JPS5822913A - Position detecting scale - Google Patents

Position detecting scale

Info

Publication number
JPS5822913A
JPS5822913A JP12193381A JP12193381A JPS5822913A JP S5822913 A JPS5822913 A JP S5822913A JP 12193381 A JP12193381 A JP 12193381A JP 12193381 A JP12193381 A JP 12193381A JP S5822913 A JPS5822913 A JP S5822913A
Authority
JP
Japan
Prior art keywords
detector
magnetic
magnetoresistive
scale
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
Application number
JP12193381A
Other languages
Japanese (ja)
Inventor
Kengo Takeuchi
武内 研吾
Wataru Nozaki
渉 野崎
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP12193381A priority Critical patent/JPS5822913A/en
Publication of JPS5822913A publication Critical patent/JPS5822913A/en
Pending legal-status Critical Current

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  • Transmission And Conversion Of Sensor Element Output (AREA)

Abstract

PURPOSE:To obtain high output and high sensitivity characteristics, and to exactly prevent generation of an erroneous decision, by constituting a position detecting scale of a magnetic scale and a magnetic resistance detector, and obtaining the result of detection in a digital value. CONSTITUTION:When a magnetic resistance detector 3 of a position detecting scale moves along a magnetic medium 1, a signal S0 is obtained in the detector 3. In this case, to a magnetic resistance element 3a and 3b of the detector, a magnetic field is applied, by one polarization respectively, and amplitude of the signal S0 becomes 2 times of that of a signal obtained by only one element. Also, N groups of detectors 3 are arrayed at a position shifted by (n+1/2N) pitch at the array interval of a magnetized area 2 of the medium 1. In this way, from each detector 3, the signal S0 being distributed to a position shifted by the 1/2N pitch is obtained.

Description

【発明の詳細な説明】 本発明は位置検出スケール、特に磁気媒体K −短間隔
て着磁書き込みされ九着磁領域と磁気抵抗効果を有する
磁気抵抗検出器との配置構造に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a position detection scale, and particularly to an arrangement structure of a magnetic medium K - nine magnetized regions which are magnetized and written at short intervals and a magnetoresistive detector having a magnetoresistive effect.

従来より位置検出スケールとして、例えば等間隔量感を
有する、いわゆるリニアスケールには、電磁誘導方式と
光学式との2種類の方式が提案されている。そして、前
者の電磁誘導方式は、微小なコイルを直線上に配置して
交流を通電しておき、一方、検出器にも同一形状のコイ
ルを配置しておいて、先の直線上に配置したコイルの近
傍を検出器が移動するとき、またはコイルが相互に近接
し九と’IKIK磁誘導によって出力電圧が検出器のコ
イルに励起されるものである。この場合、相互に近接し
たコイルの位IIIIIIl係で検出器に励起される電
圧が変化するので、直線上に配列したコイルの配列ピッ
チ以下の寸法も電気的に読み取ることができゐ。しかし
ながら、検出器に得られた信号はいずれもアナログ信号
であるため、これらの信号はアナログ−デジタル変換器
を介してム、Φ変換させなければN(、vシンやロボッ
トの駆動用信号として適用することかて鎗なかった。一
方、光学式は、例えば光源に対向してガラス板上に一定
間隔で配置されたスリットまたは光遮蔽膜を介して得ラ
レる光パルスの数を計数してこれによって位置を測定す
るものである。しかしながら、このような光学式のリニ
アスケールは、使用する環境によってその性能が著しく
左右される。すなわち、工作機械*に設置して使用する
と、切削油の飛散あるいは蒸気勢の付着によシ光学スリ
ットのガラス面が汚染されて光の透過量が減少して誤動
作の発生の原因となる。また、光源として用いる発光ダ
イオードの特性劣化による絖み取〕誤動作も無視するこ
とができなかった。
BACKGROUND ART Conventionally, two types of systems have been proposed as position detection scales, for example, so-called linear scales that have a sense of equidistant volume: an electromagnetic induction system and an optical system. In the former electromagnetic induction method, a minute coil is placed in a straight line and an alternating current is passed through it, while a coil of the same shape is placed in the detector and placed on the straight line. When the detector moves near the coils, or when the coils are close to each other, an output voltage is excited in the detector coil by magnetic induction. In this case, since the voltage excited in the detector changes depending on the position of the coils that are close to each other, it is possible to electrically read dimensions that are smaller than the arrangement pitch of the coils arranged in a straight line. However, since all the signals obtained by the detector are analog signals, these signals cannot be applied as driving signals for robots or robots unless they are converted to N(, V) via an analog-to-digital converter. On the other hand, the optical method calculates this by counting the number of light pulses obtained through slits or light shielding films placed at regular intervals on a glass plate facing the light source. However, the performance of such optical linear scales is significantly affected by the environment in which they are used.In other words, when installed and used on a machine tool*, there is a risk of cutting oil scattering or The glass surface of the optical slit is contaminated by vapor deposition, reducing the amount of light transmitted and causing malfunctions.Furthermore, malfunctions caused by deterioration of the characteristics of the light emitting diode used as the light source are also ignored. I couldn't.

したがって本発明は、上記従来の欠点を除去し、デジタ
ル信号で位置検出結果が把握でき、かつ使用環境、汚染
11jK対して特性低下の全く発生しない位置検出スケ
ールを提供することを目的としている。
SUMMARY OF THE INVENTION Therefore, it is an object of the present invention to eliminate the above-mentioned drawbacks of the conventional scale, to provide a position detection scale that allows position detection results to be grasped using digital signals, and that does not exhibit any characteristic deterioration in the environment of use or pollution.

このような目的を達成するために本発明は、磁気媒体に
着磁領域が一定間隔で形成された磁気スケールと、この
着磁領域を絖み出す磁気抵抗効果を有する2本の磁気抵
抗検出素子からなる少なくとも1組の磁気抵抗検出器と
で位置検出スケールを構成したものである。
In order to achieve such an object, the present invention provides a magnetic scale in which magnetized regions are formed at regular intervals on a magnetic medium, and two magnetoresistive sensing elements having a magnetoresistive effect that extend the magnetized regions. A position detection scale is constructed with at least one set of magnetoresistive detectors.

以下図面を用いて本発明の実施例を詳細に説明する。Embodiments of the present invention will be described in detail below with reference to the drawings.

第1図は本発明による位置検出スケールの一例を説明す
るための要部平面構成図である。llil図において、
1は磁気媒体であシ、この磁気媒体1には岬間隔に磁極
を着磁して形成され九着磁領域2が設けられて磁気スケ
ールが構成されている。また、この磁気媒体1o11気
スケール近傍には磁気抵抗効果を有する磁気抵抗検出器
3が近接配置され、この磁気抵抗検出器3は磁気抵抗効
果を有する2つの磁気抵抗素子3m、3bが、上記磁気
媒体1に着磁され九着磁領域20間隔On(正の整数)
 + x7意ピッチの間隔だけ離間して直ガ接続して配
置されている。なお、3Cは共通電極、3d、3・、3
fは信号取多出し用端子である。
FIG. 1 is a plan configuration diagram of main parts for explaining an example of a position detection scale according to the present invention. In the llil diagram,
Reference numeral 1 denotes a magnetic medium, and this magnetic medium 1 is formed by magnetizing magnetic poles at cape intervals, and nine magnetized regions 2 are provided to constitute a magnetic scale. Further, a magnetoresistive detector 3 having a magnetoresistive effect is placed close to the magnetic medium 1o11 scale, and the magnetoresistive detector 3 has two magnetoresistive elements 3m and 3b having a magnetoresistive effect, which are connected to the magnetic Magnetized on medium 1, 9 magnetized regions 20 intervals On (positive integer)
+x7 pitches apart and directly connected. Note that 3C is a common electrode, 3d, 3., 3
f is a signal output terminal.

このように構成された位置検出スケールにおいて、磁気
抵抗検出器3が磁気媒体1に沿って移動すると、磁気抵
抗検出器3が第2図で示した等価回路を有していること
から、第3図に示したよりな信号が得られる。この場合
、磁気抵抗検出器3の磁気抵抗素子3aと3bには片方
ずつ磁場が印加されるので、第3図に示した信号波形8
oの振幅Fi1個の磁気抵抗検出素子のみで得られる信
号の2倍となっている。
In the position detection scale configured in this way, when the magnetoresistive detector 3 moves along the magnetic medium 1, since the magnetoresistive detector 3 has the equivalent circuit shown in FIG. The signal shown in the figure is obtained. In this case, since a magnetic field is applied to each of the magnetoresistive elements 3a and 3b of the magnetoresistive detector 3, the signal waveform 8 shown in FIG.
The amplitude Fi of o is twice that of the signal obtained with only one magnetoresistive sensing element.

このような基本構成の磁気抵抗検出器3を複数組配列し
た場合を考えてみると、いIN組の磁気抵抗検出器3を
上記磁気媒体10着磁領域3の配列間隔を等分する位置
に配置する。すなわち、N組の磁気抵抗検出器3が着磁
領域2の配列間隔の(m+”/m)ピッチずれた位置に
各々を配列する。
Considering the case where multiple sets of magnetoresistive detectors 3 having such a basic configuration are arranged, the IN set of magnetoresistive detectors 3 are placed at positions that equally divide the arrangement interval of the magnetized regions 3 of the magnetic medium 10. Deploy. That is, N sets of magnetoresistive detectors 3 are arranged at positions shifted by (m+''/m) pitch from the arrangement interval of the magnetized regions 2.

この場合、nは正の整数である。In this case, n is a positive integer.

このような構成によると、N組の各磁気抵抗検出器3か
らは第4図に示したような信号波形s1゜Bz、S8.
g4pBm#得らtL、第3EK示L*(11)波形s
O鱒” ”/2Nピッチずつずれ九位置K)1個の波形
が分布して得られる。ここで5組の磁気抵抗検出器3を
配置した場合KFiN=5となシ、”/2N−1/1・
となる。すなわち、5組の磁気抵抗検出器3を使用する
と、磁気媒体1に着磁し九間隔のV!・の寸法まで読み
とることができる。
According to such a configuration, each of the N sets of magnetoresistive detectors 3 outputs signal waveforms s1°Bz, S8 .
g4pBm# obtained tL, 3rd EK indication L*(11) waveform s
K) One waveform is obtained with a distribution of 9 positions K) shifted by O trout ""/2N pitch. Here, if five sets of magnetoresistive detectors 3 are arranged, KFiN=5, "/2N-1/1・
becomes. That is, when five sets of magnetoresistive detectors 3 are used, the magnetic medium 1 is magnetized and the V!・Can read up to the dimensions.

#!5図は第4図に示した信号波形の微細読み取り部分
をさらに細かく読み出すための方法を説明する図である
。同図において、上記磁気抵抗検出器3(図示せず)の
2組から信号波形9r、S!があるとき、この信号波形
S1とBzとの間に存在するAXの分解能以下の位置を
槻定するKは、X点における信号波形S1と82の波高
値を読むことにより簡単な計算で算出できる。すなわち
、同図に示したように信号波形gx、g2の!軸上の交
点をそれぞれAA、B点とし、その求める点をX点とす
る。また、信号波形S1のB、a、X点からの垂直線上
の交点をそれぞれ0点、D点とし、信号波形S冨のX点
からの一直線上の交点を9点とする。この場合、信号波
形5ttstともAAから各X、B、C、D、1点まで
の距離範囲をリニアと仮定すると、そのとき、 が近似的に成立するので求めるX点の位置、すなわちA
Xは、 DX AX=AilX−・曇・・・・・(2)B となり、A B = 1/2Nであるので、磁気媒体の
着磁間隔を便宜上1とすると、1点とB点の信号波形S
1と82の波高値を求めるととKよシ、計算で求めるこ
とができる。しかしこの方法によると、時間的にタイミ
ングが異なる2点の1点と1点とで信号波形S1と8!
とを測定する必要がある。
#! FIG. 5 is a diagram illustrating a method for further finely reading out the finely read portion of the signal waveform shown in FIG. 4. In the figure, signal waveforms 9r, S! from two sets of the magnetoresistive detectors 3 (not shown) are shown. When there is, K, which determines the position below the resolution of AX that exists between signal waveforms S1 and Bz, can be calculated by simple calculation by reading the peak values of signal waveforms S1 and 82 at point X. . That is, as shown in the figure, the signal waveforms gx, g2! Let the intersection points on the axes be points AA and B, respectively, and let the desired point be point X. Further, the intersections on the vertical lines from points B, a, and X of the signal waveform S1 are respectively set as 0 point and point D, and the intersections on a straight line from the point X of the signal waveform S are set as 9 points. In this case, assuming that the distance range from AA to each point X, B, C, and D is linear for the signal waveform 5ttst, then the following approximately holds true, so the position of the X point to be found, that is, A
X is DX AX = Ail Waveform S
The peak values of 1 and 82 can be found by calculation. However, according to this method, the signal waveforms S1 and 8! at two points with different timings, 1 point and 1 point!
It is necessary to measure.

一方、測定を容易とするために同図において近似的KC
B=D]Cとす、6 ト1(21式カラI     D
X AX#−・□―・・・−−@(31 2M   DI とな抄、同一の時刻に信号波形s1と82の波高値を測
定することにより、1点を簡単に求めることができる。
On the other hand, in order to facilitate measurement, approximate KC
B=D] C, 6 To1 (21 type Kara ID
X AX#-・□----@(31 2M DI Tona-sho, one point can be easily determined by measuring the peak values of signal waveforms s1 and 82 at the same time.

そして、この測定結果は通常知られているようKA/D
変換器とマイコンとを併用することによって、瞬時的に
計算処理することができる。
This measurement result is KA/D as commonly known.
By using a converter and a microcomputer together, calculations can be processed instantaneously.

例えば、N=5組の磁気抵抗検出器3を用いるととKよ
シ、着磁領域20間隔の1/2Nの精度で測定すると、
測定精度が1桁向上し、さらに2つの信号波形の中間点
を求める手法も併用すると、最初O着磁間隔1イ01度
まで容易に精読を向上させることができる。例えば、上
記磁気媒体1に約0D5−間隔で磁気領域2を着磁した
ときは、約o、oos■の測定精度も容易に得ることが
できる。
For example, if N = 5 sets of magnetoresistive detectors 3 are used, and K is measured with an accuracy of 1/2N of the spacing of the magnetized regions 20,
If the measurement accuracy is improved by one order of magnitude and a method for finding the midpoint between two signal waveforms is also used, the initial O magnetization interval can be easily improved to 101 degrees. For example, when the magnetic regions 2 are magnetized on the magnetic medium 1 at intervals of about 0D5, it is possible to easily obtain a measurement accuracy of about o, oos.

力お、上記実施例においては、勢間隔目盛を有するリニ
アスケールを用いた場合について説明したが、本発明は
これに限定されるものではなく、磁気エンコーダスケー
ル、−長月のりニアエンコーダ、角度同転エンコーダお
よび速度回転エンコーダに適用しても前述と同様の効果
が得られる。
In addition, in the above embodiment, a linear scale having an interval scale was used, but the present invention is not limited to this. Even when applied to a rotary encoder and a speed rotary encoder, the same effects as described above can be obtained.

以上a明したように本発vi4によれば、デジタル信号
で位置検出結果が得られかつ使用環境、汚染等に対して
特性劣下が全く発生しない高出力、高感IIL%性が得
られるのて、誤判定の発生を確実に肪止することができ
る 1九、磁気抵抗検出器を複数個用いたことによって
、測定精度を向上させ、さらに2つの信号を解析するこ
とKよって、よシ欄定精度の高い位置情報を読み出すこ
とができるなどの優れた効果が得られる。
As explained above, according to the present invention VI4, position detection results can be obtained with digital signals, and high output and high sensitivity IIL% can be obtained with no characteristic deterioration due to the usage environment, pollution, etc. 19. By using multiple magnetoresistive detectors, measurement accuracy can be improved, and by analyzing two signals, it is possible to reliably prevent false judgments. Excellent effects such as being able to read position information with high accuracy can be obtained.

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

籐1図は本発1による位置検出スケールの一例を説明す
る要部千両構成図、第211は第1図に示す磁気抵抗検
出器の等個aSIII、第3WAは第2図で示し九磁気
抵抗検出器で得られる信号の波形図、第4図は複数組の
磁気抵抗検出器を用い九ときの出力信号波el1%Ia
s図は2つの出力信号波形図から正確な位置を求めゐ説
−図である。 1・・・・磁気媒体、2・・・・着磁領域、3・・・・
磁気抵抗検出器、Sm、3b・・・・磁気抵抗素子、3
c・・・・共通電極、8d、3・、$f・・・・信号域
)出し用端子。 第1図 フ 第2図 第3図
Figure 1 is a configuration diagram of the main parts explaining an example of the position detection scale according to the present invention 1, No. 211 is the equal piece aSIII of the magnetoresistive detector shown in Figure 1, and 3rd WA is the 9 magnetoresistive detector shown in Figure 2. The waveform diagram of the signal obtained by the detector, Figure 4, shows the output signal wave el1%Ia when using multiple sets of magnetoresistive detectors.
The s diagram is a diagram showing how to find an accurate position from two output signal waveform diagrams. 1... Magnetic medium, 2... Magnetized area, 3...
Magnetoresistive detector, Sm, 3b... Magnetoresistive element, 3
c...Common electrode, 8d, 3..., $f...Signal range) output terminal. Figure 1 Figure 2 Figure 3

Claims (1)

【特許請求の範囲】[Claims] (1)磁気媒体に一定の間隔で磁極を着磁し九着磁領域
が形成された磁気スケールと、前記磁気スケールの着磁
領域を読み取る磁気抵抗効果を有する2つの磁気抵抗検
出素子からなる少なくとも1組の磁気抵抗検出器とを備
え、前記磁気抵抗検出器は、前記2個の磁気抵抗検出素
子を、前記磁気スケールの着磁領域間間隔のn(正の整
数) + 171ピツチの位置で配列し直列接続して構
成したことを4+11とする位置検出スケール。 (21前記W&磁気抵抗検出器N組設けたとき、該N組
の各々はn(正の整数) + 1/!Nピツチずつずれ
た位置に配置したことを特徴とする特許請求の範H第1
項記載の位置検出スケール。
(1) At least a magnetic scale comprising nine magnetized regions formed by magnetizing magnetic poles at regular intervals on a magnetic medium, and two magnetoresistive detection elements having a magnetoresistive effect for reading the magnetized regions of the magnetic scale. a set of magnetoresistive detectors, and the magnetoresistive detector is arranged such that the two magnetoresistive detection elements are arranged at positions n (positive integer) + 171 pitches of the distance between the magnetized regions of the magnetic scale. A 4+11 position detection scale configured by arranging and connecting in series. (21) When N sets of the W&magnetic resistance detectors are provided, each of the N sets is arranged at a position shifted by n (positive integer) + 1/!N pitches. 1
Position detection scale described in section.
JP12193381A 1981-08-05 1981-08-05 Position detecting scale Pending JPS5822913A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12193381A JPS5822913A (en) 1981-08-05 1981-08-05 Position detecting scale

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12193381A JPS5822913A (en) 1981-08-05 1981-08-05 Position detecting scale

Publications (1)

Publication Number Publication Date
JPS5822913A true JPS5822913A (en) 1983-02-10

Family

ID=14823518

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12193381A Pending JPS5822913A (en) 1981-08-05 1981-08-05 Position detecting scale

Country Status (1)

Country Link
JP (1) JPS5822913A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6073415A (en) * 1983-09-30 1985-04-25 Tdk Corp Distance sensor
JPS60193771U (en) * 1984-05-31 1985-12-23 オンキヨー株式会社 Speaker unit mounting structure
JPS61197782U (en) * 1985-05-31 1986-12-10
JPS61197783U (en) * 1985-05-31 1986-12-10

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6073415A (en) * 1983-09-30 1985-04-25 Tdk Corp Distance sensor
JPS60193771U (en) * 1984-05-31 1985-12-23 オンキヨー株式会社 Speaker unit mounting structure
JPS61197782U (en) * 1985-05-31 1986-12-10
JPS61197783U (en) * 1985-05-31 1986-12-10
JPH0513112Y2 (en) * 1985-05-31 1993-04-06

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