JPH0452677B2 - - Google Patents
Info
- Publication number
- JPH0452677B2 JPH0452677B2 JP58020005A JP2000583A JPH0452677B2 JP H0452677 B2 JPH0452677 B2 JP H0452677B2 JP 58020005 A JP58020005 A JP 58020005A JP 2000583 A JP2000583 A JP 2000583A JP H0452677 B2 JPH0452677 B2 JP H0452677B2
- Authority
- JP
- Japan
- Prior art keywords
- piezoelectric
- case
- same
- electrodes
- piezoelectric effect
- 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
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; ELECTRIC HEARING AIDS; PUBLIC ADDRESS SYSTEMS
- H04R17/00—Piezoelectric transducers; Electrostrictive transducers
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
- Signal Processing (AREA)
- Piezo-Electric Transducers For Audible Bands (AREA)
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Description
【発明の詳細な説明】
産業上の利用分野
本発明は圧電素子二枚を貼り合せてなる貼り合
せ型圧電振動子に関する。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a bonded piezoelectric vibrator made by bonding two piezoelectric elements.
従来例の構成とその問題点
貼り合せ型圧電振動子の一つであるバイモルフ
型圧電振動子の応用例はそのたわみ振動を利用し
て電気入力を加えることによつて振動させる逆圧
電効果を利用するもの、また外部から機械振動を
加えることにより電気信号を加える圧電効果を利
用してなるものの二種類にわけられる。前者の場
合の応用例としては超音波や音波の送波器、振動
発生器等の応用例があり後者の場合は超音波等の
音波の受波器や振動ピツクアツプが代表的な例で
ある。Conventional structure and its problems An application example of a bimorph piezoelectric vibrator, which is one of the bonded piezoelectric vibrators, uses the inverse piezoelectric effect to vibrate by applying electrical input using its flexural vibration. There are two types: those that use external mechanical vibrations to generate electrical signals, and those that utilize piezoelectric effects. Typical examples of applications in the former case include ultrasonic and sonic wave transmitters, vibration generators, etc., and in the latter case, typical examples include ultrasonic and other sonic wave receivers and vibration pickups.
従来バイモルフ型圧電振動子には二種類があ
る。これを第1図、第2図で説明する。第1図は
並列接続法第2図は直列接続法によるバイモルフ
型圧電振動子の断面図である。第1図にのいて
1,2は矢印方向に分極された圧電素子で境界面
3において二枚が電気的、機械的に接続されてい
る。分極方向は矢印の方向でもわかるように二枚
共、同一方向に向いている。圧電素子1,2の主
面4,5にはそれぞれ電極が設けられており、そ
の電気接続は面3,5及び面4,5を電源Vに接
続している。 Conventionally, there are two types of bimorph piezoelectric vibrators. This will be explained with reference to FIGS. 1 and 2. FIG. 1 is a cross-sectional view of a bimorph piezoelectric vibrator using a parallel connection method and FIG. 2 a series connection method. In FIG. 1, numerals 1 and 2 are piezoelectric elements polarized in the direction of the arrow, and the two pieces are electrically and mechanically connected at an interface 3. As can be seen from the direction of the arrow, the polarization direction of both sheets is oriented in the same direction. Electrodes are provided on the main surfaces 4, 5 of the piezoelectric elements 1, 2, respectively, and electrical connections connect the surfaces 3, 5 and 4, 5 to a power supply V.
今この振動子を逆圧電効果で使う場合を考える
と圧電素子1は分極方向を逆方向の電界がかかる
為長さ方向に延び逆に圧電素子2は同方向に電界
がかかる為長さ方向に縮む、従つて片一方が延び
片一方が縮む為図のようなたわみ運動をおこす。 Now, if we consider the case where this vibrator is used with the inverse piezoelectric effect, piezoelectric element 1 extends in the length direction because an electric field with the polarization direction opposite is applied, and piezoelectric element 2 extends in the length direction because an electric field is applied in the same direction. It contracts, so one side extends and the other contracts, causing a bending movement as shown in the figure.
又、逆に圧電効果で使用する場合を考えてみる
と第1図のようなたわみになるように外力が与え
られたとすると圧電素子1は長さ方向に延ばされ
るので面3にの電荷、面4にの電荷がチヤー
ジされる。又圧電素子2は逆に長さ方向に縮めら
れるので面3に、面5にの電荷がチヤージさ
れ面3と面4,5の間に電圧が発生する。 Conversely, if we consider the case where the piezoelectric effect is used, if an external force is applied to cause the deflection as shown in Figure 1, the piezoelectric element 1 will be extended in the length direction, so the charge on the surface 3 and the surface 4 is charged. Moreover, since the piezoelectric element 2 is conversely contracted in the length direction, electric charges on the surfaces 3 and 5 are charged, and a voltage is generated between the surfaces 3 and 4 and 5.
次に、第2図は圧電素子6,7の分極方向が互
に180°異る方向に接続される直列接続の方法であ
る。この場合も二枚の圧電素子6,7は境界面9
において二枚が電気的、機械的に接続されてお
り、第1図と同様に分極方向に垂直な対抗する面
8,9,10にはそれぞれ電極が設けられてい
る。この場合は電気入出力端子は面8,10に接
続されている。今逆圧電効果での利用の場合を考
えると面8に、面10にの電圧を加えると第
1図と同様に圧電素子6の素子は長さ方向に延び
圧電素子7の素子は長さ方向に縮み第2図のよう
なたわみ振動を行う。逆に、圧電効果の利用を見
た場合外力が加わり、第2図のようなたわみをし
た場合、圧電素子6は長さ方向に延される為、面
8に、面9に、逆に圧電素子7は面9に、
面10にの電荷がチヤージされ面8〜10に電
圧が生じる。 Next, FIG. 2 shows a method of series connection in which the piezoelectric elements 6 and 7 are connected in directions in which the polarization directions are different from each other by 180°. In this case as well, the two piezoelectric elements 6 and 7 have an interface 9
The two plates are electrically and mechanically connected, and as in FIG. 1, electrodes are provided on opposing surfaces 8, 9, and 10 perpendicular to the polarization direction, respectively. In this case, the electrical input/output terminals are connected to the surfaces 8 and 10. Now considering the case of use in the inverse piezoelectric effect, when a voltage is applied to planes 8 and 10, the elements of piezoelectric element 6 extend in the length direction and the elements of piezoelectric element 7 extend in the length direction, as in FIG. It contracts and performs a flexural vibration as shown in Figure 2. Conversely, when looking at the use of the piezoelectric effect, if an external force is applied and the piezoelectric element 6 is bent as shown in Figure 2, the piezoelectric element 6 is extended in the length direction, so the piezoelectric Element 7 is on surface 9,
The charge on surface 10 is charged and a voltage is generated on surfaces 8-10.
今たわみ特性、電気特性を比較する為に第1図
第2図の圧電素子の形状寸法を同一としそれぞれ
の電気容量をcとし、又、圧電素子の厚みをtと
すると第1図の場合の逆圧電効果によるたわみを
ξ1第2図の場合をξ2又圧電効果による発生電圧を
V1、V2とし、逆圧電効果の入力電圧をどちらも
V、圧電効果による外力をどちらもFとするとそ
れぞれξ1=A×d31×V/π、ξ1=A×d31×V/2t
V1=B×d31×F、V2=2×B×d31×Fであ
る。又電気インピーダンスは共振周波数以下であ
ればそれぞれZ1=1/2ωC、Z2=1/ωcである。 Now, in order to compare the deflection characteristics and electrical characteristics, let us assume that the shapes and dimensions of the piezoelectric elements in Figures 1 and 2 are the same, and the capacitance of each is c, and the thickness of the piezoelectric element is t. The deflection due to the inverse piezoelectric effect is ξ 1 The case shown in Figure 2 is ξ 2 The voltage generated due to the piezoelectric effect is
Let V 1 and V 2 be V 1 and V 2 be the input voltage of the inverse piezoelectric effect, and F be the external force due to the piezoelectric effect, then ξ 1 = A×d 31 ×V/π, ξ 1 = A×d 31 ×V, respectively. /2t V 1 =B×d 31 ×F, V 2 =2×B×d 31 ×F. Moreover, if the electrical impedance is below the resonance frequency, Z 1 =1/2ωC and Z 2 =1/ωc, respectively.
従つて、逆圧電効果の場合入力電荷は並列接続
(第1図)の場合直列接続(第2図)の場合より
倍になつて倍歪んでいることになる。又、圧電効
果の場合、並列接続(第1図)の出力電荷は直列
接続(第2図)と同じで発生電圧が直列接続(第
2図)の場合の倍(6dB)アツプされることにな
る。このことから一般に逆圧電効果を利用する場
合、同一印加電圧で直列接続の場合より並列接続
の方がよく歪むため並列接続を使う方が有利であ
りこれが使われる場合も多い。又、逆に圧電効果
の利用の場合は直列接続を利用することが有利で
ある。 Therefore, in the case of the inverse piezoelectric effect, the input charge is doubled and distorted in the case of parallel connection (FIG. 1) than in the case of series connection (FIG. 2). In addition, in the case of the piezoelectric effect, the output charge of parallel connection (Fig. 1) is the same as that of series connection (Fig. 2), and the generated voltage is twice (6 dB) higher than that of series connection (Fig. 2). Become. For this reason, when using the inverse piezoelectric effect, it is generally more advantageous to use parallel connections, and this is often used, since parallel connections cause more distortion than series connections with the same applied voltage. Conversely, when utilizing the piezoelectric effect, it is advantageous to use series connection.
しかし、同一振動子で圧電効果と逆圧電効果の
両方使用するような用途(例えば超音送の送受信
を同一の素子で行う場合)にはどちらかの一つで
使わざるを得ない。従つて、入力電圧又は出力感
度のどちらかを犠牲にしているわけである。 However, in applications where the same vibrator uses both the piezoelectric effect and the inverse piezoelectric effect (for example, when transmitting and receiving ultrasonic waves using the same element), one or the other must be used. Therefore, either input voltage or output sensitivity is sacrificed.
発明の目的
本発明は入力電圧、出力感度の両方を同時に満
足できる貼り合せ型圧電振動子を提供するもので
ある。OBJECTS OF THE INVENTION The present invention provides a bonded piezoelectric vibrator that can simultaneously satisfy both input voltage and output sensitivity.
発明の構成
本発明は厚み方向に互いに分極方向が180°異な
るような分極を二つ以上有する第1、第2の圧電
振動子を備え、この圧電振動子の互いに重なる部
分の分極方向が同方向になるように貼り合せた貼
り合せ型圧電振動子である。Structure of the Invention The present invention includes first and second piezoelectric vibrators having two or more polarizations whose polarization directions differ by 180 degrees from each other in the thickness direction, and in which the polarization directions of the mutually overlapping portions of the piezoelectric vibrators are in the same direction. This is a bonded piezoelectric vibrator that is bonded together so that
実施例の説明
第3図に本発明の一実施例を示す。第3図にお
いて、圧電素子11,12はほぼ真中で分極方向
が180°異なるように分極されそれぞれの分極域に
応じて分極面に垂直な面に電極13〜18が設け
られ圧電素子11と12は電極で電気的機械的に
接続されている。DESCRIPTION OF EMBODIMENTS FIG. 3 shows an embodiment of the present invention. In FIG. 3, piezoelectric elements 11 and 12 are polarized so that their polarization directions differ by 180° approximately in the middle, and electrodes 13 to 18 are provided on a plane perpendicular to the polarization plane according to their respective polarization regions. are electrically and mechanically connected by electrodes.
本発明の圧電振動子を圧電効果で使用したい場
合、外力が加わり素子が図のようにたわんだとす
ると、圧電素子11は延びる為電極13に、電
極14に、電極17に、電極16にの電荷
が発生し、電極14,17を接続すると第2図の
場合の同じ電圧が電極13,16及び電極15,
18の間に発生する。従つて、電極13,18間
と電極15,16間を両端子とした場合の出力電
圧は第2図の場合と同じ直列接続の例となる。 When it is desired to use the piezoelectric vibrator of the present invention with the piezoelectric effect, if an external force is applied and the element is bent as shown in the figure, the piezoelectric element 11 will extend, and electric charges will be applied to the electrodes 13, 14, 17, and 16. When the electrodes 14 and 17 are connected, the same voltage as in the case of FIG.
Occurs between 18 and 18. Therefore, the output voltage when the terminals between the electrodes 13 and 18 and between the electrodes 15 and 16 are set as both terminals is the same example of series connection as in the case of FIG. 2.
又、逆圧電効果で使いたい場合は電極14に
電極13〜15に、電極17に、電極16〜
18にの電圧をそれぞれ印加すれば第1図の並
列接続と全く同じで並列型バイモルフの構成とな
る。電極13〜18をメモリーやICスイツチで
行えば逆圧電効果、圧電効果の使い方によつて並
列接続直列接続の切り換えは非常に簡単であり、
超音波の送受信のような使い方の場合は非常に有
利である。 In addition, if you want to use the inverse piezoelectric effect, connect electrodes 13 to 15 to electrode 14, electrodes 16 to 17 to
If a voltage is applied to each of 18, a parallel bimorph configuration will be obtained, which is exactly the same as the parallel connection shown in FIG. If electrodes 13 to 18 are connected using memory or IC switches, it is very easy to switch between parallel and series connections depending on how to use the inverse piezoelectric effect and piezoelectric effect.
This is very advantageous for uses such as transmitting and receiving ultrasonic waves.
発明の効果
本発明の貼り合せ型圧電振動子は1ケのトラン
スジユーサーで送信時には並列接続で同一入力電
圧でパワーを大きくとり、送信が終ればすぐ直列
接続のバイモルフにし受信すれば受信感度が大き
くとれる。Effects of the Invention The bonded piezoelectric vibrator of the present invention is a single transducer, and when transmitting, it is connected in parallel to obtain a large power with the same input voltage, and as soon as the transmission is finished, it is connected in series as a bimorph, and when receiving, the reception sensitivity is improved. It can be taken in large quantities.
第1図、第2図はそれぞれ従来の並列型、直列
型の圧電振動子の断面図、第3図は本発明の実施
例に係る圧電振動子の断面図である。
11,12……圧電振動子、13〜18……電
極。
FIGS. 1 and 2 are cross-sectional views of conventional parallel-type and series-type piezoelectric vibrators, respectively, and FIG. 3 is a cross-sectional view of a piezoelectric vibrator according to an embodiment of the present invention. 11, 12... piezoelectric vibrator, 13-18... electrode.
Claims (1)
分極を二つ以上有する第1、第2の圧電振動子を
備え上記第1、第2の圧電振動子の互いに重なる
部分の分極方向が同方向になるように貼り合せた
貼り合せ型圧電振動子。1. First and second piezoelectric vibrators having two or more polarizations whose polarization directions differ by 180 degrees from each other in the thickness direction, and the polarization directions of the overlapping parts of the first and second piezoelectric vibrators are the same. A bonded piezoelectric vibrator that is bonded in the same direction.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58020005A JPS59146298A (en) | 1983-02-09 | 1983-02-09 | Sticked type piezoelectric oscillator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58020005A JPS59146298A (en) | 1983-02-09 | 1983-02-09 | Sticked type piezoelectric oscillator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59146298A JPS59146298A (en) | 1984-08-22 |
| JPH0452677B2 true JPH0452677B2 (en) | 1992-08-24 |
Family
ID=12015012
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58020005A Granted JPS59146298A (en) | 1983-02-09 | 1983-02-09 | Sticked type piezoelectric oscillator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59146298A (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02122458U (en) * | 1989-03-22 | 1990-10-08 | ||
| US7538477B2 (en) * | 2006-11-27 | 2009-05-26 | Avago Technologies Wireless Ip (Singapore) Pte. Ltd. | Multi-layer transducers with annular contacts |
| US10129656B2 (en) | 2009-01-30 | 2018-11-13 | Avago Technologies International Sales Pte. Limited | Active temperature control of piezoelectric membrane-based micro-electromechanical devices |
| US8258678B2 (en) | 2010-02-23 | 2012-09-04 | Avago Technologies Wireless Ip (Singapore) Pte. Ltd. | Short range ultrasonic device with broadbeam ultrasonic transducers |
-
1983
- 1983-02-09 JP JP58020005A patent/JPS59146298A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59146298A (en) | 1984-08-22 |
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