JPS6031014A - Position sensor wherein magnetoresistance body is used - Google Patents

Position sensor wherein magnetoresistance body is used

Info

Publication number
JPS6031014A
JPS6031014A JP13873283A JP13873283A JPS6031014A JP S6031014 A JPS6031014 A JP S6031014A JP 13873283 A JP13873283 A JP 13873283A JP 13873283 A JP13873283 A JP 13873283A JP S6031014 A JPS6031014 A JP S6031014A
Authority
JP
Japan
Prior art keywords
magnetic flux
magnetoresistive
magnetic
position sensor
slit
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
JP13873283A
Other languages
Japanese (ja)
Inventor
Yasuo Tanii
谷井 靖夫
Yoshiichi Kenmori
芳一 権守
Kenzaburo Miura
三浦 健三郎
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.)
Tokyo Sanyo Electric Co Ltd
Sanyo Electric Co Ltd
Kawaguchiko Seimitsu KK
Sanyo Denki Co Ltd
Original Assignee
Tokyo Sanyo Electric Co Ltd
Sanyo Electric Co Ltd
Kawaguchiko Seimitsu KK
Sanyo Denki 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 Tokyo Sanyo Electric Co Ltd, Sanyo Electric Co Ltd, Kawaguchiko Seimitsu KK, Sanyo Denki Co Ltd filed Critical Tokyo Sanyo Electric Co Ltd
Priority to JP13873283A priority Critical patent/JPS6031014A/en
Publication of JPS6031014A publication Critical patent/JPS6031014A/en
Pending legal-status Critical Current

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
    • G01D5/147—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 movement of a third element, the position of Hall device and the source of magnetic field being fixed in respect to each other

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)

Abstract

PURPOSE:To supply a correct signal voltage in a sine wave shape from an intermediate terminal, by forming an irregular period, during which moving magnetic flux is changed with respect to the end surface of each magnetoresistance body. CONSTITUTION:A permanent magnet 4 forms a parallel magnetic field H. Magnetoresistance bodies 1, 1', 10 and 10' comprising InSb are provided on a yoke and supporting body 3 comprising a ferromagnetic body. The thickness of the magnetoresistance body is about 5mum, the width is 0.3mm., and the height (h) is 1.5mm.. The magnetoresistance bodies 1, 1', 10 and 10' are connected in series by conductor paths 5 formed by a copper film. Terminals 11 and 12 and an intermediate terminal 13 are provided. The magnetoresistance bodies 1, 1', 10 and 10' and the conductor paths 5 are formed by combining a vacuum evaporation method and the like and a bonding method using a bonding material.

Description

【発明の詳細な説明】 (1)発明の技術分野 本発明は磁気抵抗体を使用してなす位置センサの改良に
関する。特に、2個の磁気抵抗体(または磁気抵抗体群
)をもって構成された直列回路を少なくとも1組有し、
その埴れぞれに交流電圧を印加しておき、上記夫々2個
の磁気抵抗体(または磁気抵抗体群)のそれぞれが文楽
する磁界強度を交互に変化させ、上記直列回路の中間端
子の電位の変化を測定してなす位置センサにおいて、上
記中間端子の電位の変化として得られる交流電圧を正し
い正弦波となるようにする改良に関する。
DETAILED DESCRIPTION OF THE INVENTION (1) Technical Field of the Invention The present invention relates to an improvement in a position sensor using a magnetoresistive element. In particular, it has at least one series circuit configured with two magnetoresistive elements (or a group of magnetoresistive elements),
An alternating current voltage is applied to each of the hani, and the strength of the magnetic field produced by each of the two magnetoresistive elements (or a group of magnetoresistive elements) is alternately changed, and the potential of the intermediate terminal of the series circuit is changed. The present invention relates to an improvement in a position sensor that measures changes in the voltage so that the alternating current voltage obtained as a change in the potential of the intermediate terminal becomes a correct sine wave.

(2)技術の背景 インジウムアンチモナイド(In5b) 、 インジウ
ムアーセナイド(rnAs)等、文楽する磁界強度に対
応して自身の抵抗を変化する材料があり、磁気抵抗性材
料と呼ばれる。かかる磁気抵抗性材料よりなる素子(以
下磁気抵抗体という。)を磁界中に配置しておき、かか
る磁気抵抗体と文楽する磁路のリラクタンスに規則的な
変化を与えるような幾何学的形状を有する物体を磁気抵
抗体にそって移動させると上記の磁気抵抗体の抵抗は上
記の規則的なりラフタンスの変化に対応して変化するか
ら上記物体の位置や移動速度等の移動状態を検出するこ
とができる。
(2) Background of the technology There are materials such as indium antimonide (In5b) and indium arsenide (rnAs) that change their resistance in response to the strength of the magnetic field, and are called magnetoresistive materials. An element made of such a magnetoresistive material (hereinafter referred to as a magnetoresistive element) is placed in a magnetic field, and a geometric shape is formed so as to give regular changes to the reluctance of the magnetic path between the magnetoresistive element and the Bunraku magnetic path. When an object is moved along a magnetoresistive element, the resistance of the magnetoresistive element changes in accordance with the regular changes in roughtance, so the moving state such as the position and speed of the object can be detected. I can do it.

(3)従来技術と問題点 かかる基本原理にもとづく、磁気抵抗体を使用してなす
位置センサは1個の磁気抵抗体を用いても実現しうるが
、第1図に示すように、2個の磁気抵抗体1.1’を直
列に接続してこの直列回路の二つの端子11.12間に
電圧を印加しておき、2個の磁気抵抗体1.1゛は共通
の磁界Hと叉交させておき、2個の磁気抵抗体1、lo
に対接させて規則的にスリット23.23°、23″、
・φ・を有し、磁性材料よりなる物体24を図において
Aの方向に移動させるなり、または、第2図に示すよう
に規則的に突起21.21’ 、 21” 、・・争と
凹部22.22’ 、 22” 、・Φ・とを有し磁性
材料よりなる物体2を図において矢印Aの方向に移動さ
せるなりして、上記の直列回路の中間端子13からスリ
ット23等または突起21凹部22等の交番的移動に対
応する周期と同一の周期の交流電圧を得ることが一般で
ある。
(3) Prior art and problems A position sensor using a magnetoresistive element based on the above basic principle can be realized using one magnetoresistive element, but as shown in Fig. Magnetoresistive elements 1.1' are connected in series and a voltage is applied between the two terminals 11.12 of this series circuit. The two magnetoresistive elements 1, lo
Slits 23.23°, 23″, 23.23°, 23″,
The object 24 having φ and made of a magnetic material is moved in the direction of A in the figure, or the protrusions 21, 21', 21'', . . . 22.22', 22", .Φ. The object 2 made of a magnetic material is moved in the direction of arrow A in the figure, and the slit 23 or the like or the protrusion 21 is removed from the intermediate terminal 13 of the series circuit. It is common to obtain an alternating current voltage with the same period as the period corresponding to the alternating movement of the recesses 22 and the like.

更に、第3図、第4図に示すように上記の位置センサ2
組を互いに90°電気角を異にする位置に配設し、互い
に800位相を異にする二つの交流電圧を得ることにす
れば、位置の検出精度も向上し、回転の方向も容易に識
別しうることは下式よ゛ り明らかである。
Furthermore, as shown in FIGS. 3 and 4, the above-mentioned position sensor 2
By arranging the sets at positions with electrical angles different from each other by 90° and obtaining two AC voltages with a phase difference of 800° from each other, position detection accuracy will be improved and the direction of rotation can be easily identified. What is possible is clear from the equation below.

A cos θ sin ω t +As1n θ C
OS ω t=Bsin(ωを十〇) 但し、θは被検出電気角位置であり、 ωは直列回路の端子11.12に印加 される交流電圧の電気角速度であ る。
A cos θ sin ω t +As1n θ C
OS ω t=Bsin (ω is 10) where θ is the electrical angular position to be detected, and ω is the electrical angular velocity of the AC voltage applied to the terminals 11 and 12 of the series circuit.

第3図においては、磁気抵抗体1.1’の組はスリット
23とスリットを有しない磁性材部24とに対接し、一
方、磁気抵抗体1O110°の組は磁性材部24とスリ
ット23′ との境界とスリット23° と磁性材部2
4との境界とに対接しており互いに80°電気角位置が
ずれている。一方、第4図においては、磁気抵抗体1.
1’の組は突起21と凹部22とに対接し、一方、磁気
抵抗体1O110°の組は凹部22と突起21’ との
境界と突起21’ と凹部22″の境界と対接しており
、互いに80°電気角位置がずれている。
In FIG. 3, the set of magnetoresistive elements 1.1' is in contact with the slit 23 and the magnetic material part 24 without a slit, while the set of magnetoresistive elements 1O110 is in contact with the magnetic material part 24 and the slit 23'. The boundary between the slit 23° and the magnetic material part 2
4, and their electrical angle positions are shifted by 80° from each other. On the other hand, in FIG. 4, the magnetic resistor 1.
The set 1' is in contact with the protrusion 21 and the recess 22, while the set of magnetoresistive element 1O110 is in contact with the boundary between the recess 22 and the protrusion 21' and the boundary between the protrusion 21' and the recess 22''. The electrical angle positions are shifted by 80° from each other.

上式にもとづく機能が正しく実現されるためには、それ
ぞれの磁気抵抗体の組の中間端子から得られる交流出力
が正しい正弦波または余弦波である必要がある。
In order to correctly realize the function based on the above equation, the AC output obtained from the intermediate terminal of each magnetoresistive pair needs to be a correct sine wave or cosine wave.

磁気抵抗体1.1’の組(直列回路)の中間端子13か
ら得られる交流電圧を正弦波に近づけるためには、第5
図、第6図に示すように、2個の磁気抵抗体1.1′の
中心間距離りとスリット23または突起21の幅P1と
スリットを有しない磁性部材24または凹部22の輻P
2とを同一にすることが有効ではあるが、このように配
置することは幾何学的に困難であるとともに、磁気抵抗
体1、loの幅見が大きくなるため、磁気抵抗体1、l
oの抵抗が極端に小さくなり実用に供しえないという欠
点があり、第5図、第6図のような構造は現実的に採用
困難である。
The fifth
As shown in FIG. 6, the distance between the centers of the two magnetic resistors 1.1', the width P1 of the slit 23 or protrusion 21, and the radius P of the magnetic member 24 or recess 22 without a slit.
Although it is effective to make the magnetoresistive elements 1 and 2 the same, it is geometrically difficult to arrange them in this way, and the width of the magnetoresistive elements 1 and lo becomes large.
There is a drawback that the resistance of o becomes extremely small, making it impractical for practical use, and it is difficult to practically adopt the structures shown in FIGS. 5 and 6.

そのため、従来技術においては、第7図、第8図に示す
ように、磁気抵抗体l、1′の幅立を小さくし、かつ、
スリット23または突起21の幅P1を小さくし、スリ
ットを有しない磁性材部24または凹部22の幅P2を
大きくすることが一般であった。
Therefore, in the prior art, as shown in FIGS. 7 and 8, the width of the magnetoresistive elements l and 1' is made small, and
Generally, the width P1 of the slit 23 or the protrusion 21 is made small, and the width P2 of the magnetic material part 24 or the recessed part 22 which does not have a slit is made large.

その結果、従来技術において、磁気抵抗体の直列回路の
中間端子13から得られる電圧波形は第9図にEをもっ
て示すように、位相が反転している第3高周波を含む傾
向が避は難いという欠点があった。
As a result, in the prior art, the voltage waveform obtained from the intermediate terminal 13 of the series circuit of magnetoresistive elements inevitably tends to include a third high frequency wave whose phase is reversed, as shown by E in FIG. There were drawbacks.

(4)発明の目的 本発明の目的はこの欠点を解消することにあり、2個の
磁気抵抗体(または磁気抵抗体群)をもって構成された
直列回路を少なくとも1組有し、そのそれぞれに交流電
圧を印加しておき、上記それぞれ2個の磁気抵抗体(ま
たは磁気抵抗体群)のそれぞれが叉交する磁界強度を交
互に変化させ、上記夫々の直列回路の中間端子の電位の
変化を測定してなす位置センサにおいて、上記夫々2個
の磁気抵抗体(または磁気抵抗体群)の直列回路の中間
端子から正しい正弦波状の信号電圧を供給しうる、磁気
抵抗体を使用してなす位置センサを提供することにある
。
(4) Purpose of the Invention The purpose of the present invention is to eliminate this drawback. Apply a voltage, alternately change the strength of the magnetic field crossed by each of the two magnetoresistive elements (or group of magnetoresistive elements), and measure the change in potential at the intermediate terminal of each of the series circuits. A position sensor formed by using a magnetoresistive element, which can supply a correct sinusoidal signal voltage from an intermediate terminal of a series circuit of two magnetoresistive elements (or a group of magnetoresistive elements). Our goal is to provide the following.

(5)発明の構成 本発明の構成は、特定の方向に移動しその磁界強度を周
期的に変化する磁束と叉交する領域に該磁束の移動方向
とおおむね平行するように配設され該磁束の移動方向と
交わる端面は該磁束の移動方向とおおむね直交する直方
体の板状部材よりなる2個の磁気抵抗体(または磁気抵
抗体群)よりなり中間端子の設けられた直列回路を少な
くとも1組配設し、夫々の回路に交流電圧を印加してお
き、夫々2個の磁気抵抗体(または磁気抵抗体群)と文
楽する磁界強度に対応して変化する前記2個の磁気抵抗
体(または磁気抵抗体群)の抵抗値の変化に対応して発
生する前記夫々の中間端子の電位を測定して前記移動す
る磁束の移動状態を検出してなす、磁気抵抗体を使用し
てなす位置センサにおいて、前記移動する磁束が変化す
る時期は前記磁気抵抗体の端面に対して不整となるよう
になされていることを特徴とする磁気抵抗体を使用して
なす位置センサにある。
(5) Configuration of the Invention The configuration of the present invention is such that the magnetic flux is disposed in a region that intersects with a magnetic flux that moves in a specific direction and whose magnetic field intensity changes periodically, so as to be approximately parallel to the moving direction of the magnetic flux. At least one set of series circuits each consisting of two magnetoresistive elements (or a group of magnetoresistive elements) each made of a rectangular parallelepiped plate-like member whose end face intersects with the direction of movement of the magnetic flux and is provided with an intermediate terminal is provided. The two magnetoresistive elements (or a group of magnetoresistive elements), which change in accordance with the magnetic field strength, perform bunraku with two magnetoresistive elements (or a group of magnetic resistance elements) by applying an alternating voltage to each circuit. A position sensor using a magnetoresistive element, which detects the moving state of the moving magnetic flux by measuring the potential of each of the intermediate terminals that occurs in response to a change in the resistance value of a group of magnetoresistive elements. In the position sensor using a magnetoresistive member, the timing at which the moving magnetic flux changes is made to be irregular with respect to the end face of the magnetoresistive member.

本発明の依拠する技術思想は、第10図、第11図に示
すように、垂直方向に配設された直方体状の磁気抵抗体
1、loの端面と、リラクタンスの変化を起因するスリ
ット23等または突起21等の端面各部が対接を開始す
る時期に時間差を発生させるこ1 ととし、全体として高調波の発生を防止することとした
ものである。
As shown in FIGS. 10 and 11, the technical idea on which the present invention is based is that the rectangular parallelepiped magnetoresistance body 1 arranged in the vertical direction, the end face of lo, the slit 23 etc. that cause a change in reluctance, etc. Alternatively, a time difference is generated in the timing at which each part of the end face of the protrusion 21 etc. starts to come into contact with each other, thereby preventing the generation of harmonics as a whole.

要すれば、移動する磁束が交番する時期が磁気抵抗体の
端面の各部に対して不整となるようにし、全体として、
高調波の発生を防止し、上記の移動する磁界の波形が正
弦波状になるようにしたものである。
If necessary, the timing at which the moving magnetic flux alternates is made irregular with respect to each part of the end face of the magnetoresistive element, and as a whole,
This prevents the generation of harmonics and makes the waveform of the moving magnetic field sinusoidal.

この技術思想を実現するには、上記せるとおり磁気抵抗
体1等の端面とスリット23等または突起21等の端面
とを一致させず、これらのスリット23等または突起2
1等の端面を磁束の移動方向に対して不整形にすればよ
い。
In order to realize this technical idea, as mentioned above, the end face of the magnetoresistive element 1 etc. and the end face of the slit 23 etc. or the protrusion 21 etc. should not be made to match, and these slits 23 etc. or the protrusion 2
The end face of the first class may be made irregularly shaped with respect to the moving direction of the magnetic flux.

几体的には、スリット23等または突起21等を有する
物体24または2(リラクタンスを変化させる物体)が
線状部材すなわち棒状部材であるときは、第10図、第
11図に示すように、スリット23等または突起21等
の端面を磁気抵抗体1.1’の端面と傾斜させておくな
り、第12図、第13図に示すように、スリット23等
または突起21等の端面を磁気抵抗体1.1’の端面に
対して蛇行させておくな2 す、第14図、第15図に示すように、スリット23等
または突起21等の端面の中央部を磁気抵抗体1゜lo
の端面に対して大きくしておくなり、第18図、第17
図に示すように、スリット23等または突起21等の端
面を磁気抵抗体l、1゛の端面に対して階段状にしてお
くなりすればよい。
In terms of structure, when the object 24 or 2 (object that changes reluctance) having the slit 23 or the like or the protrusion 21 is a linear member, that is, a rod-like member, as shown in FIGS. 10 and 11, The end faces of the slits 23, etc. or the protrusions 21, etc. are inclined with respect to the end faces of the magnetoresistive element 1.1', and as shown in FIGS. 12 and 13, the end faces of the slits 23, etc. or the protrusions 21, etc. As shown in FIGS. 14 and 15, the center part of the end surface of the slit 23 or the protrusion 21 should not be made to meander with respect to the end surface of the magnetic resistor 1.1'.
18 and 17.
As shown in the figure, the end surfaces of the slits 23, etc. or the protrusions 21, etc. may be made step-like with respect to the end surfaces of the magnetic resistance elements 1 and 1''.

又、スリット23等または突起21等を有する物体(リ
ラクタンスを変化させる物体)は円筒状部材でもよく、
その場合は、円筒状部材の周面がそれぞれ、上記第10
717図のように磁束の移動方向に対して不整にされて
いればよい。
Further, the object having the slit 23 or the like or the protrusion 21 (the object that changes the reluctance) may be a cylindrical member,
In that case, the circumferential surface of the cylindrical member is
It suffices if it is made irregular with respect to the moving direction of the magnetic flux as shown in FIG. 717.

(6)発明の実施例 本発明の構成は比較的明瞭であるから、以下、図面を参
照しつつ、本発明の代表的実施例に係る磁気抵抗体を使
用してなす位置センサについて更に説明する。
(6) Embodiments of the Invention Since the structure of the present invention is relatively clear, a position sensor using a magnetic resistor according to a typical embodiment of the present invention will be further explained below with reference to the drawings. .

第18図、19図参照 図はそれぞれ特許請求の範囲第2項と第4項記載の磁気
抵抗体を使用してなす位置センサ2例(第18図は前者
すなわちスリットまたは突起を有する物体が線状部材す
なわち棒状部材である場合であり、第19図は後者すな
わちスリットまたは突起を有する物体が円筒状部材であ
る場合である)の平面図である。なお、直列回路の数は
2組とする。
18 and 19 are two examples of position sensors made using the magnetic resistance bodies according to claims 2 and 4, respectively (FIG. 18 shows the former, that is, an object having a slit or a protrusion is FIG. 19 is a plan view of the latter case, that is, the case where the object having a slit or projection is a cylindrical member. Note that the number of series circuits is two.

図において、4は永久磁石であり、約1キロガウス程度
の平行磁界Hを形成する。3はフェライト等強磁性体よ
りなるヨーク兼支持体であり、本例においては高さが数
m層幅が数層■で厚さが0.5鵬腫程度である。
In the figure, 4 is a permanent magnet, which forms a parallel magnetic field H of about 1 kilogauss. Reference numeral 3 denotes a yoke/support body made of a ferromagnetic material such as ferrite, and in this example, the height is several meters, the width is several layers, and the thickness is about 0.5 mm.

1.1’、10.10°はインジウムアンチモナイド(
Ir+Sb)よりなる磁気抵抗体であり、厚さは約51
Lmである。その幅見は0.3msであり、その高さh
は1.F+++m程度である。磁気抵抗体lと1′及び
10.10°とは銅膜をもって形成された導電路5をも
って直列に接続されており双方の端子11.12と中間
端子13とが設けられている。磁気抵抗体l、1°、1
0、lOo と導電路5とはフォトリソグラフィー法と
イオンブレーティング法、スパッタリング法、真空蒸着
法等と接着材を使用してなる接着法との組み合わせでも
って容易に形成しうる。なお、かかる構造の磁気抵抗体
の組が2対第4図に示すように配設されていることは云
うまでもない。24はスリットを有する板状部材であり
、241はスリット231を有する円筒状部材であり、
軸6を中心として回転し、磁気抵抗体1.1’、1O1
10′とは0゜3ms程度の距離を隔てて配設される。
1.1', 10.10° are indium antimonide (
It is a magnetoresistive material made of Ir+Sb) and has a thickness of approximately 51 mm.
It is Lm. Its width is 0.3ms, and its height h
is 1. It is about F+++m. The magnetoresistive elements 1, 1' and 10.10° are connected in series through a conductive path 5 formed of a copper film, and terminals 11, 12 and an intermediate terminal 13 are provided on both sides. Magnetoresistive element l, 1°, 1
0, lOo and the conductive path 5 can be easily formed by a combination of a photolithography method, an ion blating method, a sputtering method, a vacuum evaporation method, etc., and an adhesion method using an adhesive. It goes without saying that two sets of magnetoresistive elements having such a structure are arranged as shown in FIG. 24 is a plate-like member having a slit, 241 is a cylindrical member having a slit 231,
It rotates around the axis 6, and the magnetoresistive elements 1.1', 1O1
10' is arranged at a distance of about 0.3 ms.

第10図再参照 いづれの場合もスリット23.231等の端面は第11
図に示すように、直方体状の磁気抵抗体l、1゛、10
.10’ の端面とは傾斜している。
Refer to Figure 10 again. In both cases, the end faces of the slits 23, 231, etc. are the 11th
As shown in the figure, rectangular parallelepiped magnetoresistive elements l, 1゛, 10
.. It is inclined with respect to the end face of 10'.

上記のような構造の磁気抵抗体を使用してなす位置セン
サの端子11.12間に5ビ程度の電圧を印加すると中
間端子13の電位はスリット23.231等が磁気抵抗
体1.1°と対接する周期と同一の周期をもって±0.
2vの極めて正弦波に近い波形をもって交番する。
When a voltage of about 5 Bi is applied between the terminals 11 and 12 of a position sensor made using a magnetoresistive member having the above structure, the potential of the intermediate terminal 13 becomes such that the slits 23, 231, etc. are 1.1° ±0. with the same period as the period opposite to.
It alternates with a waveform extremely close to a 2V sine wave.

本発明の構成は比較的明瞭であるから特許請求の範囲の
すべてに対して記述する繁を避ける。
Since the structure of the present invention is relatively clear, it will not be necessary to describe the entire scope of the claims.

(7)発明の効果 5 以上説明せるとおり、本発明によれば、2個の磁気抵抗
体(または磁気抵抗体群)をもって構成された直列回路
を少なくとも1組有し、そのそれぞれに交流電圧を印加
しておき、上記それぞれ2個の磁気抵抗体(または磁気
抵抗体群)のそれぞれが文楽する磁界強度を交互に変化
させ、上記夫々の直列回路の中間端子の電位の変化を測
定してなす位置センサにおいて、上記夫々2個の磁気抵
抗体(または磁気抵抗体群)の直列回路の中間端子から
正しい正弦波状の信号電圧を供給しうる、磁気抵抗体を
使用してなす位置センサを提供することができる。
(7) Effect of the invention 5 As explained above, according to the present invention, there is at least one series circuit configured with two magnetoresistive elements (or a group of magnetoresistive elements), and an alternating current voltage is applied to each of the series circuits. This is done by alternately changing the strength of the magnetic field produced by each of the two magnetoresistive elements (or a group of magnetoresistive elements) and measuring the change in potential at the intermediate terminal of each of the series circuits. To provide a position sensor using a magnetoresistive member, which can supply a correct sinusoidal signal voltage from an intermediate terminal of a series circuit of the two magnetoresistive members (or a group of magnetoresistive members). be able to.

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

第1図、第2図は従来技術における磁気抵抗体を使用し
てなす位置センサの一例の斜視図である。第3図、第4
図は磁気抵抗体の直列回路を2組有する従来技術におけ
る磁気抵抗体を使用してなす位置センサの一例の平面図
である。第5図、第6図、第7図、第8図は、平面図を
第3図、第4図に示す従来技術における磁気抵抗体を使
用し6 てなす位置センサの一例の欠点すなわち本発明の詳細な
説明するために書いた従来技術における磁気抵抗体を使
用してなす位置センサの一例の平面図である。第9図は
第7図、第8図に示す従来技術における磁気抵抗体を使
用してなす位置センサの一例の中間端子から得られる出
力電圧を示す図である。第1O図、第11図は、それぞ
れ、特許請求の範囲第6項によって限定された特許請求
の範囲第2項及び第3項にかかる磁気抵抗体を使用して
゛なす位置センサの動作原理を説明するための斜視図で
ある。第12図、第13図、第14図、第15図、第1
8図、第17図は本発明の実施例に係る磁気抵抗体を使
用してなす位置センサの磁気抵抗体と移動物体との正面
図である。第18図、第19図は本発明の実施例に係る
磁気抵抗体を使用してなす位置センサの平面図である。 l、1°、10.10°、・・・磁気抵抗体、 11.
12・φ・磁気抵抗体の端子、 !3・φ・磁気抵抗体
の中間端子、2.24・・ψ移動物体、 241−・−
回転体、 21.2ビ、 21” 、 121 、12
1’・φ・突起、 22.22’ 、 22”、 12
2 、122′、ψ・・凹部、 23.23°、23”
、231.231、・・・スリット、 H・・φ磁界方
向、 A−・・物体の移動方向、 立・・e磁気抵抗体
の幅、 L・・・組をなす磁気抵抗体の中心間距離、 
Pl・・・突起の幅、P ・・・四部の幅、 E@・・
従来技術における磁気抵抗体を使用してなす位置センサ
の中間端子から得られる電圧波形、 3・・・ヨーク兼
支持部材、4・・・永久磁石、5・・・導電路、6・拳
・回転体の軸。 代理人 弁理氏 寒 川 誠 −
FIGS. 1 and 2 are perspective views of an example of a position sensor using a magnetoresistive element in the prior art. Figures 3 and 4
The figure is a plan view of an example of a position sensor using a conventional magnetic resistor having two series circuits of magnetic resistors. 5, 6, 7, and 8 show the disadvantages of an example of a position sensor using a magnetoresistive body in the prior art shown in FIGS. 3 and 4, namely, the present invention. FIG. 2 is a plan view of an example of a position sensor made using a magnetoresistive body in the prior art, written for detailed explanation of the present invention. FIG. 9 is a diagram showing an output voltage obtained from an intermediate terminal of an example of a position sensor using a magnetic resistor according to the prior art shown in FIGS. 7 and 8. FIG. FIGS. 1O and 11 illustrate the operating principle of a position sensor made using the magnetoresistive elements according to claims 2 and 3, which are limited by claim 6, respectively. FIG. Figure 12, Figure 13, Figure 14, Figure 15, Figure 1
8 and 17 are front views of a moving object and a magnetic resistor of a position sensor using a magnetic resistor according to an embodiment of the present invention. FIGS. 18 and 19 are plan views of a position sensor using a magnetoresistive element according to an embodiment of the present invention. l, 1°, 10.10°, ... magnetoresistive element, 11.
12・φ・Magnetic resistance terminal, ! 3・φ・Intermediate terminal of magnetic resistor, 2.24・・φ Moving object, 241−・−
Rotating body, 21.2 bi, 21”, 121, 12
1'・φ・Protrusion, 22.22', 22", 12
2, 122', ψ... recess, 23.23°, 23"
, 231.231,...slit, H...φ magnetic field direction, A-...direction of movement of object, vertical...width of e magnetic resistor, L...distance between centers of magnetic resistors forming a pair. ,
Pl...width of protrusion, P...width of four parts, E@...
Voltage waveform obtained from the intermediate terminal of a position sensor made using a magnetoresistive element in the prior art, 3...Yoke and support member, 4...Permanent magnet, 5...Conducting path, 6.Fist/rotation body axis. Agent Patent Attorney Makoto Samukawa −

Claims (9)

【特許請求の範囲】[Claims] (1)特定の方向に移動しその磁界強度を周期的に変化
する磁束と文楽する領域に該磁束の移動方向とおおむね
平行するように配設され該磁束の移動方向と交わる端面
は該磁束の移動方向とおおむね直交する直方体の板状部
材よりなる2個の磁気抵抗体(または磁気抵抗体群)よ
りなり中間端子の設けられた直列回路を少なくとも1組
配設し、夫々の回路に交流電圧を印加しておき、夫々2
個体(または磁気抵抗体群)の抵抗値の変化に対応して
発生する前記夫々の中間端子の電位を測定して前記移動
する磁束の移動状態を検出してなす、磁気抵抗体を使用
してなす位置センサにおいて、前記移動する磁束が変化
する時期は前記磁気抵抗体の端面に対して不整となるよ
うになされていることを特徴とする磁気抵抗体を使用し
てなす位置センサ。
(1) An end face that is arranged to be roughly parallel to the moving direction of the magnetic flux in a region that plays Bunraku with a magnetic flux that moves in a specific direction and whose magnetic field strength changes periodically, and that intersects with the moving direction of the magnetic flux is At least one set of series circuits each consisting of two magnetoresistive elements (or a group of magnetoresistive elements) each made of a rectangular parallelepiped plate member orthogonal to the direction of movement and provided with an intermediate terminal is arranged, and each circuit is connected to an alternating current voltage. are applied, and 2
The state of movement of the moving magnetic flux is detected by measuring the potential of each of the intermediate terminals that occurs in response to a change in the resistance value of an individual (or a group of magnetoresistive elements), using a magnetoresistive element. 1. A position sensor using a magnetic resistor, characterized in that the timing at which the moving magnetic flux changes is irregular with respect to an end surface of the magnetic resistor.
(2)前記特定の方向に移動しその磁界強度を周期的に
変化する磁束は、前記少なくとも1組の磁気抵抗体回路
の一方の面に対向して配設された磁束発生手段と、前記
2個の磁気抵抗体(または磁気抵抗体群)と対向して移
動し規則的に形成されたスリットを有する棒状部材の前
記特定方向への移動に起因するりラフタンスの変化とに
よって実現される、特許請求の範囲第1項記載の磁気抵
抗体を使用してなす位置センサ。
(2) The magnetic flux that moves in the specific direction and periodically changes its magnetic field strength is generated by the magnetic flux generating means disposed opposite to one surface of the at least one set of magnetoresistive circuits; A patent that is realized by a change in roughtance caused by movement of a rod-shaped member having regularly formed slits and moving in opposition to a magnetoresistive element (or a group of magnetoresistive elements) in the specific direction. A position sensor made using the magnetic resistor according to claim 1.
(3)前記特定の方向に移動しその磁界強度を周期的に
変化する磁束は、前記少なくとも1組の磁気抵抗体回路
の一方の面に対向して配設された磁束発生手段と、前記
2個の磁気抵抗体(または磁気抵抗体群)と対向して移
動し規則的に形成されたラック状凹凸を有する棒状部材
の前記特定方向への移動に起因するりラフタンスの変化
とによって実現される、特許請求の範囲第1項記載の磁
気抵抗体を使用してなす位置センサ。
(3) The magnetic flux that moves in the specific direction and periodically changes its magnetic field strength is generated by the magnetic flux generating means disposed opposite to one surface of the at least one set of magnetoresistive circuits; This is realized by the change in roughness caused by the movement in the specific direction of a rod-shaped member having regularly formed rack-like unevenness that moves opposite to a magnetoresistive element (or a group of magnetoresistive elements). , a position sensor using the magnetic resistance body according to claim 1.
(4)前記特定の方向に移動しその磁界強度を周期的に
変化する磁束は、前記少なくとも1組の磁気抵抗体回路
の一方の面に対向して配設された磁束発生手段と、前記
2個の磁気抵抗体(または磁気抵抗体群)と対向して移
動し規則的に形成されたスリットを有する円筒状部材の
回転に起因するりラフタンスの変化とによって実現され
る、特許請求の範囲第1項記載の磁気抵抗体を使用して
なす位置センサ。
(4) The magnetic flux that moves in the specific direction and periodically changes its magnetic field strength is generated by the magnetic flux generating means disposed opposite to one surface of the at least one set of magnetoresistive circuits; A change in rufftance caused by rotation of a cylindrical member that moves oppositely to a magnetoresistive element (or a group of magnetoresistive elements) and that has regularly formed slits. A position sensor made using the magnetic resistor described in item 1.
(5)前記特定の方向に移動しその磁界強度を周期的に
変化する磁束は、前記少なくとも1組の磁気抵抗体回路
の一方の面に対向して配設された磁束発生手段と、前記
2個の磁気抵抗体(または磁気抵抗体群)と対向して移
動し規則的に形成された歯車状凹凸を有する円筒状部材
の回転に起因するりラフタンスの変化とによって実現さ
れる、特許請求の範囲第1項記載の磁気抵抗体を使用し
てなす位置センサ。
(5) The magnetic flux that moves in the specific direction and periodically changes its magnetic field strength is generated by the magnetic flux generating means disposed opposite to one surface of the at least one set of magnetoresistive circuits; A change in roughness caused by rotation of a cylindrical member that moves oppositely to a magnetoresistive element (or a group of magnetoresistive elements) and has regularly formed gear-like unevenness. A position sensor made using the magnetoresistive material described in scope 1.
(6)前記移動する磁束が前記磁気抵抗体の端面に対し
て変化する時期は、前記棒状部材のスリットもしくはラ
ック状凹凸または前記円筒状部材のスリットもしくは歯
車状凹凸の端面が前記移動する磁束の移動方向に対して
傾斜していることにより不整とされる、特許請求の範囲
第2項、第3項、第4項または第5項記載の磁気抵抗体
を使用してなす位置センサ。
(6) The time when the moving magnetic flux changes with respect to the end face of the magnetic resistance body is determined when the moving magnetic flux changes with respect to the end face of the slit or rack-like unevenness of the rod-shaped member or the slit or gear-like unevenness of the cylindrical member. A position sensor made using the magnetic resistance body according to claim 2, 3, 4, or 5, which is irregular due to being inclined with respect to the direction of movement.
(7)前記移動する磁束が前記磁気抵抗体の端面に対し
て変化する時期は、前記棒状部材のスリットもしくはラ
ック状凹凸または前記円筒状部材のスリットもしくは歯
車状凹凸の端面が前記移動する磁束の移動方向に対して
蛇行していることにより不整とされる、特許請求の範囲
第2項、第3項、第4項または第5項記載の磁気抵抗体
を使用してなす位置センサ。
(7) The timing at which the moving magnetic flux changes with respect to the end face of the magnetic resistance body is determined when the slit or rack-like unevenness of the rod-shaped member or the end face of the slit or gear-like unevenness of the cylindrical member A position sensor made using the magnetic resistance body according to claim 2, 3, 4, or 5, which is irregular due to meandering with respect to the moving direction.
(8)前記移動する磁束が前記磁気抵抗体の端面に対し
て変化する時期は、前記棒状部材のスリットもしくはラ
ック状凹凸または前記円筒状部材のスリットもしくは歯
車状凹凸の中央部が膨大していることにより不整とされ
る、特許請求の範囲第2項、第3項、第4項または第5
項記載の磁気抵抗体を使用してなす位置センサ。
(8) When the moving magnetic flux changes with respect to the end face of the magnetic resistance body, the central portion of the slit or rack-like unevenness of the rod-shaped member or the slit or gear-like unevenness of the cylindrical member becomes enormous. Claims 2, 3, 4, or 5 that are irregular due to
A position sensor made using the magnetoresistive material described in 2.
(9)前記移動する磁束が前記磁気抵抗体の端面に対し
て変化する時期は、前記棒状部材のスリ・ントもしくは
ラック状凹凸または前記円筒状部材のスリットもしくは
歯車状凹凸の端面が階段状をなすことにより不整とされ
る、特許請求の範囲第2項、第3項、第4項または第5
項記載の磁気抵抗体を使用してなす位置センサ。
(9) When the moving magnetic flux changes with respect to the end surface of the magnetic resistance body, the end surface of the slit or rack-like unevenness of the rod-shaped member or the slit or gear-like unevenness of the cylindrical member has a step-like shape. Claims 2, 3, 4, or 5 that are considered irregular by
A position sensor made using the magnetoresistive material described in 2.
JP13873283A 1983-07-30 1983-07-30 Position sensor wherein magnetoresistance body is used Pending JPS6031014A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13873283A JPS6031014A (en) 1983-07-30 1983-07-30 Position sensor wherein magnetoresistance body is used

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13873283A JPS6031014A (en) 1983-07-30 1983-07-30 Position sensor wherein magnetoresistance body is used

Publications (1)

Publication Number Publication Date
JPS6031014A true JPS6031014A (en) 1985-02-16

Family

ID=15228867

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13873283A Pending JPS6031014A (en) 1983-07-30 1983-07-30 Position sensor wherein magnetoresistance body is used

Country Status (1)

Country Link
JP (1) JPS6031014A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63205514A (en) * 1987-02-23 1988-08-25 Hitachi Ltd Device that magnetically detects position and speed
JPS63286710A (en) * 1987-05-19 1988-11-24 Ono Sokki Co Ltd Moving extent detector
WO1995009447A1 (en) * 1993-09-27 1995-04-06 Commissariat A L'energie Atomique Current sensor comprising a magnetoresistive strip and method of production

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS559186A (en) * 1978-07-07 1980-01-23 Sanyo Electric Co Ltd Magnetic detector

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS559186A (en) * 1978-07-07 1980-01-23 Sanyo Electric Co Ltd Magnetic detector

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63205514A (en) * 1987-02-23 1988-08-25 Hitachi Ltd Device that magnetically detects position and speed
JPS63286710A (en) * 1987-05-19 1988-11-24 Ono Sokki Co Ltd Moving extent detector
WO1995009447A1 (en) * 1993-09-27 1995-04-06 Commissariat A L'energie Atomique Current sensor comprising a magnetoresistive strip and method of production
FR2710753A1 (en) * 1993-09-27 1995-04-07 Commissariat Energie Atomique Current sensor comprising a magnetoresistive tape and its production method.
US5708407A (en) * 1993-09-27 1998-01-13 Commissariat A L'energie Atomique Current sensor comprising a magnetoresistive tape and its production process

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