JPS58123160A - Optical function generator - Google Patents

Optical function generator

Info

Publication number
JPS58123160A
JPS58123160A JP537682A JP537682A JPS58123160A JP S58123160 A JPS58123160 A JP S58123160A JP 537682 A JP537682 A JP 537682A JP 537682 A JP537682 A JP 537682A JP S58123160 A JPS58123160 A JP S58123160A
Authority
JP
Japan
Prior art keywords
elements
pattern
light
change
function generator
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.)
Granted
Application number
JP537682A
Other languages
Japanese (ja)
Other versions
JPS6155146B2 (en
Inventor
Yonezo Kubota
米蔵 久保田
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.)
Tamagawa Seiki Co Ltd
Original Assignee
Tamagawa Seiki Co 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 Tamagawa Seiki Co Ltd filed Critical Tamagawa Seiki Co Ltd
Priority to JP537682A priority Critical patent/JPS58123160A/en
Publication of JPS58123160A publication Critical patent/JPS58123160A/en
Publication of JPS6155146B2 publication Critical patent/JPS6155146B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06GANALOGUE COMPUTERS
    • G06G7/00Devices in which the computing operation is performed by varying electric or magnetic quantities
    • G06G7/12Arrangements for performing computing operations, e.g. operational amplifiers
    • G06G7/22Arrangements for performing computing operations, e.g. operational amplifiers for evaluating trigonometric functions; for conversion of co-ordinates; for computations involving vector quantities

Landscapes

  • Physics & Mathematics (AREA)
  • Mathematical Physics (AREA)
  • Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Algebra (AREA)
  • Mathematical Analysis (AREA)
  • Mathematical Optimization (AREA)
  • Pure & Applied Mathematics (AREA)
  • Software Systems (AREA)
  • Computer Hardware Design (AREA)
  • Optical Transform (AREA)

Abstract

PURPOSE:To obtain a desired function signal, by applying an electric signal corresponding to a change of form of a pattern to an electronic circuit including a differential amplifier. CONSTITUTION:The light emitting elements 3a-3b' having 180 deg. intervals in terms of an electric angle are connected in series. At the same time, the photodetecting elements 4a-4b' corresponding to the elements 3a-3b' are connected to both minus and plus input terminals of operational amplifiers 5 and 6 of differential amplification type respectively. In addition, the variable resistors R1-R4 are provided in parallel for photodetecting control of the elements 4a- 4b. As a result, a change of form of a pattern can be converted into electric signals having phases different by 90 deg. from each other and in terms of an electric angle. Then an optional function can be decomposed to a sine wave by the Fourier decomposition to ensure an application as an optical function generator.

Description

【発明の詳細な説明】 本発明は光学式関数発生器に係る。[Detailed description of the invention] The present invention relates to an optical function generator.

今ガラス板の回転円板lを第1図aのように示すが周縁
にそって正弦波状を有する透明のバター7/aを貼付し
て備えている。尚波形の1周期な電気角で3600であ
られすと、矢印のよ5に参等分してoo、デ0°、1t
o0.コク0°。
A rotating glass plate l is shown in FIG. 1a, and is provided with a transparent butter 7/a having a sinusoidal shape pasted along its periphery. If the electrical angle for one period of the waveform is 3600, divide it into 5 equal parts as shown by the arrow, oo, de 0°, 1t.
o0. Body 0°.

340”かえられる。この角度は機械角と一致しないこ
とは勿論で 機械角n1eJ40’ 電気角 −舅J4Q’ 円板の外径Hmr+acase である。又第1図すのように固定円板−には第1図aに
相当する。0.too、izoo、コク0°の位曹にス
リットコa、コb、コa’、Jb’を設ける。
340". This angle is of course not the same as the mechanical angle, and is mechanical angle n1eJ40' electrical angle - 辅J4Q' outer diameter of the disk Hmr + acase. Also, as shown in Figure 1, the fixed disk - This corresponds to Fig. 1 a.Slits a, b, a', and Jb' are provided at the 0° position of 0.too, izoo, and depth.

次に第1図Cに示すように回転円板lと固定円板−を軸
心が一致し、又スリットコa、コb、コaI。
Next, as shown in FIG. 1C, the axes of the rotating disk l and the fixed disk coincide, and the slit cores a, b, and aI are made.

コb′の外端と回転円板Iの外周面が一致するようにし
て間隔をおい【並設し発光素子J a e J b e
Ja’、Jb’と受光素子1a、 lb、参m’、lb
’(図ではJ龜とlaのみ示している)でこれら回転円
板Iと固定円板−とをはさんで配置する。
The outer edge of the rotary disk I is aligned with the outer circumferential surface of the rotating disk I with an interval [Light-emitting elements J a e J b e
Ja', Jb' and light receiving elements 1a, lb, reference m', lb
(Only J and la are shown in the figure) These rotating disks I and fixed disks are placed in between.

このようにして、回転円板Iを回転すれば発光素子Ja
、 Jb、 Ja’、Jb’  よりの光がパターン/
aの透明部、固定円板−のスリントコ8.コb。
In this way, by rotating the rotating disk I, the light emitting element Ja
The light from Jb, Ja', Jb' forms a pattern/
Transparent part of a, fixed disk - slintco8. Cob.

コa’、Jb’をへて受光素子4!a、 参す、亭a’
 、lb’には下記の出力電圧かえられる。
Light receiving element 4 through core a' and Jb'! a, visit a'
, lb' can be changed to the following output voltages.

VIIa =acos#−1−A@@11  (1)V
eb =β5iIe + B    @ @ e  (
2)V+a’=−α’CQS#+A’   @*@  
(31vIlb’ =  −β’siI j  十 B
’        Φ ・ ・  (4)次に電気角に
して/lO°間隔をおいた発光素子Jaと3 a/、J
bとJb′とを直列接続せる本発明の一実施例電子回路
結線図を第一図に示すがこの場合発光素子3aとJa 
/、3bとJb′に応じた受光素子ダaとla’、4I
bと41b′を夫々差動増巾型演算増巾器つまり差動増
巾器!、4の一1十の内入力端子に接続する。又各受光
素子l a 、 la’ 、 lb、 41b’の受光
調整用として並列に可変抵抗R/ + Rx* R3*
 R41を挿入する。かくて可変抵抗R,,R,,R,
,R4Iを調整することによりα=β=α′=β′、A
−B =A”” B’  とすることができる。このと
き V<la =αoas#十Aass  (5)Vub 
=α5iIe 十A    −@ @  f61VII
a’=−α(6)θ+A    、、−(7)v*b’
=−αsin # + A         ・・・ 
(8)次に差動増巾器5.6でVfaとV41a’%V
やbとv41b′  の差動増巾を行う結果、MA −
V4ca  V4I&’ −J k αCoSe   
 (91vBz vvb −Vlb’ = J kal
=s    αs尚には差動増巾器j、Aの利得とする
VIIa = acos#-1-A@@11 (1)V
eb = β5iIe + B @ @ e (
2) V+a'=-α'CQS#+A' @*@
(31vIlb' = -β'siI j ten B
'Φ ・ ・ (4) Next, the light emitting elements Ja and 3 a/, J are separated by /lO° in electrical angle.
Fig. 1 shows an electronic circuit wiring diagram of an embodiment of the present invention in which the light emitting elements 3a and Jb' are connected in series.
/, 3b and Jb', the light receiving elements a and la', 4I
b and 41b' are respectively differential amplifier type operational amplifiers, that is, differential amplifiers! , 4 to 11 of the input terminals. In addition, variable resistors R/ + Rx* R3* are installed in parallel for adjusting the light reception of each light receiving element la, la', lb, and 41b'.
Insert R41. Thus, the variable resistances R,,R,,R,
, R4I, α=β=α′=β′, A
-B=A""B'. In this case, V<la = αoas#10Aass (5) Vub
=α5iIe 10A −@@f61VII
a'=-α(6)θ+A ,,-(7)v*b'
=-αsin #+A...
(8) Next, with differential amplifier 5.6, Vfa and V41a'%V
As a result of differential amplification between yb and v41b', MA -
V4ca V4I&' -J k αCoSe
(91vBz vvb −Vlb' = J kal
=s αs is the gain of the differential amplifiers j and A.

従ってパター/の形状の変化を互いに電気的に900位
相の異なる電気信号に変換することが5ることになる。
Therefore, there are five steps to convert changes in the shape of the putter into electrical signals that are electrically different in phase by 900 degrees.

以上は正弦波状のパターンについて述べたが正弦波以外
でも任意の周期関数の形状を有するパターン例えば第3
図aの正弦波に対し、同すの三角形波でも使用できる。
The above is a sine wave pattern.
In contrast to the sine wave shown in figure a, the same triangular wave can also be used.

ここで周期を3400とするとその%周期はtoOとな
る。
Here, if the period is 3400, its % period is toO.

かくて本発明による構成は簡単であり安価に製作でき直
流電源で動作できる。又NO加工技術の発達で円板が高
精度に加工可能となり関数の精度も従来のものより高精
度である。又接点が用いられないので信頼性が高い。更
に光源の光量な任意の時間関数で変化させれば出力の関
数を容易に任意の時間関数に変調できる。今光源の光量
の変化の関数をL(ωt)、パターンの関数をf(θ)
とすると出力の関数Fは F=L(ωt)・f(#) に変調されることとなる。尚ここでωは光源の光量変化
の角速度、0は関数発生器の入力軸の回転角度である。
Thus, the configuration according to the present invention is simple, can be manufactured at low cost, and can be operated with a DC power source. Furthermore, with the development of NO processing technology, it is now possible to process disks with high precision, and the precision of the function is also higher than that of conventional methods. Also, since no contacts are used, reliability is high. Furthermore, by changing the light intensity of the light source with an arbitrary time function, the output function can be easily modulated into an arbitrary time function. Now, the function of the change in the light amount of the light source is L (ωt), and the function of the pattern is f (θ).
Then, the output function F is modulated as F=L(ωt)·f(#). Here, ω is the angular velocity of the change in the light amount of the light source, and 0 is the rotation angle of the input shaft of the function generator.

又円周上に描かれたパターン例えば第ダ図a1に同図す
のように直線状のスケール上に描画することにより直線
状の動きに対応して関数を発生するリニヤ関数発生器と
することができる。
Also, by drawing a pattern drawn on the circumference on a linear scale, for example, as shown in Figure D a1, a linear function generator can be used that generates a function in response to linear movement. Can be done.

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

第1図aは回転円板l、同゛bは固定円板コの正面図、
同Cは回転円板lと固定円板−並びに発光、受光素子を
配する側断面図、第1図は本発明の一実施例電子回路結
線図、第J図a、bは同期関数の異る波形図、第ダ図a
、bは夫々円周−Fに描かれたパターンと直線状のスケ
ール上に描画するパターンである。 図でlは回転円板、コは固定円板、laは正弦波パター
ン、Ja、コa/、コb、コb′ はスリット、3龜e
 J a’ e J b * Jb’  は発光素子、
ダa。 ダa1.ダb、参b’は受光素子、j、Aは差動増巾器
。 特許出願人 多摩川精機株式会社
Figure 1a is a front view of the rotating disk l, and figure 1b is a front view of the fixed disk.
Figure C is a side cross-sectional view showing the rotating disk l, fixed disk, and light emitting and light receiving elements. Waveform diagram, Figure dA
, b are a pattern drawn on the circumference -F and a pattern drawn on a linear scale, respectively. In the figure, l is a rotating disk, C is a fixed disk, la is a sine wave pattern, Ja, Co a/, Co b, Co b' are slits, and 3 pieces e
J a' e J b * Jb' is a light emitting element,
Da a. Da a1. Da b and b' are light receiving elements, and j and A are differential amplifiers. Patent applicant Tamagawa Seiki Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] l 周縁にそって正弦波を含む任意の周期関数の形状な
有する透明或は不透明部分のパターンを含む回転円板と
、周縁方向に900間隔をおいて設けたスリットを含む
固定円板と、を軸心な一致せしめて並設しこれ等固定円
板、回転円板を挾んで900間隔を置いた亨個の発光素
子並びに受光素子を配設し、差動増巾器な含む電子回路
にパターンの形状変化に応じた電気信号を与えることに
より所望の関数信号をうろことを特命とする光学式関数
発生器。
l A rotating disk including a pattern of transparent or opaque parts having the shape of an arbitrary periodic function including a sine wave along the periphery, and a fixed disk including slits provided at 900 intervals in the circumferential direction. A large number of light-emitting elements and light-receiving elements are placed side by side with their axes aligned and spaced 900 meters apart with a fixed disk and a rotating disk sandwiched between them. An optical function generator whose mission is to generate a desired function signal by applying an electrical signal corresponding to the change in shape of the object.
JP537682A 1982-01-19 1982-01-19 Optical function generator Granted JPS58123160A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP537682A JPS58123160A (en) 1982-01-19 1982-01-19 Optical function generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP537682A JPS58123160A (en) 1982-01-19 1982-01-19 Optical function generator

Publications (2)

Publication Number Publication Date
JPS58123160A true JPS58123160A (en) 1983-07-22
JPS6155146B2 JPS6155146B2 (en) 1986-11-26

Family

ID=11609448

Family Applications (1)

Application Number Title Priority Date Filing Date
JP537682A Granted JPS58123160A (en) 1982-01-19 1982-01-19 Optical function generator

Country Status (1)

Country Link
JP (1) JPS58123160A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63212817A (en) * 1987-03-02 1988-09-05 Yokogawa Electric Corp Displacement converter

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2209807B (en) * 1987-09-17 1991-04-03 T & N Technology Ltd Cylinder head gasket

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63212817A (en) * 1987-03-02 1988-09-05 Yokogawa Electric Corp Displacement converter

Also Published As

Publication number Publication date
JPS6155146B2 (en) 1986-11-26

Similar Documents

Publication Publication Date Title
US4092579A (en) Brushless printed circuit resolver
US5598153A (en) Capacitive angular displacement transducer
US4238781A (en) Capacitive angular displacement transducer for remote meter reading
US3041486A (en) Variable reluctance device
US3162804A (en) Translating instrument employing hall-effect device
EP0009102A1 (en) A multipolar resolver
US4791366A (en) Apparatus including a pair of angularly spaced sensors for detecting angle of rotation of a rotary member
JP2001524206A (en) Clock with capacitance detection device
US2900612A (en) Variable coupling transformers
US2930033A (en) Angular position converter
JP2004508563A (en) Angle converter
US3309525A (en) Double shaft encoder using phase meter to indicate relative rotation
GB2116313A (en) Sine wave generator for position encoder
US3125716A (en) Machlis
US2701875A (en) Resistance type of phase shifter
US4336446A (en) Apparatus for the manual production of digital pulses
US4849621A (en) Rotational-position detecting apparatus with two shaped photovoltaic surfaces
JPS58123160A (en) Optical function generator
US3172023A (en) Variable capacitor
JP6507347B2 (en) Capacitance type angle detector
JP3865617B2 (en) Angle sensor
JPS5885115A (en) Optical type resolver phase shifter
US6211641B1 (en) Capacitive resolver
JPH0499913A (en) Optical encoder
US3222660A (en) Magnetic position encoder