JPS58139014A - Rotary encoder - Google Patents
Rotary encoderInfo
- Publication number
- JPS58139014A JPS58139014A JP2115782A JP2115782A JPS58139014A JP S58139014 A JPS58139014 A JP S58139014A JP 2115782 A JP2115782 A JP 2115782A JP 2115782 A JP2115782 A JP 2115782A JP S58139014 A JPS58139014 A JP S58139014A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- output
- patterns
- elements
- series
- 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
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING 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
- G01D5/00—Mechanical 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
- G01D5/12—Mechanical 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 using electric or magnetic means
- G01D5/14—Mechanical 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 using electric or magnetic means influencing the magnitude of a current or voltage
- G01D5/142—Mechanical 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 using electric or magnetic means influencing the magnitude of a current or voltage using Hall-effect devices
- G01D5/145—Mechanical 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 using electric or magnetic means influencing the magnitude of a current or voltage using Hall-effect devices influenced by the relative movement between the Hall device and magnetic fields
Abstract
Description
【発明の詳細な説明】
本発明は四−タリーエンコーダ、特に磁気媒体に対向配
置された磁気検出用磁気抵抗素子の磁気検出構造に関す
るものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a four-tally encoder, and particularly to a magnetic detection structure of a magnetoresistive element for magnetic detection disposed facing a magnetic medium.
第1図は従来より提案されているロータリーエンコーダ
の一例を示す要部断面構成図である。同図において、1
は回転手段として例えば直流−1−タなどの回転体、2
はこの回転体1に連結された回転軸、3は磁気トラック
に磁極(磁気パターン)が着磁して書き込まれ九例えば
円板状磁気ディスク4にその中心軸が連結された磁気デ
ィスク回転軸、sr;を回転体回転軸2と磁気ディスク
回転軸3とを結合するカップリング、@a + 6b
は磁気ディスク回転軸3の軸受、Tは円板状磁気ディス
ク4に対向配置され九磁気抵抗効果を有する磁気抵抗素
子、8は磁気抵抗素子Tから出力された電気信号を増幅
する増幅器、9け磁気ディスク41磁気抵抗素子1およ
び増幅器・を外界雰咄気から纏蔽するハクジングである
。FIG. 1 is a cross-sectional configuration diagram of essential parts showing an example of a conventionally proposed rotary encoder. In the same figure, 1
As the rotating means, for example, a rotating body such as a DC-1 motor, 2
3 is a rotating shaft connected to this rotating body 1; 3 is a magnetic disk rotating shaft on which magnetic poles (magnetic patterns) are magnetized and written; sr; is a coupling that connects the rotating body rotating shaft 2 and the magnetic disk rotating shaft 3, @a + 6b
8 is a bearing of the magnetic disk rotating shaft 3; T is a magnetoresistive element disposed opposite to the disc-shaped magnetic disk 4 and has a magnetoresistive effect; 8 is an amplifier for amplifying the electrical signal output from the magnetoresistive element T; This is a hack to shield the magnetic disk 41, magnetoresistive element 1, and amplifier from the outside atmosphere.
絡゛2図は第1図で示した磁気ディスク4と磁気抵抗素
子Tとが対向配置された対応関係を説明するための要部
拡大平面構成図である。同図において、円板状磁気ディ
スク4の外周部分にF1回転方向(A方向)に沿って5
−N11極を着磁して書き込まれた磁気パターン4aが
放射状に多数個等配されて磁気トラック4′が形成され
ている。そして、この円板状磁気ディスク4の磁気トラ
ツタ4′対向面上□には、上記磁気パターン4aとほぼ
同等の周方向の間隔幅を有する例えばパーマ冑イ薄膜パ
ターンからなる1組の磁気抵抗素子Tが所定間隔寸法を
介して対向配置されている。なお、Ta。FIG. 2 is an enlarged plan view of the main parts for explaining the correspondence relationship in which the magnetic disk 4 and the magnetoresistive element T shown in FIG. 1 are disposed facing each other. In the same figure, there are 5
A large number of magnetic patterns 4a written by magnetizing the -N11 pole are equally distributed radially to form a magnetic track 4'. On the surface □ of the disc-shaped magnetic disk 4 facing the magnetic tracker 4', a set of magnetoresistive elements made of, for example, a thin film pattern made of a permanent mask having a circumferential interval width approximately equal to that of the magnetic pattern 4a is provided. The T's are arranged opposite to each other with a predetermined interval between them. In addition, Ta.
1bは入出力端子、la 、 7d は磁気抵抗検出
部、T@L導体部である。1b is an input/output terminal, la and 7d are a magnetic resistance detection section, and a T@L conductor section.
このように構成されたロータリーエンコーダにおいて、
回転体1が矢印A方向に回転すると、これに同期して磁
気ディスク4も矢印方向に回転し、そして、磁気抵抗素
子7は固定配置されているので、この磁気抵抗素子Tの
磁気抵抗効果により、入出力端子7a e Tb相互間
にFi回転角度に対応して出力電圧の変化分ΔVp−p
が得られる。ま九、回転速度に応じてその出力波形
の周波数が変化する。したがって、これらの機能を利用
することにより、単に回転数の計数のみならず、回転適
度岬の情報を出力することができる。In the rotary encoder configured in this way,
When the rotating body 1 rotates in the direction of the arrow A, the magnetic disk 4 also rotates in the direction of the arrow in synchronization with this, and since the magnetoresistive element 7 is fixedly arranged, the magnetoresistive effect of the magnetoresistive element T causes , a change in output voltage ΔVp-p between input and output terminals 7a and Tb corresponding to the rotation angle of Fi
is obtained. Ninth, the frequency of the output waveform changes depending on the rotation speed. Therefore, by using these functions, it is possible not only to simply count the number of revolutions but also to output information on the degree of rotational speed.
しかしながら、上記構成によるロータリーエンコーダに
おいては、磁気ディスク4に着磁して書き込壕れた出猟
パターン41の精度が出力信号の精度に対して大匙な影
番を与えているという問題が6つ九。すなわち、第3図
(a)1缶) 、 (C)に示すように各1債磁気パタ
ーン4aかも1種類の同一相の電気的出力が出力される
が、同図−)K示すように各々の磁気パターン4aのピ
ッチまた性磁束の偏差(バラツキ)が同図(b) 、
(@)に示すようにその壕ま電気信号の偏差として出力
される。例えにピッチに偏差を有する磁気パターン4m
’ではこれに対応する同図(b) 、 (c)に示すよ
うに出力信号の波長、パルス幅を変化させ、高精度の電
気的出力が得られないという欠点があった。ま走、回転
体1が回転数1000r、p、mのエンコーダにおいて
は、1000個の磁気パターン4aが存在するが、磁気
ディスタ4上に各々磁気パターン4aをある一定の精度
で書き込み着磁することは技術的にも極めて困−である
という問題があった。However, in the rotary encoder having the above configuration, there is a problem that the accuracy of the hunting pattern 41 that is magnetized and written on the magnetic disk 4 has a large influence on the accuracy of the output signal. Nineteen. That is, as shown in FIG. 3 (a) (1 can) and (C), one type of electrical output of the same phase is output from each single bond magnetic pattern 4a, but as shown in FIG. The pitch of the magnetic pattern 4a and the deviation (dispersion) of the magnetic flux are shown in the same figure (b),
As shown in (@), the difference is output as a deviation of the electric signal. For example, a 4m magnetic pattern with deviation in pitch
', as shown in the corresponding figures (b) and (c), had the disadvantage that the wavelength and pulse width of the output signal were changed, making it impossible to obtain highly accurate electrical output. In an encoder in which the rotating body 1 has a rotation speed of 1000 r, p, m, there are 1000 magnetic patterns 4a, but each magnetic pattern 4a must be written and magnetized on the magnetic disk 4 with a certain precision. The problem was that it was technically extremely difficult.
したがって本発明は、磁気抵抗素子を、少なくとも2組
の磁気抵抗検出素子を1列接続して構成する仁とによっ
て、・1つの電気的出力を複数の磁気パターンから得る
ようにして個々の磁気パターンのピッチ、磁束の偏差を
均一化させて出力精度の偏差を小さくして読み出すよう
にしたロータリーエン冨−ダを提供することを目的とし
ている。Therefore, the present invention provides a magnetoresistive element that is configured by connecting at least two sets of magnetoresistive sensing elements in one row, so that one electrical output is obtained from a plurality of magnetic patterns, and each magnetic pattern It is an object of the present invention to provide a rotary encoder in which the pitch and magnetic flux deviations are made uniform, and the deviation in output accuracy is reduced for reading.
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 using the drawings.
1s4図は本発明による同一タリーエンコーダの一例を
説明するための磁気ディスクと磁気抵抗素子との対応関
係を示す要部拡大平面構成図であり、前述の図と同記考
は同一要素となるのでその説明嬬省略する。同図におい
て、磁気ディスク4の外周面上に多**Oa気パターン
゛4aが放射状に等配して形成され九磁気トツツク4′
対向面上には、3組の磁気抵抗素子1(A、10勝、I
DC%すなわち4)2本ずつ会計6本の磁気検出素子1
0m、16is、10・、led、10@、10f を
入出力端子10p。Figure 1s4 is an enlarged plan configuration diagram of essential parts showing the correspondence relationship between a magnetic disk and a magnetoresistive element for explaining an example of the same tally encoder according to the present invention, and the above-mentioned figure and the same description are the same elements, so I will omit that explanation. In the figure, multiple **Oa air patterns 4a are formed on the outer circumferential surface of the magnetic disk 4, and nine magnetic spots 4' are formed evenly distributed radially.
On the opposing surface, three sets of magnetoresistive elements 1 (A, 10 wins, I
DC% i.e. 4) Magnetic detection elements 1 each accounting for 2 pieces and 6 pieces
0m, 16is, 10・, led, 10@, 10f are input/output terminals 10p.
10h間の相互間にそれぞれ5本の導体[l1101で
直列接続して同一平面上に形成された3組の磁気抵抗素
子10ム、10m、10cからなる磁気抵抗素子10が
所定間幅寸法を介して対向配置されている。この場合も
前記同様にこの磁気抵抗素子1・は磁気パターン4&と
ほぼ同等の局方向の関Mi@を有してパーマレイ薄膜パ
ターンで形成されている。A magnetoresistive element 10 consisting of three sets of magnetoresistive elements 10m, 10m, and 10c formed on the same plane and connected in series with five conductors [l1101] is connected with a predetermined width dimension between them. They are placed facing each other. In this case, similarly to the above, the magnetoresistive element 1 is formed of a permalay thin film pattern having a direction Mi@ which is substantially the same as that of the magnetic pattern 4&.
このような構成によれば、磁気抵抗素子10は第5図に
示した如く等価回路となり、したがって入出力端子ta
11.10h関に電流制限抵抗In直列接続した直槻電
源Eを接続することによって、6個の磁気パターン4a
(j114図参照)からそれぞれ同種類の同一相の電気
信号が得られる。この場合、電気信号は6個の8磁気パ
ターン41のピッチ、磁束の偏差に対して6個の磁気パ
ターン4aの平均化され九4のが電気的出力となって得
られ、し九がって該出力の偏差は極めて小さくなる。ま
た、磁気パターン4aの数量をさらに増大させれば、出
力個差をさらに減少させることができる。According to such a configuration, the magnetoresistive element 10 becomes an equivalent circuit as shown in FIG. 5, and therefore the input/output terminal ta
11. By connecting the Naotsuki power supply E with the current limiting resistor In series connected to the 10h gate, the six magnetic patterns 4a
(See figure j114), electrical signals of the same type and phase are obtained. In this case, the electric signal is obtained by averaging the six magnetic patterns 4a with respect to the deviation of the pitch and magnetic flux of the six eight magnetic patterns 41, and the electric signal is obtained as an electrical output. The deviation of the output becomes extremely small. Moreover, if the number of magnetic patterns 4a is further increased, the output individual difference can be further reduced.
また、他の賓形例として蝶、上記実施例で3端子、つま
り入出力端子10F、10hおよび直流電源Eの正極側
の3端子で1組の磁気抵抗素子10を構成し友場金に対
して第6図(a) 、 (b)に示し友ように磁気抵抗
素子10と同一構造の磁気抵抗素子11を1/2磁極ピ
ツチずらして配置し、3端子で2個の磁気抵抗素子1・
、11を用いることによって、電気的出力を2倍に大き
くすることができる。さらに第65Aに示した同様に3
端子素子をし2磁極ピツチずらして配置することにより
、ブリッジ接続構造とし、電気的出力を4倍とすること
もできる。さらには同様の上記ブリッジ接続構造の素子
を14磁極ピツチずらして配置するととにより、電気角
で900位相のずれた電気的出力が得られ、図示しない
磁気ディスク4(第4図参照)の正逆1転判別を可能と
した構造とすることができる。In addition, as another example of a butterfly, in the above embodiment, one set of magnetoresistive element 10 is configured with three terminals, that is, the input/output terminals 10F and 10h, and the three terminals on the positive electrode side of the DC power supply E. As shown in FIGS. 6(a) and 6(b), a magnetoresistive element 11 having the same structure as the magnetoresistive element 10 is arranged with a 1/2 magnetic pole pitch shifted, and two magnetoresistive elements 1 and 1 with three terminals are arranged.
, 11, the electrical output can be doubled. Furthermore, similarly as shown in No. 65A, 3
By arranging the terminal elements so as to shift the pitch of two magnetic poles, a bridge connection structure can be formed, and the electrical output can be quadrupled. Furthermore, by arranging elements with the same bridge connection structure as described above, shifted by 14 magnetic pole pitches, electrical outputs with a phase shift of 900 electrical degrees can be obtained, and the magnetic disk 4 (not shown) (see FIG. 4) can be rotated in the forward and reverse directions. It is possible to have a structure that allows one-turn discrimination.
以上説明したように本発明によれば、精度の偏差が小さ
い出力信号が得られるので、高精度の磁気ロータリーエ
ンコーダが得られるという極めて優ねた効果が得られる
。As explained above, according to the present invention, an output signal with a small deviation in accuracy can be obtained, so that a highly accurate magnetic rotary encoder can be obtained, which is an extremely excellent effect.
#11図ないし第3図は従来の磁気式ロータリー工/コ
ーダの一例を説明す、るための図、IR4図。
111ゝ
第5図は本発明による磁気式ロータリーエンコーダの一
実施例を説明するための図、第6図、第7図は本発明に
よる磁気式ロータリーエンコーダの他の実施例を説明す
る丸めの図である。
411・・・磁気ディスク、4m 、 4m’ ・・
e・磁気パターン(磁極)、4′ ・・・拳磁気ト2ツ
ク、10 、10^、10m、IOC@@Φ・磁気抵抗
素子、10m+ 10b+ lee、10d、10*、
10f・・・・磁気抵抗検出素子、10F、10h
・・・舎人出力端子、101 ・・・・導体部、11
・・・・磁気抵抗素子。
代理人 弁理士 薄 1)利 幸パ\ノ
・τ″1
w41図
11112図
第3WJ#11 to 3 are diagrams IR4 diagram for explaining an example of a conventional magnetic rotary machine/coder. 111ゝFIG. 5 is a diagram for explaining one embodiment of the magnetic rotary encoder according to the present invention, and FIGS. 6 and 7 are rounded diagrams for explaining other embodiments of the magnetic rotary encoder according to the present invention. It is. 411...magnetic disk, 4m, 4m'...
e・Magnetic pattern (magnetic pole), 4′...Fist magnetic tock, 10, 10^, 10m, IOC@@Φ・Magnetic resistance element, 10m+ 10b+ lee, 10d, 10*,
10f... Magnetoresistive detection element, 10F, 10h
...Toneri output terminal, 101 ...Conductor part, 11
... Magnetoresistive element. Agent Patent Attorney Susuki 1) Yukiyuki Tori\ノ・τ″1 w41 Figure 11112 Figure 3 WJ
Claims (1)
、前記磁気パターンに対向配置されかつ賦磁気パターン
を読み取る磁気抵抗素子とを少なくとも備えた磁気式ロ
ータリーエンコーダにおいて、前記磁気抵抗素子は少な
くとも2組の磁気抵抗素子が直列接続して構成され、複
数の磁気パターンから同一相の電気信号を同時に取り出
すことを特徴とし九四−声す−エンコーダ。A magnetic rotary encoder comprising at least a magnetic medium on which a large number of magnetic patterns are magnetized and written, and a magnetoresistive element arranged to face the magnetic pattern and read the magnetized pattern, wherein the magnetoresistive element has at least two magnetoresistive elements. A 94-voice encoder comprising a set of magnetoresistive elements connected in series and capable of simultaneously extracting electrical signals of the same phase from a plurality of magnetic patterns.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2115782A JPS58139014A (en) | 1982-02-15 | 1982-02-15 | Rotary encoder |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2115782A JPS58139014A (en) | 1982-02-15 | 1982-02-15 | Rotary encoder |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS58139014A true JPS58139014A (en) | 1983-08-18 |
Family
ID=12047072
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2115782A Pending JPS58139014A (en) | 1982-02-15 | 1982-02-15 | Rotary encoder |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58139014A (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60122821U (en) * | 1984-01-27 | 1985-08-19 | 第一精工株式会社 | magnetic rotary encoder |
JPS60214219A (en) * | 1984-04-11 | 1985-10-26 | Hitachi Ltd | Magnetic rotary encoder |
JPS6288914U (en) * | 1985-11-22 | 1987-06-06 | ||
JPS62163916A (en) * | 1986-01-16 | 1987-07-20 | Hitachi Ltd | Apparatus for magnetically detecting position of moving body |
JPS63225124A (en) * | 1987-03-14 | 1988-09-20 | Hitachi Ltd | Magnetic position detector |
JPS6416924A (en) * | 1987-07-10 | 1989-01-20 | Sun Eh Electric Co | Detector and magnetic head for magnetic information |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS56115912A (en) * | 1980-02-18 | 1981-09-11 | Hitachi Ltd | Magnetic head for detecting movement |
-
1982
- 1982-02-15 JP JP2115782A patent/JPS58139014A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS56115912A (en) * | 1980-02-18 | 1981-09-11 | Hitachi Ltd | Magnetic head for detecting movement |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60122821U (en) * | 1984-01-27 | 1985-08-19 | 第一精工株式会社 | magnetic rotary encoder |
JPS60214219A (en) * | 1984-04-11 | 1985-10-26 | Hitachi Ltd | Magnetic rotary encoder |
JPS6288914U (en) * | 1985-11-22 | 1987-06-06 | ||
JPS62163916A (en) * | 1986-01-16 | 1987-07-20 | Hitachi Ltd | Apparatus for magnetically detecting position of moving body |
JPS63225124A (en) * | 1987-03-14 | 1988-09-20 | Hitachi Ltd | Magnetic position detector |
JPS6416924A (en) * | 1987-07-10 | 1989-01-20 | Sun Eh Electric Co | Detector and magnetic head for magnetic information |
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