JPH0479715B2 - - Google Patents
Info
- Publication number
- JPH0479715B2 JPH0479715B2 JP59173182A JP17318284A JPH0479715B2 JP H0479715 B2 JPH0479715 B2 JP H0479715B2 JP 59173182 A JP59173182 A JP 59173182A JP 17318284 A JP17318284 A JP 17318284A JP H0479715 B2 JPH0479715 B2 JP H0479715B2
- Authority
- JP
- Japan
- Prior art keywords
- ultrasonic transducer
- torsional
- bending
- resonator
- torsion
- 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
Links
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02N—ELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
- H02N2/00—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction
- H02N2/10—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing rotary motion, e.g. rotary motors
- H02N2/103—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing rotary motion, e.g. rotary motors by pressing one or more vibrators against the rotor
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02N—ELECTRIC MACHINES NOT OTHERWISE PROVIDED FOR
- H02N2/00—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction
- H02N2/0005—Electric machines in general using piezoelectric effect, electrostriction or magnetostriction producing non-specific motion; Details common to machines covered by H02N2/02 - H02N2/16
- H02N2/001—Driving devices, e.g. vibrators
- H02N2/0045—Driving devices, e.g. vibrators using longitudinal or radial modes combined with torsion or shear modes
Landscapes
- General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
- Apparatuses For Generation Of Mechanical Vibrations (AREA)
Description
〔産業上の利用分野および発明の目的〕
本発明は超音波振動子の改良に係り、振動子に
楕円運動の超音波振動を発生させ、しかもその励
振を容易にした超音波振動子を提供することを目
的とする。
〔従来の技術〕
従来の超音波振動子は、ランジユバン型で代表
されるように強力な縦振動を発生するのが目的で
あつた。一方、最近超音波モータ,超音波パーツ
フイーダなど超音波振動による強力な回転トルク
を利用する技術の開発が進められている。回転ト
ルクの発生方法は種々提案されているが、例えば
モータの固定子の表面に楕円運動を生じさせ、こ
れと圧着されたロータを回転させる方法が最も優
れていると考えられる。ここで、固定子として超
音波振動子の振動面が直接利用できれば好都合だ
が、1個の超音波振動子の表面に強力な楕円運動
を効率よく発生する方法が見出せなかつたので、
複数個の励振子を組み合わせるなど効率の低いし
かも強力でない振動しか発生できず実用性が不十
分であつた。
〔問題点を解決するための手段〕
この発明は上述した従来技術の欠点を解消する
もので、圧電振動子を用いて円筒状の捻り共振子
に捻り振動を励振する超音波振動子において、円
筒面に屈曲振動が寄生するごとく、円筒の直径と
肉厚の関係を選んだことを特徴とすることによつ
て、前述の目的を達成したものである。
本発明者はすでに、「捻りモードの超音波振動
子」と題して圧電厚み振動子、縦モード共振子,
捻り結合子および捻り共振子を一体構成した振動
子を提案した。その原理は、捻り共振子と縦振動
共振子とを捻り結合子で結合したものであり、双
方共に共振させる必要があつた。けれども、その
後捻り共振子は圧電厚み振動子で駆動するだけ
で、捻り振動を発振できることを見出し、本発明
が生じた。
本発明の捻り・屈曲モード結合型超音波振動子
の構成主要素は円筒状の捻り共振子だけであり、
共振条件に縦振動子,捻り共振子など余計な制約
が入らないので、効率よく捻り・屈曲モード結合
振動を発振でき、振動子の設計も容易となつた。
〔実施例〕
第1図および第2図は、超音波振動子の一例を
示す正面図おび側面図である。図中の1はセラミ
ツクからなる圧電厚み振動子、2は圧電厚み振動
子1の電極に付設されたリード線、3は捻り共振
子、4は座金、5はこれらを締めつけるキヤツプ
ボルトである。
これらの図に示すように、本発明の振動子の捻
り共振子3は底付き円筒形状を基本とし、基本形
状もしくは多少変形したものである。捻り・屈曲
モード結合条件は円筒状捻り共振子3の高さ、肉
厚が基本要素であり、両者を結合するのが円筒の
直径である。直径を変えると結合の仕方が変わる
ので、振動子に種々の振動モードを任意に実現す
ることができる。
なお、実際の振動子の見掛けの形状は例えば第
3図および第4図に示したように捻り結合子14
も利用しているが、捻り結合子14は単に圧電厚
み振動子11を用いて捻り共振子13に捻り振動
を発生させる効率を改善する手段であり、第1図
および第2図に示したように用い無くとも良い。
つまり、振動子に発生する捻り振動の共振周波数
は捻り結合子の影響を受けない。縦振動子に関し
ては全く不要であることが判明したので除外し
た。捻り結合子14を底付き円筒形捻り共振子1
3の底に、ボルト15で締め付けて接合した場
合、共振状態の励振条件に最も影響を与えるもの
は意外なことにボルト15の長さである。本発明
の捻り・屈曲モード結合型超音波振動子は設計の
仕方によつて様々なモードの振動を励振でき、機
能も異なるので用途が広い。
設計の仕方によつて励振される振動モードがど
のように変化し、振動子の機能がどのように変わ
るかを説明するのは容易でないので、実施例の中
から代表的な30例を選び次の表に示した。これら
の実施例は本発明の捻り・屈曲モード結合型超音
波振動子の各部の寸法の変更に伴つて振動子に励
振される振動モード及び振動子機能がどのように
変化するかを示したものである。ここで、まず寸
法を変更する部分を明らかにするため、各部の寸
法付号を第4図に示した。なお表に示す各実施例
において、全実施例にわたつて同一寸法にしたの
は捻り共振子の肉厚7mmと圧電振動子の厚さ2mm
である。これらを変更すると見掛け上結果が複雑
となり、混乱を招く恐れが生ずるだけで、本質的
に新規な情報として付加する内容が見い出せなか
つたので、例示を省略した。
表では変更する寸法を、捻り共振子、捻り結合
子,圧電振動子,座金,ボルトの5つのグループ
に大別し、共振子,結合子,圧電振動子について
は寸法変更が複数個所となるため、それぞれ細分
した。実施例は共振子の直径の大きさの順に示
し、各グループ間を二重罫線で区別した。寸法変
更に伴つて励振される振動モードの共振周波数と
振動モードおよび機能を右欄に示した。
本発明の捻り・屈曲モード結合型超音波振動子
の形態は第3図,第4図,第5図に示した3種類
に大別できる。第3図と第5図の振動子は同一部
品からなり、構成の仕方だけの違いである。すな
わち、第5図の振動子は捻り共振子13の内部に
捻り結合子14,セラミツクからなる圧電振動子
11,座金16を納め、ボルト15で内側から締
め付け固定した構成であり、よりコンパクトなこ
とおよび共振子底部外面の振動を利用するのに好
都合なことが特長である。
これらに対して第4図の振動子は、捻り共振子
13の円筒が直筒でなく、側面形状が台形をして
いる点に特徴がある。第2図,第4図の型式に対
する第3図の形式の違いは、円筒寸法でH=Hw
(第3図,第5図の型式)か、H≒Hw(第4図の
型式)かを見ればわかる。
表において、実施例No.4および6は第3図に示
したA型、実施例No.5および7は第5図に示した
C型であり、実施例No.8〜16はH−Hw=7mmで
あり、B型というよりはむしろA型の底部を面取
りした形状でありA型に分類される。実施例No.
1,2,3および実施例No.17〜30は第4図に示し
たB型である。表の右端欄に型式名を示す。
[Industrial Field of Application and Purpose of the Invention] The present invention relates to the improvement of an ultrasonic vibrator, and provides an ultrasonic vibrator that allows the vibrator to generate ultrasonic vibrations in an elliptical motion, and in which the excitation is facilitated. The purpose is to [Prior Art] The purpose of conventional ultrasonic transducers was to generate strong longitudinal vibrations, as typified by the Languevin type. On the other hand, the development of technologies that utilize the powerful rotational torque generated by ultrasonic vibrations, such as ultrasonic motors and ultrasonic parts feeders, has recently been progressing. Although various methods for generating rotational torque have been proposed, the most excellent method is, for example, to generate an elliptical motion on the surface of a motor stator and rotate a rotor that is crimped thereto. It would be convenient if the vibration surface of the ultrasonic vibrator could be used directly as a stator, but we could not find a way to efficiently generate strong elliptical motion on the surface of a single ultrasonic vibrator.
It was not practical because it required a combination of multiple exciters, which produced only low-efficiency and weak vibrations. [Means for Solving the Problems] The present invention solves the above-mentioned drawbacks of the prior art, and is an ultrasonic transducer that excites torsional vibration in a cylindrical torsional resonator using a piezoelectric vibrator. The above object has been achieved by selecting the relationship between the diameter and wall thickness of the cylinder so that bending vibration is parasitic on the surface. The present inventor has already developed a piezoelectric thickness vibrator, a longitudinal mode resonator, and a
We proposed a vibrator that integrates a torsion coupler and a torsion resonator. The principle is that a torsional resonator and a longitudinal vibration resonator are coupled by a torsional coupler, and it is necessary for both to resonate. However, it was subsequently discovered that a torsional resonator can oscillate torsional vibration simply by driving it with a piezoelectric thickness vibrator, and the present invention was created. The main component of the torsional/bending mode coupled ultrasonic transducer of the present invention is only a cylindrical torsional resonator,
Since there are no unnecessary restrictions such as longitudinal resonators or torsional resonators in the resonance conditions, it is possible to efficiently oscillate combined torsional and bending mode vibrations, and the design of the resonator has become easier. [Example] FIGS. 1 and 2 are a front view and a side view showing an example of an ultrasonic transducer. In the figure, 1 is a piezoelectric thickness vibrator made of ceramic, 2 is a lead wire attached to the electrode of the piezoelectric thickness vibrator 1, 3 is a torsion resonator, 4 is a washer, and 5 is a cap bolt for tightening these. As shown in these figures, the torsional resonator 3 of the vibrator of the present invention is basically a cylindrical shape with a bottom, and has a basic shape or a slightly modified shape. The basic elements of the torsion/bending mode coupling condition are the height and wall thickness of the cylindrical torsional resonator 3, and the diameter of the cylinder couples the two. Since changing the diameter changes the way of coupling, it is possible to arbitrarily realize various vibration modes in the vibrator. Note that the apparent shape of the actual vibrator is, for example, the torsion coupler 14 as shown in FIGS. 3 and 4.
However, the torsional coupler 14 is simply a means to improve the efficiency of generating torsional vibration in the torsional resonator 13 using the piezoelectric thickness vibrator 11, as shown in FIGS. 1 and 2. It is not necessary to use it.
In other words, the resonant frequency of torsional vibration generated in the vibrator is not affected by the torsional coupler. As it turned out that the longitudinal oscillator was completely unnecessary, it was excluded. The torsion coupler 14 is connected to the cylindrical torsion resonator 1 with a bottom.
When the bolts 15 are tightened and joined to the bottom of the housing 3, surprisingly, the length of the bolts 15 has the greatest influence on the excitation conditions of the resonance state. The torsional/bending mode coupled ultrasonic transducer of the present invention can excite vibrations in various modes depending on how it is designed, and has different functions, so it has a wide range of uses. Since it is not easy to explain how the excited vibration mode changes depending on the design method and how the function of the resonator changes, we selected 30 representative examples from among the examples. It is shown in the table below. These examples show how the vibration mode excited in the transducer and the transducer function change as the dimensions of each part of the torsional/bending mode coupled ultrasonic transducer of the present invention are changed. It is. First, in order to clarify the parts whose dimensions are to be changed, the dimension numbers of each part are shown in FIG. 4. In each of the examples shown in the table, the dimensions are the same for all examples: the thickness of the torsion resonator is 7 mm, and the thickness of the piezoelectric vibrator is 2 mm.
It is. If these were changed, the result would appear to be complicated and there would be a risk of confusion, and we could not find any content to be added as essentially new information, so we omitted the examples. In the table, the dimensions to be changed are roughly divided into five groups: torsion resonator, torsion coupler, piezoelectric vibrator, washer, and bolt.As for the resonator, coupler, and piezoelectric vibrator, there are multiple dimensions to be changed. , each subdivided. Examples are shown in order of the diameter of the resonator, and each group is distinguished by a double ruled line. The resonance frequency, vibration mode, and function of the vibration mode excited with the dimension change are shown in the right column. The configurations of the torsion/bending mode coupled ultrasonic transducer of the present invention can be roughly divided into three types shown in FIGS. 3, 4, and 5. The vibrators shown in FIG. 3 and FIG. 5 are made of the same parts and differ only in the way they are constructed. That is, the vibrator shown in FIG. 5 has a structure in which a torsion coupler 14, a piezoelectric vibrator 11 made of ceramic, and a washer 16 are housed inside a torsion resonator 13, and are secured by tightening from the inside with bolts 15, making it more compact. Another feature is that it is convenient for utilizing the vibration of the outer surface of the bottom of the resonator. In contrast, the vibrator shown in FIG. 4 is characterized in that the cylinder of the torsional resonator 13 is not a straight cylinder, but has a trapezoidal side surface. The difference between the model shown in Fig. 3 and the model shown in Figs. 2 and 4 is that H = Hw in the cylindrical dimension.
(models shown in Figures 3 and 5) or H≒Hw (models shown in Figure 4). In the table, Examples Nos. 4 and 6 are A type shown in FIG. 3, Example Nos. 5 and 7 are C type shown in FIG. 5, and Examples Nos. 8 to 16 are H-Hw type. = 7mm, and rather than a B-type, it is a shape with a chamfered bottom of an A-type, and is classified as an A-type. Example No.
1, 2, 3 and Example Nos. 17 to 30 are type B shown in FIG. The model name is shown in the rightmost column of the table.
【表】【table】
以上説明したように、本発明は圧電振動子によ
つて励振される円筒状の超音波捻り共振子におい
て、円筒の長さに対する直径と肉厚の関係を、円
筒面に屈曲振動が寄生するごとく選んだことを特
徴とする構成にした。従つて超音波振動子は、同
筒捻り共振子の長さに対する直径と肉厚の条件を
変えることによつて共振子の種々の面、たとえば
側面,端面,内側面,内底面および外底面さらに
これらの面の接線上に様々なモードの楕円振動を
発生させることができるので、例えば超音波モー
タの振動子としては絶好の用途であり、従来無か
つた欠陥技術を補つたものとしての効果は大き
い。
As explained above, in a cylindrical ultrasonic torsional resonator excited by a piezoelectric vibrator, the present invention changes the relationship between the diameter and wall thickness with respect to the length of the cylinder so that bending vibration is parasitic on the cylindrical surface. The structure was designed to feature the selected features. Therefore, by changing the diameter and wall thickness conditions for the length of the cylindrical torsional resonator, the ultrasonic transducer can be adjusted to various surfaces of the resonator, such as side surfaces, end surfaces, inner surfaces, inner bottom surfaces, outer bottom surfaces, and the like. Since it is possible to generate various modes of elliptical vibration on the tangents of these surfaces, it is ideal for use as a vibrator for ultrasonic motors, for example, and is effective as a compensation for defective technology that did not exist in the past. big.
図はすべて本発明の実施例に係る超音波振動子
を説明するためのもので、第1図および第2図は
超音波振動子の一例を示す正面図および側面図、
第3図,第4図,第5図,第13図および第14
図は超音波振動子の他の例を示す説明図、第6
図,第7図,第8図,第9図,第10図,第11
図,第12図,第15図,第16図,第17図,
第18図,第19図,第20図,第21図は本発
明の各実施例に係る原理説明図である。
1,11,81……圧電厚み振動子、3,1
3,71,83,111,121,123,12
5,141……捻り共振子、5,15,85……
ボルト。
The figures are all for explaining the ultrasonic transducer according to the embodiment of the present invention, and FIGS. 1 and 2 are a front view and a side view showing an example of the ultrasonic transducer,
Figures 3, 4, 5, 13 and 14
The figure is an explanatory diagram showing another example of an ultrasonic transducer.
Figure, Figure 7, Figure 8, Figure 9, Figure 10, Figure 11
Figure, Figure 12, Figure 15, Figure 16, Figure 17,
FIG. 18, FIG. 19, FIG. 20, and FIG. 21 are diagrams explaining the principle of each embodiment of the present invention. 1, 11, 81...Piezoelectric thickness vibrator, 3, 1
3,71,83,111,121,123,12
5,141...Torsional resonator, 5,15,85...
bolt.
Claims (1)
波捻り共振子において、円筒の長さに対する直径
と肉厚の関係を、円筒面に屈曲振動が寄生するご
とく選んだことを特徴とする捻り・屈曲モード結
合型超音波振動子。 2 特許請求の範囲第1項記載の超音波振動子に
おいて、捻り共振子円筒の長さに対する直径と肉
厚の関係を、円筒面に屈曲進行波が発生するごと
く選んだことを特徴とする捻り・屈曲モード結合
型超音波振動子。 3 特許請求の範囲第1項記載の超音波振動子に
おいて、捻り共振子円筒の長さに対する直径と肉
厚の関係を、円筒面に円周に沿つて対称な屈曲定
在波が発生するごとく選んだことを特徴とする捻
り・屈曲モード結合型超音波振動子。 4 特許請求の範囲第1項記載の超音波振動子に
おいて、捻り共振子円筒の長さに対する直径と肉
厚の関係を、円筒の軸対称にある端面上の少なく
とも1対の個所において、軸に対して互いに逆ま
わりの楕円振動が発生するごとく選んだことを特
徴とする捻り・屈曲モード結合型超音波振動子。 5 特許請求の範囲第1項,第2項,第3項およ
び第4項のうちのいずれかの記載の超音波振動子
において、捻り結合子を用いることにより、振動
の励振効率を高めたことを特徴とする捻り・屈曲
モード結合型超音波振動子。[Claims] 1. In a cylindrical ultrasonic torsional resonator excited by a piezoelectric vibrator, the relationship between the diameter and wall thickness with respect to the length of the cylinder is selected so that bending vibration is parasitic on the cylindrical surface. An ultrasonic transducer that combines torsion and bending modes. 2. The ultrasonic transducer according to claim 1, characterized in that the relationship between the diameter and wall thickness of the torsion resonator cylinder relative to its length is selected so that a bending traveling wave is generated on the cylindrical surface.・Bending mode coupled ultrasonic transducer. 3. In the ultrasonic transducer described in claim 1, the relationship between the diameter and wall thickness of the torsional resonator cylinder relative to its length is such that a symmetrical bending standing wave is generated along the circumference on the cylindrical surface. A torsion/bending mode coupled ultrasonic transducer featuring selected features. 4. In the ultrasonic transducer according to claim 1, the relationship between the diameter and wall thickness of the torsional resonator cylinder with respect to its length is determined along the axis at at least one pair of locations on the axially symmetrical end face of the cylinder. A torsional/bending mode coupled ultrasonic transducer is selected such that elliptical vibrations with opposite directions are generated. 5. In the ultrasonic vibrator according to any one of claims 1, 2, 3, and 4, the vibration excitation efficiency is increased by using a torsion coupler. A torsional/bending mode coupled ultrasonic transducer featuring the following.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59173182A JPS6152168A (en) | 1984-08-22 | 1984-08-22 | Twist and bent mode coupling type supersonic vibrator |
| US06/688,947 US4663556A (en) | 1984-01-11 | 1985-01-04 | Torsional mode ultrasonic vibrator |
| DE3500607A DE3500607C2 (en) | 1984-01-11 | 1985-01-10 | Torsional vibration ultrasonic vibrator and torsional vibration piezo motor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59173182A JPS6152168A (en) | 1984-08-22 | 1984-08-22 | Twist and bent mode coupling type supersonic vibrator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6152168A JPS6152168A (en) | 1986-03-14 |
| JPH0479715B2 true JPH0479715B2 (en) | 1992-12-16 |
Family
ID=15955609
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59173182A Granted JPS6152168A (en) | 1984-01-11 | 1984-08-22 | Twist and bent mode coupling type supersonic vibrator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6152168A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP3132667B2 (en) * | 1991-03-05 | 2001-02-05 | アイシン精機株式会社 | Vibration motor |
-
1984
- 1984-08-22 JP JP59173182A patent/JPS6152168A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6152168A (en) | 1986-03-14 |
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