JPH06147816A - Angle sensor - Google Patents

Angle sensor

Info

Publication number
JPH06147816A
JPH06147816A JP29729492A JP29729492A JPH06147816A JP H06147816 A JPH06147816 A JP H06147816A JP 29729492 A JP29729492 A JP 29729492A JP 29729492 A JP29729492 A JP 29729492A JP H06147816 A JPH06147816 A JP H06147816A
Authority
JP
Japan
Prior art keywords
magnetic field
angle
magnetoresistive element
magnetic
central axis
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP29729492A
Other languages
Japanese (ja)
Inventor
Hiroyuki Okubo
浩之 大久保
Takuyo Miyashita
卓世 宮下
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.)
Sony Magnescale Inc
Original Assignee
Sony Magnescale Inc
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 Sony Magnescale Inc filed Critical Sony Magnescale Inc
Priority to JP29729492A priority Critical patent/JPH06147816A/en
Publication of JPH06147816A publication Critical patent/JPH06147816A/en
Pending legal-status Critical Current

Links

Landscapes

  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)

Abstract

PURPOSE:To achieve a linear displacement-output characteristic curve over a wide range by disposing magnetoresistive elements of ferromagnetic metal symmetrically to the magnetic axis of a permanent magnet. CONSTITUTION:A rotary section 21 has a circular surface applied with a magnetizing body 23 comprising a permanent magnet having N and S poles extending spirally. A magnetic head 11 comprises a permanent magnet board for forming a bias field, and a magnetoresistive element formed of a ferromagnetic metal film. Direction of the bias field is matched with the longitudinal direction of the board and the magnetic axis extends along the longitudinal direction of the board. The magnetoresistive element has two magneto-sensitive parts crossing perpendicularly each other while making an angle of 45 deg. against the direction of the bias field. When the rotary section 21 rotates with respect to the magnetic head 11, signal field of the magnetic head 11 functioning on the magnetoresistive element varies. Since the relationship between the rotational angular speed of the rotary section 21 and the output voltage from the magnetoresistive element exhibits linearity over a wide range, microrotational angle can be measured highly accurately.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は微小な角度変位を高い精
度にて計測するための角度センサに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an angle sensor for measuring a minute angular displacement with high accuracy.

【0002】[0002]

【従来の技術】磁気抵抗素子(MR素子)を使用した変
位センサは広く使用されている。斯かる磁気抵抗素子は
ホール効果(半導体磁気抵抗効果)を利用した半導体磁
気抵抗素子と強磁性金属の磁気抵抗効果を利用した強磁
性金属磁気抵抗素子とに大別される。強磁性金属磁気抵
抗素子は磁場の強さ及び方向と抵抗値の関係において直
線性を得るのが容易である等の理由により位置センサに
広く使用されている。
2. Description of the Related Art A displacement sensor using a magnetoresistive element (MR element) is widely used. Such magnetoresistive elements are roughly classified into semiconductor magnetoresistive elements utilizing the Hall effect (semiconductor magnetoresistive effect) and ferromagnetic metal magnetoresistive elements utilizing the magnetoresistive effect of ferromagnetic metals. Ferromagnetic metal magnetoresistive elements are widely used in position sensors because it is easy to obtain linearity in the relationship between the resistance value and the strength and direction of a magnetic field.

【0003】強磁性金属磁気抵抗素子の抵抗値ρは磁化
方向の関数として次の数1の式によって表される。
The resistance value ρ of the ferromagnetic metal magnetoresistive element is expressed by the following equation 1 as a function of the magnetization direction.

【0004】[0004]

【数1】 [Equation 1]

【0005】但し、ρ(θ):磁気抵抗素子の抵抗値、 θ:電流と飽和磁化方向のなす角、 ρ1 :電流と飽和磁化方向が直交したときの磁気抵抗素
子の抵抗値、 ρ2 :電流と飽和磁化方向が平行なときの磁気抵抗素子
の抵抗値。
Where ρ (θ) is the resistance value of the magnetoresistive element, θ is the angle between the current and the saturation magnetization direction, ρ 1 is the resistance value of the magnetoresistive element when the current and the saturation magnetization direction are orthogonal, ρ 2 : The resistance value of the magnetoresistive element when the current and the saturation magnetization direction are parallel.

【0006】この式はViogt-Thomson の式として良く知
られている。強磁性金属は可逆磁場以下の強さの磁場で
は履歴作用を表すから、通常、飽和磁場にて使用され
る。
This equation is well known as the Viogt-Thomson equation. Ferromagnetic metals are usually used in a saturation magnetic field because they exhibit a hysteresis action in a magnetic field having a strength equal to or lower than the reversible magnetic field.

【0007】この式から明らかなように、強磁性金属磁
気抵抗素子は、電流と磁化方向(磁場の方向)が平行な
ときに最大抵抗値ρ2 を有し電流と磁化方向(磁場の方
向)が直角なときに最小抵抗値ρ1 を有する。
As is clear from this equation, the ferromagnetic metal magnetoresistive element has the maximum resistance value ρ 2 when the current and the magnetization direction (direction of the magnetic field) are parallel, and the current and the magnetization direction (direction of the magnetic field). Has a minimum resistance value ρ 1 when is orthogonal.

【0008】図3を参照して強磁性金属磁気抵抗素子の
原理を説明する。尚、強磁性金属磁気抵抗素子の原理及
びそれを使用した変位センサの詳細については、例え
ば、「センサ技術」(1981年11月号)〔Vol.1.N
O.4〕(47〜53頁)の『強磁性金属薄膜素子による
変位検出』を参照されたい。
The principle of the ferromagnetic metal magnetoresistive element will be described with reference to FIG. For the details of the principle of the ferromagnetic metal magnetoresistive element and the displacement sensor using the same, see, for example, "Sensor Technology" (November 1981) [Vol.1.N].
O.4] (pp. 47-53), "Displacement detection by ferromagnetic metal thin film element".

【0009】図示のように、強磁性金属磁気抵抗素子の
2つの細長い感磁部31A、31Bは互いに直交するよ
うに配置される。従って斯かる感磁部31A、31Bを
流れる電流Iの方向は互いに直交する。第1の感磁部3
1Aの長手方向をY軸としそれに直角な第2の感磁部3
1Bの長手方向をX軸とする。
As shown in the figure, the two elongated magnetic sensitive portions 31A and 31B of the ferromagnetic metal magnetoresistive element are arranged so as to be orthogonal to each other. Therefore, the directions of the currents I flowing through the magnetic sensitive sections 31A and 31B are orthogonal to each other. First magnetic sensing section 3
The second magnetic sensitive section 3 which has the longitudinal direction of 1A as the Y axis and is perpendicular to the Y axis
The longitudinal direction of 1B is the X axis.

【0010】斯かる2つの感磁部31A、31Bに直流
バイアス磁場HB が付与されているものとする。従っ
て、更に信号磁場HS が作用すると、感磁部31A、3
1Bにはバイアス磁場HB と信号磁場HS の合成磁場H
が作用する。バイアス磁場HBの方向はY軸に対して4
5度の角度をなし、信号磁場HS の方向はY軸に対して
90度の角度をなすとすれば、合成磁場Hの方向はY軸
に対して(45+Δθ)度の角度をなす。
It is assumed that a DC bias magnetic field H B is applied to the two magnetic sensitive sections 31A and 31B. Therefore, when the signal magnetic field H S is further applied, the magnetic sensitive portions 31A, 3A
1B is a combined magnetic field H of the bias magnetic field H B and the signal magnetic field H S.
Works. The direction of the bias magnetic field H B is 4 with respect to the Y axis.
5 ° an angle of the direction of the signal magnetic field H S is if an angle of 90 degrees with respect to Y axis, the direction of the resultant magnetic field H forms an angle of (45 + Δθ) degrees with respect to the Y axis.

【0011】第1の感磁部31Aと第2の感磁部31B
の抵抗値は略同一であるものとする。第1の感磁部31
Aの抵抗値ρA と第2の感磁部31Bの抵抗値ρB とは
数1の式を使用してそれぞれ次の数2の式によって表さ
れる。
First magnetic sensitive section 31A and second magnetic sensitive section 31B
The resistance values of are assumed to be substantially the same. First magnetic sensitive section 31
Each resistance value of A [rho A and the resistance value [rho B of the second sensitive portion 31B using the equation 1 is represented by the formula for a number of 2.

【0012】[0012]

【数2】 [Equation 2]

【0013】図示のように、2つの感磁部31A、31
Bは直列に接続されて更に直流電源35(電圧V0 )が
接続される。従って第2の感磁部31Bの両端の電圧は
次の数3の式によって表される。
As shown, the two magnetic sensitive parts 31A, 31
B is connected in series and further connected to a DC power supply 35 (voltage V 0 ). Therefore, the voltage across the second magnetically sensitive portion 31B is expressed by the following equation (3).

【0014】[0014]

【数3】 [Equation 3]

【0015】この数3の式に数2の式を代入すると次の
数4の式が得られる。
Substituting the expression of the expression 2 into the expression of the expression 3, the following expression of the expression 4 is obtained.

【0016】[0016]

【数4】 [Equation 4]

【0017】この式の右辺の第1項は信号磁場がない場
合、即ちHS =0の場合に出力端子に表れる電圧であ
り、第2項は信号磁場の大きさと方向によって変化する
電圧部分である。
The first term on the right side of this equation is the voltage appearing at the output terminal when there is no signal magnetic field, that is, when H S = 0, and the second term is the voltage portion that changes depending on the magnitude and direction of the signal magnetic field. is there.

【0018】尚、数2の式の両者を加算すると次の数5
の式が得られる。
When the two equations are added, the following equation 5 is obtained.
Is obtained.

【0019】[0019]

【数5】 [Equation 5]

【0020】即ち、2つの感磁部31A、31Bの抵抗
値の和は常に一定となる。
That is, the sum of the resistance values of the two magnetic sensitive sections 31A and 31B is always constant.

【0021】図4に強磁性金属磁気抵抗素子31の例を
示す。強磁性金属磁気抵抗素子31は基板41の表面に
強磁性金属薄膜を蒸着することによって形成されてい
る。基板41の裏面にはバイアス磁場HB を生成するた
めの永久磁石が付着されている。永久磁石のN極とS極
はバイアス磁場HB の方向が図示のように基板の長手方
向に整合するように配置される。即ち磁軸(N極とS極
を結ぶ線)は長手方向に沿って配置される。
FIG. 4 shows an example of the ferromagnetic metal magnetoresistive element 31. The ferromagnetic metal magnetoresistive element 31 is formed by depositing a ferromagnetic metal thin film on the surface of the substrate 41. A permanent magnet for generating a bias magnetic field H B is attached to the back surface of the substrate 41. The N and S poles of the permanent magnet are arranged so that the direction of the bias magnetic field H B is aligned with the longitudinal direction of the substrate as shown. That is, the magnetic axis (the line connecting the N pole and the S pole) is arranged along the longitudinal direction.

【0022】強磁性金属磁気抵抗素子31は感磁部43
A、43Bとリード部45A、45B、45Cよりな
る。感磁部は第1の感磁部43Aと第2の感磁部43B
とを有し、各感磁部は複数の平行な細長い帯状に形成さ
れた強磁性金属薄膜を含み、それらは直列に接続されて
いる。第1の感磁部43Aの帯状の強磁性金属薄膜と第
2の感磁部43Bの帯状の強磁性金属薄膜とは互いに直
交するように且つ基板41の長手方向に対して45度の
角度をなすように配置されており、更に、基板41の長
手方向に垂直な中心線に対して対称に配置されている。
The ferromagnetic metal magnetoresistive element 31 includes a magnetic sensing section 43.
A, 43B and lead parts 45A, 45B, 45C. The magnetic sensitive sections are the first magnetic sensitive section 43A and the second magnetic sensitive section 43B.
And each magnetic sensitive portion includes a plurality of parallel thin strip-shaped ferromagnetic metal thin films, which are connected in series. The strip-shaped ferromagnetic metal thin film of the first magnetic sensing portion 43A and the strip-shaped ferromagnetic metal thin film of the second magnetic sensing portion 43B are orthogonal to each other and formed at an angle of 45 degrees with respect to the longitudinal direction of the substrate 41. The substrates 41 are arranged so as to be arranged, and further, are arranged symmetrically with respect to a center line perpendicular to the longitudinal direction of the substrate 41.

【0023】リード部45A、45B、45Cは基準電
流を付与するための入力端子45A、45Cと出力電圧
を取り出すための出力端子45Bとを有する。
The lead portions 45A, 45B, 45C have input terminals 45A, 45C for applying a reference current and output terminals 45B for extracting an output voltage.

【0024】こうして、強磁性金属磁気抵抗素子31の
2つの感磁部43A、43Bの配向とバイアス磁場HB
の方向の間の関係は図3に示した2つの感磁部31A、
31Bの配向とバイアス磁場HB の方向の間の関係と同
一となる。尚、強磁性金属磁気抵抗素子は、好ましく
は、バイアス磁場HB の方向が信号磁場HS の方向と直
交するように配置される。
Thus, the orientations of the two magnetic sensitive portions 43A and 43B of the ferromagnetic metal magnetoresistive element 31 and the bias magnetic field H B.
The relationship between the directions of the two magnetic sensitive parts 31A shown in FIG.
The relationship between the orientation of 31B and the direction of the bias magnetic field H B is the same. The ferromagnetic metal magnetoresistive element is preferably arranged so that the direction of the bias magnetic field H B is orthogonal to the direction of the signal magnetic field H S.

【0025】図5に強磁性金属磁気抵抗素子31を使用
した変位センサの例を示す。変位センサは発磁体部51
と斯かる発磁体部51より隔置され且つそれに対して相
対的に移動する検出ヘッド53とを有し、該検出ヘッド
53によって両者間の相対的変位及び変位方向が検出さ
れるように構成されている。発磁体部51は信号磁場H
S を生成する発磁体55よりなり、斯かる発磁体55は
例えばN極とS極が交互に配列されるように構成された
永久磁石であってよい。
FIG. 5 shows an example of a displacement sensor using the ferromagnetic metal magnetoresistive element 31. The displacement sensor is the magnetism generating part 51.
And a detection head 53 which is spaced from the magnetism generator 51 and moves relative to the magnetism generator 51, and the detection head 53 is configured to detect the relative displacement and displacement direction between the two. ing. The magnetic field generator 51 has a signal magnetic field H
The magnet 55 includes a magnet 55 that generates S, and the magnet 55 may be, for example, a permanent magnet configured such that north poles and south poles are alternately arranged.

【0026】検出ヘッド53は図4にて説明した如きバ
イアス磁場HB を生成するための永久磁石47と基板4
1に形成された強磁性金属磁気抵抗素子31とを含み、
強磁性金属磁気抵抗素子31の2つの感磁部43A、4
3Bは互いに直角に且つ長手方向に対して45度の角度
をなすように配置されている。こうして、検出ヘッドの
強磁性金属磁気抵抗素子31の2つの感磁部43A、4
3Bの配向と永久磁石によって生成されるバイアス磁場
B の方向と発磁体部51の発磁体55によって生成さ
れる信号磁場HS の方向との間の関係は図3に示した2
つの感磁部31A、31Bの配向とバイアス磁場HB
方向の間の関係と同一となる。
The detection head 53 includes a permanent magnet 47 for generating the bias magnetic field H B as described with reference to FIG.
1 and a ferromagnetic metal magnetoresistive element 31 formed in
The two magnetic sensitive sections 43A, 4A of the ferromagnetic metal magnetoresistive element 31.
3B are arranged at right angles to each other and at an angle of 45 degrees with respect to the longitudinal direction. In this way, the two magnetic sensitive parts 43A, 4A of the ferromagnetic metal magnetoresistive element 31 of the detection head are
The relationship between the orientation of 3B, the direction of the bias magnetic field H B generated by the permanent magnet, and the direction of the signal magnetic field H S generated by the magnet 55 of the magnet unit 51 is shown in FIG.
The relationship between the orientations of the three magnetic sensitive portions 31A and 31B and the direction of the bias magnetic field H B is the same.

【0027】更に、検出ヘッド53はバイアス磁場HB
の方向が信号磁場HS の方向と直交するように配置され
る。
Further, the detecting head 53 has a bias magnetic field H B.
Is arranged so that the direction of is perpendicular to the direction of the signal magnetic field H S.

【0028】斯かる検出ヘッドには図示の如く適当な信
号検出回路が接続されている。斯かる信号検出回路は差
動増幅回路57を含み、第1の端子59より基準電圧が
入力され第2の端子61より出力電圧Vが出力される。
端子61より取り出された出力電圧Vは図5Bに示す如
き信号波形を有する。図5Bは変位(横軸)と出力電圧
Vの大きさ(縦軸)の関係即ち変位−出力特性を表すか
ら、斯かる関係より発磁体部51に対する検出ヘッド5
3の相対的変位量と変位方向が検出される。
An appropriate signal detection circuit is connected to the detection head as shown in the figure. Such a signal detection circuit includes a differential amplifier circuit 57, and the reference voltage is input from the first terminal 59 and the output voltage V is output from the second terminal 61.
The output voltage V taken out from the terminal 61 has a signal waveform as shown in FIG. 5B. FIG. 5B shows the relationship between the displacement (horizontal axis) and the magnitude of the output voltage V (vertical axis), that is, the displacement-output characteristic.
The relative displacement amount and displacement direction of 3 are detected.

【0029】変位センサにて高い測定精度を得るには、
出力電圧と変位の関係が線型的であることが好ましい。
しかしながら、図5Bのグラフに示す如き変位−出力特
性がでは、出力電圧が変位に対して線型的に即ち直線的
に変化する範囲が狭い。変位−出力特性が直線的である
範囲が広い程、変位センサによって高い精度にて測定す
ることができる。
In order to obtain high measurement accuracy with the displacement sensor,
It is preferable that the relationship between the output voltage and the displacement is linear.
However, in the displacement-output characteristic shown in the graph of FIG. 5B, the range in which the output voltage changes linearly, that is, linearly with respect to the displacement is narrow. The wider the range in which the displacement-output characteristic is linear, the higher the accuracy with which the displacement sensor can measure.

【0030】斯かる変位−出力特性の直線性が広い範囲
にて得られるような試みがなされている。
Attempts have been made to obtain such linearity of displacement-output characteristics in a wide range.

【0031】図6は変位−出力特性の直線性を向上させ
るように構成された変位センサの例を示す。この例で
は、図6Aに示すように、検出ヘッド53は発磁体55
のN極とS極の境界線に対して傾斜して移動するように
構成されている。斯かる場合、バイアス磁場HB のベク
トルと発磁体55の信号磁場HS のベクトルと両者の合
成磁場Hのベクトルは図6Bに示すようになる。斯くし
て変位−出力特性は、図6Cに示すように、広い範囲に
わたって直線性を有するようになる。
FIG. 6 shows an example of a displacement sensor configured to improve the linearity of the displacement-output characteristic. In this example, as shown in FIG.
It is configured so as to be inclined with respect to the boundary line between the N pole and the S pole. In such a case, the vector of the bias magnetic field H B , the vector of the signal magnetic field H S of the magnet body 55, and the vector of the combined magnetic field H are as shown in FIG. 6B. Thus, the displacement-output characteristic becomes linear over a wide range as shown in FIG. 6C.

【0032】また図7に示すように、発磁体55を構成
する永久磁石を、隣接する永久磁石より隔置することに
よっても、変位−出力特性の直線性を向上させることが
できることが知られている。
Further, as shown in FIG. 7, it is known that the linearity of the displacement-output characteristic can be improved also by arranging the permanent magnets constituting the magnet body 55 apart from the adjacent permanent magnets. There is.

【0033】[0033]

【発明が解決しようとする課題】上述のように、磁気ヘ
ッドに強磁性金属磁気抵抗素子31を使用し直線的変位
を検出するための変位センサは広く知られている。ま
た、斯かる変位センサにおいて、広い測定範囲にわたっ
て変位−出力特性が直線性を有するように構成されたも
のが提案されている。
As described above, a displacement sensor for detecting linear displacement using the ferromagnetic metal magnetoresistive element 31 in the magnetic head is widely known. Further, in such a displacement sensor, there has been proposed a displacement sensor having a linear displacement-output characteristic over a wide measurement range.

【0034】しかしながら、角度変位を検出するアナロ
グ角度センサ(以下、単に角度センサと称する。)で
は、検出ヘッドに強磁性金属磁気抵抗素子31を使用し
且つ広い測定範囲にわたって変位−出力特性が直線性を
有するように構成されたものは知られていない。
However, in the analog angle sensor for detecting the angular displacement (hereinafter, simply referred to as an angle sensor), the ferromagnetic metal magnetoresistive element 31 is used for the detection head and the displacement-output characteristic is linear over a wide measurement range. Nothing configured to have is known.

【0035】従来、検出ヘッドに半導体磁気抵抗素子を
使用した角度センサは知られている。半導体磁気抵抗素
子はノイズや振動に対する抵抗性がよくまた高速応答性
に優れているが、温度特性が悪く温度補償が必要である
欠点を有する。一方、強磁性金属磁気抵抗素子は温度特
性が良好なため温度補償を必要としない利点がある。強
磁性金属磁気抵抗素子の抵抗値の温度係数は3×10-3
Ω/°C以下であるが、半導体磁気抵抗素子の抵抗値の
温度係数はそれより1桁以上大きい。
Conventionally, an angle sensor using a semiconductor magnetoresistive element for a detection head is known. Although the semiconductor magnetoresistive element has good resistance to noise and vibration and excellent high-speed response, it has a drawback in that it has poor temperature characteristics and requires temperature compensation. On the other hand, the ferromagnetic metal magnetoresistive element has an advantage that it does not require temperature compensation because it has good temperature characteristics. The temperature coefficient of the resistance value of the ferromagnetic metal magnetoresistive element is 3 × 10 −3
Although it is Ω / ° C or less, the temperature coefficient of the resistance value of the semiconductor magnetoresistive element is larger by one digit or more.

【0036】本発明は斯かる点に鑑み、検出ヘッドに強
磁性金属磁気抵抗素子31を使用し、且つ変位−出力特
性の直線性が広い測定範囲に亘って得られる角度センサ
を提供することを目的とする。
In view of the above point, the present invention provides an angle sensor which uses a ferromagnetic metal magnetoresistive element 31 in a detection head and which has a linear displacement-output characteristic over a wide measurement range. To aim.

【0037】[0037]

【課題を解決するための手段】本発明によると、バイア
ス磁場を生成するための永久磁石と強磁性金属の磁気抵
抗素子とを含み該磁気抵抗素子は上記永久磁石の磁軸に
直交した線に対して対称的に且つその両側にそれぞれ配
置された第1の感磁部と第2の感磁部とを有し上記第1
の感磁部と第2の感磁部とは互いに90度の角度をなし
且つ永久磁石の磁軸に対して45度傾斜して配置される
ように構成された磁気ヘッド11と、信号磁場を生成す
るべく中心軸線周りに回転可能な発磁体23と、を有す
る角度センサにおいて、発磁体23は信号磁場のベクト
ルが中心軸線周りの中心角の関数として変化するように
N極とS極が中心角の関数として変化するように磁化さ
れ、磁気ヘッド11は発磁体23より隔置され磁気ヘッ
ド11の出力電圧が発磁体23の回転角度の関数として
表されるように構成されている。
According to the present invention, a magnetoresistive element including a permanent magnet for generating a bias magnetic field and a magnetoresistive element of a ferromagnetic metal is formed in a line perpendicular to the magnetic axis of the permanent magnet. The first magnetic sensitive section and the second magnetic sensitive section, which are symmetrically arranged on both sides of the first magnetic sensitive section, respectively.
Of the magnetic head 11 and the second magnetic sensor, which form an angle of 90 degrees with each other and are arranged at an angle of 45 degrees with respect to the magnetic axis of the permanent magnet. In an angle sensor having a magnetizing body 23 rotatable about a central axis to generate, the magnetizing body 23 has a north pole and a south pole so that a vector of a signal magnetic field changes as a function of a central angle around the central axis. Magnetized to vary as a function of angle, the magnetic head 11 is spaced from the magnet body 23 and is configured so that the output voltage of the magnetic head 11 is represented as a function of the rotation angle of the magnet body 23.

【0038】本発明によると、例えば図1に示すよう
に、角度センサにおいて、発磁体23は中心軸線に垂直
な円形面を有し、円形面はN極とS極の半径方向の寸法
が中心軸線周りの中心角の関数として変化し信号磁場の
方向が中心軸線に平行となるように磁化され、磁気ヘッ
ドは発磁体23の円形面より隔置され且つ上記バイアス
磁場の方向が信号磁場の方向に直交するよう中心軸線に
直交するように配置されている。
According to the present invention, as shown in FIG. 1, for example, in the angle sensor, the magnet body 23 has a circular surface perpendicular to the central axis, and the circular surface is centered in the radial dimension of the N pole and the S pole. The magnetic head is magnetized so that it changes as a function of the central angle around the axis and the direction of the signal magnetic field is parallel to the central axis, the magnetic head is spaced from the circular surface of the magnetizer 23, and the direction of the bias magnetic field is the direction of the signal magnetic field. Are arranged so as to be orthogonal to the central axis.

【0039】本発明によると、例えば図2に示すよう
に、角度センサにおいて、上記発磁体23は上記中心軸
線に平行な円周面を有し、該円周面はN極とS極の軸線
方向の寸法が上記中心軸線周りの中心角の関数として変
化し上記信号磁場の方向が上記中心軸線に直交するよう
に磁化され、上記磁気ヘッドは上記発磁体の円周面より
隔置され且つ上記バイアス磁場の方向が上記信号磁場の
方向に直交するよう上記中心軸線に平行となるように配
置されている。
According to the present invention, for example, as shown in FIG. 2, in the angle sensor, the magnetizing body 23 has a circumferential surface parallel to the central axis, and the circumferential surface is the axis line of N pole and S pole. The direction dimension changes as a function of the central angle about the central axis and the direction of the signal magnetic field is magnetized so as to be orthogonal to the central axis, the magnetic head is spaced from the circumferential surface of the magnet and The bias magnetic field is arranged so as to be parallel to the central axis so that the direction of the bias magnetic field is orthogonal to the direction of the signal magnetic field.

【0040】[0040]

【作用】本発明の磁気センサでは、回転部21に装着さ
れた発磁体23は中心角の関数として変化する永久磁石
を有し、磁気ヘッド11に対して回転部21が回転する
と磁気ヘッドの磁気抵抗素子に作用する信号磁場が変化
する。回転部21の回転角速度と磁気抵抗素子の出力電
圧の関係、即ち、変位−出力特性は広い範囲にて直線性
を有するから、微小回転角を高い精度にて計測すること
ができる。
In the magnetic sensor of the present invention, the magnetizing body 23 mounted on the rotating portion 21 has a permanent magnet that changes as a function of the central angle, and when the rotating portion 21 rotates with respect to the magnetic head 11, the magnetic field of the magnetic head is changed. The signal magnetic field acting on the resistance element changes. Since the relationship between the rotation angular velocity of the rotating unit 21 and the output voltage of the magnetoresistive element, that is, the displacement-output characteristic has linearity in a wide range, it is possible to measure a minute rotation angle with high accuracy.

【0041】[0041]

【実施例】以下に図1〜図2を参照して本発明の実施例
について説明する。図1は本発明の角度センサの第1の
例を示しており、斯かる角度センサは磁気ヘッド11と
回転部21とを有する。
Embodiments of the present invention will be described below with reference to FIGS. FIG. 1 shows a first example of the angle sensor of the present invention, which has a magnetic head 11 and a rotating portion 21.

【0042】回転部21は中心軸線O−O周りに回転可
能な略円板形をなしており、その円形面に永久磁石から
なる発磁体23が装着されている。本例の発磁体23は
図示のように永久磁石のN極とS極とが渦巻き状に延在
するように配置されている。即ち、発磁体23の円形面
にて永久磁石のN極とS極とはその半径方向の幅が中心
角とともに連続的に変化するように構成されている。円
形面上に中心軸線O−Oを通る点を極とする極座標
(r,θ)を設定すると、N極とS極の境界線は、例え
ば、半径rと偏角θの関数r=f(θ)として表現する
ことができる。
The rotating portion 21 has a substantially disk shape rotatable about the central axis O--O, and a magnetizing body 23 made of a permanent magnet is mounted on its circular surface. The magnetizer 23 of this example is arranged so that the N and S poles of the permanent magnet extend in a spiral shape as shown in the figure. That is, on the circular surface of the magnet body 23, the widths of the N pole and the S pole of the permanent magnet in the radial direction continuously change with the central angle. When polar coordinates (r, θ) having a point passing through the central axis O-O on the circular surface as a pole are set, the boundary line between the N pole and the S pole is, for example, a function r = f ( θ).

【0043】こうして、円形面上の発磁体23によって
生成される信号磁場HS の方向は図示の矢印のように回
転部21の中心軸線O−Oに平行である。
In this way, the direction of the signal magnetic field H S generated by the magnetic generator 23 on the circular surface is parallel to the central axis O--O of the rotating portion 21 as shown by the arrow in the figure.

【0044】磁気ヘッド11は、例えば図5〜図7に示
した如く従来の磁気ヘッド11と同様な形態のものであ
ってよく、バイアス磁場HB を生成するための永久磁石
からなる基板と斯かる基板に装着された強磁性金属膜よ
りなる強磁性金属磁気抵抗素子(以下単に磁気抵抗素子
という。)を含む。バイアス磁場HB の方向は基板の長
手方向に整合するように構成されており、磁軸(N極と
S極とを結ぶ線)は基板の長手方向に沿っている。
The magnetic head 11 may have the same form as the conventional magnetic head 11 as shown in FIGS. 5 to 7, for example, and a substrate made of a permanent magnet for generating the bias magnetic field H B and the magnetic head 11. A ferromagnetic metal magnetoresistive element (hereinafter simply referred to as a magnetoresistive element) including a ferromagnetic metal film mounted on such a substrate is included. The direction of the bias magnetic field H B is configured to match the longitudinal direction of the substrate, and the magnetic axis (the line connecting the N pole and the S pole) is along the longitudinal direction of the substrate.

【0045】磁気抵抗素子の2つの感磁部は互いに直交
し且つバイアス磁場HB の方向に対して45度の角度を
なすように配置され、更に、基板の長手方向に垂直な中
心線に対して対称に配置されている。
The two magnetic sensitive parts of the magnetoresistive element are arranged so as to be orthogonal to each other and form an angle of 45 degrees with respect to the direction of the bias magnetic field H B , and further, with respect to the center line perpendicular to the longitudinal direction of the substrate. Are arranged symmetrically.

【0046】磁気ヘッド11は発磁体23の円形面にて
且つそれより隔置されており、基板41の長手方向が発
磁体23の円形面の半径方向に沿うように配置されてい
る。更に、磁気ヘッド11はバイアス磁場HB の方向が
信号磁場HS の方向に直交するように配置される。こう
して、磁気ヘッド11の磁気抵抗素子の2つの感磁部の
配向と永久磁石によって生成されるバイアス磁場HB
方向の関係は図4〜図7に示した2つの強磁性金属磁気
抵抗素子の配向とバイアス磁場HB の方向の関係と同一
となる。
The magnetic head 11 is arranged on the circular surface of the magnetic body 23 and is spaced apart from the circular surface, and the longitudinal direction of the substrate 41 is arranged along the radial direction of the circular surface of the magnetic body 23. Further, the magnetic head 11 is arranged so that the direction of the bias magnetic field H B is orthogonal to the direction of the signal magnetic field H S. Thus, the relationship between the orientations of the two magnetically sensitive portions of the magnetoresistive element of the magnetic head 11 and the direction of the bias magnetic field H B generated by the permanent magnet is the same as that of the two ferromagnetic metal magnetoresistive elements shown in FIGS. It is the same as the relationship between the orientation and the direction of the bias magnetic field H B.

【0047】更に、磁気ヘッド11の磁気抵抗素子の2
つの感磁部の配向と永久磁石によって生成されるバイア
ス磁場HB の方向と回転部21の発磁体23によって生
成される信号磁場HS の方向との間の関係は図4〜図7
に示した2つの強磁性金属磁気抵抗素子の配向とバイア
ス磁場HB の方向と信号磁場HS の方向との間の関係と
同一となる。
Further, two of the magnetoresistive elements of the magnetic head 11 are used.
The relationship between the orientation of the two magnetic sensitive parts and the direction of the bias magnetic field H B generated by the permanent magnet and the direction of the signal magnetic field H S generated by the magnetizer 23 of the rotating part 21 is shown in FIGS.
The relationship between the orientations of the two ferromagnetic metal magnetoresistive elements and the direction of the bias magnetic field H B and the direction of the signal magnetic field H S shown in FIG.

【0048】磁気ヘッド11は例えば図5に示した如き
信号検出回路に接続されてよい。こうして、本例による
と回転部21が中心軸線O−O周りに微小角だけ回転す
ると磁気ヘッド11によって検出される信号磁場HS
強さ及び方向が変化するから、磁気ヘッド11に接続さ
れた信号検出回路の出力端子にて出力電圧が検出され
る。
The magnetic head 11 may be connected to a signal detection circuit as shown in FIG. 5, for example. Thus, according to the present example, when the rotating portion 21 rotates about the central axis O--O by a small angle, the strength and the direction of the signal magnetic field H S detected by the magnetic head 11 change, so that the magnetic head 11 is connected. The output voltage is detected at the output terminal of the signal detection circuit.

【0049】図1Bは斯かる回転部21の回転角度と磁
気抵抗素子の出力電圧の関係を示す。図示の如き角度変
位−出力電圧特性において、広い角度範囲にて直線性が
得られることが判る。
FIG. 1B shows the relationship between the rotation angle of the rotating portion 21 and the output voltage of the magnetoresistive element. It can be seen that the linearity can be obtained in a wide angle range in the angle displacement-output voltage characteristics as shown in the figure.

【0050】図2に本発明の角度センサの第2の例を示
す。図2Aに図A1と同様に角度センサは磁気ヘッド1
1と回転部21とを示す。
FIG. 2 shows a second example of the angle sensor of the present invention. In FIG. 2A, the angle sensor is the magnetic head 1 as in FIG.
1 and the rotating part 21 are shown.

【0051】回転部21は中心軸線O−O周りに回転可
能な略円筒形をなしており、その円周面に永久磁石から
なる発磁体23が装着されている。本例の発磁体23は
図示のように永久磁石のN極とS極とが螺旋状に延在す
るように配置されている。即ち、発磁体23の円周面に
て永久磁石のN極とS極とはその軸線方向の幅が中心軸
線O−O周りの中心角とともに連続的に変化するように
構成されている。展開した円周面上に中心軸線O−Oに
平行にz軸をとりそれに垂直にθ軸をとると、N極とS
極の境界線は、例えば、変数zと偏角θの関数z=f
(θ)として表現することができる。
The rotating part 21 has a substantially cylindrical shape rotatable about the central axis O--O, and a magnetizing body 23 made of a permanent magnet is mounted on its circumferential surface. The magnetizer 23 of this example is arranged so that the N poles and S poles of the permanent magnets extend spirally as shown in the figure. That is, the widths of the N pole and the S pole of the permanent magnet in the axial direction on the circumferential surface of the magnetizing body 23 are continuously changed with the central angle around the central axis OO. If the z axis is parallel to the central axis OO on the developed circumferential surface and the θ axis is perpendicular to it, the N pole and S
The boundary line of the pole is, for example, a function z = f of the variable z and the argument θ.
It can be expressed as (θ).

【0052】こうして、発磁体23の円周面によって生
成される信号磁場HS の方向は図示の矢印のように回転
部21の中心軸線O−Oに垂直である。
In this way, the direction of the signal magnetic field H S generated by the circumferential surface of the magnetizing body 23 is perpendicular to the central axis O--O of the rotating portion 21 as indicated by the arrow.

【0053】磁気ヘッド11は、第1の例と同様に、例
えば図5〜図7に示した如く従来の磁気ヘッド11と同
様な形態のものであってよく、バイアス磁場HB を生成
するための永久磁石からなる基板と斯かる基板に装着さ
れた磁気抵抗素子を含む。バイアス磁場HB の方向は基
板の長手方向に整合するように構成され、磁軸(N極と
S極とを結ぶ線)は基板の長手方向に沿っている。
Similar to the first example, the magnetic head 11 may have the same form as the conventional magnetic head 11 as shown in FIGS. 5 to 7, for generating the bias magnetic field H B. And a magnetoresistive element mounted on the substrate. The direction of the bias magnetic field H B is configured to match the longitudinal direction of the substrate, and the magnetic axis (the line connecting the N pole and the S pole) is along the longitudinal direction of the substrate.

【0054】磁気抵抗素子の2つの感磁部は互いに直交
し且つバイアス磁場HB の方向に対して45度の角度を
なすように配置され、更に、基板の長手方向に垂直な中
心線に対して対称に配置されている。
The two magnetic sensitive parts of the magnetoresistive element are arranged so as to be orthogonal to each other and form an angle of 45 degrees with respect to the direction of the bias magnetic field H B , and further, with respect to the center line perpendicular to the longitudinal direction of the substrate. Are arranged symmetrically.

【0055】磁気ヘッド11は発磁体23の円周面上に
て且つそれより隔置されており、基板の長手方向が軸線
方向に沿うように配置されている。更に、磁気ヘッド1
1はバイアス磁場HB の方向が信号磁場HS の方向に直
交するように即ち軸線方向に沿って配置される。こうし
て、磁気ヘッド11の強磁性金属磁気抵抗素子の2つの
感磁部の配向と永久磁石によって生成されるバイアス磁
場HB の方向と回転部21の発磁体23によって生成さ
れる信号磁場HS の方向との間の関係は図3に示した2
つの強磁性金属磁気抵抗素子の配向とバイアス磁場HB
の方向と信号磁場HS の方向との間の関係と同一とな
る。
The magnetic head 11 is arranged on the circumferential surface of the magnetizing body 23 and spaced apart from it, and is arranged such that the longitudinal direction of the substrate is along the axial direction. Furthermore, the magnetic head 1
1 is arranged so that the direction of the bias magnetic field H B is orthogonal to the direction of the signal magnetic field H S , that is, along the axial direction. Thus, the orientation of the two magnetic sensitive parts of the ferromagnetic metal magnetoresistive element of the magnetic head 11, the direction of the bias magnetic field H B generated by the permanent magnet, and the signal magnetic field H S generated by the magnetizer 23 of the rotating part 21 are controlled. The relationship between the directions is shown in FIG.
Orientation of two ferromagnetic metal magnetoresistive elements and bias magnetic field H B
And the direction of the signal magnetic field H S are the same.

【0056】磁気ヘッド11は例えば図5に示した如き
信号検出回路に接続されてよい。こうして、本例による
と回転部21が中心軸線O−O周りに微小角だけ回転す
ると磁気ヘッド11によって検出される信号磁場HS
強さが変化するから、磁気ヘッド11に接続された信号
検出回路の出力端子にて出力電圧が検出される。
The magnetic head 11 may be connected to a signal detection circuit as shown in FIG. 5, for example. Thus, according to this example, when the rotating portion 21 rotates about the central axis O--O by a small angle, the strength of the signal magnetic field H S detected by the magnetic head 11 changes, so that the signal detection connected to the magnetic head 11 is detected. The output voltage is detected at the output terminal of the circuit.

【0057】図2Bは第2の例の角度センサにおいて、
回転部21の回転角度と磁気抵抗素子の出力電圧の関係
を示す。図1Bと同様に、角度変位−出力電圧特性にお
いて、広い角度範囲にて直線性が得られることが判る。
FIG. 2B shows the angle sensor of the second example,
The relationship between the rotation angle of the rotating unit 21 and the output voltage of the magnetoresistive element is shown. As with FIG. 1B, it can be seen that in the angular displacement-output voltage characteristic, linearity can be obtained in a wide angle range.

【0058】図1に示した第1の例と図2に示した第2
の例において、回転部21の発磁体23は強磁性金属の
永久磁石より構成されるが、例えば強磁性金属粉末を含
有するゴムよりなる永久磁石により構成されてよい。ま
た、斯かる回転部21の発磁体23は渦巻き状の又は螺
旋状の2つの永久磁石を接着することによって製造して
よい。
The first example shown in FIG. 1 and the second example shown in FIG.
In the above example, the magnetizing body 23 of the rotating portion 21 is made of a permanent magnet of ferromagnetic metal, but may be made of a permanent magnet made of rubber containing ferromagnetic metal powder, for example. Further, the magnetizing body 23 of the rotating portion 21 may be manufactured by bonding two spiral or spiral permanent magnets.

【0059】以上本発明の実施例について詳細に説明し
てきたが、本発明は上述の実施例に限ることなく本発明
の要旨を逸脱することなく他の種々の構成が採り得るこ
とは当業者にとって容易に理解されよう。
Although the embodiments of the present invention have been described in detail above, those skilled in the art will understand that the present invention is not limited to the above-mentioned embodiments and various other configurations can be adopted without departing from the gist of the present invention. Easy to understand.

【0060】[0060]

【発明の効果】本発明によれば、検出ヘッドに強磁性金
属磁気抵抗素子が使用されているから、温度特性に優れ
た角度センサを提供することができる利点がある。
According to the present invention, since a ferromagnetic metal magnetoresistive element is used in the detection head, there is an advantage that an angle sensor having excellent temperature characteristics can be provided.

【0061】本発明によれば、強磁性金属磁気抵抗素子
を使用した角度センサにおいて、角度変位−出力電圧特
性の直線性を向上させることができる利点がある。
According to the present invention, in the angle sensor using the ferromagnetic metal magnetoresistive element, there is an advantage that the linearity of the angular displacement-output voltage characteristic can be improved.

【0062】本発明によれば、強磁性金属磁気抵抗素子
を使用した角度センサの角度変位−出力電圧特性の直線
性が良好となるから、微小角変位を高い精度にて計測す
ることができる利点がある。
According to the present invention, since the linearity of the angular displacement-output voltage characteristic of the angle sensor using the ferromagnetic metal magnetoresistive element becomes good, it is possible to measure the minute angular displacement with high accuracy. There is.

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

【図1】本発明の角度センサの第1の例を示す図であ
る。
FIG. 1 is a diagram showing a first example of an angle sensor of the present invention.

【図2】本発明の角度センサの第2の例を示す図であ
る。
FIG. 2 is a diagram showing a second example of the angle sensor of the present invention.

【図3】強磁性金属磁気抵抗素子によって変位を検出す
る原理を説明する説明図である。
FIG. 3 is an explanatory diagram illustrating a principle of detecting a displacement by a ferromagnetic metal magnetoresistive element.

【図4】強磁性金属磁気抵抗素子の構成例を示す図であ
る。
FIG. 4 is a diagram showing a configuration example of a ferromagnetic metal magnetoresistive element.

【図5】強磁性金属磁気抵抗素子を使用した変位センサ
の従来例の構成を示す図である。
FIG. 5 is a diagram showing a configuration of a conventional example of a displacement sensor using a ferromagnetic metal magnetoresistive element.

【図6】変位センサの変位−出力電圧特性を改善する従
来例を示す図である。
FIG. 6 is a diagram showing a conventional example for improving displacement-output voltage characteristics of a displacement sensor.

【図7】変位センサの変位−出力電圧特性を改善する他
の従来例を示す図である。
FIG. 7 is a diagram showing another conventional example for improving the displacement-output voltage characteristic of the displacement sensor.

【符号の説明】[Explanation of symbols]

11 磁気ヘッド 21 回転部 23 発磁体 31 強磁性金属磁気抵抗素子 31A、31B 感磁部 35 直流電源 37 出力端子 41 基板 43A、43B 感磁部 45A、45B、45C リード部 47 永久磁石 51 発磁体部 53 検出ヘッド 55 発磁体 57 差動増幅回路 59、61 端子 DESCRIPTION OF SYMBOLS 11 magnetic head 21 rotating part 23 magnetic generator 31 ferromagnetic metal magnetic resistance element 31A, 31B magnetic sensitive part 35 DC power supply 37 output terminal 41 substrate 43A, 43B magnetic sensitive part 45A, 45B, 45C lead part 47 permanent magnet 51 magnetic generator part 53 Detection Head 55 Magnetizer 57 Differential Amplifier Circuit 59, 61 Terminal

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 バイアス磁場を生成するための永久磁石
と強磁性金属の磁気抵抗素子とを含み該磁気抵抗素子は
上記永久磁石の磁軸に直交した線に対して対称的に且つ
その両側にそれぞれ配置された第1の感磁部と第2の感
磁部とを有し上記第1の感磁部と第2の感磁部とは互い
に90度の角度をなし且つ上記永久磁石の磁軸に対して
45度傾斜して配置されるように構成された磁気ヘッド
と、信号磁場を生成するべく中心軸線周りに回転可能な
発磁体と、を有する角度センサにおいて、 上記発磁体は上記信号磁場のベクトルが上記中心軸線周
りの中心角の関数として変化するようにN極とS極が中
心角の関数として変化するように磁化され、 上記磁気ヘッドは上記発磁体より隔置され、上記磁気ヘ
ッドの出力電圧が上記発磁体の回転角度の関数として表
されるように構成されていることを特徴とする角度セン
サ。
1. A permanent magnet for generating a bias magnetic field and a magnetoresistive element made of a ferromagnetic metal, the magnetoresistive element being symmetrical with respect to a line orthogonal to the magnetic axis of the permanent magnet and on both sides thereof. A first magnetism sensitive portion and a second magnetism sensitive portion which are arranged respectively, and the first magnetism sensitive portion and the second magnetism sensitive portion form an angle of 90 degrees with each other and the magnetism of the permanent magnet. In an angle sensor having a magnetic head configured to be arranged at an angle of 45 degrees with respect to an axis and a magnetizing body rotatable about a central axis to generate a signal magnetic field, the magnetizing body is the signal The magnetic pole is magnetized so that the N pole and the S pole change as a function of the central angle so that the vector of the magnetic field changes as a function of the central angle around the central axis, and the magnetic head is spaced apart from the magnet body. The output voltage of the head depends on the rotation angle of the magnet. An angle sensor, characterized in that it is configured to be expressed as a number.
【請求項2】 請求項1記載の角度センサにおいて、 上記発磁体は上記中心軸線に垂直な円形面を有し、該円
形面はN極とS極の半径方向の寸法が上記中心軸線周り
の中心角の関数として変化し上記信号磁場の方向が上記
中心軸線に平行となるように磁化され、 上記磁気ヘッドは上記発磁体の円形面より隔置され且つ
上記バイアス磁場の方向が上記信号磁場の方向に直交す
るよう上記中心軸線に直交するように配置されているこ
とを特徴とする角度センサ。
2. The angle sensor according to claim 1, wherein the magnetizing body has a circular surface perpendicular to the central axis, and the circular surface has N and S poles in radial directions around the central axis. The direction of the signal magnetic field changes as a function of the central angle and is magnetized so that the direction of the signal magnetic field is parallel to the central axis, the magnetic head is spaced from the circular surface of the magnetizer, and the direction of the bias magnetic field is the direction of the signal magnetic field. An angle sensor, wherein the angle sensor is arranged so as to be orthogonal to the direction and orthogonal to the central axis.
【請求項3】 請求項1記載の角度センサにおいて、 上記発磁体は上記中心軸線に平行な円周面を有し、該円
周面はN極とS極の軸線方向の寸法が上記中心軸線周り
の中心角の関数として変化し上記信号磁場の方向が上記
中心軸線に直交するように磁化され、 上記磁気ヘッドは上記発磁体の円周面より隔置され且つ
上記バイアス磁場の方向が上記信号磁場の方向に直交す
るよう上記中心軸線に平行になるように配置されている
ことを特徴とする角度センサ。
3. The angle sensor according to claim 1, wherein the magnetizing body has a circumferential surface parallel to the central axis, and the circumferential surface has N and S poles in the axial direction. The direction of the signal magnetic field changes as a function of the surrounding central angle and is magnetized so that the direction of the signal magnetic field is orthogonal to the central axis, the magnetic head is spaced from the circumferential surface of the magnet body, and the direction of the bias magnetic field is the signal. An angle sensor, which is arranged so as to be orthogonal to the direction of the magnetic field and parallel to the central axis.
JP29729492A 1992-11-06 1992-11-06 Angle sensor Pending JPH06147816A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29729492A JPH06147816A (en) 1992-11-06 1992-11-06 Angle sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29729492A JPH06147816A (en) 1992-11-06 1992-11-06 Angle sensor

Publications (1)

Publication Number Publication Date
JPH06147816A true JPH06147816A (en) 1994-05-27

Family

ID=17844651

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29729492A Pending JPH06147816A (en) 1992-11-06 1992-11-06 Angle sensor

Country Status (1)

Country Link
JP (1) JPH06147816A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102005055905A1 (en) * 2005-11-22 2007-05-24 Continental Teves Ag & Co. Ohg Length measuring arrangement for use in e.g. vehicle position sensor, has encoder with magnetic field that symmetrically runs between arrangements, where field line run has variation with respect to measuring direction over measuring area
JP2013205141A (en) * 2012-03-28 2013-10-07 Honda Motor Co Ltd Throttle opening detector
JP2015034822A (en) * 2014-09-09 2015-02-19 本田技研工業株式会社 Throttle aperture detector
JP2017161365A (en) * 2016-03-09 2017-09-14 Tdk株式会社 Magnet and displacement detector
CN115406340A (en) * 2022-08-19 2022-11-29 Oppo广东移动通信有限公司 Displacement measurement mechanism, shell assembly and electronic equipment

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102005055905A1 (en) * 2005-11-22 2007-05-24 Continental Teves Ag & Co. Ohg Length measuring arrangement for use in e.g. vehicle position sensor, has encoder with magnetic field that symmetrically runs between arrangements, where field line run has variation with respect to measuring direction over measuring area
DE102005055905B4 (en) * 2005-11-22 2016-10-27 Continental Teves Ag & Co. Ohg Length measurement arrangement with a magnetic scale with opposite magnetization
JP2013205141A (en) * 2012-03-28 2013-10-07 Honda Motor Co Ltd Throttle opening detector
JP2015034822A (en) * 2014-09-09 2015-02-19 本田技研工業株式会社 Throttle aperture detector
JP2017161365A (en) * 2016-03-09 2017-09-14 Tdk株式会社 Magnet and displacement detector
CN107179093A (en) * 2016-03-09 2017-09-19 Tdk株式会社 Magnet and displacement detector
US10401195B2 (en) 2016-03-09 2019-09-03 Tdk Corporation Magnet and displacement detection unit
CN115406340A (en) * 2022-08-19 2022-11-29 Oppo广东移动通信有限公司 Displacement measurement mechanism, shell assembly and electronic equipment

Similar Documents

Publication Publication Date Title
JP3529784B2 (en) Sensor using magnetoresistive element
US6107793A (en) Magnetic sensing device unaffected by positioning error of magnetic field sensing elements
US7141967B2 (en) Sensor arrangement
JP4907770B2 (en) Position encoder using fluxgate sensor
US7208940B2 (en) 360-Degree magnetoresistive rotary position sensor
EP3550269A1 (en) System for measuring angular position and method of stray field cancellation
JP2796391B2 (en) Physical quantity detection method and physical quantity detection device, servo motor using these methods and devices, and power steering device using this servo motor
US4875008A (en) Device for sensing the angular position of a shaft
JPH06147816A (en) Angle sensor
JPH0720218A (en) Magnetic sensor
JPH10239098A (en) Magnetic detector
JPH0426047B2 (en)
JPS58201041A (en) Device for detecting tension of tape
JPS5815113A (en) Measuring device for number of teeth
JP2550049B2 (en) Device that magnetically detects position and speed
JPH03226625A (en) Rotation positioner
JPH081387B2 (en) Magnetic sensor
JP2556851B2 (en) Magnetoresistive element
JPH10255236A (en) Magnetism detecting apparatus
JP3009274B2 (en) Angle detector
JP3067484B2 (en) Magnetic position and rotation detection element
JPS5841448Y2 (en) magnetically sensitive element
JPH06147817A (en) Angle sensor
JP2576136B2 (en) Magnetic direction measurement device
JPS6111982Y2 (en)