Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0777166B2 - Non-contact type potentiometer - Google Patents
[go: Go Back, main page]

JPH0777166B2 - Non-contact type potentiometer - Google Patents

Non-contact type potentiometer

Info

Publication number
JPH0777166B2
JPH0777166B2 JP61198776A JP19877686A JPH0777166B2 JP H0777166 B2 JPH0777166 B2 JP H0777166B2 JP 61198776 A JP61198776 A JP 61198776A JP 19877686 A JP19877686 A JP 19877686A JP H0777166 B2 JPH0777166 B2 JP H0777166B2
Authority
JP
Japan
Prior art keywords
magnetic
rotor
magnetic field
permanent magnet
ferromagnetic magnetoresistive
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 - Fee Related
Application number
JP61198776A
Other languages
Japanese (ja)
Other versions
JPS6354783A (en
Inventor
利和 松下
勝彦 有賀
好 吉野
建一 青
俊和 荒砂
Original Assignee
日本電装株式会社
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 日本電装株式会社 filed Critical 日本電装株式会社
Priority to JP61198776A priority Critical patent/JPH0777166B2/en
Priority to EP87110695A priority patent/EP0255052B1/en
Priority to DE3788831T priority patent/DE3788831T2/en
Priority to US07/076,891 priority patent/US4835509A/en
Priority to KR1019870008259A priority patent/KR900007100B1/en
Publication of JPS6354783A publication Critical patent/JPS6354783A/en
Publication of JPH0777166B2 publication Critical patent/JPH0777166B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Adjustable Resistors (AREA)
  • Hall/Mr Elements (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] この発明は、磁気力の相互作用によりロータの回転角度
を検出する非接触式ポテンショメータに関し、特には磁
気力により抵抗値が減少する強磁性磁気抵抗素子を用い
た非接触式ポテンショメータに関する。
Description: TECHNICAL FIELD The present invention relates to a non-contact potentiometer that detects a rotation angle of a rotor by the interaction of magnetic forces, and particularly, a ferromagnetic magnet whose resistance value is reduced by the magnetic force. The present invention relates to a non-contact type potentiometer using a resistance element.

[従来の技術] 非接触ポテンショメータの磁気回路は、従来より有底円
筒状コアや回転磁性体および永久磁石とともに、閉磁路
として構成され、回転磁性体の先端部分に形成した間隙
に磁気抵抗素子であるInSnを配置して回転磁性体の回転
に応じた出力を発生するようになっており、そしてしか
して回転磁性体の先端部分に形成した間隙の大きさを変
えることにより換言すれば回転磁性体の先端を所定の関
数加工することにより前述したようなInSb製の磁気抵抗
素子から所定の関数出力を得ている。
[Prior Art] The magnetic circuit of a non-contact potentiometer has conventionally been configured as a closed magnetic circuit together with a bottomed cylindrical core, a rotating magnetic body, and a permanent magnet, and a magnetic resistance element is provided in a gap formed at the tip of the rotating magnetic body. An InSn is arranged to generate an output according to the rotation of the rotating magnetic body, and in other words, by changing the size of the gap formed at the tip of the rotating magnetic body, in other words, the rotating magnetic body is changed. A predetermined function output is obtained from the InSb magnetoresistive element as described above by processing the tip of the above with a predetermined function.

[発明が解決しようとする問題点] この場合には、永久磁石は磁気抵抗素子の略半分に対応
しているが、永久磁石の両端部から磁束力が永久磁石と
は対応しない部分の磁気抵抗素子に及ぶことは避けられ
ず、回転角度と出力との関係が不正確になり、ひいては
ポテンショメータが適用される速度メータとかスロット
ルポジションセンサといった各種色々の機器の作動にお
ける信頼性が乏しくなる問題がある。
[Problems to be Solved by the Invention] In this case, the permanent magnet corresponds to approximately half of the magnetoresistive element, but the magnetic resistance of the portion where the magnetic flux force from both ends of the permanent magnet does not correspond to the permanent magnet. Inevitably, the relationship between the rotation angle and the output will be inaccurate, and the reliability of the operation of various devices such as the speedometer to which the potentiometer is applied and the throttle position sensor will be poor. .

この発明はこの問題点をなくすべく行なわれたもので、
磁界発生手段の両端部からの磁気漏洩を局力防ぐことに
より磁界発生手段の両端部の磁束力が磁界発生手段とは
対応しない部分の磁気抵抗素子に及ばないようになり、
正確な回転角度と出力との関係が保たれ、ひいては色々
の機器の作動における高い信頼性が得られるといった優
れた効果を有する非接触式ポテンショメータを提供する
ことを目的とする。
This invention was made to eliminate this problem.
By locally preventing magnetic leakage from both ends of the magnetic field generation means, the magnetic flux force at both ends of the magnetic field generation means does not reach the magnetoresistive element in a portion that does not correspond to the magnetic field generation means.
It is an object of the present invention to provide a non-contact potentiometer having an excellent effect that an accurate relationship between a rotation angle and an output is maintained, and thus high reliability in operation of various devices is obtained.

[問題点を解決するための手段] この発明は、ハウジングと、このハウジング内に回転可
能に設けられたロータと、このロータに同心的で該ロー
タから所定の間隔を隔てるようにして配設された所定形
状の強磁性磁気抵抗素子を有する絶縁基板と、前記ロー
タ側に前記強磁性磁気抵抗素子の一部分に近接して装着
されて前記ロータと共に回転すると共に、前記ロータの
同心円の径方向の面で両端部を区切られて前記ロータと
同心の円弧状に形成され、前記一部分に前記ロータの径
方向に磁界を印加する磁界発生手段と、前記径方向の面
に取付けられ前記磁界発生手段の磁界が前記径方向の面
から漏洩するのを防ぐ磁性材料製の磁気漏洩防止部材と
を備える構成を採用している。
[Means for Solving the Problems] According to the present invention, a housing, a rotor rotatably provided in the housing, and a rotor that is concentric with the rotor and is spaced apart from the rotor by a predetermined distance are provided. An insulating substrate having a ferromagnetic magnetoresistive element having a predetermined shape, and a rotor concentric with a radial surface of the rotor mounted on the rotor side in proximity to a part of the ferromagnetic magnetoresistive element. And a magnetic field generating means for applying a magnetic field in the radial direction of the rotor to the part, the magnetic field of the magnetic field generating means being attached to the radial surface, Is provided with a magnetic leakage prevention member made of a magnetic material that prevents leakage from the radial surface.

[作用] 上記のように構成したこの発明によれば、磁界発生手段
の両端部からの磁束は磁性材料製の磁気漏洩防止部材に
より吸収されるようになり、磁界発生手段の両端部から
出る磁力線が強磁性磁気抵抗素子の内磁界発生手段が近
接する一部分以外に及ばないようになり、正確な回転角
度と出力との関係が保たれ、ひいては色々の機器の作動
における高い信頼性が得られるようになる。
[Operation] According to the present invention configured as described above, the magnetic flux from both ends of the magnetic field generation means is absorbed by the magnetic leakage prevention members made of a magnetic material, and the magnetic force lines emitted from both ends of the magnetic field generation means. So that the inner magnetic field generating means of the ferromagnetic magnetoresistive element does not extend to a portion other than the adjacent portion, the accurate relationship between the rotation angle and the output is maintained, and thus high reliability in the operation of various devices can be obtained. become.

[発明の効果] 上記のように構成したこの発明によれば、磁界発生手段
の両端部からの磁束は磁性材料製の磁気漏洩防止部材に
より収束されるようになり、磁界発生手段の磁力線が強
磁性磁気抵抗素子の内磁界発生手段が近接する一部分以
外に及ばないようになり、正確な回転角度と出力との関
係が保たれ、製品相互間の出力特性のばらつきも少なく
なり、ひいては色々の機器の作動における高い信頼性が
得られるといった優れた効果を奏する非接触式ポテンシ
ョメータを提供することができる。
[Advantages of the Invention] According to the present invention configured as described above, the magnetic flux from both ends of the magnetic field generation means is converged by the magnetic leakage prevention members made of a magnetic material, and the magnetic field lines of the magnetic field generation means are strong. The internal magnetic field generating means of the magnetic magnetoresistive element does not extend beyond a portion close to the magnetic magnetoresistive element, the accurate relationship between the rotation angle and the output is maintained, the variation in output characteristics between products is reduced, and eventually various devices are used. It is possible to provide a non-contact potentiometer having an excellent effect that high reliability can be obtained in the operation of.

[実施例] 以下この発明の実施例を図面に基づいて説明する。第1
図に本発明の一実施例を示し、同図(a)にその上面
図、同図(b)に図(a)中におけるA−A線断面図を
示す。図においての構成は、回路基板としての絶縁基板
1上に、開口部を持つ円形または多角形の形状で、Ni-F
e、Ni-Coなどの薄膜から成る強磁性磁気抵抗素子2a、2b
を形成し、その開口部の一方の端部3を電源電圧Vccに
接続し、もう一方の端子4を接地(GND)している。ま
た、強磁性磁気抵抗素子2a、2b内から出力端子5をVout
として取り出すよう接続されている。そして、強磁性磁
気抵抗素子2a、2bと所定の間隔をもって半円弧状の永久
磁石6が絶縁基板1の強磁性磁気抵抗素子2a、2b側に取
り付けられている。
Embodiments Embodiments of the present invention will be described below with reference to the drawings. First
An embodiment of the present invention is shown in the figure, a top view thereof is shown in the same figure (a), and a cross-sectional view taken along line AA in the same figure is shown in the same figure (b). The configuration shown in the figure is a circular or polygonal shape with an opening on an insulating substrate 1 as a circuit board, and is made of Ni-F.
Ferromagnetic magnetoresistive elements 2a, 2b made of thin films of e, Ni-Co, etc.
Is formed, one end 3 of the opening is connected to the power supply voltage Vcc, and the other terminal 4 is grounded (GND). In addition, the output terminal 5 is Vout from within the ferromagnetic magnetoresistive elements 2a and 2b.
Connected to take out as. Then, a semi-circular arc-shaped permanent magnet 6 is attached to the ferromagnetic magnetoresistive elements 2a, 2b of the insulating substrate 1 at a predetermined distance from the ferromagnetic magnetoresistive elements 2a, 2b.

この様子ないしは態様を第2図をも参照しながら、さら
に詳らかに述べると、上端閉塞型の筒状ハウジング7内
には円盤状のロータ8が配設されており、ロータ8の回
転軸9は上下方向に指向し、ハウジング7の上面部を貫
通し軸受10により支持されている。ハウジング7の下端
開口部にはケース11が閉塞状態に設けられ、その上面に
は絶縁基板1が装着されている。磁界発生手段としての
永久磁石6は半円弧状を成し、これはロータ8の外周面
に取り付けられ強磁性磁気抵抗素子2aと上下に対向する
状態で同心的となるように配置されている。このとき、
永久磁石6の両端部には鉄片など磁性材料により形成さ
れた一対の磁気漏洩防止部材12が例えば商標名をアロン
アルファとするなどといった接着剤などにより取り付け
られている。そして、かかる永久磁石6ならびに強磁性
磁気抵抗素子2a、2bでもって第1図(b)に記号iで示
すように閉磁路が形成されるようになっている。
This state or mode will be described in more detail with reference to FIG. 2 as well. A disk-shaped rotor 8 is provided in a cylindrical housing 7 with a closed upper end, and a rotary shaft 9 of the rotor 8 is It is oriented in the vertical direction, penetrates the upper surface of the housing 7, and is supported by bearings 10. A case 11 is provided in a closed state at the lower end opening of the housing 7, and an insulating substrate 1 is mounted on the upper surface of the case 11. The permanent magnet 6 as a magnetic field generating means has a semicircular arc shape, which is attached to the outer peripheral surface of the rotor 8 and is arranged so as to be concentric with the ferromagnetic magnetoresistive element 2a so as to face it vertically. At this time,
A pair of magnetic leakage prevention members 12 made of a magnetic material such as iron pieces are attached to both ends of the permanent magnet 6 with an adhesive or the like having a trademark name of Aron Alpha. The permanent magnet 6 and the ferromagnetic magnetoresistive elements 2a and 2b form a closed magnetic path as indicated by the symbol i in FIG. 1 (b).

また、永久磁石6は強磁性磁気抵抗素子2a、2bの中心を
回転軸の中心にして強磁性磁気抵抗素子2a、2bの周方向
に回転するものであり、永久磁石6が強磁性磁気抵抗素
子2a、2bに向けて発生する磁界の強度の絶対値は強磁性
磁気抵抗素子2a、2bの飽和磁界強度以上となるように実
施例上、設定されている。また、その磁界は強磁性磁気
抵抗素子2a、2bの周方向に垂直な方向すなわち、半径方
向に印加されている。
Further, the permanent magnet 6 rotates in the circumferential direction of the ferromagnetic magnetoresistive elements 2a and 2b with the centers of the ferromagnetic magnetoresistive elements 2a and 2b as the centers of rotation axes. In the embodiment, the absolute value of the strength of the magnetic field generated toward 2a and 2b is set to be equal to or higher than the saturation magnetic field strength of the ferromagnetic magnetoresistive elements 2a and 2b. The magnetic field is applied in the direction perpendicular to the circumferential direction of the ferromagnetic magnetoresistive elements 2a and 2b, that is, in the radial direction.

つぎに上記のように構成したポテンショメータの作用に
ついて説明する。
Next, the operation of the potentiometer configured as described above will be described.

強磁性磁気抵抗素子2a、2bは永久磁石6により電流方向
に対して垂直の方向から磁界を受けるとその抵抗値が減
少する。そして永久磁石6が強磁性磁気抵抗素子2a、2b
の周方向に回転することにより強磁性磁気抵抗素子2a、
2b内の抵抗値減少部分も連続的に回転移動する。このた
め接地端子と出力端子Voutとの間の抵抗値と、出力端子
Voutと電源電圧Vcc端子との抵抗値との比によって決定
される電源電圧Vccの分圧値としての出力Voutの値は第
2図に示すような直線性を持ったものとなる。
When the permanent magnet 6 receives a magnetic field from the direction perpendicular to the current direction, the resistance values of the ferromagnetic magnetoresistive elements 2a and 2b decrease. And the permanent magnet 6 is the ferromagnetic magnetoresistive element 2a, 2b.
By rotating in the circumferential direction of the ferromagnetic magnetoresistive element 2a,
The portion where the resistance value decreases in 2b also rotates continuously. Therefore, the resistance value between the ground terminal and the output terminal Vout and the output terminal
The value of the output Vout as the divided value of the power supply voltage Vcc determined by the ratio of the resistance value of the Vout to the resistance value of the power supply voltage Vcc terminal has a linearity as shown in FIG.

なお、第3図において回転角度0degとは第1図における
永久磁石6の直線の辺6cが図中のA−A線に垂直であ
り、また、図中左側に永久磁石6が配置するときであ
る。また、第3図はその位置から第1図において右回転
する特性を示しているが、回転方向はどちらでもよい。
The rotation angle 0 deg in FIG. 3 means that the straight side 6c of the permanent magnet 6 in FIG. 1 is perpendicular to the line AA in the figure, and the permanent magnet 6 is arranged on the left side in the figure. is there. Further, although FIG. 3 shows the characteristic of right rotation from that position in FIG. 1, either direction of rotation may be used.

そして、強磁性磁気抵抗素子2a、2bは第4図のグラフに
その特性(実線)を示す如く飽和磁界(一点鎖線)以上
の磁界強度(絶対値)を受けるとその抵抗値の減少が一
定となる(抵抗値が略一定となる)ため出力Voutの値が
実際の実施例上、永久磁石6の取り付け誤差および着磁
強度の多少の変動に依存することがなくなる。なお、第
4図においてInSbの特性を点線で示すが、InSbは磁界強
度が大となる程抵抗値が大となることが分かる。
The ferromagnetic magnetoresistive elements 2a and 2b show a constant decrease in their resistance values when subjected to a magnetic field strength (absolute value) equal to or higher than the saturation magnetic field (dashed line) as shown by the characteristic (solid line) in the graph of FIG. Since (the resistance value becomes substantially constant), the value of the output Vout does not depend on the mounting error of the permanent magnet 6 and the slight fluctuation of the magnetizing strength in the actual embodiment. It should be noted that the characteristic of InSb is shown by a dotted line in FIG. 4, but it can be seen that the resistance value of InSb increases as the magnetic field strength increases.

このように上記の構成では、永久磁石6の両端部に磁気
漏洩防止部12を設けたので、永久磁石6の両端部からの
磁力は磁性材料性の磁気漏洩防止部12により吸収される
ようになり、永久磁石6の両端部の磁気力が永久磁石6
とは対応しない部分の強磁性磁気抵抗素子2bに及ばない
ようになり、回転角度と出力との関係が所定どおり正確
に保たれ、ひいては各種といった色々の機器の計測にお
ける高い信頼性が得られる。
As described above, in the above structure, since the magnetic leakage prevention portions 12 are provided at both ends of the permanent magnet 6, the magnetic force from both ends of the permanent magnet 6 is absorbed by the magnetic leakage prevention portion 12 made of a magnetic material. Therefore, the magnetic force at both ends of the permanent magnet 6 becomes
Since it does not reach the ferromagnetic magnetoresistive element 2b which does not correspond to, the relationship between the rotation angle and the output can be maintained exactly as specified, and high reliability can be obtained in the measurement of various kinds of devices.

このように永久磁石6の両端部からの磁気漏洩が防止さ
れることに伴い第3図に実線で示すように破線のものに
比較して波高値が大となり直線部分が増大するためポテ
ンショメータとしての出力処理、すなわち増幅回路処理
などが容易となる。
In this way, magnetic leakage from both ends of the permanent magnet 6 is prevented, and as shown by the solid line in FIG. 3, the peak value becomes larger and the linear portion increases as compared with the broken line, so that the potentiometer is used. Output processing, that is, amplification circuit processing and the like are facilitated.

つぎに第5図(a)、(b)はこの発明の第2実施例を
示す。この第2実施例が第1実施例と相違するところは
下記の如くである。すなわち、第1実施例では永久磁石
6を強磁性磁気抵抗素子2a、2bに対して上下に対応する
ように位置させたが、この第2実施例では、永久磁石6
の半径を強磁性磁気抵抗素子2aの半径より若干大とし、
永久磁石6が強磁性磁気抵抗素子2aの外周囲に存するよ
うに位置させている。
Next, FIGS. 5 (a) and 5 (b) show a second embodiment of the present invention. The difference between the second embodiment and the first embodiment is as follows. That is, in the first embodiment, the permanent magnet 6 is positioned so as to correspond vertically to the ferromagnetic magnetoresistive elements 2a and 2b, but in the second embodiment, the permanent magnet 6 is arranged.
The radius of is slightly larger than the radius of the ferromagnetic magnetoresistive element 2a,
The permanent magnet 6 is positioned so as to exist around the outer periphery of the ferromagnetic magnetoresistive element 2a.

このように構成しても第1実施例と同様の効果が得られ
る。
Even with this structure, the same effect as that of the first embodiment can be obtained.

なお、この第2実施例では第1実施例と同一部分には同
一符号を付して異なる部分のみ説明した。
In the second embodiment, the same parts as those in the first embodiment are designated by the same reference numerals and only different parts are described.

第6図(a)、(b)はこの発明の第3実施例を示す。
とりわけ第6図(a)は同図(b)のVI-VI線の断面図
を示している。この第3実施例では、第1実施例におけ
る永久磁石6の幅寸法を大きくなるように設定してい
る。
6 (a) and 6 (b) show a third embodiment of the present invention.
In particular, FIG. 6 (a) shows a sectional view taken along line VI-VI of FIG. 6 (b). In the third embodiment, the width dimension of the permanent magnet 6 in the first embodiment is set to be large.

このように構成すると、永久磁石6に対する磁気漏洩防
止効果が高まる。この場合、強磁性磁気抵抗素子2aを他
方の強磁性磁気抵抗素子2bよりも径寸法的に多少大きく
なるように設定している。
With this configuration, the magnetic leakage prevention effect on the permanent magnet 6 is enhanced. In this case, the ferromagnetic magnetoresistive element 2a is set to be slightly larger in diameter than the other ferromagnetic magnetoresistive element 2b.

第7図(a)、(b)はこの発明の第4実施例を示す。
この第4実施例では第3実施例における永久磁石6の径
寸法を多少大きく設定し、永久磁石6が強磁性磁気抵抗
素子2a、2bの外周囲に位置するようにしている。
7 (a) and 7 (b) show a fourth embodiment of the present invention.
In the fourth embodiment, the diameter of the permanent magnet 6 in the third embodiment is set to be slightly larger so that the permanent magnet 6 is located on the outer periphery of the ferromagnetic magnetoresistive elements 2a and 2b.

つぎに、第8図(a)、(b)はこの発明の第5実施例
を示す。この第5実施例では第4実施例における磁気漏
洩防止部12に凹部を形成し、この磁気漏洩防止部12の凹
部を永久磁石6の両端部に嵌合している。このように構
成しても上記各実施例と同様の効果が得られる。
Next, FIGS. 8 (a) and 8 (b) show a fifth embodiment of the present invention. In the fifth embodiment, a recess is formed in the magnetic leakage prevention unit 12 of the fourth embodiment, and the recess of the magnetic leakage prevention unit 12 is fitted to both ends of the permanent magnet 6. Even with this structure, the same effect as that of each of the above-described embodiments can be obtained.

なお、上記実施例では強磁性磁気抵抗素子2a、2bの形状
は円形または多角形であったが、形状はこれのみに限定
されず、例えば短冊状であってもよい。
Although the ferromagnetic magnetoresistive elements 2a and 2b have a circular or polygonal shape in the above embodiment, the shape is not limited to this and may be, for example, a strip shape.

また、上記実施例では磁気漏洩防止部12の材料として
は、鉄系の材料を用いたが、この材料のみに限定され
ず、要は例えばフエライトなどの磁性材料であればよ
い。また、界磁発生手段を強磁性磁気抵抗素子とともに
直線状に形成して直線変位を取り出すように構成しても
よい。また、ロータが回転および直線移動を弊有するよ
うに構成し、回転および直線移動を取り出すように構成
してもよい。あるいは、このばあい、ロータの回転変位
と直線移動変位とを同時に取り出すように構成してもよ
い。
Further, although the iron-based material is used as the material of the magnetic leakage prevention unit 12 in the above-mentioned embodiment, the material is not limited to this material, and the point is that a magnetic material such as ferrite may be used. Further, the field generating means may be linearly formed together with the ferromagnetic magnetoresistive element so as to take out the linear displacement. Further, the rotor may be configured to have a negative effect on rotation and linear movement, and may be configured to take out rotation and linear movement. Alternatively, in this case, the rotational displacement and the linear displacement of the rotor may be simultaneously extracted.

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

第1図はこの発明のポテンショメータの一実施例であ
り、同図(a)にその上面図、同図(b)にA−A線の
断面図を示す。第2図は縦断面図、第3図は第1図にお
ける実施例の出力特性を示すグラフ、第4図は強磁性磁
気抵抗素子の特性を示すグラフ、第5図(a)、(b)
はこの発明の第2実施例を示す上面図および断面図、第
6図(a)、(b)はこの発明の第3実施例を示す上面
図および断面図、第7図(a)、(b)はこの発明の第
4実施例を示す上面図および断面図、第8図(a)、
(b)はこの発明の第5実施例を示す上面図および断面
図である。 図中、1……絶縁基板(回路基板)、2a、2b……強磁性
磁気抵抗素子、6……永久磁石(磁界発生手段)、7…
…ハウジング、8……ロータ、9……回転軸、10……軸
受、12……磁気漏洩防止部
FIG. 1 shows an embodiment of the potentiometer of the present invention. FIG. 1 (a) is a top view thereof and FIG. 1 (b) is a sectional view taken along line AA. 2 is a longitudinal sectional view, FIG. 3 is a graph showing output characteristics of the embodiment shown in FIG. 1, FIG. 4 is a graph showing characteristics of a ferromagnetic magnetoresistive element, and FIGS. 5 (a) and 5 (b).
Shows a top view and a sectional view showing a second embodiment of the present invention, FIGS. 6 (a) and 6 (b) show a top view and a sectional view showing a third embodiment of the present invention, FIG. 7 (a), b) is a top view and a sectional view showing a fourth embodiment of the present invention, FIG. 8 (a),
(B) is a top view and a sectional view showing a fifth embodiment of the present invention. In the figure, 1 ... Insulating substrate (circuit board), 2a, 2b ... Ferromagnetic magnetoresistive element, 6 ... Permanent magnet (magnetic field generating means), 7 ...
… Housing, 8 …… Rotor, 9 …… Rotary shaft, 10 …… Bearing, 12 …… Magnetic leakage prevention section

───────────────────────────────────────────────────── フロントページの続き (72)発明者 青 建一 愛知県刈谷市昭和町1丁目1番地 日本電 装株式会社内 (72)発明者 荒砂 俊和 愛知県刈谷市昭和町1丁目1番地 日本電 装株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Kenichi Ao 1-1, Showa-cho, Kariya city, Aichi prefecture Nihon Denso Co., Ltd. (72) Inventor Toshikazu Arasa 1-1-chome, Showa town, Kariya city, Aichi prefecture Sozo Co., Ltd.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】ハウジングと、 このハウジング内に回転可能に設けられたロータと、 このロータに同心的で該ロータから所定の間隔を隔てる
ようにして配設され、全体的に環状を成す一対の強磁性
磁気抵抗素子を有する絶縁基板と、 前記ロータ側に前記強磁性磁気抵抗素子の一部分に近接
して装着されて前記ロータと共に回転すると共に、前記
ロータの同心円の径方向の面で両端部を区切られて前記
ロータと同心の円弧状に形成され、前記一部分に前記ロ
ータの径方向に磁界を印加する磁界発生手段と、 前記径方向の面に取付けられ前記磁界発生手段の磁界が
前記径方向の面から漏洩するのを防ぐ磁性材料製の磁気
漏洩防止部材と を備える非接触式ポテンショメータ。
1. A housing, a rotor rotatably provided in the housing, and a pair of concentric rotors arranged at a predetermined distance from the rotor and having a generally annular shape. An insulating substrate having a ferromagnetic magnetoresistive element, mounted on the rotor side in proximity to a part of the ferromagnetic magnetoresistive element to rotate together with the rotor, and to have both end portions on a radial surface of a concentric circle of the rotor. A magnetic field generating means that is partitioned and formed in an arc shape concentric with the rotor and applies a magnetic field in the radial direction of the rotor to the part, and a magnetic field of the magnetic field generating means that is attached to the radial surface is in the radial direction. A non-contact potentiometer equipped with a magnetic leakage prevention member made of a magnetic material that prevents leakage from the surface of the.
【請求項2】前記磁気漏洩防止部材は前記磁界発生手段
における両端部の外周部を嵌合する状態に設けられてい
ることを特徴とする特許請求の範囲第1項に記載の非接
触式ポテンショメータ。
2. The non-contact potentiometer according to claim 1, wherein the magnetic leakage prevention member is provided in such a manner that the outer peripheral portions of both end portions of the magnetic field generating means are fitted to each other. .
【請求項3】前記磁気漏洩防止部材は鉄系金属材料から
成っていることを特徴とする特許請求の範囲第1項また
は第2項に記載の非接触式ポテンショメータ。
3. The non-contact potentiometer according to claim 1 or 2, wherein the magnetic leakage prevention member is made of an iron-based metal material.
JP61198776A 1986-07-29 1986-08-25 Non-contact type potentiometer Expired - Fee Related JPH0777166B2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP61198776A JPH0777166B2 (en) 1986-08-25 1986-08-25 Non-contact type potentiometer
EP87110695A EP0255052B1 (en) 1986-07-29 1987-07-23 Noncontact potentiometer
DE3788831T DE3788831T2 (en) 1986-07-29 1987-07-23 Contactless potentiometer.
US07/076,891 US4835509A (en) 1986-07-29 1987-07-23 Noncontact potentiometer
KR1019870008259A KR900007100B1 (en) 1986-07-29 1987-07-29 Solid-state potentiometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61198776A JPH0777166B2 (en) 1986-08-25 1986-08-25 Non-contact type potentiometer

Publications (2)

Publication Number Publication Date
JPS6354783A JPS6354783A (en) 1988-03-09
JPH0777166B2 true JPH0777166B2 (en) 1995-08-16

Family

ID=16396734

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61198776A Expired - Fee Related JPH0777166B2 (en) 1986-07-29 1986-08-25 Non-contact type potentiometer

Country Status (1)

Country Link
JP (1) JPH0777166B2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5821126Y2 (en) * 1976-08-06 1983-05-04 電気音響株式会社 potentiometer

Also Published As

Publication number Publication date
JPS6354783A (en) 1988-03-09

Similar Documents

Publication Publication Date Title
US6124709A (en) Magnetic position sensor having a variable width magnet mounted into a rotating disk and a hall effect sensor
US7021160B2 (en) Apparatus for sensing position and/or torque
US4835509A (en) Noncontact potentiometer
US7378842B2 (en) Through the hole rotary position sensor with non-symmetric pole pieces
US3112464A (en) Figure
US5164668A (en) Angular position sensor with decreased sensitivity to shaft position variability
US7639004B2 (en) Apparatus for sensing angular displacement between first and second rotating shafts including flux collectors
JPH04212066A (en) Rotary speed sensor
EP1679491A1 (en) Rotation angle detection device
JPH11211410A (en) Non-contact type position sensor
US6084401A (en) Rotational position sensor employing magneto resistors
US7210360B2 (en) Apparatus for sensing position and/or torque
JPH0777166B2 (en) Non-contact type potentiometer
US5574361A (en) Switched reluctance angular velocity sensor
JPH077725B2 (en) Non-contact type potentiometer
JPS63184376A (en) Magnetic noncontact potentiometer
JP2001141412A (en) Non-contact type rotating angle sensor and sensor core
JP2002031505A (en) Non-contact rotation angle sensor and its sensor core
JP4373157B2 (en) Angle detector
JPS6354782A (en) Noncontact type potentiometer
JPH0396287A (en) Noncontact position sensor
JPH0777165B2 (en) Non-contact type potentiometer
JP3082056B2 (en) Rotary encoder
JPS63184375A (en) Potentiometer
JPH0777164B2 (en) Non-contact type potentiometer

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees