JPH01265113A - Magnetic encoder - Google Patents

Magnetic encoder

Info

Publication number
JPH01265113A
JPH01265113A JP9345688A JP9345688A JPH01265113A JP H01265113 A JPH01265113 A JP H01265113A JP 9345688 A JP9345688 A JP 9345688A JP 9345688 A JP9345688 A JP 9345688A JP H01265113 A JPH01265113 A JP H01265113A
Authority
JP
Japan
Prior art keywords
magnetic
encoder
current
output voltage
temperature
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
JP9345688A
Other languages
Japanese (ja)
Inventor
Tokio Sekiguchi
関口 時雄
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.)
Nidec Advanced Motor Corp
Original Assignee
Nidec Servo Corp
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 Nidec Servo Corp filed Critical Nidec Servo Corp
Priority to JP9345688A priority Critical patent/JPH01265113A/en
Publication of JPH01265113A publication Critical patent/JPH01265113A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain the high-accuracy encoder by supplying a current to magneto-resistance effect elements of the magnetic encoder by a power unit which has a constant current circuit. CONSTITUTION:The magnetic encoder is constituted by magnetizing magnetic records 3 of a magnetic recording medium on the outer periphery of a magnetic drum 2 fixed on a rotary shaft 1 at nearly equal intervals in alternate N and S order and arranging the magnetic sensor 4 which has the magneto-resistance effect elements R1-R4 formed of ferromagnetic thin films oppositely to the outer periphery of the magnetic drum 2 across a proper gap. The current is supplied to terminals (a) and (b) of the magnetic sensor 4 by the constant current power source Is. Consequently, even if the resistance value R0 in the absence of a magnetic field varies with temperature, the current flowing to the magnetic sensor is constant, so the output voltage e1 between terminals (c) and (d) is only an output voltage based upon the variation of a magnetic field and never varies with the temperature.

Description

【発明の詳細な説明】 (1)発明の目的 [産業上の利用分野] 本発明は回転体の速度又は位置等を検出する磁気エンコ
ーダに関するものである。
DETAILED DESCRIPTION OF THE INVENTION (1) Purpose of the Invention [Field of Industrial Application] The present invention relates to a magnetic encoder that detects the speed, position, etc. of a rotating body.

[従来技術] 第2図は従来より実施されている磁気エンコーダの概念
を示す構成図(a)と、磁気ドラムの磁気記録と磁気セ
ンサーとの相関を示す展開図(b)と、電気回路図(Q
)と、温度特性(d)、(e)である。
[Prior Art] Figure 2 shows a block diagram (a) showing the concept of a conventional magnetic encoder, a developed diagram (b) showing the correlation between magnetic recording on a magnetic drum and a magnetic sensor, and an electric circuit diagram. (Q
) and temperature characteristics (d) and (e).

図示の磁気エンコーダは回転軸1に固着した磁気ドラム
2の外周に磁気記録媒体の磁気記録3がN、S交互に略
等間隔に着磁され、磁気ドラム2の外周と適宜の空隙を
介して強磁性体の薄膜で形成された磁気抵抗効果素子R
□〜R4を有する磁気センサー4が対向配設され、前記
磁気センサーの磁気抵抗効果素子の抵抗変化を検出する
ことにより磁気ドラムを固着した回転軸の速度又は位置
を検出できるものである。
In the illustrated magnetic encoder, magnetic records 3 of a magnetic recording medium are magnetized alternately N and S at approximately equal intervals on the outer periphery of a magnetic drum 2 fixed to a rotating shaft 1. Magnetoresistive element R formed of a ferromagnetic thin film
Magnetic sensors 4 having □ to R4 are arranged opposite to each other, and the speed or position of the rotating shaft to which the magnetic drum is fixed can be detected by detecting the resistance change of the magnetoresistive element of the magnetic sensor.

磁気ドラム2の磁気記録3と磁気センサー4の磁気抵抗
効果素子R1〜R4との相関関係は(b)図に示すよう
に磁気記録3の磁極ピッチλに対し4個の磁気抵抗効果
素子R1〜R4の配設ピッチはλ/2となるように配設
されている。
The correlation between the magnetic recording 3 of the magnetic drum 2 and the magnetoresistive elements R1 to R4 of the magnetic sensor 4 is as shown in FIG. The arrangement pitch of R4 is λ/2.

更に(c)図に示すように4個の磁気抵抗効果素子R1
〜R4を接続してブリッジを構成し、該ブリッジのa、
b端子に電源Esを接続し、c、d端子には回転軸1が
回転することにより正弦波又は疑似正弦波の電圧が得ら
れるように構成されており、この出力電圧を測定するこ
とにより回転軸の位置。
Furthermore, as shown in the figure (c), four magnetoresistive elements R1
~R4 is connected to form a bridge, and the a,
The power supply Es is connected to the b terminal, and the rotation shaft 1 is connected to the c and d terminals so that a sine wave or pseudo sine wave voltage can be obtained.The rotation can be determined by measuring this output voltage. Axis position.

又は速度を検出することが出来るものである。Or it can detect speed.

磁気抵抗効果素子に電流を供給する電源Esは定電圧回
路によるのが一般的である。
The power source Es that supplies current to the magnetoresistive element is generally a constant voltage circuit.

磁気抵抗効果素子の抵抗値は該素子に作用する磁界の強
さにより変化し、磁界の強さが零のときの抵抗値をRo
とし、磁界の強さに比例して抵抗値が下がり、ある磁界
強度以上において抵抗値は最小と成る。
The resistance value of a magnetoresistive element changes depending on the strength of the magnetic field acting on the element, and the resistance value when the magnetic field strength is zero is Ro.
The resistance value decreases in proportion to the magnetic field strength, and the resistance value reaches a minimum above a certain magnetic field strength.

ここである磁界により変化する抵抗値の変化量をΔRと
すると、磁気抵抗効果素子が磁界を受けているときの抵
抗はR=R0−ΔRと表すことが出来る。
Here, if the amount of change in the resistance value that changes due to a certain magnetic field is ΔR, then the resistance when the magnetoresistive element is receiving a magnetic field can be expressed as R=R0−ΔR.

(c)図においてR□とR2の直列回路の端子a。(c) Terminal a of the series circuit of R□ and R2 in the figure.

bに電圧Eを印加したときに端子c、bに表れる出力電
圧e1は e、=R,e E/ (R,+R,)と表さ
れR工、R2を夫々Rとし、相互関係が(b)図の位置
に在るものとすると、R1は作用する磁界が零の位置で
あるからΔRが零でRoと成り、R2は作用磁界が最大
の位置であるからΔRが最大となり ex=CRo−ΔR)−E/ (2R,−ΔR)−(1
)と表されΔRに比例した電圧が出力する。
The output voltage e1 appearing at terminals c and b when voltage E is applied to b is expressed as e, = R, e E/ (R, +R,), where R and R2 are respectively R, and the mutual relationship is (b ) Assuming that R1 is at the position shown in the figure, R1 is the position where the acting magnetic field is zero, so ΔR is zero and becomes Ro, and R2 is the position where the acting magnetic field is maximum, so ΔR is maximum and ex = CRo- ΔR)-E/ (2R,-ΔR)-(1
), and a voltage proportional to ΔR is output.

磁気抵抗効果素子に作用する磁界が磁気ドラムの回転に
より正弦波状に変化すると出力電圧eユも正弦波状に変
化するものであり、ブリッジの他の辺R3R4において
も同様に端子d、b間に出力電圧e2が生じ、全体の出
力電圧e0はeo”e、−e2=ΔR−E/(2R,−
ΔR) ・(2)と表される。
When the magnetic field acting on the magnetoresistive element changes in a sinusoidal manner due to the rotation of the magnetic drum, the output voltage e also changes in a sinusoidal manner, and the output voltage is similarly output between the terminals d and b on the other sides R3R4 of the bridge. A voltage e2 is generated, and the overall output voltage e0 is eo”e, -e2=ΔR-E/(2R,-
ΔR) ・(2)

[発明が解決しようとする問題点] 第2図に示す磁気エンコーダの出力電圧は回転軸の位置
又は速度に対応した正弦波電圧が得られるのであるが、
強磁性体の薄膜で形成された磁気抵抗素子の抵抗値は、
作用する磁界の強さによって変化するのは勿論であるが
、(d)図に示すように温度によっても変化する特性で
正の温度係数を持っており、一方で(e)曲線において
磁界による変化分であるΔRは変化していないことを示
している。 このため出力電圧の振幅が周囲温度により
変化し、サーボモータの位置検出に使用する正弦波出力
の磁気エンコーダにおいては位置の検出誤差を生ずると
いう問題が有り、本発明は周囲温度が変化しても一定振
幅の電圧が得られる磁気エンコーダを提供せんとするも
のである。
[Problems to be Solved by the Invention] The output voltage of the magnetic encoder shown in FIG. 2 is a sine wave voltage corresponding to the position or speed of the rotating shaft.
The resistance value of a magnetoresistive element made of a thin film of ferromagnetic material is
Of course, it changes depending on the strength of the applied magnetic field, but as shown in figure (d), it also changes depending on temperature, and has a positive temperature coefficient, while curve (e) shows that it changes due to the magnetic field. This shows that ΔR, which is the minute, has not changed. For this reason, the amplitude of the output voltage changes depending on the ambient temperature, causing a position detection error in a magnetic encoder with a sine wave output used to detect the position of a servo motor. The present invention aims to provide a magnetic encoder that can obtain a voltage of constant amplitude.

(2)発明の構成 [問題点を解決するための手段] 本発明は前記のような問題点を解決するため、磁気抵抗
効果素子に定電流回路を有する電源装置で電流を供給す
る構成としたものである。
(2) Structure of the invention [Means for solving the problems] In order to solve the above problems, the present invention has a structure in which a power supply device having a constant current circuit supplies current to the magnetoresistive element. It is something.

[作  用] 従来技術においては磁気センサの温度が高くなると(1
)式で示した出力電圧e1は磁気抵抗効果素子のRoが
高くなり、電源電圧Eが一定であるから磁気センサの電
流工、が減少し出力電圧が低下する。
[Function] In the conventional technology, when the temperature of the magnetic sensor increases (1
) As for the output voltage e1 shown by the equation, the Ro of the magnetoresistive element increases, and since the power supply voltage E is constant, the current flow of the magnetic sensor decreases, and the output voltage decreases.

前記のような従来技術に対し電源を定電流電源に変更す
ることにより、R11が温度変化により変化しても磁気
センサを流れる電流は一定であるから出力電圧e1は磁
界の変化による出力電圧のみとなり温度により変化しな
くなる作用が有る。
By changing the power supply to a constant current power supply in contrast to the conventional technology described above, the current flowing through the magnetic sensor remains constant even if R11 changes due to temperature changes, so the output voltage e1 becomes only the output voltage due to changes in the magnetic field. It has the effect of not changing depending on the temperature.

[発明の実施例] 第1図は本発明による磁気エンコーダの電気回路を示し
、磁気センサの端子a、bに定電流電源Isを介して電
流を供給するようにした事が新しい構成で、他は従来技
術によるものと同じである。
[Embodiment of the Invention] Fig. 1 shows an electric circuit of a magnetic encoder according to the present invention, and the new configuration is that current is supplied to terminals a and b of the magnetic sensor via a constant current power supply Is. is the same as that according to the prior art.

図において磁気センサの抵抗R1R,の直列回路に定電
流電源Isより電流1.を流すと(2R0−ΔR)・工
。より端子a、bの電圧は温度により変化するR、に比
例して変化し、出力電圧。
In the figure, a current of 1. When flowing (2R0-∆R). Therefore, the voltage at terminals a and b changes in proportion to R, which changes with temperature, resulting in the output voltage.

eoは(2)式においてE/(2R−ΔR)が一定であ
るから磁界の変化に対応した変化ΔRのみとなり、温度
の影響を受けなくなる。
Since E/(2R-ΔR) is constant in Equation (2), eo only changes ΔR corresponding to changes in the magnetic field, and is not affected by temperature.

ΔRは強磁性体の材質にも因るが通常抵抗値の2〜5%
であり、R,の温度係数は0.2〜0.3%/℃である
から例えば温度が20℃〜80℃と60deg変化する
とR8が12〜18%変化したのに対し、本発明の構成
によると温度により出力電圧の変化は無くなる。
ΔR depends on the material of the ferromagnetic material, but is usually 2 to 5% of the resistance value.
Since the temperature coefficient of R is 0.2-0.3%/°C, for example, when the temperature changes by 60 degrees from 20°C to 80°C, R8 changes by 12-18%, whereas the structure of the present invention According to , the output voltage does not change due to temperature.

定電流回路は一般的に知られたもので、例えば半導体制
御素子と電流検出抵抗とを電源と負荷側との間に介挿し
、電流検出抵抗の電圧と基準電圧とをオペアンプで比較
し、オペアンプの出力で半導体制御素子を制御し、負荷
電流を一定に制御する装置等が使用される。
A constant current circuit is generally known. For example, a semiconductor control element and a current detection resistor are inserted between the power supply and the load side, and the voltage of the current detection resistor is compared with a reference voltage using an operational amplifier. A device or the like is used that controls a semiconductor control element using the output of , and controls the load current to a constant value.

[発明の効果コ 本発明になる磁気エンコーダは前記のような構成である
から、其の出力電圧が温度による影響を受けず、サーボ
モータの位置検出装置に使用できる高精度の磁気エンコ
ーダを得ることが出来る。
[Effects of the Invention] Since the magnetic encoder according to the present invention has the above-described configuration, its output voltage is not affected by temperature, and it is possible to obtain a highly accurate magnetic encoder that can be used in a position detection device for a servo motor. I can do it.

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

第1図は本発明の磁気エンコーダの回路図、第2図は従
来技術の磁気エンコーダの概念図(a)。 展開図(b)、電気回路図(C)、磁気センサの温度特
性図(d)、(e)である。 符号の説明 1・・・回転軸、2・・・磁気ドラム、3・・・磁気記
録。 4・・・磁気センサ、Es・・・定電圧電源、 Is・
・・定電流電源、R工〜R4・・・磁気抵抗効果素子。 特許出願人 日本サーボ株式会社 (a) (C) ル (J)        (e) 第2図 号3−
FIG. 1 is a circuit diagram of a magnetic encoder according to the present invention, and FIG. 2 is a conceptual diagram (a) of a conventional magnetic encoder. They are a developed view (b), an electric circuit diagram (C), and temperature characteristic diagrams (d) and (e) of the magnetic sensor. Explanation of symbols 1...rotating shaft, 2...magnetic drum, 3...magnetic recording. 4...Magnetic sensor, Es...constant voltage power supply, Is...
・・Constant current power supply, R engineering ~ R4 ・・Magnetoresistive effect element. Patent applicant Nippon Servo Co., Ltd. (a) (C) Le (J) (e) Figure 2 No. 3-

Claims (1)

【特許請求の範囲】[Claims] 回転体の外周に固着した磁気記録媒体に、其の移動方向
に略等間隔のN、S極を交互に記録した磁気ドラムと、
該磁気ドラムと空隙を介し対向配設され、強磁性体の薄
膜で形成された磁気抵抗効果素子による磁気センサーと
を有する磁気エンコーダにおいて、前記磁気センサーに
定電流回路を介して電流を供給する構成を特徴とする磁
気エンコーダ。
A magnetic drum in which N and S poles are alternately recorded at approximately equal intervals in the direction of movement of the magnetic recording medium fixed to the outer periphery of a rotating body;
A magnetic encoder having a magnetic sensor formed of a magnetoresistive element made of a thin film of ferromagnetic material, which is disposed opposite to the magnetic drum with a gap therebetween, and configured to supply current to the magnetic sensor via a constant current circuit. A magnetic encoder featuring:
JP9345688A 1988-04-18 1988-04-18 Magnetic encoder Pending JPH01265113A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9345688A JPH01265113A (en) 1988-04-18 1988-04-18 Magnetic encoder

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9345688A JPH01265113A (en) 1988-04-18 1988-04-18 Magnetic encoder

Publications (1)

Publication Number Publication Date
JPH01265113A true JPH01265113A (en) 1989-10-23

Family

ID=14082830

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9345688A Pending JPH01265113A (en) 1988-04-18 1988-04-18 Magnetic encoder

Country Status (1)

Country Link
JP (1) JPH01265113A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5589768A (en) * 1990-07-30 1996-12-31 Mitsubishi Steel Mfg. Co., Ltd. Magnetoresistance-effect magnetic sensor of the temperature compensating type
CN111239435A (en) * 2020-01-22 2020-06-05 微特技术有限公司 Wind speed and wind direction integrated detection sensor

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5826215A (en) * 1981-08-07 1983-02-16 Nippon Denso Co Ltd Rotating angle detector
JPS5868615A (en) * 1981-10-20 1983-04-23 Sharp Corp Output circuit of magnetic type rotary encoder

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5826215A (en) * 1981-08-07 1983-02-16 Nippon Denso Co Ltd Rotating angle detector
JPS5868615A (en) * 1981-10-20 1983-04-23 Sharp Corp Output circuit of magnetic type rotary encoder

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5589768A (en) * 1990-07-30 1996-12-31 Mitsubishi Steel Mfg. Co., Ltd. Magnetoresistance-effect magnetic sensor of the temperature compensating type
CN111239435A (en) * 2020-01-22 2020-06-05 微特技术有限公司 Wind speed and wind direction integrated detection sensor

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