JPH0736709B2 - Bolt tightening ultrasonic elliptical transducer for piezoelectric motor - Google Patents

Bolt tightening ultrasonic elliptical transducer for piezoelectric motor

Info

Publication number
JPH0736709B2
JPH0736709B2 JP60231020A JP23102085A JPH0736709B2 JP H0736709 B2 JPH0736709 B2 JP H0736709B2 JP 60231020 A JP60231020 A JP 60231020A JP 23102085 A JP23102085 A JP 23102085A JP H0736709 B2 JPH0736709 B2 JP H0736709B2
Authority
JP
Japan
Prior art keywords
piezoelectric
oscillator
diameter
bolt
ultrasonic
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
JP60231020A
Other languages
Japanese (ja)
Other versions
JPS6292780A (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.)
Hitachi Maxell Energy 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 JP60231020A priority Critical patent/JPH0736709B2/en
Publication of JPS6292780A publication Critical patent/JPS6292780A/en
Publication of JPH0736709B2 publication Critical patent/JPH0736709B2/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

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は圧電超音波モータに係わり、さらに詳しくはそ
のステータを構成する超音波楕円振動子の改良に関す
る。
Description: TECHNICAL FIELD The present invention relates to a piezoelectric ultrasonic motor, and more particularly to an improvement of an ultrasonic elliptical vibrator that constitutes a stator thereof.

〔従来の技術〕[Conventional technology]

本発明者は圧電超音波モータおよび、これを駆動する超
音波楕円振動子に関し、多数の提案をして来た。中でも
片持梁状超音波楕円振動子を用いたモータは実用上優れ
た特性を示すので、特願昭59−172429号を始めとし20余
件の出願をして来た。この片持梁型超音波モータは、低
速・大トルクを高効率で出力できる特徴があるので、実
用上の価値が高い。モータを駆動するには超音波楕円振
動子の共振周波数に一致する正弦波電圧を印加するの
で、高出力を得るには高電圧を要する。従来提案して来
たモータでは、モータのサイズにかかわらず少なくとも
50ボルト程度の電圧を要し、それ以下の電圧を印加して
も有効な出力は得られず、低電圧駆動のできないことが
欠点であつた。
The present inventor has made many proposals regarding a piezoelectric ultrasonic motor and an ultrasonic elliptical vibrator for driving the piezoelectric ultrasonic motor. Among them, a motor using a cantilever ultrasonic ellipsoidal vibrator shows excellent characteristics in practical use, so we have filed more than 20 applications including Japanese Patent Application No. 59-172429. This cantilever ultrasonic motor has a feature of being capable of outputting a low speed and a large torque with high efficiency, and thus has high practical value. Since a sine wave voltage that matches the resonance frequency of the ultrasonic elliptical oscillator is applied to drive the motor, a high voltage is required to obtain a high output. With the motors we have proposed so far, at least regardless of the size of the motor,
The disadvantage is that it requires a voltage of about 50 V, and even if a voltage of less than 50 V is applied, an effective output cannot be obtained, and low voltage driving cannot be performed.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

この発明は、従来の片持梁状超音波楕円振動子を用いた
圧電モータが持つていた低電圧駆動ができないという欠
点を解決し、低電圧駆動で大出力が得られる実用性に優
れた圧電モータに用いる超音波楕円振動子を提供するこ
とを目的とする。
The present invention solves the drawback that a piezoelectric motor using a conventional cantilever ultrasonic elliptical vibrator cannot drive at a low voltage, and is a highly practical piezoelectric that can obtain a large output at a low voltage drive. An object is to provide an ultrasonic elliptical oscillator used for a motor.

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

現在実用化されている超音波振動子は、そのほとんどが
ボルト締めランジユバン型振動子と呼ばれる縦振動を発
生する振動子である。ランジユバン型振動子におけるボ
ルトの役割は圧電素子を締め付けると同時に発生した振
動を金属丸棒からなる共振子に導く作用をするものであ
る。共振子の振動強度は丸棒の断面積で決まるが、一般
に丸棒の方がボルトより径がずつと太いので強度が強過
ぎる。このため丸棒の端部を中空の筒状にして強度調整
をしている。しかし、本発明の対象とする超音波楕円振
動子では、直接縦振動子を締め付けるのではなく、ねじ
り結合子を固定支持し、ねじり結合子の円盤を通して、
縦振動子および圧電素子を締め付ける。したがつて、振
動子強度は円盤の屈曲モードに対する強度で決まるが、
屈曲モードは強度が小さいので、ランジユバン振動子の
場合より細いボルトを用いて強度整合すればよい。
Most of the ultrasonic transducers currently in practical use are oscillators that generate longitudinal vibration, called bolted Langevin type transducers. The role of the bolt in the Langevin type vibrator is to actuate the vibration generated at the same time as tightening the piezoelectric element to the resonator made of a metal rod. The vibration strength of the resonator is determined by the cross-sectional area of the round bar, but in general, the round bar is thicker than the bolt, and therefore the strength is too strong. For this reason, the strength of the round bar is adjusted by forming the end of the bar into a hollow cylinder. However, in the ultrasonic elliptical oscillator that is the subject of the present invention, instead of directly tightening the longitudinal oscillator, the torsional connector is fixedly supported and passed through the disk of the torsional connector,
Tighten the vertical vibrator and piezoelectric element. Therefore, the oscillator strength is determined by the strength of the bending mode of the disk,
Since the bending mode has a small strength, it is sufficient to use a thinner bolt to perform strength matching than in the case of the Langevin vibrator.

ねじり結合子の振動強度は円盤の厚さ,直径でほぼ決ま
り溝幅,梁の厚さ梁の高さなどで詳細が決まるが、一
方、一般に共振周波数が40KHz附近になるように設計さ
れていることから、振動強度はねじり結合子の円盤の直
径によつて決まると見てよい。直径の大きい円盤には太
いボルトが、小さい円盤には細いボルトが用いられる。
The vibration strength of the torsional connector is almost determined by the thickness and diameter of the disk, and the details are determined by the groove width, beam thickness, beam height, etc. On the other hand, the resonance frequency is generally designed to be around 40 KHz. Therefore, it can be considered that the vibration intensity is determined by the diameter of the disk of the torsional connector. Thick bolts are used for disks with a large diameter, and thin bolts are used for disks with a small diameter.

〔実施例〕 以下、本発明を実施例に従つて説明する。[Examples] Hereinafter, the present invention will be described with reference to Examples.

実施例1 第1図は、本発明の一実施例を示す片持梁状超音波楕円
振子を用いた圧電振動子の構造説明図である。
Example 1 FIG. 1 is a structural explanatory view of a piezoelectric vibrator using a cantilever ultrasonic elliptical pendulum showing an example of the present invention.

構造そのものは従来のこの種超音波モータの構造と何ら
異なるところがないので、説明の詳細は省略する。異な
る点はキヤツプボルト8の太さをねじり結合子円盤7の
径に見合う太さに選んだことにあるので、従来例との差
異を図示することはできない。つまり構成は、Pb(ZrT
i)O系圧電セラミツク1,2の正電極間同志対向させ、
端子板3,4と重ねてアルミニウム座金5にセツトしたキ
ヤツプボルト8に通し、さらにアルミニウム円盤6を重
ねたのち、キヤツプボルトの先端をねじり結合子7のね
じ孔に嵌め締め付けて、一体化し超高波楕円振動子を構
成した。
Since the structure itself is not different from the structure of the conventional ultrasonic motor of this type, detailed description thereof will be omitted. The different point is that the thickness of the cap bolt 8 is selected to be the thickness corresponding to the diameter of the torsion connector disk 7, and therefore the difference from the conventional example cannot be illustrated. In other words, the configuration is Pb (ZrT
i) The positive electrodes of the O 3 -based piezoelectric ceramics 1 and 2 are opposed to each other,
After passing through the cap bolt 8 set on the aluminum washer 5 over the terminal plates 3 and 4, and further stacking the aluminum disc 6, the tip of the cap bolt is fitted into the screw hole of the torsion connector 7 and tightened to form an ultra-high wave. An elliptical oscillator was constructed.

この振動子をステータとして、端面つまりねじり結合子
7の梁部の上面中心のねじ孔にロータ9の支持ボルトを
ねじ込むことにより、ロータに圧着力を作用させた。端
子板3,4のリード線に40WHz附近にある共振周波数の正弦
波電圧を印加して、ロータ9を回転し、モータを作動さ
せた。
By using this oscillator as a stator, a support bolt of the rotor 9 was screwed into an end face, that is, a screw hole at the center of the upper surface of the beam portion of the torsional connector 7, thereby exerting a crimping force on the rotor. A sine wave voltage having a resonance frequency of about 40 WHz was applied to the lead wires of the terminal plates 3 and 4, the rotor 9 was rotated, and the motor was operated.

ここで、圧電セラミツク振動子、ボルトならびにねじり
結合子のそれぞれの直径を種々変えた場合のモータの動
作特性を調べた。
Here, the operating characteristics of the motor were investigated when various diameters of the piezoelectric ceramic oscillator, the bolt, and the torsional connector were changed.

上述した測定結果、すなわち、片持梁状超音波楕円は振
動子を構成するセラミツク振動子およびねじり結合子の
各種サイズに対する締め付けボルトの太さの影響を次の
表に示す。表中の○は3種類のボルトのなかで、もつと
も低電圧で滑らかに回転した場合であり最適条件である
ことを示し、△は使用可能な限界を示し、×は使用に適
さないことを示している。
The following table shows the above-mentioned measurement results, that is, the influence of the thickness of the tightening bolts on various sizes of the ceramic oscillator and the torsional connector forming the oscillator for the cantilever ultrasonic ellipse. Among the three types of bolts in the table, ○ indicates that the rotation is smooth at low voltage, which is the optimum condition, △ indicates the usable limit, and × indicates that it is not suitable for use. ing.

なお、表中のセラミツク径は圧電振動子の直径である。
上記表において圧電振動子の直径(D1)に対するボルト
の直径(D2)の比(D2/D1)をまとめて示せば次の通り
である。
The ceramic diameter in the table is the diameter of the piezoelectric vibrator.
In the above table, the ratio (D2 / D1) of the diameter (D2) of the bolt to the diameter (D1) of the piezoelectric vibrator is summarized as follows.

前記測定結果の表から明らかなように、圧電振動子の直
径(D1)が25mmの小径であるのに対してボルトの直径
(D2)が8mmの大径であると、すなわちD2/D1が1/3であ
ると、50ボルトより低い電圧で駆動する限界であり(△
有り)、それよりもボルトの直径が大きくなると、すな
わちD2/D1が1/3より大きくなると、従来と同様に50ボル
ト以上の電圧が必要となる。
As is clear from the table of measurement results, when the diameter (D1) of the piezoelectric vibrator is as small as 25 mm and the diameter (D2) of the bolt is as large as 8 mm, that is, D2 / D1 is 1 If it is / 3, it is a limit to drive at a voltage lower than 50 V (△
Yes), if the diameter of the bolt becomes larger than that, that is, if D2 / D1 becomes larger than 1/3, a voltage of 50 volts or more is required as in the conventional case.

一方、圧電振動子の直径(D1)が50mmの大径であるのに
対してボルトの直径(D2)が6mmの小径であると、すな
わちD2/D1が1/8であると、低圧電駆動での回転トルクの
限界であり(△有り)、D2/D1がそれ以上小さくなる
と、即ち圧電振動子の直径(D1)が35mmに対してボルト
の直径(D2)が4mmであつたり(D2/D1=1/9)、また圧
電振動子の直径(D1)が50mmであるのに対してボルトの
直径(D2)が4mmであると(D2/D1=1/13)、十分な回転
トルクが得られない(×有り)。このような理由からD2
/D1を1/3〜1/8の範囲に規制することにより、低電圧で
かつ十分な回転トルクを得ることができる。
On the other hand, when the diameter (D1) of the piezoelectric vibrator is 50 mm as large as the diameter of the bolt (D2) as small as 6 mm, that is, when D2 / D1 is 1/8, low piezoelectric drive is achieved. Is the limit of rotation torque (with △), and when D2 / D1 becomes smaller than that, that is, when the diameter (D1) of the piezoelectric vibrator is 35 mm and the diameter (D2) of the bolt is 4 mm (D2 / If the diameter (D1) of the piezoelectric vibrator is 50 mm and the diameter of the bolt (D2) is 4 mm (D2 / D1 = 1/13), sufficient rotation torque will be obtained. I can't get it. For this reason D2
By regulating / D1 within the range of 1/3 to 1/8, it is possible to obtain a low voltage and sufficient rotation torque.

〔発明の効果〕〔The invention's effect〕

以上説明したように本発明では、圧電振動子とねじり結
合子とをボルトで締め付けて、一体化した超音波楕円振
動子において、締め付けボルトの太さを圧電振動子の直
径の1/3から1/8の範囲における、ねじり結合子の振動子
強度と整合する太さに選ぶ構成をとつた。そのためアト
ミツタンスを最大にすることができ、したがつて超音波
モータのステータに用いた場合、より低い電圧を印加し
て、より大きな回転出力を得ることができ。低電圧駆動
の超音波モータのステータに適用できるなどの効果があ
る。
As described above, in the present invention, the piezoelectric vibrator and the torsional connector are tightened with bolts, and in the ultrasonic elliptical vibrator integrated, the thickness of the tightening bolt is 1/3 to 1 of the diameter of the piezoelectric vibrator. In the range of / 8, we selected a thickness that matches the oscillator strength of the torsional connector. Therefore, the atommittance can be maximized. Therefore, when it is used for the stator of the ultrasonic motor, it is possible to apply a lower voltage and obtain a larger rotation output. There is an effect that it can be applied to a stator of an ultrasonic motor driven by a low voltage.

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

第1図は本発明による圧電モータ用ボルト締め超音波楕
円振動子の一実施例を示す正面図である。 1,2……圧電セラミツク振動子、3,4……端子板、5……
キヤツプボルト用座金、6……アルミニウム円盤、7…
…ねじり結合子、8……キヤツプボルト、9……ロー
タ、10……出力シヤフト。
FIG. 1 is a front view showing an embodiment of a bolted ultrasonic elliptical vibrator for a piezoelectric motor according to the present invention. 1,2 …… Piezoelectric ceramic resonator, 3,4 …… Terminal plate, 5 ……
Wash bolt washers, 6 ... Aluminum disc, 7 ...
… Torsion connector, 8 …… Cap bolt, 9 …… Rotor, 10 …… Output shaft.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】圧電振動子で発生した縦振動をねじり結合
子でねじり振動に変換して、ねじり結合子の端面に超音
波楕円振動を発生させ、ロータをその楕円振動によつて
回転させる超音波楕円振動子であって、 前記圧電振動子が円盤状のセラミツク体からなり、前記
ねじり結合子の少なくとも前記圧電振動子と対向する側
が円盤状になつており、前記圧電振動子の中央部からね
じり結合子の中央部にかけて挿通された1本のボルトで
締め付けて圧電振動子とねじり結合子とを一体にしたも
のにおいて、 前記圧電振動子の直径の1/3よりも細く、1/8よりも太い
直径を有する前記ボルトを用いたことを特徴とする圧電
モータ用ボルト締め超音波楕用振動子。
1. A longitudinal vibration generated by a piezoelectric vibrator is converted into a torsional vibration by a torsional connector, ultrasonic elliptical vibration is generated at an end face of the torsional connector, and a rotor is rotated by the elliptical vibration. An acoustic wave elliptical oscillator, wherein the piezoelectric oscillator is formed of a disk-shaped ceramic body, and at least the side of the torsional connector facing the piezoelectric oscillator is in the shape of a disk, and from the center of the piezoelectric oscillator. In the one in which the piezoelectric vibrator and the torsional connector are integrated by tightening with one bolt inserted through the central portion of the torsional connector, the diameter is smaller than 1/3 of the diameter of the piezoelectric oscillator, and is smaller than 1/8. A bolted ultrasonic ellipsoidal oscillator for a piezoelectric motor, characterized in that the bolt having a larger diameter is used.
JP60231020A 1985-10-18 1985-10-18 Bolt tightening ultrasonic elliptical transducer for piezoelectric motor Expired - Lifetime JPH0736709B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60231020A JPH0736709B2 (en) 1985-10-18 1985-10-18 Bolt tightening ultrasonic elliptical transducer for piezoelectric motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60231020A JPH0736709B2 (en) 1985-10-18 1985-10-18 Bolt tightening ultrasonic elliptical transducer for piezoelectric motor

Publications (2)

Publication Number Publication Date
JPS6292780A JPS6292780A (en) 1987-04-28
JPH0736709B2 true JPH0736709B2 (en) 1995-04-19

Family

ID=16916996

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60231020A Expired - Lifetime JPH0736709B2 (en) 1985-10-18 1985-10-18 Bolt tightening ultrasonic elliptical transducer for piezoelectric motor

Country Status (1)

Country Link
JP (1) JPH0736709B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114915208B (en) * 2022-07-12 2024-03-01 合肥工业大学 Longitudinal cutting composite piezoelectric motor

Also Published As

Publication number Publication date
JPS6292780A (en) 1987-04-28

Similar Documents

Publication Publication Date Title
JPH0374183A (en) Ultrasonic motor
JPH0736709B2 (en) Bolt tightening ultrasonic elliptical transducer for piezoelectric motor
JPH0514512B2 (en)
JPH0150195B2 (en)
JPH0150196B2 (en)
JP3297211B2 (en) Ultrasonic motor
JPS61244280A (en) Vibration-confining type supersonic wave motor
JPS6152164A (en) Cantilever beam supersonic elliptical vibrator
JP2897259B2 (en) Ultrasonic motor
JP2814583B2 (en) Ultrasonic motor
JPS60148385A (en) Ring-shaped supersonic vibrator of twisting and bending mode
JP2615953B2 (en) Ultrasonic motor and its driving method
JPS60113672A (en) Piezoelectric rotary machine
JPS6149668A (en) Piezoelectric motor using bent supersonic vibrator
JP3392005B2 (en) Ultrasonic motor and rotor used therein
JPS61150675A (en) Biresonance supersonic wave motor
JP2605121B2 (en) Ultrasonic vibrator and ultrasonic motor using the same
JP3302156B2 (en) Ultrasonic drive
JP2568849B2 (en) Ultrasonic drive
JPS6062880A (en) Piezoelectric motor of spiral mode drive
JPH0787711B2 (en) Ultrasonic motor
JP2638943B2 (en) Ultrasonic motor and driving method thereof
JPH02228275A (en) Ultrasonic motor and method of drive thereof
JP2599920B2 (en) Ultrasonic drive
JP2566010B2 (en) Ultrasonic motor