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JPH0410570B2 - - Google Patents
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JPH0410570B2 - - Google Patents

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Publication number
JPH0410570B2
JPH0410570B2 JP13873383A JP13873383A JPH0410570B2 JP H0410570 B2 JPH0410570 B2 JP H0410570B2 JP 13873383 A JP13873383 A JP 13873383A JP 13873383 A JP13873383 A JP 13873383A JP H0410570 B2 JPH0410570 B2 JP H0410570B2
Authority
JP
Japan
Prior art keywords
magnetoresistive
circuit
circuits
magnetic flux
position sensor
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.)
Expired
Application number
JP13873383A
Other languages
Japanese (ja)
Other versions
JPS6031015A (en
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 filed Critical
Priority to JP13873383A priority Critical patent/JPS6031015A/en
Publication of JPS6031015A publication Critical patent/JPS6031015A/en
Publication of JPH0410570B2 publication Critical patent/JPH0410570B2/ja
Granted legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING 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
    • G01D5/00Mechanical 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
    • G01D5/12Mechanical 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
    • G01D5/14Mechanical 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
    • G01D5/142Mechanical 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
    • G01D5/147Mechanical 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)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)

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、特定の方向に移動する磁
界と叉交する領域に特定の距離を隔てて配設され
相互に直列に接続された磁気抵抗体(または数個
の磁気抵抗体が直列に接続された群)の組が一対
以上直列に接続されて直列回路をなし、この直列
回路は中間端子を有する構造を有する第1の磁気
抵抗体回路と、これと同一の構造ではあるがそれ
ぞれ対応する磁気抵抗体(または数個の磁気抵抗
体が直列に接続された群)は上記の移動する交番
磁界の移動方向に、上記の特定の距離の1/2ずれ
て配設されている第2の磁気抵抗体回路とよりな
り、これら二つの磁気抵抗体回路のそれぞれには
90゜位相を異にする正弦波が印加され、これらの
二つの正弦波が上記の直列に接続された磁気抵抗
体回路によつて分圧されて中間端子から得られる
二つの交流電圧を利用して、上記の移動する交番
磁界の周波数を測定し、この移動する交番磁界を
発生する移動体の位置や移動状態等を検出するこ
とを基本原理とする磁気抵抗体を使用してなす位
置センサの改良に関する。
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, magnetoresistive elements (or a group of several magnetoresistive elements connected in series) arranged in series at a certain distance in a region that intersects a magnetic field moving in a particular direction. are connected in series to form a series circuit, and this series circuit includes a first magnetoresistive circuit having a structure having an intermediate terminal, and a corresponding magnetoresistive circuit having the same structure as the first magnetoresistive circuit ( or a group of several magnetoresistive elements connected in series) is a second magnetoresistive circuit that is arranged shifted by 1/2 of the above-mentioned specific distance in the moving direction of the above-mentioned moving alternating magnetic field. Therefore, each of these two magnetoresistive circuits has
Sine waves with a phase difference of 90° are applied, and these two sine waves are divided by the above-mentioned series-connected magnetoresistive circuit, and the two AC voltages obtained from the intermediate terminal are used. The basic principle of the position sensor is to measure the frequency of the above-mentioned moving alternating magnetic field and detect the position and movement status of the moving object that generates the moving alternating magnetic field. Regarding improvements.

(2) 技術の背景 インジウムアンチモナイド(InSb)、インジウ
ムアーセナイド(InAs)等、叉交する磁界強度
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叉交する
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つ
て移動させると上記の磁気抵抗体の抵抗は上記の
規則的なリラク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 (InSb) and indium arsenide (InAs) that change their resistance in response to the strength of intersecting magnetic fields, 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 that gives a regular change to the reluctance of a magnetic path that intersects the magnetoresistive element. When an object having . be able to.

(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、第2図に示すように、
2個の磁気抵抗体1a,1b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1a,1bは共通
の磁界Hと叉交させておき、2個の磁気抵抗体1
a,1bに対接させて規則的にリラクタンスを変
化させるような移動体(スリツト23,23′等
を有する磁性体24等または凹凸を有する磁性体
2等)を図において矢印Aの方向に移動させる
と、矢印Aの方向に移動する交番磁界が発生する
ことになり、上記の端子11,12間に印加され
た電圧は、上記の移動する交番磁界の周期と同一
の周期をもつて磁気抵抗体1a,1bによつて分
圧されて中間端子13から出力される。そこで、
この中間端子13から得られる電圧の周波数を測
定すれば、磁気抵抗体1a,1bの抵抗を変化さ
せたリラクタンスの変化の原因である上記の移動
体(24等または2等)の移動状態を検出しうる
ことになる。
(3) Prior art and problems A position sensor using a magnetoresistive element based on this basic principle can be realized using a single magnetoresistive element, but as shown in Figs. To,
Two magnetoresistive elements 1a and 1b are connected in series and a voltage is applied between the two terminals 11 and 12 of this series circuit. The two magnetic resistors 1
A moving body (magnetic body 24, etc. having slits 23, 23', etc. or magnetic body 2, etc. having unevenness) that regularly changes reluctance in contact with a and 1b is moved in the direction of arrow A in the figure. As a result, an alternating magnetic field moving in the direction of arrow A is generated, and the voltage applied between the terminals 11 and 12 has a magnetic resistance with the same period as the moving alternating magnetic field. The voltage is divided by the bodies 1a and 1b and output from the intermediate terminal 13. Therefore,
By measuring the frequency of the voltage obtained from this intermediate terminal 13, the moving state of the above-mentioned moving body (24 etc. or 2 etc.), which is the cause of the change in reluctance that changes the resistance of the magnetoresistive elements 1a and 1b, can be detected. It will be possible.

ところで、この中間端子13の電圧はある程度
大きいことが望ましいから、磁気抵抗体1a,1
bと移動体のスリツトや凹凸との相対的位置関係
を同一にした磁気抵抗体の群を使用することが有
利であり、この考え方にしたがつて、第3図、第
4図に示すようになされている場合が一般であ
る。すなわち、1a,1b,1a′,1b′はそれぞ
れが2個の磁気抵抗体の直列回路であり、また、
1aと1a′、1bと1b′とはそれぞれ同一の抵抗
変化をする磁気抵抗体の直列回路である。なお、
磁気抵抗体のそれぞれの群を構成する磁気抵抗体
の数が2に限定される理由はなく、3個なり4個
なり適当な数を選択しうることは云うまでもな
い。
By the way, since it is desirable that the voltage of this intermediate terminal 13 is high to some extent, the magnetic resistors 1a, 1
It is advantageous to use a group of magnetoresistive elements that have the same relative positional relationship between b and the slits and irregularities of the moving body, and according to this idea, as shown in Figs. This is generally the case. That is, 1a, 1b, 1a', 1b' are each a series circuit of two magnetoresistive elements, and
1a and 1a', and 1b and 1b' are series circuits of magnetoresistive bodies each having the same resistance change. In addition,
There is no reason why the number of magnetoresistive elements constituting each group of magnetoresistive elements is limited to two, and it goes without saying that an appropriate number such as three or four may be selected.

更に、第5図、第6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90゜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 Figures 5 and 6, the two sets of position sensors described above are arranged at positions that differ by 90 degrees in electrical angle from each other, and two alternating current voltages having phases that differ by 90 degrees from each other can be obtained. It is clear from the equation below that the position detection accuracy is improved and the direction of rotation can be easily identified.

Acosθsinωt+Asinθcosωt =Bsin(ωt+θ) 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 ωt + Asin θ cos ωt = B sin (ω t + θ) 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5図においては、磁気抵抗体1a,1a′と1
b,1b′との組はスリツト23等とスリツトを有
しない磁性材部24とに対接して第1の磁気抵抗
体回路を構成し、一方、磁気抵抗体1c,1c′と
1d,1d′との組は磁性材部24とスリツト2
3′,23″との境界とスリツト23,23′と磁
性材部24との境界とに対接して第2の磁気抵抗
体回路を構成しており、これら二つの磁気抵抗体
回路は互いに90°電気角位置がずれている。一方、
第6図においては、磁気抵抗体1a,1a′と1
b,1b′との組は突起21等と凹部22等とに対
接して第1の磁気抵抗体回路を構成し、一方、磁
気抵抗体1c,1c′と1d,1d′との組は突起2
1,21′と凹部22′,22″との境界と凹部2
2,22′と突起21,21′との境界と対接して
第2の磁気抵抗体回路を構成しており、これら二
つの磁気抵抗体回路は互いに90°電気角位置がず
れている。
In FIG. 5, magnetoresistive elements 1a, 1a' and 1
The pair of magnetoresistive elements 1c, 1c' and 1d, 1d' constitute a first magnetoresistive circuit by being in contact with the slit 23 etc. and the magnetic material portion 24 without a slit. The pair with magnetic material part 24 and slit 2
3', 23'' and the boundary between the slits 23, 23' and the magnetic material portion 24 constitute a second magnetoresistive circuit, and these two magnetoresistive circuits are arranged at a distance of 90° from each other. °The electrical angle position is shifted.On the other hand,
In FIG. 6, magnetoresistive elements 1a, 1a' and 1
The pair of magnetoresistive elements 1c, 1c' and 1d, 1d' is in contact with the protrusion 21 etc. and the recess 22 etc. to form a first magnetoresistive circuit. 2
1, 21' and the recesses 22', 22'' and the recess 2
A second magnetoresistive circuit is formed in contact with the boundary between the projections 2 and 22' and the protrusions 21 and 21', and these two magnetoresistive circuits are electrically angularly shifted from each other by 90 degrees.

そして、端子11と端子15とは接続してお
き、端子12と端子11間すなわち第1の磁気抵
抗体回路には余弦波を、端子15と端子14との
間すなわち第2の磁気抵抗体回路には正弦波を印
加し、端子13,16間から分圧された位置信号
電圧を得るものである。
Then, the terminals 11 and 15 are connected, and a cosine wave is applied between the terminals 12 and 11, that is, the first magnetoresistive circuit, and a cosine wave is applied between the terminals 15 and 14, that is, the second magnetoresistive circuit. A sine wave is applied to the terminals 13 and 16, and a divided position signal voltage is obtained between the terminals 13 and 16.

ところで、上記の二つの磁気抵抗体回路は同一
の強磁性体板上に形成されることが一般であり、
個々の磁気抵抗体1a,1b等は幅が0.1〜0.2mm
で長さが1mm程度のインジウムアンチモナイド
(InSb)等の膜であり、個々の磁気抵抗体1a,
1b等を接続する導電路5は幅が0.3mm程度で厚
さが数ミクロンの銅膜であり、二つの磁気抵抗体
回路の相互間距離も0.05mm程度と極めて接近して
形成されることが一般であるから、二つの磁気抵
抗体回路間の静電容量はかなり大きく、この静電
容量をもつて二つの磁気抵抗体回路が静電結合し
て相互に干渉することが避け難く、位置センサと
しての検出精度を低下する欠点がある。
By the way, the above two magnetoresistive circuits are generally formed on the same ferromagnetic plate,
The width of each magnetoresistive element 1a, 1b, etc. is 0.1 to 0.2 mm.
It is a film of indium antimonide (InSb) or the like with a length of about 1 mm, and each magnetoresistive element 1a,
The conductive path 5 that connects 1b, etc. is a copper film with a width of about 0.3 mm and a thickness of several microns, and the two magnetoresistive circuits can be formed extremely close to each other with a distance of about 0.05 mm. Generally speaking, the capacitance between two magnetoresistive circuits is quite large, and with this capacitance, it is difficult to prevent the two magnetoresistive circuits from capacitively coupling and interfering with each other. This has the disadvantage of reducing detection accuracy.

(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、特定の方向に移動する磁界と叉交する領域に
特定の距離を隔てて配設され相互に直列に接続さ
れた磁気抵抗体(または数個の磁気抵抗体が直列
に接続された群)の組が一対以上直列に接続され
て直列回路をなし、この直列回路は中間端子を有
する構造を有する第1の磁気抵抗体回路と、これ
と同一の構造ではあるがそれぞれ対応す磁気抵抗
体(または数個の磁気抵抗体が直列に接続された
群)は上記の移動する交番磁界の移動方向に、上
記の特定の距離の1/2ずれて配設されている第2
の磁気抵抗体回路とよりなり、これら二つの磁気
抵抗体回路のそれぞれには90゜位相を異にする正
弦波が印加され、これらの二つの正弦波が上記の
直列に接続された磁気抵抗体回路によつて分圧さ
れて中間端子から得られる二つの交流電圧を利用
して、上記の移動する交番磁界の周波数を測定
し、この移動する交番磁界を発生する移動体の位
置や移動状態等を検出することを基本原理とする
磁気抵抗体を使用してなす位置センサにおいて、
上記第1の磁気抵抗体回路と第2の磁気抵抗体回
路との間に静電誘導現象が発生することが防止さ
れ、検出精度の向上してい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, and the purpose of the present invention is to solve this problem by using a magnetic field that is arranged at a certain distance and connected in series in a region that intersects a magnetic field moving in a certain direction. A first magnetoresistive member having a structure in which a pair or more of resistors (or a group of several magnetoresistive members connected in series) are connected in series to form a series circuit, and this series circuit has an intermediate terminal. A circuit and a corresponding magnetoresistive element (or a group of several magnetoresistive elements connected in series), each having the same structure, move along the above specified distance in the direction of movement of the above-mentioned moving alternating magnetic field. The second
A sine wave with a phase difference of 90° is applied to each of these two magnetoresistive circuits, and these two sine waves are connected to the magnetoresistive circuit connected in series. Using two alternating voltages divided by a circuit and obtained from an intermediate terminal, the frequency of the above-mentioned moving alternating magnetic field is measured, and the position and moving state of the moving object that generates this moving alternating magnetic field is measured. In a position sensor using a magnetic resistor whose basic principle is to detect
A position sensor using a magnetoresistive element that prevents electrostatic induction from occurring between the first magnetoresistive circuit and the second magnetoresistive circuit and improves detection accuracy. It is about providing.

(5) 発明の構成 本発明の構成は、(イ)特定方向に移動する交番磁
界と叉交しうる領域に特定の距離を隔てて配設さ
れ相互に直列に接続された磁気抵抗体(または磁
気抵抗体群)の組を一対以上有する直列回路より
なり、該直列回路は入・出力端子とともに中間端
子を有する第1の磁気抵抗体回路と、(ロ)該第1の
磁気抵抗体回路と同一の幾何学的構造を有するが
それぞれの磁気抵抗体は前記第1の磁気抵抗体回
路を構成する磁気抵抗体のそれぞれ対応する磁気
抵抗体に対し、前記移動する交番磁界の移動方向
に、前記特定の距離の1/2ずれて配設されてなる
第2の磁気抵抗体回路とを有し、(ハ)前記第1の磁
気抵抗体回路と前記第2の磁気抵抗体回路とには
それぞれ、位相を90゜異にする正弦波が印加され、
前記それぞれの中間端子から得られる交流電圧を
測定して前記交番磁界の周波数を検出してなす、
磁気抵抗体を使用してなす位置センサにおいて、
(ニ)前記第1の磁気抵抗体回路と前記第2の磁気抵
抗体回路とは相互に静電遮蔽されてなることを特
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) Structure of the Invention The structure of the present invention consists of (a) magnetoresistive elements (or (a) a first magnetoresistive circuit having an intermediate terminal as well as an input/output terminal; (b) the first magnetoresistive circuit; Although having the same geometrical structure, each magnetoresistive element has a direction of movement of the moving alternating magnetic field with respect to a respective one of the magnetoresistive elements constituting the first magnetoresistive element circuit. (c) the first magnetoresistive circuit and the second magnetoresistive circuit each have a , a sine wave with a phase difference of 90° is applied,
measuring the alternating current voltage obtained from each of the intermediate terminals to detect the frequency of the alternating magnetic field;
In a position sensor using a magnetoresistive element,
(d) A position sensor using a magnetoresistive element is characterized in that the first magnetoresistive circuit and the second magnetoresistive circuit are electrostatically shielded from each other.

本発明の着想自身は一般的に知られている技術
思想ではあるが、二つの磁気抵抗体回路が上記の
ように特異な形状・構造を有するので、所望の静
電遮蔽を実現することは必ずしも容易ではない。
Although the idea of the present invention itself is a generally known technical idea, since the two magnetoresistive circuits have unique shapes and structures as described above, it is not always possible to realize the desired electrostatic shielding. It's not easy.

本発明は、かかる特異的条件を有す磁気抵抗体
回路を使用してなす位置センサにおいて顕著にす
ぐれた静電遮蔽効果を発揮する手段として下記の
二つの手法を完成したものである。
The present invention has completed the following two methods as a means for exhibiting a significantly superior electrostatic shielding effect in a position sensor using a magnetoresistive circuit having such specific conditions.

第1の手段(特許請求の範囲第2項に係る手
段)は、第7図、第8図に示すように、第1の磁
気抵抗体回路と第2の磁気抵抗体回路との磁気抵
抗体を同一の板状の磁性体(フエライト板等)上
にインジウムアンチモナイド(InSb)等磁気抵
抗性材料の薄膜をもつて形成しておき、この磁気
抵抗体相互間を接続する導電体を銅膜等をもつて
形成する工程において、上記二つの回路に挟まれ
た領域に銅膜等の線状導電体を形成するものであ
る。第7図はこの第1の手段(特許請求の範囲第
2項に係る手段)の要旨である磁気抵抗体素子8
の平面図であり、第8図はそのB−B断面図であ
るが、3が板状の磁性体であり、1a,1b等が
磁気抵抗体であり、5が導電体であり、7が静電
遮蔽体であり、9は磁性体板3の表面に磁気抵抗
体1a,1b等を接着する接着剤である。効果確
認のためになした実験の結果により、相互干渉が
15〜20%程度減少することが確認されている。
As shown in FIGS. 7 and 8, the first means (means according to claim 2) includes a magnetoresistive element including a first magnetoresistive circuit and a second magnetoresistive circuit. A thin film of a magnetoresistive material such as indium antimonide (InSb) is formed on the same plate-shaped magnetic material (ferrite plate, etc.), and the conductor connecting the magnetoresistive members is made of copper. In the step of forming a film or the like, a linear conductor such as a copper film is formed in the region sandwiched between the two circuits. FIG. 7 shows a magnetoresistive element 8 which is the gist of this first means (means according to claim 2).
, and FIG. 8 is a cross-sectional view taken along the line B-B. 3 is a plate-shaped magnetic material, 1a, 1b, etc. are magnetoresistive materials, 5 is a conductor, and 7 is a It is an electrostatic shield, and 9 is an adhesive for bonding the magnetic resistors 1a, 1b, etc. to the surface of the magnetic plate 3. The results of an experiment conducted to confirm the effect showed that there was no mutual interference.
It has been confirmed that the amount decreases by about 15-20%.

第2の手段(特許請求の範囲第3項に係る手
段)における磁気抵抗体素子8′はその断面図を
第9図に示すように、第1の磁気抵抗体回路と第
2の磁気抵抗体回路との磁気抵抗体を同一の板状
の強磁性体(フエライト板等)上にインジウムア
ンチモナイド(InSb)等の磁気抵抗性材料の薄
膜をもつて形成しておき、上記二つの回路上に絶
縁物層を介して導電体層を形成してこれを接地し
ておくか、もしくは、空間を介してすなわち上記
二つの磁気抵抗体回路とはわづかに隔離してこれ
と対向する位置に導電体層を支持配設してこれを
接地しておくか、または、磁性体板の裏面に導電
体層を形成してこれを接地しておくか、あるい
は、これら二つの導電体層を双方とも形成して双
方とも接地しておくかするものである。
The magnetoresistive element 8' in the second means (means according to claim 3) has a first magnetoresistive circuit and a second magnetoresistive element, as its cross-sectional view is shown in FIG. The magnetoresistive material for the circuit is formed on the same plate-shaped ferromagnetic material (ferrite plate, etc.) with a thin film of magnetoresistive material such as indium antimonide (InSb), and the magnetoresistive material for the above two circuits is Either form a conductor layer through an insulator layer and ground it, or place it at a position facing the above two magnetoresistive circuits, slightly isolated from them through a space. Either support the conductive layer and ground it, or form a conductive layer on the back of the magnetic plate and ground it, or connect both of these two conductive layers. Both should be formed and both should be grounded.

図において、10,11が導電体接地層であ
る。ただ、導電体接地層10,11の材料は非磁
性材であることが望ましく、磁気抵抗体回路の上
面に形成される導電体接地層10の材料が非磁性
材であることは必須である。
In the figure, numerals 10 and 11 are conductor ground layers. However, it is desirable that the material of the conductive ground layers 10 and 11 is a non-magnetic material, and it is essential that the material of the conductive ground layer 10 formed on the upper surface of the magnetoresistive circuit is a non-magnetic material.

効果確認のためになした実験の結果により、相
互干渉が35〜45%程度減少することが確認されて
いる。
The results of experiments conducted to confirm the effect have confirmed that mutual interference is reduced by about 35 to 45%.

(6) 発明の実施例 以下図面を参照しつつ、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について更
に説明する。
(6) Embodiments of the Invention Hereinafter, a position sensor using a magnetoresistive element according to an embodiment of the present invention will be further described with reference to the drawings.

() 特許請求の範囲第6項によつて限定される
特許請求の範囲第2項の実施例 第10図参照 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はフエライ
ト等強磁性体よりなる板状磁性体であり、本例に
おいては高さが数mmで幅が数mmで厚さが0.5mm程
度である。
() Refer to Figure 10, an embodiment of claim 2, which is limited by claim 6. In the figure, 4 is a permanent magnet, which forms a parallel magnetic field H of approximately 1 kilogauss. . 3 is a plate-shaped magnetic body made of a ferromagnetic material such as ferrite, and in this example, the height is several mm, the width is several mm, and the thickness is about 0.5 mm.

1dはインジウムアンチモナイド(InSb)よ
りなる磁気抵抗体であり、厚さは約5μmである。
その幅は0.3mmであり、その長さは1mm程度であ
り、その高さは1.5mm程度である。銅膜をもつて
形成された導電路5と静電遮蔽体7の幅は0.3mm
程度である。磁気抵抗体1a,1b等と静電遮蔽
体7と導電路5とはフオトリソグラフイー法とイ
オンプレーテイング法、スパツタリング法、真空
蒸着法等と接着剤を使用してなす接着法との組み
合わせでもつて容易に形成しうる。
1d is a magnetoresistive material made of indium antimonide (InSb) and has a thickness of about 5 μm.
Its width is 0.3 mm, its length is about 1 mm, and its height is about 1.5 mm. The width of the conductive path 5 and electrostatic shield 7 formed with a copper film is 0.3 mm.
That's about it. The magnetoresistive elements 1a, 1b, etc., the electrostatic shield 7, and the conductive path 5 can be formed by a combination of a photolithography method, an ion plating method, a sputtering method, a vacuum evaporation method, etc., and an adhesive method using an adhesive. can be easily formed.

この磁気抵抗体素子8の構造が第7図、第8図
に示すとおりであることは云うまでもない。24
1はスリツト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1a,1b
等とは0.3mm程度の距離を隔てて配設される。
It goes without saying that the structure of this magnetoresistive element 8 is as shown in FIGS. 7 and 8. 24
1 is a cylindrical member having a slit 231;
It rotates around the axis 6, and the magnetic resistance elements 1a and 1b
etc., with a distance of approximately 0.3 mm.

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11,15,17を共通端子と
して接地し、端子12−11間に5V程度の余弦
波を印加すると、静電誘導作用により端子13,
11間のみならず15,16間にもある程度電圧
の発生は避け難いが、その程度は0.3mVであり従
来技術における場合より15〜20%程度減少してい
る。
When terminals 11, 15, and 17 of a position sensor made using a magnetic resistor with the above structure are grounded as a common terminal, and a cosine wave of about 5V is applied between terminals 12 and 11, electrostatic induction causes terminal 13,
Although it is unavoidable that a certain amount of voltage is generated not only between 11 but also between 15 and 16, the level of voltage is 0.3 mV, which is about 15 to 20% lower than in the prior art.

() 特許請求の範囲第5項によつて限定される
特許請求の範囲第3項記載の実施例 第11図参照 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はフエライ
ト等強磁性体よりなる板状磁性体であり、本例に
おいては高さが数mmで幅が数mmで厚さが0.5mm程
度である。
() Refer to Figure 11 of the embodiment described in claim 3, which is limited by claim 5. In the figure, 4 is a permanent magnet, which forms a parallel magnetic field H of approximately 1 kilogauss. do. 3 is a plate-shaped magnetic body made of a ferromagnetic material such as ferrite, and in this example, the height is several mm, the width is several mm, and the thickness is about 0.5 mm.

1dはインジウムアンチモナイド(InSb)よ
りなる磁気抵抗体であり、厚さは約5μmである。
その幅は0.3mmであり、その長さは1mm程度であ
り、その高さは1.5mm程度である。銅膜をもつて
形成された導電路5の幅は0.3mm程度であり、静
電遮蔽体10,11は厚さが0.1mm程度であるリ
ン青銅板であり、磁気抵抗体1a,1b等上にお
いて接着剤の厚さは0.1mm程度である。磁気抵抗
体1a,1bと静電遮蔽体10,11と導電路5
とはフオトリソグラフイー法とイオンプレーテイ
ング法、スパツタリング法、真空蒸着法等と接着
剤を使用してなす接着法との組み合わせでもつて
容易に形成しうる。
1d is a magnetoresistive material made of indium antimonide (InSb) and has a thickness of about 5 μm.
Its width is 0.3 mm, its length is about 1 mm, and its height is about 1.5 mm. The width of the conductive path 5 formed with a copper film is about 0.3 mm, and the electrostatic shields 10 and 11 are phosphor bronze plates with a thickness of about 0.1 mm. The thickness of the adhesive is about 0.1 mm. Magnetoresistive elements 1a and 1b, electrostatic shields 10 and 11, and conductive path 5
It can be easily formed by a combination of a photolithography method, an ion plating method, a sputtering method, a vacuum evaporation method, etc., and an adhesive method using an adhesive.

この磁気抵抗体素子8′の構造が第9図に示す
とおりであることは云うまでもない。
It goes without saying that the structure of this magnetoresistive element 8' is as shown in FIG.

2は規則的凹凸21,22等を有する棒状部材
であり、矢印Aの方向に移動する。そして、磁気
抵抗体1a,1b等とは0.3mm程度の距離を隔て
て配設される。
2 is a rod-shaped member having regular unevenness 21, 22, etc., and moves in the direction of arrow A. The magnetoresistive elements 1a, 1b, etc. are arranged at a distance of about 0.3 mm.

上記のような構造の磁気抵抗体を使用してなす
位置センサの静電遮蔽体10,11を接地し、端
子11,15間に5V程度の余弦波を印加すると、
静電誘導作用により端子13,11間のみならず
15,16間にもある程度電圧の発生は避け難い
が、その程度は0.1mV程度であり従来技術におけ
る場合より35〜45%程度減少している。
When the electrostatic shields 10 and 11 of the position sensor made using the magnetic resistor with the above structure are grounded and a cosine wave of about 5V is applied between the terminals 11 and 15,
Although it is unavoidable that some voltage is generated not only between terminals 13 and 11 but also between terminals 15 and 16 due to electrostatic induction, the level is about 0.1 mV, which is about 35 to 45% lower than in the conventional technology. .

(7) 発明の効果 以上説明せるとおり、本発明によれば特定の方
向に移動する磁界と叉交する領域に特定の距離を
隔てて配設され相互に直列に接続された磁気抵抗
体(または数個の磁気抵抗体が直列に接続された
群)の組が一対以上直列に接続されて直列回路を
なし、この直列回路は中間端子を有する構造を有
する第1の磁気抵抗体回路と、これと同一の構造
ではあるがそれぞれ対応する磁気抵抗体(または
数個の磁気抵抗体が直列に接続された群)は上記
の移動する交番磁界の移動方向に、上記の特定の
距離の1/2ずれて配設されている第2の磁気抵抗
体回路とよりなり、これら二つの磁気抵抗体回路
のそれぞれには90゜位相を異にする正弦波が印加
され、これらの二つの正弦波が上記の直列に接続
された磁気抵抗体回路によつて分圧されて中間端
子から得られる二つの交流電圧を利用して、上記
の移動する交番磁界の周波数を測定し、この移動
する交番磁界を発生する移動体の位置や移動状態
等を検出することを基本原理とする磁気抵抗体を
使用してなす位置センサにおいて、上記第1の磁
気抵抗体回路と第2の磁気抵抗体回路との間に静
電誘導現象が発生することが防止され、検出精度
の向上してい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) Effects of the Invention As explained above, according to the present invention, magnetoresistive elements (or A group of several magnetoresistive elements connected in series) are connected in series to form a series circuit, and this series circuit includes a first magnetoresistive element circuit having a structure having an intermediate terminal; Each magnetoresistive element (or a group of several magnetoresistive elements connected in series), which has the same structure as , moves in the direction of movement of the above-mentioned moving alternating magnetic field by 1/2 of the above-mentioned specific distance. A sine wave having a phase difference of 90° is applied to each of these two magnetoresistive circuits, and these two sine waves The frequency of the above-mentioned moving alternating magnetic field is measured by using the two alternating current voltages obtained from the intermediate terminal after being divided by the magnetoresistive circuit connected in series, and this moving alternating magnetic field is generated. In a position sensor using a magnetoresistive element whose basic principle is to detect the position and movement state of a moving object, there is a wire between the first magnetoresistive circuit and the second magnetoresistive circuit. It is possible to provide a position sensor using a magnetoresistive element that prevents electrostatic induction from occurring and has improved detection accuracy.

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

第1図〜第6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概念的構成図であ
る。第7図、第8図は特許請求の範囲第2項記載
の磁気抵抗体を使用してなす位置センサの要旨に
係る磁気抵抗体素子のそれぞれ平面図とB−B断
面図である。第9図は特許請求の範囲第3項記載
の磁気抵抗体を使用してなす位置センサの要旨に
係る磁気抵抗体素子の断面図である。第10図、
第11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概念的構成図である。 1a,1a′,1b,1b′,1c,1c′,1d,
1d′…磁気抵抗体、11,12,14,15…主
端子、13,16…中間端子、17…接地端子、
2,24…棒状部材、241…円筒状部材、2
1,21′…突起、22,22′…凹部、23,2
3′,231…スリツト、3…板状磁性体、4…
永久磁石、5…導電部材、6…回転体の軸、7,
10,11…静電遮蔽体、8,8′…磁気抵抗体
素子、9…接着剤、A…物体の移動方向、H…磁
界方向、E…従来技術にかか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。
1 to 6 are conceptual configuration diagrams of a position sensor using a magnetoresistive element in the prior art. 7 and 8 are a plan view and a cross-sectional view taken along line B--B of a magnetoresistive element according to the gist of a position sensor using a magnetoresistive member according to claim 2, respectively. FIG. 9 is a sectional view of a magnetoresistive element according to the gist of a position sensor using a magnetoresistive member according to claim 3. Figure 10,
FIG. 11 is a conceptual configuration diagram of a position sensor using a magnetic resistor according to an embodiment of the present invention. 1a, 1a', 1b, 1b', 1c, 1c', 1d,
1d'... Magnetic resistance element, 11, 12, 14, 15... Main terminal, 13, 16... Intermediate terminal, 17... Ground terminal,
2, 24... Rod-shaped member, 241... Cylindrical member, 2
1, 21'...protrusion, 22, 22'...recess, 23, 2
3', 231...Slit, 3...Plate magnetic material, 4...
Permanent magnet, 5... Conductive member, 6... Axis of rotating body, 7,
10, 11... Electrostatic shield, 8, 8'... Magnetoresistive element, 9... Adhesive, A... Direction of movement of object, H... Direction of magnetic field, E... Made using magnetoresistive element according to prior art. Voltage waveform obtained from the intermediate terminal of the position sensor.

Claims (1)

【特許請求の範囲】 1 (イ)特定方向に移動する交番磁界と叉交しうる
領域に特定の距離を隔てて配設され相互に直列に
接続された磁気抵抗体(または磁気抵抗体群)の
組を一対以上有する直列回路よりなり、該直列回
路は入・出力端子とともに中間端子を有する第1
の磁気抵抗体回路と、(ロ)該第1の磁気抵抗体回路
と同一の幾何学的構造を有するがそれぞれの磁気
抵抗体は前記第1の磁気抵抗体回路を構成する磁
気抵抗体のそれぞれ対応する磁気抵抗体に対し、
前記移動する交番磁界の移動方向に、前記特定の
距離の1/2ずれて配設されてなる第2の磁気抵抗
体回路とを有し、(ハ)前記第1の磁気抵抗体回路と
前記第2の磁気抵抗体回路とにはそれぞれ、位相
を90゜異にする正弦波が印加され、前記それぞれ
の中間端子から得られる交流電圧を測定して前記
交番磁界の周波数を検出してなす、磁気抵抗体を
使用してなす位置センサにおいて、(ニ)前記第1の
磁気抵抗体回路と前記第2の磁気抵抗体回路とは
相互に静電遮蔽されてな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。 2 前記第1の磁気抵抗体回路と前記第2の磁気
抵抗体回路とは同一の板状の磁性体上に形成さ
れ、前記静電遮蔽は前記二つの回路に挟まれた領
域において前記板状磁性体上に形成された線状導
電体をもつて実現されてな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 前記第1の磁気抵抗体回路と前記第2の磁気
抵抗体回路とは同一の板状の磁性体上に形成さ
れ、前記静電遮蔽は前記二つの磁気抵抗体回路上
に絶縁物層を介してまたは空間を介して前記二つ
の磁気抵抗体回路とは隔離してこれと対向する位
置に配設された導電体層及び/または前記板状磁
性体の前記二つの磁気抵抗体回路が形成されてい
ない側の面上に配設された、導電体層をもつて実
現されてな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 前記特定方向に移動する交番磁束は、前記二
つ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、前記二つの磁気抵抗体回路
の他方の面に対向して前記特定方向に移動し規則
的に形成された歯車状凹凸を有する円筒状部材の
回転に起因するリラクタンスの変化とによつて実
現される、特許請求の範囲第1項、第2項、また
は第3項記載の磁気抵抗体を使用してなす位置セ
ンサ。 5 前記特定方向に移動する交番磁束は、前記二
つ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、前記二つの磁気抵抗体回路
の他方の面に対向して前記特定方向に移動し規則
的に形成されたラツ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リラクタンスの
変化とによつて実現される、特許請求の範囲第1
項、第2項、または第3項記載の磁気抵抗体を使
用してなす位置センサ。 6 前記特定方向に移動する交番磁束は、前記二
つ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、前記二つの磁気抵抗体回路
の他方の面に対向して前記特定方向に移動し規則
的に形成されたスリツトを有する円筒状部材の回
転に起因するリラクタンスの変化とによつて実現
される、特許請求の範囲第1項、第2項、または
第3項記載の磁気抵抗体を使用してなす位置セン
サ。 7 前記特定方向に移動する交番磁束は、前記二
つ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、前記二つの磁気抵抗体回路
の他方の面に対向して前記特定方向に移動し規則
的に形成されたスリツ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リラクタンスの変化
とによつて実現される、特許請求の範囲第1項、
第2項、または第3項記載の磁気抵抗体を使用し
てなす位置センサ。
[Claims] 1. (a) Magnetoresistive elements (or a group of magnetoresistive elements) arranged in a region that can intersect an alternating magnetic field moving in a specific direction at a specific distance and connected to each other in series. The series circuit consists of a series circuit having one or more pairs of input/output terminals as well as a first terminal having an intermediate terminal.
and (b) having the same geometrical structure as the first magnetoresistive circuit, but each magnetoresistive member is a magnetoresistive member of each of the magnetoresistive members constituting the first magnetoresistive circuit. For the corresponding magnetoresistive element,
a second magnetoresistive circuit disposed offset by 1/2 of the specific distance in the moving direction of the moving alternating magnetic field, (c) the first magnetoresistive circuit and the A sine wave having a phase difference of 90° from each other is applied to each of the second magnetoresistive circuits, and the frequency of the alternating magnetic field is detected by measuring the alternating current voltage obtained from the respective intermediate terminals. A position sensor using a magnetoresistive element, characterized in that (d) the first magnetoresistive circuit and the second magnetoresistive circuit are electrostatically shielded from each other. A position sensor that uses the body. 2. The first magnetoresistive circuit and the second magnetoresistive circuit are formed on the same plate-shaped magnetic body, and the electrostatic shield is formed on the plate-shaped magnetic body in a region sandwiched between the two circuits. Claim 1 realized with a linear conductor formed on a magnetic material
A position sensor made using the magnetoresistive material described in 2. 3. The first magnetoresistive circuit and the second magnetoresistive circuit are formed on the same plate-shaped magnetic material, and the electrostatic shielding includes an insulating layer on the two magnetoresistive circuits. The two magnetoresistive circuits of the conductor layer and/or the plate-shaped magnetic body are formed in a position that is isolated from and faces the two magnetoresistive circuits through or through a space. A position sensor made using the magnetoresistive material according to claim 1, which is realized by having a conductive layer disposed on the non-conductive side surface. 4. The alternating magnetic flux moving in the specific direction is generated by a magnetic flux generating means disposed facing one surface of the two magnetoresistive circuits, and a magnetic flux generating means disposed facing the other surface of the two magnetoresistive circuits. A change in reluctance caused by the rotation of the cylindrical member that moves in the specific direction and has regularly formed gear-like unevenness. A position sensor made using the magnetic resistor described in item 3. 5. The alternating magnetic flux moving in the specific direction is generated by a magnetic flux generating means disposed facing one surface of the two magnetoresistive circuits, and a magnetic flux generating means disposed facing the other surface of the two magnetoresistive circuits. A change in reluctance caused by the movement of a rod-shaped member that moves in the specific direction and has regularly formed rack-like unevenness in the specific direction.
A position sensor made using the magnetoresistive body according to item 1, 2, or 3. 6. The alternating magnetic flux moving in the specific direction is generated by a magnetic flux generating means disposed facing one surface of the two magnetoresistive circuits and a magnetic flux generating means disposed facing the other surface of the two magnetoresistive circuits. A change in reluctance caused by the rotation of the cylindrical member that moves in the specific direction and has regularly formed slits, according to claim 1, 2, or 3. A position sensor made using the magnetoresistive material described above. 7. The alternating magnetic flux moving in the specific direction is generated by a magnetic flux generating means disposed facing one surface of the two magnetoresistive circuits and a magnetic flux generating means disposed facing the other surface of the two magnetoresistive circuits. and a change in reluctance caused by the movement of a rod-shaped member having regularly formed slits in the specific direction.
A position sensor made using the magnetic resistance body according to item 2 or 3.
JP13873383A 1983-07-30 1983-07-30 Position sensor wherein magnetoresistance body is used Granted JPS6031015A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13873383A JPS6031015A (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
JP13873383A JPS6031015A (en) 1983-07-30 1983-07-30 Position sensor wherein magnetoresistance body is used

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JPS6031015A JPS6031015A (en) 1985-02-16
JPH0410570B2 true JPH0410570B2 (en) 1992-02-25

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JP13873383A Granted JPS6031015A (en) 1983-07-30 1983-07-30 Position sensor wherein magnetoresistance body is used

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Publication number Priority date Publication date Assignee Title
JPS63122278U (en) * 1987-01-31 1988-08-09
JP2978582B2 (en) * 1991-03-29 1999-11-15 株式会社小松製作所 Method and apparatus for detecting electromagnetic characteristic change section
DE19602230A1 (en) * 1996-01-23 1997-07-24 Teves Gmbh Alfred sensor

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JPS6031015A (en) 1985-02-16

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