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JPH072028B2 - Ultrasonic motor - Google Patents
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JPH072028B2 - Ultrasonic motor - Google Patents

Ultrasonic motor

Info

Publication number
JPH072028B2
JPH072028B2 JP1062929A JP6292989A JPH072028B2 JP H072028 B2 JPH072028 B2 JP H072028B2 JP 1062929 A JP1062929 A JP 1062929A JP 6292989 A JP6292989 A JP 6292989A JP H072028 B2 JPH072028 B2 JP H072028B2
Authority
JP
Japan
Prior art keywords
piezoelectric element
rotary drum
driving body
cut
wave
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
JP1062929A
Other languages
Japanese (ja)
Other versions
JPH02241379A (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 JP1062929A priority Critical patent/JPH072028B2/en
Publication of JPH02241379A publication Critical patent/JPH02241379A/en
Publication of JPH072028B2 publication Critical patent/JPH072028B2/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〕 本発明は伸縮する積層形の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。
DETAILED DESCRIPTION OF THE INVENTION [Industrial field of use] The present invention relates to an ultrasonic motor using a stretchable laminated piezoelectric element as a drive source.

〔従来の技術〕[Conventional technology]

従来、積層形の圧電素子を用いた超音波モータの一例と
しては、第11図に示される。
FIG. 11 shows an example of a conventional ultrasonic motor using a laminated piezoelectric element.

第11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18の上部に振動板19が固着さ
れ、これらがケース15に取着されている。また、振動板
19の円板表面に対向せしめて、回転円板17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17の側面よ
り皿ばね20により押接し、これを固定する抑え金16など
一体的に軸13に回転可能なように軸着し、さらに圧電体
18に電線14を接続して超音波モータを一体構築してい
る。
FIG. 11 is a perspective view showing an example of a conventional ultrasonic motor, in which a vibration plate 19 is fixed to the upper portion of a ring-shaped piezoelectric body 18, and these are attached to a case 15. Also the diaphragm
The disc surface of 19 is made to face, the disc surface of the rotating disc 17 is brought into close contact, and the disc spring 20 is pressed from the side surface of the rotating disc 17 so that this face is strongly pressed. 16 etc. are integrally attached to the shaft 13 so that it can rotate,
The electric wire 14 is connected to 18 to integrally construct an ultrasonic motor.

かようなごとく構成された超音波モータは、電線14より
直流電源がパルス的に供給されると、圧電体18は円輪状
に複数的に分割され、交互に極性動作が隣り合わせにな
っているので、個個の円輪状の素子部位では厚み方向に
伸縮する。この表面に振動板19が固着されているので一
体的に変位し、この伸縮する振動数と振動板19の円輪部
の固有振動数が等しくなっているので、伸縮の振動は増
幅されて振動板19の表面が横振動、すなわち回転円板17
の回転方向の振動により波打ち的に厚み方向に変位を伴
って、電源の印加に相応して円輪の板面上に順次波が進
行して回転移動する。
In the ultrasonic motor configured as described above, when the DC power is supplied in a pulsed manner from the electric wire 14, the piezoelectric body 18 is divided into a plurality of circular rings, and the polar operations are alternately adjacent to each other. , Individual ring-shaped element parts expand and contract in the thickness direction. Since the diaphragm 19 is fixed to this surface, it is displaced integrally, and since the frequency of expansion and contraction is equal to the natural frequency of the circular ring portion of the diaphragm 19, the expansion and contraction vibration is amplified and vibrates. The surface of plate 19 vibrates laterally, that is, rotating disk 17
Due to the vibration in the rotation direction, the waves wavyly displace in the thickness direction, and the waves sequentially propagate and rotate on the plate surface of the circular ring in response to the application of the power source.

この表面には回転円板17が押接されているので、この押
接部の摩擦作用すなわち振動板19の横振動作用に対する
回転円板17の反作用により波の進行方向とは逆の方向へ
回転円板17は回転する。
Since the rotating disc 17 is pressed against this surface, it rotates in the direction opposite to the traveling direction of the wave due to the frictional action of this pressing portion, that is, the reaction of the rotating disc 17 against the lateral vibration action of the diaphragm 19. The disc 17 rotates.

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

しかし、上述した構成においては振動板19の表面波の速
度は、円輪の接線に対し幅方向(図中Wで示す)で一定
速に移動する。しかるに、軸13に対する変位角度θと、
その回転半径Rと、波の移動距離Sの間には、 S=Rθ の関係が必要であるが、振動板19の幅Wが線でない限り
回転半径Rは幅Wの分、上下限で差異があり、波の移動
一定とすれば、変位角度θは常に異った値となり、振動
板19が剛体である限り、変位角度θが異った運動は許さ
れず幅W上でスリップを伴って回転円板17は運動するこ
とになる。
However, in the above-mentioned configuration, the velocity of the surface wave of the diaphragm 19 moves to a constant velocity in the width direction (indicated by W in the figure) with respect to the tangent line of the circular ring. Therefore, the displacement angle θ with respect to the axis 13,
The relationship of S = Rθ is required between the radius of gyration R and the moving distance S of the wave. However, unless the width W of the diaphragm 19 is a line, the radius of gyration R is the difference of the width W in the upper and lower limits. Therefore, if the movement of the wave is constant, the displacement angle θ always has different values, and as long as the diaphragm 19 is a rigid body, movements with different displacement angles θ are not allowed, and there is a slip on the width W. The rotating disc 17 will move.

このことにより、回転トルクが有効に得られなかった
り、圧電体18側の力を増しても、それを受ける回転円板
17側の幅W0を増すと、前述のようにスリップが多くな
り、発熱などを伴い、幅W0を小さくせざるを得なくな
る。もちろん摩擦面積が小さくとも押接力を大きくすれ
ば摩擦力は増加するが、面圧が高くなると板面材の摩擦
量が増加するので実用には供されず、結果的に小さな容
量しか得られず、しかも効率が悪くなる。また半径を大
きくすれば、トルクは大きくなるが、現在の技術では大
きくすると、精度,安定性などの問題で余り大きく出来
ない。すなわち結果的に小容量のものしか製作されず、
大きな問題となっている。
As a result, even if the rotational torque cannot be effectively obtained or the force on the piezoelectric body 18 side is increased, the rotating disc that receives it can receive it.
If the width W 0 on the 17 side is increased, as described above, slips increase and heat is generated, so that the width W 0 must be reduced. Of course, even if the friction area is small, increasing the pressing force will increase the friction force, but if the surface pressure increases, the friction amount of the plate surface material will increase, so it will not be used in practice and as a result only a small capacity will be obtained. Moreover, the efficiency becomes poor. Further, if the radius is increased, the torque is increased. However, if the current technology is increased, the torque cannot be increased so much due to problems such as accuracy and stability. That is, as a result, only a small capacity is manufactured,
It's a big problem.

現在市販されている一般的な進行波型のものとしては、
容量4W,トルクT=4kg-cmと極めて小さなものが殆んど
である。
As a general traveling wave type currently marketed,
Most of them are extremely small with a capacity of 4 W and a torque T of 4 kg-cm.

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、高効率で大容量の超音波モータを提
案することにある。
The present invention has been made in view of the above points, and an object thereof is to propose an ultrasonic motor of high efficiency and large capacity.

〔問題点を解決するための手段〕 つまり、その目的を達成するための手段は、 イ.請求項第1項記載において 伸縮する積層形の圧電素子を駆動源とする超音波モータ
において、前記圧電素子の可動部先端に波動を伝播する
駆動体を固着して一体形成した駆動ブロックを得、この
先端にベアリングなどで軸支する回転ドラムを備え、前
記駆動体の先端部はこの回転ドラムの円周に沿って円弧
状または水平面状に形成すると共に、この円弧状の所要
の円周長さまたは水平長さを残して45度の角度で切り落
した面を形成し、この切り落す部位は左回転用には右側
を、右回転用には左側とし、また駆動体の幅は前記圧電
素子の幅と同等し、駆動体の先端部と回転ドラムとの隔
間は所要の隔間δをもたせ、且つ前記駆動ブロックを複
数に配設し、それぞれの圧電素子にパルス状の電圧を印
加せしめて所要の回転力を得るようにしたものである。
[Means for Solving Problems] In other words, the means for achieving the purpose are a. In the ultrasonic motor using the expanding and contracting laminated piezoelectric element as a drive source according to claim 1, a drive block is integrally formed by fixing a drive body that propagates a wave to a tip of a movable portion of the piezoelectric element, A rotary drum that is axially supported by a bearing or the like is provided at this tip, and the tip of the drive body is formed in an arc shape or a horizontal plane along the circumference of the rotary drum, and the required circumferential length of this arc shape is provided. Alternatively, a surface cut off at an angle of 45 degrees is formed leaving a horizontal length, and the cut-off portion is the right side for left rotation and the left side for right rotation, and the width of the driving body is the width of the piezoelectric element. The width of the drive block is equal to that of the rotary drum, and the gap between the tip of the driving body and the rotary drum is set to a required distance δ, and the driving blocks are arranged in plural, and a pulsed voltage is applied to each piezoelectric element. The one that obtains the required rotational force A.

ロ.請求項第2項記載において 前記駆動体の先端部は水平面とし、請求項第1項と同方
向の所要の長さを残して45度の角度で切り落し、この切
り落した先端面は水平面状または前記回転ドラムの円周
に沿って円弧状に形成し、この切り落した部位を回転ド
ラムの円周側に配設するようにしたものである。
B. In Claim 2, the tip of the drive body is a horizontal plane, and is cut off at an angle of 45 degrees leaving a required length in the same direction as in Claim 1, and the cut-off tip surface is horizontal or It is formed in an arc shape along the circumference of the rotary drum, and the cut-off portion is arranged on the circumference side of the rotary drum.

ハ.請求項第3項記載において 請求項第2項記載の駆動体の45度傾斜面に対向する側の
駆動体面が、前記回転ドラムの円周側に配設するように
したものである。
C. According to a third aspect of the present invention, the drive body surface on the side facing the 45-degree inclined surface of the drive body according to the second aspect is arranged on the circumferential side of the rotary drum.

ニ.請求項第4項記載において 前記駆動ブロックの圧電素子後端の固定部位に重り金を
取着し、これを板ばねで支持し、その板ばねの配設位置
を回転ドラムの外周面に対し略接線方向になるように
し、板ばねのばね力を駆動体の可動方向と同方向とする
と共に、所要の力を付与して静的に常に回転ドラムの外
径面を駆動体が押圧するようにし、さらに前記重り金が
板ばねの押圧方向以外には所要の隔間以上動じないよう
なストッパを設け、これらを一体構築したものである。
D. 5. The weight according to claim 4, wherein a weight is attached to a fixed portion of the rear end of the piezoelectric element of the drive block, the weight is supported by a leaf spring, and the position of the leaf spring is set substantially relative to the outer peripheral surface of the rotary drum. The tangential direction, the spring force of the leaf spring is in the same direction as the movable direction of the driving body, and the required force is applied so that the driving body always presses the outer diameter surface of the rotating drum statically. Further, a stopper is provided to prevent the weight from moving beyond a predetermined distance except in the pressing direction of the leaf spring, and these are integrally constructed.

ホ.請求項第5項記載において 前記請求項第1項記載の駆動体の先端部近傍に、回転ド
ラムの軸方向と同方向に丸,四角,三角,菱形,楕円な
どいずれかの形状の孔を穿設し、圧電素子よりの波動が
この孔部位にて応力集中できるようにし、この効果によ
り波動による変位量を増幅させたものである。
E. According to claim 5, a hole of any shape such as a circle, a square, a triangle, a rhombus, or an ellipse is bored in the vicinity of the tip of the drive body according to claim 1 in the same direction as the axial direction of the rotary drum. It is provided so that the wave from the piezoelectric element can concentrate the stress at this hole portion, and the displacement amount due to the wave is amplified by this effect.

ヘ.請求項第6項記載において 前記請求項第1項記載の駆動体の先端部を45度に切り落
した傾斜面とは反対側の端部を、圧電素子の幅側端部と
略同位置より外側へ前記傾斜面に対向せしめて45度に切
り落した凸起部を設け、さらにこの凸起部を圧電素子側
へ伸ばし、この伸ばした部分は圧電素子よりの波動伝播
系路が駆動体の側端部で反射し、回転ドラムに対設する
円周面の略中央部に入射することができる角度の切り落
した傾斜面とし、圧電素子よりの波動をサークルさせる
ようにしたものである。
F. In Claim 6, the end portion on the opposite side of the inclined surface obtained by cutting off the front end portion of the driving body according to Claim 1 at 45 degrees is outside the substantially same position as the width side end portion of the piezoelectric element. A bulge that is cut off at 45 degrees facing the inclined surface is provided, and the bulge is further extended to the piezoelectric element side, and this extended portion has the wave propagation system path from the piezoelectric element at the side end of the driver. The wave from the piezoelectric element is made to be a circle by forming an inclined surface that is cut off at an angle so that it can be reflected at a portion and can be incident on the substantially central portion of the circumferential surface opposite to the rotary drum.

ト.請求項第7項記載において 前記請求項第1項記載の駆動体の形状のものを、カギ
状、つまり圧電素子の可動方向根本より先端部に向けて
先細りの斜形に切り、その細り位置を前記45度に切り落
した底部の角位置の延直線上より(45度切り込みと反対
方向へ)所要量ずらした部位とし、ここより回転ドラム
の円周面に沿って対向する部位を、連続させて一体形成
し、圧電素子よりの波動による変位量を斜形部で増幅す
るようにしたものである。
G. In claim 7, the shape of the driving body according to claim 1 is cut into a hook shape, that is, a taper oblique shape from the root of the piezoelectric element in the movable direction toward the tip, and the narrowed position From the angled straight line of the bottom cut off at 45 degrees (in the direction opposite to the 45-degree cut), the required amount of deviation was made, and from here, the areas facing along the circumferential surface of the rotary drum were made continuous. It is formed integrally and the displacement amount due to the wave motion from the piezoelectric element is amplified by the oblique portion.

チ.請求項第8項記載において 前記請求項第1項記載の駆動体の先端部を水平面とし、
この面に対向せしめてベアリングなどで水平方向に可動
できる水平軸を備え、この水平軸と駆動体の水平面間に
所要の隙間をもたせて複数的に左右可動できるように上
下に駆動ブロックを配設し、前記水平軸が左右にリニア
ー駆動できるようにした特許請求の範囲第1項または第
2項または第5項または第6項または第7項記載したも
のである。
J. In Claim 8, the front end portion of the driving body according to Claim 1 is a horizontal plane,
It is equipped with a horizontal shaft that can be moved horizontally with bearings facing this surface, and drive blocks are arranged vertically so that multiple horizontal movements can be made with a required gap between this horizontal shaft and the horizontal plane of the driver. However, the horizontal axis can be linearly driven to the left and right, and the first, second, fifth, sixth, or seventh claims are described.

〔作用〕[Action]

その作用は、次に説明する実施例において併せて詳述す
る。
The operation will be described in detail in the embodiments described below.

以下、本発明の超音波モータの一実施例を、図面に基づ
き請求項別に説明する。
An embodiment of the ultrasonic motor of the present invention will be described below for each claim with reference to the drawings.

〔実施例〕〔Example〕

第1図は本発明の一実施例を示す全体構成図、第2図は
第1図の側面断面図である。
FIG. 1 is an overall configuration diagram showing an embodiment of the present invention, and FIG. 2 is a side sectional view of FIG.

1) 請求項第1項において 伸縮する積層形の圧電素子1を駆動源とする超音波モー
タにおいて、前記圧電素子1の可動部先端に波動を伝播
する駆動体2を固着して一体形成した駆動ブロックイを
得、この先端にベアリング4などで軸支する回転ドラム
3を備え、駆動体2の先端部はこの回転ドラム3の円周
に沿って円弧状または水平面状に形成すると共に、この
円弧状の所要の円周長さまたは水平長さを残して45度の
角度で切り落した面(以降傾斜面ともいう)2aを形成
し、この切り落す部位は左回転用には右側を、右回転用
には左側とし、また駆動体2の幅は圧電素子1の幅と同
等し、駆動体2の先端部と回転ドラム3との隔間は所要
の隔間δをもたせ、且つ前記駆動ブロックイ,ロを左回
転用と右回転用とを対称的に配設し、それぞれの圧電素
子1にパルス状の電圧Eを印加せしめて所要の回転力を
得るようにしたものである。
1) In the ultrasonic motor using the expandable and contractable laminated piezoelectric element 1 as a drive source, a driving body 2 for propagating a wave is integrally fixed to a tip of a movable portion of the piezoelectric element 1 for driving. A block drum is obtained, and a rotary drum 3 pivotally supported by a bearing 4 or the like is provided at the tip of the block. The tip of the driving body 2 is formed along the circumference of the rotary drum 3 in an arc shape or a horizontal plane shape. A surface (hereinafter also referred to as an inclined surface) 2a is formed by cutting off at an angle of 45 degrees, leaving the required arcuate circumferential length or horizontal length, and the cut-off portion is the right side for left rotation and the right rotation. The width of the driving body 2 is equal to the width of the piezoelectric element 1, the distance between the tip of the driving body 2 and the rotary drum 3 has a required distance δ, and the driving block is , B are symmetrically arranged for left rotation and right rotation, and It is obtained so as to obtain a required rotational force brought applying a pulse voltage E to conductive elements 1.

次にその作用について第6図を参照しながら説明する。Next, the operation will be described with reference to FIG.

圧電素子1へパルス状の高周波電圧Eを左用の駆動ブロ
ックイに印加すると、圧電素子1は上下方向に伸びて変
位する。この変位動は駆動体2に伝達され、これの可動
と同時にその力は波動Y,Y′(以降縦波という)となっ
て回転ドラムのある方向に伝達される。駆動体2の45度
傾斜面に包含される縦波Yは切り落した面2a、すなわち
傾斜面2a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σCが
極めて差がある場合、例えば実験では駆動体2にアルミ
ニウムを使用したので、密度ρ=2.7g/cm3,波動伝播速
度C=約4000m/sに対し、空気はρ=1.3×10-3g/cm3,C
=340m/sなので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C点においてほぼ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
度の反射のC点では入射角と直角の水平方向に伝播さ
れ、横波Yxとなって左方向に進行する。加えて駆動体2
の側表面には表面波(一般にレイレイ波)Bが発生し、
横波Yxと合流してポテンシャルを上げて波動伝播する。
同時に駆動体2より伝達される45度面以外の縦波Y′と
合成される。
When the pulsed high-frequency voltage E is applied to the left driving block B to the piezoelectric element 1, the piezoelectric element 1 is extended and displaced in the vertical direction. This displacement movement is transmitted to the driving body 2, and at the same time as the movement thereof, its force becomes waves Y, Y '(hereinafter referred to as longitudinal waves) and is transmitted in a certain direction of the rotary drum. When the longitudinal wave Y included in the 45 ° inclined surface of the driving body 2 hits the cut surface 2a, that is, the inclined surface 2a, 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 When σC is extremely different, for example, since aluminum was used for the driver 2 in the experiment, the density ρ = 2.7 g / cm 3 , the wave propagation velocity C = about 4000 m / s, and the air ρ = 1.3 × 10 − 3 g / cm 3 , C
= 340 m / s, there is a large difference, so the existence of the medium is ignored, and if the surface is smooth, almost 100% is reflected at point C. The angle of reflection in this case is treated exactly like light,
At point C, which is a reflection of degrees, the wave propagates in the horizontal direction at a right angle to the incident angle and becomes a transverse wave Y x , which travels leftward. In addition, driver 2
A surface wave (generally Ray-Ray wave) B is generated on the side surface of
It merges with the transverse wave Y x to raise the potential and propagate waves.
At the same time, it is combined with the longitudinal wave Y ′ transmitted from the driving body 2 other than the 45 ° plane.

すなわち、縦,横波の速度Vx,Vyは合成され、駆動体2
の内部でZ面を頂点とした微少移動の右廻りの楕円運動
Xが得られる。このとき、圧電素子1の変位は駆動体2
の先端面(以降単に面ともいう)Zを下方に下げ、変位
εを伴って回転ドラム3の外径面を押圧する。この押
圧力に相応して摩擦力が発生し、楕円運動により回転ド
ラム3の外径面を左方向へ移動させる。そして、次の瞬
間には電源はパルス状の電圧Eなので、電源が切れると
圧電素子1は上方向へ縮み、駆動体2の面Zを上方へ移
動させ、回転ドラム3と駆動体2を当初の間隔δまで隙
間をあける。このとき、同時に波動による微少変位は、
波動が切れるので、駆動体2の材質による密度と弾性率
に相応して元の位置に復帰する。この繰り返しにより、
回転ドラム3は連続的に左方向に回転する。一般にはこ
の高周波電源のサイクルは20KHz〜100KHzであるが、実
験では約80KHzで駆動し、良好な回転駆動が得られた。
That is, the longitudinal and transverse wave velocities V x and V y are combined, and the driving body 2
The elliptic movement X in the clockwise direction of the minute movement with the Z plane as the apex is obtained inside the. At this time, the displacement of the piezoelectric element 1 is caused by the driving body 2
The tip surface (hereinafter also simply referred to as the surface) Z of is lowered downward, and the outer diameter surface of the rotary drum 3 is pressed with displacement ε 0 . A frictional force is generated according to this pressing force, and the outer diameter surface of the rotary drum 3 is moved leftward by the elliptic motion. Then, at the next moment, the power source is a pulse voltage E, so when the power source is turned off, the piezoelectric element 1 contracts upward, the surface Z of the driving body 2 is moved upward, and the rotary drum 3 and the driving body 2 are initially moved. Make a gap up to the interval δ of. At this time, the small displacement due to the wave motion is
Since the wave breaks, it returns to the original position according to the density and elastic modulus of the material of the driving body 2. By repeating this,
The rotary drum 3 continuously rotates to the left. Generally, the cycle of this high frequency power supply is 20KHz ~ 100KHz, but in the experiment, it was driven at about 80KHz and good rotation drive was obtained.

2) 請求項第2項において 請求項第1項と異なる点は、第3図に示すごとく、駆動
体2を45度の角度で切り落した面2aを回転ドラム3の円
周側に配設したことにある。そして、この切り落した面
2aは水平面または前述した円弧状となっている。従っ
て、駆動体2の先端部は水平に形成されている。
2) Claim 2 is different from Claim 1 in that, as shown in FIG. 3, the surface 2a obtained by cutting off the driving body 2 at an angle of 45 degrees is arranged on the circumferential side of the rotary drum 3. Especially. And this cut off surface
2a has a horizontal plane or the above-mentioned arc shape. Therefore, the tip of the driving body 2 is formed horizontally.

このようにして配設された駆動体2の作用は、請求項第
1項で説明した作用とほぼ同様の動作となり、圧電素子
1の変位により駆動体2は下方向へ変位εが生じて回
転ドラム3の外径面を押圧し、摩擦力を発生させて回転
駆動する。
The operation of the driving body 2 arranged in this way is almost the same as the operation described in claim 1, and the displacement of the piezoelectric element 1 causes the driving body 2 to be displaced downward ε 3. The outer diameter surface of the rotating drum 3 is pressed to generate a frictional force and drive the rotation.

3) 請求項第3項において 本発明も請求項第1項と同じ駆動ブロックイ,ロを使用
し、駆動体2の45度傾斜面、すなわち切り落した面2aに
対向する側の駆動体面が、回転ドラム3の円周側に配設
したものである。
3) In claim 3, the present invention also uses the same drive blocks a and b as in claim 1, and the 45 ° inclined surface of the driver 2, that is, the driver surface on the side facing the cut surface 2a is It is arranged on the circumferential side of the rotary drum 3.

このようにして配設した駆動ブロックにおいて、圧電素
子1の伸び変位は、45度の傾斜面で反射する横波Yx、そ
れ以外の縦波Y′となり、傾斜面と反対側の面Pにこれ
らの横波Yx,縦波Y′が合成され、微少移動の楕円運動
が得られ、これによって変位εにより回転ドラム3は
回転する。
In the drive block thus arranged, the expansion displacement of the piezoelectric element 1 becomes a transverse wave Y x reflected on the inclined surface of 45 degrees and a longitudinal wave Y ′ other than that, which is applied to the surface P opposite to the inclined surface. The transverse wave Y x and the longitudinal wave Y'of are combined to obtain an elliptic motion with a slight movement, whereby the rotary drum 3 is rotated by the displacement ε 4 .

4) 請求項第4項において 本発明は請求項第1項で得たものを、次に示すものに固
設することにある。
4) In claim 4, the present invention is to fix what is obtained in claim 1 to the following.

つまり、第1図に示す駆動ブロックイ、ロの圧電素子後
端の固定部位に重り金8を取着し、これを板ばね9で支
持し、その板ばね9の配設位置を回転ドラム3の外周面
に対し略接線方向になるようにし、板ばね9のばね力を
駆動体2の可動方向と同方向とすると共に、所要の力を
付与して静的に常に回転ドラム3の外径面に駆動体の面
Zが押圧するようにし、さらに重り金8が板ばね9の押
圧方向以外には所要の隔間以上動じないようなストッパ
11を設け、これらを一体構築したものである。
In other words, the weight bar 8 is attached to the fixed portion of the rear end of the piezoelectric element of the drive blocks B and B shown in FIG. 1, and the weight 8 is supported by the plate spring 9, and the position of the plate spring 9 is set to the rotary drum 3. Is substantially tangential to the outer peripheral surface of the rotary drum 3 so that the spring force of the leaf spring 9 is in the same direction as the moving direction of the driving body 2 and a required force is applied to statically keep the outer diameter of the rotary drum 3 constant. A stopper that allows the surface Z of the driving body to be pressed against the surface and prevents the weight bar 8 from moving more than the required distance except in the pressing direction of the leaf spring 9.
11 is provided and these are integrated.

かくして、このような状態で固設された駆動ブロックに
おいて、圧電素子1の変位量は数+ミクロンと極めて小
さいので、回転ドラム3の偏心や回転ドラム3に当接す
る駆動体2の面Zの摩耗などによりその力学的相対条件
は極めて不安定となる。すなわち、第6図に示す隔間δ
が大きくなれば、変位εは面Zを押圧しなくなり、小
さすぎれば大きくなり、微少楕円運動を損われて停止し
てしまう。そこで、板ばね9により面Zを常に一定の所
要力で押しておくことにより、駆動ブロックイ,ロは回
転ドラム3の外径面の変動にのみ追随させ、この板ばね
9を接線方向に配して面Zの駆動反力を受けても回転モ
ーメントは発生せず、上下方向以外の作用には動じ、ま
た回転ドラム3の回転速度は一般に50〜1000rpmと極め
て遅いので、その変動加速度は小さい。これに比べ、圧
電素子1の伸び変位は数万Hzであるので極めて早く、板
ばね9の応力が圧電素子1の戻るときの運動を阻害する
こともなく、圧電素子1の変位時の瞬時的な反力は重り
金8の慣性質量で受力し、力学的なバランスを保持す
る。
Thus, in the drive block fixed in such a state, the displacement amount of the piezoelectric element 1 is a few + micron, which is extremely small, so that the eccentricity of the rotary drum 3 and the wear of the surface Z of the drive body 2 abutting on the rotary drum 3 are caused. As a result, the mechanical relative condition becomes extremely unstable. That is, the interval δ shown in FIG.
Becomes larger, the displacement ε 0 does not press the surface Z, and becomes smaller if it becomes too small, the micro elliptical motion is impaired and the displacement is stopped. Therefore, by constantly pressing the surface Z by the leaf spring 9 with a constant required force, the drive blocks a and b are made to follow only the fluctuation of the outer diameter surface of the rotary drum 3, and the leaf spring 9 is arranged in the tangential direction. Even if it receives a driving reaction force of the vertical surface Z, no rotational moment is generated, it acts on the action other than the vertical direction, and the rotational speed of the rotary drum 3 is generally extremely slow at 50 to 1000 rpm, so that its fluctuating acceleration is small. On the other hand, the elongation displacement of the piezoelectric element 1 is tens of thousands of Hz, which is extremely fast, and the stress of the leaf spring 9 does not hinder the movement of the piezoelectric element 1 when returning, and the moment when the piezoelectric element 1 is displaced. The reaction force is received by the inertial mass of the weight 8 and maintains a mechanical balance.

これにより、偏心や摩耗などがあっても、駆動体2の面
Zは安定した駆動が得られる。
As a result, even if there is eccentricity or wear, the surface Z of the driving body 2 can be stably driven.

5) 請求項第5項において 請求項第1項の駆動体2の先端部近傍に、回転ドラム3
の軸方向と同方向に丸形状の孔7bを穿設し、圧電素子1
よりの波動がこの孔7b部位にて応力集中できるように
し、この効果により波動による変位量を増幅させる駆動
体7である。なお、孔の数は1個に限ったものではな
く、また孔径についても種種のものがある。
5) In claim 5, the rotary drum 3 is provided in the vicinity of the front end portion of the driving body 2 of claim 1.
A circular hole 7b is formed in the same direction as the axial direction of the piezoelectric element 1
This is the driving body 7 that allows the further wave to concentrate the stress in the hole 7b portion and to amplify the displacement amount due to the wave by this effect. The number of holes is not limited to one, and there are various kinds of hole diameters.

かような駆動ブロックにおいて、駆動体7の縦波Y′と
横波Yxの波動は応力集中効果により顕著に増幅され、微
少移動の楕円運動が増幅されて結果として強力で回転の
速い駆動が得られる。実験結果では回転ドラム3に対設
する駆動体7の面Z′より約0.8mmの肉を残して2mmの丸
孔を設けることにより、集中拡大率は4倍になり、孔な
しに比べ約2〜3倍のパワーアップとなった。
In such a driving block, the waves of the longitudinal wave Y ′ and the transverse wave Y x of the driving body 7 are remarkably amplified by the stress concentration effect, and the elliptical movement of the minute movement is amplified, resulting in a strong and fast rotating drive. To be According to the experimental results, by providing a round hole of 2 mm with a thickness of about 0.8 mm left from the surface Z ′ of the driving body 7 opposite to the rotary drum 3, the concentrated expansion rate is four times, which is about 2 times as compared with the case without the hole. 〜3 times more power up.

6)請求項第6項において 請求項第1項記載に類した駆動体5の先端部を45度に切
り落した傾斜面5aとは反対側の端部を、圧電素子1の幅
側端部と略同位置より外側へ傾斜面に対向せしめて45度
に切り落した凸起部5bを設け、さらにこの凸起5bを圧電
素子側へ伸ばし、この伸ばした部分は圧電素子1より波
動伝播系路がこのようにして得られた駆動体5の側端部
で反射し、回転ドラムに対設する円周面の略中央部に入
射することができる角度の切り落した傾斜面5cとし、圧
電素子1よりの波動をサークルさせるようにしたもので
ある。
6) In claim 6, the end opposite to the inclined surface 5a obtained by cutting off the tip of the driving body 5 similar to claim 1 at 45 degrees is referred to as the width side end of the piezoelectric element 1. Protruding part 5b cut off at 45 degrees by facing the inclined surface outward from approximately the same position is provided, and this protruding part 5b is further extended to the piezoelectric element side. The piezoelectric element 1 is provided with an inclined surface 5c that is cut off at an angle so that it can be reflected by the side end portion of the driving body 5 thus obtained and can be incident on the substantially central portion of the circumferential surface opposite to the rotary drum. It is made to make the wave motion of the circle.

かような駆動ブロックにおいて、第1図に示す駆動体2
の縦波Y′と横波Yxは回転ドラム3の外径面でその微少
移動を回転駆動に伝達しているが、そのエネルギ変換は
駆動体2の面Zのみで行われている。従って、この面Z
より内側の駆動体2内の波動は自身の移動を熱にして運
動指先となっている。
In such a driving block, the driving body 2 shown in FIG.
The longitudinal wave Y ′ and the transverse wave Y x of the rotary drum 3 transmit the minute movement to the rotational drive on the outer diameter surface of the rotary drum 3, but the energy conversion is performed only on the surface Z of the driving body 2. Therefore, this surface Z
The wave motion inside the driving body 2 on the inner side heats its own movement and becomes a moving fingertip.

そこで、本発明の駆動体5ではこの直接駆動に寄与しな
い波動をサークルさせて有効に使用するために、45度の
傾斜面5aの反射波動を、この傾斜面5aに対向した凸起面
5bの傾斜面5dで受け、ここで上方に反射させて傾斜面5c
に入進させる。もちろんこの部位は圧電素子1の幅側端
の外側に凸起させてあるので、圧電素子1よりの縦波
Y′と対向して混乱を起さないようにしてある。次に、
傾斜面5cで反射した波動は駆動体5の側端Dに当り、こ
こで反射し、更に回転ドラム3と対設する面Z″の略中
央に入進する。これにより、圧電素子1よりの縦波
Y′,Yはこの分下方に増強される。面Z″の摩擦係数を
μとすると、このμの分だけ下方への波動Y′が強くな
いと横波Yxに見合って駆動されないので、縦波Y′の波
動増強は極めて有効となり、変位εでもって回転ドラ
ム3は回転する。
Therefore, in the driving body 5 of the present invention, in order to effectively use the wave that does not contribute to the direct drive by making a circle, the reflected wave of the inclined surface 5a of 45 degrees is used as the convex surface facing the inclined surface 5a.
It is received by the inclined surface 5d of 5b, and is reflected upwards here, and the inclined surface 5c
Advance to. Of course, since this portion is raised outside the width-side end of the piezoelectric element 1, it is arranged so as not to be confused with the longitudinal wave Y'from the piezoelectric element 1. next,
The wave reflected on the inclined surface 5c hits the side end D of the driving body 5, is reflected there, and further advances to approximately the center of the surface Z ″ facing the rotating drum 3. The longitudinal waves Y ', Y are strengthened downward by this amount. If the friction coefficient of the surface Z ″ is μ, then the downward wave Y ′ is not strong enough by this μ, so it cannot be driven in proportion to the transverse wave Y x . , The wave enhancement of the longitudinal wave Y ′ is extremely effective, and the rotating drum 3 rotates with the displacement ε 1 .

7) 請求項第7項において 請求項第1項記載の駆動体2の形状のものを、カギ状、
つまり圧電素子1の可動方向根本より先端部に向けて先
細りの斜形6aに切り、その細り位置6bを45度に切り落し
た底部の角位置の延直線上より(45度切り込みと反対方
向へ)所要量ずらした部位6cとし、ここより回転ドラム
3の円周面に沿って対向する部位6cを連続させて一体形
成し、圧電素子1よりの波動による変位量を斜形部で増
幅するようにしたものである。
7) In claim 7, the shape of the driving body 2 according to claim 1 is changed to a key shape,
In other words, from the movable direction of the piezoelectric element 1 to a taper slanted shape 6a toward the tip, cut the tapering position 6b to 45 degrees from the bottom straight line of the angular position (in the direction opposite to the 45 degree cut) The portion 6c is deviated by a required amount, and the portion 6c facing the circumferential surface of the rotary drum 3 is continuously formed integrally from here, so that the displacement amount due to the wave from the piezoelectric element 1 is amplified by the oblique portion. It was done.

かくしてこのように構成された駆動ブロックにおいて、
第1図に示す駆動体2の縦波Yに対し、本発明の駆動体
6においては、根本へ向けて斜形6aに細らせてあるの
で、この根本の断面積と細り先端の断面積の比率分だけ
縦波Y,Y′は増幅強化され、45度の反射面に縦波Yは入
射して直角に移動し、横波Yxとなる。またこの45度傾斜
面の底端部の左寄りの部位の下方面、回転ドラム3に対
設する面Zでは、増幅された縦波Y′と、横波Yxが合成
され、強力な微少移動の楕円波が得られる。
Thus, in the drive block configured in this way,
In contrast to the longitudinal wave Y of the driving body 2 shown in FIG. 1, in the driving body 6 of the present invention, since the slanting shape 6a is narrowed toward the root, the cross-sectional area of this root and the cross-sectional area of the tapered tip are shown. The longitudinal waves Y and Y ′ are amplified and strengthened by the ratio of, and the longitudinal wave Y is incident on the reflection surface of 45 degrees and moves at a right angle to become a transverse wave Y x . Further, on the lower surface of the left end portion of the bottom end of the 45-degree inclined surface, the surface Z facing the rotary drum 3, the amplified longitudinal wave Y ′ and the transverse wave Y x are combined, and a strong slight movement is generated. An elliptical wave is obtained.

8) 請求項第8項において 請求項第1項記載の駆動体2の先端部を水平面とし、こ
の面に対向せしめてベアリングなどで水平方向に可動で
きる水平軸12を備え、この水平軸12が上下に備えた駆動
体2,2の水平面間に所要の隙間δをもたせて複数的に左
右可動できる駆動ブロックを配設し、水平軸12がリニア
ー駆動できるようにしたものである。
8) In claim 8, the tip end portion of the driving body 2 according to claim 1 is a horizontal plane, and a horizontal shaft 12 that is opposed to this surface and can be horizontally moved by a bearing or the like is provided. The horizontal shaft 12 can be linearly driven by disposing a drive block that can be horizontally moved in a plurality with a required gap δ between the horizontal planes of the upper and lower driving bodies 2, 2.

ここに、かようなごとく配設された駆動ブロックにおい
て、水平軸12を左または右側に移動させる場合には、左
用電源または右用電源により、圧電素子1にパルスを入
力する。このことによって、第1図で示した駆動体2の
作用によってその先端部の面Z′は水平軸12を押圧し、
水平軸12を所定の方向に移動させる。
Here, in the drive block thus arranged, when the horizontal axis 12 is moved to the left or right, a pulse is input to the piezoelectric element 1 by the left power source or the right power source. As a result, the surface Z'of the tip portion of the drive body 2 shown in FIG.
The horizontal shaft 12 is moved in a predetermined direction.

〔発明の効果〕〔The invention's effect〕

以上説明のごとく本発明のよれば、請求項第1項〜7項
に示した超音波モータは、従来のように駆動摩擦面の幅
Wによる半径差に起因するすべり摩擦運動がなく、回転
ドラム3の円周表面に面状に加力されるので、駆動効率
が高く長寿命が得られる。また、回転ドラム3の径およ
び長さを増し、これに対応させて駆動体2,5,6,7のブロ
ックの数を増せば大容量の製作は容易に無理なく可能と
なる。すなわち、従来のものはせいぜい容量4W程度が実
用的な限界であったものが、本発明では極めて大容量ま
で実用的に可能である。また従来例では回転円板17に摩
擦力を得るために皿ばね20によりスラスト力を付与して
いるので、この力はベアリング、軸13に加えられ、寿
命,強度など相応して不利になっていたが、本発明では
駆動体2,5,6,7のブロックを対称的に配し、回転ドラム
3の内力として相互にキャンセルするようにしたのでベ
アリング,軸へのこの種の付加はないので極めて経済的
に長寿命が得られる。
As described above, according to the present invention, the ultrasonic motor according to claims 1 to 7 has no sliding frictional motion due to the radius difference due to the width W of the driving friction surface unlike the conventional case, and the rotary drum is Since a force is applied to the circumferential surface of No. 3 like a plane, the driving efficiency is high and a long service life is obtained. Further, by increasing the diameter and length of the rotary drum 3 and correspondingly increasing the number of blocks of the driving bodies 2, 5, 6, 7, it is possible to easily and reasonably manufacture a large capacity. That is, the conventional one had a practical limit of about 4 W at the most, but the present invention allows a practically large capacity. Further, in the conventional example, since the thrust force is applied to the rotating disc 17 by the disc spring 20 to obtain the frictional force, this force is applied to the bearing and the shaft 13, which is disadvantageous in terms of life and strength. However, in the present invention, the blocks of the driving bodies 2, 5, 6, 7 are arranged symmetrically so as to cancel each other out as the internal force of the rotary drum 3, so this kind of addition to the bearing and shaft is not necessary. Extremely economical long service life.

さらに、請求項第5項,第7項では駆動体6,7の形状に
孔を明けたり、斜形にするなどの簡単な方法で効率が極
めて向上し、例えば当方の実験では2〜3倍の容量アッ
プが得られる効果的なものである。
Further, in claims 5 and 7, the efficiency is remarkably improved by a simple method such as making holes in the shape of the driving bodies 6 and 7 or making it oblique, and for example, in our experiment, it is 2-3 times as much. It is effective because it can increase the capacity.

また、請求項第6項では、駆動体5の形状を45度面に対
向した凸部を追加する簡易な方法で波動伝播をサークル
させ、縦波Y′を増強して極めて高い効率が得られる。
Further, in claim 6, the wave propagation is circled by a simple method in which the convex shape facing the 45 ° surface is added to the shape of the driving body 5, and the longitudinal wave Y ′ is enhanced to obtain extremely high efficiency. .

請求項第4項では回転ドラム3に偏心や押圧面Zに摩耗
が生じても、この面位置変動に追随して駆動体2,5,6,7
は回転ドラム3に対して一定の力学的要件を与えるので
実用化に極めて有効なものである。また、駆動体2,5,6,
7と回転ドラム3との間隔δはゼロになり、加えて駆動
体2,5,6,7内部での波動による微少の移動により力が伝
達されるので、実験では騒音は皆無であった。
According to the fourth aspect, even if the rotating drum 3 is eccentric or the pressing surface Z is worn, the driving bodies 2, 5, 6, 7 are tracked according to the surface position fluctuation.
Provides a certain mechanical requirement for the rotating drum 3 and is extremely effective for practical use. In addition, the driver 2,5,6,
The distance δ between the 7 and the rotary drum 3 becomes zero, and in addition, the force is transmitted by the minute movement due to the wave motion inside the driving bodies 2, 5, 6, 7, so that there was no noise in the experiment.

さらにまた、請求項第8項では回転駆動に替えて直線
(リニア)駆動を回転ドラム3の代りに水平軸12に配設
する簡単な手段で得られ、近年超精密な位置決めが要求
さる駆動源に用いれば1回の電源ON・OFFでサブミクロ
ンの可動が得られ、これを高周波で連続的に可動させる
のでデジタル指令により容易に高精度の位置決めが得ら
れる。
Furthermore, in claim 8, a linear drive instead of the rotary drive can be obtained by a simple means of arranging on the horizontal shaft 12 instead of the rotary drum 3, and in recent years, a drive source which requires ultra-precision positioning. If it is used for, the power of submicron can be obtained by turning the power supply on and off once, and this can be continuously moved at high frequency, so high precision positioning can be easily obtained by digital command.

よって本発明の超音波モータは、高容量,高効率でしか
も従来の電気モータに比べ極小の慣性モーメントで同等
の容量が得られ、しかも静止ブレーキも付与できサブミ
クロの駆動設定が容易に得るなど省力機器,ロボットな
ど極めて多用に実用的に供される有用なものである。
Therefore, the ultrasonic motor of the present invention has high capacity and high efficiency, and has the same capacity with a very small moment of inertia as compared with the conventional electric motor. Moreover, the static brake can be applied and the sub-micro drive setting can be easily achieved. It is a useful item that is practically used for a wide variety of equipment and robots.

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

第1図は請求項第1項の本発明の超音波モータの構造体
の一実施例を示す要部正面概念図、第2図は第1図の側
面概念図、第3図は請求項第2項の要部正面図、第4図
は請求項第3項の要部正面図、第5図は請求項第4項の
全体構成図、第6図は第1図の作用説明図、第7図は請
求項第5項の要部正面図、第8図は請求項第6項の要部
正面図、第9図は請求項第7項の要部正面図、第10図は
請求項第10項の全体構成図、第11図は従来のものの斜視
図である。 1……圧電素子、2,5,6,7……駆動体、3……回転ドラ
ム、4……ベアリング、8……重り金、9……板ばね、
10……受金、11……ストッパ、12……水平軸、13……
軸、14……電線、15……ケース、16……抑え金、17……
回転円板、18……圧電体、19……振動板、20……皿ば
ね。
FIG. 1 is a conceptual front view of an essential part showing an embodiment of the structure of the ultrasonic motor of the present invention according to claim 1, FIG. 2 is a side view conceptual view of FIG. 1, and FIG. 2 is a front view of an essential part of claim 3, FIG. 5 is an overall configuration diagram of claim 4, and FIG. 6 is an operation explanatory view of FIG. FIG. 7 is a front view of an essential part of claim 5, FIG. 8 is a front view of an essential part of claim 6, FIG. 9 is a front view of an essential part of claim 7, and FIG. FIG. 10 is an overall configuration diagram of item 10, and FIG. 11 is a perspective view of a conventional device. 1 ... Piezoelectric element, 2,5,6,7 ... driving body, 3 ... rotating drum, 4 ... bearing, 8 ... weight, 9 ... leaf spring,
10 …… Receipt, 11 …… Stopper, 12 …… Horizontal axis, 13 ……
Axis, 14 …… electric wire, 15 …… case, 16 …… presser plate, 17 ……
Rotating disk, 18 ... Piezoelectric body, 19 ... Vibration plate, 20 ... Disc spring.

Claims (8)

【特許請求の範囲】[Claims] 【請求項1】伸縮する積層形の圧電素子を駆動源とする
超音波モータにおいて、前記圧電素子の可動部先端に波
動を伝播する駆動体を固着して一体形成した駆動ブロッ
クを得、この先端にベアリングなどで軸支する回転ドラ
ムを備え、前記駆動体の先端部はこの回転ドラムの円周
に沿って円弧状または水平面状に形成すると共に、この
円弧状の所要の円周長さまたは水平長さを残して45度の
角度で切り落した面を形成し、この切り落す部位は左回
転用には右側を、右回転用には左側とし、また駆動体の
幅は前記圧電素子の幅と同等し、駆動体の先端部と回転
ドラムとの隔間は所要の隔間δをもたせ、且つ前記駆動
ブロックを複数に配設し、それぞれの圧電素子にパルス
状の電圧を印加せしめて所要の回転力を得るようにした
ことを特徴とする超音波モータ。
1. In an ultrasonic motor using an expanding and contracting laminated piezoelectric element as a drive source, a drive block for integrally propagating a wave is fixed to the tip of the movable portion of the piezoelectric element to obtain a drive block, and the tip is obtained. A rotary drum that is supported by bearings and the like, and the tip of the driving body is formed in an arc shape or a horizontal plane along the circumference of the rotary drum, and the arc has a required circumferential length or horizontal. Form a surface cut off at an angle of 45 degrees leaving the length, the cut-off part is the right side for left rotation, the left side for right rotation, and the width of the driving body is the width of the piezoelectric element. Similarly, the required distance δ is provided between the tip of the driving body and the rotary drum, and a plurality of the driving blocks are arranged, and a pulsed voltage is applied to each piezoelectric element to obtain the required distance. Super characterized by trying to obtain rotational force Sonic motor.
【請求項2】前記駆動体の先端部は水平面とし、請求項
第1項と同方向の所要の長さを残して45度の角度で切り
落し、この切り落した先端面は水平面状または前記回転
ドラムの円周に沿って円弧状に形成し、この切り落した
面を回転ドラムの円周側に配設するようにしたことを特
徴とする特許請求の範囲第1項記載の超音波モータ。
2. A tip end portion of the drive body is a horizontal plane, and is cut off at an angle of 45 degrees leaving a required length in the same direction as in claim 1, and the cut-out tip end surface is a horizontal plane or the rotary drum. An ultrasonic motor according to claim 1, wherein the ultrasonic motor is formed in an arc shape along the circumference of the rotary drum, and the cut-off surface is arranged on the circumferential side of the rotary drum.
【請求項3】請求項第2項記載の駆動体の45度傾斜面に
対向する側の駆動体面が、前記回転ドラムの円周側に配
設するようにしたことを特徴とする特許請求の範囲第1
項および第2項記載の超音波モータ。
3. The drive body surface of the drive body according to claim 2, which is opposed to the 45-degree inclined surface, is arranged on the circumferential side of the rotary drum. Range first
Item 2. The ultrasonic motor according to item 2 or item 2.
【請求項4】前記駆動ブロックの圧電素子後端の固定部
位に重り金を取着し、これを板ばねで支持し、その板ば
ねの配設位置を回転ドラムの外周面に対し略接線方向に
なるようにし、板ばねのばね力を駆動体の可動方向と同
方向とすると共に、所要の力を付与して静的に常に回転
ドラムの外径面を駆動体が押圧するようにし、さらに前
記重り金が板ばねの押圧方向以外には所要の隔間以上動
じないようなストッパを設け、これらを一体構築したこ
とを特徴とする特許請求の範囲第1項記載の超音波モー
タ。
4. A weight is attached to a fixed portion of the rear end of the piezoelectric element of the drive block, and the weight is supported by a leaf spring, and the position of the leaf spring is arranged substantially tangential to the outer peripheral surface of the rotary drum. So that the spring force of the leaf spring is in the same direction as the movable direction of the driving body, and the required force is applied so that the driving body constantly presses the outer diameter surface of the rotating drum. The ultrasonic motor according to claim 1, wherein a stopper is provided so that the weight does not move beyond a predetermined distance except in the pressing direction of the leaf spring, and these are integrally constructed.
【請求項5】前記請求項第1項記載の駆動体の先端部近
傍に、回転ドラムの軸方向と同方向に丸,四角,三角,
菱形,楕円などいずれかの形状の孔を穿設し、圧電素子
よりの波動がこの孔部位にて応力集中できるようにし、
この効果により波動による変位量を増幅させることを特
徴とした特許請求の範囲第1項記載の超音波モータ。
5. A circle, a square, a triangle, in the same direction as the axial direction of the rotary drum, in the vicinity of the tip of the driving body according to claim 1.
A hole of any shape, such as a rhombus or an ellipse, is drilled so that waves from the piezoelectric element can concentrate stress at this hole.
The ultrasonic motor according to claim 1, wherein the displacement amount due to the wave is amplified by this effect.
【請求項6】前記請求項第1項記載の駆動体の先端部を
45度に切り落した傾斜面とは反対側の端部を、圧電素子
の幅側端部と略同位置より外側へ前記傾斜面に対向せし
めて45度に切り落した凸起部を設け、さらにこの凸起部
を圧電素子側へ伸ばし、この伸ばした部分は圧電素子よ
りの波動伝播系路が駆動体の側端部で反射し、回転ドラ
ムに対設する円周面の略中央部に入射することができる
角度の切り落した傾斜面とし、圧電素子よりの波動をサ
ークルさせるようにしたことを特徴とする特許請求の範
囲第1項記載の超音波モータ。
6. The front end portion of the driving body according to claim 1
An end on the opposite side of the inclined surface cut off at 45 degrees is provided with a raised portion cut off at 45 degrees by facing the inclined surface outward from substantially the same position as the width side end of the piezoelectric element. The raised portion is extended to the piezoelectric element side, and the extended portion is reflected by the wave propagation system path from the piezoelectric element at the side end portion of the driving body and is incident on the substantially central portion of the circumferential surface opposite to the rotary drum. The ultrasonic motor according to claim 1, characterized in that the inclined surface is cut off at an angle that allows the wave to be generated from the piezoelectric element to be circled.
【請求項7】前記請求項第1項記載の駆動体の形状のも
のを、カギ状、つまり圧電素子の可動方向根本より先端
部に向けて先細りの斜形に切り、その細り位置を前記45
度に切り落した底部の角位置の延直線上(45度切り込み
と反対方向へ)より所要量ずらした部位とし、ここより
回転ドラムの円周面に沿って対向する部位を連続させて
一体形成し、圧電素子よりの波動による変位量を斜形部
で増幅するようにしたことを特徴とする特許請求の範囲
第1項記載の超音波モータ。
7. The shape of the driving body according to claim 1 is cut into a hook shape, that is, an oblique taper from the root of the piezoelectric element in the movable direction toward the tip, and the narrowed position is 45.
The part that is offset by the required amount from the straight line of the angular position of the bottom part that is cut off in the opposite direction (in the direction opposite to the 45-degree cut) is formed continuously from this part so that the facing parts along the circumferential surface of the rotating drum are continuous. The ultrasonic motor according to claim 1, wherein the displacement amount due to the wave from the piezoelectric element is amplified by the oblique portion.
【請求項8】前記請求項第1項記載の駆動体の先端部を
水平面とし、この面に対向せしめてベアリングなどで水
平方向に可動できる水平軸を備え、この水平軸と駆動体
の水平面間に所要の隙間をもたせて複数的に左右可動で
きるよう上下に駆動ブロックを配設し、前記水平軸が左
右にリニアー駆動できるようにしたことを特徴とする特
許請求の範囲第1項または第2項または第5項または第
6項または第7項記載の超音波モータ。
8. A front end portion of the driving body according to claim 1 is formed into a horizontal plane, and a horizontal shaft which is opposed to this surface and can be horizontally moved by a bearing or the like is provided, and between the horizontal shaft and the horizontal plane of the driving body. The drive block is arranged vertically so that a plurality of movable blocks can be moved to the left and right with a required clearance, and the horizontal axis can be linearly driven to the left and right. The ultrasonic motor according to item 5, item 5, item 6, or item 7.
JP1062929A 1989-03-15 1989-03-15 Ultrasonic motor Expired - Lifetime JPH072028B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1062929A JPH072028B2 (en) 1989-03-15 1989-03-15 Ultrasonic motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1062929A JPH072028B2 (en) 1989-03-15 1989-03-15 Ultrasonic motor

Publications (2)

Publication Number Publication Date
JPH02241379A JPH02241379A (en) 1990-09-26
JPH072028B2 true JPH072028B2 (en) 1995-01-11

Family

ID=13214462

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1062929A Expired - Lifetime JPH072028B2 (en) 1989-03-15 1989-03-15 Ultrasonic motor

Country Status (1)

Country Link
JP (1) JPH072028B2 (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2574577B2 (en) * 1991-10-31 1997-01-22 松下電器産業株式会社 Linear actuator
JP2013255958A (en) * 2012-06-12 2013-12-26 Seiko Epson Corp Robot hand and robot
JP2021035213A (en) * 2019-08-27 2021-03-01 セイコーエプソン株式会社 Piezoelectric drive device and robot
CN110932594A (en) * 2019-11-15 2020-03-27 河南大学 Self-driven novel elastic actuating mechanism based on micro electro mechanical system
EP4391349B1 (en) * 2022-12-23 2025-10-01 The Swatch Group Research and Development Ltd Shock-resistant piezoelectric rotary motor, in particular for timepieces

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3309239A1 (en) 1983-03-15 1984-09-20 Siemens AG, 1000 Berlin und 8000 München Piezo-electric motor

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3309239A1 (en) 1983-03-15 1984-09-20 Siemens AG, 1000 Berlin und 8000 München Piezo-electric motor

Also Published As

Publication number Publication date
JPH02241379A (en) 1990-09-26

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