JPS61207940A - Measuring method for torque - Google Patents

Measuring method for torque

Info

Publication number
JPS61207940A
JPS61207940A JP4857885A JP4857885A JPS61207940A JP S61207940 A JPS61207940 A JP S61207940A JP 4857885 A JP4857885 A JP 4857885A JP 4857885 A JP4857885 A JP 4857885A JP S61207940 A JPS61207940 A JP S61207940A
Authority
JP
Japan
Prior art keywords
light
slit
torque
receiving element
pulse
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
Application number
JP4857885A
Other languages
Japanese (ja)
Inventor
Shigeru Mori
茂 森
Masaaki Hatano
波多野 雅昭
Kazuo Iida
和男 飯田
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.)
Mitsubishi Heavy Industries Ltd
Original Assignee
Mitsubishi Heavy Industries 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 Mitsubishi Heavy Industries Ltd filed Critical Mitsubishi Heavy Industries Ltd
Priority to JP4857885A priority Critical patent/JPS61207940A/en
Publication of JPS61207940A publication Critical patent/JPS61207940A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L3/00Measuring torque, work, mechanical power, or mechanical efficiency, in general
    • G01L3/02Rotary-transmission dynamometers
    • G01L3/04Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft
    • G01L3/10Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft involving electric or magnetic means for indicating
    • G01L3/12Rotary-transmission dynamometers wherein the torque-transmitting element comprises a torsionally-flexible shaft involving electric or magnetic means for indicating involving photoelectric means

Abstract

PURPOSE:To measure torque working on a revolving shaft by a device of a low cost, and also with a high accuracy, by receiving light which has transmitted through a superposed part of a slit, counting a high frequency electric pulse transmitted from a pulse transmitter, and calculating the torque. CONSTITUTION:A driving shaft 1 and a shaft to be driven 2 are connected by a torsion bar 3, a slit is cut at every interval in a slit disk 4 and 5, and an optical fiber 6 and 7 are opposed and placed by placing the slit between them. A continuous light emitted from a light source 8 is irradiated toward the slit disk 5 from the end face of the optical fiber 6. The optical fiber 7 receives a light transmitting through a gap being proportional to a magnitude of a shift quantity of the slit caused by a superposed state of the slits of the slit disk 5 and 6, namely, a magnitude of a torque applied to a torsion bar 1, and propagates it to a light-receiving element 9. The light-receiving element 9 generates a rectangular pulse by the received light, and by taking AND with a pulse signal from a pulse transmitter 10, the number of pulses being proportional to a gap is obtained, and the torque is derived.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は1回転軸系に働いているトルクを測定する装置
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a device for measuring torque acting on a single rotation shaft system.

[従来の技術〕 回転軸に作用しているトルクを計測するものとして、従
来歯環と電磁ピックアップを用いるものが多用されてい
る。これは歯環の製作精度を要求され、また、歯環と電
磁ピックアップとの取りつけ位置を正確に決める必要が
あり、使いかっても悪いものであった。
[Prior Art] Conventionally, a gear ring and an electromagnetic pickup are often used to measure the torque acting on a rotating shaft. This required precision in manufacturing the tooth ring, and also required accurate determination of the mounting position of the tooth ring and the electromagnetic pickup, making it difficult to use even after repeated use.

そこで、光学的にトルクを計るものとしてトーションバ
ーの変形容易部を挟む両側に2枚のスリット円板を固定
し、スリット円板に光を照射する光源と、上記2枚のス
リット円板のスリットを透過した光を受光する受光素子
とを備えたものが提供されている。
Therefore, two slit disks are fixed on both sides of the easily deformable part of the torsion bar as a device to optically measure the torque, and a light source that irradiates the slit disks with light and a slit between the two slit disks are installed. A light-receiving element that receives light transmitted through the light receiving element is provided.

すなわち、トーションバーの捩れ量に応じて2枚のスリ
ット円板のスリットの重なり量が変化することを利用す
るもので、受光素子で受光される光の量の変化量を計測
しトルクを求めるものである。
In other words, it utilizes the fact that the amount of overlap between the slits in two slit disks changes depending on the amount of twist of the torsion bar, and calculates the torque by measuring the amount of change in the amount of light received by the light receiving element. It is.

上記光の量の変化を求めるものとして二通りの方法が提
供されている。
Two methods are provided for determining the change in the amount of light.

羊の一つは、光量そのものを計る方法で2例えば、特開
昭59−111029号公報に記載されたものがある。
One method for sheep is to measure the amount of light itself.For example, there is a method described in Japanese Patent Laid-Open No. 111029/1983.

これは、光の強度に応じた電圧を発生する光電変換器に
より、電圧から光量、つまり、スリットの重なり具合を
求めてトルクを計るものである。
This uses a photoelectric converter that generates a voltage according to the intensity of light to determine the amount of light from the voltage, that is, the degree to which the slits overlap, and then measure the torque.

また他の方法は、光が透過する時間を計るもので1例え
ば、実開昭58−163840号公報に記載されたよう
なものである。これは、光源に高周波パルス光源を用い
、スリットの間隙を透過するパルスの数を数え、スリッ
トの重なり度合を計るものである。
Another method is to measure the time during which light passes, such as the one described in Japanese Utility Model Application No. 58-163840. This uses a high-frequency pulsed light source as a light source, counts the number of pulses that pass through the gap between the slits, and measures the degree of overlap of the slits.

[発明が解決しようとする問題点〕 上記第1の方法は、トルクレンチ等のトルクを計測する
場合に通しているが1回転軸のトルクを計測する時には
、軸の回転数を求める別途の装置が必要となる。また、
軸の回転数が高くなるとスリットを透過する光の量は少
なくなり、精度を十分保つことができなくなる。
[Problems to be Solved by the Invention] The first method described above is used to measure the torque of a torque wrench, etc., but when measuring the torque of a single rotation shaft, a separate device is required to determine the rotation speed of the shaft. Is required. Also,
As the rotation speed of the shaft increases, the amount of light that passes through the slit decreases, making it impossible to maintain sufficient accuracy.

一方、第2の方法では1回転軸の回転数を求める必要は
ないが、トルクの計測精度を上げようとすると高周波パ
ルス光源の周波数を高くしなければならないが。しかし
、現在の市販の光源では極めて高価なものであり、かつ
、その周波数もトルク計測に十分なものが得ることはで
きない。
On the other hand, in the second method, it is not necessary to determine the number of rotations of one rotating shaft, but if the accuracy of torque measurement is to be improved, the frequency of the high-frequency pulse light source must be increased. However, current commercially available light sources are extremely expensive, and their frequencies are not sufficient for torque measurement.

[問題点を解決するための手段〕 本発明は、上記問題点を解決するための方法で。[Means for solving problems] The present invention is a method for solving the above problems.

捩れ変形が生じやすい変形容易部を備えたトーションバ
ー挟む両側にそれぞれスリット円板を固定し、同2枚の
スリット円板に向けてトーションバーと平行な連続光を
照射すると共にスリットの重ね合わせ部を透過した光を
受光素子で受光し、パルス発信器から発信される高周波
電気パルスを上記受光素子の出力で開閉してパルス数を
カウントし、このカウント数からトーションバーの両端
に作用するトルクを計測するようにした。
A slit disk is fixed on each side of the torsion bar, which has an easily deformable part where twisting deformation easily occurs, and a continuous light parallel to the torsion bar is irradiated to the two slit disks, and the overlapping part of the slits is The light that passes through is received by a light receiving element, and the high frequency electric pulse transmitted from the pulse transmitter is opened and closed by the output of the above light receiving element to count the number of pulses, and from this counted number, the torque acting on both ends of the torsion bar is calculated. I tried to measure it.

〔作用〕[Effect]

本発明の方法でも、上記従来の方法と同様に。 The method of the present invention is similar to the conventional method described above.

2枚のスリット円板のスリットの重なり具合が。The degree to which the slits of the two slit disks overlap.

トルクにより変化することを利用している。また。It takes advantage of the fact that it changes depending on the torque. Also.

そのスリットを光が透過する時間を計測する点でも、第
2の方法と同一である。
This method is also the same as the second method in that the time taken for light to pass through the slit is measured.

しかし、その時間の計測に高周波電気パルスを用い、ス
リットを透過する光で作動する受光素子で該高周波電気
パルスを開閉するようにした。つまり、アンド回路など
により、受光素子が光を受光したときに電気パルスを数
え始め、受光を終わった時にパルスのカウントを止める
ようにした。
However, high-frequency electric pulses were used to measure the time, and the high-frequency electric pulses were opened and closed by a light-receiving element operated by light transmitted through the slit. In other words, an AND circuit or the like is used to start counting electrical pulses when the light-receiving element receives light, and to stop counting the pulses when it finishes receiving light.

そして、カウンタ等によりそのカウントされたパルス数
と、受光素子が光を受ける時間間隔、つまり、トーショ
ンバーの回転数に比例する値を得て。
Then, a value proportional to the number of pulses counted by a counter or the like and the time interval at which the light-receiving element receives light, that is, the rotational speed of the torsion bar, is obtained.

トルクを計算する。Calculate torque.

[実施例] 以下1本発明を第1図ないし第3図に示す具現化した装
置について説明する。
[Example] Hereinafter, a device embodying the present invention as shown in FIGS. 1 to 3 will be described.

第1図において、1が駆動軸、2が該駆動軸1により回
転させられる被駆動軸で2両者はトーションバー3によ
り連結されている。4と5はスリット円板で、上記トー
ションバー3の両端に夫々固定されている。このスリッ
ト円板4と5には。
In FIG. 1, 1 is a drive shaft, 2 is a driven shaft rotated by the drive shaft 1, and both are connected by a torsion bar 3. 4 and 5 are slit disks fixed to both ends of the torsion bar 3, respectively. In these slit disks 4 and 5.

等間隔ごとにスリットが切られていて、光ファイバ6と
7が、スリットを挟み対向して配置されている。(第2
図に詳細を拡大しである)第3図において8は光源で、
上記光ファイバ6に連続光を導入するもの、9は受光素
子で上記光ファイバ7で伝播された光を電気信号に変換
するものである。
Slits are cut at equal intervals, and optical fibers 6 and 7 are placed facing each other with the slits in between. (Second
(Details are enlarged in the figure) In Figure 3, 8 is a light source,
A light receiving element 9 introduces continuous light into the optical fiber 6, and a light receiving element 9 converts the light propagated through the optical fiber 7 into an electrical signal.

lOは高周波パルス発信器、 11はカウンタで、上記
受光素子9の立ち上がり信号でパルス発信器10のパル
スをカウントしはじめ、立ち下がりでカウントの停止と
データホールドの動作を繰り換えずものである。
10 is a high frequency pulse oscillator, and 11 is a counter which starts counting pulses from the pulse oscillator 10 at the rising edge of the light receiving element 9, and repeats the operation of stopping the count and holding data at the falling edge.

12はトルク演算器で、上記カウンタ11の出力と。12 is a torque calculator, which outputs the output of the counter 11;

受光素子9の出力を受け、トルクを演算するもので、従
来方法におけるものと同一の回路により構成される。
It receives the output of the light receiving element 9 and calculates the torque, and is constructed of the same circuit as that used in the conventional method.

さて、光源8からでる連続光は、光ファイバ6により伝
播され、その端面からスリット円板5に向けて照射され
る。光ファイバ7では、スリット円板5と6のスリット
の重なり具合、つまりトーションバー1に掛かるトルク
の大きさによるスリットのずれ量の大きさに比例した隙
間を透る光を受け、受光素子9に伝播する。
Now, the continuous light emitted from the light source 8 is propagated by the optical fiber 6, and is irradiated toward the slit disk 5 from its end face. The optical fiber 7 receives light passing through a gap proportional to the degree of overlapping of the slits in the slit discs 5 and 6, that is, the amount of deviation of the slits due to the amount of torque applied to the torsion bar 1, and the light is transmitted to the light receiving element 9. propagate.

受光素子9は、光ファイバ7を介して受けた光により、
第4図イに示すような矩形のパルスを発生する。第4図
口においてTIが光を受けたときの出力、TOが次の光
を受けるまでの周期を示している。パルス発信器10か
らはパルス信号が出されていて、上記受光素子9とのア
ンドをとることにより、つまり、受光素子9の立ち上が
りでカンウドを開始し、立ち下がりでカウントを終了さ
せることにより上記T1に比例したパルス数が得られ、
逆に1時間T1からトルクが求められる。
The light receiving element 9 receives light via the optical fiber 7,
A rectangular pulse as shown in FIG. 4A is generated. Figure 4 shows the output when TI receives light at the mouth and the cycle until TO receives the next light. A pulse signal is output from the pulse transmitter 10, and by ANDing it with the light receiving element 9, that is, counting starts at the rising edge of the light receiving element 9 and ends at the falling edge, thereby achieving the above T1. The number of pulses proportional to is obtained,
Conversely, the torque is determined from 1 hour T1.

第5図には1周期Toを求めるための一つの回路が提案
されている。第3図と変わるところは、フリップフロッ
プ回路等で構成される分周装置13と。
In FIG. 5, one circuit for determining one period To is proposed. The difference from FIG. 3 is that the frequency divider 13 is composed of a flip-flop circuit or the like.

クロック発信装置14と、パルスカウンタ15を有する
ことである。上記フリップフロップ回路で構成される分
周装置13は、受光素子9の出力パルスをA分周し1周
期2TOの矩形パルス信号(デユーティ比50%)を出
力する。その出力信号は上記トルク算器12へ入力され
ると共に、上記パルスカウンタ15のゲート端子15G
にも接続されており。
It has a clock transmitting device 14 and a pulse counter 15. The frequency divider 13 constituted by the flip-flop circuit divides the output pulse of the light receiving element 9 by A and outputs a rectangular pulse signal (duty ratio 50%) with one cycle of 2TO. The output signal is input to the torque calculator 12 and is also input to the gate terminal 15G of the pulse counter 15.
is also connected to.

そのゲートを開閉する。パルスカウンタ15のデータ入
力端子15Dには、クロック発信装置14(発信周波数
は、上記高周波パルス発信器10の発信周波数程に高周
波である必要はない。)の発信出力信号が接続されてお
り、上記分周装置13の立ち上がりでカウントを開始し
、立ち下がりでカウント停止とデータホールドを行う。
Open and close that gate. The data input terminal 15D of the pulse counter 15 is connected to the oscillation output signal of the clock oscillator 14 (the oscillation frequency does not have to be as high as the oscillation frequency of the high-frequency pulse oscillator 10). Counting starts when the frequency divider 13 rises, and stops counting and holds data when the frequency divider 13 falls.

トルク演算器12は3分周装置13の立ち下がりを検知
してカウンタ15の出力データを読み取り、受光パルス
信号(第4図イ)の−周期の時間Toを計算する。
The torque calculator 12 detects the fall of the frequency divider 13, reads the output data of the counter 15, and calculates the -period time To of the light reception pulse signal (FIG. 4A).

なお9時間TOはクロック発信装置14の発信周波数を
f  (llz)カウンタ15のカウントデータをmと
すると。
Note that for 9 hours TO, the oscillation frequency of the clock generator 14 is f (llz), and the count data of the counter 15 is m.

TO=m/ f   (sec ) にて計算される。TO=m/f (sec) Calculated at

〔効果〕〔effect〕

本発明の方法によれば9回転軸に作用するとトルクを低
価格の装置でもって、しかも、精度よく計測できるよう
になる。
According to the method of the present invention, it is possible to measure torque acting on nine rotating axes with a low-cost device and with high accuracy.

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

第1図は本発明の方法を具現化するための装置の例示図
、第2図はその要部拡大図、第3図は処理回路のブロッ
ク図、第4図は信号の例示図、第5図は他の実施例の処
理回路ブロック図である。 3・・トーションバー、4:5・・スリット円板、6:
7・・光ファイバ、8・・光源。 9・・受光素子、10・・高周波パルス発信器。 11・・カウンタ、12・・トルク演算器。 第1に
FIG. 1 is an illustrative diagram of an apparatus for embodying the method of the present invention, FIG. 2 is an enlarged view of its main parts, FIG. 3 is a block diagram of a processing circuit, FIG. 4 is an exemplary diagram of signals, and FIG. The figure is a processing circuit block diagram of another embodiment. 3... Torsion bar, 4: 5... Slit disk, 6:
7. Optical fiber, 8. Light source. 9... Light receiving element, 10... High frequency pulse transmitter. 11...Counter, 12...Torque calculator. Firstly

Claims (1)

【特許請求の範囲】[Claims] 捩れ変形が生じやすい変形容易部を備えたトーションバ
ー挟む両側にそれぞれスリット円板を固定し、同2枚の
スリット円板に向けてトーションバーと平行な連続光を
照射すると共にスリットの重ね合わせ部を透過した光を
受光素子で受光し、パルス発信器から発信される高周波
電気パルスを上記受光素子の出力で開閉してパルス数を
カウントし、このカウント数からトーションバーの両端
に作用するトクルを計測することを特徴とするトルク測
定装置。
A slit disk is fixed on each side of the torsion bar, which has an easily deformable part where twisting deformation easily occurs, and a continuous light parallel to the torsion bar is irradiated to the two slit disks, and the overlapping part of the slits is The light that passes through is received by a light receiving element, and the high frequency electric pulse transmitted from the pulse transmitter is opened and closed by the output of the above light receiving element to count the number of pulses, and from this counted number, the torque acting on both ends of the torsion bar is calculated. A torque measuring device characterized by measuring torque.
JP4857885A 1985-03-12 1985-03-12 Measuring method for torque Pending JPS61207940A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4857885A JPS61207940A (en) 1985-03-12 1985-03-12 Measuring method for torque

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4857885A JPS61207940A (en) 1985-03-12 1985-03-12 Measuring method for torque

Publications (1)

Publication Number Publication Date
JPS61207940A true JPS61207940A (en) 1986-09-16

Family

ID=12807281

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4857885A Pending JPS61207940A (en) 1985-03-12 1985-03-12 Measuring method for torque

Country Status (1)

Country Link
JP (1) JPS61207940A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02504378A (en) * 1988-03-14 1990-12-13 ヤマハ・モーター・ヨーロッパ・エヌ・フィー motor auxiliary pedal bicycle
JPH0419392A (en) * 1990-05-10 1992-01-23 Kubota Corp Method for detecting operation condition of pump and method for supplying lubricating water to bearing of pump
EP0556734A2 (en) * 1992-02-18 1993-08-25 Asea Brown Boveri Ab Mechanical coupling for torque transducer

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02504378A (en) * 1988-03-14 1990-12-13 ヤマハ・モーター・ヨーロッパ・エヌ・フィー motor auxiliary pedal bicycle
JPH0419392A (en) * 1990-05-10 1992-01-23 Kubota Corp Method for detecting operation condition of pump and method for supplying lubricating water to bearing of pump
EP0556734A2 (en) * 1992-02-18 1993-08-25 Asea Brown Boveri Ab Mechanical coupling for torque transducer

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