JPH0340773A - Ultrasonic motor - Google Patents

Ultrasonic motor

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Publication number
JPH0340773A
JPH0340773A JP1176519A JP17651989A JPH0340773A JP H0340773 A JPH0340773 A JP H0340773A JP 1176519 A JP1176519 A JP 1176519A JP 17651989 A JP17651989 A JP 17651989A JP H0340773 A JPH0340773 A JP H0340773A
Authority
JP
Japan
Prior art keywords
piezoelectric ceramic
torsional vibration
plate
stator
ultrasonic motor
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.)
Granted
Application number
JP1176519A
Other languages
Japanese (ja)
Other versions
JP3000591B2 (en
Inventor
Osamu Onishi
修 大西
Osamu Myoga
修 冥加
Takeshi Inoue
武志 井上
Tadayasu Uchikawa
内川 忠保
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.)
NEC Corp
Original Assignee
NEC Corp
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 NEC Corp filed Critical NEC Corp
Priority to JP1176519A priority Critical patent/JP3000591B2/en
Publication of JPH0340773A publication Critical patent/JPH0340773A/en
Application granted granted Critical
Publication of JP3000591B2 publication Critical patent/JP3000591B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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

Abstract

PURPOSE:To drive a motor under optimum conditions by disposing a piezoelectric plate polarized circumferentially between a supporting plate at the center of a stator and a torsional vibration exciting piezoelectric ceramic element, and leading resonance state detecting electrodes from the main surface of the plate. CONSTITUTION:A disc-like or annular piezoelectric ceramic plate 13 polarized circumferentially for detecting a torsional vibration state is disposed between a supporting plate 15 and a torsional vibration exciting piezoelectric ceramic element 12. Resonance state detecting metal electrodes are formed on both side surfaces of the plate 13, and electric terminals 131, 132 are led therefrom. Accordingly, since whether the torsional vibration state is resonant or nonresonant can be detected, a motor can be driven in a state that its driving frequency is always resonance frequency of the torsional vibration. Thus, even if environments such as temperature, etc., is varied, it can be always continuously driven under optimum conditions.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、圧電振動子をステータとし、それに超音波槽
円振動を励振させ、前記ステータに圧接されたロータを
摩擦力を介して回転させる超音波モータに関するもので
ある。
Detailed Description of the Invention (Industrial Application Field) The present invention uses a piezoelectric vibrator as a stator, excites ultrasonic tank circular vibration in the stator, and rotates a rotor press-welded to the stator through frictional force. This relates to ultrasonic motors.

(従来の技術) 縦−捩り複合圧電振動子をステータとし、ステータの端
面にロータを圧接することにより回転力を発生させる構
成の超音波モータの例として、本発明者らの提案による
ものが特開昭63−149726号公報で開示されてい
る。この超音波モータの構成の側断面図を第3図に示す
。以下、図面を参照にしながら説明する。
(Prior Art) As an example of an ultrasonic motor having a configuration in which a vertical-torsion composite piezoelectric vibrator is used as a stator and a rotor is pressed against the end face of the stator to generate rotational force, the one proposed by the present inventors is particularly proposed. It is disclosed in JP-A-63-149726. A side sectional view of the configuration of this ultrasonic motor is shown in FIG. The following description will be made with reference to the drawings.

円筒あるいは円柱状で厚さ方向に分極された縦振動励振
用圧電セラミック素子11と円周方向に分極された捩り
振動励振用圧電セラミック素子12を、支持板15とと
もに、両圧電素子と同様に円筒あるいは円柱状の弾性体
16.17で挟んだものをステータとし、縦振動励振用
圧電セラミック素子11と捩り振動励振用圧電セラミッ
ク素子12にそれぞれ交流電源から同一周波数で位相が
異なる交流電圧を印加することによりステータの端面に
超音波楕円振動を励起する。このとき、駆動周波数ステ
ータの捩り振動の共振周波数に一致させると、ステータ
の円周方向の振動振幅が非常に大きい超音波楕円振動を
得ることができる。ステータの端面にはロータ21が配
置され、このロータ21は、ステータに固定されている
シャフト26に、ベアリング22、スペーサ23、バネ
24、ナツト25を設置することにより、ステータに対
して圧接されている。このように、超音波楕円振動状態
にあるステータにロータを圧接することにより、ロータ
に強い回転力が発生する。
A cylindrical or cylindrical piezoelectric ceramic element 11 for longitudinal vibration excitation polarized in the thickness direction and a piezoelectric ceramic element 12 for torsional vibration excitation polarized in the circumferential direction are mounted together with a support plate 15 in a cylindrical shape similar to both piezoelectric elements. Alternatively, a stator sandwiched between cylindrical elastic bodies 16 and 17 is used, and AC voltages having the same frequency and different phases are applied from an AC power source to the piezoelectric ceramic element 11 for longitudinal vibration excitation and the piezoelectric ceramic element 12 for torsional vibration excitation, respectively. This excites ultrasonic elliptical vibrations on the end face of the stator. At this time, if the driving frequency is made to match the resonant frequency of the torsional vibration of the stator, ultrasonic elliptic vibration with a very large vibration amplitude in the circumferential direction of the stator can be obtained. A rotor 21 is arranged on the end face of the stator, and the rotor 21 is pressed against the stator by installing a bearing 22, a spacer 23, a spring 24, and a nut 25 on a shaft 26 fixed to the stator. There is. In this way, by pressing the rotor against the stator that is in a state of ultrasonic elliptic vibration, a strong rotational force is generated in the rotor.

(発明が解決しようとする課題) 第3図に示す従来の超音波モータでは、あらかじめ設定
した周波数で駆動せざるを得ないため、温度変化や負荷
変動により超音波モータの捩り振動の共振周波数が変化
した場合に、駆動周波数が捩り振動の共振周波数からず
れてしまい、回転速度が遅くなってしまう問題があった
(Problems to be Solved by the Invention) The conventional ultrasonic motor shown in Fig. 3 has no choice but to be driven at a preset frequency, so temperature changes and load fluctuations may cause the ultrasonic motor's torsional vibration resonance frequency to change. When the frequency changes, there is a problem in that the drive frequency deviates from the resonance frequency of torsional vibration, resulting in a slow rotation speed.

(課題を解決するための手段) 本発明は、縦−捩り複合振動子をステータとして超音波
楕円振動を励起し、そのステータにロータを圧接するこ
とにより回転力を発生させる超音波モータにおいて、ス
テータ中央部の支持板と捩り振動励振用圧電セラミック
の間に、円周方向に分極された圧電セラミック板を駆動
電源には接続されない状態で配置し、該圧電セラミック
板の主面から共振状態検出用電極を取り出した構造を特
徴とする超音波モータである。
(Means for Solving the Problems) The present invention provides an ultrasonic motor that excites ultrasonic elliptical vibration using a vertical-torsion compound vibrator as a stator, and generates rotational force by press-contacting a rotor to the stator. A piezoelectric ceramic plate polarized in the circumferential direction is placed between the support plate in the center and the piezoelectric ceramic for torsional vibration excitation without being connected to a drive power source, and a piezoelectric ceramic plate is arranged from the main surface of the piezoelectric ceramic plate for resonance state detection. This is an ultrasonic motor characterized by a structure in which electrodes are taken out.

(作用) 第1図は、本発明における超音波モータの、ステータ部
の構成例を示す断面図である。以下、図面を参照しなが
ら説明する。
(Function) FIG. 1 is a cross-sectional view showing a configuration example of a stator portion of an ultrasonic motor according to the present invention. This will be explained below with reference to the drawings.

機械エネルギーの発生源は、第3図に示す従来の超音波
モータと同様に、円筒あるいは円柱状で厚さ方向に分極
された縦振動励振用圧電セラミック素子11と円周方向
に分極された捩り振動励振用圧電セラミック素子12が
支持板15をはさんだ構造のステータである。本発明の
超音波モータでは、これら二つの駆動用圧電セラミック
素子以外に、捩り振動状態検出用として、円板あるいは
円環状で円周方向に分極された圧電セラミック板13を
支持板15と捩り振動励振圧電セラミック素子12の間
に配置する。この圧電セラミック板13の両面には金属
電極を形成しそこから電気端子131,132を取り出
す。
The source of mechanical energy is a piezoelectric ceramic element 11 for longitudinal vibration excitation, which is cylindrical or cylindrical and polarized in the thickness direction, and a torsion polarized in the circumferential direction, as in the conventional ultrasonic motor shown in FIG. The stator has a structure in which a piezoelectric ceramic element 12 for vibration excitation is sandwiched between support plates 15. In the ultrasonic motor of the present invention, in addition to these two drive piezoelectric ceramic elements, a disk or annular piezoelectric ceramic plate 13 polarized in the circumferential direction is used to detect torsional vibration states in conjunction with a support plate 15. It is arranged between the excitation piezoelectric ceramic elements 12. Metal electrodes are formed on both sides of this piezoelectric ceramic plate 13, and electrical terminals 131 and 132 are taken out from there.

また、この金属電極とステータの間の電気的絶縁を保つ
ためにスペーサ14を配置する。圧電セラミック素子1
1.12.13とスペーサ14を支持板15とともに、
圧電素子と同様に円筒あるいは円柱状の弾性体16.1
7で挾んだものをステータとする。
Further, a spacer 14 is arranged to maintain electrical insulation between the metal electrode and the stator. Piezoelectric ceramic element 1
1.12.13 and spacer 14 together with support plate 15,
A cylindrical or cylindrical elastic body 16.1 similar to a piezoelectric element
Let the thing sandwiched in step 7 be the stator.

縦振動励振用圧電セラミック素子11と捩り振動励振用
圧電セラミック素子12からはそれぞれ111゜112
.121.122の電気端子を取り出す(第2図)。電
子端子111.112間には縦振動駆動用の交流電源か
ら交流電圧V、= A、sinωtを印加する。一方、
電気端子121,122間には捩り振動駆動用の交流電
源から同一周波数で位相が異なる交流電圧vT=ATS
in(ωt+Φ)を印加する。このように二つの圧電セ
ラミック素子に交流電圧を印加することにより、縦振動
と捩り振動の合成された超音波楕円振動が励起される。
111° and 112° from the piezoelectric ceramic element 11 for longitudinal vibration excitation and the piezoelectric ceramic element 12 for torsional vibration excitation, respectively.
.. Take out the electrical terminals 121 and 122 (Figure 2). An AC voltage V, = A, sin ωt is applied between the electronic terminals 111 and 112 from an AC power source for longitudinal vibration drive. on the other hand,
Between the electric terminals 121 and 122, an AC voltage vT=ATS with the same frequency and different phase is applied from an AC power source for torsional vibration drive.
Apply in(ωt+Φ). By applying an alternating current voltage to the two piezoelectric ceramic elements in this manner, ultrasonic elliptical vibration, which is a combination of longitudinal vibration and torsional vibration, is excited.

第1図のステータが捩り振動状態にある時、捩り振動の
変位はu=Bsin(ωt+Φ+0)で表され、■駆動
周波数が共振周波数よりも低い場合はO’<e<90°
、■駆動周波数が共振周波数と等しければe=90’、
■駆動周波数が共振周波数よりも高い場合は90’< 
e < isooの関係がある。また振動の歪は、S=
 −Csin(ωt+Φ+e)で表される。ここで歪量
Cは位置の関数であり、このCが最も大きくなるのは振
動の節の位置である支持板15の付近である。そこで、
支持板15に隣接する様に圧電セラミック板13を配置
すれば、電気端子131.132間には圧電効果により
歪に比例した電圧V8= −A35in(ωt+Φ十e
)が発生する。この電圧■8のOは、先に示したように
振動状態により変化する。逆にこの0を測定することに
より、駆動周波数と共振周波数のずれを知ることが可能
である。
When the stator in Fig. 1 is in a state of torsional vibration, the displacement of torsional vibration is expressed as u = B sin (ωt + Φ + 0), and ■ If the driving frequency is lower than the resonance frequency, O'< e < 90°
,■If the driving frequency is equal to the resonant frequency, e=90',
■If the driving frequency is higher than the resonance frequency, 90'<
There is a relationship of e < isoo. Also, the vibration distortion is S=
−Csin(ωt+Φ+e). Here, the amount of strain C is a function of position, and this C is largest near the support plate 15, which is the position of the vibration node. Therefore,
If the piezoelectric ceramic plate 13 is placed adjacent to the support plate 15, a voltage V8=-A35in(ωt+Φ10e
) occurs. This voltage (8) O changes depending on the vibration state as shown above. Conversely, by measuring this 0, it is possible to know the deviation between the drive frequency and the resonance frequency.

(実施例) 以下、本発明の実施例について図を参照にしながら説明
する。
(Example) Hereinafter, an example of the present invention will be described with reference to the drawings.

第2図は本発明の実施例の一つを示す超音波モータの断
面図である。第2図中、11は縦振動励振用の円筒状圧
電セラミック素子で、外径20mm、内径8mm、厚さ
0.5mmの厚み方向に分極されたセラミック板を12
2枚積したものである。各セラミック板の上下面はメタ
ライズされ、電極取り出し用の金属薄板を挾みながら分
極の向きが交互になるように積層されている。金属薄板
から取り出した電極は電気端子111112を通して外
部で縦振動駆動用交流電源に接続され、電圧■、が印加
される。
FIG. 2 is a sectional view of an ultrasonic motor showing one embodiment of the present invention. In Figure 2, 11 is a cylindrical piezoelectric ceramic element for longitudinal vibration excitation, and 12
It is a stack of two sheets. The top and bottom surfaces of each ceramic plate are metallized, and the ceramic plates are stacked with thin metal plates for taking out the electrodes in between so that the directions of polarization alternate. The electrodes taken out from the thin metal plate are externally connected to an AC power source for longitudinal vibration driving through electric terminals 111112, and a voltage 1 is applied thereto.

一方、12は捩り振動励振用円筒状圧電セラミック素子
で、外径20mm、内径8mm、厚さ1mmの円周方向
に分極されたセラミックを8枚積層したものである。積
層方法は前記圧電セラミック素子11と同様で電気端子
121.122を通して外部で捩り振動駆動用交流電源
に接続され、電圧■7が印加される。13は捩り振動状
態検出用の円板状圧電セラミック板で、外径20mm、
内径8mm、厚さ0.5mmの円周方向に分極された圧
電セラミック板で、上下主面はメタライズされ電気端子
131,132が接続されている。14は絶縁用のアル
ミナ板で、外径20mmN内径8mm、厚さ0.5mm
である。第2図では圧電セラミック板13の両主面にア
ルミナ板14を配置しているが、駆動電源と捩り振動状
態検出電圧を共通アースにし、今回は金属を用いた支持
板15に絶縁体を用いれば、アルミナ板14は省略可能
である。2個の駆動用圧電セラミック素子11,12、
捩り振動検出用圧電セラミック板13、アルミナ板14
を円柱状の金属製弾性体16.17で挟み、ステータを
構成している。
On the other hand, reference numeral 12 denotes a cylindrical piezoelectric ceramic element for torsional vibration excitation, which is made by laminating eight ceramic pieces polarized in the circumferential direction and having an outer diameter of 20 mm, an inner diameter of 8 mm, and a thickness of 1 mm. The lamination method is the same as that of the piezoelectric ceramic element 11, and the piezoelectric ceramic element 11 is connected to an AC power supply for driving torsional vibration externally through electric terminals 121 and 122, and a voltage 7 is applied. 13 is a disk-shaped piezoelectric ceramic plate for detecting torsional vibration state, with an outer diameter of 20 mm;
It is a piezoelectric ceramic plate polarized in the circumferential direction with an inner diameter of 8 mm and a thickness of 0.5 mm, and the upper and lower main surfaces are metallized and electrical terminals 131 and 132 are connected. 14 is an alumina plate for insulation, outer diameter 20 mm N inner diameter 8 mm, thickness 0.5 mm
It is. In Fig. 2, alumina plates 14 are arranged on both main surfaces of the piezoelectric ceramic plate 13, but the driving power source and torsional vibration state detection voltage are connected to a common ground, and this time an insulator is used for the metal support plate 15. For example, the alumina plate 14 can be omitted. two driving piezoelectric ceramic elements 11, 12;
Piezoelectric ceramic plate 13 for torsional vibration detection, alumina plate 14
is sandwiched between cylindrical metal elastic bodies 16 and 17 to constitute a stator.

ステータの上部にはシャフト26を固定しである。さら
に、円筒状のロータ21をステータに接触するように配
置し、ベアリング22、スペーサ23、コイルバネ24
、ナツト25により、ロータ21をステータに対して圧
接している。超音波モータの特性はロータの圧接力によ
り変化するが、この圧接力はナツト25を締め付けるこ
とにより最適値に調整可能である。
A shaft 26 is fixed to the upper part of the stator. Furthermore, a cylindrical rotor 21 is arranged so as to be in contact with the stator, and a bearing 22, a spacer 23, a coil spring 24
, a nut 25 presses the rotor 21 against the stator. The characteristics of the ultrasonic motor change depending on the pressure force of the rotor, and this pressure force can be adjusted to an optimum value by tightening the nut 25.

この超音波モータの捩り振動の共振周波数は、インピー
ダンス測定の結果32.3kHzであった。この超音波
モータを共振周波数よりも低い27kHzで駆動したと
ころ捩り振動駆動電圧■7と捩り振動状態検出電圧■8
の位相差0は18°であった。ここから駆動周波数を上
げて行くとともに位相差eも増加し、共振周波数付近の
32.1kHzで90’となり、36KHzでは163
゜となった。
The resonance frequency of torsional vibration of this ultrasonic motor was 32.3 kHz as a result of impedance measurement. When this ultrasonic motor was driven at 27kHz, which is lower than the resonance frequency, the torsional vibration drive voltage ■7 and the torsional vibration state detection voltage ■8
The phase difference 0 was 18°. From here, as the drive frequency increases, the phase difference e also increases, reaching 90' at 32.1kHz near the resonance frequency, and 163' at 36kHz.
It became ゜.

(発明の効果) 以上述べたように、本発明によれば捩り振動の状態が共
振、非共振のどちらであるがが検出できるので、駆動周
波数が常に捩り振動の共振周波数である状態で超音波モ
ータの駆動ができる。そのため温度等の環境が変化して
も常に最適な条件で駆動を続けることができるといった
長所を有し、工業的価値が多大である。
(Effects of the Invention) As described above, according to the present invention, it is possible to detect whether the state of torsional vibration is resonant or non-resonant. Can drive a motor. Therefore, it has the advantage that it can always continue to be driven under optimal conditions even if the environment such as temperature changes, and has great industrial value.

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

第1図は本発明のステータ部の一例を示す構成断面図、
第2図は本発明の超音波モータの実施例を示す断面図、
第3図は従来の超音波モータの側断面図である。 図において、11・・・縦振動駆動用圧電セラミック素
子、12・・・捩り振動駆動用圧電セラミック素子、1
3・・・捩り振動状態検出用圧電セラミック板、14・
・・絶縁板、15・・・金属製支持板、16.17・・
・金属製弾性体、21・・・ロータ、22・・・ベアリ
ング、23・・・スペーサ、24・・・コイルバネ、 25・・・ナツト、 26・・・シャフト、 111、112゜ 121、122.131.132・・・電気端子。
FIG. 1 is a structural sectional view showing an example of the stator section of the present invention,
FIG. 2 is a sectional view showing an embodiment of the ultrasonic motor of the present invention;
FIG. 3 is a side sectional view of a conventional ultrasonic motor. In the figure, 11... Piezoelectric ceramic element for longitudinal vibration drive, 12... Piezoelectric ceramic element for torsional vibration drive, 1
3... Piezoelectric ceramic plate for torsional vibration state detection, 14.
...Insulating plate, 15...Metal support plate, 16.17...
- Metal elastic body, 21... Rotor, 22... Bearing, 23... Spacer, 24... Coil spring, 25... Nut, 26... Shaft, 111, 112° 121, 122. 131.132...Electrical terminal.

Claims (2)

【特許請求の範囲】[Claims] (1)縦振動圧電素子と捩り振動圧電素子とが支持板を
介して配置された縦−捩り複合振動子を有するステータ
と、このステータに圧接されたロータとを備えた超音波
モータにおいて、ステータ中央部の支持板と捩り振動圧
電素子の間に、円周方向に分極され両面に電極が形成さ
れた圧電セラミック板が配置されている構造を特徴とす
る超音波モータ。
(1) In an ultrasonic motor that includes a stator having a longitudinal-torsional composite vibrator in which a longitudinally vibrating piezoelectric element and a torsionally vibrating piezoelectric element are arranged via a support plate, and a rotor that is press-welded to the stator, the stator An ultrasonic motor characterized by a structure in which a piezoelectric ceramic plate polarized in the circumferential direction and having electrodes formed on both sides is arranged between a support plate in the center and a torsionally vibrating piezoelectric element.
(2)円周方向に分極され両面に電極が形成された圧電
セラミック板は絶縁板を介して支持板と捩り振動圧電素
子の間に配置されている特許請求の範囲第1項記載の超
音波モータ。
(2) The ultrasonic wave according to claim 1, wherein the piezoelectric ceramic plate polarized in the circumferential direction and having electrodes formed on both sides is disposed between the support plate and the torsionally vibrating piezoelectric element with an insulating plate interposed therebetween. motor.
JP1176519A 1989-07-06 1989-07-06 Ultrasonic motor Expired - Lifetime JP3000591B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1176519A JP3000591B2 (en) 1989-07-06 1989-07-06 Ultrasonic motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1176519A JP3000591B2 (en) 1989-07-06 1989-07-06 Ultrasonic motor

Publications (2)

Publication Number Publication Date
JPH0340773A true JPH0340773A (en) 1991-02-21
JP3000591B2 JP3000591B2 (en) 2000-01-17

Family

ID=16015044

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1176519A Expired - Lifetime JP3000591B2 (en) 1989-07-06 1989-07-06 Ultrasonic motor

Country Status (1)

Country Link
JP (1) JP3000591B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0810675A1 (en) * 1991-10-21 1997-12-03 Canon Kabushiki Kaisha Vibration driven motor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0810675A1 (en) * 1991-10-21 1997-12-03 Canon Kabushiki Kaisha Vibration driven motor
US5886455A (en) * 1991-10-21 1999-03-23 Canon Kabushiki Kaisha Vibration driven motor

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