JPH0376281A - Piezoelectric element and polarization thereof - Google Patents
Piezoelectric element and polarization thereofInfo
- Publication number
- JPH0376281A JPH0376281A JP1212482A JP21248289A JPH0376281A JP H0376281 A JPH0376281 A JP H0376281A JP 1212482 A JP1212482 A JP 1212482A JP 21248289 A JP21248289 A JP 21248289A JP H0376281 A JPH0376281 A JP H0376281A
- Authority
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- Japan
- Prior art keywords
- piezoelectric element
- thin plate
- electrodes
- polarization
- lower surfaces
- 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.)
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Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は圧電素子の分極方法およびその方法により製造
した圧電素子に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a method for polarizing a piezoelectric element and a piezoelectric element manufactured by the method.
より詳しくは、本発明は、超音波距離センサー圧電アク
チュエータ、圧電モータ等に使用する圧電素子の分極方
法に関する。More specifically, the present invention relates to a method for polarizing piezoelectric elements used in ultrasonic distance sensor piezoelectric actuators, piezoelectric motors, and the like.
ある種の結晶に電界を加えると歪が発生する現象は、逆
圧電効果と呼ばれており、この現象を利用した圧電素子
が広く使われている。このような圧電素子は電界を加え
ることにより直接に歪が得られるため、構造的に簡単で
精密な制御が行われる特徴がある。The phenomenon in which strain occurs when an electric field is applied to a certain type of crystal is called the inverse piezoelectric effect, and piezoelectric elements that take advantage of this phenomenon are widely used. Since such a piezoelectric element can directly obtain strain by applying an electric field, it is characterized by a simple structure and precise control.
しかし、逆圧電効果によって発生する歪は小さく、この
ような圧電素子の変位を大きく取るためには薄板状の圧
電材料を多数枚積層した構造とすることが普通である。However, the strain caused by the inverse piezoelectric effect is small, and in order to obtain a large displacement of such a piezoelectric element, it is common to use a structure in which a large number of thin plate-shaped piezoelectric materials are laminated.
積層する圧電材料の各素子としては、水晶、ロッシェル
塩、チタン酸バリウム、チタン酸ジルコン酸鉛磁器、P
CM圧電磁器等のセラミックスや、ある種の強誘電ポリ
マーが用いられている。The piezoelectric material elements to be laminated include crystal, Rochelle salt, barium titanate, lead zirconate titanate porcelain, and P.
Ceramics such as CM piezoelectric ceramics and certain ferroelectric polymers are used.
強誘電体の等方性で圧電性のない多結晶焼結体(セラミ
ックス)や薄膜に高電界を印加し、それらの自発分極の
方向をある程度そろえる(分極する)ことにより、圧電
体とすることができる(ポーリング)。By applying a high electric field to a polycrystalline sintered body (ceramics) or thin film that is isotropic and has no piezoelectric properties of a ferroelectric substance, and aligning the direction of their spontaneous polarization to some extent (polarization), it becomes a piezoelectric substance. (polling).
従来、このような圧電素子を分極する方法として行われ
ていたのは、例えばねじり振動素子について言えば、円
板状をした圧電素子においては、セラミックスを焼結し
てドーナツ形状とし、このセラミックスを、例えば4等
分して扇形とし、各扇形の端面に電極を形成して扇形に
ついて分極を行い、分極した後、電極を削除し、4つの
扇形を再度接着をして再度ドーナツ状の圧電素子を形成
している。Conventionally, the method used to polarize such piezoelectric elements is, for example, in the case of torsional vibration elements, in the case of disk-shaped piezoelectric elements, ceramics are sintered into a donut shape and this ceramic is polarized. For example, divide it into quarters to form a fan shape, form an electrode on the end face of each fan shape, polarize the fan shape, remove the electrode after polarization, re-glue the four fan shapes, and create a doughnut-shaped piezoelectric element again. is formed.
このようにして、ねじり振動素子を作っており、また同
様にすべり振動用圧電素子においては、例えば四角形状
に形成した薄板状にセラミックスを焼結し、その分極方
向両端面に電極を形成し、分極をした後、電極を削除し
、分極形成用の電極面を削除して、それと直交する方向
に電極面を形成して、すべり振動用素子を作っている。In this way, a torsional vibration element is made, and similarly, in a piezoelectric element for shear vibration, ceramics are sintered into a thin plate shape formed into a rectangular shape, and electrodes are formed on both end faces in the polarization direction. After polarization, the electrodes are removed, the electrode surface for polarization formation is removed, and an electrode surface is formed in a direction perpendicular to the electrode surface to form a shear vibration element.
しかしながら、このような方法による場合には、ねじり
圧電素子においては、圧電素子自体を接着し結合してい
るために圧電素子の強度が弱いという問題があり、また
切断、接着等複雑な工程を経るため、コスト高となって
いる。また、すべり圧電素子においても、同様にコスト
高になっている。However, when using this method, there is a problem that the strength of the piezoelectric element is weak because the piezoelectric element itself is bonded and bonded, and it also requires complicated processes such as cutting and bonding. Therefore, the cost is high. Furthermore, the cost of the sliding piezoelectric element is similarly high.
本発明は上述するような従来の技術に付随する問題点を
解決して、圧電素子の分極に要するコストを低減でき、
強度の大きい圧電素子を、しかも、その品質を向上して
製作できる方法を提供することを目的とする。The present invention solves the problems associated with the conventional techniques as described above, reduces the cost required for polarization of piezoelectric elements,
It is an object of the present invention to provide a method for manufacturing a piezoelectric element with high strength and improved quality.
本発明においては圧電素子材料を薄板に形成し、該薄板
の上下両面に、分極方向に独立した複数の電極をそれぞ
れ形成し、分極方向に偏倚した上下両面の電極対間で高
電圧を印加して分極し、上記分極操作を複数の電極対間
で繰返して薄板全体を分極することを特徴とする圧電素
子の分極方法により上記の目的を達成する。In the present invention, the piezoelectric element material is formed into a thin plate, a plurality of electrodes are formed on the upper and lower surfaces of the thin plate, each independent in the polarization direction, and a high voltage is applied between the pairs of electrodes on the upper and lower surfaces that are biased in the polarization direction. The above object is achieved by a method of polarizing a piezoelectric element, which is characterized in that the entire thin plate is polarized by repeating the above polarization operation between a plurality of electrode pairs.
本発明をねじり圧電素子の分極方法に適用するに際して
は、前記圧電素子材料を円形薄板に形成し、該円形薄板
の上下両面に円形薄板の中心まわりに複数の扇形電極を
形成することを特徴とする。When the present invention is applied to a method for polarizing a torsion piezoelectric element, the piezoelectric element material is formed into a circular thin plate, and a plurality of sector-shaped electrodes are formed around the center of the circular thin plate on both upper and lower surfaces of the circular thin plate. do.
また、本発明の圧電素子の分極方法を、すべり圧電素子
の分極方法に適用する際には、前記圧電素子材料を四辺
形薄板に形成し、該四辺形薄板の上下両面に帯状の複数
の電極を形成することを特徴とする。Furthermore, when applying the piezoelectric element polarization method of the present invention to a sliding piezoelectric element polarization method, the piezoelectric element material is formed into a rectangular thin plate, and a plurality of band-shaped electrodes are formed on the upper and lower surfaces of the quadrilateral thin plate. It is characterized by the formation of
本発明においては、薄板状に形成した圧電素子の上下面
を厚み方向に見た場合に、大きくずらすことにより、偏
倚させて画電極界に高電圧をかけ分極する。In the present invention, the upper and lower surfaces of a piezoelectric element formed in a thin plate shape are shifted significantly when viewed in the thickness direction, thereby biasing the piezoelectric element and polarizing the piezoelectric element by applying a high voltage to the field of the picture electrode.
これにより厳密に言えば、分極方向が厚さ方向と直角方
向(すなわち、薄板の面と平行)ではなく、薄板の面に
対して僅かに傾いた状態とはなるが、電極対の選定を十
分に注意、例えば、分極傾斜角を15度以下とすること
により、暑さ方向変形成分が極めて小さくなり、この傾
斜による影響は殆ど無視することができる。Strictly speaking, this means that the polarization direction is not perpendicular to the thickness direction (i.e., parallel to the plane of the thin plate), but is slightly inclined to the plane of the thin plate, but it is important to carefully select the electrode pair. Note that, for example, by setting the polarization inclination angle to 15 degrees or less, the heat direction deformation component becomes extremely small, and the influence of this inclination can be almost ignored.
また、縦振動圧電素子の枚数を増加して所要縦振動の値
を大きくすることにより、このような傾斜の影響という
ものは殆ど無視することができる状態となる。In addition, by increasing the number of longitudinally vibrating piezoelectric elements and increasing the required value of longitudinal vibration, the effect of such inclination can be almost ignored.
本発明によれば、薄板状に形成した圧電素子をそのまま
分極することができ、切断、再接着等の工程が不要であ
り、非常に生産コストが低減できる。According to the present invention, a piezoelectric element formed in a thin plate shape can be polarized as it is, and processes such as cutting and re-adhesion are not necessary, and production costs can be significantly reduced.
ま′た、切断、再接着等の工程を要しないために圧電素
子の強度も極めて増加し、また、出来上がった圧電素子
の品質も均質なものとすることができる。Furthermore, since processes such as cutting and re-bonding are not required, the strength of the piezoelectric element is greatly increased, and the quality of the finished piezoelectric element can be made uniform.
以下、本発明の実施例を図示した図面を参照し、本発明
をより詳細に説明する。Hereinafter, the present invention will be explained in more detail with reference to the drawings, which illustrate embodiments of the invention.
最初に、ねじり振動用圧電素子を本発明により分極する
方法を実施例につき説明する。First, a method for polarizing a piezoelectric element for torsional vibration according to the present invention will be explained using examples.
この実施例においては、セラミックス1を第1図に示す
ようにドーナツ形状に焼結する。この場合のセラミック
ス1の厚さは出来るだけ薄くしている。第1図に示すよ
うに薄板状ドーナツ形状に形成したセラミックス1の上
下面(第1図は上面が見えている)を、このドーナツ状
円板の中心Pを中心とする扇形状に、多数の区画に区分
する。In this example, the ceramic 1 is sintered into a donut shape as shown in FIG. The thickness of the ceramic 1 in this case is made as thin as possible. As shown in Fig. 1, the top and bottom surfaces of the ceramic 1 formed into a thin donut shape (the top surface is visible in Fig. 1) are arranged in a fan shape centered on the center P of this donut-shaped disk. Divide into sections.
これら区分した多数の区画間には僅かな間隙ICを開け
ており、各区画に蒸着により電極1aを形成する。同様
に下面にも多数の電極1bを形成する。A small gap IC is provided between a large number of these divided sections, and an electrode 1a is formed in each section by vapor deposition. Similarly, a large number of electrodes 1b are formed on the lower surface.
次に第3図に示すように、ドーナツ板状の圧電素子の上
下面の電極1a、lbの上下位置をずらした状態とする
。すなわち、第3図においては、上方の電極■と下方の
電極■とは3ピッチ分ずれている。Next, as shown in FIG. 3, the vertical positions of the electrodes 1a and lb on the top and bottom surfaces of the donut plate-shaped piezoelectric element are shifted. That is, in FIG. 3, the upper electrode (2) and the lower electrode (2) are shifted by 3 pitches.
このように、ずらした状態で、上下の電極1as1b間
に高電圧を印加する。In this way, a high voltage is applied between the upper and lower electrodes 1as1b in the shifted state.
これにより、第3図に示すように、圧電素子内には薄板
の面に対して、僅かに傾斜した方向ではあるが、上下の
電極■の間で分極される。As a result, as shown in FIG. 3, the inside of the piezoelectric element is polarized between the upper and lower electrodes (2), albeit in a direction slightly inclined with respect to the surface of the thin plate.
この分極操作を、次に■■の電極間、■■の電極間にて
行う。なお、この分極操作の間に、他所の電極との間に
分極の操作の妨げとならない場合には、複数の電極間に
おける分極を同時に行ってもよい。This polarization operation is then performed between the electrodes (■■) and between the electrodes (■■). Note that during this polarization operation, polarization between a plurality of electrodes may be performed simultaneously if the polarization operation with other electrodes is not hindered.
上述のように、本発明においては、分極操作を行う際に
、圧電素子を切断せず、丸のままで分極操作を行ってい
る。As described above, in the present invention, when polarizing the piezoelectric element, the piezoelectric element is not cut but is polarized as it is.
このようにして分極操作を行った圧電素子の上面と下面
とには、圧電素子駆動用の電圧を印加するための電極を
形成する。このために、上述のように扇形に形成した小
電極相互を間通する。この方法として上下面の電極の上
に連続した1枚の電極を接着してもよい。または、互い
に独立している扇形の小電極を削除し、薄板の上下面全
域に金属を蒸着する等して薄膜の電極を形成してでもよ
い。Electrodes for applying a voltage for driving the piezoelectric element are formed on the upper and lower surfaces of the piezoelectric element which has been polarized in this manner. For this purpose, the small electrodes formed in a fan shape as described above are passed through each other. As this method, one continuous electrode may be bonded onto the electrodes on the upper and lower surfaces. Alternatively, a thin film electrode may be formed by omitting the fan-shaped small electrodes that are independent from each other and depositing metal over the entire upper and lower surfaces of the thin plate.
以上のようにすることにより、本発明に係るねじり振動
用圧電素子が得られる。By doing as described above, a piezoelectric element for torsional vibration according to the present invention can be obtained.
次に、第4図、第5図、第6図を参照して、すべり振動
用圧電素子の分極に本発明方法を適用する例を説明する
。Next, an example in which the method of the present invention is applied to polarization of a piezoelectric element for sliding vibration will be described with reference to FIGS. 4, 5, and 6.
この場合には、上述と同様であるが、円形ではなく圧電
素子11は長方形状の薄板状に形成する。In this case, the piezoelectric element 11 is formed in the same manner as described above, but instead of being circular, the piezoelectric element 11 is formed in a rectangular thin plate shape.
この薄板状の圧電素子11に帯状に多数の電極11a、
llbを独立した状態、すなわち、隣接する電極間では
導通しないようにして、多数の帯状の電極11a、ll
bを上下の面に第5図のように形成する。次いで、上下
面の電極を前述と同様にして、そのピッチをずらした状
態で分極し、これにより、全体に見れば面に対して僅か
に傾斜した方向に分極する。This thin plate-like piezoelectric element 11 has a large number of electrodes 11a in a band shape,
A large number of strip-shaped electrodes 11a, 11a, 11a, 11a, 11a, 11a, 11a, 11a, 11a, 11a, 11a, 11a, 11a, llb are made independent, that is, there is no conduction between adjacent electrodes.
b are formed on the upper and lower surfaces as shown in FIG. Next, the electrodes on the upper and lower surfaces are polarized in the same manner as described above, with their pitches shifted, and as a result, the electrodes are polarized in a direction slightly inclined with respect to the surface when viewed as a whole.
このようにして、形成した圧電素子の駆動用電圧を印加
するための電極形成は前述のねじり振動用圧電素子と同
様にする。Formation of electrodes for applying a driving voltage to the piezoelectric element thus formed is performed in the same manner as in the piezoelectric element for torsional vibration described above.
〔1発明の効果〕
本発明によれば、薄板状に形成した圧電素子の上下面を
厚み方向に見た場合に、大きくずらすことにより、偏倚
させて両電極界に高電圧をかけ分極する。[1] Effects of the Invention According to the present invention, the upper and lower surfaces of a piezoelectric element formed in a thin plate shape are significantly shifted when viewed in the thickness direction, thereby being biased and polarized by applying a high voltage to both electrode fields.
従って、本発明によれば、薄板状に形成した圧電素子を
そのまま分極することができ、切断、再接着等の工程が
不要であり、非常に生産コストが低減できる。また、切
断、再接着等の工程を要しないために圧電素子の強度も
非常に増加し、また、出来上がった圧電素子の品質も均
質なものとすることができる。Therefore, according to the present invention, a piezoelectric element formed in a thin plate shape can be polarized as it is, and processes such as cutting and re-adhesion are not necessary, and production costs can be significantly reduced. Further, since processes such as cutting and re-adhesion are not required, the strength of the piezoelectric element is greatly increased, and the quality of the finished piezoelectric element can be made uniform.
第1図から第3図は、本発明に係るねじり振動用圧電素
子の分極方法を説明する図であり、第1図は平面図、第
2図も平面図、第3図は概略的に示した側面図、第4図
から第6図は本発明に係るすべり振動用圧電素子の分極
方法を示す図であり、第4図および第5図は平面図、第
6図は概略的に示した側面図である。
1.11・・・圧電素子、
la、lb、lla、 11b−・・電極。
図面の浄書(内容に変更なし)
第1図1 to 3 are diagrams for explaining the polarization method of the piezoelectric element for torsional vibration according to the present invention, in which FIG. 1 is a plan view, FIG. 2 is also a plan view, and FIG. 3 is a schematic diagram. FIGS. 4 to 6 are diagrams showing a polarization method of the piezoelectric element for sliding vibration according to the present invention, FIGS. 4 and 5 are plan views, and FIG. 6 is a schematic diagram. FIG. 1.11...Piezoelectric element, la, lb, lla, 11b-...electrode. Engraving of the drawing (no changes to the content) Figure 1
Claims (5)
、分極方向に独立した複数の電極をそれぞれ形成し、分
極方向に偏倚した上下調面の電極対間で高電圧を印加し
て分極し、上記分極操作を複数の電極対間で繰返して薄
板全体を分極することを特徴とする圧電素子の分極方法
。1. A piezoelectric element material is formed into a thin plate, a plurality of electrodes are formed independently in the polarization direction on the upper and lower surfaces of the thin plate, and a high voltage is applied between the pairs of electrodes with upper and lower tone planes biased in the polarization direction to polarize. A method for polarizing a piezoelectric element, characterized in that the above polarization operation is repeated between a plurality of electrode pairs to polarize the entire thin plate.
素子材料を円形薄板に形成し、該円形薄板の上下両面に
円形薄板の中心まわりに複数の扇形電極を形成すること
を特徴とするねじり圧電素子の分極方法。2. 2. The method for polarizing a piezoelectric element according to claim 1, wherein the piezoelectric element material is formed into a circular thin plate, and a plurality of sector-shaped electrodes are formed around the center of the circular thin plate on both upper and lower surfaces of the circular thin plate. polarization method.
素子材料を四辺形薄板に形成し、該四辺形薄板の上下調
面に帯状の複数の電極を形成することを特徴とするすべ
り圧電素子の分極方法。3. A method for polarizing a piezoelectric element according to claim 1, characterized in that the piezoelectric element material is formed into a rectangular thin plate, and a plurality of band-shaped electrodes are formed on the upper and lower tone surfaces of the rectangular thin plate. Method.
板に形成した多数の電極を取り除き、該薄板の上下面全
域に蒸着により電極を形成したことを特徴とする圧電素
子。4. A piezoelectric element characterized in that a large number of electrodes formed on a thin plate polarized by the method according to any one of claims 1 to 3 are removed, and electrodes are formed on the entire upper and lower surfaces of the thin plate by vapor deposition.
板に形成した多数の独立した電極間を導通するよう、薄
板の上下面にそれぞれ電極板を接着したことを特徴とす
る圧電素子。5. 4. A piezoelectric element characterized in that electrode plates are respectively bonded to the upper and lower surfaces of the thin plate so as to establish conduction between a large number of independent electrodes formed on the thin plate polarized by the method according to any one of claims 1 to 3.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1212482A JPH0376281A (en) | 1989-08-18 | 1989-08-18 | Piezoelectric element and polarization thereof |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1212482A JPH0376281A (en) | 1989-08-18 | 1989-08-18 | Piezoelectric element and polarization thereof |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0376281A true JPH0376281A (en) | 1991-04-02 |
Family
ID=16623381
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1212482A Pending JPH0376281A (en) | 1989-08-18 | 1989-08-18 | Piezoelectric element and polarization thereof |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0376281A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR20180047277A (en) * | 2016-10-31 | 2018-05-10 | 숭실대학교산학협력단 | Piezoelectric transducer for multiple vibration modes and level switch sensor comprising the same |
| KR20180067074A (en) * | 2016-12-12 | 2018-06-20 | 숭실대학교산학협력단 | Level switch sensor for measuring powder level |
-
1989
- 1989-08-18 JP JP1212482A patent/JPH0376281A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR20180047277A (en) * | 2016-10-31 | 2018-05-10 | 숭실대학교산학협력단 | Piezoelectric transducer for multiple vibration modes and level switch sensor comprising the same |
| KR20180067074A (en) * | 2016-12-12 | 2018-06-20 | 숭실대학교산학협력단 | Level switch sensor for measuring powder level |
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