JPS61187627A - Method for measuring torque - Google Patents

Method for measuring torque

Info

Publication number
JPS61187627A
JPS61187627A JP2654285A JP2654285A JPS61187627A JP S61187627 A JPS61187627 A JP S61187627A JP 2654285 A JP2654285 A JP 2654285A JP 2654285 A JP2654285 A JP 2654285A JP S61187627 A JPS61187627 A JP S61187627A
Authority
JP
Japan
Prior art keywords
torque
light
angle
inclination
optical fiber
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
JP2654285A
Other languages
Japanese (ja)
Inventor
Shigeru Mori
茂 森
Tatsuhiko Shigemura
繁村 龍彦
Masaaki Hatano
波多野 雅昭
Yuuzou Kageyama
陰山 優造
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.)
Ryomei Engineering Co Ltd
Mitsubishi Heavy Industries Ltd
Original Assignee
Ryomei Engineering Co Ltd
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 Ryomei Engineering Co Ltd, Mitsubishi Heavy Industries Ltd filed Critical Ryomei Engineering Co Ltd
Priority to JP2654285A priority Critical patent/JPS61187627A/en
Publication of JPS61187627A publication Critical patent/JPS61187627A/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 enable the accurate measurement of torque, by automatically correcting a torque measuring error due to the change in the mount angle of a composite sensor by combining inclination angle measuring sensors. CONSTITUTION:In two circular rings 7, 8 with slits, the length of the slit part of the circular ring 8 in the radius direction is made longer than that of the other circular ring 7 and a pair of light emitting and receiving optical fibers 21, 22 are arranged to said part is inclination angle measuring sensors in the same way as existing light emitting and receiving optical fibers 11, 12. From the relation between a time permitting the transmission of light through the slits of the circular rings 7, 8 and a light blocking time, angle of inclination is operated by a torque operation apparatus 17. The operation result is displayed by one of display apparatus 18-20 to make it possible to know the angle of inclination of an optical axis at the measuring time of torque and the resetting to a normal state is also enabled. By this method, the effect of the angle of inclination contained in a light receiving time within one cycle of a cyclic pulse signal detected by the measuring sensor can be excluded and highly accurate measurement of torque is enabled.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、光軸(投光、受光用ファイバの組)とスリッ
ト付き円環との間の取付は角の変化を非接触で測定する
方法と、上記角度の測定結果を用いて、トルクの測定値
を補正する方法の技術分野で利用される。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention provides a method for non-contactly measuring changes in angle between an optical axis (a set of light emitting and light receiving fibers) and a slitted ring. , is used in the technical field of a method of correcting a torque measurement value using the above-mentioned angle measurement result.

従来の技術 第3図により従来のトルク測定装置を用いて、回転軸系
の駆動トルクを測定する方法について述べる。
BACKGROUND OF THE INVENTION A method of measuring the driving torque of a rotating shaft system using a conventional torque measuring device will be described with reference to FIG.

、lはトルク測定装置のうち回転軸上に装着される回転
部で、駆動装置2と負荷装置30間に駆動軸4を介して
接続されている。
, l is a rotating part of the torque measuring device mounted on the rotating shaft, and is connected between the driving device 2 and the load device 30 via the driving shaft 4.

回転部1の内部は、トルクを伝達するトーション軸6の
両端へ円周上に等ピッチのスリットを設けたスリット付
き円環7.8を取り付ける構造のものであるが、トルク
測定を容易とするため、一方のスリット付き円環8はト
ルクの作用しないチューブ10を介して、他方の円環に
近接設置しである。2つのスリット付き円環7.8の外
形寸法、スリット数、スリットピッチ等は等しく製作し
、組立時には双方のスリットを予め僅かにずらした状態
で取り付けてあり、トルクの作用によってトーション軸
6が捩れると、スリットのずれ量がトルクに比例して変
化するようになっている。上記2つのスリット付き円環
7,8のスリット部を挾み、対向するように投光゛月光
ファイバ11と受光用光ファイバ12が基礎等、移動し
ない場所から支持、固定されている。
The inside of the rotating part 1 has a structure in which a slitted ring 7.8 is attached to both ends of the torsion shaft 6 that transmits torque, with slits provided at equal pitches on the circumference, which facilitates torque measurement. Therefore, one of the slit rings 8 is installed close to the other ring via the tube 10 on which no torque is applied. The two slit rings 7.8 are manufactured with the same external dimensions, number of slits, slit pitch, etc., and when assembled, both slits are installed with a slight shift in advance, so that the torsion shaft 6 is not twisted by the action of torque. When the torque is applied, the amount of deviation of the slit changes in proportion to the torque. A light emitting optical fiber 11 and a light receiving optical fiber 12 are supported and fixed from a place where they do not move, such as a foundation, so as to face each other across the slit portions of the two slit rings 7 and 8.

13はトルク測定装置の演算部で、内部は高周波発振器
14、LED等で構成される発光装置15、フォトダイ
オード等で構成される光電変換装置(光信号を電気信号
へ変換する)16、並びにトルク演算装置17で構成さ
れており、トルク演算装置17の出力部には三つのディ
スプレイ装置18゜19.20が接続されている。
Reference numeral 13 denotes a calculation unit of the torque measuring device, which includes a high-frequency oscillator 14, a light emitting device 15 composed of an LED, etc., a photoelectric conversion device (converts an optical signal into an electrical signal) 16 composed of a photodiode, etc., and a torque measuring device. It is composed of a calculation device 17, and three display devices 18, 19, and 20 are connected to the output section of the torque calculation device 17.

発光装置15は、高周波発振器14の出力で変調された
高周波のパルスを発光し、その光を投光用光ファイバ1
1を介して受光用光ファイバ12へ向けて投光する。受
光用光ファイバ12で受光し、た光パルス信号は光電変
換装置16へ伝達され、電気パルス信号に変換されるが
、投光用光ファイバ11と受光用光フアイバ120光路
の中間にスリット付き円環7.8があるため、駆動軸4
0回転に伴って、光信号が周期的に断続されることとな
り、光電変換装置16の出力は高周波発振器14で発信
したと同一周波数の高周波信号が周期的に断続されたバ
ースト信号の列となる。
The light emitting device 15 emits high frequency pulses modulated by the output of the high frequency oscillator 14, and transmits the light to the light emitting optical fiber 1.
1 to a light-receiving optical fiber 12. The light pulse signal received by the light receiving optical fiber 12 is transmitted to the photoelectric conversion device 16 and converted into an electric pulse signal. Because of the ring 7.8, the drive shaft 4
With the zero rotation, the optical signal is periodically interrupted, and the output of the photoelectric conversion device 16 becomes a series of burst signals in which high-frequency signals of the same frequency as that transmitted by the high-frequency oscillator 14 are periodically interrupted. .

単位時間(例えば1秒間)の間にカウントされる高周波
信号の数をカウントすることによって、軸系に作用する
トルクT(kg、m)を演算し、トルクTと軸回転数N
の積上り駆動装置2の出力動力P(KW)を演算し、各
々の結果を三つのディスプレイ装置18.19.20に
表示する。
By counting the number of high-frequency signals counted during a unit time (for example, 1 second), the torque T (kg, m) acting on the shaft system is calculated, and the torque T and shaft rotation speed N are calculated.
The output power P (KW) of the accumulating drive device 2 is calculated, and each result is displayed on three display devices 18, 19, and 20.

第4図に投入用光ファイバ11,12をスリット円環の
スリット部をはさみ、対向設置した例を示す。図中、寸
法A(mm)は2枚のスリットの円周方向へのずれ量を
表わしている。
FIG. 4 shows an example in which input optical fibers 11 and 12 are placed opposite each other with the slit portion of the slit ring sandwiched therebetween. In the figure, dimension A (mm) represents the amount of deviation of the two slits in the circumferential direction.

光ファイバとスリットの間の幾何学的形状を理解し易く
するために、円周上に配列されたスリットを一軸上に展
開した図を第5図に示す。図中の符号r、p、ノ、t、
wは2枚のスリット付き円環7.8のスリット部の形状
、寸法(単位mm)を示す。投光、受光用光ファイバ1
2,12はスリット円環の側面に対して直角に取付けら
れており、スリットは周速V (m / sec )で
図の左方向へ移動するものとすると光ファイバ12で受
光される光信号は第6図のようになる。
In order to make it easier to understand the geometric shape between the optical fiber and the slit, FIG. 5 shows a diagram in which the slits arranged on the circumference are expanded on one axis. Symbols r, p, ノ, t in the figure,
w indicates the shape and dimensions (unit: mm) of the slit portions of the two slit rings 7.8. Optical fiber for transmitting and receiving light 1
2 and 12 are attached at right angles to the side surface of the slit ring, and assuming that the slit moves to the left in the figure at a circumferential velocity V (m/sec), the optical signal received by the optical fiber 12 is It will look like Figure 6.

第6図において、Tlは投光用光ファ・fバエ1からの
光を受光している時間(See )で、Toはスリット
によって周期的に断続される光パルス信号の一周期の時
間(Sec)を表わす。第5図の幾何学的形状を考慮し
てTo、T、を求めると、T o= p / V (s
ee )       (1)Tl= D −A)/V
 (see )    (2)となる。ここで、スリッ
トのずれ量l(m)は1回転軸に作用するトルクによっ
て、!+Δl(m)と変化し、T1もTI+ΔT、と変
化する。
In FIG. 6, Tl is the time (See) during which light is received from the light projecting optical fiber f-fly 1, and To is the time (Sec) of one cycle of the optical pulse signal periodically interrupted by the slit. ). When To and T are determined by considering the geometrical shape shown in Fig. 5, we obtain To=p/V(s
ee) (1) Tl=D-A)/V
(see) (2). Here, the amount of deviation l (m) of the slit is determined by the torque acting on the axis of one rotation! +Δl(m), and T1 also changes as TI+ΔT.

この時間の変化量ΔT工な先に述べた高周波信号の数を
カウントする方法によって測定し、トルクへ演算してい
る。
The amount of change in time ΔT is measured by the method of counting the number of high frequency signals mentioned above, and calculated into torque.

この方法は次のような欠点がある。This method has the following drawbacks.

いま、第5図において、投、受光用光ファイバ11.1
2で形成される光路がスリット面に対して角θ(rad
 )だけ傾いた場合、受光時間Tlは、TI = (r
 −l + w −tanθ)/V  (3)となり、
T1はトルクの作用によるlの変化Δノのみでなく、傾
き角θによっても変化することとなり1.トルク測定中
に光軸と回転軸とでなす角θが変わると、トルク測定誤
差となる。
Now, in FIG. 5, the optical fiber 11.1 for transmitting and receiving light
The optical path formed by 2 is at an angle θ (rad
), the light reception time Tl is TI = (r
−l + w −tanθ)/V (3),
T1 changes not only by the change Δ in l due to the action of torque, but also by the inclination angle θ.1. If the angle θ between the optical axis and the rotating axis changes during torque measurement, a torque measurement error will occur.

発明が解決しようとする問題点 本発明は、従来のトルク測定センサに、新規な角度測定
センサを組合せ、複合上ンサ(投入、受光用光ファイバ
の組と2枚のスリット円環)の取付角変化によるトルク
測定誤差を自動的に補正し、正確なトルク測定を可能と
することにある。
Problems to be Solved by the Invention The present invention combines a conventional torque measurement sensor with a new angle measurement sensor to improve the mounting angle of a composite upper sensor (a set of input and light receiving optical fibers and two slit rings). The object of this invention is to automatically correct torque measurement errors due to changes and enable accurate torque measurement.

問題点を解決するための手段 本発明は、上述の問題を解決するために、次ののような
手段を採っている。すなわち、2枚のスリット付き円環
の一方、あるいは回転軸へ同軸に別途取り付けられるス
リット付き円環を挾んで第2の投光用光ファイバと受光
用光ファイバとを対向配置し、該円環のスリットを光が
透過している時間と遮光されている時間との関係から上
記回転軸の傾きを求め、上記受光用光ファイバで求めら
れる透光量を補正してトルクを測定する。
Means for Solving the Problems The present invention employs the following means in order to solve the above-mentioned problems. That is, the second light-emitting optical fiber and the light-receiving optical fiber are arranged opposite to each other by sandwiching one of the two slit rings or a slit ring separately attached coaxially to the rotating shaft. The inclination of the rotation axis is determined from the relationship between the time during which the light is transmitted through the slit and the time during which the light is blocked, and the amount of light transmitted through the light receiving optical fiber is corrected to measure the torque.

作用 従来のトルク測定センサに新たに角度測定センナを組み
合わせ複合センサとしたことにより、センナ(投光・受
光用光ファイバの組と2枚のスリット円環)の取り付は
角変化をパルス波により演算するトルク演算装置により
、トルク測定時に回転軸の変形、移動によって発生する
光軸とスリット円環との傾きによるトルク測定誤差を補
正し、常に高精度なトルク測定を可能とする。
Function By combining a conventional torque measurement sensor with a new angle measurement sensor to create a composite sensor, the installation of the sensor (a set of optical fibers for transmitting and receiving light and two slit rings) detects angular changes using pulse waves. The torque calculation device that performs calculations corrects torque measurement errors due to the inclination between the optical axis and the slit ring caused by deformation and movement of the rotating shaft during torque measurement, and enables highly accurate torque measurement at all times.

実施例 次に、本発明の実施例につき、第1図および第2図を参
照して詳述する。
Embodiments Next, embodiments of the present invention will be described in detail with reference to FIGS. 1 and 2.

第1図に本発明のトルク測定方法を行う測定装置の系統
を示す。
FIG. 1 shows a system of measuring equipment for carrying out the torque measuring method of the present invention.

符号2−20は前記説明した従来例と同様であるが、2
枚のスリット付き円環7.8の内の一方のスリット付き
円環8のスリット部の半径方向の長さを他方よりも長く
し、その部分へ一対の投・受光用光ファイバ21.22
を傾き角測定用センサとして既存の投・受光用光ファイ
バ11,12と同様の方法で設置しである。4本の光フ
ァイバは相互の位置関係が測定中に変化しないような方
法で固定部に固定されているものとする。
Reference numeral 2-20 is the same as the conventional example described above;
The radial length of the slit portion of one of the slit rings 7.8 is made longer than the other, and a pair of light emitting/receiving optical fibers 21.22 are connected to that portion.
The optical fibers 11 and 12 are installed as inclination angle measurement sensors in the same manner as the existing optical fibers 11 and 12 for light emission and light reception. It is assumed that the four optical fibers are fixed to the fixed part in such a way that their mutual positional relationship does not change during measurement.

2本の投光用光ファイバ11.21は、発光装置15へ
接続されている。2本の受光用ファイバ12.22は各
々の光電変換装置16.26へ接続されており、その光
電変換装置16.26の出力はトルク演算装置17へ接
続されている。
The two light emitting optical fibers 11.21 are connected to the light emitting device 15. The two light receiving fibers 12.22 are connected to each photoelectric conversion device 16.26, and the output of the photoelectric conversion device 16.26 is connected to the torque calculation device 17.

従来と同じく駆動装置2より光電変換装置16によって
測定される光信号時間Tlは、光ファイバ11,12の
間で形成される光軸とスリット円環側面との角が90度
の場合には上記(2)式となり、傾きのある場合には(
3)式となる。
As in the conventional case, the optical signal time Tl measured by the photoelectric conversion device 16 from the drive device 2 is as described above when the angle between the optical axis formed between the optical fibers 11 and 12 and the side surface of the slit ring is 90 degrees. Equation (2) becomes, and if there is a slope, (
3) Equation becomes.

投・受光用光ファイバ21.22とスリット円環7の延
長されたスリット部分は上記傾き角変化を測定するため
のセンサで、投・受光用光ファイバ21.22で形成さ
れる光軸とスリット円環7の関係を第5図の場合と同様
な方法で示すと第2図のようになり、受光ファイバ22
で受光される光信号は第6図で示したと同様な周期的パ
ルス波となる。
The emitting/receiving optical fibers 21.22 and the extended slit portion of the slit ring 7 are sensors for measuring the above-mentioned tilt angle changes, and the optical axis formed by the emitting/receiving optical fibers 21.22 and the slit If the relationship of the ring 7 is shown in the same way as in FIG. 5, it will be as shown in FIG.
The optical signal received by the laser beam becomes a periodic pulse wave similar to that shown in FIG.

上記周期的パルス波の一周期の時間Toは(1)式と同
じであり、−周期のうち、光を受光している時間T1は
、取り付は角θ(rad )のある場合には、 T’=(r−乞X tanθ) /V (Sea ) 
 (4)となる。
The time To of one cycle of the above periodic pulse wave is the same as equation (1), and the time T1 during which light is being received during the period is, if the mounting has an angle θ (rad), T'=(r-Tanθ)/V (Sea)
(4) becomes.

上記(4)式では、トルクの作用による2枚のスリット
の相対ずれ量w(m)の影響を受けず、スリット円環の
幾何学的形状で定まる寸法(半径、厚さ、スリットピッ
チ)と回転軸を与えれば、時間測定値T’(Sea)よ
り、傾きθを逆算することが可能である。
Equation (4) above is not affected by the relative displacement w (m) of the two slits due to the action of torque, and the dimensions (radius, thickness, slit pitch) determined by the geometric shape of the slit ring. If the axis of rotation is given, it is possible to back-calculate the slope θ from the time measurement value T' (Sea).

すなわち、第1図におけるトルク演算装置17に上記演
算機能を持たされることにより、傾き角θを演算でき、
その結果をディスプレイ装置18.19.20のうち、
一つを利用して表示させることにより、トルク測定時に
おける光軸の傾き角を知ることができ、正規の状態(例
えば0(rad))に再セットも可能となる。これによ
り、トルク測定センサで検出される周期的パルス信号の
一周期のうちの受光時間T1((31式)中に含まれる
傾き角θの影響の項をキャンセルすることができ、高精
度なトルク測定を可能とする。
That is, by providing the torque calculation device 17 in FIG. 1 with the above calculation function, the inclination angle θ can be calculated.
The result is displayed on the device 18.19.20.
By displaying one of them, it is possible to know the inclination angle of the optical axis at the time of torque measurement, and it is also possible to reset it to the normal state (for example, 0 (rad)). As a result, it is possible to cancel the term of the influence of the inclination angle θ included in the light reception time T1 ((Equation 31)) in one cycle of the periodic pulse signal detected by the torque measurement sensor, and to obtain high-precision torque. Enables measurement.

あるいは、上記傾き角の演算結果θ(rad)を(3)
式のθに代入することにより、傾き角の影響を補正する
ことも可能(トルク演算装置17に演算機能を持たせて
おく)であり、センサ取りつけ角の再修正なしで高精度
なトルク測定が可能である。
Alternatively, the calculation result θ (rad) of the above tilt angle can be expressed as (3)
By substituting θ in the equation, it is also possible to correct the influence of the inclination angle (the torque calculation device 17 has a calculation function), allowing highly accurate torque measurement without re-correcting the sensor mounting angle. It is possible.

次に、補正の方法としては、(al傾き角の測定・演算
結果を用いて、光軸を正規の状態に動かす方法と、(b
l傾き角の測定・演算結果を用いて、トルク測定データ
をソフトウェア上で補正計算する方法とがある。
Next, as correction methods, there are two methods: (a method of moving the optical axis to the normal state using the measurement and calculation results of the al inclination angle, and a method of (b)
There is a method in which torque measurement data is corrected and calculated on software using the measurement and calculation results of the inclination angle.

発明の効果 トルク測定のための投・受光用光ファイバ11.12で
形成される光軸がスリット円環に対して互角でない時、
その傾き角θはトルク測定誤差要因となるが、本発明測
定方法により、常に正確なトルク測定が可能となる。
Effects of the invention When the optical axis formed by the optical fibers 11 and 12 for transmitting and receiving light for torque measurement is not equilateral to the slit ring,
Although the inclination angle θ becomes a cause of torque measurement error, the measuring method of the present invention allows accurate torque measurement at all times.

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

第1図、第2図は本発明に関し、第1図はトルク測定装
置の系統図、第2図は円周上に配列されたスリットを仮
に一軸上に示した展開図、第3図以降は従来例に係り、
第3図は従来のトルク測定装置を用いて駆動トルクを測
定する例の系統図、第4図は光ファイバを円環のスリッ
ト部をはさみ対向設置した例の概略図、第5図は円周上
に配列されたスリットを一軸上に仮に示した展開図、第
6図は受光用光ファイバで受光される光信号を示す簡略
図である。 2・・駆動装置、3・・負荷装置、4・・駆動軸、6@
・トーション軸、7.8−−ス゛リット付き円環、10
・・チューブ、11・・投光用光ファイバ、12・・受
光用光ファイバ、14・・高周波発振器、15・・発光
装置、16・・光電変換装置、17・中トルク演算装置
、18,19.20・・ディスプレイ装置、21・・投
入用光ファイバ、22・・受光用光ファイバ、26・・
光電変換装置。
Figures 1 and 2 relate to the present invention; Figure 1 is a system diagram of the torque measuring device, Figure 2 is a developed view showing slits arranged on the circumference on one axis, and Figures 3 and onwards are Regarding the conventional example,
Figure 3 is a system diagram of an example in which drive torque is measured using a conventional torque measuring device, Figure 4 is a schematic diagram of an example in which optical fibers are placed opposite each other across the slit of a ring, and Figure 5 is a circumference diagram. FIG. 6 is a developed view temporarily showing the slits arranged above on one axis, and is a simplified diagram showing the optical signal received by the light receiving optical fiber. 2...Drive device, 3...Load device, 4...Drive shaft, 6@
・Torsion shaft, 7.8--ring with slit, 10
...Tube, 11.. Optical fiber for light emission, 12.. Optical fiber for light reception, 14.. High frequency oscillator, 15.. Light emitting device, 16.. Photoelectric conversion device, 17. Medium torque calculation device, 18, 19. .20...Display device, 21...Optical fiber for input, 22...Optical fiber for light reception, 26...
Photoelectric conversion device.

Claims (1)

【特許請求の範囲】[Claims] 同心円上へ等間隔に設けられたスリットを有する2枚の
円環を回転軸の異なる2点へ同軸に取付け、同2枚のス
リット付き円環を挾んで対向配置された投光用光ファイ
バと受光用光ファイバとの間で上記スリットを介して光
の授受を行い、受光用光ファイバで求められる透光量か
ら回転軸に作用するトルクを測定する方法であつて、上
記スリット付き円環の一方、あるいは、上記回転軸へ同
軸に別途取り付けられるスリット付き円環を挾んで第2
の投光用光ファイバと受光用光ファイバとを対向配置し
、該円環のスリットを光が透過している時間と遮光され
ている時間との関係から上記回転軸の傾きを求め、上記
受光用光ファイバで求められる透光量を補正してトルク
を測定するトルク測定方法。
Two circular rings having slits provided at equal intervals on concentric circles are attached coaxially to two different points on the rotation axis, and optical fibers for light projection are placed facing each other with the same two circular rings with slits sandwiched between them. A method of exchanging light with a light-receiving optical fiber through the slit and measuring the torque acting on the rotating shaft from the amount of light transmitted through the light-receiving optical fiber, the method comprising: On the other hand, or alternatively, a second
A light emitting optical fiber and a light receiving optical fiber are arranged facing each other, and the inclination of the rotation axis is determined from the relationship between the time when the light is transmitted through the annular slit and the time when the light is blocked. A torque measurement method that measures torque by correcting the amount of light transmitted through the optical fiber.
JP2654285A 1985-02-15 1985-02-15 Method for measuring torque Pending JPS61187627A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2654285A JPS61187627A (en) 1985-02-15 1985-02-15 Method for measuring torque

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2654285A JPS61187627A (en) 1985-02-15 1985-02-15 Method for measuring torque

Publications (1)

Publication Number Publication Date
JPS61187627A true JPS61187627A (en) 1986-08-21

Family

ID=12196384

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2654285A Pending JPS61187627A (en) 1985-02-15 1985-02-15 Method for measuring torque

Country Status (1)

Country Link
JP (1) JPS61187627A (en)

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