JP2625653B2 - Vibration wave motor - Google Patents
Vibration wave motorInfo
- Publication number
- JP2625653B2 JP2625653B2 JP7098595A JP9859595A JP2625653B2 JP 2625653 B2 JP2625653 B2 JP 2625653B2 JP 7098595 A JP7098595 A JP 7098595A JP 9859595 A JP9859595 A JP 9859595A JP 2625653 B2 JP2625653 B2 JP 2625653B2
- Authority
- JP
- Japan
- Prior art keywords
- vibration
- diaphragm
- energy conversion
- mechanical energy
- electro
- 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
Links
Landscapes
- Apparatuses For Generation Of Mechanical Vibrations (AREA)
- General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)
Description
【0001】[0001]
【発明の利用分野】本発明は進行性振動波により進行駆
動する振動波モータの改良に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an improved vibration wave motor driven by traveling vibration waves.
【0002】[0002]
【発明の背景】前記振動波モータは移動体の進行方向に
沿って多数配置した電気−機械エネルギー変換素子例え
ば電歪素子により弾性体からなる振動板に曲げ進行波を
つくり、その駆動力により振動板上に載置された移動体
を駆動するもので、従来公知の一例を図5及び図6に示
す。図中、1は長円形の閉ループをなす弾性体からなる
振動板で2は電歪素子である。電歪素子2は、前記振動
板1の二つの直線部の各々にA相、B相の2組に分かれ
て1/4波長(λ/4)の位相差をもって図示の如く配
置され、それぞれの相はλ/2間隔で+,−交互に接合
されている。3は前記振動板1上に圧接された接触体と
しての移動体で、4は振動板の支持材である。BACKGROUND OF THE INVENTION The vibration wave motor generates a bending traveling wave on a diaphragm made of an elastic body by means of an electro-mechanical energy conversion element such as an electrostrictive element which is arranged along the traveling direction of a moving body, and vibrates by its driving force. FIGS. 5 and 6 show one example of a conventionally known device for driving a moving body placed on a plate. In the drawing, reference numeral 1 denotes a diaphragm made of an elastic body forming an oval closed loop, and 2 denotes an electrostrictive element. The electrostrictive element 2 is divided into two sets of A-phase and B-phase on each of the two linear portions of the diaphragm 1 and arranged with a phase difference of 波長 wavelength (λ / 4) as shown in the drawing. The phases are alternately joined at +/- intervals at [lambda] / 2. Reference numeral 3 denotes a moving body as a contact body pressed against the diaphragm 1, and reference numeral 4 denotes a support for the diaphragm.
【0003】前記A相,B相の電歪素子2,2…に90
°の位相差の交番電圧を印加すると振動板1に曲げ進行
波が発生し、移動体3は振動板1との接触部における摩
擦力により振動板1に沿って移動する。直線駆動型の振
動波モータは上記した様に直線部と円弧部を有してお
り、定在波を発生させた時の振動モードは、単純形状の
円形或いは直線梁と比べ複雑になる。また、振動板1に
は電歪素子2が接合されているため接合部では振動板の
剛性が他の部分と異なる事により、さらに振動モードが
複雑になる。このため前記した様にA相,B相でλ/4
の位相差をもって定在波をつくっているが、上記の要因
により波長の長短等のずれが起こり、各相の定在波の腹
の位置と電歪素子2の中心とがずれてしまうので、これ
ら2つの定在波を重ね合わせた進行波は振幅が不均一と
なりモータの性能上の不利益を免かれない。The A-phase and B-phase electrostrictive elements 2, 2,.
When an alternating voltage having a phase difference of 0 ° is applied, a bending traveling wave is generated in the diaphragm 1, and the moving body 3 moves along the diaphragm 1 by a frictional force at a contact portion with the diaphragm 1. As described above, a linear drive type vibration wave motor has a straight portion and a circular arc portion, and the vibration mode when a standing wave is generated is more complicated than a simple circular or straight beam. Further, since the electrostrictive element 2 is joined to the diaphragm 1, the rigidity of the diaphragm is different from that of the other portions at the joining portion, so that the vibration mode is further complicated. For this reason, as described above, A / 4
Although the standing wave is created with the phase difference of the above, a shift such as the length of the wavelength occurs due to the above factors, and the position of the antinode of the standing wave of each phase and the center of the electrostrictive element 2 are shifted. The traveling wave obtained by superimposing these two standing waves has a non-uniform amplitude, and a disadvantage in the performance of the motor cannot be avoided.
【0004】[0004]
【発明の目的】本発明の目的は、上記従来例の欠点を改
善し、効率的に振動エネルギーを振動体に伝達して有効
に振動板振幅を取り出し、もって振幅の揃った進行波が
得られる改良された振動波モータを提供することにあ
る。SUMMARY OF THE INVENTION It is an object of the present invention to improve the drawbacks of the prior art and to efficiently transmit vibration energy to a vibrating body to effectively extract a diaphragm amplitude, thereby obtaining a traveling wave having a uniform amplitude. An object of the present invention is to provide an improved vibration wave motor.
【0005】[0005]
【発明の概要】本出願に係る発明の目的を実現する構成
は、直線部と円弧部を有する長円形の振動体に、該振動
体の周長より短い長さとなる2組の電気−機械エネルギ
ー変換素子群を接合することによって、少なくとも前記
電気−機械エネルギー変換素子群の非接合領域を設け、
該素子群によって振動体に発生される進行性振動波によ
り振動体上の接触体と該接触体とを直線的に相対移動さ
せる振動波モータにおいて、前記2組の電気−機械エネ
ルギー変換素子群の全ての個々の電気−機械エネルギー
変換素子の中心を、前記振動体に発生する各組の定在波
の腹の位置と実質上一致させたものである。SUMMARY OF THE INVENTION A configuration for realizing the object of the invention according to the present application
Is an oblong vibrating body having a linear portion and an arc portion,
Two sets of electro-mechanical energy that are shorter than the circumference of the body
-By joining the conversion element group, at least
Providing a non-joining region of the electro-mechanical energy conversion element group,
The progressive vibration wave generated in the vibrating body by the element group
The contact body on the vibrating body and the contact body are linearly moved relative to each other.
The two sets of electro-mechanical energy
All individual electro-mechanical energies of the energy conversion elements
The center of the conversion element, the standing wave of each set generated in the vibrating body
Is substantially matched with the position of the belly .
【0006】[0006]
【発明の実施例】図1は本発明による振動波モータの一
実施例におけるステータの構成を示し、同図中1は振動
体としての振動板で2は電気−機械エネルギー変換素子
としての電歪素子である。1箇の電歪素子2についてそ
の表裏の電極に交番電圧を加えると該電歪素子2は伸縮
するため、振動板に接合すると図2に示す様に振動板1
が曲げられ電歪素子2の中央が定在波の腹になる様な振
動をする。また、長円形の振動板1の定在波は、図3
(a)(b)に示す様に振動板の中心軸に対し対称な位
置に節が出来る振動特性をもっている。このため図3
(a)(b)に示す各定在波の振動モードの腹の位置と
各電歪素子の中心とが合う様に電歪素子を振動板に接合
すると効率よく励振できる。FIG. 1 shows a configuration of a stator in an embodiment of a vibration wave motor according to the present invention. In FIG. 1, reference numeral 1 denotes a diaphragm as a vibrating body and 2 denotes an electrostriction as an electromechanical energy conversion element. Element. When an alternating voltage is applied to the electrodes on the front and back of one electrostrictive element 2, the electrostrictive element 2 expands and contracts.
Vibrates so that the center of the electrostrictive element 2 becomes the antinode of the standing wave. The standing wave of the elliptical diaphragm 1 is shown in FIG.
(A) As shown in (b), the diaphragm has a vibration characteristic in which nodes are formed at symmetrical positions with respect to the center axis of the diaphragm. Therefore, FIG.
(A) When the electrostrictive element is joined to the diaphragm so that the antinode position of the vibration mode of each standing wave shown in (b) is aligned with the center of each electrostrictive element, efficient excitation can be achieved.
【0007】また振動板1に電歪素子2を接合する事に
より接合部の剛性が変化して図3(a)(b)の様な一
様な波長の振動は得られないが、電歪素子を接合してい
ない側の直線部ではこれらによる影響が少なく揃った振
動が得られるものである。したがって、図1に示す様に
片側の直線部の表面にA相をつくり、裏面のA相のλ/
4の位相差をもってB相をつくると他方の直線部には振
幅の揃った進行波を得ることができる。またステータ全
体としての剛性を中心軸S’に関して対称にするためB
相は図示の様に中心位置の電歪素子をぬいている。When the electrostrictive element 2 is joined to the diaphragm 1, the rigidity of the joint changes, so that a vibration having a uniform wavelength as shown in FIGS. 3A and 3B cannot be obtained. In the straight portion on the side where the element is not joined, uniform vibration is obtained with little influence of these. Therefore, as shown in FIG. 1, an A-phase is formed on the surface of the straight portion on one side, and the λ /
When the B phase is formed with a phase difference of 4, a traveling wave having the same amplitude can be obtained in the other linear portion. Further, in order to make the rigidity of the entire stator symmetrical with respect to the central axis S ′, B
The phases wipe the electrostrictive element at the center as shown.
【0008】上記のように構成したことによりA相とB
相の駆動周波数もよく一致し効率よく駆動する事が可能
である。[0008] With the above construction, the phase A and the phase B
The driving frequencies of the phases match well, and efficient driving is possible.
【0009】図4に本発明による他の実施例を示す。こ
の実施例において振動板1は幅に対し高さが高い長方形
断面形状をしており電歪素子2は振動板1の片側の直線
部の両側面にλ/4の位相差をもって接合されている。
A相,B相にはそれぞれ90°の位相差をもった交番電
圧が印加され振動板1には、図4の矢印A方向に進行波
が発生し、この進行波によって接触体としての移動体3
が矢印方向Bに駆動される。FIG. 4 shows another embodiment according to the present invention. In this embodiment, the diaphragm 1 has a rectangular cross-sectional shape whose height is higher than the width, and the electrostrictive element 2 is joined to both side surfaces of one straight portion of the diaphragm 1 with a phase difference of λ / 4. .
An alternating voltage having a phase difference of 90 ° is applied to each of the A phase and the B phase, and a traveling wave is generated in the diaphragm 1 in the direction of arrow A in FIG. 3
Is driven in the arrow direction B.
【0010】尚本実施例の説明では振動板に接合される
素子は、電歪素子としたが、他に磁歪素子、圧電素子等
の電気−機械エネルギー変換素子のいずれであってもよ
い。In the description of this embodiment, the element to be joined to the diaphragm is an electrostrictive element, but may be any other electro-mechanical energy converting element such as a magnetostrictive element or a piezoelectric element.
【0011】[0011]
【発明の効果】以上説明したように、本発明によれば、
直線部と円弧部を有する長円形の振動体に、該振動体の
周長より短い長さとなる2組の電気−機械エネルギー変
換素子群を接合することによって、少なくとも前記電気
−機械エネルギー変換素子群の非接合領域を設け、該素
子群によって振動体に発生される進行性振動波により振
動体上の接触体と該接触体とを直線的に相対移動させる
振動波モータにおいて、前記2組の電気−機械エネルギ
ー変換素子群の全ての個々の電気−機械エネルギー変換
素子の中心を、前記振動体に発生する各組の定在波の腹
の位置と実質上一致させたため、以下のような効果が得
られる。As described above, according to the present invention,
An elliptical vibrating body having a linear portion and an arc portion
Two sets of electro-mechanical energy changes that are shorter than the circumference
By joining the exchange element group, at least the electric
Providing a non-bonding region for the mechanical energy conversion element group,
Vibration generated by the vibrating body
The contact body on the moving body is linearly moved relative to the contact body
In an oscillatory wave motor, the two sets of electro-mechanical energy
-All individual electro-mechanical energy conversion of the conversion elements
The center of the element is positioned at the antinode of each set of standing waves generated in the vibrator.
The following effects can be obtained
Can be
【0012】1.効率的に振動エネルギーを振動体に伝
達できる。1. Vibration energy can be efficiently transmitted to the vibrating body.
【0013】2.上記1により有効に振動体振幅を取り
出せる。2. By the above 1, the vibration body amplitude can be effectively taken out.
【0014】3.振幅の揃った進行波が得られる。3. A traveling wave with uniform amplitude is obtained.
【0015】4.2組の電気−機械エネルギー変換素子
群の駆動周波数の差を少なくできる。[0015] The difference in drive frequency between the two sets of electromechanical energy conversion elements can be reduced.
【図1】本発明による振動波モータの一実施例における
ステータの構成図を示す。FIG. 1 shows a configuration diagram of a stator in an embodiment of a vibration wave motor according to the present invention.
【図2】振動波発生の原理を示す。FIG. 2 shows the principle of vibration wave generation.
【図3】(a),(b)は長円形振動板の2種類の定在
波の面外曲げ振動モードを示す。3 (a) and 3 (b) show out-of-plane bending vibration modes of two types of standing waves of an oval diaphragm.
【図4】本発明による他の実施例を示す。FIG. 4 shows another embodiment according to the present invention.
【図5】従来の振動波リニアモータの外観図および同モ
ータのステータ構成図である。FIG. 5 is an external view of a conventional vibration wave linear motor and a stator configuration diagram of the motor.
【図6】従来の振動波リニアモータの外観図および同モ
ータのステータ構成図である。FIG. 6 is an external view of a conventional vibration wave linear motor and a stator configuration diagram of the motor.
【符号の説明】 1…長円形振動板 2…電歪素子 3…移動体 4…防振支持材[Explanation of Signs] 1: Oval diaphragm 2: Electrostrictive element 3: Moving body 4: Vibration-proof support
Claims (1)
に、該振動体の周長より短い長さとなる2組の電気−機
械エネルギー変換素子群を接合することによって、少な
くとも前記電気−機械エネルギー変換素子群の非接合領
域を設け、該素子群によって振動体に発生される進行性
振動波により振動体上の接触体と該接触体とを直線的に
相対移動させる振動波モータにおいて、 前記2組の電気−機械エネルギー変換素子群の全ての個
々の電気−機械エネルギー変換素子の中心を、前記振動
体に発生する各組の定在波の腹の位置と実質上一致させ
たことを特徴とする振動波モータ。To 1. A oblong vibrator having a straight portion and an arc portion, two sets of electric to be shorter than the circumferential length the length of the vibrator - by joining the mechanical energy conversion element groups, small
At least the non-joining area of the electro-mechanical energy conversion element group
The band is provided, in the vibration wave motor linearly moved relative to the contact body and the contact body on the vibrating body by traveling vibration waves generated in the vibration member by the element group, said two sets of electrical - mechanical All of the energy conversion elements
A vibration wave motor, wherein the center of each of the electro-mechanical energy conversion elements substantially coincides with the position of the antinode of each set of standing waves generated in the vibrating body.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7098595A JP2625653B2 (en) | 1995-04-24 | 1995-04-24 | Vibration wave motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7098595A JP2625653B2 (en) | 1995-04-24 | 1995-04-24 | Vibration wave motor |
Related Parent Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP60066092A Division JPH0632570B2 (en) | 1985-03-29 | 1985-03-29 | Vibration wave motor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0884488A JPH0884488A (en) | 1996-03-26 |
JP2625653B2 true JP2625653B2 (en) | 1997-07-02 |
Family
ID=14223993
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP7098595A Expired - Lifetime JP2625653B2 (en) | 1995-04-24 | 1995-04-24 | Vibration wave motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2625653B2 (en) |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6135177A (en) * | 1984-07-27 | 1986-02-19 | Matsushita Electric Ind Co Ltd | Piezoelectric linear motor |
-
1995
- 1995-04-24 JP JP7098595A patent/JP2625653B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPH0884488A (en) | 1996-03-26 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
EXPY | Cancellation because of completion of term |