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JPH0640745B2 - Twin resonance type ultrasonic motor - Google Patents
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JPH0640745B2 - Twin resonance type ultrasonic motor - Google Patents

Twin resonance type ultrasonic motor

Info

Publication number
JPH0640745B2
JPH0640745B2 JP59269630A JP26963084A JPH0640745B2 JP H0640745 B2 JPH0640745 B2 JP H0640745B2 JP 59269630 A JP59269630 A JP 59269630A JP 26963084 A JP26963084 A JP 26963084A JP H0640745 B2 JPH0640745 B2 JP H0640745B2
Authority
JP
Japan
Prior art keywords
twin
ultrasonic
ultrasonic motor
rotor
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.)
Expired - Lifetime
Application number
JP59269630A
Other languages
Japanese (ja)
Other versions
JPS61150675A (en
Inventor
明生 熊田
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.)
Maxell Ltd
Original Assignee
Hitachi Maxell Energy 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 Hitachi Maxell Energy Ltd filed Critical Hitachi Maxell Energy Ltd
Priority to JP59269630A priority Critical patent/JPH0640745B2/en
Publication of JPS61150675A publication Critical patent/JPS61150675A/en
Publication of JPH0640745B2 publication Critical patent/JPH0640745B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02NELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
    • H02N2/00Electric machines in general using piezoelectric effect, electrostriction or magnetostriction
    • H02N2/10Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing rotary motion, e.g. rotary motors
    • H02N2/103Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing rotary motion, e.g. rotary motors by pressing one or more vibrators against the rotor
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02NELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
    • H02N2/00Electric machines in general using piezoelectric effect, electrostriction or magnetostriction
    • H02N2/0005Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing non-specific motion; Details common to machines covered by H02N2/02 - H02N2/16
    • H02N2/001Driving devices, e.g. vibrators
    • H02N2/0045Driving devices, e.g. vibrators using longitudinal or radial modes combined with torsion or shear modes

Landscapes

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

Description

【発明の詳細な説明】 〔産業上の利用分野および発明の目的〕 本発明は超音波モータの改良に係り、構造が簡単で体積
当たりの出力が大きい効率の高い、回転の向きを電気的
に任意に制御することのできる超音波モータを提供する
ことを目的とする。
DETAILED DESCRIPTION OF THE INVENTION [Industrial field of use and object of the invention] The present invention relates to an improvement of an ultrasonic motor, and has a simple structure, a large output per volume, a high efficiency, and an electrically rotating direction. An object is to provide an ultrasonic motor that can be controlled arbitrarily.

〔従来の技術〕[Conventional technology]

固定子の端面に圧着された回転子が回転トルクを受ける
ように構成された超音波モータでは、固定子の端面に超
音波楕円振動を発生させなければならない。このために
は固定子がねじりモードの超音波楕円振動子であればよ
いが、従来はこのようなねじりモードの楕円振動子が見
当らないので、超音波モータを実現するのが困難であつ
た。
In the ultrasonic motor configured such that the rotor crimped to the end surface of the stator receives the rotational torque, ultrasonic elliptical vibration must be generated at the end surface of the stator. For this purpose, the stator may be a torsion mode ultrasonic elliptical oscillator, but conventionally, since such a torsion mode elliptical oscillator is not found, it has been difficult to realize an ultrasonic motor.

すなわち、従来実用されてきた超音波振動子はほとんど
がランジユバン型のたてモード振動子であり、これを用
いてねじりモードの楕円振動を発生させるのは容易なこ
とでなく、構造が複雑になたりしてコンパクト化し難い
欠点があつた。さらに超音波振動子から固定子への超音
波エネルギーの伝達損失が多く、モータとしての効率の
低いこと、モータの回転の向きを電気的に容易に変える
ことができないことなどが欠点であつた。
In other words, most of the ultrasonic transducers that have been put into practical use in the past are Langevin-type vertical mode transducers, and it is not easy to generate torsional mode elliptical vibrations using them, and the structure becomes complicated. However, there was a drawback that it was difficult to make it compact. Further, there are many transmission losses of ultrasonic energy from the ultrasonic oscillator to the stator, the efficiency of the motor is low, and the direction of rotation of the motor cannot be electrically changed easily.

〔問題点を解決するための手段〕[Means for solving problems]

この発明は上述した従来技術の欠点を解消するもので、
等しい共振周波数を有する複数個の屈曲振動子を結合し
た構造からなり、圧電体でねじり振動が励振されるよう
構成された超音波ねじり振動子を別の圧電体を用いてね
じり軸と平行に励振することにより、端面にねじり楕円
運動が発生する双共振型超音波楕円振動子の端面に回転
子を圧着することにより、回転子に回転トルクが発生す
ることを特徴とした双共振型超音波モータによつて目的
を達成したものである。
This invention solves the above-mentioned drawbacks of the prior art.
An ultrasonic torsional oscillator composed of a structure in which a plurality of bending oscillators having the same resonance frequency are coupled to each other and configured to excite torsional vibration with a piezoelectric body is excited in parallel with the torsion axis by using another piezoelectric body. The twin resonance ultrasonic motor is characterized in that a rotating torque is generated in the rotor by crimping the rotor to the end surface of the twin resonance type ultrasonic elliptical oscillator in which a twist elliptical motion is generated in the end surface. That is why the purpose was achieved.

〔実施例〕〔Example〕

以下、本発明の実施例を図面に従つて説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図は、本発明に係る双共振型超音波モータの一実施
例を示す正面図である。回転出力シヤフト21は回転子
17に固定されており、回転数10〜60rpmでゆつく
りと回転し、これを停止させるには数10kg・cmのトル
クを要するほど力強く回転している。回転子17は、ベ
アリング20で支えたコイルスプリング19を通した直
径4mmのキヤツプボルト18によつて双共振子1に圧着
されている。双共振子1と回転子17との圧着面には超
音波楕円振動が発生しているので、圧着された鋼鉄製の
厚さ5mm,直径30mmの回転子17に強力な回転トルク
が生じるのである。
FIG. 1 is a front view showing an embodiment of a twin resonance type ultrasonic motor according to the present invention. The rotation output shaft 21 is fixed to the rotor 17, rotates at a rotational speed of 10 to 60 rpm slowly, and is rotated so strongly that a torque of several tens of kg · cm is required to stop it. The rotor 17 is crimped to the twin resonator 1 by a cap bolt 18 having a diameter of 4 mm which is passed through a coil spring 19 supported by a bearing 20. Since ultrasonic elliptical vibration is generated on the crimping surface between the twin resonator 1 and the rotor 17, a strong rotational torque is generated in the crimped rotor 17 having a thickness of 5 mm and a diameter of 30 mm. .

ここで超音波楕円振動子は、第2図および第3図を示し
たように、アルミニウム製の双共振子1にねじり屈曲振
動を励振する励振源は、10mm×10mmの大きさで2mm
厚のPb(Zr,Ti)O圧電セラミツク角板からな
り2枚ずつ一対とした4組の圧電振動子2,3,4(図
示せず),5と座金6を介して重ねた同じセラミツク製
圧電体からなる直径35mm,内径15mm,厚さ2mmのド
ーナツ状圧電厚み振動子7とからなる。これらは直径3
5mm,厚さ12.5mmの円板状をしたボルト状座金6に
通した直径8mm,長さ20mmのキヤツプボルト9によつ
て双共振子1のネジ穴に対して数10Kg・cmのトルクで
締め付けられ、一体化されている。圧電振動子2および
4は正分極面と向かい合わせリード線12および14の
ついた端子板を挾んで重ね合わせ、圧電振動子3および
5は負分極面を向かい合わせ同様にして重ねられてい
る。リード線12,13,14,15を共通にして、こ
れらとリード線16との間に38KHzの正弦波電圧を印
加すると双共振子1の2本の梁が互いに逆位相で屈曲共
振する結果、2本の梁の先端面1′を見るとねじり振動
力が生じている。圧電厚み振動子7のリード線10をリ
ード線12,13,14,15と接続し、リード線11
をリード線16と接続した状態で、再び電圧を印加する
と双共振子1の先端面1′にねじり楕円運動が発生し、
回転子17が約60rpmで力強く回転を始めた。印加電
圧の周波数を同一に保つたまま、電圧を50V,70V
と増大して行くと、回転数、トルクともに増大した。回
転数の可変範囲は10〜100rpm程度であつた。
As shown in FIGS. 2 and 3, the ultrasonic elliptical oscillator has an excitation source that excites torsional bending vibration in the aluminum biresonator 1 having a size of 10 mm × 10 mm and 2 mm.
Four sets of piezoelectric vibrators 2, 3, 4 (not shown), 5 made of thick Pb (Zr, Ti) O 3 piezoelectric ceramic square plates, two pairs each, and the same ceramics stacked via a washer 6. The doughnut-shaped piezoelectric thickness vibrator 7 having a diameter of 35 mm, an inner diameter of 15 mm and a thickness of 2 mm is formed of a piezoelectric body. These are diameter 3
With a cap bolt 9 having a diameter of 8 mm and a length of 20 mm, which is passed through a disk-shaped bolt washer 6 having a thickness of 5 mm and a thickness of 12.5 mm, a torque of several tens of kg · cm is applied to the screw hole of the twin resonator 1. Tightened and integrated. The piezoelectric vibrators 2 and 4 are superposed on each other with terminal plates with lead wires 12 and 14 facing each other facing the positive polarization surface, and the piezoelectric vibrators 3 and 5 are facing each other with the negative polarization surface facing each other. When the lead wires 12, 13, 14, 15 are made common and a sinusoidal voltage of 38 KHz is applied between these and the lead wire 16, the two beams of the twin resonator 1 bend and resonate in opposite phases, Looking at the tip surfaces 1'of the two beams, a torsional vibration force is generated. The lead wire 10 of the piezoelectric thickness oscillator 7 is connected to the lead wires 12, 13, 14, and 15, and the lead wire 11
When the voltage is applied again with the lead wire connected to the lead wire 16, a twist elliptical motion is generated in the front end surface 1 ′ of the twin resonator 1,
The rotor 17 started to rotate strongly at about 60 rpm. While keeping the frequency of the applied voltage the same, the voltage is 50V, 70V
Both the number of rotations and the torque increased. The variable range of the rotation speed was about 10 to 100 rpm.

なお、第1図に示した超音波モータの構成図は、概略説
明のための図であるからモータケースは省略されている
が、実用品は保護のためにケースに収めることもできる
のは言うまでもない。
The configuration of the ultrasonic motor shown in FIG. 1 is a schematic diagram, so the motor case is omitted, but it goes without saying that a practical product can be housed in the case for protection. Yes.

この実施例では双共振型超音波振動子に用いた双共振子
1には断面が10mm×10mmの正方形アルミニウム製の
2本の梁からなる屈曲振動子を結合したものを例示した
が、屈曲振動子は共振周波数を揃えられるかぎり何本結
合しても差し支えない。たとえば、3本の3極双共振子
および4本の4極双共振子における屈曲振動子の形状を
それぞれ第4図および第5図に示した。これらの図にお
いて31,41は3本または4本の双共振子、31′,
41′はその双共振子31,41の先端面、32,42
は座金である。
In this embodiment, the twin resonator 1 used in the twin resonance type ultrasonic vibrator is exemplified by a bending vibrator composed of two beams made of square aluminum having a cross section of 10 mm × 10 mm. As long as the resonance frequencies can be equalized, any number of children can be combined. For example, the shapes of bending oscillators in three 3-pole twin resonators and four 4-pole twin resonators are shown in FIGS. 4 and 5, respectively. In these figures, 31, 41 are three or four twin resonators, 31 ',
41 'is the front end face of the twin resonators 31, 41, 32, 42
Is a washer.

〔発明の効果〕〔The invention's effect〕

以上説明したように本発明は、等しい共振周波数を有す
る複数個の屈曲振動子を結合した構造からなり、圧電体
によつてねじり振動子が励振されるよう構成された超音
波ねじり振動子を別の圧電体を用いてねじり軸と平行に
励振することにより、端面にねじり楕円運動が発生する
双共振型超音波楕円振動子の端面に回転子を圧着するこ
とにより、回転子に回転トルクが発生することを特徴と
したものである。従つて、本発明に係る双共振型超音波
モータは、ねじり楕円振動を発生する超音波振動子を固
定子とし、これに回転子を圧着した簡単な構造にするこ
とができ、コンパクト化できたので体積の割に大きな出
力を出すことができ、高能率の効果があり、しかも、入
力電気信号の極性を反転することによりモータの回転方
向を任意に制御できる効果がある。
INDUSTRIAL APPLICABILITY As described above, the present invention has a structure in which a plurality of bending oscillators having the same resonance frequency are coupled, and an ultrasonic torsion oscillator configured to excite the torsion oscillator by a piezoelectric body When a rotor is crimped to the end face of a bi-resonant ultrasonic elliptical oscillator in which a torsion elliptical motion is generated at the end face by exciting the piezoelectric body in parallel with the torsion axis, rotational torque is generated in the rotor. It is characterized by doing. Therefore, the twin resonance type ultrasonic motor according to the present invention can be made compact with a simple structure in which an ultrasonic oscillator that generates torsional elliptical vibration is used as a stator and a rotor is crimped thereto. Therefore, there is an effect that a large output can be output for the volume, a high efficiency is obtained, and further, the rotation direction of the motor can be arbitrarily controlled by reversing the polarity of the input electric signal.

このように本発明に係る双共振型超音波モータは、超音
波モータの中でも、高効率、高出力が特徴であるから、
ましてや通常の電磁モータと比較すると、重量当たりの
出力が大きく、低速回転で高出力が得られる点で抜群に
優れており、さらに回転量の角度分解能が高く、イナー
シアレスに即動,即停止できるなど実用上の見地から優
れた資質を有するモータである。
As described above, the twin resonance ultrasonic motor according to the present invention is characterized by high efficiency and high output among ultrasonic motors.
Compared with ordinary electromagnetic motors, the output per weight is large, and it is outstandingly superior in that it can obtain high output at low speed rotation. Furthermore, the angular resolution of the rotation amount is high, and it is possible to move immediately and stop instantly without inertia. The motor has excellent qualities from a practical point of view.

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

第1図は本発明に係る双共振型超音波モータの一実施例
を示す正面図、第2図および第3図はそのモータに用い
る双共振型超音波楕円振動子の正面図および側面図、第
4図および第5図は双共振型超音波楕円振動子の変形例
を示す平面図である。 1,31,41……双共振子、1′,31′,41′…
…双共振子の先端面、2〜5……圧電振動子、7……圧
電厚み振動子、17……回転子、21……出力シヤフ
ト。
FIG. 1 is a front view showing an embodiment of a twin resonance ultrasonic motor according to the present invention, and FIGS. 2 and 3 are front views and side views of a twin resonance ultrasonic elliptical vibrator used in the motor. FIG. 4 and FIG. 5 are plan views showing modified examples of the biresonance ultrasonic elliptical transducer. 1, 31, 41 ... Twin resonator, 1 ', 31', 41 '...
… Twin resonator tip surface, 2 to 5 …… Piezoelectric vibrator, 7 …… Piezoelectric thickness vibrator, 17 …… Rotor, 21 …… Output shaft.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】等しい共振周波数を有する複数個の屈曲振
動子を結合した構造からなり、圧電体によつてねじり振
動が励振されるよう構成された超音波ねじり振動子を別
の圧電体を用いてねじり軸と平行に励振することによ
り、端面にねじり楕円運動が発生する双共振型超音波楕
円振動子の端面に回転子を圧着することにより、回転子
に回転トルクが発生することを特徴とした双共振型超音
波モータ。
1. An ultrasonic torsional oscillator having a structure in which a plurality of bending oscillators having the same resonance frequency are coupled to each other, and a torsional vibration is excited by the piezoelectric substance using another piezoelectric substance. The torsional elliptical motion is generated by exciting the rotor parallel to the torsion axis, and the rotating torque is generated in the rotor by crimping the rotor on the end face of the twin resonance type ultrasonic elliptical oscillator. Twin resonance type ultrasonic motor.
【請求項2】特許請求の範囲第1項記載の双共振型超音
波モータにおいて、ねじり振動を励振する圧電体と、ね
じり軸に平行に励振する別の圧電体とに印加する交番電
圧の極性相互関係を変えることにより、回転の向きをス
イツチすることを特徴とした双共振型超音波モータ。
2. The twin resonance ultrasonic motor according to claim 1, wherein the polarity of the alternating voltage applied to the piezoelectric body that excites torsional vibration and another piezoelectric body that excites in parallel with the torsion axis. A bi-resonant ultrasonic motor characterized by switching the direction of rotation by changing the mutual relationship.
JP59269630A 1984-12-22 1984-12-22 Twin resonance type ultrasonic motor Expired - Lifetime JPH0640745B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59269630A JPH0640745B2 (en) 1984-12-22 1984-12-22 Twin resonance type ultrasonic motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59269630A JPH0640745B2 (en) 1984-12-22 1984-12-22 Twin resonance type ultrasonic motor

Publications (2)

Publication Number Publication Date
JPS61150675A JPS61150675A (en) 1986-07-09
JPH0640745B2 true JPH0640745B2 (en) 1994-05-25

Family

ID=17475023

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59269630A Expired - Lifetime JPH0640745B2 (en) 1984-12-22 1984-12-22 Twin resonance type ultrasonic motor

Country Status (1)

Country Link
JP (1) JPH0640745B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2596129B2 (en) * 1989-07-06 1997-04-02 日本電気株式会社 Ultrasonic motor
JP2010226895A (en) * 2009-03-24 2010-10-07 Nikon Corp Actuator, drive device, lens unit, and imaging device

Also Published As

Publication number Publication date
JPS61150675A (en) 1986-07-09

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