JPH02228266A - Ultrasonic vibrator and ultrasonic motor - Google Patents
Ultrasonic vibrator and ultrasonic motorInfo
- Publication number
- JPH02228266A JPH02228266A JP1046865A JP4686589A JPH02228266A JP H02228266 A JPH02228266 A JP H02228266A JP 1046865 A JP1046865 A JP 1046865A JP 4686589 A JP4686589 A JP 4686589A JP H02228266 A JPH02228266 A JP H02228266A
- Authority
- JP
- Japan
- Prior art keywords
- elastic body
- vibration
- ultrasonic
- vibrator
- plate
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 238000005452 bending Methods 0.000 claims abstract description 8
- 230000005284 excitation Effects 0.000 claims description 10
- 230000002457 bidirectional effect Effects 0.000 abstract 1
- 238000010276 construction Methods 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000035515 penetration Effects 0.000 description 1
- 230000001902 propagating effect Effects 0.000 description 1
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- General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は、略楕円振動が励振される超音波振動子及び該
振動子を利用した超音波モータに関するものである。DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to an ultrasonic vibrator that is excited with approximately elliptical vibration, and an ultrasonic motor that utilizes the vibrator.
[従来技術]
従来、上記のような超音波振動子は主に定在波型超音波
モータに利用されている。[Prior Art] Conventionally, the above-mentioned ultrasonic transducers have been mainly used in standing wave type ultrasonic motors.
定在波型超音波モータの動作原理は、略楕円運動が励起
される超音波振動子に対して所定圧力で移動子を当接さ
せ、略楕円運動する各質点と移動子との摩擦力により移
動子を駆動するものである。The operating principle of a standing wave type ultrasonic motor is that a moving element is brought into contact with a predetermined pressure against an ultrasonic vibrator that is excited in approximately elliptical motion, and the friction force between each mass point moving approximately in an elliptical manner and the moving element is used. It drives the mover.
定在波型超音波振動子は、高効率振動を実現する構成が
得やすいために、定在波型モータは進行波型モータに比
較して高効率、大出力という長所がある。Since the standing wave type ultrasonic vibrator can easily be configured to achieve highly efficient vibration, the standing wave type motor has the advantage of higher efficiency and larger output than the traveling wave type motor.
従来の定在波型モータに利用される超音波振動子は、略
楕円運動を高効率に励起するために、弾性体と励振体と
の接触面では単一方向振動を、また一方、弾性体と移動
子との接触面では楕円振動を行う固有振動モードを有す
る機械共振系を用いることで略楕円運動を得ている。The ultrasonic vibrator used in conventional standing wave motors generates unidirectional vibration at the contact surface between the elastic body and the exciting body in order to excite approximately elliptical motion with high efficiency. At the contact surface between the rotor and the mover, approximately elliptical motion is obtained by using a mechanical resonance system having a natural vibration mode that performs elliptical vibration.
[発明が解決しようとする課題]
しかしながら、同一周波数で2方向に振動する弾性体に
単一方向振動を励振しようとする場合、弾性体や励振体
の構造上のわずかな非対称性などの影響を受け、もう一
方の方向の振動をまったく励振しない事は難しかった。[Problems to be Solved by the Invention] However, when attempting to excite unidirectional vibrations in an elastic body that vibrates in two directions at the same frequency, it is difficult to overcome the effects of slight asymmetry in the structure of the elastic body or the exciting body. It was difficult to not excite vibrations in the other direction at all.
そのため、該不要振動により振動がさまたげられ、高効
率、大出力の振動子が得られないという欠点があった。Therefore, there is a drawback that vibration is hindered by the unnecessary vibration, and a vibrator with high efficiency and high output cannot be obtained.
また、前記弾性体に単一振動だけを励振するために、振
動子の構成が著しく制限されてしまうという欠点もあっ
た。Furthermore, since only a single vibration is excited in the elastic body, there is a drawback that the configuration of the vibrator is severely limited.
本発明は、上述した問題点を解決するためになされたも
のであり、その目的は弾性体に不要振動が発生すること
のない構成とすることにより弾性体や励振体の構成条件
の自由度が大きく、高効率、大出力動作が可能な超音波
振動子を提供する事にある。The present invention has been made to solve the above-mentioned problems, and its purpose is to increase the degree of freedom in the configuration of the elastic body and the exciting body by creating a configuration that does not generate unnecessary vibrations in the elastic body. The object of the present invention is to provide an ultrasonic transducer that is large, highly efficient, and capable of high output operation.
[課題を解決するための手段]
上記目的を達成するために本発明の超音波振動子は、第
1及び第2方向に大略同一周波数で共振する弾性体と、
該弾性体の双方の方向に前記大略同一周波数の振動を励
振する第1励振体と、前記弾性体の第1方向に対し、前
記周波数の振動を励振し、同時に該振動と大略同一周波
数で位相が逆の振動を第2方向に対し励振する第2励振
体とを有している。[Means for Solving the Problems] In order to achieve the above object, the ultrasonic transducer of the present invention includes an elastic body that resonates at approximately the same frequency in the first and second directions;
a first excitation body that excites vibrations of the substantially same frequency in both directions of the elastic body; and a second excitation body that excites opposite vibrations in a second direction.
また、本発明の超音波モータは上記超音波振動子と該超
音波振動子の弾性体に接する可動子とを備えている。Further, the ultrasonic motor of the present invention includes the ultrasonic transducer described above and a movable element in contact with the elastic body of the ultrasonic transducer.
[作用]
上記の構成を有する本発明の超音波振動子においては、
前記第1励振体は前記弾性体に異なる2方向の振動を与
える。[Function] In the ultrasonic transducer of the present invention having the above configuration,
The first excitation body applies vibrations to the elastic body in two different directions.
同時に、前記第2励振体は前記弾性体に、前記2方向振
動と振動方向が同じ振動を与える。At the same time, the second excitation body applies vibration to the elastic body in the same vibration direction as the two-way vibration.
このとき、該2方向振動に対する位相関係が、一方が同
相で他方が逆相となっている。そのため各振動のエネル
ギーが不要振動として消費されることなく有効に利用さ
れる。At this time, the phase relationship for the two-way vibration is such that one side is in phase and the other side is out of phase. Therefore, the energy of each vibration is effectively used without being consumed as unnecessary vibrations.
そして、上記2つの励振体の振動位相を調節する事によ
り、前記弾性体に任意の形状の略楕円振動を得る事がで
きる。By adjusting the vibration phases of the two excitation bodies, substantially elliptical vibration of an arbitrary shape can be obtained in the elastic body.
また、上記構成を何する本発明の超音波モータは、前記
超音波振動子の振動により可動子に駆動力が生じる。Further, in the ultrasonic motor of the present invention having the above-mentioned configuration, a driving force is generated in the movable element by the vibration of the ultrasonic vibrator.
[実施例]
以下、本発明を具体化した一実施例を図面を参照して説
明する。[Example] Hereinafter, an example embodying the present invention will be described with reference to the drawings.
第1図乃至第3図は、本実施例の超音波振動子である。1 to 3 show the ultrasonic transducer of this embodiment.
本実施例の超音波振動子11は、第1圧電体12及び第
2圧電体13が、ボルト14を中心として対称となる位
置で台15に固定されている。前記第1圧電体12及び
′N52圧電体13は、第1図中の上下方向に分極され
、厚み方向振動する。該第1圧電体12及び第2圧電体
13の上面には、板状弾性体16が前記ボルト14によ
り台15に固定されている。In the ultrasonic transducer 11 of this embodiment, a first piezoelectric body 12 and a second piezoelectric body 13 are fixed to a stand 15 at symmetrical positions with a bolt 14 as the center. The first piezoelectric body 12 and the 'N52 piezoelectric body 13 are polarized in the vertical direction in FIG. 1 and vibrate in the thickness direction. On the upper surfaces of the first piezoelectric body 12 and the second piezoelectric body 13, a plate-shaped elastic body 16 is fixed to the stand 15 by the bolts 14.
前記第1圧電体12及び第2圧電体13の下面には電極
17及び18が着設されている。また、前記板状弾性体
16は、圧電体12及び13の電極を兼ねている。Electrodes 17 and 18 are installed on the lower surfaces of the first piezoelectric body 12 and the second piezoelectric body 13. Further, the plate-like elastic body 16 also serves as an electrode for the piezoelectric bodies 12 and 13.
更にこの板状弾性体16は、その厚さ方向に所定の周波
数fで曲げ振動する。また大略同一の周波数fにより長
さ方向に縦振動する。Furthermore, this plate-shaped elastic body 16 bends and vibrates at a predetermined frequency f in its thickness direction. Further, they longitudinally vibrate in the length direction at approximately the same frequency f.
一般に、板状弾性体中を伝播する縦振動の共振周波数は
、該板状弾性体の長さに依存する。また同板状弾性体の
厚さ方向の曲げ振動の共振周波数は、前記長さ及び厚さ
に依存する。従って、前述のような板状弾性体16を設
計することは容易である。Generally, the resonant frequency of longitudinal vibration propagating in an elastic plate depends on the length of the elastic plate. Further, the resonant frequency of bending vibration in the thickness direction of the plate-like elastic body depends on the length and thickness. Therefore, it is easy to design the plate-like elastic body 16 as described above.
以上のように構成された振動子の作用を第3図を参照し
て以下に説明する。The operation of the vibrator configured as described above will be explained below with reference to FIG.
まず、第1圧電体12に周波数fの交流電圧を印加して
振動させると、前記板状弾性体16は縦振動1次モード
で共振し、図中点Aは+X方向に伸びる。このとき、該
板状弾性体16は、曲げ振動2次モードにおいても共振
し、図中点Aは+y力方向動く。First, when an AC voltage of frequency f is applied to the first piezoelectric body 12 to cause it to vibrate, the plate-like elastic body 16 resonates in the first-order mode of longitudinal vibration, and point A in the figure extends in the +X direction. At this time, the plate-like elastic body 16 also resonates in the second-order mode of bending vibration, and point A in the figure moves in the +y force direction.
次に、第2圧電体13に周波数fで前記第1圧電体12
に印加した交流電圧と同相の電圧を印加して振動させる
と前記板状弾性体16は縦振動1次モードで共振し、図
中点Aは+X方向に伸びる。Next, the first piezoelectric body 12 is applied to the second piezoelectric body 13 at a frequency f.
When a voltage in phase with the AC voltage applied to is applied to vibrate, the plate-shaped elastic body 16 resonates in the first mode of longitudinal vibration, and point A in the figure extends in the +X direction.
このとき、該板状弾性体16は、曲げ振動2次モトにお
いても共振し、図中点Aは−y力方向動く。At this time, the plate-like elastic body 16 also resonates in the second-order bending vibration, and the point A in the figure moves in the -y force direction.
すなわち、前記第1圧電体12及び第2圧電体13を同
時に振動させると、両圧電体に印加される電圧が同相の
ときは前記曲げ振動がまったく打ち消され、y方向には
振幅が現れない。また、前記両圧電体に印加される電圧
が逆相のときは、前記縦振動がまったく打ち消され、X
方向には振幅が現れない。That is, when the first piezoelectric body 12 and the second piezoelectric body 13 are vibrated simultaneously, when the voltages applied to both piezoelectric bodies are in the same phase, the bending vibration is completely canceled and no amplitude appears in the y direction. Furthermore, when the voltages applied to both piezoelectric bodies are of opposite phase, the longitudinal vibration is completely canceled out, and the
No amplitude appears in the direction.
このように、2つの圧電体12及び13に印加する電圧
の位相を調節することで、前記板状弾性体16の端部A
点には任意の形状の略楕円振動を発生する事が可能とな
る。In this way, by adjusting the phase of the voltage applied to the two piezoelectric bodies 12 and 13, the end portion A of the plate-like elastic body 16 can be adjusted.
It is possible to generate approximately elliptical vibration of any shape at a point.
以上のような超音波振動子11において、2つの圧電体
12及び13により発生した振動を効率良く板状弾性体
16に伝えるために、該圧電体12及び13と板状弾性
体16との間に、複数の傾斜片が形成された結合子21
及び22をはさむ事も可能である。前記圧電体12及び
13で発生された厚さ振動は、該結合子によって振動方
向が変換され、前記板状弾性体16に効率良く縦振動を
発生する。In the ultrasonic vibrator 11 as described above, in order to efficiently transmit the vibrations generated by the two piezoelectric bodies 12 and 13 to the plate-like elastic body 16, there is a gap between the piezoelectric bodies 12 and 13 and the plate-like elastic body 16. A connector 21 on which a plurality of inclined pieces are formed.
It is also possible to sandwich 22 and 22. The vibration direction of the thickness vibration generated in the piezoelectric bodies 12 and 13 is changed by the coupler, and longitudinal vibration is efficiently generated in the plate-shaped elastic body 16.
次に以上のような超音波振動子11を好適に利用するリ
ニア超音波モータの構成について、第5図に基づき説明
する。同図において、第1図乃至第4図と同じ符号の付
された各部材は前記詳述した各構成部材と同一である事
を意味している。Next, the configuration of a linear ultrasonic motor that suitably utilizes the ultrasonic transducer 11 as described above will be explained based on FIG. 5. In this figure, each member given the same reference numeral as in FIGS. 1 to 4 means the same as each component described in detail above.
リニア超音波モータ31は、ヨーク32に前記超音波振
動子11が固定されており、該超音波振動子11の板状
弾性体16の端部に出力部33が形成されている。In the linear ultrasonic motor 31, the ultrasonic transducer 11 is fixed to a yoke 32, and an output section 33 is formed at the end of the plate-shaped elastic body 16 of the ultrasonic transducer 11.
該出力部33には、可動子34が板バネ35により圧着
されており、該板バネの一端はヨーク32に固定されて
いる。A movable element 34 is crimped to the output portion 33 by a leaf spring 35, and one end of the leaf spring is fixed to the yoke 32.
上述のように構成されたリニア超音波モータ31におい
て、超音波振動子11を励振すると、前記可動子34は
前記板状弾性体16の略楕円浸透による駆動力を受け、
図中矢印Bの方向に動く。In the linear ultrasonic motor 31 configured as described above, when the ultrasonic vibrator 11 is excited, the movable element 34 receives a driving force due to approximately elliptical penetration of the plate-like elastic body 16,
It moves in the direction of arrow B in the figure.
この駆動力は、前記板状弾性体16と前記可動子34と
の摩擦力によって発生するものである。This driving force is generated by the frictional force between the plate-shaped elastic body 16 and the movable element 34.
なお、上記実施例は振動子の駆動素子として圧電体を使
用したが、これに限定されるものではなく電気エネルギ
ーを機械エネルギーに変換できるその他の素子、例えば
電歪素子、磁歪素子等を用いてもよい。また、実施例で
は超音波振動子の形状を平板状とする例について説明し
たが長さ方向に振動、軸方向に曲げ振動が励起され、略
楕円運動が発生するものならばその形状は平板形状に限
定されるものではない。その他、本発明の趣旨を逸脱し
ない範囲で種々の変形が可能である。Although the above embodiment uses a piezoelectric material as the driving element of the vibrator, it is not limited to this, and other elements capable of converting electrical energy into mechanical energy, such as an electrostrictive element or a magnetostrictive element, may be used. Good too. In addition, in the embodiment, an example was explained in which the shape of the ultrasonic transducer is a flat plate, but if vibration is excited in the length direction and bending vibration is excited in the axial direction, and approximately elliptical motion is generated, the shape is a flat plate. It is not limited to. In addition, various modifications can be made without departing from the spirit of the present invention.
[発明の効果]
以上詳述したことから明らかなように、本発明によれば
、弾性体に不要振動を発生させないので、弾性体や励振
体の構成条件の自由度が大きく、高効率、大出力動作が
可能な超音波振動子を提供する事ができる。[Effects of the Invention] As is clear from the detailed description above, according to the present invention, unnecessary vibrations are not generated in the elastic body, so there is a large degree of freedom in the configuration conditions of the elastic body and the exciting body, and high efficiency and large An ultrasonic transducer capable of output operation can be provided.
該超音波振動子を好適に利用する事により、高効率、大
出力の特性を備え、しかも略楕円運動軌跡が容易に制御
できる超音波モータを提供する事ができる。By appropriately utilizing the ultrasonic vibrator, it is possible to provide an ultrasonic motor that has characteristics of high efficiency and large output, and can easily control a substantially elliptical motion locus.
第1図から第5図までは本発明を具体化した実施例を示
すもので、第1図は本発明を適用する超音波振動子の側
面図、第2図は上記超音波振動子の分解斜視図、第3図
は超音波振動子における励振位置と振幅を対比して示す
図、第4図は他の実施例としての超音波振動子の分解斜
視図、第5図は上記超音波振動子を適用したリニア超音
波モータの側面図である。
図中、12は第1励振体に対応する第1圧電素子、13
は第2励振体に対応する第2圧電素子、14は保持部に
対応するボルト、16は弾性体に対応する板状弾性体、
21.22は結合子、34は可動子である。1 to 5 show embodiments embodying the present invention. FIG. 1 is a side view of an ultrasonic transducer to which the present invention is applied, and FIG. 2 is an exploded view of the ultrasonic transducer. A perspective view, FIG. 3 is a diagram showing a comparison of the excitation position and amplitude in an ultrasonic vibrator, FIG. 4 is an exploded perspective view of an ultrasonic vibrator as another embodiment, and FIG. 5 is a diagram showing the above-mentioned ultrasonic vibration. FIG. 2 is a side view of a linear ultrasonic motor to which a child is applied. In the figure, 12 is a first piezoelectric element corresponding to the first exciter, 13
14 is a bolt corresponding to the holding part; 16 is a plate-shaped elastic body corresponding to the elastic body;
21 and 22 are connectors, and 34 is a mover.
Claims (5)
対し大略同一周波数で共振する弾性体と、該弾性体の第
1方向及び第2方向の双方に対し同時に前記周波数の振
動を励振する第1励振体と、前記弾性体の第1方向及び
第2方向の双方に対し同時に前記周波数の振動を励振し
、かつ、両振動の位相関係が前記第1励振体の場合と逆
相となる第2励振体とを有すことを特徴とする超音波振
動子。1. an elastic body that resonates at substantially the same frequency in a first direction and a second direction substantially orthogonal to the first direction, and simultaneously exciting vibrations at the frequency in both the first direction and the second direction of the elastic body; Vibration of the frequency is simultaneously excited in both the first direction and the second direction of the first exciting body and the elastic body, and the phase relationship of both vibrations is opposite to that of the first exciting body. An ultrasonic transducer comprising a second excitation body.
向振動は少なくとも一つ以上の一致する節を有し、該節
部の重なりとなる位置を保持する保持部を有すことを特
徴とする超音波振動子。2. 2. The ultrasonic transducer according to claim 1, wherein the two-way vibration has at least one coinciding node, and the ultrasonic vibrator has a holding part that holds the overlapping nodes. Sound wave vibrator.
動方向を変換するための結合子を備え、かつ該結合子の
前記板状弾性体との当接面に複数の傾斜片が形成されて
いる事を特徴とする超音波振動子。3. The ultrasonic vibrator according to claim 1 or 2, further comprising a connector for converting a vibration direction between the elastic body and at least one of the respective excitation bodies, and the plate-like elastic body of the connector. An ultrasonic transducer characterized in that a plurality of inclined pieces are formed on the contact surface with the ultrasonic transducer.
、 前記弾性体に少なくとも曲げ振動と縦振動が励振され、 前記第1励振体及び第2励振体は、該板状弾性体の同一
面上でかつ該曲げ振動の逆相となる腹の位置に着設され
ている事を特徴とする超音波振動子。4. The ultrasonic transducer according to claim 2 or 3, wherein at least bending vibration and longitudinal vibration are excited in the elastic body, and the first excitation body and the second excitation body are arranged on the same surface of the plate-like elastic body. An ultrasonic vibrator characterized in that the ultrasonic vibrator is installed at an antinode position that is in the opposite phase of the bending vibration.
、可動子を当接した事を特徴とする超音波モータ。5. An ultrasonic motor comprising a movable element in contact with the ultrasonic vibrator according to any one of claims 1 to 4.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1046865A JPH02228266A (en) | 1989-02-28 | 1989-02-28 | Ultrasonic vibrator and ultrasonic motor |
US07/485,517 US5039899A (en) | 1989-02-28 | 1990-02-27 | Piezoelectric transducer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1046865A JPH02228266A (en) | 1989-02-28 | 1989-02-28 | Ultrasonic vibrator and ultrasonic motor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02228266A true JPH02228266A (en) | 1990-09-11 |
Family
ID=12759237
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1046865A Pending JPH02228266A (en) | 1989-02-28 | 1989-02-28 | Ultrasonic vibrator and ultrasonic motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02228266A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2016092879A (en) * | 2014-10-30 | 2016-05-23 | キヤノン株式会社 | Vibrator and ultrasonic motor |
-
1989
- 1989-02-28 JP JP1046865A patent/JPH02228266A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2016092879A (en) * | 2014-10-30 | 2016-05-23 | キヤノン株式会社 | Vibrator and ultrasonic motor |
US10069440B2 (en) | 2014-10-30 | 2018-09-04 | Canon Kabushiki Kaisha | Vibrator and ultrasonic motor |
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