JPS63204113A - Magnetoelectric converter element - Google Patents

Magnetoelectric converter element

Info

Publication number
JPS63204113A
JPS63204113A JP3539887A JP3539887A JPS63204113A JP S63204113 A JPS63204113 A JP S63204113A JP 3539887 A JP3539887 A JP 3539887A JP 3539887 A JP3539887 A JP 3539887A JP S63204113 A JPS63204113 A JP S63204113A
Authority
JP
Japan
Prior art keywords
pitch
lambda
magnetic flux
flux supply
substrate
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
JP3539887A
Other languages
Japanese (ja)
Inventor
Ichiro Izawa
一朗 伊澤
Toshikazu Arasuna
荒砂 俊和
Yoshi Yoshino
吉野 好
Kenichi Ao
建一 青
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 JP3539887A priority Critical patent/JPS63204113A/en
Publication of JPS63204113A publication Critical patent/JPS63204113A/en
Pending legal-status Critical Current

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  • Transmission And Conversion Of Sensor Element Output (AREA)

Abstract

PURPOSE:To eliminate the pitch shift of electric output, by mounting a substrate arranged in almost parallel to the circumferential contact surface of a ring- shaped flux supply body and a plurality of a magnetism-sensitive resistor patterns mounted on the substrate in almost parallel to the flux supply body. CONSTITUTION:A magnetoelectric converter element 2 is used so as to make a pair along with a ring-shaped multipolar magnet 1 wherein m-pieces of poles are magnetized to the circumferential surface thereof at an equal pitch lambda and arranged in parallel to the circumferential contact surface of the magnet 1. The magnetoelectric converter element 2 is constituted so that magnetism- sensitive resistor patterns 3, 4 each formed of a membrane composed of a ferromagnetic material having the anisotropic effect of magnetic resistance such as NiCo or NiFe are formed to the surface of a planar insulating substrate 10 by vapor-depositing of the ferromagnetic material in a rectangular shape. When the pitch of the resistor patterns 3, 4 is set to lambda', the pitch lambda' is shift so as to become a range of lambda/n>lambda'>=lambda/2n with respect to the magnetizing pitch lambda. Herein, (n) is the number of the magnetism-sensitive resistor patterns.

Description

【発明の詳細な説明】 「産業上の利用分野」 本発明は、繰り返し磁気信号の検出に用いる磁電変換素
子の構造に関する。
DETAILED DESCRIPTION OF THE INVENTION "Field of Industrial Application" The present invention relates to the structure of a magnetoelectric transducer used for detecting repetitive magnetic signals.

「従来の技術」 従来のリング状多極磁石を磁束供給体とする磁電変換素
子は、多極磁石の着磁ピッチλに対して、感磁抵抗パタ
ーンがn個ある場合には、それぞれの感磁抵抗パターン
をλ/nのピッチで基板に配置し、多極磁石の一回転に
対しその磁石の着磁個数mの整数倍の電気出力を得る構
造を採っている。
``Prior art'' A magnetoelectric transducer using a conventional ring-shaped multipolar magnet as a magnetic flux supplying body has a magnetoelectric transducer that has n magnetic resistance patterns for each magnetization pitch λ of the multipolar magnet. Magnetoresistive patterns are arranged on the substrate at a pitch of λ/n, and a structure is adopted in which an electrical output that is an integral multiple of the number m of magnetized magnets is obtained for one rotation of the multipolar magnet.

ところが、この構造では基板が平面であるのに対して、
リング状多極磁石の着磁部は曲面であることから、感磁
抵抗パターンの中央部の抵抗パターンと端部の抵抗パタ
ーンとで磁束の受は方が異なり、電気出力がピッチずれ
を起こすという欠点を有していた。
However, while the substrate in this structure is flat,
Since the magnetized part of a ring-shaped multipolar magnet is a curved surface, the magnetic flux is received differently by the resistance pattern at the center and the resistance pattern at the ends of the magneto-sensitive resistance pattern, causing a pitch shift in the electrical output. It had drawbacks.

「発明が解決しようとする問題点」 本発明は、前述した欠点をなくし、電気出力のピッチず
れがない磁電変換素子を提供することを目的とする。
"Problems to be Solved by the Invention" An object of the present invention is to eliminate the above-mentioned drawbacks and to provide a magnetoelectric conversion element without pitch deviation of electric output.

「間転点を解決するための手段」 しかして、本発明によれば、円周面に略等ピッチλで任
意様の磁束供給部をもつ環状磁束供給体と一対に使用す
る磁電変換素子において、前記環状磁束供給体の円周接
面に略平行に配置する基板と、該基板に、前記磁束供給
部と略平行に複数本(n本)具備された感磁抵抗パター
ンとを具備するとともに、該感磁抵抗パターンのうち、
少なくとも2本の感磁抵抗パターンのピッチλ’を、λ
/n〉^゛≧^7/2nの範囲に配置することを特徴と
する磁電変換素子が提供される。
"Means for Solving Interchange Points" According to the present invention, in a magneto-electric transducer used in a pair with an annular magnetic flux supply body having arbitrary magnetic flux supply parts at approximately equal pitch λ on the circumferential surface. , comprising a substrate disposed substantially parallel to a circumferential surface of the annular magnetic flux supply body, and a plurality (n) of magnetosensitive resistance patterns provided on the substrate substantially parallel to the magnetic flux supply section; , of the magneto-sensitive resistance pattern,
The pitch λ' of at least two magneto-sensitive resistance patterns is set to λ
Provided is a magnetoelectric transducer characterized in that it is arranged in a range of /n>^゛≧^7/2n.

「作用」 上記構成によれば、環状磁束供給体の円周面における磁
束供給部から平面状配置の感磁抵抗パターンに直角方向
に供給される磁束が、いずれの感磁抵抗パターンに対し
ても略均等に加わる。
"Operation" According to the above configuration, the magnetic flux supplied from the magnetic flux supply part on the circumferential surface of the annular magnetic flux supplier in the direction perpendicular to the magneto-sensitive resistance patterns arranged in a planar manner is applied to any of the magneto-sensitive resistance patterns. Approximately evenly distributed.

「実施例」 次に、本発明の実施例を第1図から第3図について説明
する。
"Example" Next, an example of the present invention will be described with reference to FIGS. 1 to 3.

本実施例の磁電変換素子2は、第1図に示すように、円
周面に^の等ピッチでm極着磁されたリング状多極磁石
1と一対に使用され、この磁石1の円周接面に平行に配
置されている。磁電変換素子2は、第2図に示すごとく
平面状の絶縁性基板10の表面に、ニッケルコバルトあ
るいはニッケル鉄のような磁気抵抗の異方性効果を有す
る強磁性体の薄膜による感磁抵抗パターン3.4を形成
したものである。この感磁抵抗パターン3,4は強磁性
体を矩形状あるいは櫛歯パターン状に蒸着し、又は全面
に蒸着した後エツチングして形成される。そして、感磁
抵抗パターン3.4を飽和磁化させるに充分な強さの磁
束を垂直方向に加えると各抵抗パターン3,4の抵抗値
が変化し、リング状多極磁石1の一回転に対しその磁石
1の着磁個数mの整数倍(本実施例では2倍)のパルス
出力が得られる。第2図に示すように、抵抗パターン3
.4のピッチをλ′とするとき、このλ′は磁石1の着
磁ピッチλに対して次式の範囲になるようにずらしであ
る。
As shown in FIG. 1, the magnetoelectric conversion element 2 of this embodiment is used in a pair with a ring-shaped multipolar magnet 1, which is magnetized with m poles on the circumferential surface at an equal pitch of ^. It is arranged parallel to the circumferential surface. As shown in FIG. 2, the magnetoelectric transducer 2 has a magnetoresistive pattern formed on the surface of a planar insulating substrate 10 by a thin film of a ferromagnetic material such as nickel cobalt or nickel iron that has an anisotropic effect of magnetoresistive resistance. 3.4 was formed. The magneto-sensitive resistance patterns 3 and 4 are formed by depositing a ferromagnetic material in a rectangular or comb-teeth pattern, or by depositing it on the entire surface and then etching it. When a magnetic flux strong enough to saturate the magneto-sensitive resistance patterns 3.4 is applied in the vertical direction, the resistance value of each resistance pattern 3, 4 changes, and for one rotation of the ring-shaped multipolar magnet 1, the resistance value of each resistance pattern 3, 4 changes. A pulse output that is an integral multiple (in this embodiment, twice) of the number m of magnetized magnets 1 can be obtained. As shown in Figure 2, resistance pattern 3
.. When the pitch of magnet 1 is λ', λ' is shifted from the magnetization pitch λ of magnet 1 so that it falls within the range of the following equation.

λ/4≦λ“くλ/2 ・・・・・(n)すなわち、第
3図に示すように円周面着磁のリ−3= ング状多極磁石1の磁束を平面状の磁電変換素子2で受
けることから、感磁抵抗パターン4が垂直磁束Φを受け
る時の磁石1の極(例えばN極)の位置は、疑似的に着
磁ピッチ^が小さくなる方向に中心角でΔθだけずれる
ことになる。そのため、抵抗パターン3,4のピッチλ
′をλ/2(着磁ピッチの1/2)より小さくすること
でこのずれΔθを補正するようにしである。但し、抵抗
パターン3.4のピッチλ°が着磁ピッチλの1/4よ
り小さい範囲に入る領域においては磁石1と、各々の抵
抗パターン3,4の距離が離れすぎる為抵抗値変化に歪
みを生じ波形整形後の出力パルス波形がバラツクため、
現実的ではない。よって、(n)式のごとくピッチλ′
は着磁ピッチλの1/4以上に大きくしな。
λ/4≦λ" λ/2 (n) In other words, as shown in Fig. 3, the magnetic flux of the ring-shaped multipolar magnet 1 is transferred to the magnetic flux of the ring-shaped multipolar magnet 1. Since the magnetic flux is received by the conversion element 2, the position of the pole (for example, the N pole) of the magnet 1 when the magnetosensitive resistance pattern 4 receives the vertical magnetic flux Φ is Δθ at the central angle in the direction in which the pseudo magnetization pitch ^ becomes smaller. Therefore, the pitch of resistor patterns 3 and 4 is λ
This deviation Δθ is corrected by making ′ smaller than λ/2 (1/2 of the magnetized pitch). However, in a region where the pitch λ° of the resistor patterns 3.4 is smaller than 1/4 of the magnetization pitch λ, the distance between the magnet 1 and each resistor pattern 3, 4 is too far, causing distortion in the resistance value change. This causes variations in the output pulse waveform after waveform shaping.
It's not realistic. Therefore, as shown in equation (n), the pitch λ′
should be larger than 1/4 of the magnetization pitch λ.

本発明者は、(n〉式の範囲で抵抗パターン3゜4をの
ピッチλ′を適切に選ぶことにより、第4図(a) 、
 (b)に示すように、従来、波形整形後のパルス周期
t/Tのずれが約5%であったのが、本実施例により約
1%にまで改善することができた。
By appropriately selecting the pitch λ' of the resistor pattern 3°4 within the range of (n>), the present inventor succeeded in obtaining the results shown in FIG. 4(a),
As shown in (b), conventionally, the difference in pulse period t/T after waveform shaping was about 5%, but this embodiment was able to improve it to about 1%.

[他の実施例」 抵抗パターンを4本とした場合の磁電変換素子の構成を
第5図および第6図に示す。この場合は、磁電変換素子
中央部の抵抗パターン4.5のピッチはλ/4とし、素
子端部の抵抗パターン3,4および5,6のピッチはλ
°としである。ここでピッチλ′は次式の範囲にある。
[Other Embodiments] FIGS. 5 and 6 show the configuration of a magnetoelectric transducer with four resistance patterns. In this case, the pitch of the resistance patterns 4.5 at the center of the magnetoelectric conversion element is λ/4, and the pitch of the resistance patterns 3, 4 and 5, 6 at the end of the element is λ/4.
°It's Toshishita. Here, the pitch λ' is within the range of the following equation.

λ/8≦λ′くλ/4・・・・・(2)但しこの場合で
も、抵抗パターン4,5のピッチをλ/4より小さい値
λ”としてもよく、この時はλ′、λ′′の範囲は(3
)式となる。
λ/8≦λ' λ/4 (2) However, even in this case, the pitch of the resistor patterns 4 and 5 may be set to a value λ" smaller than λ/4, and in this case, λ', λ The range of '' is (3
).

λ/8≦λ′≦λ″≦λ/4・・・(3)抵抗パターン
がn本(4本以上)の場合も同様に抵抗パターンRIR
2のピッチをλ′1・・・Rn−1−Rnのピッチをλ
′n−4とすると、ピッチλ’・・・λ′n−1は次式
の範囲にある。
λ/8≦λ′≦λ″≦λ/4...(3) Similarly, when there are n resistance patterns (4 or more), the resistance pattern RIR
The pitch of 2 is λ'1...The pitch of Rn-1-Rn is λ
'n-4, the pitches λ'...λ'n-1 are within the range of the following equation.

λ/ 2 n≦λ°1−λ′n−1≦λ°2−λ″n−
2≦・・・・・・(4) また、第7図に示すような磁性体ギア20およびバイア
ス磁石30から構成される環状磁束供給体を持つ回転検
出装置の磁電変換素子2にも本発明は同様に実施するこ
とができる。
λ/2 n≦λ°1−λ′n−1≦λ°2−λ″n−
2≦...(4) The present invention can also be applied to the magnetoelectric transducer 2 of a rotation detecting device having an annular magnetic flux supply body composed of a magnetic gear 20 and a bias magnet 30 as shown in FIG. can be implemented similarly.

「効果」 以上述べたように、本発明の磁電変換素子は上記の構成
を有するものであり、環状磁束供給体の円周面における
磁束供給部から平面状配置の感磁抵抗パターンに直角方
向に供給される磁束が、いずれの感磁抵抗パターンに対
しても略均等に加わるため、電気出力のピッチずれがな
いという優れた効果がある。
"Effects" As described above, the magnetoelectric transducer of the present invention has the above configuration, and the magnetic flux supply section on the circumferential surface of the annular magnetic flux supply body extends in the direction perpendicular to the magnetosensitive resistance pattern arranged in a planar manner. Since the supplied magnetic flux is applied substantially equally to all magnetosensitive resistance patterns, there is an excellent effect that there is no pitch shift in the electrical output.

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

第1図は本発明の実施例を示す斜視図、第2図は第1図
のA規正面図、第3図は第1図のB幌上面図、第4図は
実験結果を示す波形図、第5図および第6図は他の実施
例を示す正面図および上面図、第7図は更に他の実施例
を示す斜視図である。 115.リング状多極磁石、 211.磁電変換素子、
3〜611.感磁抵抗パターン、 10.、、基板、2
0 、、、磁性体ギヤ、 30 、、、バイアス磁石。 第1図 B視 1・・・・リング状多極磁石 2・−・・磁電変換素子 第2図 1−−−・リング状多極磁石 2−−−一磁電変換素子 3.4−・・−感磁抵抗パターン 10−・−基板 第5図 S                  N、¥  −
λ′ 第6図 2−−−一磁電変換素子 3〜6・−感磁抵抗パターン 第 70 1−−一−リング状多極磁石 2・−・磁電変換素子
Fig. 1 is a perspective view showing an embodiment of the present invention, Fig. 2 is a front view of the A standard in Fig. 1, Fig. 3 is a top view of the B hood in Fig. 1, and Fig. 4 is a waveform diagram showing experimental results. , FIG. 5 and FIG. 6 are front and top views showing another embodiment, and FIG. 7 is a perspective view showing still another embodiment. 115. Ring-shaped multipolar magnet, 211. magnetoelectric conversion element,
3-611. Magnetoresistance pattern, 10. ,,substrate,2
0, , Magnetic gear, 30, , Bias magnet. Fig. 1 B view 1... Ring-shaped multipolar magnet 2... Magnetoelectric conversion element Fig. 2 1-- Ring-shaped multipolar magnet 2---One magnetoelectric conversion element 3.4... - Magnetoresistance pattern 10 - - Substrate Figure 5 S N, ¥ -
λ' Fig. 6 2--One magnetoelectric conversion element 3 to 6 - Magneto-sensitive resistance pattern No. 70 1--One ring-shaped multipolar magnet 2 - Magnetoelectric conversion element

Claims (1)

【特許請求の範囲】  円周面に略等ピッチλで任意極の磁束供給部をもつ環
状磁束供給体と一対に使用する磁電変換素子において、 前記環状磁束供給体の円周接面に略平行に配置する基板
と、 該基板に、前記磁束供給部と略平行に複数本(n本)具
備された感磁抵抗パターンとを具備するとともに、 該感磁抵抗パターンのうち、少なくとも2本の感磁抵抗
パターンのピッチλ’を、λ/n>λ’≧λ/2nの範
囲で配置することを特徴とする磁電変換素子。
[Scope of Claims] In a magnetoelectric transducer used in a pair with an annular magnetic flux supply body having magnetic flux supply parts of arbitrary poles at approximately equal pitches λ on a circumferential surface, substantially parallel to the circumferential contact surface of the annular magnetic flux supply body. a substrate disposed in the magneto-sensitive resistance pattern; and a plurality (n) magneto-sensitive resistance patterns provided on the substrate substantially parallel to the magnetic flux supply section, and at least two of the magneto-sensitive resistance patterns A magnetoelectric transducer characterized in that the pitch λ' of the magnetoresistive pattern is arranged in the range λ/n>λ'≧λ/2n.
JP3539887A 1987-02-18 1987-02-18 Magnetoelectric converter element Pending JPS63204113A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3539887A JPS63204113A (en) 1987-02-18 1987-02-18 Magnetoelectric converter element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3539887A JPS63204113A (en) 1987-02-18 1987-02-18 Magnetoelectric converter element

Publications (1)

Publication Number Publication Date
JPS63204113A true JPS63204113A (en) 1988-08-23

Family

ID=12440808

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3539887A Pending JPS63204113A (en) 1987-02-18 1987-02-18 Magnetoelectric converter element

Country Status (1)

Country Link
JP (1) JPS63204113A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5918458A (en) * 1982-07-23 1984-01-30 Nippon Denso Co Ltd Rotation detector
JPS61182505A (en) * 1985-02-08 1986-08-15 Hitachi Ltd Crank angle sensor

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5918458A (en) * 1982-07-23 1984-01-30 Nippon Denso Co Ltd Rotation detector
JPS61182505A (en) * 1985-02-08 1986-08-15 Hitachi Ltd Crank angle sensor

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