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JPS6131409B2 - - Google Patents
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JPS6131409B2 - - Google Patents

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Publication number
JPS6131409B2
JPS6131409B2 JP3606681A JP3606681A JPS6131409B2 JP S6131409 B2 JPS6131409 B2 JP S6131409B2 JP 3606681 A JP3606681 A JP 3606681A JP 3606681 A JP3606681 A JP 3606681A JP S6131409 B2 JPS6131409 B2 JP S6131409B2
Authority
JP
Japan
Prior art keywords
pattern
signals
light
signal
circuit means
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.)
Expired
Application number
JP3606681A
Other languages
Japanese (ja)
Other versions
JPS57149914A (en
Inventor
Yasuo Ebara
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.)
IHI Corp
Original Assignee
Ishikawajima Harima Heavy Industries 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 Ishikawajima Harima Heavy Industries Co Ltd filed Critical Ishikawajima Harima Heavy Industries Co Ltd
Priority to JP3606681A priority Critical patent/JPS57149914A/en
Publication of JPS57149914A publication Critical patent/JPS57149914A/en
Publication of JPS6131409B2 publication Critical patent/JPS6131409B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/26Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
    • G01D5/32Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
    • G01D5/34Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/36Forming the light into pulses
    • G01D5/38Forming the light into pulses by diffraction gratings

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Transform (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

この発明は検出対象物の移動にともなつて信号
を発生させその波形数をカウントすることにより
該対象物の位置を検出する装置に関する。 検出対象物の移動にともなつて信号を発生させ
その波形数をカウントすることにより該対象物の
位置を検出する方法を利用した位置検出装置とし
てインクリメンタルロータリエンコーダと呼ばれ
るものが従来より知られている。その原理は第1
図に示すように回転スリツト板1に光を透過する
部分1aと遮断する部分1bを所定のピツチで連
続的にかつ回転軸5と同心で同一周上に配置した
パターンを刻み込み、この回転スリツト板1およ
びそれと同じピツチでパターンを刻み込んだ固定
スリツト2をはさんで発光ダイオード3およびフ
オトダイオード4を配設し、回転軸5を介して回
転スリツト板1を位置検出対象物(例えば工作機
械)の移動にともなつて回転させることによつ
て、その移動量に応じた回数だけ発光ダイオード
3からフオトダイオード4に入射する光が遮断さ
れるようにし、これによりフオトダイオード4か
ら得られる信号の波形数(パルス数)をカウント
することにより前記対象物の位置を検出するよう
にしたものである。 かかる位置検出装置においては位置検出の分解
能は回転スリツト板1の1回転当たりに得られる
パルス数によつて決まる。従来は回転スリツト板
における明暗模様の数を多くする(密度を高くす
る)ことにより1回転回当りのパルス数を増やし
て分解能を高めるようにしていた。しかし、この
方法では明暗模様の数を増やすにしたがい個々の
明暗幅は狭くしなければならないのに対し、明暗
模様の刻み精度には限界があるため、回転スリツ
ト板の径を大きくすることによつて広い明暗幅を
確保しなければならなかつた。このため検出装置
の形状が大型化し重くなる欠点があつた。 この発明は従来のものにおける以上のような欠
点を除去して、装置を大型化せずに分解能を高め
ることができる位置検出装置を提供することを目
的とするものである。この発明によれば明暗模様
と複数のフオトカプラとの組合せ等により、それ
ぞれが位置検出対象物の移動量に対応した信号で
あつて相互に所定の角度ずつ位相をずらした複数
本の信号をつくり、これら複数本の信号を位相が
隣りあうもの同士をそれぞれ比較してそれらのク
ロスポイントを検出しその数を累積することによ
つて前記対象物の位置(直線位置または角度位
置)を検出するようにしている。すなわち、所定
の角度ずつ位相のずれた複数の信号を用いること
により該信号をその位相角ずつに分割した情報が
得られるようにして明暗模様等の密度が低いまま
でも高い分解能が得られるようにしている。しか
も、この発明では単に信号数に等しい分解能でな
く、信号数よりも高い分解能が得られるようにし
ている。 このように、本来得られる情報を分割して分解
能を高めるという場合各分割幅が等しいことが必
要である。このためには分割数に応じた数の信号
を分割数に応じた角度ずつ位相をずらしてつくり
出すことが必要である。ところで位相のずれた2
信号を比較するという場合においては第2図に示
すように信号S1,S2は180゜ごとにクロスす
るため、このクロスポイントX1,X2,X3,
X4,X5,X6,…をカウントすれば個々の信
号S1またはS2の波形数をカウントする場合に
比べてこれだけで2倍の分解能が得られることに
なる。この発明ではこれを利用して少ない検出信
号数で高い分解能を実現している。位相が隣りあ
うもの同士を比較する場合においては検出信号
(フオトカプラ等の検出手段から得られる信号)
の数をnとすればn−1の組合せが得られるか
ら、各組合せにおいて2倍ずつ分解能が高められ
れば全体で2(n−1)倍に分解能を高められる
ことになる。ただし、この場合分割幅を等しくす
る(各分割幅を1波長の1/2(n−1)ずつにする。
)た めに検出信号の位相はその数に応じた値に適宜設
定する必要がある。具体的には検出信号の数によ
つてそれらの位相を第1表に示す関係に設定すれ
ば等しい分割幅が得られる。なお、n=2の場合
は例外的に信号数と分解能が等しくなつて、信号
数以上の分解能を得るというこの発明の目的に合
致しないので、この発明から除外される。
The present invention relates to a device that detects the position of an object by generating signals as the object moves and counting the number of waveforms. An incremental rotary encoder has been known as a position detection device that detects the position of an object by generating a signal as the object moves and counting the number of waveforms. . The principle is the first
As shown in the figure, a pattern is carved into the rotary slit plate 1 in which light transmitting portions 1a and light blocking portions 1b are arranged continuously at a predetermined pitch and concentrically with the rotating shaft 5 on the same circumference. A light emitting diode 3 and a photodiode 4 are arranged across a plate 1 and a fixed slit 2 in which a pattern is engraved at the same pitch. By rotating the light emitting diode 3 as it moves, the light incident on the photodiode 4 from the light emitting diode 3 is blocked a number of times corresponding to the amount of movement, thereby changing the waveform of the signal obtained from the photodiode 4. The position of the object is detected by counting the number of pulses. In such a position detection device, the resolution of position detection is determined by the number of pulses obtained per rotation of the rotary slit plate 1. Conventionally, resolution has been improved by increasing the number of light and dark patterns on the rotating slit plate (increasing the density) to increase the number of pulses per rotation. However, with this method, as the number of bright and dark patterns increases, the width of each bright and dark pattern must be narrowed, but since there is a limit to the precision of marking the bright and dark patterns, it is possible to increase the diameter of the rotating slit plate. It was necessary to ensure a wide range of brightness and darkness. This has resulted in the disadvantage that the detection device becomes larger and heavier. It is an object of the present invention to provide a position detection device that can eliminate the above-mentioned drawbacks of the conventional device and improve resolution without increasing the size of the device. According to this invention, a plurality of signals each corresponding to the amount of movement of the object to be detected and whose phases are shifted by a predetermined angle from each other are created by a combination of a light and dark pattern and a plurality of photocouplers, The position (linear position or angular position) of the object is detected by comparing these multiple signals with adjacent phases, detecting their cross points, and accumulating the number of cross points. ing. That is, by using a plurality of signals whose phases are shifted by a predetermined angle, information obtained by dividing the signal into each phase angle can be obtained, so that high resolution can be obtained even when the density of bright and dark patterns remains low. ing. Moreover, in the present invention, it is possible to obtain not only a resolution equal to the number of signals but also a resolution higher than the number of signals. In this way, when dividing originally obtained information to improve resolution, it is necessary that each division width be equal. For this purpose, it is necessary to generate a number of signals corresponding to the number of divisions by shifting the phase by an angle corresponding to the number of divisions. By the way, the phase shift 2
When comparing signals, as shown in Figure 2, the signals S1 and S2 cross every 180 degrees, so the cross points X1, X2, X3,
By counting X4, X5, X6, . . . , twice the resolution can be obtained compared to counting the number of waveforms of each signal S1 or S2. This invention utilizes this to achieve high resolution with a small number of detection signals. When comparing items with adjacent phases, a detection signal (a signal obtained from a detection means such as a photocoupler)
If the number of is n, then n-1 combinations are obtained, so if the resolution is increased by a factor of 2 in each combination, the overall resolution will be increased by a factor of 2 (n-1). However, in this case, the division widths are made equal (each division width is 1/2 (n-1) of one wavelength).
), it is necessary to appropriately set the phase of the detection signal to a value corresponding to the number of detection signals. Specifically, if the phases of the detection signals are set in the relationship shown in Table 1 depending on the number of detection signals, equal division widths can be obtained. Note that in the case of n=2, the number of signals and the resolution are exceptionally equal, and this does not meet the purpose of the present invention of obtaining a resolution greater than the number of signals, and is therefore excluded from the present invention.

【表】 次に、この発明の実施例を添付図面を参照して
詳しく説明する。 第3図はこの発明を適用したインクリメンタル
ロータリエンコーダの内部構成の一例を概略で示
したものである。第3図の実施例は検出信号の数
を3とした場合すなわち分解能を4倍とした場合
のものである。第3図において回転スリツト板1
0には光を透過する部分10aと遮断する部分1
0bからなるパターンが所定のピツチで連続的に
かつ回転軸11と同心で同一周上に形成されてい
る。回転スリツト板10の回転軸11は位置検出
対象物(図示せず)の移動に応じて回転される。
回転スリツト板10に対してはそれを挾んでフオ
トカプラP1,P2,P3(発光ダイオードD
1,D2,D3およびフオトダイオードd1,d
2,d3)が配設され、発光ダイオードD1,D
2,D3からの光が回転スリツト板10の透過部
分10aを介してフオトダイオードd1,d2,
d3にそれぞれ入射するようになつている。フオ
トダイオードd1,d2,d3からは第1表に従
つて90゜ずつ位相がずれた信号を取出すようにす
る。このためにはフオトカプラP1,P2,P3
を回転スリツト板10の明暗パターンの90゜/360
゜=1/4 ピツチずつその連続方向(回転スリツト板10の
円周方向)にずらして配置すればよい。もちろん
1ピツチは極めて短い距離でありその間に1/4ピ
ツチずつずらしてフオトカプラP1,P2,P3
を並べることは困難であるため、ピツチをいくつ
かおきにとびこした位置において相対的に1/4ピ
ツチずつずれるように配置し、結果的に1/4ずつ
位相がずれた信号が得られるようにすればよい。 回転スリツト板10とフオトダイオードd1,
d2,d3との間にはスリツト群12−1,12
−2,12−3を形成した受光用固定スリツト板
12が配置されている。この固定スリツト板12
はフオトダイオードd1,d2,d3に対する斜
め方向からの光の照射を遮断して、各フオトカプ
ラP1,P2,P3の光軸と回転スリツト板10
の透過部分10aとが完全に一致した位置におい
てのみ発光ダイオードD1,D2,D3の光がフ
オトダイオードd1,d2,d3に入射されるよ
うにするためのものである。したがつてスリツト
群12−1,12−2,12−3はフオトカプラ
P1,P2,P3の光軸上にそれぞれ形成されて
いる。尚、各スリツト群12−1,12−2,1
2−3は前記回転スリツト板10のパターンと同
じピツチで形成された複数本のスリツトからな
り、大きな光量がフオトダイオードd1,d2,
d3に入射されるようにしてS/N比の向上を図
つている。 第4図は第3図の実施例における回転スリツト
板10の透過部分(スリツト)10aと固定スリ
ツト板12のスリツト12−1,12−2,12
−3との位置関係を概略的に示したものである。
すなわち、固定スリツト板12のスリツト12−
1,12−2,12−3は回転スリツト板10の
パターンの1ピツチTに対し1/4ピツチずつ位相
がずれており、スリツト12−1が透過部分10
aに一致してから1/4T回転した位置でスリツト
12−2が透過部分10aに一致し、更に1/4T
回転した位置でスリツト12−3が透過部分10
aに一致するようになつている。したがつてフオ
トカプラP1,P2,P3からは第5図に示すよ
うに1周期が回転スリツト板10の所定の回転量
(すなわち位置検出対象物の所定の移動量)Tに
対応し相互に1/4周期ずつ位相がずれた信号SA
1,SA2,SA3が取出される。 第6図は信号SA1,SA2,SA3にもとづい
て検出対象物の位置を求める回路の一例を示すも
のである。第7図は第6図の動作波形図で、(a)は
信号SA1,SA2,SA3、(b)は信号SB12、(c)
は信号SB23、(d)はエツジトリガパルス発振器
21−1の出力、(e)はエツジトリガパルス発振器
21−2の出力、(f)はオア回路22の出力であ
る。第6図においてフオトダイオードd1,d
2,d3から出力される信号SA1,SA2,SA
3は位相がとなりあうもの同士すなわち信号SA
1と信号SA2、信号SA2と信号SA3が比較増
幅器20−1,20−2でそれぞれ比較される。
これにより比較増幅器20−1,20−2からは
第7図b,cにそれぞれ示すパルス信号SB1
2,SB23が出力される。このパルス信号SB1
2,SB23は周期が検出信号SA1,SA2,SA
3の周期Tと同じで、デユーテイサイクルが50%
で、位相が相互に1/4周期ずれた信号である。 比較増幅器20−1,20−2の出力信号SB
12,SB23はエツジトリガパルス発信器21
−1,21−2でそれぞれの立上りおよび立下り
が抽出される。第7図d,eは各々で抽出された
パルスを示すものである。エツジトリガパルス発
信器21−1,21−2の出力はオア回路22で
論理和がとられアツプ/ダウンカウンタ23で累
算される。オア回路22の出力SB12+SB23
は第7図fに示すように検出信号SA1,SA2,
SA3の周期の1/4の周期であるから信号SA1
(または信号SA2または信号SA3)の波形数を
直接累算する場合に比べて4倍の分解能で位置検
出を行なえることになる。 尚、カウンタ23による累算は回転スリツト板
10の回転方向に応じて(すなわち検出対象物の
移動方向に応じて)加算または減算に切換えられ
る。回転スリツト板10の回転方向は比較増幅器
20−1,20−2の出力パルスSB12,SB2
3を利用してそれらのうちいずれが先に立上るか
を検出することにより判別することができる。す
なわち、第6図の方向識別回路24に示すように
ゲーテドモノマルチバイブレータ25を信号SB
12と信号12で駆動し、ゲーテドモノマル
チバイブレータ26を信号12とSB23で駆
動し、それらの出力でフリツプフロツプ回路27
をセツト、リセツトすれば、フリツプフロツプ回
路27からは第8図に示すように回転方向に応じ
た信号が得られる。この信号によつてアツプ/ダ
ウンカウンタ23をアツプカウントもしくはダウ
ンカウントに切換えればそのカウント値は検出対
象物の位置に正確に対応したものとなる。 以上はフオトカプラを3つ使用して分解能を4
倍にする場合について示したがその他の場合でも
同様に行なうことができる。例えばフオトカプラ
を6つ使用する場合は第1表に示す通り位相を36
゜ずつずらして配置すればよい。そのときの動作
波形図を第9図に示す。第9図において(a)は6つ
の検出信号SC1〜SC6、(b)はSC1〜SC2の比
較、(c)はSC2、SC3の比較、(d)はSC3,SC4
の比較、(e)はSC4,SC5の比較、(f)はSC5,
SC6の比較、(g)は上記の比較により得られるパ
ルス信号である。すなわち、フオトカプラからは
第9図aに示すように36゜ずつ位相がずれた信号
SC1〜SC6が得られる。これらを位相が隣りあ
うもの同士比較すれば第9図b〜fに示すように
周期が検出信号SC1〜SC6の周期と同じで、デ
ユーテイサイクルが50%で、位相が36゜ずつ(す
なわち1/10周期ずつ)ずれた5つのパルス信号が
得られる。これらのパルス信号のエツジをそれぞ
れ抽出し、それらの論理和を取れば第9図gに示
すようにもとの信号SC1〜SC6の周期Tを1/10
分割したパルス信号が得られる。従つてこのパル
ス信号をカウントすれば10倍の分解能で位置検出
を行なうことができる。 また、この発明は上記実施例で示したもの以外
にも例えば次のような様々なバリエーシヨンが考
えられる。 光学式以外の方法への適用 回転スリツト板の透過部分を溝として形成し、
そこに複数のリミツトスイツチを所定の角度ずつ
位相をずらして配置し、機械的に信号をつくり出
す。 リニアスケールへの適用 前述した実施例では検出対象物の直線方向の移
動を回転スリツト板1の回転運動に変換して検出
を行なつたが、直線方向の移動を直接検出するこ
ともできる。すなわち、直線上のスリツト板を検
出対象物の移動方向に配し、かつフオトカプラを
それを挾んで対向させ、それらの位置関係が検出
対象物の移動にともなつて直線的に変化するよう
にすれば同様に位置検出を行なえる。この場合も
複数のフオトカプラを所定の角度(1周期360゜
とした場合の電気角)ずつ位相をずらして配置す
れば分解能を高めることができる。 角度位置検出器としての利用 前述した実施例では直線方向の位置を検出する
場合について示したが、角度が変化する機械の角
度位置検出手段として用いることもできる。 前述した実施例では1列の明暗パターンに対
し複数のフオトカプラを所定の角度ずつ位相を
ずらして配置したが、これと逆に複数本の明暗
パターンを所定の角度ずつ位相をずらして並列
に形成し、各パターンに対応してその連続方向
の同じ位置にフオトカプラをそれぞれ配置する
ようにしても同様の検出を行なうことができ
る。例えば分解能を4倍にする場合は第10図
に示すように3本の明暗パターン31,32,
33をそれらのピツチTの1/4ずつ位相をずら
して形成し、各パターン31,32,33に対
応してフオトカプラP31,P32,P33を
それらの連続方向に対し同じ位置に配置すれば
よい。 第3図の実施例ではフオトカプラP1,P
2,P3をそれぞれ独立に配置したが、第11
図に示すように1つの発光素子D40で複数の
受光素子d40−1,d40−2,d40−3
をまとめて照射するようにすれば発光素子D4
0が経時劣化しても検出信号のレベルは全部が
同じ割合で変化し各検出信号間のクロスポイン
トの間隔は一定となるので検出精度が低下する
ことがなく、また、素子数が少ないので経済的
でもある。 以上説明したようにこの発明によれば所定の角
度ずつ位相がずれた複数の検出信号をつくり、そ
れらの信号によつてもとの信号の周期を分割した
信号を得るようにしたので、検出信号の周波数を
高くしなくても(すなわち光学式エンコーダにお
いては明暗パターンの密度を高くしなくても)高
い分解能で位置検出を行なうことができる。ま
た、2信号の比較にもとづき検出されるそれらの
クロスポイントはもとの信号の1周期に2箇所検
出されるので、少ない検出信号の数で高い分解能
が得られるので小型化、高信頼化、および経済性
の高い検出器が実現できる。(第1表に示すよう
にn本の検数信号で2(n−1)倍に分解能を高
めることができる)。
[Table] Next, embodiments of the present invention will be described in detail with reference to the accompanying drawings. FIG. 3 schematically shows an example of the internal configuration of an incremental rotary encoder to which the present invention is applied. The embodiment shown in FIG. 3 is an example in which the number of detection signals is three, that is, the resolution is four times as large. In Fig. 3, the rotating slit plate 1
0 has a portion 10a that transmits light and a portion 1 that blocks light.
A pattern consisting of 0b is formed continuously at a predetermined pitch, concentrically with the rotating shaft 11, and on the same circumference. The rotating shaft 11 of the rotating slit plate 10 is rotated in accordance with the movement of a position detection target (not shown).
For the rotating slit plate 10, photocouplers P1, P2, P3 (light emitting diodes D
1, D2, D3 and photodiodes d1, d
2, d3) are arranged, and light emitting diodes D1, D
2, the light from D3 passes through the transparent portion 10a of the rotating slit plate 10 to the photodiodes d1, d2,
d3, respectively. From the photodiodes d1, d2, and d3, signals are taken out of phase by 90° according to Table 1. For this purpose, photocouplers P1, P2, P3
90°/360 of the light and dark pattern of the rotating slit plate 10
They may be arranged by shifting them by 1/4 pitch in the continuous direction (circumferential direction of the rotating slit plate 10). Of course, one pitch is an extremely short distance, and the photo couplers P1, P2, P3 are shifted by 1/4 pitch during that distance.
Since it is difficult to line up the pitches, the pitches are placed so that they are relatively shifted by 1/4 pitch at every few positions, and as a result, signals with the phase shifted by 1/4 are obtained. Just do it. Rotating slit plate 10 and photodiode d1,
There are slit groups 12-1 and 12 between d2 and d3.
A light-receiving fixed slit plate 12 having numbers -2 and 12-3 formed therein is arranged. This fixed slit plate 12
blocks the photodiodes d1, d2, d3 from being irradiated with light from an oblique direction, and connects the optical axis of each photocoupler P1, P2, P3 with the rotating slit plate 10.
This is to allow the light from the light emitting diodes D1, D2, D3 to be incident on the photodiodes d1, d2, d3 only at positions where the transparent portions 10a of the light emitting diodes D1, D2, and D3 completely coincide with each other. Therefore, the slit groups 12-1, 12-2, and 12-3 are formed on the optical axes of the photocouplers P1, P2, and P3, respectively. In addition, each slit group 12-1, 12-2, 1
2-3 consists of a plurality of slits formed at the same pitch as the pattern of the rotating slit plate 10, and a large amount of light is transmitted to the photodiodes d1, d2,
The S/N ratio is improved by making the light incident on d3. FIG. 4 shows the transparent portion (slit) 10a of the rotating slit plate 10 and the slits 12-1, 12-2, 12 of the fixed slit plate 12 in the embodiment shown in FIG.
This figure schematically shows the positional relationship with -3.
That is, the slit 12- of the fixed slit plate 12
1, 12-2, and 12-3 are out of phase by 1/4 pitch with respect to 1 pitch T of the pattern of the rotating slit plate 10, and the slit 12-1 is in the transparent part 10.
The slit 12-2 coincides with the transparent part 10a at a position rotated by 1/4T after aligning with point a, and further rotated by 1/4T.
In the rotated position, the slit 12-3 is the transparent part 10
It is designed to match a. Therefore, as shown in FIG. 5, from the photocouplers P1, P2, and P3, one period corresponds to a predetermined amount of rotation T of the rotating slit plate 10 (i.e., a predetermined amount of movement of the object to be detected), and each period is 1/1. Signal SA whose phase is shifted by 4 periods
1, SA2, and SA3 are extracted. FIG. 6 shows an example of a circuit for determining the position of the object to be detected based on the signals SA1, SA2, and SA3. Figure 7 is an operating waveform diagram of Figure 6, (a) is the signal SA1, SA2, SA3, (b) is the signal SB12, (c)
is the signal SB23, (d) is the output of the edge trigger pulse oscillator 21-1, (e) is the output of the edge trigger pulse oscillator 21-2, and (f) is the output of the OR circuit 22. In Fig. 6, photodiodes d1, d
Signals SA1, SA2, SA output from 2, d3
3 are signals whose phases are adjacent to each other, that is, signals SA
1 and signal SA2, and signal SA2 and signal SA3 are compared by comparison amplifiers 20-1 and 20-2, respectively.
As a result, the comparator amplifiers 20-1 and 20-2 output pulse signals SB1 as shown in FIG. 7b and c, respectively.
2, SB23 is output. This pulse signal SB1
2, SB23 has a cycle of detection signals SA1, SA2, SA
Same as period T in 3, duty cycle is 50%
These are signals whose phases are shifted by 1/4 period from each other. Output signal SB of comparison amplifiers 20-1 and 20-2
12, SB23 is the edge trigger pulse oscillator 21
-1 and 21-2, respective rising and falling edges are extracted. Figures 7d and 7e show the pulses extracted in each case. The outputs of the edge trigger pulse generators 21-1 and 21-2 are logically summed by an OR circuit 22 and accumulated by an up/down counter 23. Output of OR circuit 22 SB12+SB23
As shown in Fig. 7f, the detection signals SA1, SA2,
Since the period is 1/4 of the period of SA3, signal SA1
Position detection can be performed with four times the resolution compared to the case where the number of waveforms of (or signal SA2 or signal SA3) is directly accumulated. Incidentally, the accumulation by the counter 23 is switched to addition or subtraction depending on the rotational direction of the rotating slit plate 10 (that is, depending on the moving direction of the object to be detected). The rotation direction of the rotating slit plate 10 is determined by the output pulses SB12 and SB2 of the comparison amplifiers 20-1 and 20-2.
This can be determined by detecting which of them rises first using 3. That is, as shown in the direction identification circuit 24 in FIG.
12 and signal 12, gated mono multivibrator 26 is driven by signal 12 and SB23, and their outputs drive flip-flop circuit 27.
By setting and resetting the flip-flop circuit 27, a signal corresponding to the direction of rotation is obtained from the flip-flop circuit 27 as shown in FIG. If the up/down counter 23 is switched to up counting or down counting by this signal, the count value will accurately correspond to the position of the object to be detected. The above uses 3 photocouplers to increase the resolution to 4.
Although the case of doubling is shown, it can be carried out similarly in other cases as well. For example, when using six photocouplers, the phase is set to 36 as shown in Table 1.
It is only necessary to arrange them by shifting them by ゜. The operating waveform diagram at that time is shown in FIG. In Figure 9, (a) shows the six detection signals SC1 to SC6, (b) compares SC1 to SC2, (c) compares SC2 and SC3, and (d) shows SC3 and SC4.
(e) is a comparison of SC4 and SC5, (f) is a comparison of SC5,
Comparison of SC6, (g) is the pulse signal obtained by the above comparison. In other words, the photocoupler outputs a signal whose phase is shifted by 36 degrees as shown in Figure 9a.
SC1 to SC6 are obtained. If we compare these signals with adjacent phases, we can see that the period is the same as that of the detection signals SC1 to SC6, the duty cycle is 50%, and the phase is 36° each (i.e., Five pulse signals shifted by 1/10 period) are obtained. By extracting the edges of these pulse signals and taking their logical sum, the period T of the original signals SC1 to SC6 can be reduced to 1/10 as shown in Figure 9g.
A divided pulse signal is obtained. Therefore, by counting these pulse signals, position detection can be performed with ten times the resolution. Further, the present invention may have various variations other than those shown in the above embodiments, such as the following. Application to non-optical methods The transparent part of the rotating slit plate is formed as a groove,
Multiple limit switches are placed there with their phases shifted by a predetermined angle to mechanically generate signals. Application to Linear Scale In the embodiments described above, the linear movement of the object to be detected was converted into the rotational movement of the rotary slit plate 1 for detection, but linear movement can also be directly detected. In other words, a linear slit plate is arranged in the direction of movement of the object to be detected, and the photocoupler is sandwiched between it and opposed to each other, so that the positional relationship between them changes linearly as the object to be detected moves. Position detection can be performed in the same way. In this case as well, resolution can be improved by arranging a plurality of photocouplers with their phases shifted by a predetermined angle (electrical angle when one cycle is 360°). Use as an angular position detector In the above-described embodiment, the case of detecting a position in a linear direction was shown, but it can also be used as an angular position detecting means for a machine whose angle changes. In the above-mentioned embodiment, a plurality of photocouplers were arranged with the phase shifted by a predetermined angle for one row of bright and dark patterns, but conversely, a plurality of light and dark patterns were formed in parallel with the phase shifted by a predetermined angle. , similar detection can be carried out by arranging photocouplers at the same position in the continuous direction corresponding to each pattern. For example, to quadruple the resolution, three bright and dark patterns 31, 32,
33 are formed with their phases shifted by 1/4 of the pitch T, and photocouplers P31, P32, P33 corresponding to each pattern 31, 32, 33 are arranged at the same position in the continuous direction thereof. In the embodiment of FIG. 3, photocouplers P1, P
2 and P3 were placed independently, but the 11th
As shown in the figure, one light emitting element D40 has multiple light receiving elements d40-1, d40-2, d40-3.
If it is irradiated all at once, the light emitting element D4
Even if 0 deteriorates over time, the levels of all detection signals change at the same rate, and the interval between the cross points between each detection signal is constant, so detection accuracy does not decrease, and since the number of elements is small, it is economical. It is also a target. As explained above, according to the present invention, a plurality of detection signals whose phases are shifted by a predetermined angle are created, and a signal obtained by dividing the period of the original signal is obtained by these signals, so that the detection signal Position detection can be performed with high resolution without increasing the frequency (that is, without increasing the density of the bright and dark pattern in the optical encoder). In addition, the cross points detected based on the comparison of two signals are detected at two points in one period of the original signal, so high resolution can be obtained with a small number of detection signals, resulting in miniaturization, high reliability, and a highly economical detector can be realized. (As shown in Table 1, the resolution can be increased by 2(n-1) times with n counting signals).

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

第1図はインクリメンタルロータリエンコーダ
の内部構造の概略を示す斜視図、第2図は位相の
ずれた2信号が互いにクロスする状態を示す波形
図、第3図はこの発明をインクリメンタリロータ
リエンコーダに適用した場合における機械的構成
部分の一実施例を示す斜視図、第4図は第3図に
おける回転スリツト板10のスリツト10aと固
定スリツト12−1,12−2,12−3の位置
関係を模式的に示した図、第5図は第3図のフオ
トカプラP1,P2,P3から得られる信号波形
を示す図、第6図は第3図のフオトカプラP1,
P2,P3から得られる信号にもとづいて位置検
出を行なう回路の一実施例を示すブロツク図、第
7図は第6図の回路の動作波形図、第8図は第6
図の方向識別回路の動作説明図、第9図は6つの
検出信号にもとづいて位置検出を行なう場合の動
作波形図、第10図はフオトカプラを所定の角度
ずつ位相をずらすかわりに複数の明暗パターンを
所定の角度ずつ位相をずらして形成するようにし
たこの発明の他の実施例を示す図、第11図はフ
オトカプラの変更例を示す斜視図である。 10……回転スリツト板、11……回転軸、1
2……固定スリツト板、P1,P2,P3……フ
オトカプラ(D1,D2,D3……発光ダイオー
ド、d1,d2,d3……フオトダイオード)、
20−1,20−2……比較増幅器、21−1,
21−2……エツジトリガパルス発信器、24…
…方向識別回路、31,32,33……明暗パタ
ーン列、P31,P32,P33……フオトカプ
ラ、40……発光素子、d40−1,d40−
2,d40−3……受光素子。
Fig. 1 is a perspective view schematically showing the internal structure of an incremental rotary encoder, Fig. 2 is a waveform diagram showing a state in which two signals with different phases cross each other, and Fig. 3 is an application of the present invention to an incremental rotary encoder. FIG. 4 is a perspective view showing an embodiment of the mechanical components in the case where the positional relationship between the slit 10a of the rotating slit plate 10 and the fixed slits 12-1, 12-2, and 12-3 in FIG. 3 is schematically shown. FIG. 5 is a diagram showing the signal waveforms obtained from the photocouplers P1, P2, and P3 of FIG. 3, and FIG.
A block diagram showing an embodiment of a circuit that performs position detection based on signals obtained from P2 and P3, FIG. 7 is an operating waveform diagram of the circuit in FIG. 6, and FIG.
Figure 9 is an operation waveform diagram when position detection is performed based on six detection signals, Figure 10 is a diagram showing the operation of the direction identification circuit shown in Figure 9, and Figure 10 is a diagram showing multiple bright and dark patterns in which the photocoupler is shifted in phase by a predetermined angle. FIG. 11 is a perspective view showing a modified example of the photocoupler. 10... Rotating slit plate, 11... Rotating shaft, 1
2... fixed slit plate, P1, P2, P3... photo coupler (D1, D2, D3... light emitting diode, d1, d2, d3... photo diode),
20-1, 20-2...comparison amplifier, 21-1,
21-2...edge trigger pulse oscillator, 24...
... Direction identification circuit, 31, 32, 33 ... Bright and dark pattern row, P31, P32, P33 ... Photocoupler, 40 ... Light emitting element, d40-1, d40-
2, d40-3... Light receiving element.

Claims (1)

【特許請求の範囲】 1 光線を透過する部分と遮断する部分とを所定
のピツチで連続的に形成したパターンと、前記ピ
ツチの1/2(n−1)ずつ位相をずらして光線を受光
す るように前記パターンの連続方向に対し当該パタ
ーンを挟んで各々配置され、前記パターンとの相
対位置が位置検出対象物の移動に応じて変化する
よう配置されたn(n≧3)組のフオトカプラ
と、前記フオトカプラから得られるn本の信号を
位相が隣りあうもの同士(n番目と1番目同士を
除く。)を各々比較してそれらのクロスポイント
を検出する回路手段と、前記回路手段により検出
されたクロスポイントの数を累算し、累算値を前
記位置検出対象物の位置として求める回路手段と
を具えた位置検出装置。 2 光線を透過する部分と遮断する部分とを所定
のピツチで連続的に形成したパターンを前記ピツ
チの1/2(n−1)ずつの位相をずらしてn(n≧3
) 列に並列配列したパターン列と、前記パターン列
の連続方向に対し同じ位置において光線を受光す
るように各パターンを挟んで各々配置され、前記
パターン列との相対位置が位置検出対象物の移動
に応じて変化するように配置されたn組のフオト
カプラと、前記フオトカプラから得られるn本の
信号を位相が隣りあうもの同士(n番目と1番目
同士を除く。)を各々比較してそれらのクロスポ
イントを検出する回路手段と、前記回路手段によ
り検出されたクロスポイントの数を累算し、累算
値を前記位置対象物の位置として求める回路手段
とを具えた位置検出装置。
[Scope of Claims] 1. A pattern in which parts that transmit light and parts that block light are continuously formed at a predetermined pitch, and the light is received with the phase shifted by 1/2 (n-1) of the pitch. n (n≧3) pairs of photocouplers, each arranged with the pattern in between in the continuous direction of the pattern, and arranged so that the relative position with the pattern changes in accordance with the movement of the position detection target. , circuit means for comparing n signals obtained from the photocoupler with adjacent phases (excluding the n-th and 1-th signals) and detecting their cross points; A position detecting device comprising circuit means for accumulating the number of cross points detected and determining the accumulated value as the position of the position detection object. 2. A pattern in which parts that transmit light and parts that block light are continuously formed at a predetermined pitch is shifted by 1/2 (n-1) of the pitch to form a pattern of n (n≧3).
) The pattern rows are arranged in parallel, and the pattern rows are arranged in such a way that each pattern is received at the same position in the continuous direction of the pattern rows, and the relative position with respect to the pattern rows corresponds to the movement of the position detection target. n sets of photocouplers arranged so as to change according to A position detection device comprising circuit means for detecting cross points, and circuit means for accumulating the number of cross points detected by the circuit means and obtaining the accumulated value as the position of the position object.
JP3606681A 1981-03-13 1981-03-13 Method and device for position detection Granted JPS57149914A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3606681A JPS57149914A (en) 1981-03-13 1981-03-13 Method and device for position detection

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3606681A JPS57149914A (en) 1981-03-13 1981-03-13 Method and device for position detection

Publications (2)

Publication Number Publication Date
JPS57149914A JPS57149914A (en) 1982-09-16
JPS6131409B2 true JPS6131409B2 (en) 1986-07-19

Family

ID=12459342

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3606681A Granted JPS57149914A (en) 1981-03-13 1981-03-13 Method and device for position detection

Country Status (1)

Country Link
JP (1) JPS57149914A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61198018A (en) * 1985-02-28 1986-09-02 Nissan Motor Co Ltd Position detecting device
JPS6255511A (en) * 1985-09-05 1987-03-11 Sharp Corp Rotary encoder

Also Published As

Publication number Publication date
JPS57149914A (en) 1982-09-16

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