JPH072229B2 - Piezoelectric elliptical motion oscillator - Google Patents
Piezoelectric elliptical motion oscillatorInfo
- Publication number
- JPH072229B2 JPH072229B2 JP63185414A JP18541488A JPH072229B2 JP H072229 B2 JPH072229 B2 JP H072229B2 JP 63185414 A JP63185414 A JP 63185414A JP 18541488 A JP18541488 A JP 18541488A JP H072229 B2 JPH072229 B2 JP H072229B2
- Authority
- JP
- Japan
- Prior art keywords
- piezoelectric
- boundary surface
- elliptical motion
- disk
- divided
- 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 - Lifetime
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- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
- Apparatuses For Generation Of Mechanical Vibrations (AREA)
- General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は電子機器などに用いられる小型モータに関し、
特にローター直径の小さい小型の超音波モータに用いら
れる圧電楕円運動振動子に関するものである。TECHNICAL FIELD The present invention relates to a small motor used in electronic equipment,
In particular, it relates to a piezoelectric elliptical motion oscillator used for a small ultrasonic motor having a small rotor diameter.
(従来の技術) 一般に、超音波モータは従来の電磁モータと比較して、
低回転で高いトルクが得られること、停止保持力を有す
ること、電磁ノイズが少ないことなどの利点を有してお
り、カメラのオートフォーカス用や自動車用パワーモー
タなどに使用されている。第9図は小型超音波モータに
使用されている従来の圧電楕円運動振動子即ち各柱振動
子100の構造を示す概略図であり、略正方形断面を有す
る金属角柱120の隣り合う二つの面に、各々電極が形成
され、厚さ方向分極された圧電セラミックス薄板121a,1
21bが接着されている。(Prior Art) Generally, an ultrasonic motor is
It has advantages such as high torque at low rotation, stop holding force, and little electromagnetic noise, and is used for autofocus of cameras and power motors for automobiles. FIG. 9 is a schematic diagram showing the structure of a conventional piezoelectric elliptical motion oscillator used in a small ultrasonic motor, that is, each column oscillator 100. Two adjacent faces of a metal prism 120 having a substantially square cross section are shown. , Piezoelectric ceramic thin plates 121a, 1 each having electrodes formed and polarized in the thickness direction
21b is glued.
圧電セラミックス薄板121a,121bの表面電極からリード
端子122a,122bが引き出され、金属角柱120から共通アー
ス端子123が引き出されている。金属角柱120の断面形状
が略正方形であるので金属角柱120は互いに直角方向に
ほぼ同じ共振周波数で屈曲振動する。The lead terminals 122a and 122b are drawn out from the surface electrodes of the piezoelectric ceramic thin plates 121a and 121b, and the common ground terminal 123 is drawn out from the metal prism 120. Since the cross-sectional shape of the metal prism 120 is substantially square, the metal prism 120 flexurally vibrates in a direction orthogonal to each other at substantially the same resonance frequency.
従って、リード端子122a−123および122b−123にそれぞ
れ周波数が共振周波数に等しく、位相が90°異なる交流
電圧を印加すると金属角柱120の両端部は円振動あるい
は楕円振動する。第10図は第9図に示した角柱振動子10
0を用ぢた超音波モータの構成例を示す図である。角柱
振動子100の両端部に円板124a,124bが装着され、さらに
角柱振動子100の振動の節の位置に支持ピン125a,125bが
形成され、角柱振動子100は支持ピン125a,125bにより安
定に支持されている。角柱振動子100の両端部に設けら
れた円板124a,124bは、回転自在に回転軸に支持された
カップ状回転ローラー126a,126bの空洞部に挿入され、
空洞部内壁に加圧接触されている。Therefore, when AC voltages having frequencies equal to the resonance frequency and phases different by 90 ° are applied to the lead terminals 122a-123 and 122b-123, both ends of the metal prism 120 vibrate circularly or elliptically. FIG. 10 shows the prismatic vibrator 10 shown in FIG.
It is a figure which shows the structural example of the ultrasonic motor which used 0. Discs 124a and 124b are attached to both ends of the prismatic oscillator 100, and support pins 125a and 125b are formed at the vibration nodes of the prismatic oscillator 100. The prismatic oscillator 100 is stabilized by the support pins 125a and 125b. Supported by. The discs 124a, 124b provided at both ends of the prismatic vibrator 100 are inserted into the cavities of the cup-shaped rotating rollers 126a, 126b rotatably supported by the rotating shaft,
It is in pressure contact with the inner wall of the cavity.
従って、角柱振動子100の端部が円振動あるいは楕円振
動した場合にカップ状回転ローラー126a,126bを回転さ
せる。Therefore, when the end of the prismatic vibrator 100 vibrates circularly or elliptically, the cup-shaped rotating rollers 126a and 126b are rotated.
(発明が解決しようとする課題) しかしながら、第9図に示すような従来の角柱状楕円運
動振動子においては、振動子が正方形断面の角柱である
ため、互いに直角な方向の屈曲モードの共振周波数を精
度良く一致させるためには、角柱の加工精度を厳しくお
さえなければならない。(Problems to be Solved by the Invention) However, in the conventional prismatic elliptical motion oscillator as shown in FIG. 9, since the oscillator is a prism having a square cross section, the resonance frequencies of bending modes in directions orthogonal to each other. In order to accurately match with each other, it is necessary to strictly control the machining accuracy of the prism.
また圧電セラミックス薄板を金属角柱に接着するときの
接着状態のばらつきが大きい。さらに第10図に示したよ
うな構造の超音波モータを構成する場合においては、カ
ップ状回転ローラーとの接触状態を良くするために金属
角柱の両端部に円板などを付加する必要があるという欠
点を有していた。そこで、本発明の技術課題は、円板等
の接触部材を必要とせず、又加工精度にとらわれず組み
立てが容易な圧電楕円運動振動子を提供することにあ
る。Further, when the piezoelectric ceramic thin plate is bonded to the metal prism, the bonding state varies widely. Further, in the case of constructing an ultrasonic motor having a structure as shown in FIG. 10, it is necessary to add a disc or the like to both ends of the metal prism in order to improve the contact state with the cup-shaped rotating roller. It had drawbacks. Therefore, a technical object of the present invention is to provide a piezoelectric elliptical motion oscillator that does not require a contact member such as a disk and is easy to assemble without being restricted by processing accuracy.
(課題を解決するための手段) 本発明によれば、圧電セラミックス円柱の外周面に、長
さ方向と平行に所定の間隔をおいて、複数の電極対を設
け、前記電極対の少なくとも一つに直流電圧を印加し
て、前記圧電セラミックス円柱に長さ方向と直角な方向
の分極処理を施し、前記電極対のうちの2つに互いに異
なる位相を有する交流電圧を印加して、前記圧電セラミ
ックス円柱の両端部に円を含む楕円運動を励起可能とし
たことを特徴とする圧電楕円運動振動子が得られる。(Means for Solving the Problems) According to the present invention, a plurality of electrode pairs are provided on the outer peripheral surface of the piezoelectric ceramic cylinder at predetermined intervals in parallel with the length direction, and at least one of the electrode pairs is provided. DC voltage is applied to the piezoelectric ceramics column to perform polarization treatment in a direction perpendicular to the longitudinal direction, and AC voltages having different phases are applied to two of the electrode pairs to obtain the piezoelectric ceramics. A piezoelectric elliptical motion oscillator is obtained which is capable of exciting an elliptical motion including a circle at both ends of a cylinder.
ここで、本発明においては、これらの分割電極対に印加
される交流電流はそれぞれ90°位相差を有することが望
ましい。Here, in the present invention, it is desirable that the alternating currents applied to these divided electrode pairs have a 90 ° phase difference.
本発明によれば、第1及び第2の圧電セラミック円板
と、これらの第1及び第2の圧電セラミック円板の一端
間に挟まれた第1の金属円柱と、これらの第1及び第2
の圧電セラミック円板の他端に夫々設けられた第2及び
第3の金属円柱とを有する圧電楕円運動振動子であっ
て、前記第1の圧電セラミック円板は、この第1の圧電
セラミック円板の中心軸に沿う方向で2分割する第1の
境界面を境にして厚さ方向に互いに逆向きとなるように
分極されており、前記第2の圧電セラミック円板は、該
圧電セラミック円板の中心軸に沿う方向で2分割し且つ
前記第1の境界面と所定角度で傾斜した第2の境界面を
境にして厚さ方向に互いに逆向きとなるように分極され
ており、前記第1の金属円柱を共通アースとし、前記第
2及び第3の金属円柱に互いに異なる位相を有する交流
電圧を印加して、前記圧電楕円運動振動子の両端部に円
を含む楕円運動を励起可能としたことを特徴とする圧電
楕円運動振動子が得られる。According to the present invention, first and second piezoelectric ceramic discs, a first metal cylinder sandwiched between one ends of these first and second piezoelectric ceramic discs, and these first and second piezoelectric ceramic discs. Two
A piezoelectric elliptical motion oscillator having second and third metal cylinders respectively provided at the other end of the first piezoelectric ceramic disc, wherein the first piezoelectric ceramic disc is the first piezoelectric ceramic disc. The second piezoelectric ceramic discs are polarized so as to be opposite to each other in the thickness direction with a first boundary surface that is divided into two in the direction along the central axis of the plate as a boundary, and the second piezoelectric ceramic disc is the piezoelectric ceramic disc. The plate is divided into two along the central axis of the plate, and is polarized so as to be opposite to each other in the thickness direction with the second boundary surface inclined at a predetermined angle from the first boundary surface as a boundary. The first metal cylinder can be used as a common ground, and alternating voltages having different phases can be applied to the second and third metal cylinders to excite elliptical motion including circles at both ends of the piezoelectric elliptical motion oscillator. A piezoelectric elliptical motion oscillator characterized by It is.
本発明によれば、第1及び第2の円板状圧電振動子と、
これらの第1及び第2の円板状圧電振動子の一端間に挟
まれた第1の金属円柱と、これらの第1及び第2の円板
状圧電振動子の他端に夫々設けられた第2及び第3の金
属円柱とを有する圧電楕円運動振動子であって、前記第
1の円板状圧電振動子は、該第1の円板状圧電振動子の
中心軸に沿う方向で2分割する第1の境界面及び厚さ方
向で2分割する第2の境界面を境として厚さ方向に互い
に逆向きとなるように分極されており、前記第2の円板
状圧電振動子は、この第2の円板状圧電振動子の中心軸
に沿う方向で2分割され且つ前記第1の境界面と所定角
度で傾斜した第3の境界面及び且つ厚さ方向で2分割す
る第4の境界面を境にして厚さ方向に互いに逆向きとな
るように分極されており、前記第1,第2及び第3の金属
円柱を共通アースとし、前記第2及び第4の境界面に互
いの異なる位相の交流電圧を印加して、前記圧電楕円運
動振動子の両端部に円を含む楕円運動を励起可能とした
ことを特徴とする圧電楕円運動振動子が得られる。According to the present invention, the first and second disk-shaped piezoelectric vibrators,
A first metal cylinder sandwiched between one ends of the first and second disk-shaped piezoelectric vibrators and a first metal cylinder provided at the other ends of the first and second disk-shaped piezoelectric vibrators, respectively. A piezoelectric elliptical motion oscillator having a second and a third metal cylinder, wherein the first disk-shaped piezoelectric vibrator is 2 in a direction along a central axis of the first disk-shaped piezoelectric vibrator. Polarizations are made so as to be opposite to each other in the thickness direction with the first boundary surface to be divided and the second boundary surface divided into two in the thickness direction as boundaries, and the second disk-shaped piezoelectric vibrator is A third boundary surface which is divided into two parts in a direction along the central axis of the second disk-shaped piezoelectric vibrator and which is inclined at a predetermined angle with the first boundary surface, and a second part which is divided into two parts in the thickness direction. Are polarized so as to be opposite to each other in the thickness direction with the boundary surface of the first and second metal columns as a common ground. Then, by applying alternating voltages of different phases to the second and fourth boundary surfaces, it is possible to excite an elliptic motion including a circle at both ends of the piezoelectric elliptical motion oscillator. An elliptical motion oscillator is obtained.
ここで、本発明においては、圧電セラミックス円板の分
極境界線は互いに直角に交差するように配置されること
が望ましい。Here, in the present invention, it is desirable that the polarization boundary lines of the piezoelectric ceramic disk are arranged so as to intersect each other at right angles.
本発明によれば、第1及び第2の円筒状圧電振動子と、
この第1及び第2の円筒状圧電振動子の一端間に挟まれ
た第1の金属円筒と、この第1及び第2の円筒状圧電振
動子の他端に夫々設けられた第2及び第3の金属円柱と
を貫通部材により固着した圧電楕円運動振動子であっ
て、前記第1の円筒状圧電振動子は、この第1の円筒状
圧電振動子の中心軸に沿う方向で2分割する第1の境界
面及び厚さ方向で2分割する第2の境界面を境として厚
さ方向に互いに逆向きとなるように分極されており、前
記第2の円筒状圧電振動子は、この第2の円筒状圧電振
動子の中心軸に沿う方向で2分割され且つ前記第1の境
界面と所定角度で傾斜した第3の境界面及び厚さ方向で
2分割する第4の境界面を境にして厚さ方向に互いに逆
向きとなるように分極されており、前記第2及び第4の
境界面に夫々第1及び第2の中間端子板を有し、前記第
1,第2,及び第3の金属円筒を共通アースとし、前記端子
板に互いに異なる位相の交流電圧を印加して、前記圧電
楕円運動振動子の両端部に円を含む楕円運動を励起可能
としたことを特徴とする圧電楕円運動振動子が得られ
る。ここで、本発明においては、圧電セラミックス穴あ
き円板は、各々の分極境界線の方向は直角に交差するよ
うに配置されることが望ましい。According to the present invention, the first and second cylindrical piezoelectric vibrators,
A first metal cylinder sandwiched between one ends of the first and second cylindrical piezoelectric vibrators, and second and second cylinders provided at the other ends of the first and second cylindrical piezoelectric vibrators, respectively. 3 is a piezoelectric elliptical motion oscillator in which a metal cylinder of 3 is fixed by a penetrating member, and the first cylindrical piezoelectric oscillator is divided into two in a direction along the central axis of the first cylindrical piezoelectric oscillator. The second cylindrical piezoelectric vibrator is polarized so as to be opposite to each other in the thickness direction with the first boundary surface and the second boundary surface divided in two in the thickness direction as boundaries. A second boundary surface is divided into two in the direction along the central axis of the two cylindrical piezoelectric vibrators and a third boundary surface inclined at a predetermined angle from the first boundary surface and a fourth boundary surface divided into two in the thickness direction. And are polarized so as to be opposite to each other in the thickness direction, and the first and second boundary surfaces are respectively polarized. A second intermediate terminal plate, said first
It is possible to excite an elliptic motion including circles at both ends of the piezoelectric elliptical motion oscillator by applying alternating voltages of different phases to the terminal plate with the first, second, and third metal cylinders as a common ground. A piezoelectric elliptic motion oscillator characterized by the above is obtained. Here, in the present invention, it is desirable that the piezoelectric ceramic perforated discs are arranged so that the directions of the polarization boundary lines intersect each other at a right angle.
(作用) 本発明の作用について述べる。(Operation) The operation of the present invention will be described.
本発明の圧電楕円運動振動子は、円柱に円周方向を等分
する位置に複数対の分割電極を設けて、この電極対の直
流電圧を印加し、分極処理を施し、この分割電極対に少
くとも二対の交流電圧を印加すると、各電極は印加方向
に略垂直方向に屈曲振動を行う。これらの電極は交流電
圧印加方向が互いに交差するように形成して、0〜180
°の範囲内の位相差を有するように交流電圧を印加する
と、位相差に応じて、円柱振動子両端は円を含む楕円振
動を行う。The piezoelectric elliptical motion oscillator of the present invention is provided with a plurality of pairs of divided electrodes on a cylinder at positions that equally divide the circumferential direction, apply a DC voltage to the electrode pairs, and subject the divided electrodes to a polarization treatment. When at least two pairs of AC voltages are applied, each electrode vibrates in a direction substantially perpendicular to the applied direction. These electrodes are formed so that the AC voltage application directions cross each other, and
When an AC voltage is applied so as to have a phase difference within a range of °, both ends of the cylindrical vibrator perform elliptical vibration including a circle according to the phase difference.
本発明の圧電楕円運動振動子においては、複数の導体の
間に複数の圧電振動子を介在させてなり、この圧電振動
子の互いに分極境界面を交差させて構成したので、この
圧電振動子に位相差を有する交流電流を印加すると、圧
電楕円運動振動子の両端は円を含む楕円運動を行う。In the piezoelectric elliptical motion oscillator of the present invention, a plurality of piezoelectric oscillators are interposed between a plurality of conductors, and the polarization boundary surfaces of the piezoelectric oscillators are made to intersect with each other. When an alternating current having a phase difference is applied, both ends of the piezoelectric elliptical motion oscillator make an elliptical motion including a circle.
(実施例) 本発明の実施例を図面を参照して説明する。(Example) The Example of this invention is described with reference to drawings.
実施例1 本発明の実施例1について説明する。Example 1 Example 1 of the present invention will be described.
第1図は本発明の実施例1に係る圧電楕円運動振動子の
斜視図であり、圧電セラミックス円柱1の側面の円周方
向4等分の位置に、長さ方向と平行に電極2,3,4,5が形
成されている。一本の電極幅と電極のない部分の寸法比
はおよそ1:1となっている。第2図は圧電セラミックス
円柱断面図であり、分極方向と駆動電圧による歪みの発
生の状態の説明図である。第2図(a)は電極2,4をプ
ラス、電極3,5をマイナスとして、電圧を印加した場合
の分極の向きを示す図であり、分極の向きを破線の矢印
で示してある。FIG. 1 is a perspective view of a piezoelectric elliptical motion oscillator according to a first embodiment of the present invention, in which electrodes 2, 3 are arranged in parallel with the length direction at positions on a side surface of a piezoelectric ceramic cylinder 1 in four circumferential directions. , 4,5 are formed. The ratio of the width of one electrode to the dimension without electrode is about 1: 1. FIG. 2 is a sectional view of a piezoelectric ceramic cylinder, and is an explanatory view of a state in which distortion occurs due to a polarization direction and a driving voltage. FIG. 2 (a) is a diagram showing the direction of polarization when a voltage is applied with the electrodes 2 and 4 being positive and the electrodes 3 and 5 being negative, and the direction of polarization is indicated by broken line arrows.
第2図(b)は第2図(a)のように分極された圧電セ
ラミックス円柱において、電極2,3および4,5をそれぞれ
接続し、電極2,3にプラス、電極4,5にマイナス電圧を印
加した場合の円柱の断面方向の歪いの発生を示したもの
である。2 (b) is a piezoelectric ceramic cylinder polarized as shown in FIG. 2 (a), in which electrodes 2, 3 and 4, 5 are connected to each other, the electrodes 2, 3 are positive, and the electrodes 4, 5 are negative. It shows the occurrence of distortion in the cross-sectional direction of the cylinder when a voltage is applied.
第2図(b)において実線の矢印で示したように電極2
から電極5の方向および電極3から電極4の方向に電圧
が印加されるため、電極2と電極5の間には伸び歪みが
発生し、電極3と電極4の間には縮み歪みが発生する。
第2図(b)に示す方向に断面方向の歪みが発生した場
合において、圧電セラミックス円柱1は、電極3と電極
4の間の部分の長さが伸び、同時に電極2と電極5の間
の部分の長さが縮む。その結果、圧電セラミックス1は
第2図(b)においては下側が膨らむように屈曲する。
印加電圧の極性を逆にした場合には、圧電セラミックス
円柱1は逆方向に屈曲する。As shown by the solid line arrow in FIG.
Since a voltage is applied in the direction from the electrode 5 to the electrode 5 and in the direction from the electrode 3 to the electrode 4, expansion strain occurs between the electrodes 2 and 5, and contraction strain occurs between the electrodes 3 and 4. .
When a cross-sectional strain occurs in the direction shown in FIG. 2 (b), the piezoelectric ceramic cylinder 1 extends in the length between the electrodes 3 and 4, and at the same time, between the electrodes 2 and 5. The length of the part shrinks. As a result, the piezoelectric ceramics 1 bends so that the lower side bulges in FIG. 2 (b).
When the polarity of the applied voltage is reversed, the piezoelectric ceramic cylinder 1 bends in the opposite direction.
第3図は第1図に示した圧電セラミックス円柱1に交流
電圧を加えた場合の振動状態の説明図であり、電極2,3
と電極4,5の間に振動子の共振周波数に等しい周波数の
交流電圧印加した場合には、第3図(a)に示すように
矢印6の方向の屈曲共振を生ずる。FIG. 3 is an explanatory view of a vibrating state when an AC voltage is applied to the piezoelectric ceramic cylinder 1 shown in FIG.
When an AC voltage having a frequency equal to the resonance frequency of the vibrator is applied between the electrodes and the electrodes 4 and 5, bending resonance occurs in the direction of arrow 6 as shown in FIG.
電極2,5および電極3,4をそれぞれ接続して同様に振動子
の共振周波数に等しい周波数の交流電圧を印加すれば、
屈曲振動の方向は第3図(a)の振動方向と直角な方向
になる。従って以上示した二つの方向の屈曲振動の位相
を90°ずらせること、具体的には各々の駆動電圧の位相
を90°ずらせることにより、圧電セラミックス円柱1の
両端部に、第3図(b)に示すように円振動あるいは楕
円振動を励振することが可能である。If electrodes 2 and 5 and electrodes 3 and 4 are connected to each other and an AC voltage having a frequency equal to the resonance frequency of the vibrator is applied,
The bending vibration direction is perpendicular to the vibration direction shown in FIG. Therefore, by shifting the phase of the flexural vibration in the two directions shown above by 90 °, specifically by shifting the phase of each drive voltage by 90 °, the piezoelectric ceramic cylinder 1 is provided with the two ends shown in FIG. It is possible to excite circular vibration or elliptical vibration as shown in b).
実施例2 本発明の実施例2について説明する。Example 2 Example 2 of the present invention will be described.
第4図(a)は本発明の実施例2に係る圧電楕円運動振
動子の構造の一例を示す斜視図である。第4図(b)に
おいて、圧電セラミックス円板11,12はそれぞれ中心に
沿う方向で2分割する境界面とし、この分極境界線の両
側のほぼ対称な二つの領域の分極方向が厚さ方向に互い
に逆向きになるように分極されている。互いに境界面を
90度傾斜させた圧電セラミックス円板11,12の間に金属
円柱14を挾み、さらに圧電セラミックス11,12の両側に
金属円柱13,15を配置し、第4図(b)に示すようにこ
れら二枚の圧電セラミックス円板と三個の金属円柱を一
体に接合する。接合の方法は、エポキシ樹脂などの接着
剤を用いるか、半田づけによって行う。第5図は本発明
の実施例2に係る圧電楕円運動振動子の他の構造例を示
すの斜視図である。第5図において、円板状圧電振動子
16は第4図に示したものと同様の圧電セラミックス円板
16a,16bの二枚を、それぞれ分極境界面を合わせ、互い
に分極の向きを対向させるように構成されており、また
円板状圧電振動子17も同様に圧電セラミックス円板17a,
17bの二枚をそれぞれの分極境界面を合せて互いの分極
の向きを対向させるように構成されている。二個の円板
状圧電振動子16,17を第4図の場合と同様に三個の金属
円柱13,14,15の間に挾んで一体に接合されている。FIG. 4 (a) is a perspective view showing an example of the structure of the piezoelectric elliptical motion oscillator according to the second embodiment of the present invention. In FIG. 4 (b), the piezoelectric ceramic disks 11 and 12 are boundary surfaces that are divided into two in the direction along the center, respectively, and the polarization directions of two substantially symmetrical regions on both sides of this polarization boundary line are in the thickness direction. They are polarized so that they are in opposite directions. Bound each other
A metal cylinder 14 is sandwiched between piezoelectric ceramic disks 11 and 12 tilted by 90 degrees, and metal cylinders 13 and 15 are arranged on both sides of the piezoelectric ceramics 11 and 12, as shown in FIG. 4 (b). These two piezoelectric ceramic discs and three metal cylinders are joined together. The joining method is performed by using an adhesive such as an epoxy resin or by soldering. FIG. 5 is a perspective view showing another structural example of the piezoelectric elliptical motion oscillator according to the second embodiment of the present invention. In FIG. 5, a disk-shaped piezoelectric vibrator
16 is a piezoelectric ceramic disc similar to that shown in FIG.
16a and 16b are arranged so that their polarization boundary surfaces are aligned with each other, and the polarization directions thereof are opposed to each other.
The two 17b are arranged so that their polarization boundary surfaces are aligned with each other so that their polarization directions face each other. The two disk-shaped piezoelectric vibrators 16 and 17 are sandwiched between the three metal cylinders 13, 14 and 15 and integrally bonded as in the case of FIG.
第6図は本発明の実施例2に係る圧電楕円運動振動子の
動作原理の説明図である。第6図(b)に示すように
(イ)の圧電セラミックス円板に電圧を印加した場合第
6図(b)(イ)の上半分には伸び歪みが発生し、下半
分には縮み歪みが発生する。従ってリード端子19及び20
間に共振周波数に等しい交流電圧を印加すれば第6図
(a)に示すように矢印6の方向の屈曲共振を生ずる。FIG. 6 is an explanatory diagram of the operation principle of the piezoelectric elliptical motion oscillator according to the second embodiment of the present invention. As shown in FIG. 6 (b), when a voltage is applied to the piezoelectric ceramic disk of (a), elongation strain occurs in the upper half of FIG. 6 (b) (a) and contraction strain occurs in the lower half. Occurs. Therefore, lead terminals 19 and 20
If an AC voltage equal to the resonance frequency is applied between them, a bending resonance in the direction of arrow 6 is generated as shown in FIG. 6 (a).
同様に第6図(b)(ロ)の圧電セラミックス円板に同
様の交流電圧を印加すれば、分極境界線の方向が第6図
(b)(イ)の場合と直角であるため、第6図(a)の
振動方向と直角な方向に屈曲共振を生ずる。従ってリー
ド端子19−20とリード端子21−20に印加する駆動電圧の
位相を90°ずらすことにより圧電楕円運動振動子16の両
端部に第6図(c)の矢印で示すような円振動あるいは
楕円振動を励振することができる。Similarly, when a similar AC voltage is applied to the piezoelectric ceramic disk of FIG. 6 (b) (b), the direction of the polarization boundary line is perpendicular to that of the case of FIG. 6 (b) (a). A bending resonance occurs in a direction perpendicular to the vibration direction of FIG. Therefore, by shifting the phase of the drive voltage applied to the lead terminals 19-20 and 21-20 by 90 °, the circular vibration as shown by the arrow in FIG. Elliptical vibration can be excited.
以上の説明は第4図に示した圧電楕円運動振動子につい
て行ったが第5図に示した圧電楕円運動振動子において
は、二枚の圧電セラミックス円板の接合部から駆動電気
端子を取り出すことにより、二枚の圧電セラミックス圧
電楕円運動円板を並列駆動することが可能となり、第4
図に示した場合より低い電圧での駆動が可能となる。Although the above explanation has been given for the piezoelectric elliptic motion oscillator shown in FIG. 4, in the piezoelectric elliptic motion oscillator shown in FIG. 5, the drive electric terminal is taken out from the joint portion of the two piezoelectric ceramic disks. This makes it possible to drive two piezoelectric ceramics piezoelectric elliptical motion disks in parallel.
Driving at a lower voltage than that shown in the figure is possible.
実施例3 第7図は本発明の実施例3に係る圧電楕円運動振動子の
構造の一例を示す斜視図である。第7図において、円筒
状圧電振動子31,31′はそれぞれ中心に沿う方向で2分
割する分極の境界面を有し、この分極境界面の両側のほ
ぼ対称な二つの領域の分極方向が厚さ方向に互いに逆向
きになるように分極されている圧電セラミックス穴あき
円板二枚32,33を穴あき円板状金属端子34をはさんで分
極境界面合わせ、互いに分極向きを対向させるようにし
て構成されている。実施例3においては、前記した円筒
状圧電振動子の二つを金属円筒35を挾んで互いに分極境
界面が直角な方向を示すようにそれぞれ配置し、さらに
前記した二対の圧電振動子対の外側に金属円筒36,37を
それぞれ配置しこれらを第7図(b)に示すように中心
ボルト38とナット39,39′により一体に締め付けて構成
される。Third Embodiment FIG. 7 is a perspective view showing an example of the structure of a piezoelectric elliptical motion oscillator according to a third embodiment of the invention. In FIG. 7, each of the cylindrical piezoelectric vibrators 31 and 31 ′ has a polarization boundary surface that is divided into two in the direction along the center, and the polarization directions of two substantially symmetrical regions on both sides of this polarization boundary surface are thick. Piezoelectric ceramics that are polarized so that they are polarized in opposite directions to each other in the vertical direction Is configured. In the third embodiment, two of the above-mentioned cylindrical piezoelectric vibrators are arranged so as to sandwich the metal cylinder 35 so that their polarization boundary surfaces show directions at right angles to each other. Metal cylinders 36 and 37 are arranged on the outside, respectively, and they are integrally tightened by a central bolt 38 and nuts 39 and 39 'as shown in FIG. 7 (b).
実施例3においては、第7図に示すように2個の圧電振
動子対と金属円筒35,36,37を中心ボルト38とナット39,3
9′で一体に締付けて構成しているが、金属円筒36,37に
直接ネジを切り、ナットとして使用しても同様な効果が
得られる。In the third embodiment, as shown in FIG. 7, the two piezoelectric vibrator pairs and the metal cylinders 35, 36 and 37 are connected to the center bolt 38 and the nuts 39 and 3, respectively.
9'is integrally tightened, but the same effect can be obtained by directly threading the metal cylinders 36, 37 and using them as nuts.
第8図は本発明の圧電楕円運動振動子の動作原理の説明
図である。第8図(b)(イ)において円筒状圧電振動
子31の中間端子板を共通アースとし、両端面にプラス電
圧を印加した場合、円筒状圧電振動子の上半分に伸び歪
みを発生し、下半分には縮み歪みが発生する。従って、
リード端子41及び42間に圧電振動子の共振周波数に等し
い周波数の交流電圧を印加すれば第8図(a)に示すよ
うに矢印の方向の屈曲共振を生ずる。FIG. 8 is an explanatory diagram of the operating principle of the piezoelectric elliptical motion oscillator of the present invention. In FIG. 8 (b) (a), when the intermediate terminal plate of the cylindrical piezoelectric vibrator 31 is used as a common ground and a positive voltage is applied to both end surfaces, expansion strain occurs in the upper half of the cylindrical piezoelectric vibrator, Shrinkage distortion occurs in the lower half. Therefore,
When an AC voltage having a frequency equal to the resonance frequency of the piezoelectric vibrator is applied between the lead terminals 41 and 42, bending resonance in the direction of the arrow is generated as shown in FIG. 8 (a).
同様にして第8図(b)(ロ)円筒状圧電振動子に同様
の交流電圧を印加すれば第8図(a)の矢印の方向と直
角な方向に屈曲共振を生ずる。従ってリード端子41−42
とリード端子43−42に印加する駆動電圧の位相を90°ず
らせることにより圧電楕円運動振動子40の両端部に第8
図(c)に示すような円振動あるいは楕円振動を励振す
ることができる。Similarly, when a similar AC voltage is applied to the cylindrical piezoelectric vibrator of FIG. 8 (b) and (b), bending resonance occurs in the direction perpendicular to the direction of the arrow in FIG. 8 (a). Therefore, lead terminals 41-42
By shifting the phase of the drive voltage applied to the lead terminals 43-42 by 90 °, the piezoelectric elliptical motion oscillator 40 is provided with an eighth
Circular vibration or elliptical vibration as shown in FIG. 7C can be excited.
(発明の効果) 以上説明したように、本発明の圧電楕円運動振動子にお
いては、圧電振動子の形状が単純で、特に断面が円形と
なっているため、高精度の加工が可能であり、互いに直
角な方向の共振周波数のばらつきの少ない振動子が得ら
れる。また断面が円形であることは、例えば第10図に示
したような超音波モータを構成する場合にカップ状回転
ローラーとの接触状態が良く、安定したモータが得られ
る。さらに本発明の圧電楕円運動振動子においては、接
着剤を使用していないため、接着による特性のばらつき
も少なく、実用上その効果が大きい。(Effects of the Invention) As described above, in the piezoelectric elliptical motion oscillator of the present invention, since the piezoelectric oscillator has a simple shape, and in particular, has a circular cross section, high-precision machining is possible. It is possible to obtain a vibrator with little variation in resonance frequency in the directions orthogonal to each other. In addition, the circular cross section makes it possible to obtain a stable motor with a good contact state with the cup-shaped rotating roller when the ultrasonic motor as shown in FIG. 10 is constructed. Further, in the piezoelectric elliptic motion oscillator of the present invention, since no adhesive is used, there is little variation in characteristics due to adhesion, and the effect is practically large.
さらに本発明の他の圧電楕円運動振動子においては、各
々の部材をボルトトナットで締め付けて構成しているた
め高いパワーを入力して駆動しても接着が剥がれるとい
う危険もなく信頼性の高い振動子が得られる。また寸法
的には、必要なパワーとの関係で決められるが直径5mm
程度の振動子も容易に製造可能であり、小型の超音波モ
ータが実現できる。Further, in another piezoelectric elliptical motion oscillator of the present invention, since each member is tightened with bolts and nuts, it is highly reliable without risk of peeling even if high power is input and driven. A vibrator is obtained. Also, in terms of dimensions, it is determined in relation to the required power, but the diameter is 5 mm
It is possible to easily manufacture oscillators of a certain size and realize a small ultrasonic motor.
第1図は本発明の実施例1に係る圧電楕円運動振動子の
斜視図、第2図(a)及び(b)は第1図の圧電楕円運
動振動子の歪みの発生状態の説明に供する断面図、第3
図(a)及び(b)は第1図の圧電楕円運動振動子の振
動を示す図、第4図(a)及び(b)は本発明の実施例
2に係る圧電楕円運動振動子及びその組立てを示す斜視
図、第5図(a)及び(b)は本発明の実施例2に係る
他の圧電楕円運動振動子及びその組立てを示す斜視図、
第6図(a),(b)(イ),(b)(ロ)及び(c)
は本発明の実施例2に係る圧電楕円運動振動子の動作原
理を示す斜視図、第7図(a)及び(b)は本発明の実
施例3に係る圧電楕円運動振動子及びその組立てを示す
斜視図、第8図(a),(b)及び(c)は本発明の実
施例3に係る圧電楕円運動振動子の動作原理を示す斜視
図、第9図は従来例に係る圧電楕円運動振動子の動作原
理を示す斜視図、第10図は従来例に係る圧電楕円運動振
動子の構成を示す斜視図である。 図中、1はセラミックス円柱、2,3,4及び5は電極、11
及び12はセラミックス円板、13,14及び15は金属円柱、1
6及び17は圧電振動子、16a,16b,17a,17bは圧電セラミッ
クス円板、18は圧電楕円運動振動子、19,20,及び21はリ
ード端子、31,31′は圧電振動子、32及び33は圧電セラ
ミックス円板、34は円板状金属端子、35,36及び37は金
属円筒、38はボルト、39,39′はナット、40は圧電楕円
運動振動子、41,42及び43はリード端子、100は角柱振動
子、120は金属角柱、121a,121bは圧電セラミックス薄
板、122a,122bはリード端子、123はアース端子、124a及
び124bは円板、125a,125bは支持ピン、126a,126bはカッ
プ状回転ローラーである。FIG. 1 is a perspective view of a piezoelectric elliptical motion oscillator according to a first embodiment of the present invention, and FIGS. 2A and 2B are provided for explaining a strain generation state of the piezoelectric elliptical motion oscillator of FIG. Sectional view, third
FIGS. 4A and 4B are diagrams showing vibration of the piezoelectric elliptical motion oscillator shown in FIG. 1, and FIGS. 4A and 4B are piezoelectric elliptical motion oscillators according to a second embodiment of the present invention and the same. FIG. 5A and FIG. 5B are perspective views showing assembly, FIG. 5A and FIG. 5B are perspective views showing another piezoelectric elliptical motion oscillator and its assembly according to the second embodiment of the present invention.
Fig. 6 (a), (b) (a), (b) (b) and (c)
Is a perspective view showing the operating principle of the piezoelectric elliptical motion oscillator according to the second embodiment of the present invention, and FIGS. 7A and 7B show a piezoelectric elliptical motion oscillator according to the third embodiment of the present invention and its assembly. 8A, 8B, and 8C are perspective views showing the operating principle of the piezoelectric elliptical motion oscillator according to the third embodiment of the present invention, and FIG. 9 is a piezoelectric ellipse according to the conventional example. FIG. 10 is a perspective view showing the operation principle of the motion oscillator, and FIG. 10 is a perspective view showing the configuration of a piezoelectric elliptical motion oscillator according to a conventional example. In the figure, 1 is a ceramic cylinder, 2, 3, 4 and 5 are electrodes, 11
And 12 are ceramic discs, 13, 14 and 15 are metal cylinders, 1
6 and 17 are piezoelectric vibrators, 16a, 16b, 17a and 17b are piezoelectric ceramic disks, 18 is a piezoelectric elliptical motion vibrator, 19, 20 and 21 are lead terminals, 31 and 31 'are piezoelectric vibrators, 32 and 33 is a piezoelectric ceramic disk, 34 is a disk-shaped metal terminal, 35, 36 and 37 are metal cylinders, 38 is a bolt, 39, 39 'is a nut, 40 is a piezoelectric elliptical motion oscillator, 41, 42 and 43 are leads. Terminal, 100 is a prismatic vibrator, 120 is a metal prism, 121a and 121b are piezoelectric ceramic thin plates, 122a and 122b are lead terminals, 123 is a ground terminal, 124a and 124b are discs, 125a and 125b are support pins, 126a and 126b. Is a cup-shaped rotating roller.
フロントページの続き (56)参考文献 特開 昭63−240380(JP,A) 特開 昭63−224681(JP,A) 特開 昭61−55012(JP,A) 特開 昭63−11075(JP,A) 特開 昭63−220781(JP,A) 米国特許2439499(US,A) 日本音響学会講演論文集、昭和62年3 月、P.673〜674 「電気・機械振動子とその応用」、コロ ナ社、昭和49年3月30日P.271、Continuation of the front page (56) Reference JP 63-240380 (JP, A) JP 63-224681 (JP, A) JP 61-55012 (JP, A) JP 63-11075 (JP , A) JP 63-220781 (JP, A) US Patent 2439499 (US, A) Proceedings of the Acoustical Society of Japan, March 1987, p. 673-674 “Electrical and mechanical oscillators and their applications”, Corona Publishing Co., Ltd., March 30, 1974, p. 271,
Claims (4)
向と平行に所定の間隔をおいて、複数の電極対を設け、
該電極対の少なくとも1つに直流電圧を印加して前記圧
電セラミックス円柱に長さ方向と直角な方向の分極処理
を施し、前記電極対のうちの2つに互いに異なる位相を
有する交流電圧を印加して、前記圧電セラミックス円柱
の両端部に円を含む楕円運動を励起可能としたことを特
徴とする圧電楕円運動振動子。1. A plurality of electrode pairs are provided on an outer peripheral surface of a piezoelectric ceramics column at predetermined intervals in parallel with a length direction,
A DC voltage is applied to at least one of the electrode pairs to subject the piezoelectric ceramic cylinder to polarization treatment in a direction perpendicular to the length direction, and AC voltages having different phases are applied to two of the electrode pairs. Then, a piezoelectric elliptic motion oscillator capable of exciting an elliptic motion including a circle at both ends of the piezoelectric ceramic cylinder.
第1及び第2の圧電セラミック円板の一端間に挟まれた
第1の金属円柱と、該第1及び第2の圧電セラミック円
板の他端に夫々設けられた第2及び第3の金属円柱とを
有する圧電楕円運動振動子であって、前記第1の圧電セ
ラミック円板は、該第1の圧電セラミック円板の中心軸
に沿う方向で2分割する第1の境界面を境にして厚さ方
向に互いに逆向きとなるように分極されており、前記第
2の圧電セラミック円板は、該圧電セラミック円板の中
心軸に沿う方向で2分割し且つ前記第1の境界面と所定
角度で傾斜した第2の境界面を境にして厚さ方向に互い
に逆向きとなるように分極されており、前記第1の金属
を共通のアースとし、前記第2及び第3の金属円柱に互
いに異なる位相を有する交流電圧を印加して、前記圧電
楕円運動振動子の両端部に円を含む楕円運動を励起可能
としたことを特徴とする圧電楕円運動振動子。2. A first and a second piezoelectric ceramic disk, a first metal cylinder sandwiched between one ends of the first and the second piezoelectric ceramic disk, and a first and a second piezoelectric material. A piezoelectric elliptical motion oscillator having second and third metal cylinders respectively provided on the other end of the ceramic disc, wherein the first piezoelectric ceramic disc is the same as the first piezoelectric ceramic disc. The second piezoelectric ceramic discs are polarized so as to be opposite to each other in the thickness direction with a first boundary surface that is divided in two in the direction along the central axis as a boundary. It is divided in two in the direction along the central axis and is polarized so as to be opposite to each other in the thickness direction with a second boundary surface inclined at a predetermined angle from the first boundary surface as a boundary. The metal of the above is used as a common earth, and the phases different from each other are applied to the second and third metal cylinders. An AC voltage is applied to the piezoelectric elliptical motion oscillator, characterized in that the excitable an elliptical motion comprising a circle at both ends of the piezoelectric elliptical motion oscillator.
1及び第2の円板状圧電振動子の一端間に挟まれた第1
の金属円柱と、該第1及び第2の円板状圧電振動子の他
端に夫々設けられた第2及び第3の金属円柱とを有する
圧電楕円運動振動子であって、前記第1の円板状圧電振
動子は、該第1の円板状圧電振動子の中心軸に沿う方向
で2分割する第1の境界面及び厚さ方向で2分割する第
2の境界面を境として厚さ方向に互いに逆向きとなるよ
うに分極されており、前記記第2の円板状圧電振動子
は、該第2の円板状圧電振動子の中心軸に沿う方向で2
分割され且つ前記第1の境界面と所定角度で傾斜した第
3の境界面及び且つ厚さ方向で2分割する第4の境界面
を境にして厚さ方向に互いに逆向きとなるように分極さ
れており、前記第1,第2及び第3の金属円柱を共通のア
ースとし、前記第2及び第4の境界面に互いの異なる位
相の交流電圧を印加して、前記圧電楕円運動振動子の両
端部に円を含む楕円運動を励起可能としたことを特徴と
する圧電楕円運動振動子。3. A first and a second disk-shaped piezoelectric vibrators, and a first sandwiched between one ends of the first and the second disk-shaped piezoelectric vibrators.
A piezoelectric elliptical motion oscillator having: a metal cylinder; and a second and a third metal cylinder provided at the other ends of the first and second disk-shaped piezoelectric vibrators, respectively. The disk-shaped piezoelectric vibrator has a thickness that is divided by a first boundary surface that divides the first disk-shaped piezoelectric vibrator in a direction along the central axis and a second boundary surface that divides the first disk-shaped piezoelectric vibrator in the thickness direction. The second disk-shaped piezoelectric vibrators are polarized in opposite directions to each other in the vertical direction, and the second disk-shaped piezoelectric vibrators are arranged in a direction along the central axis of the second disk-shaped piezoelectric vibrators.
Polarization is performed so as to be opposite to each other in the thickness direction with a third boundary surface that is divided and inclined at a predetermined angle with the first boundary surface and a fourth boundary surface that is divided into two in the thickness direction as boundaries. The first, second, and third metal cylinders are used as a common ground, and alternating voltages having mutually different phases are applied to the second and fourth boundary surfaces to generate the piezoelectric elliptical motion oscillator. A piezoelectric elliptical motion oscillator characterized in that it is possible to excite an elliptical motion including a circle at both ends.
1及び第2の円筒状圧電振動子の一端間に挟まれた第1
の金属円筒と、該第1及び第2の円筒状圧電振動子の他
端に夫々設けられた第2及び第3の金属円柱とを貫通部
材により固着した圧電楕円運動振動子であって、前記第
1の円筒状圧電振動子は、該第1の円筒状圧電振動子の
中心軸に沿う方向で2分割する第1の境界面及び厚さ方
向で2分割する第2の境界面を境として厚さ方向に互い
に逆向きとなるように分極されており、前記第2の円筒
状圧電振動子は、該第2の円筒状圧電振動子の中心軸に
沿う方向で2分割され且つ前記第1の境界面と所定角度
で傾斜した第3の境界面及び厚さ方向で2分割する第4
の境界面を境にして厚さ方向に互いに逆向きとなるよう
に分極されており、前記第2及び第4の境界面に夫々第
1及び第2の中間端子板を有し、前記第1,第2及び第3
の金属円筒を共通アースとし、前記中間端子板に互いに
異なる位相の交流電圧を印加して、前記圧電楕円運動振
動子の両端部に円を含む楕円運動を励起可能としたこと
を特徴とする圧電楕円運動振動子。4. A first and a second cylindrical piezoelectric vibrators, and a first sandwiched between one ends of the first and the second cylindrical piezoelectric vibrators.
A piezoelectric elliptic motion oscillator in which a metal cylinder and a second and a third metal cylinder provided at the other ends of the first and second cylindrical piezoelectric vibrators are fixed by a penetrating member, respectively. The first cylindrical piezoelectric vibrator has a first boundary surface divided into two in a direction along a central axis of the first cylindrical piezoelectric vibrator and a second boundary surface divided into two in a thickness direction as boundaries. Polarized so as to be opposite to each other in the thickness direction, the second cylindrical piezoelectric vibrator is divided into two in a direction along the central axis of the second cylindrical piezoelectric vibrator, and the first cylindrical piezoelectric vibrator is divided into two. The third boundary surface inclined at a predetermined angle with the second boundary surface and the fourth divided into two in the thickness direction.
Are polarized so as to be opposite to each other in the thickness direction with the boundary surface of the first boundary surface as a boundary, and the first and second intermediate terminal plates are provided on the second and fourth boundary surfaces, respectively. , Second and third
A piezoelectric body characterized in that the metal cylinder is used as a common ground, and alternating voltages having different phases are applied to the intermediate terminal plate to excite elliptical motion including circles at both ends of the piezoelectric elliptical motion oscillator. Elliptical motion oscillator.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63185414A JPH072229B2 (en) | 1988-07-27 | 1988-07-27 | Piezoelectric elliptical motion oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63185414A JPH072229B2 (en) | 1988-07-27 | 1988-07-27 | Piezoelectric elliptical motion oscillator |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0236776A JPH0236776A (en) | 1990-02-06 |
JPH072229B2 true JPH072229B2 (en) | 1995-01-18 |
Family
ID=16170373
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63185414A Expired - Lifetime JPH072229B2 (en) | 1988-07-27 | 1988-07-27 | Piezoelectric elliptical motion oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH072229B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US8159763B2 (en) | 2006-03-22 | 2012-04-17 | Nikon Corporation | Vibrating element, vibration actuator, lens barrel, camera system and method for driving vibration actuator |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5146129A (en) * | 1986-12-01 | 1992-09-08 | Canon Kabushiki Kaisha | Vibration wave motor |
US5410204A (en) * | 1992-02-28 | 1995-04-25 | Olympus Optical Co. Ltd. | Ultrasonic oscillator |
JP5285969B2 (en) | 2008-06-11 | 2013-09-11 | シロキ工業株式会社 | Door lock device |
-
1988
- 1988-07-27 JP JP63185414A patent/JPH072229B2/en not_active Expired - Lifetime
Non-Patent Citations (2)
Title |
---|
「電気・機械振動子とその応用」、コロナ社、昭和49年3月30日P.271、 |
日本音響学会講演論文集、昭和62年3月、P.673〜674 |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US8159763B2 (en) | 2006-03-22 | 2012-04-17 | Nikon Corporation | Vibrating element, vibration actuator, lens barrel, camera system and method for driving vibration actuator |
Also Published As
Publication number | Publication date |
---|---|
JPH0236776A (en) | 1990-02-06 |
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