JPS6262215A - Encoder apparatus - Google Patents

Encoder apparatus

Info

Publication number
JPS6262215A
JPS6262215A JP20161885A JP20161885A JPS6262215A JP S6262215 A JPS6262215 A JP S6262215A JP 20161885 A JP20161885 A JP 20161885A JP 20161885 A JP20161885 A JP 20161885A JP S6262215 A JPS6262215 A JP S6262215A
Authority
JP
Japan
Prior art keywords
magnetized
phase
range
reference position
magnetic flux
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
JP20161885A
Other languages
Japanese (ja)
Other versions
JPH0711429B2 (en
Inventor
Hiroichi Goto
博一 後藤
Shuzo Abiko
安彦 修三
Masakazu Kuhara
正和 久原
Hisanori Hayashi
林 久範
Takeshi Osato
毅 大里
Hideto Sano
佐野 秀人
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.)
Canon Electronics Inc
Original Assignee
Canon Electronics Inc
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 Canon Electronics Inc filed Critical Canon Electronics Inc
Priority to JP60201618A priority Critical patent/JPH0711429B2/en
Priority to US06/893,215 priority patent/US4785241A/en
Publication of JPS6262215A publication Critical patent/JPS6262215A/en
Publication of JPH0711429B2 publication Critical patent/JPH0711429B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To minimize a detection error with narrowed expanse of magnetic flux for the reference position detection, by installing, before and behind a magnetized range for the reference position detection, a magnetized range of shorter recording wave length than this magnetized range. CONSTITUTION:An incremental phase 7 of a rotor is provided with the usual magnetized pattern 5, and the magnetized pattern 5 as a index phase 6 is provided with magnetized range 12 of a single magnetic field given the same recording wave length as the phase 7 in the reference position and with a magnetized range 13 given a shorter recording wave length before and after of it. As the same poles of each range 13 are arranged before and behind N and S poles of the range 12, a magnetic flux 14 of the range 12 becomes a distribution of small expanses in the same order as the magnetic flux of the phase 7. Consequently, a detecting output wave length of the phase 6 becomes of the same order of the pulse width as the output wave length of the phase 7 thus preventing the reference position detecting error.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明はエンコーダ装置、特に磁気センサを用いて被検
出体の基準位置を検出するエンコーダ装置に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an encoder device, and particularly to an encoder device that detects a reference position of a detected object using a magnetic sensor.

[従来の技術] 磁気抵抗効果素子(以下MR素子という)は素子の抵抗
変化により印加磁界の変化を検出する。
[Prior Art] A magnetoresistive element (hereinafter referred to as an MR element) detects a change in an applied magnetic field based on a change in resistance of the element.

従って各種のエンコーダの検出手段に利用する場合、被
検出体は永久磁石などの磁界発生手段を用いればよい。
Therefore, when used as a detection means for various encoders, a magnetic field generating means such as a permanent magnet may be used as the object to be detected.

これに対して所謂光学式のエンコーダ装置に於いてはL
EDなどの光源に対する電源が必要で、また検出手段と
しては消耗しうる光源が不可欠なフォトセンサなどを用
いている。そのためMR素子を用いた磁気式エンコーダ
は光学式エンコーダに比べても構成が簡単で耐久性にも
優れたものとなる。
On the other hand, in the so-called optical encoder device, L
A power source is required for a light source such as an ED, and a photosensor or the like that requires a consumable light source is used as a detection means. Therefore, a magnetic encoder using an MR element has a simpler structure and superior durability than an optical encoder.

第4図は従来のMR素子を用いたロータリーエンコーダ
を示している。第4図において、符号lはロータでその
円周面に磁化パターン5が形成されている。この磁化パ
ターン5はロータの回転方向9回転角度9回転速度など
の検出のためのインクリメンタル相7、及び検出に伴な
うロータに基準位置の検出のためのインデックス相6を
形成している。そして各相に近接して基板2上に形成し
たMR素子3.4を対向配置してロータリーエンコーダ
が構成されている。
FIG. 4 shows a rotary encoder using a conventional MR element. In FIG. 4, reference numeral 1 denotes a rotor having a magnetization pattern 5 formed on its circumferential surface. This magnetization pattern 5 forms an incremental phase 7 for detecting the rotor's rotation direction, rotation angle, rotation speed, etc., and an index phase 6 for detecting a reference position of the rotor accompanying the detection. A rotary encoder is constructed by arranging MR elements 3.4 formed on the substrate 2 close to each phase and facing each other.

ここで、MR素子3(4)の動作原理につき説明する。Here, the operating principle of the MR element 3 (4) will be explained.

MR素子は基板2にストライブ状番こFe−Ni 、N
i−Coなどの合金を薄膜形成することにより構成され
る。
The MR element has a striped number plate on the substrate 2 made of Fe-Ni, N
It is constructed by forming a thin film of an alloy such as i-Co.

一般にMR素子の抵抗変化率は素子に流れる電流と平行
に磁界を加えた時の抵抗Raと、電流と直角方向に磁界
を加えた時の抵抗Rhの関数として示され、実際の磁化
方向と電流のなす角をθとすると、この角度に関して抵
抗R(θ)はR(θ) =Ra sin 2θ+Rbc
os 2θと示される。
In general, the resistance change rate of an MR element is expressed as a function of resistance Ra when a magnetic field is applied parallel to the current flowing through the element, and resistance Rh when a magnetic field is applied perpendicular to the current, and is a function of the actual magnetization direction and current. When the angle formed by
It is denoted as os 2θ.

エンコーダ用としては、MR素子にl軸異方性を持たせ
、素子に流す電流Iと直角方向に磁界Hを印加し、MR
素子3の抵抗変化として磁界の強弱を取り出すようにし
ている。
For encoders, the MR element is made to have l-axis anisotropy, and a magnetic field H is applied in a direction perpendicular to the current I flowing through the element.
The strength of the magnetic field is extracted as a resistance change of the element 3.

[発明が解決しようとする問題点] 一方、第4図のインデックス相6.インクリメンタル相
7の磁束の分布は第5図のようになる。
[Problems to be Solved by the Invention] On the other hand, index phase 6 in FIG. The distribution of magnetic flux in the incremental phase 7 is as shown in FIG.

インクリメンタル相7では連続的に反転磁化されている
ため、すぐ隣りに同じ極があり、互いの反発により磁束
10が狭くなっているが、インデックス相6ではS及び
N極の1つの磁化パターンしか設けていないので磁束1
1が広がってしまう。
In the incremental phase 7, since the magnetization is continuously reversed, there are the same poles right next to each other, and the magnetic flux 10 is narrowed due to mutual repulsion, but in the index phase 6, only one magnetization pattern of S and N poles is provided. Since the magnetic flux is not 1
1 will spread.

従って、前述のような構成を有するMR素子3.4を用
いて得られる検出信号は第6図のようになる。
Therefore, the detection signal obtained using the MR element 3.4 having the above-mentioned configuration is as shown in FIG.

第6図において、符号AはMR素子4の再生出力に基づ
く検出信号、符号CはMR素子3の再生出力に基づく検
出信号である。インデックス相用のMR素子3による検
出信号波形Cがこのように広いと、ロータlの回転方向
によりインデックスパルスの検出タイミングに誤差が生
じてしまう問題がある。
In FIG. 6, symbol A is a detection signal based on the reproduced output of the MR element 4, and symbol C is a detection signal based on the reproduced output of the MR element 3. If the detection signal waveform C by the MR element 3 for the index phase is thus wide, there is a problem that an error occurs in the detection timing of the index pulse depending on the rotational direction of the rotor l.

インデックス相の出力波形は、第6図符号Bのようにイ
ンクリメンタル相の分解能と同程度、あるいはさらにそ
れより狭いパルスとなるのが好ましい。
It is preferable that the output waveform of the index phase is a pulse having a resolution similar to that of the incremental phase, or even narrower than that of the incremental phase, as shown by reference numeral B in FIG.

[問題点を解決するための手段] 以上の問題を解決するため1本発明においては、基準位
置検出用磁化領域の前後にこの磁化領域よりも記録波長
の短い磁化領域を設ける構成を採用した。
[Means for Solving the Problems] In order to solve the above problems, the present invention employs a configuration in which magnetized regions having a recording wavelength shorter than that of the magnetized regions are provided before and after the magnetized region for detecting the reference position.

[作 用] 以上のような構成により、基準位置検出用磁化領域の磁
束が、となり合った記録波長の短い磁化領域の反発によ
り被検出体の移動方向へ広がらなくなり、検出パルスの
幅をより狭くできるので、前述のような検出誤差を減少
できる。また、記録波長の短い磁化部分はその短波長ゆ
えに磁束の飛び出しが小さいので、磁気センサとのスペ
ーシングロスにより磁気センサに検出されにくく、誤検
出を生じることがない。
[Function] With the above configuration, the magnetic flux of the magnetized region for reference position detection is prevented from spreading in the moving direction of the detected object due to the repulsion of the adjacent magnetized regions with short recording wavelengths, and the width of the detection pulse is made narrower. Therefore, the above-mentioned detection error can be reduced. Furthermore, since the magnetized portion with a short recording wavelength has a small amount of magnetic flux protruding due to its short wavelength, it is difficult to be detected by the magnetic sensor due to spacing loss with the magnetic sensor, and erroneous detection does not occur.

[実施例] 以下、図面に示す実施例に基づき、本発明の詳細な説明
する。
[Example] Hereinafter, the present invention will be described in detail based on the example shown in the drawings.

第1図は本発明によるロータリーエンコーダのロータ部
分を示している。本実施例において、ロータlのインク
リメンタル相7は第4図の従来例と同様の磁化パターン
5となっている。インデックス相4としての磁化パター
ン5は基準位置にインクリメンタル相7と同一の記録波
長を有する1磁界による磁化領域12と、その前後に連
続して設けたより小さな記録波長を有する磁化領域13
から構成されている。
FIG. 1 shows the rotor portion of a rotary encoder according to the invention. In this embodiment, the incremental phase 7 of the rotor I has a magnetization pattern 5 similar to that of the conventional example shown in FIG. The magnetization pattern 5 as the index phase 4 includes a magnetization region 12 at a reference position caused by one magnetic field having the same recording wavelength as that of the incremental phase 7, and a magnetization region 13 having a smaller recording wavelength continuously provided before and after the magnetization region 12.
It consists of

MR素子部は図示を省略したが、第4図の従来例と同様
に構成されているものとする。
Although illustration of the MR element section is omitted, it is assumed that the structure is similar to that of the conventional example shown in FIG.

以上のような構成によれば、インデックス相6の磁化パ
ターンによる磁束分布は第2図のようになる。磁化領域
12のS、N極の前後には、それぞれ磁化領域13の同
極があるので、この反発による磁化領域12の磁束14
はインクリメンタル相7の磁束lOと同程度に絞られた
広がりの小さな分布となる。
According to the above configuration, the magnetic flux distribution due to the magnetization pattern of the index phase 6 is as shown in FIG. Since there are the same poles of the magnetized region 13 before and after the S and N poles of the magnetized region 12, the magnetic flux 14 of the magnetized region 12 due to this repulsion
becomes a distribution with a small spread narrowed to the same extent as the magnetic flux lO of the incremental phase 7.

従って、MR素子で磁界を検出すると、インデックス相
6の検出出力波形は、第6図でいえば符号Bのようにイ
ンクリメンタル相7の出力波形Aと同程度のパルス幅と
なるので、従来のようにロータの回転方向による基準位
置検出誤差が生じることがない。
Therefore, when a magnetic field is detected by the MR element, the detected output waveform of the index phase 6 has a pulse width comparable to the output waveform A of the incremental phase 7, as indicated by the symbol B in FIG. There is no reference position detection error caused by the rotational direction of the rotor.

一方、磁化領域13の記録波長は充分小さいので、ロー
タ表面からMR素子の方向への磁束の飛び出しが小さく
、このためスペーシングロスによりMR素子に磁束が到
達しにくい。磁化領域13の記録波長はMR素子とロー
タの間隔、素子感度、磁化領域12の波長その他の組み
合わせに応じで最適値を定めるとよい。例えば、MR素
子とロータの間隔が0.1mm、素子のストライプ幅が
lOILmの場合、磁化領域13の記録波長は磁化領域
12のh以下であれば良いことがわかった。
On the other hand, since the recording wavelength of the magnetized region 13 is sufficiently small, the projection of magnetic flux from the rotor surface toward the MR element is small, so that it is difficult for the magnetic flux to reach the MR element due to spacing loss. The recording wavelength of the magnetized region 13 may be determined to be an optimum value depending on a combination of the distance between the MR element and the rotor, the element sensitivity, the wavelength of the magnetized region 12, and other factors. For example, it has been found that when the distance between the MR element and the rotor is 0.1 mm and the stripe width of the element is lOILm, the recording wavelength of the magnetized region 13 should be equal to or less than h of the magnetized region 12.

第1図では磁化領域12の前後1周分を磁化領域13と
したが、第3図のように基準位置の前後に短波長の記録
部分を1磁界ずつ設けるようにしても同様の効果を得る
ことができる。
In Figure 1, the magnetized area 13 is one round before and after the magnetized area 12, but the same effect can be obtained by providing one short wavelength recording area before and after the reference position as shown in Figure 3. be able to.

また、以上ではロータリーエンコーダを例示したが、直
線状にトラックを配置するリニアエンコーダなどにも本
発明を同様に実施することができる。さらに、検出素子
としてMR素子以外に誘導型の磁気センサを用いる場合
にも同様の効果を得ることができる。
Furthermore, although a rotary encoder has been exemplified above, the present invention can be similarly applied to a linear encoder in which tracks are arranged in a straight line. Furthermore, similar effects can be obtained when using an inductive magnetic sensor other than an MR element as the detection element.

[効 果] 以上の説明から明らかなように、本発明によれば基準位
置検出用磁化領域の前後にこの磁化領域よりも記録波長
の短い磁化領域を設ける構成を採用しているので、基準
位置検出用の磁束の広がりを狭くでき、検出誤差を低減
できる優れたエンコーダ装置を提供できる。
[Effect] As is clear from the above explanation, according to the present invention, a configuration is adopted in which magnetized regions having a recording wavelength shorter than that of the magnetized region are provided before and after the magnetized region for detecting the reference position. It is possible to provide an excellent encoder device that can narrow the spread of magnetic flux for detection and reduce detection errors.

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

第1図は本発明によるロータリーエンコーダのロータ部
の実施例を示す斜視図、第2図は第1図のロータの磁束
分布を示した説明図、第3図は本発明の異なる実施例を
示した斜視図、第4図は従図の装置による検出信号を示
した波形図である。 l・・・ロータ     5・・・磁化パターン6・・
・インデックス相 7…インクリメンタル相 12.13・・・磁化領域 10.14・・・磁束 人 5p
Fig. 1 is a perspective view showing an embodiment of the rotor section of a rotary encoder according to the present invention, Fig. 2 is an explanatory diagram showing the magnetic flux distribution of the rotor in Fig. 1, and Fig. 3 shows a different embodiment of the invention. FIG. 4 is a waveform diagram showing a detection signal by the apparatus shown in FIG. l... Rotor 5... Magnetization pattern 6...
・Index phase 7...Incremental phase 12.13...Magnetization area 10.14...Magnetic flux person 5p

Claims (1)

【特許請求の範囲】[Claims] 被検出体の基準位置を磁気センサを用いて検出するエン
コーダ装置において、被検出体の基準位置検出用の磁化
領域の前後にこの磁化領域よりも記録波長の短い磁化領
域を設けたことを特徴とするエンコーダ装置。
An encoder device that detects the reference position of a detected object using a magnetic sensor, characterized in that magnetized regions having a recording wavelength shorter than that of the magnetized region are provided before and after a magnetized region for detecting the reference position of the detected object. encoder device.
JP60201618A 1985-08-08 1985-09-13 Encoder device Expired - Lifetime JPH0711429B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP60201618A JPH0711429B2 (en) 1985-09-13 1985-09-13 Encoder device
US06/893,215 US4785241A (en) 1985-08-08 1986-08-05 Encoder unit using magnetoresistance effect element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60201618A JPH0711429B2 (en) 1985-09-13 1985-09-13 Encoder device

Related Child Applications (1)

Application Number Title Priority Date Filing Date
JP2218196A Division JP2619621B2 (en) 1996-02-08 1996-02-08 Encoder device

Publications (2)

Publication Number Publication Date
JPS6262215A true JPS6262215A (en) 1987-03-18
JPH0711429B2 JPH0711429B2 (en) 1995-02-08

Family

ID=16444042

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60201618A Expired - Lifetime JPH0711429B2 (en) 1985-08-08 1985-09-13 Encoder device

Country Status (1)

Country Link
JP (1) JPH0711429B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06160112A (en) * 1992-11-25 1994-06-07 Mitsubishi Steel Mfg Co Ltd Magnetic encoder
JP2002243498A (en) * 2001-02-22 2002-08-28 Honda Motor Co Ltd Apparatus for detecting rotary angle of rotor

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5925441A (en) * 1982-08-02 1984-02-09 Hitachi Ltd Photocoupled multiplex circuit
JPS59189500A (en) * 1983-04-13 1984-10-27 株式会社日立製作所 Magnetic type rotary encoder

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5925441A (en) * 1982-08-02 1984-02-09 Hitachi Ltd Photocoupled multiplex circuit
JPS59189500A (en) * 1983-04-13 1984-10-27 株式会社日立製作所 Magnetic type rotary encoder

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH06160112A (en) * 1992-11-25 1994-06-07 Mitsubishi Steel Mfg Co Ltd Magnetic encoder
JP2002243498A (en) * 2001-02-22 2002-08-28 Honda Motor Co Ltd Apparatus for detecting rotary angle of rotor
JP4673489B2 (en) * 2001-02-22 2011-04-20 本田技研工業株式会社 Vehicle generator

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