JPS6354784A - Noncontact type potentiometer - Google Patents

Noncontact type potentiometer

Info

Publication number
JPS6354784A
JPS6354784A JP61198777A JP19877786A JPS6354784A JP S6354784 A JPS6354784 A JP S6354784A JP 61198777 A JP61198777 A JP 61198777A JP 19877786 A JP19877786 A JP 19877786A JP S6354784 A JPS6354784 A JP S6354784A
Authority
JP
Japan
Prior art keywords
magnetic field
field generating
generating means
rotor
magnetic
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.)
Granted
Application number
JP61198777A
Other languages
Japanese (ja)
Other versions
JPH077725B2 (en
Inventor
Toshikazu Matsushita
松下 利和
Katsuhiko Ariga
勝彦 有賀
Yoshi Yoshino
吉野 好
Kenichi Ao
建一 青
Toshikazu Arasuna
荒砂 俊和
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.)
Denso Corp
Original Assignee
NipponDenso 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 NipponDenso Co Ltd filed Critical NipponDenso Co Ltd
Priority to JP61198777A priority Critical patent/JPH077725B2/en
Priority to EP87110695A priority patent/EP0255052B1/en
Priority to US07/076,891 priority patent/US4835509A/en
Priority to DE3788831T priority patent/DE3788831T2/en
Priority to KR1019870008259A priority patent/KR900007100B1/en
Publication of JPS6354784A publication Critical patent/JPS6354784A/en
Publication of JPH077725B2 publication Critical patent/JPH077725B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To easily magnetize magnetic field generating means by forming the magnetic field generating means of a flexible magnetic material, and magnetizing the means in a linear state immediately before the means is bent in a predetermined shape. CONSTITUTION:A rotatable rotor 8 provided in a housing 10, and an insulating substrate 1 having ferromagnetic magnetic resistance elements 2a, 2b of predetermined shape disposed at a predetermined interval from the rotor 8 concentrically with the rotor 8 are provided. Further, magnetic field generating means 6 so mounted as to form a closed magnetic path with the elements 2a, 2b at the rotor 8 side. The means 6 is formed of a flexible magnetic material, and magnetized in a linear state before the means 6 is bent in a predetermined shape. The means 6 is, for example, composed of a material in which magnetic material powder is dispersed in the plastic of the flexible material, disposed concentrically with the elements 2a, 2b, and escapes 6a, 6b directed externally are provided at both ends.

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、特には磁気力により抵抗値が減少する強【
a性(む気抵抗A!−を用いた非接触式ポテンショメー
タに関するものである。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a non-contact potentiometer that rotates a rotor, and particularly to a potentiometer that reduces resistance by magnetic force.
This relates to a non-contact potentiometer using a resistance (A!-).

[従来の技((i] 非接触ポテンショメータの磁気回路は、従来より右底円
筒状二]アや回転磁刊体および永久隘石ととbに、閉(
(主路として構成され、回転(、n性体の先端部分に形
成した間隙に磁気抵抗水子であるIn3n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い
る。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さすれば回転1硅性体の先
端を所定の形状に加工することにより前述したような1
nsbfiの磁気抵抗素子から所定の関数出力を19で
いる。
[Conventional Technique (i) The magnetic circuit of a non-contact potentiometer has conventionally been formed into a right-bottom cylindrical shape 2] A, a rotating magnetic body, a permanent stone, and a closed (B).
In3n, which is a magnetoresistive water element, is arranged in a gap formed at the tip of the rotating magnetic body to generate an output corresponding to the rotation of the rotating magnetic body. However, by changing the size of the gap formed at the tip of the rotating magnetic body, it is possible to change the size of the gap formed at the tip of the rotating magnetic body by processing the tip of the rotating magnetic body into a predetermined shape.
The predetermined function output from the nsbfi magnetoresistive element is 19.

[発明が解決しようとする問題点1 この場合に、特願昭61−72201号に開示した如く
、永久磁石は半円弧状に曲成されていることから、これ
の径方向に着磁するとき、この方向に6磁しにくいとい
う問題がある。
[Problem to be solved by the invention 1 In this case, as disclosed in Japanese Patent Application No. 72201/1980, since the permanent magnet is curved in a semicircular arc shape, when magnetized in the radial direction of the permanent magnet, , there is a problem that 6 magnetization is difficult in this direction.

この発明は上記の事情に鑑みてなされたもので、磁界発
生手段を可撓竹材材料により形成することにより、あら
かじめ直線状態にて着Ill することができ、かかる
着磁がきわめて容易に行なわれるといった優れた効果を
有する非接触式ボアンシ]メータを提供することを目的
とする。
This invention was made in view of the above circumstances, and by forming the magnetic field generating means from a flexible bamboo material, magnetization can be performed in advance in a straight line state, and such magnetization can be performed extremely easily. The purpose of the present invention is to provide a non-contact bouncy meter with excellent effects.

[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〔1−夕と、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1・n性tn気抵抗M’rを右する絶縁桔根と
、11h記ローク側に^り記強…慴磁気抵抗累rとで閉
)n路を形成するように装着されたLn磁界発生手段を
備え、前記磁界発牛手[グを可撓性(n竹材TNlによ
り形成し、該1.fi ’i’i1発生手段を所定の形
状に曲成する前の直線状態で着磁したことを特徴とする
構成を採用している。
[Means for Solving the Problems] The present invention includes a housing, a rotor rotatably provided within the housing, and a rotor that is concentric with the rotor and spaced from the rotor by a predetermined distance. A closed (closed) n path is formed by the insulating tube which holds the strong 1-n magnetic resistance M'r of a predetermined shape and the 11h magnetic resistance resistor R on the low side. The Ln magnetic field generating means is mounted as shown in FIG. The structure is characterized by magnetization in a straight line state.

し作用1 上記のように構成したこの発明によれば、磁界発作手段
を可撓竹材材料により形成1〕たことにより、(n界発
生手段を所定の形状に曲成する以前の直線状態にて厚さ
方向に着…することができるようになり、大型の着L1
) +;31により強力な磁界を印加でき、6ってその
看…を行ない易くなる。
Effect 1 According to the present invention configured as described above, by forming the magnetic field generation means from a flexible bamboo material (1), it is possible to You can now wear it in the thickness direction, making it possible to wear large clothes L1.
) +; 31 allows a stronger magnetic field to be applied, and 6 makes it easier to monitor.

[発明の効果1 上記のように構成したこの発明によれば、磁界発生手段
を可撓竹材材料により形成1)だことにより、(4磁界
発生手段を非直線状に形成する以前の直線状態にて着磁
することができるようになり、もってそのiffを行な
い安くなるといった優れた効果を奏する非接触式ボテフ
シ1メータを提供することができる。
[Effect of the invention 1] According to the invention configured as described above, by forming the magnetic field generating means from a flexible bamboo material (1), It is possible to provide a non-contact type 1-meter with excellent effects such as being able to be magnetized by using the IF method and being inexpensive.

[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(al中におけるX−XI2断面図を
示す。図においての(14或は、回路基板としての絶縁
基板1上に、間口部を持つ円形または多角形の形状で、
Ni  −Fe 、N1−coなどの薄膜から成る強t
o tq、 ta気抵抗素了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を出力■O
utとして取り出ザように接続されている。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が界磁発生手段として絶縁g%板1
の強磁性磁気抵抗素子2a 、2b側に取り付けられC
いる。
[Example] Hereinafter, an example of the present invention will be described based on the drawings. 1st
The figure shows an embodiment of the present invention, and figure (a) is a top view thereof, and figure (b) is a cross-sectional view taken along line X-XI2 in figure (al). On the insulating substrate 1 as a circular or polygonal shape with a frontage part,
A strong material consisting of a thin film of Ni-Fe, N1-co, etc.
otq, tac resistors 2a and 2b are 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 output from inside the ferromagnetic magnetoresistive elements 2a and 2b.
Take it out as ut and connect it like so. A semicircular arc-shaped permanent magnet 6 is attached to the insulating g% plate 1 as a field generating means at a predetermined distance from the ferromagnetic magnetoresistive elements 2a and 2b.
The ferromagnetic magnetoresistive elements 2a and 2b are attached to the C
There is.

この様子ないしは態様を第2図を4黒して、さらに訂ら
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の回転軸っ
け上下方向に指向し、ハウジング7の上面部を円通し軸
受10により支持されている。ハウジング7の下端間口
部にはケース11が閉塞状態に設けられ、そのト面には
絶縁基(反1が装着されている。磁界発作手段としての
永久磁石6は21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、2bの外周
囲に同心的となるように配置されている。
To explain this state or mode more clearly by highlighting 4 in FIG. It is oriented in the vertical direction, and the upper surface of the housing 7 is supported by a circular bearing 10. A case 11 is provided in a closed state at the lower end of the housing 7, and an insulating base (reverse 1) is attached to the top surface of the case 11.A permanent magnet 6, which serves as a magnetic field generating means, has a 21-arc shape; is attached to the outer peripheral surface of the rotor 8 and arranged concentrically around the outer periphery of the ferromagnetic magnetoresistive elements 2a and 2b.

このとき、永久磁石6の両0::’部には外方に指向す
るように形成された逃げ部6t’! 、 6bがあり、
これにより腎けJが永久磁石6とtま反対側の部分の強
磁性■気抵抗素F2a 、2bにはなるべく及ばないよ
うにしている。
At this time, both 0::' portions of the permanent magnet 6 have relief portions 6t' formed so as to be oriented outward. , there is 6b,
This prevents the magnetic field J from reaching the ferromagnetic resistance elements F2a, 2b on the opposite side from the permanent magnet 6 as much as possible.

この永久磁石6は可撓性(4祠料例えば、スヂレンブク
ジ1ンゴム(SBR)にLn気性材料粉末を分散し、こ
の状態で第1図(a)に記号Mにて示すように径方向に
着磁している。そして、かかる永久磁石6ならびに強磁
悄Vt!気抵抗素子2a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 permanent magnet 6 is made of a flexible material (for example, Ln material powder is dispersed in SBR rubber), and in this state it is attached in the radial direction as shown by the symbol M in FIG. 1(a). The permanent magnet 6 and the ferromagnetic resistance element 2a are shown as symbol i in FIG. 1(b).
A closed magnetic path is formed as shown in .

また、永久磁石6は強磁性(n気抵抗ds r2 a 
−。
Moreover, the permanent magnet 6 has ferromagnetism (n-resistance ds r2 a
−.

2bの中心を回転軸の中心にして強磁性磁気抵抗素子2
a 、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に向けて発生する磁界の強度
の絶体値は強磁性磁気抵抗素子2aの飽和[0界強度以
上となるように実際の実施例上、設定されている。また
、その磁界は強磁性t6気抵抗晃子2aの周方向に垂直
な方向すなわら、半径方向に印1)0されている。
Ferromagnetic magnetoresistive element 2 with the center of 2b as the center of the rotation axis.
It rotates in the circumferential direction of a and 2b, and the permanent magnet 6
In actual embodiments, the absolute value of the strength of the magnetic field generated toward the ferromagnetic magnetoresistive element 2a is set to be equal to or higher than the saturation (zero field strength) of the ferromagnetic magnetoresistive element 2a. Further, the magnetic field is marked 1) in a direction perpendicular to the circumferential direction of the ferromagnetic t6 resistor 2a, 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メータ 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[I気抵抗累子
2a、2bの周方向に回転げることにより強磁性磁気抵
抗素子28内の抵抗1直減少部分も連続的に回転移動す
る。このため)8地端子と出力端子■outとの間の抵
抗(直と、出力端子voutと電源電圧Vcc端子との
抵抗(1口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0′!2図に示づよ
うなスj・レートな直線性を持つたちのとなる。
Next, when the potentiometer ferromagnetic magnetoresistive elements 2a and 2b constructed as described above are subjected to a magnetic field from the permanent magnet 6 in a direction perpendicular to the current direction, their resistance value decreases. As the permanent magnet 6 rotates in the circumferential direction of the ferromagnetic resistance elements 2a and 2b, the part of the ferromagnetic resistance element 28 in which the resistance is reduced by one rotation also rotates continuously. Therefore, the resistance (direct) between the 8 ground terminal and the output terminal ■out, and the resistance (as a divided voltage value of the power supply voltage VCC determined by the ratio with the resistance between the output terminal vout and the power supply voltage Vcc terminal) The value of the output Vout is 0'!2, which has a straight linearity as shown in Figure 2.

なお、第3図において回転角度Qdcgとは第1図にお
ける永久磁石6の直線の辺6Cが図中のX−X線に垂直
であり、ま1a図中左側に永久un ’fli6を配置
づるときである。また、第3図はその(q冒から第1図
において右回転する特性を示しているが、その回転方向
は、所望といった必要に応じて右左どららでもよい。
In addition, in Fig. 3, the rotation angle Qdcg means that the straight side 6C of the permanent magnet 6 in Fig. 1 is perpendicular to the line X-X in the figure, and when the permanent un 'fli 6 is placed on the left side in Fig. 1a. It is. Further, although FIG. 3 shows the characteristic of clockwise rotation in FIG.

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II界(−点鎖線
)双子の磁界強度(絶体圃)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VO
ut(7)値が実施(り1上、永久磁G6の取り付C)
誤7!iお31;び着1n強m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l nsbの特
性を点線で示すが、l nsbは磁界強度が大となる稈
抵抗■が大となることが分かる、。
As shown in the graph of FIG. 4 (solid line), the ferromagnetic magnetoresistive elements 2a and 2b decrease their resistance when subjected to the magnetic field intensity (absolute field) of the saturated II field (-dotted chain line). is constant (the resistance value is approximately constant), so the output VO
ut(7) value is implemented (on RI1, permanent magnet G6 installation C)
Wrong 7! 31; This eliminates the dependence on slight fluctuations in adhesion of just over 1nm. In addition, in FIG. 4, the characteristics of lnsb are shown by dotted lines, and it can be seen that in lnsb, the culm resistance ■ becomes large as the magnetic field strength becomes large.

このように上記の構成では、永久磁石6を磁気粉末を分
散させた可!Q性材材料により形成したことがら着磁時
には永久16石6を直線状態にて19さ方向に着…でき
ることとなり、着磁がきわめて容易になるといった著し
く勝れた効果を右づる非接触型ポテンショメータを記供
することができる。
In this way, in the above configuration, it is possible to use the permanent magnet 6 with magnetic powder dispersed therein! Due to the fact that it is made of Q material, it is possible to attach the permanent 16 stones 6 in a straight line in the 19 horizontal direction during magnetization, making magnetization extremely easy. can be provided.

つぎに第5図<a)、(b)はこの発明の第2実滴例を
示す。この第2実施例が第1実施例とI’fl違すると
ころは下記の如くである。すなわら、第1実施例では永
久磁石6を強磁性磁気11(波素子2a、2bの外周囲
に位置させたが、この第2実施例では永久磁石6と強を
公性磁気抵抗素了2a、2bとの平均半径を一致させ永
久磁石6と強磁性【j気抵抗木子2aとが上下に対応す
るように位置させている。また、この第2実施例では第
1実施IZIでの逃げ部6a 、6bを省略している。
Next, FIGS. 5(a) and 5(b) show a second actual droplet example of the present invention. The differences between this second embodiment and the first embodiment are as follows. In other words, in the first embodiment, the permanent magnet 6 was positioned around the ferromagnetic magnet 11 (wave elements 2a, 2b), but in this second embodiment, the permanent magnet 6 and the strong magnetic field were located at the outer periphery of the ferromagnetic magnet 11 (wave elements 2a, 2b). 2a and 2b, and are positioned so that the permanent magnet 6 and the ferromagnetic resistor 2a correspond vertically.In addition, in this second embodiment, the escape in the first embodiment IZI is Sections 6a and 6b are omitted.

なんとなれば、この逃げ部6a、6bは必ずしも必要な
ものではなく不要なばあいには省略してbよく、昔は必
要に応じて設けろようにt6i成づればよい。
The escape parts 6a and 6b are not necessarily necessary, and can be omitted if they are unnecessary.

このように構成しても第1実施例と同様の1A東がI’
?られる。なお、この第2実施例では第1実燕例と同一
部分には同一符号を付して異なる部分のみ説明した。
Even with this configuration, 1A east is I' as in the first embodiment.
? It will be done. In this second embodiment, the same parts as in the first swallow example are given the same reference numerals, and only the different parts are explained.

第6図(al、(b)はこの発明の第3実施例を示す。FIGS. 6(a) and 6(b) show a third embodiment of the present invention.

この第3実施例では第1実施例における永久C4に石6
のる(イ1方向を第6図(blに記号N・1′で示すよ
うに径り向と(J直角方向にしている。そして、同図に
記号iで示すような(1路が形成されろ1゜第7図(a
)、(b)はこの発明の第4実施例を示す。この第4実
tJ色例では第2実施例における永久磁石6の着磁1ノ
向を第7図(b)に記号M ”で示すように厚さ方向と
は直角方向にしている。そし″C1同図に記号iで示す
ようなm路が形成される。
In this third embodiment, a stone 6 is added to the permanent C4 in the first embodiment.
(1 direction is shown in Fig. 6 (bl) as the radial direction and (J direction) as shown by the symbol i. Let's do it 1゜Figure 7 (a
) and (b) show a fourth embodiment of the present invention. In this fourth actual tJ color example, the direction of magnetization of the permanent magnet 6 in the second embodiment is perpendicular to the thickness direction, as shown by the symbol M'' in FIG. 7(b). C1 An m path as shown by the symbol i in the same figure is formed.

なj3、」−記実施(列では強10性11i気抵抗X’
j”2a、2bの形状【ま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。また、ロータが回転変位と直線変位どを併有す
る新奇なものに構成し、これらの両変位をそれぞれ取り
出すように構成してもよい。または、ロータの回転変位
と直P2☆位とを同時に取り出すように構成するように
してしよい。
j3,'' - implementation (in the column, strong 10 resistance 11i resistance X'
The shape of the rotor 2a, 2b (although the shape is circular or polygonal, the shape is not limited to this, and may be a strip shape, for example. Alternatively, the rotational displacement of the rotor and the direct P2☆ position may be taken out simultaneously.

また、上記実施例では磁界発生手段としての永久…石6
を形成するときに、スヂレンブタジ1ンゴムを用いたが
、これのみに限定されず、要はプラスデックなどの無方
向に自由に)尭み得る可撓性材料であればよい、。
Further, in the above embodiment, a permanent stone 6 as a magnetic field generating means is used.
Although styrene-butadiene rubber was used to form the rubber, it is not limited to this, and any flexible material that can be freely gripped in any direction, such as Plus Deck, may be used.

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, various changes may be made in the specific implementation without departing from the gist and gist of the invention.

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

第1回はこの発明のボjンシコメータの一実施例であり
、同図(a)にその上面図、同図(b)にX−Xaの断
面図を示す。第2図は縦断面図、第3図(ま第1図にお
ける実施例の出力特性を示ザグラフ、第4図は強t−n
性磁気抵抗素子の特性を示づグラフ、第5図(a)、(
b)はこの発明の第2実施例を示す上面図及び断面図、
第6図(a)、(b)はこの発明の第3実施例を示す上
面図及び断面図、第7図(a)、(b)はこの発明の第
4実施例を示す上面図及び断面図、第8図は出力特性を
示すグラフである1゜ 図中、1・・・絶縁林板(回路基1反)  2a、2b
・・・強1149611気爪抗素子 6・・・永久…石
(ta磁界発生手段 7・・・ハウジング 8・・・ロ
ータ 9・・・回転軸 10・・・軸受
The first example shows an embodiment of the bonsicometer of the present invention, and FIG. 11A shows a top view thereof, and FIG. Fig. 2 is a vertical cross-sectional view, Fig. 3 is a graph showing the output characteristics of the embodiment in Fig. 1, and Fig. 4 is a graph showing the output characteristics of the embodiment in Fig. 1.
Graphs showing the characteristics of magnetic magnetoresistive elements, Fig. 5(a), (
b) is a top view and a sectional view showing a second embodiment of the present invention;
FIGS. 6(a) and (b) are a top view and a sectional view showing a third embodiment of the invention, and FIGS. 7(a) and (b) are a top view and a sectional view showing a fourth embodiment of the invention. Figure 8 is a graph showing the output characteristics. In the figure, 1... Insulation board (1 circuit board) 2a, 2b
...Strong 1149611 Claw resistance element 6...Permanent...Stone (ta) Magnetic field generating means 7...Housing 8...Rotor 9...Rotating shaft 10...Bearing

Claims (1)

【特許請求の範囲】 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とで閉磁路を形
成するように装着された磁界発生手段とを備え、 前記磁界発生手段を可撓性磁性材料により形成し、該磁
界発生手段を所定の形状に曲成する前の直線状態で着磁
したことを特徴とする非接触式ポテンショメータ。 2)前記磁界発生手段は、両端部に外方に指向する逃げ
部を有し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。 3)前記磁界発生手段は、可撓性材のプラスチックに磁
気材料粉末を分散して成る材料を構成することを特徴と
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。 4)前記磁界発生手段は、前記強磁性磁気抵抗素子と同
心的に配置さ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。
[Claims] 1) A housing, a rotor rotatably provided within the housing, and a ferromagnetic material of a predetermined shape disposed concentrically with the rotor and spaced from the rotor by a predetermined distance. an insulating substrate having a magnetoresistive element; and a magnetic field generating means mounted on the rotor side so as to form a closed magnetic path with the ferromagnetic magnetoresistive element, the magnetic field generating means being formed of a flexible magnetic material. A non-contact type potentiometer, characterized in that the magnetic field generating means is magnetized in a straight state before being bent into a predetermined shape. 2) The non-contact potentiometer according to claim 1, wherein the magnetic field generating means has outwardly directed relief portions at both ends. 3) The non-contact potentiometer according to claim 1, wherein the magnetic field generating means is made of a material in which magnetic material powder is dispersed in a flexible plastic material. 4) The non-contact potentiometer according to claim 1, wherein the magnetic field generating means is arranged concentrically with the ferromagnetic magnetoresistive element.
JP61198777A 1986-07-29 1986-08-25 Non-contact type potentiometer Expired - Lifetime JPH077725B2 (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP61198777A JPH077725B2 (en) 1986-08-25 1986-08-25 Non-contact type potentiometer
EP87110695A EP0255052B1 (en) 1986-07-29 1987-07-23 Noncontact potentiometer
US07/076,891 US4835509A (en) 1986-07-29 1987-07-23 Noncontact potentiometer
DE3788831T DE3788831T2 (en) 1986-07-29 1987-07-23 Contactless potentiometer.
KR1019870008259A KR900007100B1 (en) 1986-07-29 1987-07-29 Non-contact potentiometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61198777A JPH077725B2 (en) 1986-08-25 1986-08-25 Non-contact type potentiometer

Publications (2)

Publication Number Publication Date
JPS6354784A true JPS6354784A (en) 1988-03-09
JPH077725B2 JPH077725B2 (en) 1995-01-30

Family

ID=16396749

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61198777A Expired - Lifetime JPH077725B2 (en) 1986-07-29 1986-08-25 Non-contact type potentiometer

Country Status (1)

Country Link
JP (1) JPH077725B2 (en)

Also Published As

Publication number Publication date
JPH077725B2 (en) 1995-01-30

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