JPS5885113A - Optical type resolver signal generator - Google Patents
Optical type resolver signal generatorInfo
- Publication number
- JPS5885113A JPS5885113A JP18222881A JP18222881A JPS5885113A JP S5885113 A JPS5885113 A JP S5885113A JP 18222881 A JP18222881 A JP 18222881A JP 18222881 A JP18222881 A JP 18222881A JP S5885113 A JPS5885113 A JP S5885113A
- Authority
- JP
- Japan
- Prior art keywords
- signal
- sine
- signals
- shaft encoder
- resolver signal
- 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
Landscapes
- Optical Transform (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は光学式レゾルバ信号発生器に係り%にインク
リメンタルシャフトエンコーダを用いてレゾルバ信号(
可変位相信号)を発生するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an optical resolver signal generator that uses an incremental shaft encoder to generate a resolver signal (
(variable phase signal).
インクリメンタルシャフトエンコーダハ角度信号とし”
’cn個の正弦9sinθ、cos# 信号を発生しこ
のsinθ、come信号は完全な正弦波でな(三角波
に近いが近似正弦波として考え説明することができ、実
用上においても差し支えない。しかして完全な正弦波信
号を得るには回転格子板に正弦波の形をしたパターンを
作る必要がありこれには回転格子板のカッティングに大
きな費用を畏する。この発明では回転格子板の製作が簡
単で低価格なインクリメンタルシャフトエンコーダの回
転格子板を使用して発生するsin#、 cos#信号
と基準信号gina+t 、 co−ωtとを使用しn
@O位相可変信号5in(a+t+#) t−電子回路
を用いて発生するものでここで作られる位相可変信号5
in(ωt+#)は、エンコーダの分解能を高めるため
、速度制御装置、計算費嵩尋に有効に使用される様に考
案され応用面は極めて広い。Incremental shaft encoder serves as angle signal
'cn sine 9 sin θ, cos # signals are generated, and this sin θ, come signal is a perfect sine wave (close to a triangular wave, but can be considered and explained as an approximate sine wave, and there is no problem in practical use. In order to obtain a perfect sine wave signal, it is necessary to create a sine wave-shaped pattern on the rotating grating plate, which requires a large expense in cutting the rotating grating plate.With this invention, the rotating grating plate can be manufactured easily. Using the sin#, cos# signals and the reference signals gina+t, co-ωt, which are generated using the rotating grating plate of a low-cost incremental shaft encoder,
@O Phase variable signal 5in (a+t+#) t- Phase variable signal 5 generated using an electronic circuit and created here
in(ωt+#) has been devised to be effectively used in speed control devices and to reduce calculation costs in order to increase the resolution of encoders, and has an extremely wide range of applications.
以下この発明を図の実施例について説明する。The present invention will be described below with reference to the embodiments shown in the drawings.
インクリメンタルシャフトエンコーダt[/図の構成図
に示す様に回転格子板/と第1.第JO/対の固定格子
板Ja、Jbとl対の光源(XJID )、J&、Jl
l:fiびに第7、第コ、#!3、第ダの受光素子(フ
オトセy)、$a、参1)、$6゜*aそれに第3図或
hg+図の電子回路よシ構成される。今第7図にてU社
格子板lが矢印方向に回転したとき固定格子&/l−通
る光源J1の元は第1の受光素子41IaK入υ第21
図のgin#信号となる。また固定格子板コaと明暗が
逆でおる格子が近接した位置にあり第21図の8in#
倍号を第一の受光素子41bに発生する。Incremental shaft encoder t[/As shown in the configuration diagram in the figure, the rotating grating plate/ and the first... JO/pair of fixed grating plates Ja, Jb and l pair of light sources (XJID), J&, Jl
l: fi and 7th, ko, #! 3. It is composed of the second light receiving element (photograph), $6゜*a, and the electronic circuit shown in Fig. 3 or hg+. Now, in FIG. 7, when the U company grating plate l rotates in the direction of the arrow, the source of the light source J1 passing through the fixed grating &/l is the first light receiving element 41IaK input υ21
This becomes the gin# signal in the figure. In addition, there is a lattice with opposite brightness and darkness in the vicinity of the fixed lattice plate core a, which is 8 inch # in Fig. 21.
A double sign is generated in the first light receiving element 41b.
さらに固定格子板−す會通る光源3bよシの元は第3の
受光素+−〇に入りco8θ信号となる。Further, the source of the light source 3b passing through the fixed grating plate enters the third light receiving element +-〇 and becomes a co8θ signal.
また第一の固足格子板コbと明暗が逆でToる格子が近
接した位置にあり第21図のcoa#僅号を第参の受光
素子ダdに発生する。又第11図に基準信号θ1nωt
、 OO+I*t f示すがこれらの信号は水晶IS
m子吟+1り作成されJ0KHg尋にて使用される。以
上のsinθ、 sin# 、 cos# 。Further, a grating having opposite brightness and darkness to that of the first solid foot grating plate B is located close to the first solid foot grating plate B, and generates the coa# in FIG. In addition, the reference signal θ1nωt is shown in FIG.
, OO+I*t f, but these signals are crystal IS
mzigin+1ri was created and used in J0KHghiro. The above sinθ, sin#, cos#.
coa # 、 sinωz 、 001(altの各
信号に対して第3図、第参図の電子回路を用いて下記に
より合成し可変位相信号−1n(*t+#) ’ft作
成する。Coa #, sinωz, 001(alt) are synthesized as shown below using the electronic circuit shown in FIG. 3 to create a variable phase signal -1n(*t+#)'ft.
5infscoaωt+cos#*eina+t=gi
n(*t+#)この可変位相信号−1n(ωを十〇)は
第11図に示すIIK正弦波信号であるが波形整形して
矩形波信号としても使用可能である。次に受光素子*a
、$b、亭o、参直からの電気信号sin a 、 s
inθ。5infscoaωt+cos#*eina+t=gi
n(*t+#) This variable phase signal -1n (ω is 10) is a IIK sine wave signal shown in FIG. 11, but it can also be used as a rectangular wave signal after waveform shaping. Next, the light receiving element*a
, $b, Tei o, electrical signal from the inspector sin a, s
inθ.
aOs # 、 coo #を変調増幅し、可変位相信
号を得る電子回路を先づ第JriAK示す。この図にお
いて光源Ll!jD J& 、 Jbからの元便号は受
光素子(フォト;ル)#1.ダ)、参〇、亭dに”cm
電気信号各々変換され演算増幅回路QI&t Qtbに
てsin#とsin#、oos #とcos#が夫々差
動増幅されるもので差動増幅することにより光源Ja。An electronic circuit for modulating and amplifying aOs # and coo # to obtain a variable phase signal will first be shown in JriAK. In this figure, the light source Ll! The original number from JD J&, Jb is photodetector (photo) #1. d), san〇, tei d”cm
The electric signals are each converted and sin# and sin#, oos# and cos# are differentially amplified by the operational amplifier circuits QI&tQtb, respectively, and the light source Ja is generated by differential amplification.
3zの光量変動に対する補償をする。差動増幅された一
1n$ 、 aog#信号はトランジスタ”rl Iテ
1.のベースに加えられるeoIωi 、 @inωを
信号にてスイッチνlされ合成される。この信号は次O
バッファ用演算増幅回路Q、t−通シ、 演算増幅回路
Q、で構成されるアクティブフィルタを通り正弦波O可
変位相信号gin(ωを十〇)をうるOである。第3図
の電子回路と同じ出力信号が得られる別の実施例を第参
図に示す、第参図では受光素+−aと*b、参CとダC
LO信号を夫々直接スイッチング回路Q4a + Q4
1)でスイッチングして合成し演算増幅回路Q、にて反
転増幅の後第3図と同様演算増幅回16’Ls で構
成されるアクディプフィルタを通り可変位相信号81n
(ωt+#)i作成するものである。3z Compensation for light intensity fluctuations. The differentially amplified 1n$ and aog# signals are added to the base of the transistor ``rl Ite1.'' and are combined by switching νl using the eoIωi and @inω signals. This signal is
A sine wave O variable phase signal gin (ω is 10) is obtained through an active filter consisting of a buffer operational amplifier circuit Q, a t-channel, and an operational amplifier circuit Q. Another embodiment in which the same output signal as the electronic circuit shown in FIG. 3 can be obtained is shown in FIG.
Direct switching circuit for each LO signal Q4a + Q4
The variable phase signal 81n is switched and synthesized in step 1), inverted and amplified in the operational amplifier circuit Q, and then passed through an accutip filter consisting of an operational amplifier circuit 16'Ls as shown in Fig. 3.
(ωt+#)i is created.
かくてこの発明ではインクリメンタルシャフトエンコー
ダを用いて1回転あたり、n個の正弦波信号かえられ、
これt−電子回路において基準信号を用いてスイッチン
グすることにより1回転あたりn個の位相可変信号をう
ろことができるO
以上によりこの発明では下記の様な特徴が得られる。Thus, in this invention, n sine wave signals are changed per revolution using an incremental shaft encoder,
By switching using the reference signal in the t-electronic circuit, it is possible to pass n phase variable signals per rotation.As a result of the above, the present invention has the following features.
即ち第1に基準信号として水晶振動子より作成されたテ
イジタル信号を使用することが可能なため精度の高いレ
ゾルバ信号全作成することができる。That is, first, since it is possible to use a digital signal created by a crystal oscillator as a reference signal, it is possible to create all highly accurate resolver signals.
第一に高い周波数の基準信号で動作できる。First, it can operate with a high frequency reference signal.
第3に刷子等の接触部がないため信頼性が高い。Third, there is no contact part such as a brush, so reliability is high.
第参に元11KL11fDを使用できるため信頼性が高
い。First of all, it is highly reliable because it can use the original 11KL11fD.
第1に受光素子からの電気信号を差動増幅しているので
光源の光量変化、経年変化に強い。First, because the electrical signals from the light-receiving elements are differentially amplified, it is resistant to changes in the amount of light from the light source and changes over time.
第6にインクリメンタルシャフトエンコーダの回転格子
板管使用しているため低価格で簡単にシゾルバ僅号が得
られる。Sixth, since the rotating grid plate tube of the incremental shaft encoder is used, it is possible to easily obtain a small sizsolver at a low cost.
第7に磁気式レゾルバに比べ回転速度を大きくできる。Seventhly, the rotation speed can be increased compared to a magnetic resolver.
#!亭図はこの発F!i4に係る実施例を示す′越子回
路構成図である。
図でlはV:AI!格子板1.21.コbは固定格子板
、J a e J bは光源、参a、*b、*c、4<
dは受光素子、Qsa a ’Ltbは演算増幅回路、
Q、 、 GL、は演算増幅回路、’Lea e GL
abはスイッチング回路。#! Teizu is from this F! FIG. 2 is a block diagram of a circuit diagram showing an embodiment related to i4. In the figure, l is V:AI! Lattice plate 1.21. Cob is a fixed grid plate, J ae J b is a light source, reference a, *b, *c, 4<
d is a light receiving element, Qsa a'Ltb is an operational amplifier circuit,
Q, GL are operational amplifier circuits, 'Lea e GL
ab is a switching circuit.
Claims (1)
るインクリメンタルシャフトエンコーダにおいてノ回転
あたりn個発生する一1n#。 CO5−のシャフトエンコーダ信号に対して水晶畿動子
等により作成される基準信号alnωt。 COOωtt′用いて電子回路でスイッチングするよう
にしたことt−特徴とする光学式レゾルバ信号発生器。[Claims] In an incremental shaft encoder consisting of a light source, a light receiving element, a rotating grating plate, and a fixed grating plate, n signals are generated per revolution. A reference signal alnωt is created using a crystal oscillator or the like for the shaft encoder signal of CO5-. An optical resolver signal generator characterized in that switching is performed by an electronic circuit using COOωtt'.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18222881A JPS5885113A (en) | 1981-11-16 | 1981-11-16 | Optical type resolver signal generator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18222881A JPS5885113A (en) | 1981-11-16 | 1981-11-16 | Optical type resolver signal generator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5885113A true JPS5885113A (en) | 1983-05-21 |
Family
ID=16114580
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP18222881A Pending JPS5885113A (en) | 1981-11-16 | 1981-11-16 | Optical type resolver signal generator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5885113A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60526U (en) * | 1983-06-15 | 1985-01-05 | 株式会社 小野測器 | Measuring device for rotation angle variation |
US5276323A (en) * | 1991-06-13 | 1994-01-04 | Kabushiki Kaisha Tokai Rika Denki Seisakusho | Optical movement detector detecting a position of an optical gravity center |
-
1981
- 1981-11-16 JP JP18222881A patent/JPS5885113A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60526U (en) * | 1983-06-15 | 1985-01-05 | 株式会社 小野測器 | Measuring device for rotation angle variation |
US5276323A (en) * | 1991-06-13 | 1994-01-04 | Kabushiki Kaisha Tokai Rika Denki Seisakusho | Optical movement detector detecting a position of an optical gravity center |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
Woltring | Single-and dual-axis lateral photodetectors of rectangular shape | |
KR870005252A (en) | Encoder Circuit of Rotating Body Sensor | |
GB1495320A (en) | Magnetic field sensing apparatus | |
JPH0246087B2 (en) | ||
JPS58157203A (en) | Optical device for generating sinusoidal wave of low harmonic wave content | |
JPS5885113A (en) | Optical type resolver signal generator | |
JP2005017116A (en) | Photo detector for optical encoder | |
JPS60260812A (en) | Digital controller | |
US3147374A (en) | Resolver apparatus using variable capacitors comprising toothed rotor and stator | |
US3942002A (en) | Signal combining circuits | |
JPS5885114A (en) | Optical type resolver signal generator | |
JPS60135768A (en) | Rotation detector | |
GB2061523A (en) | Measuring an Incrementally Subdivided Path or Angle Digitally | |
JPS5885115A (en) | Optical type resolver phase shifter | |
JPH0996544A (en) | Optical absolute encoder | |
SU453562A1 (en) | MAGNETORESISTIVE CONVERTER OF ANGLE OF TURNING INTO ELECTRIC SIGNAL | |
JP2767281B2 (en) | Magnetic sensor | |
SU788140A1 (en) | Shaft angular position-to-code converter | |
JP2691942B2 (en) | Rotary type absolute encoder | |
SU660064A1 (en) | Biharmonic sine-cosine multiplying arrangement | |
JPS6155146B2 (en) | ||
JPS61292503A (en) | Detector for angle of rotation | |
JPS6163111U (en) | ||
JPH0425260A (en) | Phase modulation circuit | |
RU2226695C1 (en) | Device for measurement of accelerations |