JPS5843684B2 - Genten Shingo Kenshiyutsuhouhou - Google Patents

Genten Shingo Kenshiyutsuhouhou

Info

Publication number
JPS5843684B2
JPS5843684B2 JP13773875A JP13773875A JPS5843684B2 JP S5843684 B2 JPS5843684 B2 JP S5843684B2 JP 13773875 A JP13773875 A JP 13773875A JP 13773875 A JP13773875 A JP 13773875A JP S5843684 B2 JPS5843684 B2 JP S5843684B2
Authority
JP
Japan
Prior art keywords
pulse
origin
signal
signals
counter
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
JP13773875A
Other languages
Japanese (ja)
Other versions
JPS5262046A (en
Inventor
淑孝 柳尾
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.)
Nikon Corp
Original Assignee
Nippon Kogaku KK
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 Nippon Kogaku KK filed Critical Nippon Kogaku KK
Priority to JP13773875A priority Critical patent/JPS5843684B2/en
Publication of JPS5262046A publication Critical patent/JPS5262046A/en
Publication of JPS5843684B2 publication Critical patent/JPS5843684B2/en
Expired legal-status Critical Current

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  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Length Measuring Devices With Unspecified Measuring Means (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)

Description

【発明の詳細な説明】 本発明は、長さや角度の増分方式の測定装置における原
点を一時的に求める原点信号検出方法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an origin signal detection method for temporarily determining the origin in an incremental length or angle measuring device.

増分方式のエンコーダからの出力信号は90゜の位相差
をもって現われる(第1図aの信号A。
The output signals from the incremental encoder appear with a phase difference of 90° (signal A in FIG. 1a).

B)。B).

この信号A、Bの矩形波出力は第1図す。Cに示す通り
である。
The rectangular wave outputs of the signals A and B are shown in FIG. As shown in C.

順方向に計数した際のパルス及び逆方向計数のパルスを
それぞれ第1図d。
The pulses when counting in the forward direction and the pulses when counting in the backward direction are shown in FIG. 1d, respectively.

eに示す。Shown in e.

−1,0、+1・・・・・・等は任意のP点で零リセッ
トしたときのカウンターの表示である。
-1, 0, +1, etc. are the counter displays when the counter is reset to zero at any P point.

このディジタル増分方式では、任意の位置でゼロリセッ
トが出来る。
This digital incremental method allows zero reset at any position.

しかし、ディジタルエラーが避けられない;原点が決っ
ていないために精度測定の基準がない、あるいは精度よ
く原点に復帰させることができない、等の欠点がある。
However, digital errors are unavoidable; since the origin is not determined, there is no standard for accuracy measurement, or it is not possible to accurately return to the origin.

すなわち、第1図の任意のP点でゼロリセットしたとす
ると、順方向に計数する場合を考えると第1図dのP、
Q間か1デイジツト分の長さより短かいにもかかわらず
Q点を過ぎると「+1」とカウンターに表示してしまう
That is, if we reset to zero at an arbitrary point P in Figure 1, then when counting in the forward direction, P in Figure 1 d,
Even though the length is shorter than the Q interval or one digit, when the Q point is passed, "+1" is displayed on the counter.

逆方向に計数する場合についても同様に、このディジタ
ルエラーが発生する。
This digital error also occurs when counting in the opposite direction.

また、上記のような信号を出力する増分方式エンコーダ
の再現性の測定を行う場合、正確に原点に復帰させよう
とすると、P点を測定の基準として検出する装置(例え
は、電子マイクロメータやリミットスイッチあるいは第
1図のような原点信号を発生させるためにエンコーダの
スケール上の1個所のみから信号を出力するための信号
系)を別に用意しなければならない。
In addition, when measuring the repeatability of an incremental encoder that outputs a signal like the one above, if you want to accurately return to the origin, it is necessary to use a device that detects point P as a measurement reference (for example, an electronic micrometer or A limit switch or a signal system (signal system for outputting a signal from only one point on the scale of the encoder) must be separately prepared in order to generate the origin signal as shown in FIG.

また、累積精度を測定する場合でも、nディジット(n
は整数)だけの精度を他の測長装置で測定しようとする
と1+n“のカウンターの表示を示す範囲は1デイジツ
トたけあるので、正確にnディジットの精度測定が行な
えないことになる。
Also, even when measuring cumulative accuracy, n digits (n
If an attempt is made to measure the precision of only n digits with another length measuring device, the range in which the counter displays 1+n'' is 1 digit long, so it will not be possible to accurately measure the precision of n digits.

本発明は、以上のような従来の増分方式のエンコーダに
避けられない欠点を解決する原点信号検出方法の提供を
目的とする。
SUMMARY OF THE INVENTION An object of the present invention is to provide an origin signal detection method that solves the above-mentioned drawbacks of conventional incremental encoders.

以下に、0°、900の正弦波2信号を出力する増分方
式のエンコーダを例にとって本発明による原点信号検出
回路の実施例を説明する。
An embodiment of the origin signal detection circuit according to the present invention will be described below, taking as an example an incremental encoder that outputs two 0° and 900 sine wave signals.

第2図では、O0相信号と90°相信号をそれぞれ抵抗
2,3を通して入れこの両抵抗の接続点に加算増幅器1
と抵抗4とを並列接続する。
In Figure 2, the O0 phase signal and the 90° phase signal are passed through resistors 2 and 3, respectively, and a summing amplifier 1 is connected to the connection point between these two resistors.
and resistor 4 are connected in parallel.

これによりベクトル台底した信号例えば45° (又は
225° )の正弦波信号を出力する。
This outputs a signal with a vector base, for example, a 45° (or 225°) sine wave signal.

第3図では、0°相信号と90°相信号をそれぞれバッ
ファアンプ5,6を通して入れ、この両バッファアンプ
の出力信号を直列接続した抵抗7゜8に入力して両抵抗
の接続点からベクトル合成した信号例えば45°の正弦
波信号をとり出している。
In Figure 3, the 0° phase signal and the 90° phase signal are input through buffer amplifiers 5 and 6, respectively, and the output signals of both buffer amplifiers are input to a resistor 7°8 connected in series, and a vector is generated from the connection point of both resistors. A synthesized signal, for example a 45° sine wave signal, is extracted.

第4図において、aは、0090° 45゜の正弦波信
号を、bはO0信号の矩形波、Cは45°の矩形波、d
は90°の矩形波、eは周知の方法によって計数した9
0°矩形波のカフントパルス列、fは周知の方法によっ
て計数した45゜矩形波の合成位相パルス列(図には理
解を容易にするため矩形波の立下り点でパルスを発生さ
せているが立上り点でも同様な作動が可能なことは容易
に理解できる。
In Figure 4, a is a 0090° 45° sine wave signal, b is a rectangular wave of the O0 signal, C is a 45° rectangular wave, and d
is a 90° square wave, and e is 9 calculated by a well-known method.
Cafund pulse train of 0° square wave, f is composite phase pulse train of 45° square wave counted by a well-known method (in the figure, a pulse is generated at the falling point of the square wave for ease of understanding, but the pulse is generated at the falling point of the rectangular wave, but the rising It is easy to understand that a similar operation is also possible at points.

)gはカウンター表示状態″0“を検出したゼロ信号、
hは原点パルスを示す。
) g is the zero signal that detected the counter display state "0",
h indicates the origin pulse.

原点パルスhはパルス列fとカウンタのO状態を示す信
号gとの論理積として得られているものである。
The origin pulse h is obtained as the logical product of the pulse train f and the signal g indicating the O state of the counter.

本発明では原点パルスhをエンコーダ装置の基準原点と
する。
In the present invention, the origin pulse h is used as the reference origin of the encoder device.

以上に本発明の詳細な説明する。The present invention will now be described in detail.

エンコーダ装置のカウンターはパルス列eを計数するも
のであるが操作者によりゼロリセットされうる。
The counter of the encoder device counts the pulse train e and can be reset to zero by the operator.

今、エンコーダがp点に対応する位置にあるとき、カウ
ンターがリセットされたとする。
Suppose now that the counter is reset when the encoder is at a position corresponding to point p.

この位置からエンコーダを第4図の右方向に動かしてい
ってパルス列eの最初に来るパルスの立上り(パルスの
左エツジ)でカウンタはO状態でなくなる。
As the encoder is moved to the right in FIG. 4 from this position, the counter is no longer in the O state at the rising edge of the first pulse (left edge of the pulse) of the pulse train e.

第4図の例ではカウンタが0状態でなくなる前にパルス
列fのパルスがないからこの間でパルス列fと信号gと
の論理積出力はなく、従ってエンコーダの右方向へ動か
すことにより原点パルスhは生じない。
In the example of Fig. 4, there is no pulse of the pulse train f before the counter goes to the 0 state, so there is no AND output of the pulse train f and the signal g during this time, and therefore, by moving the encoder to the right, the origin pulse h is generated. do not have.

この場合次に操作者はエンコーダを左方向へ動かす。In this case, the operator then moves the encoder to the left.

カウンタはパルス列のp点から左側の最初のパルスeの
立上り(今度はパルスの右エツジ)でO状態でなくなる
The counter ceases to be in the O state at the rising edge of the first pulse e to the left of point p in the pulse train (this time at the right edge of the pulse).

第4図の例ではカウンタが0状態でなくなる迄にパルス
fがあるから原点パルスhが生ずる。
In the example shown in FIG. 4, since there is a pulse f until the counter is no longer in the 0 state, an origin pulse h is generated.

操作者は原点パルスhの生じた位置を測定基準とする。The operator uses the position where the origin pulse h occurs as a measurement reference.

測定用パルスとしてパルス列fを用いれば、パルス列f
の生ずる位置は原点パルスの生ずる位置から1デイジツ
ト毎にあるから前述のディジットエラーが生じない。
If the pulse train f is used as the measurement pulse, the pulse train f
Since the positions where the digits are generated are one digit apart from the position where the origin pulse is generated, the above-mentioned digit error does not occur.

計測用パルスをパルス列e又は分解能を上ゆるためOo
と90°の立上りと立下りにおけるパルス列を用い原点
パルス位置を測定基準としても誤差を防ぐことはできる
Set the measurement pulse to pulse train e or Oo to increase the resolution.
Errors can also be prevented by using a pulse train at the rise and fall of 90° and using the origin pulse position as a measurement standard.

例数ならば原点パルス位置とそれらの計測用パルス列の
位置の関係は予じめ分かつているから、後にこれを補償
することができるからである。
This is because, in the case of examples, the relationship between the origin pulse position and the positions of these measurement pulse trains is known in advance, and this can be compensated for later.

以上の如く構成した本発明によれば、エンコーダ装置の
カウンターをゼロリセットした後、原点パルスの出る位
置を測定基準とすれば、他に原点を定める装置がなくと
も正確に原点が決定される。
According to the present invention configured as described above, after the counter of the encoder device is reset to zero, if the position where the origin pulse appears is used as the measurement standard, the origin can be accurately determined even without any other device for determining the origin.

このため工作機械等において加工中に原点へ戻す必要の
ある時はカウンタの0表示までもどしてこの原点パルス
の発生する位置を得れば正確に再現性をチェックするこ
とができる。
Therefore, when it is necessary to return to the origin during machining in a machine tool or the like, reproducibility can be accurately checked by returning the counter to 0 and obtaining the position where this origin pulse is generated.

特に、本発明はディジタル秤や液面測定装置などのよう
に容易に原点を変える必要があり、かつ精度の検定が重
要な装置においては本装置による原点を使用すれば有効
である。
In particular, the present invention is effective if the origin provided by this device is used in devices such as digital scales and liquid level measuring devices in which the origin needs to be easily changed and accuracy verification is important.

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

第1図は増分方式エンコーダの信号の説明図、第2図は
本発明の装置に使用する位相合成回路の説明図、第3図
は本発明の装置に使用する別の位相合成回路の説明図、
第4図は原点信号波形図である。 (主要部分の符号の説明つ 1・・・・・・増幅器、2,3,4・・・・・・抵抗、
5,6・・・・・・バッファアンプ、7,8・・・・・
・抵抗。
Fig. 1 is an explanatory diagram of signals of an incremental encoder, Fig. 2 is an explanatory diagram of a phase synthesis circuit used in the device of the present invention, and Fig. 3 is an explanatory diagram of another phase synthesis circuit used in the device of the present invention. ,
FIG. 4 is an origin signal waveform diagram. (Explanation of symbols of main parts 1...Amplifier, 2, 3, 4...Resistance,
5, 6...Buffer amplifier, 7, 8...
·resistance.

Claims (1)

【特許請求の範囲】[Claims] 1 長さや角度の増分方式のエンコーダ測定装置から2
つの位相差の異る信号を出力し、該2信号を受けて可逆
計数し、前記2信号を位相合成し、該位相合成された信
号をパルス化し、該パルス列と前記計数のゼロ状態との
論理積をとり、該論理積により得られた単一パルスを測
定基準の原点信号とする原点信号検出方法。
1. From incremental length and angle encoder measuring devices to 2.
output two signals with different phase differences, receive the two signals and perform reversible counting, phase synthesize the two signals, pulse the phase synthesized signal, and logic between the pulse train and the zero state of the count. An origin signal detection method in which a product is calculated and a single pulse obtained by the logical product is used as a measurement reference origin signal.
JP13773875A 1975-11-18 1975-11-18 Genten Shingo Kenshiyutsuhouhou Expired JPS5843684B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13773875A JPS5843684B2 (en) 1975-11-18 1975-11-18 Genten Shingo Kenshiyutsuhouhou

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13773875A JPS5843684B2 (en) 1975-11-18 1975-11-18 Genten Shingo Kenshiyutsuhouhou

Publications (2)

Publication Number Publication Date
JPS5262046A JPS5262046A (en) 1977-05-23
JPS5843684B2 true JPS5843684B2 (en) 1983-09-28

Family

ID=15205665

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13773875A Expired JPS5843684B2 (en) 1975-11-18 1975-11-18 Genten Shingo Kenshiyutsuhouhou

Country Status (1)

Country Link
JP (1) JPS5843684B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0238613Y2 (en) * 1984-12-24 1990-10-17

Also Published As

Publication number Publication date
JPS5262046A (en) 1977-05-23

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