13の分極領
域14をそれ等の電極12.13の平面形状に合致させ
る。
The second embodiment is a rectangular piezoelectric plate 1 such as a piezoelectric ceramic or a piezoelectric rubber plate.
An electrode 12.13 having the same shape as the electrode 2.3 shown in FIG. match.

尤も本実施態様のものは、音波放射及び受波に一つの電
極の形成面を使用するものであり、例えば電極12の形
成面を使用するのであれば、電極13は電極12の全面
積に対応出来る矩形、楕円形等の形状であっても分極効
果は均等である。
However, in this embodiment, one electrode forming surface is used for sound wave emission and wave reception. For example, if the forming surface of electrode 12 is used, electrode 13 corresponds to the entire area of electrode 12. Even if the shape is rectangular, elliptical, etc., the polarization effect is uniform.

il記mi実施例及び第2実施例の各電極の形成は、銀
!膜の焼付け、もしくは銀箔の接着など従来公知の工法
によって施す。
The formation of each electrode in the first embodiment and the second embodiment is made of silver! It is applied using conventionally known methods such as baking a film or gluing silver foil.

(乍用) クロロブレンゴムとチタン酸鉛とを体積比で40:60
の割合で混合した圧電複合材料よりよこ(a)Xたて(
b)×厚み= 100 X 20 X 2 ++n。
(For use) Chloroprene rubber and lead titanate in a volume ratio of 40:60.
Horizontal (a)
b) x thickness = 100 x 20 x 2 ++n.

の矩形寸法に成形した圧電ゴム板11の表裏面に銀粉末
入り導電ゴム材料よりなる厚さ0.5+amの電極12
.13を一体に被着してなる第3.4図の矩形板の構成
において、電極12.13につき、上下側辺を、ケープ
−窓関係の公式中、i=LOOmm、b=20+am、
ダ=3πの条件で求めた関数曲線に沿って整形した上下
対称の波形に整形した本発明の圧電素子の指向特性を測
定した結果は、!@7図に示した如く、サイドローブを
一30dB以下に抑制することを確認した。このことか
らも本発明の効果を立証し得る。なお、第8図は従来の
矩形板(、=100ma+5b=20、α=0)の指向
特性の測定結果で、多くのサイドローブが観測される。
Electrodes 12 with a thickness of 0.5+am made of a conductive rubber material containing silver powder are placed on the front and back surfaces of a piezoelectric rubber plate 11 formed into a rectangular size.
.. In the structure of the rectangular plate shown in Fig. 3.4, in which the electrode 12.13 is integrally adhered, the upper and lower sides of the electrode 12.13 are defined by the formula of the cape-window relationship: i=LOOmm, b=20+am,
The results of measuring the directivity characteristics of the piezoelectric element of the present invention, which was shaped into a vertically symmetrical waveform along the function curve determined under the condition of Da = 3π, are as follows! @ As shown in Figure 7, we confirmed that the side lobe was suppressed to -30 dB or less. This also proves the effectiveness of the present invention. Note that FIG. 8 shows the measurement results of the directional characteristics of a conventional rectangular plate (=100 ma+5b=20, α=0), in which many side lobes are observed.

(効果) 本発明の送受波用圧電素子は、Y軸上の所定の長さ寸法
(、)と、該長さ寸法(a)より短いY軸上の中寸法(
b)を有し、いずれか一面を音波送受面として利用する
圧電板と、該圧電板の両面に形成した励振電極とからな
るものにおいて、前記圧電板の少なくとも一つの電極形
状を、圧電板の長さの中央部で最大の1寸法を有すると
ともに該圧電板の両端に向かって中寸法が漸減する上下
対称の波形としたものであり、少なくとも一つの電極の
対称の波形形状を、ケーザー窓関数の公式によりもとめ
た窓形状と同一にすることを実施態様とするもので、こ
の構成によりサイドローブを抑制した形状シェージング
の電極形状を備える圧電素子の大量生産を可能にして、
ノ)イドロホーン、ffi音波探傷器等の用途に供給で
きる効果を生ずる。
(Effects) The wave transmitting and receiving piezoelectric element of the present invention has a predetermined length dimension (, ) on the Y-axis and a middle dimension (, ) on the Y-axis that is shorter than the length dimension (a).
b), which consists of a piezoelectric plate whose one side is used as a sound wave transmitting/receiving surface, and excitation electrodes formed on both sides of the piezoelectric plate, in which the shape of at least one electrode of the piezoelectric plate is The piezoelectric plate has a vertically symmetrical waveform having a maximum dimension at the center and a gradually decreasing middle dimension toward both ends of the piezoelectric plate, and the symmetrical waveform shape of at least one electrode is defined by the Kaeser window function. This is an embodiment in which the window shape is the same as that determined by the formula, and this configuration makes it possible to mass produce piezoelectric elements having an electrode shape with shape shading that suppresses side lobes.
(g) It produces an effect that can be applied to applications such as hydrophones and ffi sonic flaw detectors.

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

第1〜4図は本発明の実施例を示し、第1図は第1実施
例の一部切欠平面図、第2図は第1図A−Ai切断側面
図、第3図は第2実施例の平面図、第4図は第3図B−
B線切断側面図、PtIJ5図は説明のだめの斜視図、
第6図は同側面図、第7図は本発明に係る送受波用圧電
素子の指向特性図、第8図は従来の送受波用圧電素子の
指向特性図である。
1 to 4 show embodiments of the present invention, FIG. 1 is a partially cutaway plan view of the first embodiment, FIG. 2 is a side view taken along the line A-Ai in FIG. The example plan view, Figure 4 is Figure 3B-
B-line cut side view, PtIJ5 figure is a perspective view for illustration purposes only,
FIG. 6 is a side view of the same, FIG. 7 is a directional characteristic diagram of a piezoelectric element for wave transmission and reception according to the present invention, and FIG. 8 is a directional characteristic diagram of a conventional piezoelectric element for wave transmission and reception.

Claims (1)

【特許請求の範囲】 1)X軸上の所定の長さ寸法(a)と、該長さ寸法(a
)より短いY軸上の巾寸法(b)を有し、いずれか一面
を音波送受面として利用する圧電板と、該圧電板の両面
に形成した励振電極とからなるものであって、前記圧電
板の少なくとも一つの電極形状を、圧電板の長さの中央
部で最大の巾寸法を有するとともに該圧電板の両端に向
かって巾寸法が漸減する上下対称の波形としたことを特
徴とする送受波用圧電素子。 2)電極の波形形状がケーザー窓関数の下記公式▲数式
、化学式、表等があります▼ (ただしα>0) によって求めた窓形状と同形状にしたことを特徴とする
特許請求の範囲第1項記載の送受波用圧電素子。
[Claims] 1) A predetermined length dimension (a) on the X-axis and the length dimension (a
), the piezoelectric plate has a width dimension (b) on the Y axis that is shorter than A transmission/reception device characterized in that the shape of at least one electrode of the plate is a vertically symmetrical waveform having a maximum width at the center of the length of the piezoelectric plate and gradually decreasing the width toward both ends of the piezoelectric plate. Piezoelectric element for waves. 2) Claim 1, characterized in that the waveform shape of the electrode is the same as the window shape determined by the following Kaeser window function formula ▲There are mathematical formulas, chemical formulas, tables, etc.▼ (where α>0) A piezoelectric element for transmitting and receiving waves as described in .
JP6685386A 1986-03-25 1986-03-25 Piezoelectric element for sound wave transmission and reception Pending JPS62224199A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6685386A JPS62224199A (en) 1986-03-25 1986-03-25 Piezoelectric element for sound wave transmission and reception

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6685386A JPS62224199A (en) 1986-03-25 1986-03-25 Piezoelectric element for sound wave transmission and reception

Publications (1)

Publication Number Publication Date
JPS62224199A true JPS62224199A (en) 1987-10-02

Family

ID=13327822

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6685386A Pending JPS62224199A (en) 1986-03-25 1986-03-25 Piezoelectric element for sound wave transmission and reception

Country Status (1)

Country Link
JP (1) JPS62224199A (en)

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5830394U (en) * 1981-08-24 1983-02-28 三菱電機株式会社 dome speaker
JPS58161493A (en) * 1982-02-16 1983-09-26 ゼネラル・エレクトリツク・カンパニイ Shaded supersonic converter array
JPS58161492A (en) * 1982-02-16 1983-09-26 ゼネラル・エレクトリツク・カンパニイ Shaded supersonic converter

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5830394U (en) * 1981-08-24 1983-02-28 三菱電機株式会社 dome speaker
JPS58161493A (en) * 1982-02-16 1983-09-26 ゼネラル・エレクトリツク・カンパニイ Shaded supersonic converter array
JPS58161492A (en) * 1982-02-16 1983-09-26 ゼネラル・エレクトリツク・カンパニイ Shaded supersonic converter

Similar Documents

Publication Publication Date Title
US3833825A (en) Wide-band electroacoustic transducer
JPS58161493A (en) Shaded supersonic converter array
JPH01291840A (en) Ultrasonic probe
JPS597280B2 (en) Impedance matching device and acoustic transducer assembly using the same
US4322651A (en) Acoustic surface wave device
Toda Phase-matched air ultrasonic transducers using corrugated PVDF film with half wavelength depth
JP4134911B2 (en) Ultrasonic transducer and method for manufacturing the same
JPS62224199A (en) Piezoelectric element for sound wave transmission and reception
US2989725A (en) Electroacoustic transducer
JPS60264200A (en) Ultrasonic wave vibrator
US2411551A (en) Radiating system
JPS6123913Y2 (en)
JPH08275295A (en) Acoustic transducer
JPH03112300A (en) Vibrator unit
JPS6153562A (en) Ultrasonic probe
WO2021193788A1 (en) Piezoelectric acoustic component
JP3009529B2 (en) Ultrasonic transducer
JPS63250996A (en) Piezo-electric vibrator
JP3255658B2 (en) Surface acoustic wave convolver
JPH07112316B2 (en) Method of polarization treatment of piezoelectric flexible sheet for piezoelectric wave transmitter
JPS62231591A (en) Piezoelectric wave transmitter-receiver
JPH0564919B2 (en)
JPH0538335A (en) Ultrasonic probe and manufacture thereof
JP3181949B2 (en) Ultrasonic vibrator and method of manufacturing ultrasonic vibrator
JPH0564918B2 (en)