JPH0429280B2 - - Google Patents
Info
- Publication number
- JPH0429280B2 JPH0429280B2 JP29959886A JP29959886A JPH0429280B2 JP H0429280 B2 JPH0429280 B2 JP H0429280B2 JP 29959886 A JP29959886 A JP 29959886A JP 29959886 A JP29959886 A JP 29959886A JP H0429280 B2 JPH0429280 B2 JP H0429280B2
- Authority
- JP
- Japan
- Prior art keywords
- diaphragm
- vibration
- length
- piezoelectric
- piezoelectric ceramic
- 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
- H04R17/04—Gramophone pick-ups using a stylus; Recorders using a stylus
- H04R17/08—Gramophone pick-ups using a stylus; Recorders using a stylus signals being recorded or played back by vibration of a stylus in two orthogonal directions simultaneously
Landscapes
- Measurement Of Mechanical Vibrations Or Ultrasonic Waves (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
本発明は長さ方向の電気的歪変化(長さ振動)
を厚み方向の機械的振動に転換する捩れ振動子に
関する。[Detailed description of the invention] Industrial application field The present invention is directed to electric strain change in the longitudinal direction (length vibration).
This invention relates to a torsional oscillator that converts vibration into mechanical vibration in the thickness direction.
従来技術
電圧印加によつて長さ振動する圧電セラミツク
の特性を利用し、長さ振動を厚み方向の機械的振
動に変換するものとして、圧電セラミツクに金属
板を貼り合せた振動子(圧電バイモルフ)が知ら
れている。又、二枚の圧電セラミツクを電圧印加
時の伸縮方向が逆方向となるように貼り合せ、一
方に伸び、他方に縮みを交互に生じさせることに
よつて厚み方向の機械的振動に転換する振動子が
提供されている。Conventional technology A vibrator (piezoelectric bimorph) made by bonding a metal plate to a piezoelectric ceramic is used to convert the length vibration into mechanical vibration in the thickness direction by utilizing the characteristic of piezoelectric ceramic that vibrates in length when a voltage is applied. It has been known. In addition, two pieces of piezoelectric ceramic are pasted together so that the directions of expansion and contraction are opposite when a voltage is applied, and by alternately causing expansion and contraction on one side and contraction on the other side, vibration is converted into mechanical vibration in the thickness direction. Child is provided.
上記圧電セラミツクは自発分極を持つ強誘電セ
ラミツクに、高電圧を印加し分極方向を一方向に
固定する、所謂分極処理(ポーリング処理)を施
したものである。 The piezoelectric ceramic described above is a ferroelectric ceramic having spontaneous polarization which is subjected to a so-called polarization treatment (poling treatment) in which a high voltage is applied to fix the polarization direction in one direction.
発明が解決しようとする問題点
而して上記圧電セラミツク振動子は何れも、電
圧印加時の厚み方向の振動動作が単純なベンデイ
ング運動である。Problems to be Solved by the Invention In all of the piezoelectric ceramic vibrators described above, the vibration motion in the thickness direction when voltage is applied is a simple bending motion.
従つて、上記圧電セラミツク振動子はベンデイ
ング運動を振動源とする用途、例えば電気音響変
換機や圧電形フイルター等の限定された用途に狭
められている。 Therefore, the use of the piezoelectric ceramic vibrator is limited to applications where bending motion is used as a vibration source, such as electroacoustic transducers and piezoelectric filters.
上記の如く従来の圧電セラミツクは、基本的に
は上記の如きベンデイング運動源等とする長さ振
動か、又は厚み方向の振動、或は径方向振動等の
振動モードに限られていたが、本発明は上記圧電
セラミツクに異方向複屈曲性を具有させ、圧電セ
ラミツクが厚み方向の一方に部分屈曲すると同時
に、厚み方向の他方に部分屈曲する、所謂捩れ振
動を生起させるようにした固有の振動モードを有
する、工業上好適に利用し得る捩れ振動子を提供
せんとするものである。 As mentioned above, conventional piezoelectric ceramics are basically limited to vibration modes such as length vibration, thickness direction vibration, or radial vibration using the bending motion source as described above. The invention provides a unique vibration mode in which the piezoelectric ceramic has birefringence in different directions, and the piezoelectric ceramic partially bends in one direction in the thickness direction and at the same time partially bends in the other direction in the thickness direction, causing so-called torsional vibration. It is an object of the present invention to provide a torsional oscillator having the following characteristics and which can be suitably used industrially.
これによつて、上記捩れ振動モードを利用する
新分野への圧電セラミツクの用途拡張を図り、例
えば粘度検出素子又は比重計等の検出用振動子と
して富適性を持つたものを提供するものである。 Through this, we aim to expand the use of piezoelectric ceramics to new fields that utilize the above-mentioned torsional vibration mode, and provide products that are highly suitable as detection oscillators, such as viscosity detection elements or hydrometers. .
問題点を解決するための手段
本発明は上記問題点を解決する手段として、長
さ振動する圧電素子間に振動板を介在し積層して
成る振動子であつて、振動板の片面側と他面側の
両長さ振動圧電素子をその長さ振動方向が交叉す
るように配置し、両長さ振動圧電素子が振動板の
片面側と他面側において同時に伸び又は同時に縮
みを生ずるように長さ振動させることにより、上
記振動板の捩れ振動を得る構成としたものであ
る。Means for Solving the Problems As a means for solving the above problems, the present invention provides a vibrator in which a diaphragm is interposed between longitudinally vibrating piezoelectric elements and laminated, one side of the diaphragm and the other. The two-length vibrating piezoelectric elements on the surface side are arranged so that their length vibration directions intersect, and the two-length vibrating piezoelectric elements are lengthened so that they simultaneously expand or contract on one side and the other side of the diaphragm. By causing the diaphragm to vibrate, torsional vibration of the diaphragm is obtained.
作 用
本発明によれば、上記交叉する両圧電素子の振
動モードが、一方の交叉圧電素子で縮みを生じた
時、同時に他方の交叉圧電素子で縮みを生じ、逆
に一方で伸びを生じた時、同時に他方で伸びを生
じ、各圧電素子において同方向の伸縮振動モード
が複合して生ずる。従つて、これに貼り合せられ
た振動板は交叉する一方の長さ振動圧電素子の両
端部分において厚み方向の一方に屈曲し、同時に
交叉する他方の長さ振動圧電素子の両端部分にお
いて厚み方向に屈曲することとなる。これを交互
に生ずることにより、所謂複屈曲振動(捩れ振
動)を誘起する。Effects According to the present invention, when the vibration modes of the above-mentioned crossing piezoelectric elements cause contraction in one crossing piezoelectric element, contraction occurs in the other crossing piezoelectric element at the same time, and conversely, an extension occurs in one crossing piezoelectric element. At the same time, the other piezoelectric element elongates, and a plurality of elongation and contraction vibration modes in the same direction occur in each piezoelectric element. Therefore, the diaphragm bonded to this is bent in one direction in the thickness direction at both ends of the vibrating piezoelectric element of one length that intersects, and at the same time bends in the thickness direction at both ends of the vibrating piezoelectric element of the other length that intersects. It will be bent. By causing this alternately, so-called double bending vibration (torsional vibration) is induced.
実施例 以下本発明の実施例を図面に基いて説明する。Example Embodiments of the present invention will be described below based on the drawings.
圧電素子として、前記の如く強誘電セラミツク
に分極処理(ポーリング処理)を施して圧電性を
付与した圧電セラミツクを用いる。分極処理は分
極方向を一方向に固定する処理であり、その分極
方向によつて正電圧又は負電圧に対する伸び又は
縮み方向(長さ振動方向)が逆方向となる。 As the piezoelectric element, a piezoelectric ceramic is used, which is obtained by subjecting ferroelectric ceramic to polarization treatment (poling treatment) to impart piezoelectricity as described above. The polarization process is a process in which the polarization direction is fixed in one direction, and depending on the polarization direction, the elongation or contraction direction (length vibration direction) with respect to a positive voltage or a negative voltage becomes opposite.
第1図乃至第11図に示すように、本発明は上
記長さ振動する圧電セラミツク1,2間に振動板
3を介在し積層して成る振動子であつて、振動板
3の片面側と他面側の両長さ振動圧電セラミツク
1,2をその長さ振動方向が交叉するように配置
し、両長さ振動圧電セラミツク1,2が振動板3
の片面側と他面側において同時に伸び又は縮みを
生ずるように長さ振動させ、上記振動板3の捩れ
振動を得る構成としたものである。 As shown in FIGS. 1 to 11, the present invention is a vibrator in which a diaphragm 3 is interposed and laminated between piezoelectric ceramics 1 and 2 that vibrate along the length, and one side of the diaphragm 3 is The vibrating piezoelectric ceramics 1 and 2 with both lengths on the other side are arranged so that their length vibration directions intersect, and the vibrating piezoelectric ceramics 1 and 2 with both lengths are connected to the diaphragm 3.
The diaphragm 3 is vibrated in length so as to cause expansion or contraction simultaneously on one side and the other side, thereby obtaining torsional vibration of the diaphragm 3.
これを具体的に説明すると、第1図乃至第3図
(第1実施例)に示すように、一対の長手方向に
長さ振動する短冊形を呈する細長圧電セラミツク
1,2を準備し、一方の細長圧電セラミツク1を
方形の振動板3の片面側に貼付し、他方の細長圧
電セラミツク2を同振動板3の他面側に貼付し
て、一方の細長圧電セラミツク1を振動板3の一
方の対角線上に配置すると共に、他方の細長圧電
セラミツク2を振動板3の他方の対角線上に配置
し、両細長圧電セラミツク2の長さ振動方向が交
叉するように配置する。各圧電セラミツク1,2
は方形の振動板3の中心部において交叉し、夫々
の両端部が対角線上にある振動板3の各コーナ部
分に位置する。 To explain this specifically, as shown in FIGS. 1 to 3 (first embodiment), a pair of elongated piezoelectric ceramics 1 and 2 each having a rectangular shape that vibrates in the longitudinal direction is prepared, and one An elongated piezoelectric ceramic 1 is attached to one side of a rectangular diaphragm 3, and the other elongated piezoelectric ceramic 2 is attached to the other side of the diaphragm 3. and the other elongated piezoelectric ceramic 2 is arranged on the other diagonal of the diaphragm 3 so that the longitudinal vibration directions of both elongated piezoelectric ceramics 2 intersect. Each piezoelectric ceramic 1, 2
intersect at the center of the rectangular diaphragm 3, and both ends thereof are located at diagonal corner portions of the diaphragm 3.
第4図Aに示すように並列接続の場合、両細長
圧電セラミツク1,2を夫々の分極方向Pが互い
に逆方向となるように振動板3の片面側と他の片
面側に貼り合せ、前記交叉状態を形成する。 In the case of parallel connection as shown in FIG. 4A, both elongated piezoelectric ceramics 1 and 2 are bonded to one side and the other side of the diaphragm 3 so that their respective polarization directions P are opposite to each other. Form a crossover state.
又、第4図Bに示すように、直列接続の場合、
細長圧電セラミツク1,2を互いに同一分極方向
となるように、各々を振動板3に前記交叉配置で
積層する。 Also, as shown in Figure 4B, in the case of series connection,
The elongated piezoelectric ceramics 1 and 2 are stacked on the diaphragm 3 in the above-mentioned crossed arrangement so that the polarization directions are the same.
上記圧電セラミツク1,2は単層構造のものを
示したが、これを前記説明の如く長さ振動する圧
電セラミツクの特性を利用した複数枚のセラミツ
クバイモルフを用い、ベンデイング運動を生起さ
せるようにしたものを用いても良い。 The piezoelectric ceramics 1 and 2 shown above have a single-layer structure, but as explained above, a plurality of ceramic bimorphs that utilize the characteristic of piezoelectric ceramics to vibrate along their length are used to generate bending motion. You can also use something.
上記によつて、第5図に示すように各圧電セラ
ミツク1,2の振動モードが、一方の圧電セラミ
ツク1で伸びx1を生じた時、他方の圧電セラミ
ツク2でも伸びx2を生じ、逆に一方の圧電セラ
ミツク1で縮みを生じた時、他方の圧電セラミツ
ク2でも縮みを生じ、互いに同方向の伸縮振動モ
ードが交叉軸線上において同時に生ずるようにす
る。従つてこれに貼り合せられた振動板3は、交
叉する一方の長さ振動圧電素子1の両端部分にお
いて厚み方向の一方に屈曲y1し、同時に交叉す
る他方の長さ振動圧電素子2の両端部分において
厚み方向の他方に屈曲y2することとなる。これ
を交互に生ずることにより、所謂複屈曲振動(捩
れ振動)zを誘起する。 According to the above, as shown in FIG. 5, when the vibration mode of each piezoelectric ceramic 1 and 2 causes elongation x1 in one piezoelectric ceramic 1, elongation x2 also occurs in the other piezoelectric ceramic 2, and vice versa. When one piezoelectric ceramic 1 contracts, the other piezoelectric ceramic 2 also contracts, so that stretching vibration modes in the same direction occur simultaneously on the intersecting axes. Therefore, the diaphragm 3 bonded to this is bent in one direction in the thickness direction y1 at both end portions of the vibrating piezoelectric element 1 of one length that intersect, and at the same time, the both end portions of the vibrating piezoelectric element 2 of the other length that intersect. It is bent y2 in the other direction in the thickness direction. By causing this alternately, so-called double bending vibration (torsional vibration) z is induced.
又、他の実施例として第6図に示すように、第
1図乃至第3図の実施例において、一方又は双方
の細長圧電セラミツク1,2を複分割して前記交
叉状に配置する。一方の圧電セラミツク1と他方
の圧電セラミツク2とはその長さ振動軸線が方形
の振動板3の中心部において交叉し、各セラミツ
ク両端が振動板3の各コーナ部分に位置し、各セ
ラミツク1,2は中心部において等分割される。 As another embodiment, as shown in FIG. 6, in the embodiment shown in FIGS. 1 to 3, one or both of the elongated piezoelectric ceramics 1, 2 are divided into two parts and arranged in the cross shape. The longitudinal vibration axes of one piezoelectric ceramic 1 and the other piezoelectric ceramic 2 intersect at the center of the rectangular diaphragm 3, and both ends of each ceramic are located at each corner of the diaphragm 3. 2 is equally divided at the center.
この場合、振動板3の片面側に配置した複分割
圧電セラミツク1は互いに同一振動モード(伸縮
モード)を示し、他の片面側に配置した複分割圧
電セラミツク2も上記圧電セラミツク1と同方向
で且つ互いに同一振動モードを示す。即ち、一方
の圧電セラミツク1が伸びを生じた時、同時に他
方の圧電セラミツク2も伸びを生じ、逆に一方が
縮みを生じた時、他方も縮みを生ずる構成とす
る。 In this case, the multi-segmented piezoelectric ceramics 1 placed on one side of the diaphragm 3 exhibit the same vibration mode (expansion/contraction mode), and the multi-segmented piezoelectric ceramics 2 placed on the other side also exhibit the same vibration mode as the piezoelectric ceramic 1. Moreover, they exhibit the same vibration mode. That is, when one piezoelectric ceramic 1 expands, the other piezoelectric ceramic 2 also expands, and conversely, when one of the piezoelectric ceramics 1 contracts, the other also contracts.
又他の実施例として、第7図乃至第11図に示
すように、第1、第2実施例で示した長さ振動方
向が交叉するように配置された長さ振動圧電セラ
ミツクの組を振動板3の両面において二組形成す
る。 As another example, as shown in FIGS. 7 to 11, a set of length-vibrating piezoelectric ceramics arranged so that the length-vibration directions shown in the first and second embodiments intersect is vibrated. Two sets are formed on both sides of the plate 3.
即ち、振動板3の片面側の両対角線上に長さ振
動モードが互いに逆方向となる一対の圧電セラミ
ツク1a,1b(一方1aが伸びを生じた時、他
方1bは縮みを生じ、一方1aが縮みを生じた
時、他方1bが伸びを生ずる)を長さ振動方向が
交叉するように配置すると共に、振動板3の他の
片面側の両対角線上に長さ振動モードが互いに逆
方向となる一対の圧電セラミツク2a,2bを長
さ振動方向が交叉するように配置し、振動板3の
片面側の一方の対角線上に配置された圧電セラミ
ツク1aが伸びを生じた時、これに対応する他の
片面側の一方の対角線上に配置された圧電セラミ
ツク2aが縮みを生じ、又振動板3の片面側の他
方の対角線上に配置された圧電セラミツク1bが
縮みを生じた時、これに対応する他の片面側の他
方の対角線上に配置された圧電セラミツク2bが
伸びを生じるように組合せ配置する。 That is, a pair of piezoelectric ceramics 1a and 1b whose length vibration modes are in opposite directions are placed on both diagonals on one side of the diaphragm 3 (when one 1a expands, the other 1b contracts, and one 1a When contraction occurs, the other side 1b expands) are arranged so that their length vibration directions intersect, and the length vibration modes are in opposite directions on both diagonals on the other side of the diaphragm 3. A pair of piezoelectric ceramics 2a and 2b are arranged so that their longitudinal vibration directions intersect, and when the piezoelectric ceramic 1a arranged on one diagonal on one side of the diaphragm 3 expands, the other When the piezoelectric ceramic 2a arranged on one diagonal line on one side of the diaphragm 3 shrinks, and the piezoelectric ceramic 1b arranged on the other diagonal line on one side of the diaphragm 3 shrinks, the The piezoelectric ceramics 2b disposed on the other diagonal on the other side are arranged in combination so as to cause elongation.
上記によつても、振動板3に第5図で説明した
と同様の捩れ振動をもたらす。 The above also causes torsional vibration in the diaphragm 3 similar to that explained in FIG. 5.
尚、理解を助けるため第8図,第9図において
は圧電セラミツク1a,1bと2a,2bの配置
を夫々同一方向から平面視して示した。即ち、第
9図は第8図と同一方向から見て、振動板3の背
面側にある圧電セラミツク2a,2bを仮想線で
示した。従つて、圧電セラミツク1aと2aが一
方の同一対角線上で対向し、圧電セラミツク1b
と2bが他方の同一対角線上で対向した上記説明
の配置状態を示している。 8 and 9, the arrangement of the piezoelectric ceramics 1a, 1b and 2a, 2b is shown as viewed from the same direction, respectively. That is, FIG. 9 shows piezoelectric ceramics 2a and 2b on the back side of the diaphragm 3 with imaginary lines when viewed from the same direction as FIG. 8. Therefore, piezoelectric ceramics 1a and 2a face each other on the same diagonal line, and piezoelectric ceramic 1b
2b and 2b face each other on the same diagonal as described above.
第8図乃至第9図は上記の如く配置した二組の
長さ振動圧電セラミツク1a,2bの組と1b,
2aの組とを夫々複分割圧電セラミツクで構成
し、第10図,第11図は振動板3の片面側に配
置した何れか一方の圧電セラミツク1bを複分割
圧電セラミツクとし、同様に他の片面側に配置し
た何れか一方の圧電セラミツク2aを複分割圧電
セラミツクとした場合を示す。 FIGS. 8 to 9 show two sets of length vibrating piezoelectric ceramics 1a, 2b and 1b, arranged as described above.
10 and 11, one of the piezoelectric ceramics 1b placed on one side of the diaphragm 3 is made of a multi-segment piezoelectric ceramic, and similarly the other one side is made of a multi-segment piezoelectric ceramic. A case is shown in which one of the piezoelectric ceramics 2a disposed on the side is a multi-divided piezoelectric ceramic.
尚、本発明は各実施例で示した各圧電セラミツ
ク1,2として前記の如く夫々複層構造にしたも
のを用いるか、又は振動板3を積層構造にして用
いる場合を含む。 It should be noted that the present invention includes cases in which the piezoelectric ceramics 1 and 2 shown in each embodiment have a multilayer structure as described above, or the diaphragm 3 has a laminated structure.
又、圧電セラミツクの外形は方形又は帯状の
他、円形、多角形等の採用が可能である。方形の
振動板を用いる場合、各長さ振動圧電セラミツク
は長さ振動軸線と対角線とが正確に一致すること
までも要求するものではない。 Furthermore, the outer shape of the piezoelectric ceramic may be rectangular or strip-shaped, as well as circular or polygonal. In the case of using a rectangular diaphragm, it is not required that the length vibration axis and the diagonal line of each length vibrating piezoelectric ceramic precisely coincide with each other.
発明の効果
前記の如く現在、工業上利用し得る圧電セラミ
ツク振動子として提供されているものは、基本的
には単なるベンデイング運動による厚み方向の振
動、又は長さ振動、或は径方向振動等の振動モー
ドに限られていたが、本発明は上記振動板の片面
側と他面側の両長さ振動圧電素子をその長さ振動
方向が交叉するように配置し、両長さ振動圧電素
子が振動板の片面側と他面側において同時に伸び
又は同時に縮みを生ずるように長さ振動させるこ
とにより、前記の如き異方向複屈曲性を具有さ
せ、振動子が厚み方向の一方に部分屈曲すると同
時に、厚み方向の他方に部分屈曲する、所謂捩れ
振動を生起させることができ、固有の捩れ振動モ
ードを有有する捩れ振動子を提供することができ
た。Effects of the Invention As mentioned above, piezoelectric ceramic vibrators that are currently available for industrial use basically generate vibrations in the thickness direction due to simple bending motion, or vibrations in the length direction or radial direction. Although it was limited to the vibration mode, the present invention arranges both length vibrating piezoelectric elements on one side and the other side of the diaphragm so that their length vibration directions intersect, and the both length vibrating piezoelectric elements By vibrating the length of the diaphragm so that one side and the other side of the diaphragm simultaneously expand or contract, the oscillator can be partially bent in one direction in the thickness direction and simultaneously , it was possible to generate so-called torsional vibration that is partially bent in the other direction in the thickness direction, and it was possible to provide a torsional vibrator having a unique torsional vibration mode.
本発明は上記捩れ振動子を振動板の片面側と他
面側に細長圧電素子等をその長さ振動方向が交叉
するように配置する単純な構成で形成でき、簡素
な積層構造にして確実な捩れ振動が得られる捩れ
振動子を提供でき、積層構造が単純であるから、
価格も廉価なる利点を有する。 The present invention can form the above-mentioned torsional vibrator with a simple structure in which elongated piezoelectric elements, etc. are arranged on one side and the other side of a diaphragm so that their lengths and vibration directions intersect. It is possible to provide a torsional oscillator that produces torsional vibration, and the laminated structure is simple.
It also has the advantage of being inexpensive.
又、本発明に係る捩れ振動子は上記の如く量産
を容易にし、且つ性能が安定であり工業上好適に
利用し得、例えば粘度検出素子、比重検知子等の
検出用振動子の駆動源として適性を有する捩れ振
動子を提供できる。 Furthermore, the torsional oscillator according to the present invention can be easily mass-produced as described above, has stable performance, and can be suitably used in industry, for example, as a drive source for detection oscillators such as viscosity detection elements and specific gravity detectors. It is possible to provide a torsional oscillator with suitable properties.
第1図乃至第3図は本発明に係る捩れ振動子の
第一実施例を示し、第1図は同捩れ振動子の斜視
図、第2図は同側面図、第3図は同平面図、第4
図Aは同振動子の並列接続状態を示す側面図、第
4図Bは同直列接続状態を示す側面図、第5図は
同振動子の捩れ振動モードを説明する斜視図、第
6図は第2実施例を示す捩れ振動子の平面図、第
7図乃至第9図は第3実施例を示し、第7図は捩
れ振動子側面図、第8図は同平面図、第9図は第
8図に対応する圧電セラミツクの配置を平面視し
て示す図、第10図,第11図は第4実施例を示
し、第10図は捩れ振動子平面図、第11図は第
10図に対応する圧電セラミツクの配置を平面視
して示す図である。
1,2……長さ振動圧電素子たる圧電セラミツ
ク、3……振動板。
1 to 3 show a first embodiment of the torsional oscillator according to the present invention, FIG. 1 is a perspective view of the torsional oscillator, FIG. 2 is a side view, and FIG. 3 is a plan view. , 4th
Figure A is a side view showing the parallel connection state of the same vibrator, Figure 4B is a side view showing the same series connection state, Figure 5 is a perspective view illustrating the torsional vibration mode of the same vibrator, and Figure 6 is 7 to 9 show the third embodiment, FIG. 7 is a side view of the torsional oscillator, FIG. 8 is a plan view of the same, and FIG. FIG. 8 is a plan view showing the arrangement of piezoelectric ceramics, FIGS. 10 and 11 show the fourth embodiment, FIG. 10 is a plan view of the torsional vibrator, and FIG. FIG. 3 is a plan view showing the arrangement of piezoelectric ceramics corresponding to the above. 1, 2... Piezoelectric ceramic which is a length vibrating piezoelectric element, 3... Vibration plate.
Claims (1)
層して成る振動子であつて、振動板の片面側と他
面側の両長さ振動圧電素子をその長さ振動方向が
交叉するように配置し、両長さ振動圧電素子が振
動板の片面側と他面側において同時に伸び又は同
時に縮みを生ずるように長さ振動させ、上記振動
板の捩れ振動を得る構成としたことを特徴とする
捩れ振動子。1 A vibrator consisting of laminated layers with a diaphragm interposed between length-vibrating piezoelectric elements, in which both the length-vibrating piezoelectric elements on one side and the other side of the diaphragm are arranged so that their length-vibrating directions intersect. The vibrating piezoelectric element is vibrated in length so as to cause simultaneous expansion or contraction on one side and the other side of the diaphragm, thereby obtaining torsional vibration of the diaphragm. A torsional oscillator.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP29959886A JPS63151298A (en) | 1986-12-16 | 1986-12-16 | Twisting resonator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP29959886A JPS63151298A (en) | 1986-12-16 | 1986-12-16 | Twisting resonator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63151298A JPS63151298A (en) | 1988-06-23 |
| JPH0429280B2 true JPH0429280B2 (en) | 1992-05-18 |
Family
ID=17874707
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP29959886A Granted JPS63151298A (en) | 1986-12-16 | 1986-12-16 | Twisting resonator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS63151298A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100610181B1 (en) | 2004-10-27 | 2006-08-09 | 경북대학교 산학협력단 | Microphones in Implantable Hearing Aids |
-
1986
- 1986-12-16 JP JP29959886A patent/JPS63151298A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63151298A (en) | 1988-06-23 |
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| LAPS | Cancellation because of no payment of annual fees |