JPH0251380A - Driving circuit for ultrasonic motor - Google Patents
Driving circuit for ultrasonic motorInfo
- Publication number
- JPH0251380A JPH0251380A JP63199464A JP19946488A JPH0251380A JP H0251380 A JPH0251380 A JP H0251380A JP 63199464 A JP63199464 A JP 63199464A JP 19946488 A JP19946488 A JP 19946488A JP H0251380 A JPH0251380 A JP H0251380A
- Authority
- JP
- Japan
- Prior art keywords
- feedback voltage
- ultrasonic motor
- electrode
- circuit
- cable
- 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.)
- Pending
Links
- 230000005284 excitation Effects 0.000 claims description 9
- 239000003990 capacitor Substances 0.000 abstract description 9
- 230000004048 modification Effects 0.000 abstract 1
- 238000012986 modification Methods 0.000 abstract 1
- 230000006641 stabilisation Effects 0.000 abstract 1
- 238000011105 stabilization Methods 0.000 abstract 1
- 230000000087 stabilizing effect Effects 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- XTKDAFGWCDAMPY-UHFFFAOYSA-N azaperone Chemical compound C1=CC(F)=CC=C1C(=O)CCCN1CCN(C=2N=CC=CC=2)CC1 XTKDAFGWCDAMPY-UHFFFAOYSA-N 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 229920002635 polyurethane Polymers 0.000 description 1
- 239000004814 polyurethane Substances 0.000 description 1
- 230000009291 secondary effect Effects 0.000 description 1
Landscapes
- General Electrical Machinery Utilizing Piezoelectricity, Electrostriction Or Magnetostriction (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は弾性体と電気−機械変換振動子からなるステー
タに生じさせた進行波により動体を摩擦駆動させる超音
波モータの駆動回路において、弾性体の振動周波数を最
適に制御する場合、弾性体の振動を検出した周波電圧信
号を安定に駆動電源回路に帰還するに適切なものに関す
るものである。Detailed Description of the Invention [Field of Industrial Application] The present invention provides a drive circuit for an ultrasonic motor that frictionally drives a moving body by a traveling wave generated in a stator consisting of an elastic body and an electro-mechanical transducer. In order to optimally control the vibration frequency of the body, the present invention relates to something suitable for stably feeding back a frequency voltage signal detected from vibration of an elastic body to a drive power supply circuit.
超音波モータにおいては入力する励振周波電圧の周波数
を、弾性体と電気−機械変換振動子とで構成されるステ
ータの共振周波数またはその極近傍周波数にしなければ
ステータは効率的に振動しない。In an ultrasonic motor, the stator does not vibrate efficiently unless the frequency of the input excitation frequency voltage is at or near the resonance frequency of the stator, which is composed of an elastic body and an electro-mechanical transducer.
この共振周波数および振動振幅は、一般に温度の変化や
負荷の大小など環境条件により、それぞれが同時あるい
は独立に変動するため、この共振点および振動振幅の変
動を検出して駆動回路に帰還し、その最適値に励振周波
数を制御する必要がある。The resonance frequency and vibration amplitude generally fluctuate simultaneously or independently depending on environmental conditions such as changes in temperature and the size of the load. Therefore, fluctuations in the resonance point and vibration amplitude are detected and fed back to the drive circuit. It is necessary to control the excitation frequency to an optimal value.
そこで、振動を検出する方法としては電気−機械変換振
動子の励振周波電圧が印加されていない部分から、励振
によって生ずる励起電圧を検出し、駆動回路源に帰還し
て利用している(以下、フィードバック電圧と言う)。Therefore, as a method of detecting vibration, the excitation voltage generated by excitation is detected from the part of the electro-mechanical transducer to which the excitation frequency voltage is not applied, and is used by returning it to the drive circuit source (hereinafter referred to as feedback voltage).
このフィードバック電圧は弾性体の励振周波数と同一の
周波数で通常数十キロヘルツの値である、また、ケーブ
ルは電磁波の漏洩を防ぐためにシールド線が用いらてい
る。This feedback voltage has the same frequency as the excitation frequency of the elastic body, and usually has a value of several tens of kilohertz, and the cable is shielded to prevent leakage of electromagnetic waves.
このため、モータ本体と駆動電源回路間のケーブルが長
くなると、その線間浮遊容量Cf2が大きくなり、モー
タ本体側から見た入力インピーダンスの容量成分
は小さくなり、フィードバック電圧はケーブル長さに反
比例して著しく減衰してしまう。Therefore, as the cable between the motor body and the drive power supply circuit becomes longer, the line-to-line stray capacitance Cf2 increases, the capacitance component of the input impedance seen from the motor body side becomes smaller, and the feedback voltage becomes inversely proportional to the cable length. This results in significant attenuation.
そのため、駆動電源回路のフィードバック電圧が入力さ
れる回路部分をケーブル長゛さに応じて調整したり、回
路定数を変更する煩わしさがある。Therefore, it is troublesome to adjust the circuit portion into which the feedback voltage of the drive power supply circuit is input according to the cable length or to change the circuit constants.
また、このことは汎用モータとしてのユーザ側にとって
、容易にケーブル長さを変更出来ないと言う欠点となっ
ている。Furthermore, this is a drawback for the user of the general-purpose motor in that the cable length cannot be easily changed.
本発明は前記問題点に鑑みなされたもので、−穀実用の
ケーブル長さlOメートル程度の範囲内であれば、駆動
電源回路を再調整することなく容易にケーブル長さを変
更出来るように成した超音波モータ駆動回路を提供する
ことにある。The present invention has been made in view of the above-mentioned problems, and it is possible to easily change the cable length without readjusting the drive power circuit, as long as the cable length is within the range of about 10 meters for practical use. An object of the present invention is to provide an ultrasonic motor drive circuit that provides an improved ultrasonic motor drive circuit.
図面は本発明の一実施例を示すものである。 The drawings show one embodiment of the invention.
−船釣な超音波モータの駆動回路は第1図に示すように
、フィードバック電圧は可変抵抗器VRIにより降圧さ
れ、ダイオードDで半波整流され、コンデンサC1で平
滑された直流電圧となってオペアンプOFへ入力される
。なお、可変抵抗器VR2はモータ速度設定ポリウムで
ある。- As shown in Figure 1, the drive circuit for an ultrasonic motor used for boat fishing is such that the feedback voltage is stepped down by a variable resistor VRI, half-wave rectified by a diode D, and smoothed by a capacitor C1 to become a DC voltage, which is then connected to an operational amplifier. Input to OF. Note that the variable resistor VR2 is a motor speed setting polyurethane.
フィードバック電圧が発生される振動子電極1より可変
抵抗器VR,までのケーブルは通常シールド線によりあ
る長さをもって接続される。The cable from the vibrator electrode 1, where the feedback voltage is generated, to the variable resistor VR is usually connected over a certain length by a shielded wire.
第2図は本願発明の回路構成を示したものであり、駆動
電源回路のフィードバック電圧入力部に安定化用のコン
デンサC1を接続しである。FIG. 2 shows the circuit configuration of the present invention, in which a stabilizing capacitor C1 is connected to the feedback voltage input section of the drive power supply circuit.
電極1の固有の静電容量をCrtとし、−穀実用的な最
大長さである約10メートルでのシールド線のもつ浮遊
容量をCf2とする。Let Crt be the specific capacitance of the electrode 1, and Cf2 be the stray capacitance of the shielded wire at a practical maximum length of approximately 10 meters.
ここで、フィードバック電圧安定化のために設けたコン
デンサC1の値を浮遊容量Cf2の少なくとも数倍から
10倍程度の値とすれば、電極lから見た合成容量は。Here, if the value of the capacitor C1 provided for stabilizing the feedback voltage is at least several times to ten times the value of the stray capacitance Cf2, the combined capacitance as seen from the electrode l is.
Cfft +Cf2 +C@ =Cf1+(2〜10)Cfz となる。Cfft +Cf2 +C@ =Cf1+(2~10)Cfz becomes.
一般的に、静電容量Crtは数百PF(ピコファラッド
)、浮遊容量Cf2は数百〜1千PF(ピコファラド)
程度であるから、例えば、ケーブル長さが最も多く用い
られる1メートル前後で駆動電源回路を調整したとして
も、その時のケーブル浮遊容量はCf2 /l Oに減
少するものの前記合成容量Cfft +Cf2 +CB
に代入すれば、例えば、コンデンサC1を浮遊容量cr
tの5倍にとった場合、
a ケーブル10メートル時容量
=Cf1+Cf2 +5C(2
=Cf 鵞 + 6Cf2
b ケーブル1メートル時容量
■
=Cf 1+5.1Cf2
となり、ケーブル長さ10倍の変化(1メ一トル→lO
メートル)に対しても合成容量の変化は約20%の変化
で済むことが分る。Generally, the capacitance Crt is several hundred PF (picofarad), and the stray capacitance Cf2 is several hundred to 1,000 PF (picofarad).
For example, even if the drive power circuit is adjusted to a cable length of around 1 meter, which is the most commonly used cable length, the cable stray capacitance at that time will decrease to Cf2 /l O, but the combined capacitance Cfft +Cf2 +CB
For example, if we substitute capacitor C1 into stray capacitance cr
When t is taken as 5 times, a Capacity at 10 meters of cable = Cf1 + Cf2 + 5C (2 = Cf + 6Cf2 b Capacity at 1 meter of cable ■ = Cf 1 + 5.1Cf2, and the change of cable length by 10 times (1 meter) Tor→lO
It can be seen that the change in the combined capacity is only about 20% even with respect to the distance (meters).
このように電極1か−ら見たケーブル長さ変更に伴なう
静電容量の変化は微少なもので済み、フィードバック電
圧の増減は著しく軽減でき。In this way, the change in capacitance caused by changing the cable length as seen from the electrode 1 is minimal, and the increase or decrease in feedback voltage can be significantly reduced.
回路に与える影響が少なくケーブルの長さが容易に変更
が可能となる。The cable length can be easily changed with little effect on the circuit.
なお、コンデンサC1の接続位置は駆動電源回路側で説
明をしたが、電極静電容量Off+側近部またはケーブ
ル浮遊容量Cf2側近部のいず°れでも電気的作用は全
く同一であることは言うまでもない。The connection position of capacitor C1 has been explained on the drive power supply circuit side, but it goes without saying that the electrical action is exactly the same whether it is near the electrode capacitance Off+ or near the cable stray capacitance Cf2. .
以上のように、本発明によれば、フィードバック用電極
lに静電容量を並列に接続することにより、実用範囲内
でのケーブル長さの変更が容易に出来ることが可能とな
った。As described above, according to the present invention, by connecting a capacitor in parallel to the feedback electrode 1, it is possible to easily change the cable length within a practical range.
また、電極lの固有の静電容量Crtはステータ温度に
より変化するから、本願発明によりその容量変化が圧縮
されて駆動電源回路に伝達されることになり、フィード
バック電圧はステータ温度変化に対しても安定であると
言う副次的効果をも併せ有する。Further, since the specific capacitance Crt of the electrode l changes depending on the stator temperature, the present invention compresses the capacitance change and transmits it to the drive power supply circuit, so that the feedback voltage can be adjusted against the stator temperature change. It also has the secondary effect of being stable.
図面は本発明の一実施例を示すもので、第1図は一般的
に用いられる超音波モータの駆動回路および第2図は本
願発明であるフィードバック電圧の入力部を示した超音
波モータの駆動回路である。
11口
1−−−−一電極
C、−−−−一安定化用コンデンサThe drawings show one embodiment of the present invention, and FIG. 1 shows a commonly used ultrasonic motor drive circuit, and FIG. 2 shows an ultrasonic motor drive circuit showing a feedback voltage input section according to the present invention. It is a circuit. 11 ports 1------One electrode C,---One stabilizing capacitor
Claims (1)
させた進行波により動体を摩擦駆動させる超音波モータ
の電気−機械変換振動子の励振周波電圧が印加されてい
ない電極から、励振によって生ずる励起電圧を駆動回路
源に帰還する際、該電極に静電容量を並列に接続される
よう回路構成したことを特徴とする超音波モータ駆動回
路。Excitation generated by excitation from an electrode to which no excitation frequency voltage is applied to the electro-mechanical transducer of an ultrasonic motor that frictionally drives a moving body by a traveling wave generated in a stator consisting of an elastic body and an electro-mechanical transducer. An ultrasonic motor drive circuit characterized in that the circuit is configured such that a capacitance is connected in parallel to the electrode when a voltage is fed back to the drive circuit source.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63199464A JPH0251380A (en) | 1988-08-10 | 1988-08-10 | Driving circuit for ultrasonic motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63199464A JPH0251380A (en) | 1988-08-10 | 1988-08-10 | Driving circuit for ultrasonic motor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0251380A true JPH0251380A (en) | 1990-02-21 |
Family
ID=16408240
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63199464A Pending JPH0251380A (en) | 1988-08-10 | 1988-08-10 | Driving circuit for ultrasonic motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0251380A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0397391U (en) * | 1990-01-22 | 1991-10-07 | ||
JPH03101190U (en) * | 1990-01-30 | 1991-10-22 | ||
JPH04131189U (en) * | 1991-05-17 | 1992-12-02 | 五洋電子工業株式会社 | Ultrasonic motor drive power supply device |
-
1988
- 1988-08-10 JP JP63199464A patent/JPH0251380A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0397391U (en) * | 1990-01-22 | 1991-10-07 | ||
JPH03101190U (en) * | 1990-01-30 | 1991-10-22 | ||
JPH04131189U (en) * | 1991-05-17 | 1992-12-02 | 五洋電子工業株式会社 | Ultrasonic motor drive power supply device |
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