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JPH01202174A - Two-dimensional vibration wave motor - Google Patents

Two-dimensional vibration wave motor

Info

Publication number
JPH01202174A
JPH01202174A JP63027024A JP2702488A JPH01202174A JP H01202174 A JPH01202174 A JP H01202174A JP 63027024 A JP63027024 A JP 63027024A JP 2702488 A JP2702488 A JP 2702488A JP H01202174 A JPH01202174 A JP H01202174A
Authority
JP
Japan
Prior art keywords
longitudinal
wave motor
resonant
vibration wave
resonance
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
Application number
JP63027024A
Other languages
Japanese (ja)
Inventor
Takayuki Tsukimoto
貴之 月本
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP63027024A priority Critical patent/JPH01202174A/en
Publication of JPH01202174A publication Critical patent/JPH01202174A/en
Pending legal-status Critical Current

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  • General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)

Abstract

PURPOSE:To compactly increase a thrust force by combining longitudinal vibration resonance vibrators and a nonresonance longitudinal displacement element. CONSTITUTION:Longitudinal resonance vibrators A1...A2 are composed of PZT (lead titanate-zirconate) of one of electro-mechanical energy converter and aluminum or the like of the material having a small vibration attenuation. A nonresonance longitudinal displacement element (b) is formed by laminating PZT, and adhered to the vibrators A1...A2 by a coupling element (d). The mass point of the element (b) is combined to be vibrated at the contact with a moving element (c), thereby performing an elliptical motion. Thus, the element (c) can be easily frictionally driven in two-dimensional direction, thereby compactly obtaining a low speed and a large torque.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、2次元振動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 a two-dimensional vibration wave motor.

[従来の技術] たとえば、特開昭58−148682号公報に記載され
ているように、電気−機械エネルギー変換素子により、
進行波を励起し、移動体を摩擦駆動する振動波モータが
、カメラのAF用として実用化されているが、それは、
移動体を押し上げる振幅をAとすると、物体を駆動する
速度はkA (kは振動子断面形状と波長および材料定
数によって定まる一定値)となり、駆動速度を上げるた
めには、押し上げ振幅Aも同時に増加するため、音を発
生しやすく、また速度を下げるためには、振幅Aが減る
ため、移動体と振動体の接触面を高精度に仕上げ、かつ
、波の沈み込みを防ぐために硬い材料を使うなどの必要
があり、モータとしての速度可変範囲がせまかった。
[Prior Art] For example, as described in Japanese Patent Application Laid-Open No. 58-148682, an electric-mechanical energy conversion element
Vibratory wave motors that excite traveling waves and frictionally drive moving objects have been put into practical use for camera AF;
If the amplitude of pushing up the moving object is A, then the speed of driving the object is kA (k is a constant value determined by the transducer cross-sectional shape, wavelength, and material constant), and in order to increase the driving speed, the pushing amplitude A must also be increased at the same time. Therefore, it is easy to generate sound, and in order to reduce the speed, the amplitude A is reduced, so the contact surface between the moving body and the vibrating body must be finished with high precision, and a hard material must be used to prevent waves from sinking. As a result, the variable speed range of the motor was narrow.

そこで、たとえば、特開昭61−55012号公報に記
載されているように、2方向の曲げ振動を棒・状体に生
ぜしめ、これにより棒状体を螺旋形に変形せしめ、かつ
、該変形された棒状体をその長さ方向の軸のまわりに回
転せしめることにより、移動体を摩擦駆動することが提
案されている。
Therefore, for example, as described in Japanese Patent Application Laid-open No. 61-55012, bending vibrations are generated in two directions in a bar/shaped body, thereby deforming the bar/shaped body into a spiral shape, and the deformed body is It has been proposed to frictionally drive a movable body by rotating a rod-shaped body around its longitudinal axis.

[発明が解決しようとする課題] 前述の特開昭61−55012号公報に記載されている
振動波モータは、物体を押し上げる方向と送り方向振巾
Iを独立に可変できるため、速度可変範囲を広くとれる
が、振動子の機械的品質係数Qが非常に高いため、両振
動の共振周波数をそろえるためには、きびしい加工精度
が要求され、また初期的に合わせておいても、加圧むら
や温度等の変化による共振周波数のずれ量が各々異なる
ため、理想的な質点運動ができず、効率が悪いという問
題点がある。
[Problems to be Solved by the Invention] The vibration wave motor described in the above-mentioned Japanese Patent Application Laid-Open No. 61-55012 can independently vary the direction of pushing up an object and the amplitude I in the feed direction, so the speed variable range can be varied. However, since the mechanical quality factor Q of the vibrator is extremely high, strict machining precision is required to align the resonance frequencies of both vibrations, and even if the resonance frequencies are aligned initially, uneven pressure may occur. Since the amount of deviation of the resonant frequency due to changes in temperature and the like is different, there is a problem that ideal mass point motion cannot be achieved and efficiency is poor.

本発明は、このような問題点を解決しようとするもので
ある。すなわち、本発明は、速度可変範囲が広く、かつ
、製作が容易であって、コンパクトで、低速時に大推力
を発生することができる2次元振動波モータを提供する
ことを目的とするものである。
The present invention attempts to solve these problems. That is, an object of the present invention is to provide a two-dimensional vibration wave motor that has a wide variable speed range, is easy to manufacture, is compact, and can generate large thrust at low speeds. .

[課題を解決するための手段] 上記目的を達成するためには、本発明の2次元振動波モ
ータは、電気−機械エネルギー変換素子により駆動され
る縦振動共振振動子と、J1共振縦変位素子が3つ以上
組み合わせ、各変位方向に角度をもたせて結合したもの
とした。
[Means for Solving the Problems] In order to achieve the above object, the two-dimensional vibration wave motor of the present invention includes a longitudinal vibration resonance vibrator driven by an electro-mechanical energy conversion element, and a J1 resonance longitudinal displacement element. It is assumed that three or more are combined and connected with an angle in each direction of displacement.

[作  用] 本発明によれば、縦振動共振振動子と非共振縦変位素子
を組み合わせることで、容易に物体を2次元方向に摩擦
駆動することが可能となり、かつコンパクトで低速大ト
ルクを得ることが可能である。
[Function] According to the present invention, by combining a longitudinal vibration resonant oscillator and a non-resonant longitudinal displacement element, it becomes possible to easily frictionally drive an object in two-dimensional directions, and obtain a large torque at low speed with a compact size. Is possible.

[実施例コ 第1図は本発明の第1実施例を示している。[Example code] FIG. 1 shows a first embodiment of the invention.

第1図において、AI + A2は縦振動共振振動子で
、a2+、a3 + aa 、a7は電気−機械エネル
ギー変換素子の一種であるチタン酸ジルコン酸鉛(PZ
T)からなり、al + a4 +a5+a6は振動減
衰の小さい材料、たとえば、アルミなどでできており、
各々は接合またはボルトにて締め付けられている。
In Fig. 1, AI + A2 is a longitudinal vibration resonance oscillator, and a2+, a3 + aa, and a7 are lead zirconate titanate (PZ), which is a type of electro-mechanical energy conversion element.
T), and al + a4 + a5 + a6 are made of a material with low vibration damping, such as aluminum,
Each is joined or bolted together.

またbは非共振縦変位素子で、たとえばPZTを積層し
たものを用いる。Cは移動体であり、非共振縦変位素子
すと移動体Cの接触面は、各々耐摩耗処理がほどこされ
ている。dは結合部材で、振動減衰の小さい金属または
樹脂などが用いられ、縦振動共振振動子AI 、A2お
よび非共振縦変位素子すと各々接合されている。
Further, b is a non-resonant longitudinal displacement element, for example, a layered PZT element is used. C is a moving body, and the contact surfaces of the non-resonant longitudinal displacement element and the moving body C are each subjected to wear-resistant treatment. A coupling member d is made of metal or resin with low vibration damping, and is connected to the longitudinal vibration resonant vibrators AI, A2 and the non-resonant longitudinal displacement element.

第2図は第1図に示した2次元振動波モータの座標系を
示している。
FIG. 2 shows the coordinate system of the two-dimensional vibration wave motor shown in FIG.

以下、第1図に示した2次元振動波モータの作動原理に
ついて説明する。
The operating principle of the two-dimensional vibration wave motor shown in FIG. 1 will be explained below.

各軸は、縦振動共振振動子A、、A、 、非共振縦変位
素子すの軸の中心を通り、第2図の斜線部は該振動子A
、、A2を中央部支持にて半波長縦振動を励起させたと
きの縦変位を示す。
Each axis passes through the center of the axis of the longitudinal vibration resonant transducer A, , A, and the non-resonant longitudinal displacement element, and the shaded area in FIG. 2 is the transducer A.
, , shows the longitudinal displacement when A2 is centrally supported and half-wavelength longitudinal vibration is excited.

前記振動子A1を周波数ω1にて駆動する。The vibrator A1 is driven at a frequency ω1.

このとき、中央部を拘束すると、結合部材dにおける質
点は、振幅をAとすると、 x=Asin ω、 t なる運動を行なう。一方、前記変位素子すを周波数ω、
にてX変位に対し、90°位相をずらして駆動を行なう
と、移動体Cとの接触部における質点は、無振動時に2
=0になるように座標変換すると、振幅をBとして、 z = B cosω1t なる運動を行なう。
At this time, when the central part is restrained, the mass point in the connecting member d moves as follows, where A is the amplitude: x=A sin ω, t. On the other hand, the displacement element has a frequency ω,
When driving is performed with a 90° phase shift with respect to the X displacement at
When the coordinates are transformed so that = 0, the motion becomes z = B cosω1t with the amplitude as B.

したがって、移動体Cと接触部において前記変位素子す
の質点は、両振動が合成され、なる楕円運動を行なう。
Therefore, the mass point of the displacement element at the contact portion with the moving body C performs an elliptical motion due to the combination of both vibrations.

このため、移動体Cは、接触と非接触を繰り返えしなが
ら、X方向へ摩擦駆動される。一方、運動方向は前記変
位素子すの該振動子A1に対する位相を90°進めるか
、遅らせるかで、反転可能である。この間、該振動子A
1には通電せず、X方向へ曲げ変形をする。
Therefore, the moving body C is frictionally driven in the X direction while repeating contact and non-contact. On the other hand, the direction of movement can be reversed by advancing or delaying the phase of the displacement element relative to the vibrator A1 by 90°. During this time, the vibrator A
1 is not energized and is bent and deformed in the X direction.

つぎに、前記振動子A2を周波数ω2にて駆動し、前記
変位素子すを同じ周波数ω2で90’ずらして駆動する
と、それぞれの振幅をC,Dとすれば、移動体Cとの接
触部において、前記変位素子すの質点は、 なる楕円運動を行ない、移動体CはX方向へ駆動される
Next, when the vibrator A2 is driven at a frequency ω2 and the displacement element is driven at the same frequency ω2 with a shift of 90', and if the respective amplitudes are C and D, then at the contact part with the moving body C, , the mass point of the displacement element S performs an elliptical motion, and the moving body C is driven in the X direction.

上記説明では、ω1≠ω2としたが、ωl;ω2なるよ
うに、前記振動子AI、A2を設計すれば、同時駆動も
可能であり、この場合、xy平面上、任意の方向への駆
動がなめらかにできる。
In the above explanation, ω1≠ω2, but if the oscillators AI and A2 are designed so that ωl; ω2, simultaneous driving is also possible. In this case, driving in any direction on the xy plane is possible. It can be done smoothly.

第3図は本発明の第2実施例を示している。FIG. 3 shows a second embodiment of the invention.

第3図において、電気−機械エネルギー変換素子a2+
 83+  aa +  ay +  alo+  a
ll+a14+ a15はPZTからなり、振動子の構
成材料al 、 a4− a5.aa 、aa + a
12+ a16はアルミからなっている。
In FIG. 3, the electric-mechanical energy conversion element a2+
83+ aa + ay + alo+ a
ll+a14+ a15 is made of PZT, and the constituent materials of the vibrator are al, a4- a5. aa, aa + a
12+ a16 is made of aluminum.

振動子は前記素子a2とa3の中間およびaloとal
lの中間が支持されており、各々が振動節となる一波長
縦振動が励起される。X方向も同様である。
The vibrator is located between the elements a2 and a3 and between the alo and al
1 is supported, and single-wavelength longitudinal vibrations, each of which is a vibration node, are excited. The same applies to the X direction.

このように、両持ち支持とすることで、曲げ剛性が増し
、従来のものより、より強く、移動体Cを非共振縦変位
素子すに加圧することが可能で、より強い摩擦力、つま
り、大きな推力を得ることができる。
In this way, by supporting on both sides, the bending rigidity is increased, and it is possible to press the moving body C against the non-resonant longitudinal displacement element more strongly than in the conventional case, and a stronger frictional force, that is, A large amount of thrust can be obtained.

なお上記実施例では電気−機械エネルギー変換素子aI
O+  a ll+  a 14+ a 1.を設けた
が、省略してもよい。また縦振動共振振動子A1とA2
のなす角は、必ずしも直角である必要はなく、必要に応
じて変えることは可能である。させら、移動体Cの移動
は固定体と相対的なものであるから、逆に上記実施例の
8動体Cを固定して用いて、他を移動させるようにして
もよい。また縦振動共振振動子A、、A2と非共振′縦
変位素子すの役割を逆にしてもよい。
In the above embodiment, the electric-mechanical energy conversion element aI
O+ a ll+ a 14+ a 1. is provided, but it may be omitted. Also, longitudinal vibration resonance oscillators A1 and A2
The angles formed by the two do not necessarily have to be right angles, and can be changed as necessary. However, since the movement of the movable body C is relative to the fixed body, conversely, the eight movable bodies C of the above embodiment may be fixed and used while the others are moved. Further, the roles of the longitudinal vibration resonant vibrators A, A2 and the non-resonant longitudinal displacement element may be reversed.

[発明の効果] 以上説明したように、本発明によれば、縦振動共振振動
子と非共振縦変位素子を組み合わせることで、容易に物
体を2次元方向に摩擦駆動することが可能で、コンパク
トで、かつ、大推力を得ることが可能となる。
[Effects of the Invention] As explained above, according to the present invention, by combining a longitudinal vibration resonant vibrator and a non-resonant longitudinal displacement element, it is possible to easily frictionally drive an object in two-dimensional directions, and it is compact. At the same time, it becomes possible to obtain large thrust.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の第1実施例を示した斜視図、第2図は
第1図の2次元振動波モータの摩擦系および振動子の縦
変位を示した説明図、第3図は本発明の第2実施例を示
した斜視図である。 A、、A2・・・縦振動共振振動子 a In  a 4+ a S+ a 8+a  9+
a  12+   a  16・・・振動子の構成材 a2+a3+a6+a7+alo+all+a14+a
I5・・・電気−機械エネルギー変換素子 b・・・非共振縦変位素子 C・・・移動体 d・・・結合部材
FIG. 1 is a perspective view showing the first embodiment of the present invention, FIG. 2 is an explanatory diagram showing the friction system and vertical displacement of the vibrator of the two-dimensional vibration wave motor shown in FIG. 1, and FIG. FIG. 3 is a perspective view showing a second embodiment of the invention. A,, A2...Longitudinal vibration resonance vibrator a In a 4+ a S+ a 8+ a 9+
a 12+ a 16... vibrator constituent material a2+a3+a6+a7+alo+all+a14+a
I5...Electro-mechanical energy conversion element b...Non-resonant longitudinal displacement element C...Moving body d...Coupling member

Claims (1)

【特許請求の範囲】 1 電気−機械エネルギー変換素子により駆動される縦
振動共振振動子と、非共振縦変位素子が3つ以上組み合
わされていて、各変位方向に角度をもたせて結合されて
いることを特徴とする2次元振動波モータ。 2 複数の縦振動共振振動子を変位方向が垂直になるよ
うに組み合わせ、両者により形成された平面に垂直方向
に非共振縦振動子を結 合させた請求項1記載の2次元振動波モー タ。 3 複数の非共振縦変位素子を変位方向が垂直になるよ
うに組み合せ、両者により形成された平面に垂直方向に
縦振動共振振動子を結 合させた請求項1記載の2次元振動波モー タ。
[Claims] 1. A longitudinal vibration resonant vibrator driven by an electro-mechanical energy conversion element and three or more non-resonant longitudinal displacement elements are combined, and are coupled at an angle in each displacement direction. A two-dimensional vibration wave motor characterized by: 2. The two-dimensional vibration wave motor according to claim 1, wherein a plurality of longitudinal vibration resonance oscillators are combined so that their displacement directions are perpendicular, and a non-resonance longitudinal oscillator is coupled in a direction perpendicular to a plane formed by both. 3. The two-dimensional vibration wave motor according to claim 1, wherein a plurality of non-resonant longitudinal displacement elements are combined so that their displacement directions are perpendicular, and a longitudinal vibration resonance vibrator is coupled in a direction perpendicular to a plane formed by both elements.
JP63027024A 1988-02-08 1988-02-08 Two-dimensional vibration wave motor Pending JPH01202174A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63027024A JPH01202174A (en) 1988-02-08 1988-02-08 Two-dimensional vibration wave motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63027024A JPH01202174A (en) 1988-02-08 1988-02-08 Two-dimensional vibration wave motor

Publications (1)

Publication Number Publication Date
JPH01202174A true JPH01202174A (en) 1989-08-15

Family

ID=12209511

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63027024A Pending JPH01202174A (en) 1988-02-08 1988-02-08 Two-dimensional vibration wave motor

Country Status (1)

Country Link
JP (1) JPH01202174A (en)

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