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JPH0777165B2 - Non-contact type potentiometer - Google Patents
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JPH0777165B2 - Non-contact type potentiometer - Google Patents

Non-contact type potentiometer

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Publication number
JPH0777165B2
JPH0777165B2 JP61198774A JP19877486A JPH0777165B2 JP H0777165 B2 JPH0777165 B2 JP H0777165B2 JP 61198774 A JP61198774 A JP 61198774A JP 19877486 A JP19877486 A JP 19877486A JP H0777165 B2 JPH0777165 B2 JP H0777165B2
Authority
JP
Japan
Prior art keywords
magnetic field
magnetoresistive element
generating means
field generating
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
JP61198774A
Other languages
Japanese (ja)
Other versions
JPS6354781A (en
Inventor
好 吉野
建一 青
俊和 荒砂
勝彦 有賀
利和 松下
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 JP61198774A priority Critical patent/JPH0777165B2/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 JPS6354781A publication Critical patent/JPS6354781A/en
Publication of JPH0777165B2 publication Critical patent/JPH0777165B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • 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、ロータを回転させる非接触式ポテンショメ
ータに関し、特には磁界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 for rotating a rotor, and particularly to a non-contact potentiometer using a ferromagnetic magnetoresistive element whose resistance value is reduced by a magnetic field. .

[従来の技術] 非接触式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InSb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、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] A 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 magnetoresistive element is provided in a gap formed at the tip of the rotating magnetic body. InSb is arranged to generate an output according to the rotation of the rotating magnetic body.In other words, by changing the size of the gap formed at the tip of the rotating magnetic body, in other words, the tip of the rotating magnetic body. Is processed by a predetermined function to obtain a predetermined function output from the InSb magnetoresistive element as described above.

[発明が解決しようとする問題点] この場合、先に提案した特願昭61-72201のように磁界発
生手段としての永久磁石は磁極が径方向に指向するよう
に着磁することが考えられるが、このように円弧形状の
永久磁石に着磁することは容易ではなく着磁させにくい
という問題がある。
[Problems to be Solved by the Invention] In this case, it is considered that the permanent magnet as the magnetic field generating means is magnetized so that the magnetic poles are oriented in the radial direction as in the previously proposed Japanese Patent Application No. 61-72201. However, it is not easy to magnetize the arc-shaped permanent magnet in this way, and it is difficult to magnetize it.

この発明はこの問題点をなくすべく行なわれたもので、
磁界発生手段が弧状などの非直線状を成すどのような形
状の場合でも、前述の径方向と直交する方向に着磁すれ
ば済むようになるので着磁を容易に行うことができると
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.
Even if the magnetic field generating means has any shape such as an arc shape or a non-linear shape, it suffices to magnetize in a direction orthogonal to the above-mentioned radial direction, which is excellent in that it can be easily magnetized. An object is to provide a non-contact potentiometer having an effect.

[問題点を解決するための手段] この発明は、ハウジングと、ハウジング内に回転可能に
設けられた可動部と、この可動部に同心的で該可動部か
ら所定の間隔を隔てるようにして配設され、全体的に環
状となる一対の強磁性磁気抵抗素子を有する平面状の絶
縁基板と、前記可動部側に、磁極が前記可動部の回転軸
方向に指向するとともに、前記強磁性磁気抵抗素子の一
方の側面に位置する前記絶縁基板の1部と相対向するよ
うに装着された磁界発生手段とを備え、該磁界発生手段
からの磁束が環状の前記強磁性磁気抵抗素子の径方向に
指向して閉磁路を形成するようにしたことを特徴とする
構成を採用しているものである。
[Means for Solving the Problems] According to the present invention, a housing, a movable portion rotatably provided in the housing, and a movable portion arranged concentrically with the movable portion with a predetermined distance from the movable portion. A planar insulating substrate having a pair of ferromagnetic magnetoresistive elements that are provided in an annular shape as a whole, and a magnetic pole on the movable portion side that is directed in the rotation axis direction of the movable portion, and the ferromagnetic magnetoresistive element. Magnetic field generating means mounted so as to face a part of the insulating substrate located on one side surface of the element, and the magnetic flux from the magnetic field generating means is directed in the radial direction of the annular ferromagnetic magnetoresistive element. The configuration employs a feature that a closed magnetic circuit is formed by directing.

[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
が1例として弧状を成す場合でも、これの着磁方向は径
方向ではなく径方向に直角する方向つまり絶縁基板の平
面と直角する方向ですむようになり、磁界発生手段の着
磁が容易となる。
[Operation] According to the present invention configured as described above, even when the magnetic field generating means has an arc shape as an example, the magnetization direction of the magnetic field generating means is not the radial direction but the direction perpendicular to the radial direction, that is, the plane of the insulating substrate. Since it is only necessary to make a perpendicular direction, it becomes easy to magnetize the magnetic field generating means.

[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
が弧状あるいは角状とは関係なくいかなる形状でもとい
った非直線状を成す場合でも、これの着磁方向はロータ
の軸心方向で済むようになり、磁界発生手段の着磁が容
易とな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。また、磁界発生手段
の形状が任意であるので、自由に特性を設定できる。
[Effects of the Invention] According to the present invention configured as described above, even if the magnetic field generating means has a non-linear shape such as any shape regardless of the arc shape or the angular shape, the magnetization direction of the magnetic field generation means is the axis of the rotor. It is possible to provide a non-contact potentiometer which has an excellent effect that the magnetic field generating means can be easily magnetized because the magnetic field generating means can be easily magnetized. Further, since the shape of the magnetic field generating means is arbitrary, the characteristics can be set freely.

[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。ま
ず、第1図(a)、(b)は本発明の第1実施例を示
す。この第1図において、絶縁基板1上に開口部を持つ
円形または多角形の形状Ni-Fe、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、両端子部、およ
び中点部に電極3、4、5を形成する。(いわゆるハー
フブリッジ形成)。かかる強磁性磁気抵抗素子2a、2bの
電極端子3を接地GND、電極端子4を電源端子Vccとし中
点部5から出力Voutを導出する。そして、強磁性磁気抵
抗素子2a、2bのプリントパターンの中心に上蓋9aのボー
ルベアリングから成る軸受8が設けられている。軸受8
には非磁性体材料から形成され上下方向に指向する回転
軸6が可動部として軸まわりに回転可能に枢支されてい
る。この回転軸6の片側には、磁性材製の板状の取付部
材9を介して半円弧状の永久磁石7が磁界発生手段とし
て取り付けられている。この永久磁石7は回転軸6の軸
方向に沿って、すなわち永久磁石7の径方向とは直交す
る方向に着磁されている。そして、この永久磁石7は一
方の強磁性磁気抵抗素子2aに対しこれの外周の側面で上
下方向に対面状態に位置するように配置されている。な
お10はハウジング、11はワイヤーハーネスである。
Embodiments Embodiments of the present invention will be described below with reference to the drawings. First, FIGS. 1A and 1B show a first embodiment of the present invention. In FIG. 1, ferromagnetic magnetoresistive elements 2a and 2b made of thin films of circular or polygonal shape Ni-Fe, Ni-Co or the like having an opening portion are formed on an insulating substrate 1, and both terminal portions, and The electrodes 3, 4, and 5 are formed at the midpoints. (So-called half bridge formation). The output terminal Vout is derived from the midpoint 5 with the electrode terminal 3 of the ferromagnetic magnetoresistive elements 2a and 2b as the ground GND and the electrode terminal 4 as the power supply terminal Vcc. A bearing 8 formed of a ball bearing on the upper lid 9a is provided at the center of the printed pattern of the ferromagnetic magnetoresistive elements 2a and 2b. Bearing 8
A rotary shaft 6 made of a non-magnetic material and vertically oriented is rotatably supported around the shaft as a movable portion. A semi-circular arc-shaped permanent magnet 7 is attached as magnetic field generating means to one side of the rotary shaft 6 via a plate-shaped attachment member 9 made of a magnetic material. The permanent magnet 7 is magnetized along the axial direction of the rotary shaft 6, that is, in the direction orthogonal to the radial direction of the permanent magnet 7. The permanent magnet 7 is arranged so as to face the one ferromagnetic magnetoresistive element 2a in the vertical direction on the side surface of the outer circumference thereof. In addition, 10 is a housing and 11 is a wire harness.

さて、強磁性磁気抵抗素子2a、2bにおいては下記の事実
が理論上、知られている。すなわち、強磁性磁気抵抗素
子は電流の流れる方向に対して直角方向から磁界を受け
ると、その部分の抵抗値が減少する特性を有しており、
また、飽和磁界以上の磁界を受けたときには、抵抗値の
減少は一定となり、半導体式磁気抵抗素子やホール素子
と相違して安定な出力が得られる特徴を有している。
The following facts are theoretically known in the ferromagnetic magnetoresistive elements 2a and 2b. That is, a ferromagnetic magnetoresistive element has a characteristic that when a magnetic field is applied from a direction perpendicular to the direction of current flow, the resistance value of that portion decreases.
Further, when receiving a magnetic field equal to or higher than the saturation magnetic field, the decrease in the resistance value becomes constant, and unlike the semiconductor type magnetoresistive element and the Hall element, it has a characteristic that a stable output can be obtained.

つぎに、永久磁石7に直接対面する強磁性磁気抵抗素子
2aには第1図(b)に矢印Hで示すように、回転軸6の
軸方向に沿う上下方向に磁界が印加されており、この磁
界は強磁性磁気抵抗素子2aに第1図(b)に矢印iで示
すように径方向に作用し、その抵抗値が減少する。回転
軸6の回転に伴い強磁性磁気抵抗素子2aの抵抗値は第2
図に示すように連続的に変化し、ポテンショメータの出
力は略直線状態になる。この第2図の場合、縦軸に出力
(Vcc)を現わし、横軸に回転軸6の回転角度(度)を
示している。
Next, a ferromagnetic magnetoresistive element that directly faces the permanent magnet 7.
As shown by an arrow H in FIG. 1 (b), a magnetic field is applied to 2a in the vertical direction along the axial direction of the rotary shaft 6, and this magnetic field is applied to the ferromagnetic magnetoresistive element 2a as shown in FIG. ) Acts in the radial direction as indicated by the arrow i, and its resistance value decreases. With the rotation of the rotating shaft 6, the resistance value of the ferromagnetic magnetoresistive element 2a becomes the second value.
As shown in the figure, it changes continuously and the output of the potentiometer becomes almost linear. In the case of FIG. 2, the vertical axis represents the output (Vcc) and the horizontal axis represents the rotation angle (degree) of the rotary shaft 6.

このように、永久磁石7を半円弧状に形成しながらも、
永久磁石7の着磁方向は径方向ではなく、この径方向と
は直交する方向で済むので、着磁が容易になり、ひいて
は磁界発生手段の製作が容易になりコスト的にも有利と
なる。
In this way, while forming the permanent magnet 7 in a semi-circular shape,
Since the magnetizing direction of the permanent magnet 7 is not the radial direction but the direction orthogonal to the radial direction, the magnetizing is facilitated, and the magnetic field generating means is easily manufactured, which is advantageous in cost.

また、半導体磁気抵抗素子やホール素子を用いたときに
は、磁界強度がばらつくと特性に大きく影響してくる
が、この実施例に示すように強磁性磁気抵抗素子を用い
たときには、飽和磁界以上の磁界をあらかじめ印加して
おけば、実施例上ではポテンショメータの安定した出力
が得られる。
Further, when a semiconductor magnetoresistive element or a Hall element is used, variations in magnetic field strength greatly affect the characteristics, but when a ferromagnetic magnetoresistive element is used as shown in this embodiment, a magnetic field above the saturation magnetic field is used. If is applied in advance, a stable output of the potentiometer can be obtained in the embodiment.

つぎに、この発明の第2実施例を第4図(a)、(b)
を参照して説明する。この第2実施例が第1実施例と相
違するところは第2実施例では、取付部材9を回転軸6
の下端部に直接取り付け、強磁性磁気抵抗素子の中心に
円形の集磁部材15を取り付けたことである。回転軸6の
下端には、磁性材料により形成された取付部材9の一端
が取り付けられ、取付部材9の他端には永久磁石7が接
着剤などにより取り付けられている。そして、永久磁石
7が強磁性磁気抵抗素子の外周面に位置している。
Next, a second embodiment of the present invention will be described with reference to FIGS. 4 (a) and 4 (b).
Will be described with reference to. The second embodiment is different from the first embodiment in that the mounting member 9 is attached to the rotary shaft 6 in the second embodiment.
That is, the circular magnetism collecting member 15 is attached directly to the lower end of the, and the circular magnetism collecting member 15 is attached to the center of the ferromagnetic magnetoresistance element. One end of an attachment member 9 made of a magnetic material is attached to the lower end of the rotary shaft 6, and a permanent magnet 7 is attached to the other end of the attachment member 9 with an adhesive or the like. The permanent magnet 7 is located on the outer peripheral surface of the ferromagnetic magnetoresistive element.

第5図(a)、(b)はこの発明の第3実施例を示す。5 (a) and 5 (b) show a third embodiment of the present invention.

この第3実施例では、回転軸6の下端にロータ12を取り
付け、このロータ12の下面に断面コの字状を成す磁性材
製の集磁部材13を取着している。そして、集磁部材13の
一端を強磁性磁気抵抗素子2a、2bの中心部に位置させ、
他端部は強磁性磁気抵抗素子2aの外周囲に位置して永久
磁石7を取着している。このように構成してもよい。
In the third embodiment, the rotor 12 is attached to the lower end of the rotary shaft 6, and the magnetic flux collecting member 13 made of a magnetic material and having a U-shaped cross section is attached to the lower surface of the rotor 12. Then, one end of the magnetism collecting member 13 is positioned at the center of the ferromagnetic magnetoresistive elements 2a and 2b,
The other end is located on the outer periphery of the ferromagnetic magnetoresistive element 2a and has a permanent magnet 7 attached thereto. You may comprise in this way.

第6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2実施例の状態で回転軸6の下
端に永久磁石14を接着剤などにより取り付けている。こ
の永久磁石14は永久磁石7と磁極の指向方向は同じであ
り、互いに異極となる関係に設定しているものである。
このように構成すると、永久磁石7と永久磁石14との間
には第6図(b)にiで示すように閉路が生じるが、こ
のとき強磁性磁気抵抗素子2aを通過する磁束が増加する
ため第7図に示すような特性が得られる。この第7図に
おいて、縦軸に出力(Vout)、横軸に回転角度(度)を
取っている。これによれば、第1実施例に比較して立上
りが大となり、大きな出力が得られることが理解され
る。
6 (a) and 6 (b) show a fourth embodiment of the present invention.
In the fourth embodiment, in the state of the second embodiment, the permanent magnet 14 is attached to the lower end of the rotary shaft 6 with an adhesive or the like. The permanent magnet 14 and the permanent magnet 7 have the same direction of the magnetic poles and are set to have different polarities.
With this structure, a closed circuit is generated between the permanent magnet 7 and the permanent magnet 14 as indicated by i in FIG. 6B, but at this time, the magnetic flux passing through the ferromagnetic magnetoresistive element 2a increases. Therefore, the characteristics shown in FIG. 7 are obtained. In FIG. 7, the vertical axis represents output (Vout) and the horizontal axis represents rotation angle (degrees). According to this, it is understood that the rising is large and a large output is obtained as compared with the first embodiment.

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、強磁性磁気抵抗素子を直線状に形成した場合に
は、磁界発生手段も直線状に形成して、直線変位を取り
出すように構成してもよい。また、ロータが直線移動と
回転変位とを併有するように構成してもよい。
When the ferromagnetic magnetoresistive element is formed in a linear shape, the magnetic field generating means may also be formed in a linear shape so as to extract the linear displacement. Further, the rotor may have both linear movement and rotational displacement.

さらには、上記各実施例では、永久磁石を強磁性磁気抵
抗素子に対して回転変位させるように構成したが、これ
とは逆に、強磁性磁気抵抗素子を永久磁石に対して変位
させることもできるが、このように構成すると、外部に
導出する端子を電気伝導可能に摺動させる構成が必要に
なり、全体の構造が複雑化する不利益があるものであ
る。このためにこの実施例では上記の構成を採用するに
は至らなかった。
Furthermore, in each of the above-described embodiments, the permanent magnet is configured to be rotationally displaced with respect to the ferromagnetic magnetoresistive element, but conversely, the ferromagnetic magnetoresistive element may be displaced with respect to the permanent magnet. However, such a structure requires a structure in which a terminal led out to the outside is slidable so as to be electrically conductive, which is a disadvantage that the entire structure is complicated. For this reason, in this embodiment, the above configuration was not adopted.

その他、具体的な実施にあたっては、発明の要旨を逸脱
しない範囲で種々変更できる。
In addition, in concrete implementation, various modifications can be made without departing from the gist of the invention.

【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図は回転角度と出力との関係を示す
出力特性グラフ、第3図は強磁磁気抵抗素子の特性を示
すグラフ、第4図(a)、(b)は第2実施例の上面図
及び断面図、第5図(a)、(b)は第3実施例の上面
図及び断面図、第6図(a)、(b)はこの発明の第4
実施例を示す上面図及び断面図、第7図はこの発明の第
4実施例を示す特性を示すグラフである。 図中、1……絶縁基板(回路基板)、2a、2b……強磁性
磁気抵抗素子、3……永久磁石(磁界発生手段)、6…
…回転軸(可動部)、10……ハウジング
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. FIG. 2 is an output characteristic graph showing the relationship between the rotation angle and the output, FIG. 3 is a graph showing the characteristic of the strong magnetic magnetoresistive element, and FIGS. 4 (a) and 4 (b) are top views of the second embodiment. And a sectional view, FIGS. 5 (a) and 5 (b) are a top view and a sectional view of the third embodiment, and FIGS. 6 (a) and 6 (b) are a fourth embodiment of the present invention.
FIG. 7 is a top view and a sectional view showing an embodiment, and FIG. 7 is a graph showing characteristics showing a fourth embodiment of the present invention. In the figure, 1 ... Insulating substrate (circuit board), 2a, 2b ... Ferromagnetic magnetoresistive element, 3 ... Permanent magnet (magnetic field generating means), 6 ...
… Rotary shaft (movable part), 10 …… Housing

───────────────────────────────────────────────────── フロントページの続き (72)発明者 有賀 勝彦 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 松下 利和 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 Katsuhiko Ariga 1-1, Showa-cho, Kariya, Aichi Nihon Denso Co., Ltd. (72) Inventor Toshikazu Matsushita 1-1, Showa-cho, Kariya, Aichi Nihon Denso Within the corporation

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可動部と、 この可動部に同心的で該可動部から所定の間隔を隔てる
ようにして配設され、全体的に環状となる一対の強磁性
磁気抵抗素子を有する平面状の絶縁基板と、 前記可動部側に、磁極が前記可動部の回転軸方向に指向
するとともに、前記強磁性磁気抵抗素子の一方の側面に
位置する前記絶縁基板の1部と相対向するように装着さ
れた磁界発生手段とを備え、 該磁界発生手段からの磁束が環状の前記強磁性磁気抵抗
素子の径方向に指向して閉磁路を形成するようにしたこ
とを特徴とする非接触式ポテンショメータ。
1. A housing, a movable part rotatably provided in the housing, a concentric part provided to the movable part at a predetermined distance from the movable part, and an annular shape as a whole. A planar insulating substrate having a pair of ferromagnetic magnetoresistive elements, the magnetic pole being directed to the movable portion side in the rotation axis direction of the movable portion and being located on one side surface of the ferromagnetic magnetoresistive element A part of the insulating substrate, and a magnetic field generating means mounted so as to face each other, and a magnetic flux from the magnetic field generating means is directed in a radial direction of the annular ferromagnetic magnetoresistive element to form a closed magnetic path. A non-contact type potentiometer characterized in that
【請求項2】前記磁界発生手段は、前記強磁性磁気抵抗
素子の内側または外側の近傍に配され、前記可動部には
前記磁界発生手段に対する集磁を行なう磁性材料製の集
磁部材が、前記強磁性磁気抵抗素子を前記磁界発生手段
と共に前記強磁性磁気抵抗素子の径方向に挟む位置に設
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 magnetic field generating means is arranged in the vicinity of the inside or outside of the ferromagnetic magnetoresistive element, and the movable part is provided with a magnetic collecting member made of a magnetic material for collecting the magnetic field generating means. 2. The non-contact potentiometer according to claim 1, wherein the ferromagnetic magnetoresistive element is provided at a position sandwiching the ferromagnetic magnetoresistive element in the radial direction of the ferromagnetic magnetoresistive element together with the magnetic field generating means.
【請求項3】前記磁界発生手段は永久磁石から成ってい
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 field generating means comprises a permanent magnet.
JP61198774A 1986-07-29 1986-08-25 Non-contact type potentiometer Expired - Fee Related JPH0777165B2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP61198774A JPH0777165B2 (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
JP61198774A JPH0777165B2 (en) 1986-08-25 1986-08-25 Non-contact type potentiometer

Publications (2)

Publication Number Publication Date
JPS6354781A JPS6354781A (en) 1988-03-09
JPH0777165B2 true JPH0777165B2 (en) 1995-08-16

Family

ID=16396702

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61198774A Expired - Fee Related JPH0777165B2 (en) 1986-07-29 1986-08-25 Non-contact type potentiometer

Country Status (1)

Country Link
JP (1) JPH0777165B2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6032997B2 (en) * 1977-07-06 1985-07-31 電気音響株式会社 polyphase potentiometer

Also Published As

Publication number Publication date
JPS6354781A (en) 1988-03-09

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