JPH0222510A - Magnetic sensor - Google Patents

Magnetic sensor

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Publication number
JPH0222510A
JPH0222510A JP63172417A JP17241788A JPH0222510A JP H0222510 A JPH0222510 A JP H0222510A JP 63172417 A JP63172417 A JP 63172417A JP 17241788 A JP17241788 A JP 17241788A JP H0222510 A JPH0222510 A JP H0222510A
Authority
JP
Japan
Prior art keywords
disk
magnetic
deltar
resistance
resistance value
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
JP63172417A
Other languages
Japanese (ja)
Inventor
Yoshiaki Ichikawa
義明 市川
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.)
Proterial Ltd
Original Assignee
Hitachi Metals 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 Metals Ltd filed Critical Hitachi Metals Ltd
Priority to JP63172417A priority Critical patent/JPH0222510A/en
Priority to US07/361,202 priority patent/US5057678A/en
Publication of JPH0222510A publication Critical patent/JPH0222510A/en
Pending legal-status Critical Current

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  • Transmission And Conversion Of Sensor Element Output (AREA)
  • Measuring Magnetic Variables (AREA)
  • Lens Barrels (AREA)
  • Automatic Focus Adjustment (AREA)

Abstract

PURPOSE:To nearly eliminate variation in the amplitude of an output signal and to improve the stability of the output signal by arranging magnetism sensing parts at constant intervals to the entire periphery radially from a center of rotation. CONSTITUTION:The distance between the surface of a sensor element 1 and the surface of a disk 2 varies owing to the play of the disk surface in the direction of the rotary shaft 3 as the disk rotates. For example, when the disk approaches magnetism sensing parts 9a and 9h, their resistance values vary by DELTAr+DELTAR. (DELTAr is the quantity of resistance abnormal variation due to the approach of the disk and DELTAR is the quantity of resistance value variation due to normal magneto-resistance effect). Further, resistances 9d and 9e which are at positions of point symmetry about the rotary shaft 3 vary in resistance value by -DELTAr+DELTAR. Then the total of the resistance value variation of the magnetism sensing part resistances 8 and 9 is overall resistance value variation. The output of the element 1 is determined depending upon only DELTAR, so a signal with a constant amplitude is obtained finally.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、磁気式のエンコーダ、タコジェネレータにお
いて用いられる磁気式センサのうち、磁気抵抗変化型磁
気センサに関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a variable magnetoresistive magnetic sensor among magnetic sensors used in magnetic encoders and tacho generators.

〔従来の技術〕[Conventional technology]

磁気抵抗型磁気センサ(以下磁気センサと略す)は、外
部磁界の変化により抵抗値が変化することを利用して周
期的な磁界変化を出力電圧の変化に変換する素子である
(例えば特願昭48−79655号公報参照)。周期的
な磁界変化を発生させる回転体としては、例えは第9図
に示すような磁気ドラム、あるいは第8図に示すような
磁気ディスクが知られている。磁気ドラム型では、回転
軸方向の厚さが増加するため、小型化には不向きであシ
、磁気ディスク型回転体が望ましい。磁気ディスクを用
いた磁気センサでは、ディスクの一部の面に対向してセ
ンサ素子を固定し、ディスク面からの磁界の変化を検出
する方式が用いられていた(第8因)0 〔発明が解決しようとする課題〕 上記の構造を持つ磁気センサでは、回転磁気ディスクと
回転軸のズレにより、ディスクの回転に伴い、ディスク
面が回転軸方向に変動する。従って、磁気センサ素子と
ディスク面との距離が常に変動する。第6図では、ディ
スク面とセンサ間距離が小さく、センサ素子は振幅の大
きい信号を出力する。第7図では、ディスク面とセンサ
素子の距離が大きく、センサ素子の受ける磁界が弱いた
め、出力信号振幅が小さい。ディスク回転に伴い第6図
と第7図の場合が交互に生じ、センサ素子からの信号出
力は富に振幅の変動を持ち、一定振幅の出力信号が取り
出せないという問題点があった0 本発明の目的は、上記の様な出力振幅変動を持たず、常
に一定の振幅を持つ出力信号を発生させることができる
磁気センサを提供することである。
A magnetoresistive magnetic sensor (hereinafter abbreviated as magnetic sensor) is an element that converts periodic changes in magnetic field into changes in output voltage by utilizing changes in resistance due to changes in external magnetic field. 48-79655). As a rotating body that generates periodic magnetic field changes, for example, a magnetic drum as shown in FIG. 9 or a magnetic disk as shown in FIG. 8 are known. A magnetic drum type rotating body increases the thickness in the direction of the rotating shaft and is not suitable for miniaturization, so a magnetic disk type rotating body is preferable. In magnetic sensors using magnetic disks, a method was used in which a sensor element was fixed opposite a part of the disk surface to detect changes in the magnetic field from the disk surface (factor 8)0. Problems to be Solved] In the magnetic sensor having the above structure, the disk surface fluctuates in the direction of the rotation axis as the disk rotates due to misalignment between the rotating magnetic disk and the rotation axis. Therefore, the distance between the magnetic sensor element and the disk surface constantly changes. In FIG. 6, the distance between the disk surface and the sensor is small, and the sensor element outputs a signal with a large amplitude. In FIG. 7, the distance between the disk surface and the sensor element is large and the magnetic field received by the sensor element is weak, so the output signal amplitude is small. As the disk rotates, the cases shown in FIG. 6 and FIG. 7 occur alternately, and the signal output from the sensor element has a large amplitude fluctuation, and there is a problem that an output signal with a constant amplitude cannot be obtained. The object of the present invention is to provide a magnetic sensor that does not have the above-mentioned output amplitude fluctuations and can generate an output signal that always has a constant amplitude.

〔課題を解決するための手段〕[Means to solve the problem]

本発明は、センサ素子の感磁部をディスク面に対向する
支持体の一周全体にわたり、回転中心に対して放射状に
所定のピッチで配置することを特徴とする磁気式センサ
である。磁気抵抗型磁気センサの場合、センサ素子内に
は感磁部抵抗が設けられておp1外部磁界の変化により
この抵抗値が変化する。ひとつの抵抗を分割してディス
ク面に対向する支持体の一周全体に配置することにより
、仮に回転中にディスクの片方の端部がセンサ素子に接
近しても、それと点対称な位置にある端部では逆に離れ
てしまう。センサ素子の受ける磁界の大きさは、ディス
ク面からセンサ素子までの距離に比例し、しかも抵抗値
変化も磁界の大きさに比例する。従って、ディスクとセ
ンサ間距離の大きい所での抵抗値変化は小さく、距離の
小さい所では変化は大きい。しかしこれらの抵抗が、ひ
とつの長い抵抗の一部として形成されているため、この
長い抵抗全体としては、抵抗値の変化は常に一定に保た
れる。それ故、この長い抵抗全体から生じる磁気抵抗変
化は一定に保たれ、出力振幅も常に一定となる。
The present invention is a magnetic sensor characterized in that the magnetically sensitive parts of the sensor element are arranged radially at a predetermined pitch with respect to the center of rotation over the entire circumference of a support facing the disk surface. In the case of a magnetoresistive magnetic sensor, a magnetically sensitive portion resistance is provided within the sensor element, and the value of this resistance changes with changes in the external magnetic field p1. By dividing one resistor and placing it around the entire circumference of the support facing the disk surface, even if one end of the disk approaches the sensor element during rotation, the end that is symmetrical to that On the contrary, they drift apart in the club. The magnitude of the magnetic field received by the sensor element is proportional to the distance from the disk surface to the sensor element, and the change in resistance value is also proportional to the magnitude of the magnetic field. Therefore, the change in resistance value is small where the distance between the disk and the sensor is large, and the change is large where the distance is small. However, since these resistors are formed as part of one long resistor, the change in resistance value of this long resistor as a whole always remains constant. Therefore, the magnetoresistance change resulting from this entire long resistance remains constant and the output amplitude is always constant.

〔実施例〕〔Example〕

第1図に本発明の実施例を示す。8aから8h及び9a
から9hは磁気抵抗変化型の感磁部で、これらは薄膜や
細線を用いて形成されている。電圧印加用端子4から接
地用端子5までの間に、8aから8h及び9aから9h
の感磁部は夫々抵抗として直列に接続されている。これ
らの配線は通常ガラスを九は有機物樹脂またはセラミッ
クからなる支持体26上に形成されているが、金属を支
持体26として用いる場合には、配線と支持体260間
に絶縁物を介装する。4と5の配線の中間地点に信号出
力端子6が設けられている。一方、回転するディスク状
回転板には第2図中の2の様に一定のトラック幅でN極
とS極が局方向に沿って交互に着磁されておシ、−周あ
えりの極数は2から5000極の範囲の所定の極数とな
っている。N極とS極間距離を着磁ピッチとすると、感
磁部抵抗8aから8hは互いにそのピッチが着磁ピッチ
の整数倍になっており、感磁部抵抗9aから9hkおい
ても互いに同様の配置関係になりている。
FIG. 1 shows an embodiment of the present invention. 8a to 8h and 9a
to 9h are magnetoresistive magnetic sensing parts, which are formed using thin films or thin wires. Between the voltage application terminal 4 and the grounding terminal 5, from 8a to 8h and from 9a to 9h
The magnetic sensing parts of each are connected in series as a resistor. These wirings are usually formed on a support 26 made of glass, organic resin, or ceramic, but when metal is used as the support 26, an insulator is interposed between the wiring and the support 260. . A signal output terminal 6 is provided at an intermediate point between the wirings 4 and 5. On the other hand, as shown in 2 in Figure 2, the rotating disc-shaped rotating plate has N and S poles alternately magnetized along the local direction with a constant track width. The number is a predetermined number of poles ranging from 2 to 5000 poles. If the distance between the north pole and the south pole is the magnetized pitch, the pitch of the magnetically sensitive part resistors 8a to 8h is an integral multiple of the magnetized pitch, and the pitch of the magnetically sensitive part resistors 9a to 9hk is also similar to each other. It has to do with placement.

ただし8aから8hの中のひとつの感磁部抵抗と9aか
ら9hの中のひとつの抵抗とは常に互いに(η十η)λ
(η:整数、λ:着磁ピッチ)の位置関係となっている
。着磁されたディスク板を回転させて信号を取り出す場
合、第2図の様にディスク板とセンサ素子を対向させ、
10μmから3′x。
However, one of the magnetic sensing part resistances from 8a to 8h and one of the resistances from 9a to 9h are always mutually (η+η)λ
The positional relationship is (η: integer, λ: magnetization pitch). When rotating a magnetized disk plate to extract a signal, the disk plate and sensor element are placed opposite each other as shown in Figure 2.
3′x from 10μm.

までの間の所定の距離だけ離して設置する。ディスク板
の回転に伴い、第5図の様に、ディスク面の回転軸方向
のガタによりセンサ素子面とディスク面の距離が変化す
る。例えは第5図の様にディスク板が感磁部抵抗9aお
よび9hに接近した場合、これらの抵抗値は△r+△R
だけ変化する。
Install them at a specified distance from each other. As the disk plate rotates, as shown in FIG. 5, the distance between the sensor element surface and the disk surface changes due to play in the direction of the rotation axis of the disk surface. For example, when the disk plate approaches the magnetically sensitive resistors 9a and 9h as shown in Figure 5, these resistance values are △r + △R.
only changes.

△rはディスク板が接近したことによる抵抗異常変化量
、△Rは通常の磁気抵抗効果による抵抗値変化量である
。△Rは感磁部を構成する材料の物性により正又は負の
値をとる。一方、これらと回転軸に対して点対称の位置
にある抵抗9dおよび9eでは抵抗値は−△r+△Rだ
け変化する。端子5と端子6間においては、各感磁部抵
抗の抵抗値変化の総和が全体としての抵抗値変化となシ
現れる。この合計は、次の様になる。
Δr is the amount of abnormal change in resistance due to the approach of the disk plate, and ΔR is the amount of change in resistance value due to the normal magnetoresistive effect. ΔR takes a positive or negative value depending on the physical properties of the material constituting the magnetically sensitive part. On the other hand, the resistance values of the resistors 9d and 9e, which are located point-symmetrically to these with respect to the rotation axis, change by -Δr+ΔR. Between the terminal 5 and the terminal 6, the sum of the resistance value changes of the respective magnetically sensitive portion resistances appears as the overall resistance value change. This total is as follows.

2(△r+△R)+2(−△r+△R)+4△R=8八
Rすなわちディスク板回転時のガタに基ずく抵抗値変化
△rの影響は、互いに中心に対して点対称の位置にある
抵抗の異常変化量が相殺するため、全体の抵抗値変化量
としては含まれてこない。材料の物性により決まる一定
変化量△Rのみが出現する。センサ素子からの出力は結
果としてこの△Rのみに依存して決まるので、最終的に
一定振幅の信号が得られる。同様の効果は端子4と端子
6間にある感磁部抵抗8aから8hまでについても生じ
る。従って信号出力には抵抗8 a −8hと抵抗9 
a −9h間の位相差のみが現れ、振幅も一定のため出
力として十分に安定な信号となる。
2 (△r + △R) + 2 (-△r + △R) + 4 △R = 88R In other words, the influence of resistance change △r due to the backlash during rotation of the disk plate is due to the influence of △r on points symmetrical to each other with respect to the center. This is not included in the overall resistance value change because the abnormal change in resistance cancels it out. Only a constant variation ΔR determined by the physical properties of the material appears. Since the output from the sensor element ultimately depends only on this ΔR, a signal with a constant amplitude is finally obtained. A similar effect also occurs for the magnetically sensitive resistors 8a to 8h located between the terminals 4 and 6. Therefore, for signal output, resistor 8a-8h and resistor 9
Only the phase difference between a and 9h appears and the amplitude is constant, resulting in a sufficiently stable signal as an output.

第3図は2a!類の信号(A相出力およびB相出力)を
取り出すことのできる磁気センサ素子の実施例である。
Figure 3 is 2a! This is an example of a magnetic sensor element that can extract similar signals (A-phase output and B-phase output).

素子内には感磁部抵抗として14a〜14hおよび15
a〜15h、16a〜16h、17a〜17hの4種が
あり、人相出力は抵抗16a〜16hと17a〜17h
の直列接続において三端子出力として信号端子18から
敗り出せる〇一方B相出力は抵抗14a〜14hと15
a〜15hの直列接続において三端子出力として信号端
子19から取り出せる。A相とB相信号は互いに位相差
が電気角で90度の関係にある。人相又はB相それぞれ
についての信号の発生する機構は第1図における実施例
の場合と同様でろる。
Inside the element, there are resistors 14a to 14h and 15 as magnetically sensitive parts.
There are four types: a to 15h, 16a to 16h, and 17a to 17h, and the physiognomic output is resistor 16a to 16h and 17a to 17h.
In the series connection of
When a to 15h are connected in series, it can be taken out from the signal terminal 19 as a three-terminal output. The A-phase and B-phase signals have a phase difference of 90 degrees in electrical angle. The mechanism for generating signals for the human phase or B phase, respectively, is the same as in the embodiment shown in FIG.

第4図はブリッジ回路を取り入れた場合の磁気センサ実
施例である。感磁部抵抗の配置は、抵抗20a〜20h
と21a 〜21hの位相差が、(η+1/12)λ(
η:整数、λ:Jf磁ピッチ)となりており、抵抗22
a〜22hと抵抗23a〜23hの関係も一様である。
FIG. 4 shows an example of a magnetic sensor incorporating a bridge circuit. The arrangement of the magnetic sensing part resistors is resistors 20a to 20h.
The phase difference between and 21a to 21h is (η+1/12)λ(
η: integer, λ: Jf magnetic pitch), and the resistance is 22
The relationship between a to 22h and resistors 23a to 23h is also the same.

一方、抵抗20a 〜20hと抵抗23a 〜23hは
全く同位相の信号を得る様な配置であり、抵抗21a〜
21hと抵抗22a〜22hの関係も同機である。
On the other hand, the resistors 20a to 20h and the resistors 23a to 23h are arranged so as to obtain signals of exactly the same phase, and the resistors 21a to 20h are arranged so as to obtain signals of exactly the same phase.
The relationship between 21h and resistors 22a to 22h is also the same.

ブリッジ回路を用いることにより、素子の周囲温度に対
する安定性を高めることができ、しかも出力信号の珈幅
を実施例第1図又は第3図の場合に比べて2倍に増大さ
せることができる。第1図。
By using the bridge circuit, it is possible to improve the stability of the element with respect to the ambient temperature, and moreover, the amplitude of the output signal can be doubled compared to the case of the embodiments shown in FIGS. 1 and 3. Figure 1.

第6図、第4図の実施例のどの場合においても、感磁部
抵抗が回転ディスク板の一周にわたりて配置されている
ので、振幅変動のない安定した信号出力が得られる。第
4図の実施例において、A相およびB相の信号出力を取
り出す場合には、さらに32本のg′g1部抵抗全抵抗
し、それぞれの位相関係が第1図および第3図の実施例
の条件を満たす配置とすることで得られる。第1図、第
6図。
In either of the embodiments shown in FIGS. 6 and 4, since the magnetically sensitive resistors are arranged around the entire circumference of the rotating disk plate, stable signal output without amplitude fluctuations can be obtained. In the embodiment shown in FIG. 4, when taking out the A-phase and B-phase signal outputs, 32 g'g1 part resistors are added in total, and the phase relationship between them is the same as in the embodiment shown in FIGS. 1 and 3. This can be obtained by arranging a configuration that satisfies the following conditions. Figures 1 and 6.

第4図の実施例の場合には、ひとつの感磁部抵抗を8分
割している。例えば第1図において8a〜8hの8本に
分割している。この分割数は大きい程、振幅の安定した
出力信号を取シ出すことができ、しかも全体の抵抗値を
大きく出来るので、低油*’nt、力の磁気センサを実
現することができる0〔発明の効果〕 本発明によれば、回転磁気ディスクを用いた磁気センサ
において、従来達成できなかった、出力係号の振幅変動
をはぼ零にすることができ、出力信号の安定性に著しい
向上が達成できる。
In the case of the embodiment shown in FIG. 4, one magnetically sensitive portion resistance is divided into eight parts. For example, in FIG. 1, it is divided into eight parts 8a to 8h. The larger the number of divisions, the more stable the amplitude of the output signal can be obtained, and the greater the overall resistance value, making it possible to realize a magnetic sensor with low oil *'nt and force. Effects] According to the present invention, in a magnetic sensor using a rotating magnetic disk, it is possible to reduce the amplitude fluctuation of the output coefficient to almost zero, which could not be achieved in the past, and the stability of the output signal is significantly improved. It can be achieved.

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

第1図は本発明に係る磁気センサ素子の一実施例を示す
平面図、第2図は本発明による磁気センサ素子と回転磁
気ディスクの組立て図、第6図は本発明による他の実施
例の平面図、第4図は不発・明による他の実施例の平面
図、第5図は本発明の実施例のための説明図、第6図お
よび第7図は従来のセンサの問題点を示す説明図、第8
図および第9図は従来の磁気センサの構成図である。 1:磁気センサ素子  2:回転磁′気ディスク3:回
転軸      4:N、源端子5:接地端子    
 6:信号出力端子7:回転磁気ドラム 8.9.14〜17.20〜26:感磁部抵抗10〜1
6:配籾用パターン 18.19.24.25 :信号出力端子第 1 図 12番 6椙号ボtJ搗チ 8厳宴卦琢洸 9   / 26支片体 ′$ 3 図 4@;7i搗子 5鋒輩端子 14 I7E、rat+rxm 194富号用搗子 ′I$2  図 1  h軌気jゴン“す′11子 2 回@h^気ディスク 3 回Mす由 4 電諏鳩子 5接jf!!tI4I子 6イぢ号里t3f&子 8屑1逗身ド抵抗 9    〃 26 表1今休 第4 図 4 tオ鍋子 5才妾少f#i予 24 516jA1’An淘蛤f 25 三J高子A2ボカJ扇子 第 5 目 石劫J氏でンブJ1子 回季九ωに一テ)スフ 回転軸 電汎鴻子 S燻訪千 6信号ムカ搗子 8慮風部為札 9   〃 26  交將体 第 6 図 第7 図 1 万1餓、こンブー先子 2 瓜■嗅請気デン又り 3回軒軸 6郡号瓜ny鵡子
FIG. 1 is a plan view showing one embodiment of the magnetic sensor element according to the present invention, FIG. 2 is an assembled diagram of the magnetic sensor element and rotating magnetic disk according to the present invention, and FIG. 6 is a plan view showing another embodiment of the magnetic sensor element according to the present invention. 4 is a plan view of another embodiment of the invention, FIG. 5 is an explanatory diagram for the embodiment of the present invention, and FIGS. 6 and 7 show problems with conventional sensors. Explanatory diagram, No. 8
9 and 9 are configuration diagrams of a conventional magnetic sensor. 1: Magnetic sensor element 2: Rotating magnetic disk 3: Rotating shaft 4: N, source terminal 5: Ground terminal
6: Signal output terminal 7: Rotating magnetic drum 8.9.14~17.20~26: Magnetic sensing part resistance 10~1
6: Pattern for paddy arrangement 18.19.24.25: Signal output terminal No. 1 Figure 12 No. 6 Bot J Punch 8 Gan Banquet Triangle 9 / 26 Branch body'$ 3 Figure 4 @; 7i Pun Child 5 Fenghai terminal 14 I7E, rat+rxm 194 Togo's tsuko'I$2 Figure 1 h rail j gon'su'11 child 2 times @h^ Ki disk 3 times M path 4 Den Suwa Hatoko 5 contact jf !!tI4I child 6 Iji No. ri t3f & child 8 scraps 1 tamashin de resistance 9 〃 26 Table 1 Imakyu No. 4 Figure 4 tOnabeko 5 year old concubine f #iyo 24 516jA1'An tatama f 25 3J Takako A2 Boka J Sensu No. 5 Meishi Kou J Mr. Nbu J1 Child Kaiki 9 ω 1 te) Sufu rotation axis electric fan Koko S Fuwa Sen 6 signal Muka Kiko 8 Kikafube Tamefuda 9 〃 26 Figure 6 Figure 7 Figure 1 10,000 starvation, konbu senshi 2 gourd ■ olfactory chengkei den matari 3 times eaves axis 6 gun name urony nyuzi

Claims (1)

【特許請求の範囲】 1、円板の面上に磁性体層を有し、その上に一定のピッ
チで着磁がされている回転磁気ディスクと、このディス
クに対向して配置され、感磁部が板状の支持体表面に金
属薄膜パターンもしくは導体の細線あるいはそれらの両
方を用いて形成されている磁気式の回転センサにおいて
、感磁部が回転中心から放射状にしかも全周にわたり一
定の間隔で配置されていることを特徴とする磁気式セン
サ。 2、特許請求の範囲第1項記載の磁気式の回転センサに
おいて、感磁部から信号出力端子までの検出回路を三端
子構成としたことを特徴とする磁気式センサ。 3、特許請求の範囲第1項記載の磁気式の回転センサに
おいて、感磁部から信号出力端子までの検出回路をブリ
ッジ型回路としたことを特徴とする磁気式センサ。
[Claims] 1. A rotating magnetic disk having a magnetic layer on the disk surface and magnetized at a constant pitch, and a magnetically sensitive disk placed opposite to this disk. In a magnetic rotation sensor in which the magnetic sensing part is formed on the surface of a plate-shaped support using a metal thin film pattern, a thin conductor wire, or both, the magnetic sensing part is radially spaced from the center of rotation and at constant intervals over the entire circumference. A magnetic sensor characterized by being arranged in. 2. A magnetic rotation sensor according to claim 1, characterized in that the detection circuit from the magnetic sensing part to the signal output terminal has a three-terminal configuration. 3. A magnetic rotation sensor according to claim 1, characterized in that the detection circuit from the magnetic sensing part to the signal output terminal is a bridge type circuit.
JP63172417A 1988-06-09 1988-07-11 Magnetic sensor Pending JPH0222510A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP63172417A JPH0222510A (en) 1988-07-11 1988-07-11 Magnetic sensor
US07/361,202 US5057678A (en) 1988-06-09 1989-06-05 Magnetic sensor and card reader containing it

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63172417A JPH0222510A (en) 1988-07-11 1988-07-11 Magnetic sensor

Publications (1)

Publication Number Publication Date
JPH0222510A true JPH0222510A (en) 1990-01-25

Family

ID=15941577

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63172417A Pending JPH0222510A (en) 1988-06-09 1988-07-11 Magnetic sensor

Country Status (1)

Country Link
JP (1) JPH0222510A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2016013347A1 (en) * 2014-07-25 2017-04-27 株式会社村田製作所 Magnetic sensor

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPWO2016013347A1 (en) * 2014-07-25 2017-04-27 株式会社村田製作所 Magnetic sensor

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