JPH05223592A - Origin signal detector - Google Patents

Origin signal detector

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Publication number
JPH05223592A
JPH05223592A JP4030675A JP3067592A JPH05223592A JP H05223592 A JPH05223592 A JP H05223592A JP 4030675 A JP4030675 A JP 4030675A JP 3067592 A JP3067592 A JP 3067592A JP H05223592 A JPH05223592 A JP H05223592A
Authority
JP
Japan
Prior art keywords
origin
signal
detection
signals
distance
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
JP4030675A
Other languages
Japanese (ja)
Other versions
JP3195019B2 (en
Inventor
Ichiro Tokunaga
一郎 徳永
Katsuya Mitsuzuka
克也 三塚
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.)
Alps Alpine Co Ltd
Original Assignee
Alps Electric Co 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 Alps Electric Co Ltd filed Critical Alps Electric Co Ltd
Priority to JP03067592A priority Critical patent/JP3195019B2/en
Publication of JPH05223592A publication Critical patent/JPH05223592A/en
Application granted granted Critical
Publication of JP3195019B2 publication Critical patent/JP3195019B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To detect origin signals without requiring high-performance sensors and comparison circuits. CONSTITUTION:The following are provided: a magnetoresistance element 6 map of two pairs of sensors MR1-MR4 connected in series, respectively; a differential amplification circuit which differentially amplifies signals outputted from the respective intermediate points of the series-connected sensors; and a comparison circuit which wave-shapes signals differentially amplified to obtain origin signals; and, the ratio of distance Dy between the sensors MR2, MR3 to width Pz of the magnetizing part of an origin recording signal 10 is set by the value of 0.5. Therefore, manufacture of an encoder is easy, and the component cost can be reduced.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、磁気式エンコーダ等の
磁気記録媒体に着磁された原点記録信号を検出して原点
信号を出力する原点信号検出装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an origin signal detecting device for detecting an origin recording signal magnetized on a magnetic recording medium such as a magnetic encoder and outputting the origin signal.

【0002】[0002]

【従来の技術】一般に磁気式エンコーダにおいて、回転
型、直線移動型のものを問わず、所定の変位量ごとのイ
ンクリメンタル信号と原点位置を示す原点信号とを出力
するようになっている。
2. Description of the Related Art Generally, magnetic encoders of both rotary type and linear movement type are designed to output an incremental signal for each predetermined displacement amount and an origin signal indicating an origin position.

【0003】図7はこの種の従来の磁気式エンコーダの
原点信号検出装置を示す電気回路図、図8は図7の原点
信号検出装置に備えられる磁気抵抗素子の構成を示す
図、図9は図8の磁気抵抗素子が対向する磁気記録媒体
の原点記録信号の着磁部分を示す斜視図、図10は図7
の原点信号検出装置の動作を示すタイミングチャート、
図11は図7の原点信号検出装置の問題点を説明するた
めのタイミングチャートである。
FIG. 7 is an electric circuit diagram showing an origin signal detecting device of a conventional magnetic encoder of this kind, FIG. 8 is a diagram showing a structure of a magnetoresistive element provided in the origin signal detecting device of FIG. 7, and FIG. 8 is a perspective view showing a magnetized portion of the origin recording signal of the magnetic recording medium facing the magnetoresistive element of FIG. 8, and FIG.
Timing chart showing the operation of the origin signal detector of
FIG. 11 is a timing chart for explaining the problems of the origin signal detecting device of FIG.

【0004】図9に示す磁気記録媒体1には、N極とS
極の一対の極を有する原点記録信号2が着磁される。図
7に示す原点信号検出装置は、2つの検出素子Ra、R
bからなり信号Vaを出力する磁気抵抗素子3と、該信
号Vaを参照電圧Vrfaと比較する比較回路4とから
なっている。前記磁気抵抗素子3では、図8に示すよう
に、検出素子Ra、Rbの各一端が電源Vcが直列に接
続されて電流通路となっており、該検出素子Ra、Rb
は、それぞれ短冊状に形成され、互いに平行に配置され
る。また、検出素子Ra、Rbは、図10の(a)に示
すように、磁気記録媒体1と対向して設けられるととも
に、該磁気記録媒体1の移動方向に並ぶように配置され
る。そして、これらの検出素子Ra、Rbの各中心線間
の距離をDaとし、前記原点記録信号2の着磁部分の幅
をDcとしたとき、この幅Dcは前記距離Daの1.5
倍程度に設定される。なお、前記参照電圧Vrfaは、
Vc/2より高いレベルに設定されている。
The magnetic recording medium 1 shown in FIG. 9 has an N pole and an S pole.
The origin recording signal 2 having a pair of poles is magnetized. The origin signal detection device shown in FIG. 7 has two detection elements Ra and R.
It is composed of a magnetoresistive element 3 which is composed of b and outputs a signal Va, and a comparison circuit 4 which compares the signal Va with a reference voltage Vrfa. In the magnetoresistive element 3, as shown in FIG. 8, one end of each of the detection elements Ra and Rb is connected in series with a power source Vc to form a current path, and the detection elements Ra and Rb are connected.
Are formed in strips and are arranged in parallel with each other. Further, as shown in FIG. 10A, the detection elements Ra and Rb are provided so as to face the magnetic recording medium 1 and are arranged side by side in the moving direction of the magnetic recording medium 1. When the distance between the center lines of the detection elements Ra and Rb is Da and the width of the magnetized portion of the origin recording signal 2 is Dc, the width Dc is 1.5 of the distance Da.
It is set about twice. The reference voltage Vrfa is
It is set to a level higher than Vc / 2.

【0005】この従来の原点信号検出装置では、図10
の(b)に示すような磁気記録媒体1に平行な磁界成分
Hのみを検出素子Ra、Rbが感知し、この磁界成分H
が大きくなるに伴い、図10の(c)に示すように抵抗
値が小さくなる。この図10の(c)は、各検出素子R
a、Rbの抵抗値の変化を示しており、図10の(a)
に示す矢印の向きに磁気記録媒体1を移動させると、検
出素子Ra、Rbの抵抗値は磁気記録媒体1の原点記録
信号2を感知して検出素子Ra、Rbの距離Daに見合
う位相差をもって変化する。検出素子Ra、Rbは図7
に示すように直列接続され、これに電圧Vcが印加され
ているため、Rb>RaのときVa>Vc/2、一方、
Rb<RaのときVa<Vc/2となり、磁気抵抗素子
3の出力信号Vaは図10の(d)のようになる。この
信号Vaと参照電圧Vrfaとを比較回路4で比較する
とき、図10の(e)に示す幅Pのパルス信号が原点信
号として出力される。
In this conventional origin signal detecting device, FIG.
(B), the detecting elements Ra and Rb sense only the magnetic field component H parallel to the magnetic recording medium 1, and the magnetic field component H
As becomes larger, the resistance value becomes smaller as shown in FIG. FIG. 10C shows each detection element R
The change in the resistance value of a and Rb is shown in FIG.
When the magnetic recording medium 1 is moved in the direction indicated by the arrow, the resistance values of the detection elements Ra and Rb have a phase difference corresponding to the distance Da between the detection elements Ra and Rb by sensing the origin recording signal 2 of the magnetic recording medium 1. Change. The detection elements Ra and Rb are shown in FIG.
Since it is connected in series and a voltage Vc is applied to it, Va> Vc / 2 when Rb> Ra, while
When Rb <Ra, Va <Vc / 2, and the output signal Va of the magnetoresistive element 3 becomes as shown in FIG. When the comparison circuit 4 compares the signal Va with the reference voltage Vrfa, a pulse signal having a width P shown in (e) of FIG. 10 is output as the origin signal.

【0006】[0006]

【発明が解決しようとする課題】ところで上述した従来
の原点信号検出装置にあっては、2個の電流通路を有す
る1組の検出素子Ra、Rbの中間点の出力信号Vaか
ら原点信号を得るようになっていることから、図10の
(d)のように、前記出力信号Vaの振幅Bが小さく、
この信号Vaに基づいて得られる原点信号の信号対雑音
比が劣る。
By the way, in the above-mentioned conventional origin signal detecting device, the origin signal is obtained from the output signal Va at the midpoint between the pair of detecting elements Ra and Rb having two current paths. Therefore, as shown in (d) of FIG. 10, the amplitude B of the output signal Va is small,
The signal-to-noise ratio of the origin signal obtained based on this signal Va is poor.

【0007】また、磁気抵抗素子の検出素子の感度およ
び信号磁界の強さはマイナスの温度特性をもっているこ
とから、前記信号Vaの振幅Bもマイナスの温度特性を
もっており、信号Vaは低温時に図11の破線で示すよ
うに振幅Bが大きく、高温時に図11の実線で示すよう
に振幅Bが小さくなり、すなわち信号Vaの振幅は温度
変化により大きく変わる。一方、上述した従来の原点信
号検出装置では、図10の(d)に示す部分Aのよう
に、前記信号Vaの参照電圧Vrfaと交差する立上り
部分および立下がり部分の勾配が緩い。このため、前記
信号Vaと参照電圧Vrfaとの比較の結果、出力され
る原点信号のパルス幅がかなり変化して、図11の示す
ように、低温時にパルス幅Pa、高温時にパルス幅Pb
となり、原点検出の信頼性が損なわれる。
Further, since the sensitivity of the detection element of the magnetoresistive element and the strength of the signal magnetic field have a negative temperature characteristic, the amplitude B of the signal Va also has a negative temperature characteristic, and the signal Va has a low temperature characteristic as shown in FIG. The amplitude B is large as shown by the broken line and becomes small as shown by the solid line in FIG. 11 when the temperature is high, that is, the amplitude of the signal Va largely changes due to temperature change. On the other hand, in the above-described conventional origin signal detecting device, the slope of the rising portion and the falling portion that intersects with the reference voltage Vrfa of the signal Va is gentle as in the portion A shown in FIG. Therefore, as a result of the comparison between the signal Va and the reference voltage Vrfa, the pulse width of the output origin signal changes considerably, and as shown in FIG. 11, the pulse width Pa at low temperature and the pulse width Pb at high temperature.
Therefore, the reliability of origin detection is impaired.

【0008】したがって、上記のように原点信号の信号
対雑音比が劣るとともに原点信号のパルス幅がかなり変
化することから、高性能の検出素子および比較回路を要
し、コストが大きくなるという問題があった。
Therefore, as described above, since the signal-to-noise ratio of the origin signal is inferior and the pulse width of the origin signal changes considerably, there is a problem that a high-performance detecting element and a comparison circuit are required, and the cost increases. there were.

【0009】本発明はこのような従来技術における実情
に鑑みてなされたもので、その目的は、高性能の検出素
子および比較回路を特別に要せずに、原点信号を確実に
検出することのできる原点信号検出装置を提供すること
にある。
The present invention has been made in view of the actual situation in the prior art, and an object thereof is to reliably detect the origin signal without requiring a high-performance detection element and a comparison circuit. An object of the present invention is to provide an origin signal detecting device.

【0010】[0010]

【課題を解決するための手段】この目的を達成するため
に本発明は、磁気記録媒体に着磁された原点記録信号を
検出する複数個の検出素子を備え、該原点記録信号の検
出に応じて原点信号を出力する原点信号検出装置におい
て、それぞれ直列接続された2組の前記検出素子からな
る磁気抵抗素子と、該直列接続された検出素子の各中間
点からそれぞれ出力された信号を差動増幅する差動増幅
回路と、該差動増幅された信号を波形整形して原点信号
を得る比較回路とを設けるとともに、前記原点記録信号
の着磁部分の幅に対する前記検出素子の2組間の距離の
比率を0.3〜0.7のいずれかの値で設定し、さら
に、前記原点記録信号の着磁部分の幅に対する前記検出
素子の2組間の距離の比率を0.5の値で設定した構成
にしてある。
In order to achieve this object, the present invention comprises a plurality of detecting elements for detecting an origin recording signal magnetized on a magnetic recording medium, and responds to the detection of the origin recording signal. In the origin signal detecting device that outputs the origin signal as a differential signal, a magnetoresistive element including two sets of the detecting elements connected in series, and a signal output from each intermediate point of the detecting elements connected in series are differentiated. A differential amplifier circuit for amplifying and a comparator circuit for waveform-shaping the differentially amplified signal to obtain an origin signal are provided, and between the two sets of the detection elements with respect to the width of the magnetized portion of the origin recording signal. The distance ratio is set to any value of 0.3 to 0.7, and the ratio of the distance between the two sets of the detection elements to the width of the magnetized portion of the origin recording signal is set to a value of 0.5. It has the configuration set in.

【0011】[0011]

【作用】本発明は上記のように構成したので、磁気記録
媒体に着磁された原点記録信号を2組の直列接続された
検出素子により検出し、該直列接続された検出素子の各
中間点から出力される信号を差動増幅回路により差動増
幅した後、比較回路により波形整形して原点信号を得
る。上記のように直列接続された検出素子の各中間点か
ら出力される信号を差動増幅回路により差動増幅すると
ともに、前記原点記録信号の着磁部分の幅に対する前記
検出素子の2組間の距離の比率を例えば0.5の値で設
定してあることから、原点記録信号に対応する位置で振
幅の大きく、勾配の急な信号が得られる。これによっ
て、高性能の検出素子および比較回路を特別に要せず
に、原点信号を確実に検出することができる。
Since the present invention is configured as described above, the origin recording signal magnetized on the magnetic recording medium is detected by the two sets of detection elements connected in series, and the intermediate points of the detection elements connected in series are detected. The signal output from is differentially amplified by a differential amplifier circuit, and then waveform-shaped by a comparison circuit to obtain an origin signal. As described above, the signals output from the respective intermediate points of the detection elements connected in series are differentially amplified by the differential amplifier circuit, and the width between the two detection elements with respect to the width of the magnetized portion of the origin recording signal is increased. Since the distance ratio is set to a value of 0.5, for example, a signal having a large amplitude and a steep slope can be obtained at the position corresponding to the origin recording signal. This makes it possible to reliably detect the origin signal without requiring a high-performance detecting element and a comparison circuit.

【0012】[0012]

【実施例】以下、本発明の原点信号検出装置の実施例を
図に基づいて説明する。図1は本発明の原点信号検出装
置の一実施例に備えられる磁気抵抗素子を示す説明図、
図2は本実施例の原点信号検出装置の構成を示す電気回
路図、図3は図2に示す原点信号検出装置に備えられる
差動増幅回路から出力される信号の波形を示す特性図、
図4は実験により求められた原点記録信号上空の磁界分
布を示す特性図、図5は図4に示す磁界分布などから得
られた検出素子のギャップと読取り可能電圧幅との関係
を示す特性図、図6は図5のグラフより得られた磁気抵
抗素子間の距離と許容ギャップ範囲との関係を示す特性
図である。
Embodiments of the origin signal detecting device of the present invention will be described below with reference to the drawings. FIG. 1 is an explanatory view showing a magnetoresistive element provided in an embodiment of the origin signal detecting device of the present invention,
2 is an electric circuit diagram showing the configuration of the origin signal detecting device of the present embodiment, and FIG. 3 is a characteristic diagram showing waveforms of signals output from the differential amplifier circuit provided in the origin signal detecting device shown in FIG.
FIG. 4 is a characteristic diagram showing a magnetic field distribution above the origin recording signal obtained by an experiment, and FIG. 5 is a characteristic diagram showing a relationship between the gap of the detection element and the readable voltage width obtained from the magnetic field distribution shown in FIG. FIG. 6 is a characteristic diagram showing the relationship between the distance between the magnetoresistive elements and the allowable gap range obtained from the graph of FIG.

【0013】図2に示す本実施例の原点信号検出装置
は、直列接続された1組の検出素子MR1、MR2、お
よび直列接続された他の1組の検出素子MR3、MR4
からなる磁気抵抗素子6と、該検出素子MR1、MR2
の中間点、および検出素子MR3、MR4の中間点から
それぞれ出力された信号を差動増幅する差動増幅回路7
と、該差動増幅された信号を波形整形して原点信号を得
る比較回路8とを備えている。
The origin signal detecting apparatus of the present embodiment shown in FIG. 2 has one set of detection elements MR1 and MR2 connected in series and another set of detection elements MR3 and MR4 connected in series.
And the detection elements MR1 and MR2.
Differential amplifier circuit 7 that differentially amplifies the signals respectively output from the intermediate point of 1 and the intermediate points of the detection elements MR3 and MR4.
And a comparison circuit 8 for waveform-shaping the differentially amplified signal to obtain an origin signal.

【0014】図1に示す磁気記録媒体9には、N極とS
極の一対の極を有する原点記録信号10が着磁され、こ
の原点記録信号10の着磁部分の幅Pzは所定寸法、例
えば100μmに設定される。該磁気記録媒体9に対し
て前記検出素子MR1〜MR4が順次配列され、前記幅
Pzに対する検出素子MR1〜MR4の2組間の距離、
すなわち隣合う検出素子MR2、MR3間の距離Dyの
比率は、0.35〜0.7のいずれかの値、例えば0.
5の値で設定されている。また、一方の組のMR1、M
R2間の距離Dx1、および他方の組のMR3、MR4
間の距離Dx2は、それぞれ前記幅Pzに対して0.8
〜1.2倍、例えば等倍で設定されている。
The magnetic recording medium 9 shown in FIG. 1 has an N pole and an S pole.
The origin recording signal 10 having a pair of poles is magnetized, and the width Pz of the magnetized portion of the origin recording signal 10 is set to a predetermined dimension, for example, 100 μm. The detection elements MR1 to MR4 are sequentially arranged on the magnetic recording medium 9, and a distance between two sets of the detection elements MR1 to MR4 with respect to the width Pz,
That is, the ratio of the distance Dy between the adjacent detection elements MR2 and MR3 is any value from 0.35 to 0.7, for example, 0.
It is set with a value of 5. Also, one pair of MR1 and M
The distance Dx 1 between R2 and the other pair of MR3, MR4
The distance Dx 2 between them is 0.8 with respect to the width Pz.
.About.1.2 times, for example, the same size is set.

【0015】この実施例にあっては、磁気記録媒体9に
着磁された原点記録信号10を2組の直列接続された検
出素子MR1〜MR4により検出し、該検出素子MR
1、MR2の中間点、および検出素子MR3、MR4の
中間点からそれぞれ出力された信号を差動増幅回路7に
より差動増幅した後、比較回路8により波形整形して原
点信号を得るようになっている。
In this embodiment, the origin recording signal 10 magnetized on the magnetic recording medium 9 is detected by two sets of detecting elements MR1 to MR4 connected in series, and the detecting element MR is detected.
The differential amplifier circuit 7 differentially amplifies the signals output from the midpoints of 1 and MR2 and the midpoints of the detection elements MR3 and MR4, and then the waveform is shaped by the comparison circuit 8 to obtain the origin signal. ing.

【0016】上述した幅Pzに対する距離Dyの比率
は、該距離Dyを例えば0、0.3Pz、0.5Pz、
0.7Pz、1.0Pzの5種類に設定して、次のよう
な手順で実験結果に基づき比較検討することができる。
すなわち、第1の手順として磁気記録媒体9の表面に1
個の検出素子いわゆるMRセンサを配置し、磁気記録媒
体9を回転させて、検出素子の抵抗変化を読み取り、原
点記録信号10上空の磁界分布を測定する。このとき、
抵抗変化率3%、感度30 Oeの検出素子を用い、アン
プの増幅率を30倍に設定し、磁気記録媒体9と検出素
子とのギャップを40μmから160μmまで20μm
おきに設定し、空間の磁界分布を測定した。その後、D
yの値を0〜1.0Pzまで変化させて得られる原点信
号をシュミレーションで求めたものが図4である。な
お、図4の(a)、(b)、(c)は距離Dyをそれぞ
れ0、0.5Pz、1.0Pzに設定してある。
The ratio of the distance Dy to the width Pz described above is such that the distance Dy is 0, 0.3 Pz, 0.5 Pz,
Five types of 0.7 Pz and 1.0 Pz can be set, and comparative examination can be performed based on experimental results in the following procedure.
That is, as the first procedure, 1 is applied to the surface of the magnetic recording medium 9.
A single detection element, a so-called MR sensor, is arranged, the magnetic recording medium 9 is rotated, the resistance change of the detection element is read, and the magnetic field distribution above the origin recording signal 10 is measured. At this time,
A detection element having a resistance change rate of 3% and a sensitivity of 30 Oe was used, the amplification factor of the amplifier was set to 30 times, and the gap between the magnetic recording medium 9 and the detection element was 20 μm from 40 μm to 160 μm.
It was set every other time and the magnetic field distribution in the space was measured. Then D
FIG. 4 shows the origin signal obtained by changing the value of y from 0 to 1.0 Pz by simulation. In FIGS. 4A, 4B, and 4C, the distance Dy is set to 0, 0.5 Pz, and 1.0 Pz, respectively.

【0017】第2の手順として、一般に磁気式エンコー
ダの原点信号のパルス幅Dzは、0.5Pz以上かつ
1.5Pz以下であることが要求されるので、図3に示
すように、Dz(min)=0.5Pz、Dz(ma
x)=1.5Pzになるように作図することにより、図
4の(a)、(b)、(c)などの磁界分布から読取り
可能電圧幅を測定する。その結果、上記のように磁気記
録媒体9と検出素子とのギャップを40μmで設定した
場合、距離Dy=0では1.1V、距離Dy=0.5P
zでは1.0V、距離Dy=1.0Pzでは0Vとな
る。このようにして得た読取り可能電圧幅を横軸方向に
とり、ギャップを縦軸方向にとると、距離Dyがそれぞ
れ0、0.3Pz、0.5Pz、0.7Pz、1.0P
zの場合の読取り可能電圧幅は、図5に示すように作図
される。
As the second procedure, the pulse width Dz of the origin signal of the magnetic encoder is generally required to be 0.5 Pz or more and 1.5 Pz or less, so that as shown in FIG. 3, Dz (min ) = 0.5 Pz, Dz (ma
By plotting so that x) = 1.5 Pz, the readable voltage width is measured from the magnetic field distributions of FIG. 4A, FIG. 4B, and FIG. As a result, when the gap between the magnetic recording medium 9 and the detection element is set to 40 μm as described above, 1.1 V at the distance Dy = 0 and the distance Dy = 0.5P
It is 1.0 V for z and 0 V for the distance Dy = 1.0 Pz. When the readable voltage width thus obtained is taken in the horizontal axis direction and the gap is taken in the vertical axis direction, the distance Dy is 0, 0.3 Pz, 0.5 Pz, 0.7 Pz, 1.0 P, respectively.
The readable voltage range for z is plotted as shown in FIG.

【0018】一般に、上記の読取り可能電圧幅が大きい
場合、ドリフト特性の悪い安価なIC、センサを用いる
ことができることから設計上望ましく、また、上記の検
出素子の磁気記録媒体との許容ギャップ範囲が広いと、
比較的大きな部品公差で設計でき、組立が容易であるこ
とから設計上望ましい。そこで、第3の手順として、読
取り可能電圧幅を0.8V、1.1V、1.4Vに設定
して図5のグラフより許容ギャップ範囲を測定する。そ
の結果、距離Dyを横軸方向に、許容ギャップ範囲を縦
軸方向にとると、読取り可能電圧幅がそれぞれ0.8
V、1.1V、1.4Vの場合の許容ギャップ範囲は、
図6に示すように作図される。したがって、この図6の
グラフを検討すると、許容ギャップ範囲が比較的良好な
のは0.35Pz≦距離Dy≦0.7Pz、また、特に
良好なのは距離Dy=0.5Pzである。したがって、
上述したように距離Dyを例えば0.5Pzの値で設定
するようになっている。
Generally, when the readable voltage width is large, it is desirable in design because an inexpensive IC and sensor having poor drift characteristics can be used, and the allowable gap range of the detection element with respect to the magnetic recording medium is large. Wide,
It is desirable in terms of design because it can be designed with relatively large component tolerances and is easy to assemble. Therefore, as the third procedure, the readable voltage range is set to 0.8V, 1.1V, and 1.4V, and the allowable gap range is measured from the graph of FIG. As a result, when the distance Dy is set in the horizontal axis direction and the allowable gap range is set in the vertical axis direction, the readable voltage width is 0.8.
The allowable gap range for V, 1.1V, 1.4V is
It is constructed as shown in FIG. Therefore, considering the graph of FIG. 6, the allowable gap range is relatively good at 0.35 Pz ≦ distance Dy ≦ 0.7 Pz, and particularly good is the distance Dy = 0.5 Pz. Therefore,
As described above, the distance Dy is set to a value of 0.5 Pz, for example.

【0019】このように構成した実施例では、直列接続
された1組の検出素子MR1、MR2、および直列接続
された他の1組の検出素子MR3、MR4の各中間点か
ら出力される信号を差動増幅回路7により差動増幅する
とともに、原点記録信号10の着磁部分の幅Pzに対す
る検出素子MR2、MR3間の距離Dyの比率を例えば
0.5の値で設定してあることから、原点記録信号10
に対応する位置で振幅の大きく、勾配の急な信号が得ら
れ、これによって、高性能の検出素子および比較回路を
特別に要せずに、原点信号を確実に検出することができ
る。なお、本実施例では距離Dyを例えば0.5Pzに
設定したが、必要に応じて、該距離Dyを0.35Pz
〜0.7Pzのいずれかに設定することもできる。さら
に、本実施例では距離Dx1、Dx2をそれぞれ1Pzで
設定したが、必要に応じて、距離Dx1、Dx2を0.8
Pz〜1.2Pzのいずれかに設定することもでき、こ
のことは上記と同様の実験によって確かめることができ
る。
In the embodiment thus constructed, the signals output from the respective intermediate points of the one set of detection elements MR1 and MR2 connected in series and the other one set of detection elements MR3 and MR4 connected in series are transmitted. Since the differential amplification circuit 7 performs differential amplification and the ratio of the distance Dy between the detection elements MR2 and MR3 to the width Pz of the magnetized portion of the origin recording signal 10 is set to a value of 0.5, for example, Origin recording signal 10
A signal having a large amplitude and a steep slope is obtained at a position corresponding to, which enables reliable detection of the origin signal without specially requiring a high-performance detection element and a comparison circuit. Although the distance Dy is set to 0.5 Pz in this embodiment, the distance Dy is set to 0.35 Pz as necessary.
It can also be set to any of .about.0.7 Pz. Further, in the present embodiment, the distances Dx 1 and Dx 2 are set to 1 Pz, but the distances Dx 1 and Dx 2 are set to 0.8 as required.
It can be set to any of Pz to 1.2Pz, and this can be confirmed by the same experiment as above.

【0020】[0020]

【発明の効果】本発明は以上のように構成したので、高
性能の検出素子および比較回路を特別に要せずに、原点
信号を確実に検出することができ、したがって、エンコ
ーダの製造時の許容誤差範囲が広くて製造が容易である
とともに、部品コストの低減を図ることができる。
Since the present invention is configured as described above, the origin signal can be reliably detected without specially requiring a high-performance detecting element and a comparison circuit. The allowable error range is wide and the manufacturing is easy, and the cost of parts can be reduced.

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

【図1】本発明の原点信号検出装置の一実施例に備えら
れる磁気抵抗素子を示す説明図である。
FIG. 1 is an explanatory diagram showing a magnetoresistive element included in an embodiment of an origin signal detection device of the present invention.

【図2】本実施例の原点信号検出装置の構成を示す電気
回路図である。
FIG. 2 is an electric circuit diagram showing a configuration of an origin signal detection device of the present embodiment.

【図3】図2に示す原点信号検出装置に備えられる差動
増幅回路から出力される信号の波形を示す特性図であ
る。
3 is a characteristic diagram showing a waveform of a signal output from a differential amplifier circuit included in the origin signal detection device shown in FIG.

【図4】図4は実験により求められた原点記録信号上空
の磁界分布を示す特性図である。
FIG. 4 is a characteristic diagram showing a magnetic field distribution above the origin recording signal obtained by an experiment.

【図5】図4に示す磁界分布などから得られた検出素子
のギャップと読取り可能電圧幅との関係を示す特性図で
ある。
5 is a characteristic diagram showing a relationship between a gap of a detection element and a readable voltage width obtained from the magnetic field distribution shown in FIG.

【図6】図5のグラフより得られた磁気抵抗素子間の距
離と許容ギャップ範囲との関係を示す特性図である。
6 is a characteristic diagram showing a relationship between a distance between magnetoresistive elements and an allowable gap range obtained from the graph of FIG.

【図7】従来の磁気式エンコーダの原点信号検出装置を
示す電気回路図である。
FIG. 7 is an electric circuit diagram showing a conventional origin signal detection device for a magnetic encoder.

【図8】図7の原点信号検出装置に備えられる磁気抵抗
素子の構成を示す図である。
8 is a diagram showing a configuration of a magnetoresistive element included in the origin signal detection device of FIG.

【図9】図8の磁気抵抗素子が対向する磁気記録媒体の
原点記録信号の着磁部分を示す斜視図である。
9 is a perspective view showing a magnetized portion of the origin recording signal of the magnetic recording medium facing the magnetoresistive element of FIG. 8;

【図10】図7の原点信号検出装置の動作を示すタイミ
ングチャートである。
10 is a timing chart showing the operation of the origin signal detection device of FIG.

【図11】図7の原点信号検出装置の問題点を説明する
ためのタイミングチャートである。
11 is a timing chart for explaining a problem of the origin signal detection device of FIG.

【符号の説明】[Explanation of symbols]

6 磁気抵抗素子 7 差動増幅回路 8 比較回路 9 磁気記録媒体 10 原点記録信号 MR1〜MR4 検出素子 6 Magnetoresistive Element 7 Differential Amplifier Circuit 8 Comparison Circuit 9 Magnetic Recording Medium 10 Origin Recording Signal MR1 to MR4 Detection Element

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 磁気記録媒体に着磁された原点記録信号
を検出する複数個の検出素子を備え、該原点記録信号の
検出に応じて原点信号を出力する原点信号検出装置にお
いて、それぞれ直列接続された2組の前記検出素子から
なる磁気抵抗素子と、該直列接続された検出素子の各中
間点からそれぞれ出力された信号を差動増幅する差動増
幅回路と、該差動増幅された信号を波形整形して原点信
号を得る比較回路とを設けるとともに、前記原点記録信
号の着磁部分の幅に対する前記検出素子の2組間の距離
の比率を0.3〜0.7のいずれかの値で設定したこと
を特徴とする原点信号検出装置。
1. An origin signal detecting device, comprising a plurality of detection elements for detecting origin recording signals magnetized to a magnetic recording medium, and outputting origin signals in response to detection of the origin recording signals. And a differential amplifier circuit for differentially amplifying signals output from respective intermediate points of the detection elements connected in series, and the differentially amplified signal. And a comparison circuit for waveform-shaping the origin signal to obtain the origin signal, and the ratio of the distance between the two sets of the detection elements to the width of the magnetized portion of the origin recording signal is 0.3 to 0.7. An origin signal detection device characterized by being set by a value.
【請求項2】 磁気記録媒体に着磁された原点記録信号
を検出する複数個の検出素子を備え、該原点記録信号の
検出に応じて原点信号を出力する原点信号検出装置にお
いて、それぞれ直列接続された2組の前記検出素子から
なる磁気抵抗素子と、該直列接続された検出素子の各中
間点からそれぞれ出力された信号を差動増幅する差動増
幅回路と、該差動増幅された信号を波形整形して原点信
号を得る比較回路とを設けるとともに、前記原点記録信
号の着磁部分の幅に対する前記検出素子の2組間の距離
の比率を0.5の値で設定したことを特徴とする原点信
号検出装置。
2. An origin signal detecting device comprising a plurality of detecting elements for detecting origin recording signals magnetized to a magnetic recording medium, and outputting origin signals in response to the detection of the origin recording signals. And a differential amplifier circuit for differentially amplifying signals output from respective intermediate points of the detection elements connected in series, and the differentially amplified signal. And a comparison circuit that obtains an origin signal by waveform shaping, and the ratio of the distance between the two sets of the detection elements to the width of the magnetized portion of the origin recording signal is set to a value of 0.5. Origin signal detector.
JP03067592A 1992-02-18 1992-02-18 Origin signal detector Expired - Fee Related JP3195019B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP03067592A JP3195019B2 (en) 1992-02-18 1992-02-18 Origin signal detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP03067592A JP3195019B2 (en) 1992-02-18 1992-02-18 Origin signal detector

Publications (2)

Publication Number Publication Date
JPH05223592A true JPH05223592A (en) 1993-08-31
JP3195019B2 JP3195019B2 (en) 2001-08-06

Family

ID=12310292

Family Applications (1)

Application Number Title Priority Date Filing Date
JP03067592A Expired - Fee Related JP3195019B2 (en) 1992-02-18 1992-02-18 Origin signal detector

Country Status (1)

Country Link
JP (1) JP3195019B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009116365A1 (en) * 2008-03-17 2009-09-24 三菱電機株式会社 Origin position signal detector

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2009116365A1 (en) * 2008-03-17 2009-09-24 三菱電機株式会社 Origin position signal detector
DE112009000497T5 (en) 2008-03-17 2011-04-21 Mitsubishi Electric Corp. Origin position signal detector

Also Published As

Publication number Publication date
JP3195019B2 (en) 2001-08-06

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