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JPH0710193B2 - Ultrasonic motor - Google Patents
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JPH0710193B2 - Ultrasonic motor - Google Patents

Ultrasonic motor

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Publication number
JPH0710193B2
JPH0710193B2 JP2227750A JP22775090A JPH0710193B2 JP H0710193 B2 JPH0710193 B2 JP H0710193B2 JP 2227750 A JP2227750 A JP 2227750A JP 22775090 A JP22775090 A JP 22775090A JP H0710193 B2 JPH0710193 B2 JP H0710193B2
Authority
JP
Japan
Prior art keywords
wave
driving
piezoelectric element
ultrasonic motor
piezoelectric
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
JP2227750A
Other languages
Japanese (ja)
Other versions
JPH04109880A (en
Inventor
重雄 桑原
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.)
Toyo Electric Manufacturing Ltd
Original Assignee
Toyo Electric Manufacturing 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 Toyo Electric Manufacturing Ltd filed Critical Toyo Electric Manufacturing Ltd
Priority to JP2227750A priority Critical patent/JPH0710193B2/en
Publication of JPH04109880A publication Critical patent/JPH04109880A/en
Publication of JPH0710193B2 publication Critical patent/JPH0710193B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は伸縮する圧電素子を駆動源とする超音波モータ
に関するものである。
The present invention relates to an ultrasonic motor having a piezoelectric element that expands and contracts as a drive source.

〔従来の技術〕[Conventional technology]

従来の伸縮形の圧電素子を用いた超音波モータの一例を
第3図に示す。
FIG. 3 shows an example of a conventional ultrasonic motor using a stretchable piezoelectric element.

第3図は従来の超音波モータの一例を示す斜視図であ
り、円輪状にした圧電体12の上部に振動板11が固着され
これらがケース14に取着されている。振動板11の円板表
面に対向させて回転円板10の円輪板面を密接させ、この
面を強く押すように回転円板10の側面より皿ばね9によ
り押接し、これを固定するように抑え金8で固定し、こ
れらを一体的に軸13に回転可能なように取着する。圧電
体12の構造は第4図に示すように円輪上を各々8個の伸
縮圧電素子に機能分割し、図中部分は電圧印加により
伸び、部分は縮むように分極化された機能をもち、こ
の,の素子を交互に配して8個連接してこれをA区
分とし、このブロックと3/4波長(入)間隔をあけて前
記同様,の交互に連接した8個の素子をB区分と
し、この各々の素子に通電されるようにA区分用の電線
15とB区分用の電線15′を接続して超音波モータを一体
構築している。15″は位相変換部である。
FIG. 3 is a perspective view showing an example of a conventional ultrasonic motor, in which a vibration plate 11 is fixed to an upper portion of a ring-shaped piezoelectric body 12 and these are attached to a case 14. The disc surface of the vibrating plate 11 is opposed to the disc surface of the rotating disc 10 so that the disc surface is brought into close contact, and the disc spring 9 is pressed from the side face of the rotating disc 10 so as to firmly fix it. Are fixed with a presser plate 8 and are integrally attached to a shaft 13 so as to be rotatable. As shown in FIG. 4, the structure of the piezoelectric body 12 is divided into eight expanding and contracting piezoelectric elements on a circular ring, and the portion in the figure has a function of being polarized so that it is extended by applying a voltage and the portion is contracted. The elements of this are alternately arranged and connected to each other to form section A, and this block is divided into eight elements which are alternately connected to this block with a 3/4 wavelength (on) interval. And the electric wire for division A so that each element is energized.
The ultrasonic motor is integrally constructed by connecting 15 and the wire 15 'for B division. 15 ″ is a phase converter.

このように構成された超音波モータのA区分の電線15よ
り、パルス状の直流電源を供給すると、伸縮する素子が
連接されているので厚み方向で凹凸の変位がなされ、定
在波が発生する。この定在波は円輪全体に伝播される。
A区分への電源供給と同時にB区分へも同じ周波数でA
区分の電源に対し90度の位相遅れをもたせて電圧供給す
ると、ここでも凹凸の波動が発生し、A区分の波動と重
なりあって位相が90゜ずれているので、定在波が進行波
となり圧電体12と一体固着されている振動板11の円板表
面では波動がだ円運動する。この面に押圧されている回
転円板10は摩擦力により当然のことながら回転する。例
えばこの時(B区分の電源パルスが90度位相遅れ)回転
円板10が右回転するとすれば、左回転させる場合はA区
分の電源パルスに対し90度位相を進めて供給すればよ
い。すなわち、左,右自在に回転させるためには2系統
の各々同周波数で90度の位相遅れ,進みの電源供給が必
要となる。
When a pulsed DC power supply is supplied from the electric wire 15 of section A of the ultrasonic motor configured as described above, since the expanding and contracting elements are connected, unevenness is displaced in the thickness direction and a standing wave is generated. . This standing wave propagates throughout the ring.
At the same time as supplying power to section A, the same frequency is applied to section B as well.
When a voltage is applied to the power source of the section with a phase delay of 90 degrees, uneven waves are generated here as well, and because the wave overlaps with the wave of section A and the phase is shifted by 90 °, the standing wave becomes a traveling wave. On the disk surface of the vibrating plate 11 integrally fixed to the piezoelectric body 12, the wave motion makes an elliptic motion. The rotating disk 10 pressed against this surface naturally rotates due to the frictional force. For example, if the rotating disk 10 is rotated to the right at this time (the power supply pulse of the section B is delayed by 90 degrees), the phase may be advanced by 90 degrees with respect to the power supply pulse of the section A to rotate the disk 10 to the left. That is, in order to freely rotate left and right, it is necessary to supply power to the two systems at the same frequency and with a phase delay and lead of 90 degrees.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

しかし、上述した構成において、左,右自在の回転方向
を得るためには2系統で、同周波数の電源と90度の位相
差を必要とする。一方、超音波域の周波数は最低でも20
KHzで、実用の超音波モータでは約40KHzと高周波数であ
る。
However, in the above-mentioned configuration, in order to obtain left and right freely rotating directions, two systems require a power source of the same frequency and a phase difference of 90 degrees. On the other hand, the frequency in the ultrasonic range is at least 20.
At a frequency of KHz, a practical ultrasonic motor has a high frequency of about 40 KHz.

この高い周波数に対し、正確に90度の位相差を付けると
すれば、一例として40KHzの駆動周波数では(1/40KHz)
×(90゜/360゜)=6.25×10-6秒のパルス差をもたせて
電源供給する必要があるが、この精度が確保できず、効
率のよい回転駆動と安定した回転方向が得られない。更
に、この電源装置は極めて高価となり、超音波モータの
実用化に大きな問題となっている。
Assuming that a phase difference of 90 degrees is accurately applied to this high frequency, as an example, at a drive frequency of 40 KHz (1/40 KHz)
× (90 ° / 360 °) = 6.25 × 10 -6 It is necessary to supply power with a pulse difference of 10 -6 seconds, but this accuracy cannot be secured, and efficient rotation drive and stable rotation direction cannot be obtained. . Further, this power supply device becomes extremely expensive, which poses a serious problem in putting the ultrasonic motor into practical use.

本発明は上述した点に鑑みて創案されたもので、その目
的とするところは、高効率で安定した回転と経済性に富
んだ超音波モータを提案することにある。
The present invention has been made in view of the above points, and an object of the present invention is to propose an ultrasonic motor that is highly efficient, stable in rotation, and economical.

〔課題を解決するための手段〕[Means for Solving the Problems]

つまり、その目的を達成するための手段は、伸縮する圧
電素子を2個1対にして並列に配し,その一端に各々独
立した慣性体を配し,他端に2個の圧電素子を連係する
ように1個の駆動体を配してこれらをボルトなどにより
一体化して駆動ユニットを得,これを駆動源にする超音
波モータにおいて、 慣性体の上部位に横波動中の余剰波動が駆動時に阻
害をしないような反射経路となる所要の寸法のレ字状に
切り込みを設け,且つその上面を一直線上になし、 駆動体は略M字状に形成し,このM字状の両傾斜面
を45度に傾斜させ,且つ中央上部に溝を設け,余剰波動
が駆動時に阻害せず同時に縦波動の共振効果を高めるよ
うにM字状の両端と中央のそれぞれの底辺を一直線状に
なるよう形成し、 慣性体が弾性的に下方へ常に押圧するような機能を持た
せるよう圧電素子、慣性体および駆動体を一体化して高
性能の出力が得られる駆動ユニットを組み立て、駆動体
の先端を回転ドラムに弾性力を付与して押設させ、この
回転ドラムを軸,ベアリングなどで軸支してこれら一体
構成し、2個1対の圧電素子のいずれかに電源を供給す
ることにより、回転振動の正,逆回転を得るようにした
ものである。
In other words, the means for achieving the object is that two expanding and contracting piezoelectric elements are paired and arranged in parallel, independent inertial members are arranged at one end, and two piezoelectric elements are linked at the other end. As shown in Fig.2, one driving body is arranged and these are integrated by bolts etc. to obtain a driving unit. In an ultrasonic motor using this as a driving source, the surplus wave in the transverse wave is driven on the upper part of the inertial body. Sometimes, a cutout is provided in the shape of a letter to form a reflection path that does not interfere with it, and its upper surface is aligned, and the driving body is formed in a substantially M shape. Is inclined at 45 degrees, and a groove is provided in the upper part of the center, so that both ends of the M-shape and the bases of the center are in a straight line so that the excess wave does not hinder driving and at the same time enhances the resonance effect of the longitudinal wave. A machine that allows the inertial body to elastically press downward at all times. Assemble the piezoelectric element, the inertial body, and the driving body so as to have a high-performance output, and assemble the driving unit by pushing the tip of the driving body by applying elastic force to the rotating drum. A shaft, a bearing, and the like are pivotally supported to integrally form these members, and by supplying power to either one of a pair of piezoelectric elements, the forward and reverse rotations of the rotational vibration are obtained.

〔作 用〕[Work]

その作用は、次の述べる実施例と併せて説明する。 The operation will be described in combination with the embodiment described below.

〔実施例〕〔Example〕

第1図は本発明の一実施例を示す超音波モータの主要部
正面図、第2図はその側面図である。第1図,第2図に
おいて、伸縮する圧電素子1−a,1−aを2個一対にし
て左右並列に配し,その一端に各々独立した慣性体1−
cを配し,他端に2個の圧電素子1−a,1−aを連係す
るように1個の駆動体1−bを配してボルトなどで一体
構築した駆動ユニットを得,前記駆動体1−bは略M
字状に形成してその両傾斜面1−b1の角度をそれぞれ45
度にしかつ溝を設け、更にこれらの両側部と中央の三者
の底面を一直線状にして所要の形状寸法とし、また前記
慣性体1−cの上部位には、横波動中の余剰波動が駆動
時に阻害をしないような反射経路となる所要の寸法の
「レ」字状の切り込みを設けて傾斜面1−c1を形成し、
且つその上面を一直線上になし、更にこの外側部の上面
1−c3の幅と、前記駆動体1−bの外側部の底面1−b3
とを略同じ幅とし、慣性体1−cの中央部の上面の幅1
−c2と駆動体1−bの中央部の底面の幅1−b2とを略同
じ幅としてそれぞれ駆動体1−b,慣性体1−cを形成
し、これらと前記圧電素子1−aの三者をボルト7で締
結している。
FIG. 1 is a front view of a main part of an ultrasonic motor showing an embodiment of the present invention, and FIG. 2 is a side view thereof. In FIG. 1 and FIG. 2, two expanding and contracting piezoelectric elements 1-a and 1-a are arranged in a pair in the left-right direction, and independent inertial bodies 1-
c is arranged, and one driving body 1-b is arranged at the other end so as to link two piezoelectric elements 1-a and 1-a to obtain a driving unit 1 integrally constructed by bolts or the like. Driver 1-b is approximately M
It is formed in a letter shape and the angle of both inclined surfaces 1-b 1 is 45
And a groove is provided, and the bottom surfaces of the both sides and the center of the three members are aligned in a straight line to obtain a required shape and dimension. Further, the upper portion of the inertial body 1-c has a surplus wave during transverse wave motion. Forming the inclined surface 1-c 1 by providing a "L" -shaped notch of a required dimension that becomes a reflection path that does not obstruct when driving,
And without the upper surface in alignment, further the width of the upper surface 1-c 3 of the outer portion, the bottom surface 1-b 3 of the outer portion of the drive member 1-b
And have almost the same width, and the width 1 of the upper surface of the central portion of the inertial body 1-c
-C 2 and the width 1-b 2 of the bottom surface of the central portion of the driving body 1-b are set to have substantially the same width to form the driving body 1-b and the inertia body 1-c, respectively, and these and the piezoelectric element 1-a. The three members are fastened with bolts 7.

更に慣性体1−cを弾性的に下方に押圧するように慣性
体1−cの両側によりアームをL字状1−c4に形成し、
このそれぞれの先端にばね5を設け、慣性体1−cが上
下方向には自在に移動可能とし、その他の方向には固定
保持するようなガイド棒6を配している。
Further, arms are formed in an L-shape 1-c 4 by both sides of the inertial body 1-c so as to elastically press the inertial body 1-c downward.
A spring 5 is provided at the tip of each of them, and a guide rod 6 is arranged so that the inertial body 1-c can freely move in the vertical direction and is fixedly held in the other directions.

この駆動体1−bの先端を回転ドラム2にばね5の作用
により、弾性力を付与して押設させ、この回転ドラム2
を軸3,ベアリング4などで回転支持して一体構成する。
The tip of the driving body 1-b is applied to the rotating drum 2 by the action of the spring 5 so that the driving drum 1-b is elastically pressed and pushed.
Is integrally supported by rotatingly supporting the shaft 3 and the bearing 4.

次にその作用について説明する。Next, the operation will be described.

まず、左回転の場合について説明する。First, the case of counterclockwise rotation will be described.

二個一対に配した左右の圧電素子1−a,1−aの内、右
側のみパルス状の高周波電源Eを電線1−dを通して供
給すると、右側の圧電素子1−aは上下方向に伸びて変
位する。この変位は振動となって駆動体1−bに伝播さ
れ、下方向へY,Y′,Y″の縦波となって進行する。
Of the left and right piezoelectric elements 1-a, 1-a arranged in pairs, only the right side is supplied with the pulsed high frequency power source E through the electric wire 1-d, and the right side piezoelectric element 1-a extends vertically. Displace. This displacement is vibrated and propagated to the driving body 1-b, and propagates downward as Y, Y ′, Y ″ longitudinal waves.

この波動伝播は、駆動体1−bの右側の45度傾斜面1−
b1に包含される縦波Yは45度に切り落した面に当ると、
この面に接触する媒体の音響インピーダンス、つまり密
度ρと波動伝播速度Cとの積、ρ・Cが極めて差がある
場合、例えば実験では駆動体1−bにをアルミニウムを
使用したので、密度ρ=2.7g/cm3,波動伝播速度C=約4
000m/sに対し、空気はρ=1.3×10-3g/cm3,C=340m/sで
このρ・Cは極めて差があるので媒体の存在は無視さ
れ、面が平滑であれば傾斜面1−b1においてほぼ100%
反射される。この場合の反射の角度は光と全く同じに扱
われ、45度の傾斜面1−b1では入射角と直角の水平方向
に伝播され、横浜Yxとなって左方向に進行する。する
と、駆動体1−bの先端面1−b2に進行する縦波Y′と
波動が直角状な交じわり、合成されて波動はベクトル速
度(第1図中Q)をもっただ円運動となり、先端面1−
b2部位では右方から左方へ向けた微動変位が電源のパル
スサイクルで発生する。この先端面1−b2に回転ドラム
2が押接されているのでその摩擦力によって回転ドラム
2は右方から左方へ運動する。すなわち左回転する。
This wave propagation is due to the 45-degree inclined surface 1- on the right side of the driver 1-b.
When the longitudinal wave Y included in b 1 hits the surface cut off at 45 degrees,
When the acoustic impedance of the medium in contact with this surface, that is, the product of the density ρ and the wave propagation velocity C, ρ · C is extremely different, for example, since aluminum was used for the driver 1-b in the experiment, the density ρ = 2.7 g / cm 3 , wave velocity C = approx. 4
In contrast to 000m / s, air is ρ = 1.3 × 10 -3 g / cm 3 , C = 340m / s, and this ρ ・ C is very different, so the existence of the medium is ignored, and if the surface is smooth, it is inclined. Almost 100% on surface 1-b 1
Is reflected. The angle of reflection in this case is treated exactly the same as that of light, and is propagated in the horizontal direction at a right angle to the incident angle on the inclined surface 1-b 1 of 45 degrees, and becomes Yokohama Yx and proceeds to the left. Then, the longitudinal wave Y ′ traveling on the front end surface 1-b 2 of the driving body 1-b and the wave intersect at a right angle, and the wave is combined and the wave has an elliptic motion with a vector velocity (Q in FIG. 1). And the tip surface 1-
At the b 2 site, a slight displacement from right to left occurs in the pulse cycle of the power supply. Since the rotary drum 2 is pressed against the tip surface 1-b 2 , the rotary drum 2 moves from the right to the left due to the frictional force. That is, it rotates counterclockwise.

前記縦波動のうち右側部の縦波Y″はそのまま下方に進
行して駆動体1−bの底面1−b3で反射し、上方向へ進
行する。更にこの波動は慣性体1−cの上面1−c3で反
対して下方へ進行する。すなわち圧電素子1−aよりの
縦波動Y′とY″は慣性体1−cの上面1−c2,1−c3
駆動体1−bの底面1−b2,1−b3の対向面の距離Lに依
存する固有振動数fで反復伝播する。今縦波動の伝播速
度をC0とすれば、この固有振動数fは f=(C0/λ)=C0/2L ……………(1) λ:波長 となり、この固有振動数fと同数のパルス電源を圧電素
子1−aに供給することにより駆動ユニットは共振す
る。これにより圧電素子1−aの電流の流入値は共振効
果により3〜15倍も大きくなり、流入エネルギーは電気
→機械運動エネルギーに変換される。これに相応して圧
電素子1−aの歪み,力が増大する。一般に圧電素子1
−aは熱特性が低く、約150℃ぐらいで圧電特性が損な
われ、その体積が決まると最大電流値が決まり、相応し
て歪み,力も決まってしまう。しかもこの値は極めて低
く、例えば歪みなどは共振させない場合、約1μm以下
で、アクチュエータとして実用化するうえで障害とな
る。
The longitudinal wave Y ″ on the right side of the longitudinal wave travels downward as it is, is reflected by the bottom surface 1-b 3 of the driving body 1-b, and travels upward. Further, this wave is generated by the inertial body 1-c. Opposite to the upper surface 1-c 3 , the waves travel downward, that is, the longitudinal waves Y ′ and Y ″ from the piezoelectric element 1-a are the upper surfaces 1-c 2 and 1-c 3 of the inertial body 1-c and the driver 1. -B propagates repeatedly at a natural frequency f depending on the distance L of the opposing surfaces of the bottom surfaces 1-b 2 and 1-b 3 of -b. Assuming that the propagation velocity of the longitudinal wave is C 0 , this natural frequency f is f = (C 0 / λ) = C 0 / 2L ………… (1) λ: wavelength, and this natural frequency f The driving unit 1 resonates by supplying the same number of pulse power supplies to the piezoelectric element 1-a. As a result, the inflow value of the current of the piezoelectric element 1-a becomes 3 to 15 times larger due to the resonance effect, and the inflow energy is converted from electricity to mechanical kinetic energy. Correspondingly, the strain and force of the piezoelectric element 1-a increase. Generally piezoelectric element 1
-A has a low thermal property, and the piezoelectric property is impaired at about 150 ° C. When the volume is determined, the maximum current value is determined, and accordingly the strain and force are also determined. Moreover, this value is extremely low. For example, if strain is not resonated, the value is about 1 μm or less, which is an obstacle to practical use as an actuator.

本発明の駆動ユニット中の平行面のL寸法の形成(図
中、1−b3面と1−c3面との距離)は、前記の共振効果
を得るために極めて有益である。もし駆動体1−bの45
度面1−b1が延長され平行面1−b3が無い場合、縦波動
Y,Y′,Y″のうち共振に寄与するL寸法の部位は、1−c
2〜1−b2面の縦波動Y′のみが基本波動の振動伝播に
関与するので、圧電素子1−aに対する共振効果は小さ
くなり、結果として大きな出力鵜が得られない。もちろ
んの平行面1−b3が大きすぎると横波Yxの量が小さくな
り、合成楕円波動Qが適切に得られないので、バランス
よく設計することが必要である。
The formation of the L dimension of the parallel planes in the drive unit 1 of the present invention (the distance between the 1-b 3 plane and the 1-c 3 plane in the figure) is extremely useful for obtaining the above resonance effect. If driver 1-b 45
When the 1-b 1 surface is extended and the 1-b 3 parallel surface is absent, longitudinal wave motion
Of the Y, Y ′, Y ″, the part of L dimension that contributes to resonance is 1-c
Since only the longitudinal wave Y'of the 2 to 1-b 2 plane participates in the vibration propagation of the fundamental wave, the resonance effect on the piezoelectric element 1-a becomes small, and as a result, a large output cormorant cannot be obtained. Of course, if the parallel surface 1-b 3 is too large, the amount of the transverse wave Yx becomes small, and the synthetic elliptic wave Q cannot be obtained appropriately. Therefore, it is necessary to design with good balance.

前記横波となった波動Yxは、時差,その他の自由で完全
にベクトル化(楕円波動Q)されず余剰波動Zが生ず
る。これは左側の45度の傾斜面1−b1まで進行し、反射
して上方へ伝播する。更に左側の圧電素子1−aを通過
して慣性体1−cの「レ」字状に形成した傾斜面1−c1
に達し、ここで反射し、駆動ユニットの左側面で反射
する。
The wave Yx that has become the transverse wave is not vectorized completely (elliptic wave Q) due to time difference and other freedom, and a surplus wave Z is generated. This propagates to the 45-degree inclined surface 1-b 1 on the left side, is reflected, and propagates upward. Further, it passes through the left piezoelectric element 1-a, and the inclined surface 1-c 1 of the inertial body 1-c is formed in a "L" shape.
, And is reflected here, and is reflected on the left side surface of the drive unit 1 .

更にの余剰波動ZHF中央の溝W面で反射して進行し、左
側の駆動体1−bの45度面1−b1面で反射する。すなわ
ち余剰波動ZはZ1〜Z5までの経路を取り、その波動Zの
部位と進行方向は中央部の駆動力に直接寄与するベクト
ル化された楕円波動に干渉することなく進路を取り、駆
動を阻害しない。また上部位でベクトル化される楕円波
動Qの余剰波動の経路は、前記余剰波動ZのZ1〜Z5の経
路とは異なる。すなわちZ1′〜Z4′までは同経路である
が、Z5′以降は駆動体1−bの左側の反射面1−b1の代
わりにM字状の左側面で反射し、以下同様にしてZ5′〜
Zi′までの波動伝播となる。
Further, the surplus wave ZHF is reflected by the surface of the groove W in the center and travels, and is reflected by the 45-degree surface 1-b 1 of the left driver 1-b. That is, the surplus wave Z takes a path from Z 1 to Z 5 , and the part and the traveling direction of the wave Z take a path without interfering with the vectorized elliptical wave that directly contributes to the driving force of the central portion, and drive. Does not hinder. The path of the surplus wave of the elliptic wave Q vectorized at the upper portion is different from the path of Z 1 to Z 5 of the surplus wave Z. That is, the path from Z 1 ′ to Z 4 ′ is the same, but after Z 5 ′, instead of the left reflecting surface 1-b 1 of the driving body 1-b, the light is reflected by the M-shaped left side surface, and so on. And then Z 5 ′ ~
Wave propagation up to Zi '.

これにより、前述したことと相まって余剰波動Z,Z′は
総ての領域で駆動に寄与する楕円波動Qを阻害すること
なく処理される。
As a result, in combination with the above, the surplus waves Z and Z'are processed without obstructing the elliptic wave Q that contributes to driving in all regions.

従ってM字状の両側部の形成は、縦波動Y″の共振効果
の向上と余剰波動Z′の駆動阻害の防止の二つの効用目
的をもってなされている。もし前記の慣性体1−cの
「レ」字状の傾斜面1−c1がなく面一状とした場合、余
剰波動Z1はこの面で反射し、向きを変えて駆動体1−b
の左側の45度面1−b1に進入し、ここで反射して左から
右に向けて波動進行する。
Therefore, the formation of the both sides of the M-letter is performed for the two purposes of improving the resonance effect of the longitudinal wave Y ″ and preventing the driving inhibition of the surplus wave Z ′. In the case where there is no “” -shaped inclined surface 1-c 1 and the surface is made flush, the surplus wave Z 1 is reflected by this surface and changes its direction to change to the driving body 1-b.
It enters the 45-degree surface 1-b 1 on the left side of, and is reflected here and propagates in waves from left to right.

而して、この波動は駆動時の回転に寄与する楕円波動Q
を合成する横波動Yxと向きをまったく逆にして作用する
ので、極めて駆動を阻害し、性能低下をもたらす。すな
わち、本発明の有益性の主旨もここにある。
Thus, this wave is an elliptic wave Q that contributes to rotation during driving.
The transverse wave Yx that synthesizes is acted in the direction completely opposite to that of the transverse wave Yx, so that the drive is extremely hindered and the performance is deteriorated. That is, the gist of the usefulness of the present invention is also here.

次に右回転させる場合には、前記同様パルス状の高周波
電源Eを左側の圧電素子1−aに供給し、右側は切電し
ておけばよい。すなわち、左右任意の回転は二個一対の
圧電素子1−aの右側または左側のいづれか一方へ通電
切り換えすることにより容易に確実に得られる。
Next, when rotating to the right, the pulsed high frequency power source E may be supplied to the piezoelectric element 1-a on the left side and the right side may be turned off. That is, an arbitrary left / right rotation can be easily and surely obtained by switching energization to either the right side or the left side of the pair of piezoelectric elements 1-a.

今、駆動ユニットを複数個回転ドラム2に配し、その
摩擦が一様にならず、併せて回転ドラム2の偏心により
駆動摩擦面1−b2が径方向へ変動した場合でも、駆動ユ
ニットはここに独立して回転ドラム2に常に押設する
ようにばね5により弾性力を付与され追従するので、微
小な波動の歪みでも効率がよく駆動力に結びつき、長時
間使用してもその駆動性能は安定し、長寿命が得られ
る。
Now, even if a plurality of drive units 1 are arranged on the rotary drum 2 and the friction thereof is not uniform, and the drive friction surface 1-b 2 also fluctuates in the radial direction due to the eccentricity of the rotary drum 2, the drive unit 1 Since 1 independently follows and is elastically applied by the spring 5 so as to be always pressed against the rotary drum 2, even a slight distortion of the wave efficiently leads to the driving force, and even when used for a long time, The driving performance is stable and long life is obtained.

〔発明の効果〕〔The invention's effect〕

以上述べたように本発明によれば、従来では左右任意の
回転と安定な回転を得るためには、例えば40KHzの駆動
周波数に対し、2系統の同周波数でしかも90度の位相
差、すなわち (1/40KHz)×(90゜/360゜)=6.25×10-6秒 の遅速を正確に付した電源供給が必要であったが、本発
明では二個の圧電素子1−a,1−aの一方に電源を供給
し、他方を切ればよいので操作は簡単で容易に安定した
左右の回転が得られる。更に同種の実施例に比べても、
慣性体,駆動体の「レ」字状の凹み、M字状の形成によ
り、従来、例えば駆動時に余剰波動Zが駆動阻害してい
たものを無害な波動路に導き、縦波動Y′,Y″の共振効
果を高めるなどして駆動性能を飛躍的に向上させてい
る。また、経済性に関しても2系統の電源に対し1系統
でよく、その上、6.25×10-6秒の極小時間の位相差を必
要としないので、極めて電源装置が安価になるなど、本
発明の超音波モータは技術的にも経済的にも大きなメリ
ットが得られる有用なものである。
As described above, according to the present invention, conventionally, in order to obtain an arbitrary left / right rotation and stable rotation, for example, with respect to a drive frequency of 40 KHz, a phase difference of 90 degrees at the same frequency of two systems, that is, 1/40 KHz) × (90 ° / 360 °) = 6.25 × 10 −6 sec. It was necessary to accurately supply a power source, but in the present invention, two piezoelectric elements 1-a and 1-a are required. Since it suffices to supply power to one side and turn off the other side, the operation is simple and a stable left and right rotation can be obtained. Furthermore, compared to the same type of embodiment,
Due to the "L" -shaped depression and the M-shaped formation of the inertial body and the driving body, what was conventionally hindered by the surplus wave Z during driving, for example, is guided to a harmless wave path, and longitudinal waves Y ', Y The driving performance has been dramatically improved by increasing the resonance effect of the ″. In terms of economic efficiency, only one system is required for two power sources, and a minimum time of 6.25 × 10 −6 seconds is achieved. Since the phase difference is not required, the power supply device is extremely inexpensive, and the ultrasonic motor of the present invention is useful in that it has great technical and economic advantages.

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

第1図は本発明の一実施例を示す主要正面図、第2図は
その側面図、第3図は従来の一例を示す斜視図、第4図
は第3図中の圧電体の構造と電源関係を各々示す説明図
である。 ……駆動ユニット、1−a……圧電素子、1−b……
駆動体、1−c……慣性体、1−d……電線、2……回
転ドラム、3……軸、4……ベアリング、5……ばね、
6……ガイド棒、7……ボルト、8……抑え金、9……
皿ばね、10……回転円板、11……振動板、12……圧電
体、13……軸、14……ケース、15,15′……電線。
1 is a main front view showing an embodiment of the present invention, FIG. 2 is a side view thereof, FIG. 3 is a perspective view showing an example of the prior art, and FIG. 4 is a structure of the piezoelectric body in FIG. It is explanatory drawing which shows each power supply relationship. 1 ... Drive unit, 1-a ... Piezoelectric element, 1-b ...
Driver, 1-c ... Inertia, 1-d ... Electric wire, 2 ... Rotating drum, 3 ... Shaft, 4 ... Bearing, 5 ... Spring,
6 ... guide rod, 7 ... bolt, 8 ... presser foot, 9 ...
Disc springs, 10 ... rotating discs, 11 ... diaphragms, 12 ... piezoelectric bodies, 13 ... shafts, 14 ... cases, 15,15 '... electric wires.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】伸縮する圧電素子を2個一対にして並列に
配し,その一端に各々独立した慣性体を配し,他端に前
記2個の圧電素子を連係するように1個の駆動体を配し
てこれらをボルトなどにより一体化して駆動ユニットを
得,これを駆動源にする超音波モータにおいて、前記慣
性体の上部位に横波動中の余剰波動が駆動時に阻害をし
ないような反射経路となる所要の寸法のレ字状の切り込
みを設け,且つその上面を一直線上になし、前記駆動体
は略M字状に形成し,このM字状の両傾斜面を45度に傾
斜させ,且つ中央上部に溝を設け,余剰波動が駆動時に
阻害せず同時に縦波動の共振効果を高めるようにM字状
の両端と中央のそれぞれの底辺を一直線状になるよう形
成し、前記慣性体が弾性的に下方へ常に押圧するような
機能を持たせるよう前記圧電素子、慣性体および駆動体
を一体化して高性能の出力が得られる駆動ユニットを組
み立て、駆動体の先端を回転ドラムに弾性力を付与して
押設させ、この回転ドラムを軸,ベアリングなどで軸支
してこれら一体構成し、2個1対の圧電素子のいずれか
に電源を供給することにより、回転振動の正,逆回転を
得るようにしたことを特徴とする超音波モータ。
1. A pair of expanding and contracting piezoelectric elements are arranged in parallel, one independent body is provided at one end of the piezoelectric element, and the other piezoelectric element is connected to the other end of the piezoelectric element. In an ultrasonic motor using a body arranged and integrated with bolts or the like to obtain a drive unit, and using this as a drive source, surplus wave during transverse wave does not hinder during driving. A L-shaped notch with a required size to be a reflection path is provided, and the upper surface thereof is aligned, and the driving body is formed in a substantially M shape, and both M-shaped inclined surfaces are inclined at 45 degrees. In addition, a groove is provided at the upper center, and both ends of the M-shape and the bases of the center are formed in a straight line so as to enhance the resonance effect of the longitudinal wave without disturbing the excessive wave at the time of driving. It has a function that the body elastically presses downward all the time. The piezoelectric element, the inertial body, and the driving body are integrated to assemble a driving unit capable of obtaining a high-performance output, and the tip of the driving body is elastically applied to the rotating drum so as to push the rotating drum. An ultrasonic motor characterized by being configured such that they are integrally supported by means of, for example, and power is supplied to either one of a pair of piezoelectric elements to obtain normal and reverse rotation of rotational vibration.
JP2227750A 1990-08-29 1990-08-29 Ultrasonic motor Expired - Lifetime JPH0710193B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2227750A JPH0710193B2 (en) 1990-08-29 1990-08-29 Ultrasonic motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2227750A JPH0710193B2 (en) 1990-08-29 1990-08-29 Ultrasonic motor

Publications (2)

Publication Number Publication Date
JPH04109880A JPH04109880A (en) 1992-04-10
JPH0710193B2 true JPH0710193B2 (en) 1995-02-01

Family

ID=16865787

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2227750A Expired - Lifetime JPH0710193B2 (en) 1990-08-29 1990-08-29 Ultrasonic motor

Country Status (1)

Country Link
JP (1) JPH0710193B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105680718A (en) * 2016-04-11 2016-06-15 哈尔滨工业大学 Frog-shaped first-order longitudinal-vibration linear ultrasonic motor

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2013236470A (en) * 2012-05-09 2013-11-21 Seiko Epson Corp Piezoelectric motor, robot hand, robot, electronic component transfer device, electronic component inspection device, liquid sending pump, printing device, electronic clock, projection device, and transfer device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105680718A (en) * 2016-04-11 2016-06-15 哈尔滨工业大学 Frog-shaped first-order longitudinal-vibration linear ultrasonic motor

Also Published As

Publication number Publication date
JPH04109880A (en) 1992-04-10

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