JPH0619339Y2 - Ultrasonic linear motor - Google Patents

Ultrasonic linear motor

Info

Publication number
JPH0619339Y2
JPH0619339Y2 JP13515687U JP13515687U JPH0619339Y2 JP H0619339 Y2 JPH0619339 Y2 JP H0619339Y2 JP 13515687 U JP13515687 U JP 13515687U JP 13515687 U JP13515687 U JP 13515687U JP H0619339 Y2 JPH0619339 Y2 JP H0619339Y2
Authority
JP
Japan
Prior art keywords
elastic base
driving
nodes
linear motor
vibrator
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
Application number
JP13515687U
Other languages
Japanese (ja)
Other versions
JPS6440294U (en
Inventor
一正 大西
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Alps Alpine Co Ltd
Original Assignee
Alps Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Alps Electric Co Ltd filed Critical Alps Electric Co Ltd
Priority to JP13515687U priority Critical patent/JPH0619339Y2/en
Publication of JPS6440294U publication Critical patent/JPS6440294U/ja
Application granted granted Critical
Publication of JPH0619339Y2 publication Critical patent/JPH0619339Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【考案の詳細な説明】 「技術分野」 本考案は、圧電振動子または電歪振動子を用いたリニア
モータに関する。
TECHNICAL FIELD The present invention relates to a linear motor using a piezoelectric vibrator or an electrostrictive vibrator.

「従来技術およびその問題点」 圧電振動子や電歪振動子を利用したモータは、従来各種
提案されているが、特開昭58-148682号は振動子の界面
に励振される横波と縦波の合成された進行波によって駆
動力を得るモータを提案している。この超音波振動を利
用したモータは、その進行波を縦波と横波を合成して得
ているために、電歪素子に特定の分極処理を施し、これ
らに位相の異なる二つ以上の周波電圧を振動子に印加し
なければならない。このためその製造工程が複雑で、ま
た電源回路も複雑なものを要した。
"Prior art and its problems" Various types of motors using piezoelectric vibrators and electrostrictive vibrators have been proposed in the past, but JP-A-58-148682 discloses a transverse wave and a longitudinal wave excited at the interface of the vibrator. Has proposed a motor which obtains a driving force by the traveling wave synthesized by the above. A motor that uses this ultrasonic vibration obtains its traveling wave by combining longitudinal and transverse waves.Therefore, the electrostrictive element is subjected to a specific polarization process, and these two or more frequency voltages with different phases are applied. Must be applied to the oscillator. Therefore, the manufacturing process is complicated and the power supply circuit is also complicated.

「考案の目的」 本考案は、以上の超音波モータとは異なる動作原理によ
って作動し、製造が容易で、かつ振動子として特別なも
のを要しない、新規な超音波リニアモータを得ることを
目的とする。
[Purpose of Invention] The present invention aims to obtain a novel ultrasonic linear motor that operates according to a different operation principle from the ultrasonic motors described above, is easy to manufacture, and does not require a special vibrator. And

「考案の概要」 本考案のリニアモータは、複数の駆動足を、隣り合うも
の同士共振周波数を異ならせて弾性基体の節と節の間に
一つづつ設け、これらの駆動足のそれぞれに、対応する
圧電振動子または電歪振動子によって振動を与えると、
隣り合う一方の駆動足の方は、弾性基体の正のたわみ変
形に応じてたわみ共振するが、他方の駆動足の方は、弾
性基体が負のたわみ変形によって足自体はたわみ振動を
せず、その結果、リニアな駆動力が得られることに着目
してなされたものである。
[Outline of the Invention] The linear motor of the present invention is provided with a plurality of drive feet, one for each of the adjacent ones of the elastic base, with different resonance frequencies between adjacent ones. When vibration is applied by the corresponding piezoelectric vibrator or electrostrictive vibrator,
One of the driving feet adjacent to each other flexurally resonates according to the positive flexural deformation of the elastic base, while the other driving foot does not flexurally vibrate itself due to the negative flexural deformation of the elastic base, As a result, it was made paying attention to obtaining a linear driving force.

すなわち本考案は、少なくとも三つのたわみ変動の節を
有し、各節が剛体により支持された弾性基体の各節間の
腹部に、隣り合うもの同士が共振周波数の異なる少なく
とも二本の駆動足を設け、かつこの弾性基体に、該弾性
基体を正負の関係でたわみ変形させるとともに各駆動足
に振動を与える、各駆動足に対応した圧電振動子または
電歪振動子を設け、この圧電振動子または電歪振動子に
所定の周波電圧を印加することを特徴とする。
That is, according to the present invention, at least two driving feet having different resonance frequencies are provided in the abdomen between the nodes of the elastic base body having at least three flexural fluctuation nodes, each node being supported by a rigid body. A piezoelectric vibrator or an electrostrictive vibrator corresponding to each driving foot is provided on the elastic base, which flexibly deforms the elastic base in a positive / negative relationship and gives vibration to each driving foot. A feature is that a predetermined frequency voltage is applied to the electrostrictive vibrator.

上記弾性基体の各節間の正または負のたわみ変形と各駆
動足のたわみ共振は、各駆動足の特定共振周波数、およ
び圧電振動子または電歪振動子に加える周波電圧の周波
数によって変化する。よって周波数を変化させることに
よって、弾性基体と駆動足とを備えた移動子の移動速度
の調整および移動方向の変換を行なうことができる。
The positive or negative flexural deformation between the nodes of the elastic substrate and the flexural resonance of each driving foot change depending on the specific resonance frequency of each driving foot and the frequency of the frequency voltage applied to the piezoelectric vibrator or the electrostrictive vibrator. Therefore, by changing the frequency, it is possible to adjust the moving speed and change the moving direction of the moving element having the elastic base and the driving foot.

「考案の実施例」 以下図示実施例について本考案を説明する。第1図、第
2図は本考案による超音波リニアモータの一つの実施例
を示すものである。移動子10は、弾性基体11と二本
の駆動足12、13を備えている。弾性基体11は、た
わみ振動をするもので、所定間隔Lの少なくとも三つの
たわみ振動における節F1,F2,F3を有しており、この各節
F1,F2,F3が剛性枠体14に支持されている。したがっ
て、この弾性基体11は、各節にが所定周波電圧が与え
られると、たわみ変形(変動)する。また、駆動足1
2、13は、この弾性基体11の各節F1,F2,F3の中間、
すなわち腹の部分に固定されており、それぞれの下端面
が走行面20と接触する。そして、弾性基体11には、
各駆動足12,13に対応した圧電振動子または電歪振
動子(以下単に振動子という)15,16が設けられて
いる。これらの要素の接着は例えばエポキシ樹脂系の接
着材によって行なうことができる。
"Embodiment of the Invention" The present invention will be described below with reference to illustrated embodiments. 1 and 2 show one embodiment of an ultrasonic linear motor according to the present invention. The mover 10 includes an elastic base 11 and two drive legs 12 and 13. The elastic base body 11 is for flexural vibration, and has at least three flexural vibration nodes F1, F2, F3 at a predetermined interval L.
F1, F2 and F3 are supported by the rigid frame body 14. Therefore, the elastic substrate 11 is flexibly deformed (changed) when a predetermined frequency voltage is applied to each node. Also, drive foot 1
2 and 13 are intermediate points of the nodes F1, F2, F3 of the elastic base 11,
That is, they are fixed to the belly portion, and their lower end surfaces come into contact with the running surface 20. And, in the elastic substrate 11,
Piezoelectric vibrators or electrostrictive vibrators (hereinafter simply referred to as vibrators) 15 and 16 corresponding to the drive feet 12 and 13 are provided. Adhesion of these elements can be performed by using, for example, an epoxy resin adhesive.

移動子10は、弾性材料、例えばアルミニウム、黄銅、
ステンレス、鉄、合成樹脂材料、セラミック材料、ガラ
ス材料、あるいはこれらを複合した複合材料等、振動を
良好に伝達し得る弾性材料(音響材料)から構成され
る。
The mover 10 is made of an elastic material such as aluminum, brass,
It is composed of an elastic material (acoustic material) capable of favorably transmitting vibration, such as stainless steel, iron, a synthetic resin material, a ceramic material, a glass material, or a composite material combining these materials.

また振動子15,16は、積層型の圧電または電歪素
子、単板の圧電または電歪素子から構成されるもので、
駆動周波電圧を加えると、それ自体がその周波電圧の周
波数に応じた周波数で伸縮する。そしてこの伸縮(振
動)が、弾性基体11を正負いずれかの方向にたわみ変
形させ、駆動足12と13に増幅されて伝達される。
The vibrators 15 and 16 are composed of laminated piezoelectric or electrostrictive elements or single-plate piezoelectric or electrostrictive elements.
When a drive frequency voltage is applied, the drive frequency expands and contracts at a frequency corresponding to the frequency of the frequency voltage. Then, this expansion / contraction (vibration) causes the elastic base 11 to be flexibly deformed in either the positive or negative direction, and is amplified and transmitted to the drive legs 12 and 13.

そして本考案は、以上の移動子10の駆動足12と13
の共振周波数を異ならせたうえで、弾性基体11をこの
異なる共振周波数に同期させた関係で、たわみ振動させ
る。つまり、節と節の間の一方が下方変形(これを正と
する)するとき、他方が上方変形(これを負とする)す
る関係に位相を異ならせるべく、対応する振動子15と
16に別々に所定周波数の駆動電圧を加えるようにした
ものである。駆動足12と13の共振周波数は、例えば
その厚さ、材質あるいは長さ等を違えることにより異な
らせることができる。この共振周波数は、振動子15と
16に加える駆動電圧の周波数を勘案して決定する。ま
た、弾性基体11のたわみ変形方向は、駆動足12と1
3の共振周波数に合わせられる。そして、振動子15と
16の駆動電圧の周波数を適宜変更することで、移動子
10の移動方向を変えることができ、駆動電圧の印加量
を変えることで、移動子19の移動速度を変えることが
できる。このように駆動足12と13の異なる共振周波
数を、対応する振動子15と16に加える駆動電圧の周
波数と同一に設定すると、最も効率的に、駆動足12と
13を振動させてリニアな駆動力を得ることができる。
The present invention is based on the driving feet 12 and 13 of the moving element 10 described above.
The resonance frequencies of the elastic base 11 and the elastic base 11 are flexibly vibrated in synchronization with the different resonance frequencies. That is, when one of the nodes between the nodes deforms downward (this is positive), the other vibrators 15 and 16 have different phases so that the other deforms upward (this is negative). The driving voltage of a predetermined frequency is separately applied. The resonance frequencies of the drive legs 12 and 13 can be made different by changing their thickness, material, length, or the like. The resonance frequency is determined in consideration of the frequency of the drive voltage applied to the vibrators 15 and 16. In addition, the direction of flexural deformation of the elastic base 11 is such that the drive feet 12 and 1
Tuned to a resonance frequency of 3. The moving direction of the moving element 10 can be changed by appropriately changing the frequency of the driving voltage of the vibrators 15 and 16, and the moving speed of the moving element 19 can be changed by changing the application amount of the driving voltage. You can In this way, when the different resonance frequencies of the drive feet 12 and 13 are set to be the same as the frequency of the drive voltage applied to the corresponding vibrators 15 and 16, the drive feet 12 and 13 are oscillated most efficiently for linear drive. You can get the power.

上記構成の本超音波リニアモータは、振動子15と16
に異なった所定の駆動周波数の駆動電圧を同時に与える
と、移動子10は、第2図(A),(B)に示すように右行ま
たは左行する。
The ultrasonic linear motor having the above-described configuration is provided with the vibrators 15 and 16
When driving voltages having different predetermined driving frequencies are simultaneously applied to the moving elements, the mover 10 moves rightward or leftward as shown in FIGS. 2 (A) and 2 (B).

その理由は次の通りであると考えられる。いま振動子1
5と16に異なった所定周波数の駆動電圧を与えると、
弾性基体11における節F1とF2との間、および節F2とF3
との間が、与えられたそれぞれの周波数に応じて、一方
が下方(正方向)変動しているとき他方は上方(負方
向)変動する関係でたわみ変形する。例えば、節F1とF2
の間が正変形、節F2とF3の間が負変形したとする。する
と、同時に、駆動足12と13も上下に振動(たて振
動)する。駆動足12と13には、それぞれその共振周
波数と同一の周波電圧が与えられているので、両方の駆
動足12と13はたわみ共振する。このたて振動とたわ
み振動は合成されて楕円運動となる。しかし、駆動足1
3の方は、弾性基体11の節F2とF3の間が負の関係とな
っているため、走行面20に対しては浮いた状態となっ
て、この楕円運動は作用しない。したがって、駆動足1
2の楕円運動だけが走行面20に作用し、駆動足12は
左右への推力となる。その結果、リニアな駆動力が得ら
れる。逆に、弾性基体11の節F1とF2の間が負変形、節
F2とF3の間が正変形した場合には、上記とは逆の関係と
なる。すなわち、走行面20に対して、駆動足12の方
は浮いた状態となり、駆動足13の方だけ接触状態とな
るので、この駆動足13先端の楕円運動だけが、走行面
20に作用する。よって、駆動足13は左右への推力と
なる。その結果、リニアな駆動力が得られる。そして、
移動子10の移動方向は、振動子15,16に与えられ
る駆動電圧の周波数を、対応する駆動足12と13の共
振周波数と同一にするかによって、設定することができ
る。
The reason is considered to be as follows. Now oscillator 1
When 5 and 16 are given different driving voltages of predetermined frequencies,
Between the nodes F1 and F2 in the elastic base 11, and between the nodes F2 and F3
Between 1 and 2, depending on the respective given frequencies, the one deforms downward (positive direction) while the other changes upward (negative direction). For example, clauses F1 and F2
It is assumed that the area between the nodes is positively deformed and the area between the nodes F2 and F3 is negatively deformed. Then, at the same time, the driving feet 12 and 13 also vibrate vertically (vertically). Since the same frequency voltage as the resonance frequency is applied to the drive feet 12 and 13, both drive feet 12 and 13 resonate flexibly. The vertical vibration and the flexural vibration are combined into an elliptic motion. But the driving foot 1
In the case of No. 3, since the nodes F2 and F3 of the elastic substrate 11 have a negative relationship, they are in a floating state with respect to the traveling surface 20, and this elliptic motion does not act. Therefore, drive foot 1
Only two elliptic motions act on the running surface 20, and the driving foot 12 becomes a thrust to the left and right. As a result, a linear driving force can be obtained. On the contrary, between the nodes F1 and F2 of the elastic base 11 is negatively deformed,
When the area between F2 and F3 is positively deformed, the opposite relationship is obtained. That is, since the driving foot 12 is in a floating state and only the driving foot 13 is in contact with the running surface 20, only the elliptic movement of the tip of the driving foot 13 acts on the running surface 20. Therefore, the driving foot 13 becomes a thrust to the left and right. As a result, a linear driving force can be obtained. And
The moving direction of the mover 10 can be set by setting the frequency of the drive voltage applied to the vibrators 15 and 16 to be the same as the resonance frequency of the corresponding drive legs 12 and 13.

なお、上記の動作原理は一つの推論であるが、本リニア
モータは、実際に駆動することができ、したがって、動
作原理が仮に以上とは異なっていたとしても、本考案の
範囲は狭められない。
It should be noted that the above-mentioned operation principle is one reasoning, but the present linear motor can be actually driven, and therefore, even if the operation principle is different from the above, the scope of the present invention is not narrowed. .

「考案の効果」 以上のように本考案の超音波リニアモータは、従来の超
音波モータとは異なる動作原理を持つものであって、し
かも極めて簡単な構造の移動子と、特別な分極処理を要
しない圧電振動子または電歪振動子とによって構成する
ことができる。また移動方向の変更も圧電振動子または
電歪振動子に加える駆動電圧の周波数の変更で行なうこ
とができ、製造および使用が容易な新規なリニアモータ
を提供できる。
"Effects of the Invention" As described above, the ultrasonic linear motor of the present invention has a different operation principle from the conventional ultrasonic motor, and has a very simple structure of the mover and special polarization treatment. It can be constituted by a piezoelectric vibrator or an electrostrictive vibrator which is unnecessary. Further, the moving direction can be changed by changing the frequency of the drive voltage applied to the piezoelectric vibrator or the electrostrictive vibrator, and a novel linear motor that is easy to manufacture and use can be provided.

【図面の簡単な説明】[Brief description of drawings]

第1図は本考案の超音波リニアモータの一つの実施例を
示す正面図、第2図(A),(B)は本考案によるリニアモー
タの動作原理を示す、駆動足および移動子の変形の様子
を描いた模式図である。 10……移動子、11……弾性基体、12,13……駆
動足、14……剛性枠体、15,16……振動子、20
……走行面、F1,F2,F3……節。
FIG. 1 is a front view showing one embodiment of the ultrasonic linear motor of the present invention, and FIGS. 2 (A) and 2 (B) show the operation principle of the linear motor according to the present invention, which is a modification of the driving foot and the mover. It is a schematic diagram depicting the situation. 10 ... mover, 11 ... elastic base, 12, 13 ... drive foot, 14 ... rigid frame, 15, 16 ... vibrator, 20
…… Running surface, F1, F2, F3 …… Section.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】少なくとも三つのたわみ振動の節を有し、
この各節が剛体により支持された弾性基体;この弾性基
体の各節の間の腹部にそれぞれ固定させた、隣り合うも
の同士が共振周波数の異なる少なくとも二本の駆動足;
およびこの弾性基体に、該弾性基体を正負の関係でたわ
み変形させるとともに上記駆動足に振動を与える、各駆
動足に対応して設けられた圧電振動子または電歪振動
子;とを備え、これらの圧電振動子または電歪振動子に
所定の周波電圧を印加することを特徴とする超音波リニ
アモータ。
1. Having at least three flexural vibration nodes,
An elastic base body in which each node is supported by a rigid body; at least two driving feet fixed to the abdomen between the nodes of the elastic base body and having mutually different resonance frequencies;
And a piezoelectric vibrator or an electrostrictive vibrator provided corresponding to each driving foot, which flexibly deforms the elastic base in a positive / negative relationship and gives vibration to the driving foot, and An ultrasonic linear motor characterized in that a predetermined frequency voltage is applied to the piezoelectric vibrator or the electrostrictive vibrator.
JP13515687U 1987-09-04 1987-09-04 Ultrasonic linear motor Expired - Lifetime JPH0619339Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13515687U JPH0619339Y2 (en) 1987-09-04 1987-09-04 Ultrasonic linear motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13515687U JPH0619339Y2 (en) 1987-09-04 1987-09-04 Ultrasonic linear motor

Publications (2)

Publication Number Publication Date
JPS6440294U JPS6440294U (en) 1989-03-10
JPH0619339Y2 true JPH0619339Y2 (en) 1994-05-18

Family

ID=31394534

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13515687U Expired - Lifetime JPH0619339Y2 (en) 1987-09-04 1987-09-04 Ultrasonic linear motor

Country Status (1)

Country Link
JP (1) JPH0619339Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4565850B2 (en) * 2004-01-28 2010-10-20 京セラ株式会社 Ultrasonic motor and lens device

Also Published As

Publication number Publication date
JPS6440294U (en) 1989-03-10

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