JPH022086B2 - - Google Patents
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- Publication number
- JPH022086B2 JPH022086B2 JP54029208A JP2920879A JPH022086B2 JP H022086 B2 JPH022086 B2 JP H022086B2 JP 54029208 A JP54029208 A JP 54029208A JP 2920879 A JP2920879 A JP 2920879A JP H022086 B2 JPH022086 B2 JP H022086B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- magnetic
- signal
- bias
- magnetoresistive element
- 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 - Lifetime
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- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Transmission And Conversion Of Sensor Element Output (AREA)
Description
【発明の詳細な説明】
本発明は、回転軸に取り付けられ磁気記憶媒体
を有する円板に、等間隔のビツト長を有する磁化
の形で記録されている磁気信号を、強磁性体薄膜
磁気抵抗効果素子より成る磁気センサーで、読み
取ることにより、前記回転軸の回転角を検知する
角度検出器に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention utilizes a ferromagnetic thin film magnetoresistive system to transfer a magnetic signal recorded in the form of magnetization having equally spaced bit lengths to a disk attached to a rotating shaft and having a magnetic storage medium. The present invention relates to an angle detector that detects the rotation angle of the rotating shaft by reading it with a magnetic sensor comprising an effect element.
従来、この種の角度検出器においては、回転軸
の回転角度検出は、前記回転軸の回転に伴つて前
記円板から生じる信号磁界の変化を、磁気抵抗効
果素子の電気抵抗の変化として直接読み取ること
によりなされていた。ここで、信号磁界による磁
気抵抗効果素子の抵抗変化量は、その抵抗値の数
パーセント程度であり、角度位置信号出力として
は、この抵抗変化分だけを、回転軸の回転速度に
よらず静止時から高速回転時迄、正確に検出する
必要がある。従つて、角度位置検出方法として通
常は、前記磁気抵抗効果素子をブリツジ状に構成
し、この差動出力を広帯域の直流増幅層で増幅
し、しかる後、所望の位置信号に整形する方法が
とられている。この角度検出器において、安定な
動作を得るために肝要なことは、ブリツジを構成
する磁気抵抗効果素子の抵抗値のバラツキによつ
て生じる直流オフセツト電圧及び直流増幅器のオ
フセツト電圧を信号出力電圧に比べて極めて小さ
くすることである。しかし、このブリツジのオフ
セツト電圧が極めて小さくなる様に、磁気抵抗効
果素子の作製するには、精密なプロセスコントロ
ールが要求され、又オフセツト電圧の低い直流増
幅器は高価であるので、従来の構成では、高性能
で、低価格な角度検出器は得られなかつた。 Conventionally, in this type of angle detector, the rotation angle of the rotating shaft is detected by directly reading the change in the signal magnetic field generated from the disk as the rotating shaft rotates as a change in the electrical resistance of the magnetoresistive element. This was done by Here, the amount of resistance change of the magnetoresistive element due to the signal magnetic field is about a few percent of its resistance value, and the angular position signal output is based on only this resistance change, regardless of the rotation speed of the rotating shaft. Accurate detection is required from the start to high-speed rotation. Therefore, the usual angular position detection method is to configure the magnetoresistive element in a bridge shape, amplify this differential output with a broadband DC amplification layer, and then shape it into a desired position signal. It is being In order to obtain stable operation in this angle detector, it is important to compare the DC offset voltage caused by variations in the resistance values of the magnetoresistive elements that make up the bridge and the offset voltage of the DC amplifier with the signal output voltage. The goal is to make it extremely small. However, in order to manufacture a magnetoresistive element so that the offset voltage of this bridge is extremely small, precise process control is required, and a DC amplifier with a low offset voltage is expensive, so in the conventional configuration, A high-performance, low-cost angle detector could not be obtained.
本発明の目的は、上記欠点を解決した高性能で
安価な角度検出器を提供することにある。本発明
の特徴は、角度位置情報発生源としての磁気記憶
媒体とこの位置情報の磁気センサーとして強磁性
磁気抵抗効果素子とを組み合せた角度検出器にお
いて、上記構成要素のほかに、磁気センサーへの
微小振幅交流バイアス磁界印加手段と振幅復調回
路を設けて、角度位置信号磁界を交流バイアス磁
界を搬送波として振幅変調された形で交流的に検
出し復調する全く新しい方法により、従来の直流
的な信号磁界検出方式で最大の問題となつていた
直流オフセツト電圧に起因する欠点を克服でき、
その結果、高性能で低価格な角度検出器を実現で
きることにある。 An object of the present invention is to provide a high-performance and inexpensive angle detector that solves the above-mentioned drawbacks. A feature of the present invention is that in an angle detector that combines a magnetic storage medium as a source of angular position information and a ferromagnetic magnetoresistive element as a magnetic sensor for this position information, in addition to the above-mentioned components, A completely new method of detecting and demodulating the angular position signal magnetic field in an amplitude-modulated form using the AC bias magnetic field as a carrier wave by installing a minute amplitude AC bias magnetic field applying means and an amplitude demodulation circuit, it is possible to detect and demodulate the angular position signal magnetic field in an AC manner using the AC bias magnetic field as a carrier wave. It can overcome the drawbacks caused by DC offset voltage, which was the biggest problem with magnetic field detection methods, and
As a result, a high-performance, low-cost angle detector can be realized.
すなわち、本発明の構成は、回転体の回転軸に
取り付けられ、磁気信号が円周に沿つて等間隔の
ビツト長を有する磁化の形で記録されている磁気
記憶媒体を有する円板と、前記回転軸の前記に伴
つて前記円板から生じる磁界の変化を電気抵抗の
変化として感知できる様に配置された強磁性薄膜
磁気抵抗効果素子より成る磁気センサーと、この
磁気センサーへの微小交流バイアス磁界印加手段
と、前記磁気センサーの駆動回路と、前記磁気セ
ンサーの出力信号を増巾する増巾回路と、この増
巾回路出力波形を整流して積分する振幅復調回路
と、この振幅復調回路出力をパルス化するコンパ
レータとから成る。 That is, the configuration of the present invention includes a disk having a magnetic storage medium attached to the rotating shaft of a rotating body and in which magnetic signals are recorded in the form of magnetization having bit lengths at equal intervals along the circumference; A magnetic sensor consisting of a ferromagnetic thin film magnetoresistive element arranged so as to be able to sense changes in the magnetic field generated from the disk as a change in electrical resistance as the rotating shaft moves forward, and a minute alternating current bias magnetic field applied to the magnetic sensor. an application means, a drive circuit for the magnetic sensor, an amplification circuit for amplifying the output signal of the magnetic sensor, an amplitude demodulation circuit for rectifying and integrating the output waveform of the amplification circuit, and an amplitude demodulation circuit for rectifying and integrating the output signal of the amplitude demodulation circuit. It consists of a comparator that pulses.
磁気抵抗効果素子へ交流バイアス磁界を印加し
て再生する方式、IEEETransacion on Audio、
Vol Au−13No.2、March1965、P41〜43に示さ
れている。 A method for reproducing by applying an alternating current bias magnetic field to a magnetoresistive element, IEEETransacion on Audio,
It is shown in Vol Au-13 No. 2, March 1965, P41-43.
これは、信号磁界に比べて大きな振幅を有する
交流バイアス磁界を印加して、信号磁界を検知し
このバイアス磁界の向きが逆の時の出力振幅エン
ベロープの差を信号として再生するもので、これ
と全く同一原理に基づく例として特開昭53−
57810号、又この方式をを発展させた例として米
国特許第3979775号等が報告されている。しかし、
この方式では原理上、交流バイアス磁界の強度を
信号磁界に比べて大きくする必要があるので、発
熱に起因する種々の問題を生じ易く、又信号磁界
発生源を減磁する等の欠点を有する。 This applies an AC bias magnetic field with a larger amplitude than the signal magnetic field, detects the signal magnetic field, and reproduces as a signal the difference in the output amplitude envelope when the bias magnetic field is in the opposite direction. As an example based on the exact same principle, JP-A-53-
No. 57810, and U.S. Pat. No. 3,979,775 as an example of developing this method have been reported. but,
In principle, this method requires the strength of the AC bias magnetic field to be greater than that of the signal magnetic field, so it tends to cause various problems due to heat generation, and has drawbacks such as demagnetization of the signal magnetic field generation source.
本発明の再生原理によれば、以上の様な欠点を
容易に改善できる。 According to the regeneration principle of the present invention, the above-mentioned drawbacks can be easily improved.
まず本発明の特徴をなす強磁性磁気抵抗効果素
子への微小振幅交流バイアス磁界印加による磁気
信号磁界検知の原理を第1図を用いて説明する。
1は強磁性磁気抵抗効果素子のストライプ幅方向
印加磁界Hとその磁気抵抗効果素子の抵抗変化量
ΔRとの関係を示したものである。この両者の関
係は、周知の如く、印加磁界Hの大きさが、飽和
磁界Hoを越えない範囲(|H|<Ho)では近似
的に
ΔR∝H2 ……
と表わされる。従つて
|∂ΔF/∂H|∝|H| ……
が成り立つ。これは、磁気抵抗効果素子にある信
号磁界Hを中心にして、微小振幅の交流磁界を印
加した時の、ΔRの変化量が、信号磁界Hの大き
さに比例することを示す。例えば、磁気抵抗効果
素子に微小振幅の交流バイアス磁界2を加えなが
ら信号磁界を検出する場合、信号磁界H1,H2及
びH3に対して、それぞれ信号磁界の大きさにほ
ぼ比例した大きさ交流的なΔRの変化3,4及び
5を生じる。このΔRの変化を、磁気抵抗効果素
子に流す電流を介して電圧の変化に直すことによ
り、磁気抵抗効果素子からは、出力信号としての
信号磁界の大きさに比例した大きさの交流出力電
圧を生じる。 First, the principle of detecting a magnetic signal magnetic field by applying a minute amplitude AC bias magnetic field to a ferromagnetic magnetoresistive element, which is a feature of the present invention, will be explained with reference to FIG.
1 shows the relationship between the magnetic field H applied in the stripe width direction of the ferromagnetic magnetoresistive element and the resistance change amount ΔR of the magnetoresistive element. As is well known, the relationship between the two is approximately expressed as ΔR∝H 2 . . . in a range where the magnitude of the applied magnetic field H does not exceed the saturation magnetic field Ho (|H|<Ho). Therefore, |∂ΔF/∂H|∝|H|... holds true. This shows that the amount of change in ΔR is proportional to the magnitude of the signal magnetic field H when an alternating current magnetic field of minute amplitude is applied to the magnetoresistive element, centering on the signal magnetic field H. For example, when detecting a signal magnetic field while applying a minute amplitude AC bias magnetic field 2 to the magnetoresistive element, the signal magnetic fields H 1 , H 2 and H 3 each have a magnitude approximately proportional to the magnitude of the signal magnetic field. This produces alternating current ΔR changes 3, 4 and 5. By converting this change in ΔR into a change in voltage via a current flowing through the magnetoresistive element, the magnetoresistive element generates an AC output voltage proportional to the magnitude of the signal magnetic field as an output signal. arise.
本発明の再生方式は、従来の交流バイアス磁界
印加方式と比べて、交流バイアス磁界強度が微小
であるので、信号磁界発生源の特性に影響を与え
ないこと及び交流バイアス磁界印加手段の構成が
容易であること等の利点を有する。 In the reproduction method of the present invention, the AC bias magnetic field strength is minute compared to the conventional AC bias magnetic field application method, so it does not affect the characteristics of the signal magnetic field generation source and the AC bias magnetic field application means can be easily configured. It has advantages such as:
次に本発明の実施例について第2図、第3図お
よび第4図を参照して説明する。第2図は、本発
明の一実施例を基本機能に着目して模式的に示し
たものである。回転体の回転軸6に取り付けら
れ、磁気信号が円周に沿つて等間隔のビツト長L
の磁化7の形で記録されている磁気記憶媒体9を
有する円板10と、前記回転軸6の回転に伴つて
生じる磁気信号8の変化を電気抵抗の変化として
感知できる様に配置された磁気センサー11と、
この磁気センサー11へ微小交流バイアス磁界1
6を記憶する手段17と、前記磁気センサー11
の磁気抵抗効果素子へ一定電流を供給する定電流
回路等の駆動回路18と、磁気センサー11の出
力信号19,20,21,22を増巾する増巾回
路24と、この増巾回路出力波形の直流オフセツ
ト電圧をカツトし整流して、積分する振幅復調回
路25と、この振幅復調回路出力をパルス化され
た、角度位置信号27,28と17として取り出
すコンパレータ26とを含む。ここで磁気センサ
ー11は、長手方向に一軸異方性を有するストラ
イプ状の4本の強磁性磁気抵抗効果素子12,1
3,14,15が互いに、1/4Lのピツチで形成
されたものから成り、磁気記憶媒体9から生じる
信号磁界8の水平成分に検知できる様に、前記円
板10に対応して略平行に配置されている。又、
交流バイアス磁界印加手段117としては後述す
る様に種々の方式が与えられるが、いずれも信号
磁界8の周波数より高い周波数の交流バイアス磁
界16が信号磁界の水平成分方向、つまり磁気抵
抗効果素子のストライプ幅方向に加わる様に形成
されている。又交流バイアス磁界の大きさは、通
常数〜数十エルステツドの大きさに設定される。 Next, embodiments of the present invention will be described with reference to FIGS. 2, 3, and 4. FIG. 2 schematically shows an embodiment of the present invention focusing on basic functions. The bit length L is attached to the rotating shaft 6 of the rotating body, and the magnetic signals are distributed at equal intervals along the circumference.
a disk 10 having a magnetic storage medium 9 recorded in the form of magnetization 7; and a magnetic disk 10 arranged so that a change in a magnetic signal 8 caused by the rotation of the rotating shaft 6 can be detected as a change in electrical resistance. sensor 11 and
A minute alternating current bias magnetic field 1 is applied to this magnetic sensor 11.
6, and the magnetic sensor 11.
a drive circuit 18 such as a constant current circuit that supplies a constant current to the magnetoresistive element; an amplification circuit 24 that amplifies the output signals 19, 20, 21, and 22 of the magnetic sensor 11; and an amplification circuit output waveform. It includes an amplitude demodulation circuit 25 that cuts, rectifies, and integrates the DC offset voltage of , and a comparator 26 that extracts the output of the amplitude demodulation circuit as pulsed angular position signals 27, 28, and 17. Here, the magnetic sensor 11 includes four striped ferromagnetic magnetoresistive elements 12, 1 having uniaxial anisotropy in the longitudinal direction.
3, 14, and 15 are formed with a pitch of 1/4L, and are arranged substantially parallel to the disk 10 so that the horizontal component of the signal magnetic field 8 generated from the magnetic storage medium 9 can be detected. It is located. or,
Various methods are available as the AC bias magnetic field applying means 117 as described later, but in all of them, the AC bias magnetic field 16 with a frequency higher than the frequency of the signal magnetic field 8 is applied in the horizontal component direction of the signal magnetic field, that is, in the stripe of the magnetoresistive element. It is formed so as to be applied in the width direction. Further, the magnitude of the alternating current bias magnetic field is usually set to a magnitude of several to several tens of oersteds.
第3図は、第2図中の磁気抵抗効果素子12,
13,14,15及び駆動回路18及び再生回路
23の部分の具体例を示す回路図、第4図は検出
過程を説明するための図である。 FIG. 3 shows the magnetoresistive element 12 in FIG.
FIG. 4 is a circuit diagram showing a specific example of the parts 13, 14, 15, the drive circuit 18, and the reproduction circuit 23, and is a diagram for explaining the detection process.
回転軸6が第2図の矢印の方向45に回転する
と、第4図aに示す様な磁化7の繰り返しによつ
て、磁気抵抗効果素子12には、第4図bに示す
様な磁気信号8の水平成分46が信号磁界として
加わる。この信号磁界46を、信号磁界の最大周
波数より高い周波数の微小振幅交流バイアス磁界
を印加しながら再生し交流増幅すると、増巾回路
出力33として第4図cに示す様に交流バイアス
磁界を搬送波として、信号磁界46で振幅変調さ
れた波形に類似の出力47が得られる。この出力
の直流オフセツト分を、コンデンサ69でカツト
した後これをダイオード31と積分回路32から
成る振幅復調回路25を通すことにより第4図e
に示す復調出力49生じる。同様にして磁気抵抗
効果素子12と1/2Lはなれた磁気抵抗効果素子
14からは前記復調出力49と180゜位相のずれた
復調出力50を生じる。この両者を差動コンパレ
ータ26に入ることにより、第1信号出力(A相
出力と略称する)端子27には、第4図fに示す
様な磁気記憶媒体のビツトに対応したパルス出力
51を生じる。 When the rotating shaft 6 rotates in the direction 45 of the arrow in FIG. 2, the magnetoresistive element 12 receives a magnetic signal as shown in FIG. 4b due to repeated magnetization 7 as shown in FIG. 4a. 8 horizontal components 46 are added as a signal magnetic field. When this signal magnetic field 46 is regenerated and AC amplified while applying a minute amplitude AC bias magnetic field with a frequency higher than the maximum frequency of the signal magnetic field, the AC bias magnetic field is used as a carrier wave as an amplification circuit output 33 as shown in FIG. 4c. , an output 47 similar to a waveform amplitude modulated by the signal magnetic field 46 is obtained. After cutting off the DC offset portion of this output with a capacitor 69, it is passed through an amplitude demodulation circuit 25 consisting of a diode 31 and an integrating circuit 32, as shown in Fig. 4e.
A demodulated output 49 shown in FIG. Similarly, a demodulated output 50 which is 180° out of phase with the demodulated output 49 is produced from the magnetoresistive element 14 which is separated from the magnetoresistive element 12 by 1/2L. By inputting both of them into the differential comparator 26, a pulse output 51 corresponding to the bit of the magnetic storage medium as shown in FIG. .
同様に、磁気抵抗効果素子13と15とから
は、A相出力から1/4周期遅れれて、第4図gに
示す様な第2信号出力(B相出力と略称する)5
2を生じる。回転軸6が逆方向に回転するとB相
出力52の位相がA相より1/4周期進む。従つて、
回転軸6の回転角度は回転によつて生じるA相出
力又はB相出力のパルス数、もしくはこの両者を
電気的に合成して得られる出力のパルス数を計数
することによつて検知でき、回転方向は両相の位
相関係により判定できる。 Similarly, the magnetoresistive elements 13 and 15 output a second signal (abbreviated as B-phase output) 5 as shown in FIG.
2. When the rotating shaft 6 rotates in the opposite direction, the phase of the B-phase output 52 advances by 1/4 cycle than the A-phase. Therefore,
The rotation angle of the rotating shaft 6 can be detected by counting the number of pulses of the A-phase output or B-phase output generated by the rotation, or the number of pulses of the output obtained by electrically combining both. The direction can be determined by the phase relationship between both phases.
磁気情報発生源である円板10には厚さ数mm直
径数十cmのアルミ板が用いられ、このアルミ板端
面に飽和磁化5000〜10000ガウス、抗磁力200エル
ステツド以上の磁性媒体9が数〜数十ミクロンの
厚さに形成されている。この磁性媒体としては、
Co−Ni等の金属強磁性体やγ−Fe2O3等が使用
される。磁気抵抗効果素子12,13,14,1
15としては、パーマロイやコバルト等を主成分
とする金属強磁性合金をシリコン単結晶やガラス
等の表面の滑らかな基板上に厚さ数百オングスト
ローム、ストライプ幅数十ミクロン、長さ数ミリ
メートル形状になる様、両端の電気端子と共に薄
膜作製技術で作製されたものが用いられ、磁気セ
ンサー部11を形成している。 An aluminum plate with a thickness of several mm and a diameter of several tens of centimeters is used as the disk 10 which is a source of magnetic information, and several to several magnetic media 9 with a saturation magnetization of 5000 to 10000 Gauss and a coercive force of 200 Oersted or more are placed on the end face of this aluminum plate. It is formed to a thickness of several tens of microns. This magnetic medium is
Metal ferromagnetic materials such as Co-Ni and γ-Fe 2 O 3 are used. Magnetoresistive elements 12, 13, 14, 1
15, a metal ferromagnetic alloy containing permalloy, cobalt, etc. as the main component is formed into a shape several hundred angstroms thick, several tens of microns wide, and several millimeters long on a substrate with a smooth surface such as silicon single crystal or glass. As can be seen, the magnetic sensor section 11 is formed by using the electrical terminals at both ends, which are fabricated by thin film fabrication technology.
この磁気センサー部11が回転軸6の回転に伴
つて変わる磁性媒体9から生じる数なないし数百
エルテツドの信号磁界8の水平成分を十分減知で
きる様な位置、例えば磁性媒体9端面から数十〜
数百ミクロン離れた位置に水平方向に配置され
る。円板10の大きさや磁気抵抗効果素子の数及
びピツチは、所望の回転角度検出精度により適宜
選定される。 The magnetic sensor section 11 is located at a position where it can sufficiently detect the horizontal component of the signal magnetic field 8 of several to several hundred degrees generated from the magnetic medium 9 that changes with the rotation of the rotating shaft 6, for example, several tens of degrees from the end surface of the magnetic medium 9. ~
They are placed horizontally several hundred microns apart. The size of the disk 10 and the number and pitch of the magnetoresistive elements are appropriately selected depending on the desired rotational angle detection accuracy.
次に微小振幅交流バイアス磁界印加手段17の
具体例について説明する。 Next, a specific example of the minute amplitude AC bias magnetic field applying means 17 will be explained.
第5図は、本発明における交流バイアス磁界印
加手段の第1の例を示したもので、絶縁層(第5
図中では省略してある)を介して磁気抵抗効果素
子12,13,14,15に平行に形成された導
電体層53と、この導電体層53へ交流バイアス
信号電流iを流す発振器54とから成る。導電体
層53に流れる交流バイアス電流iにより磁気抵
抗素子12,13,14,15には、ストライプ
幅方向の交流バイアス磁界が印加される。交流バ
イアス磁界の大きさは、磁気抵抗効果素子12,
13,14,15と導電体層53との間に形成さ
れる絶縁体層の厚さ及び交流バイアス電流値によ
り、適宜設定される。導電体層53としては、厚
さ数千〜数十ミクロンの金・銅・アルミニウム
等、又、導電体層としては厚さ数千オングストロ
ーム〜数ミクロンのSiO、SiO2、Al2O3等の薄膜
が適する。 FIG. 5 shows a first example of the AC bias magnetic field applying means in the present invention, in which the insulating layer (the fifth
A conductor layer 53 formed in parallel to the magnetoresistive elements 12, 13, 14, and 15 via magnetoresistive elements (omitted in the figure), and an oscillator 54 that flows an AC bias signal current i to the conductor layer 53. Consists of. An AC bias magnetic field in the stripe width direction is applied to the magnetoresistive elements 12, 13, 14, and 15 by the AC bias current i flowing through the conductor layer 53. The magnitude of the AC bias magnetic field is determined by the magnetoresistive element 12,
It is appropriately set depending on the thickness of the insulator layer formed between the conductor layer 53 and the conductor layer 13, 14, 15 and the AC bias current value. The conductive layer 53 is made of gold, copper, aluminum, etc. with a thickness of several thousand to several tens of microns, and the conductive layer is made of SiO, SiO 2 , Al 2 O 3 , etc. with a thickness of several thousand angstroms to several microns. A thin film is suitable.
第6図は本発明における交流バイアス磁界印加
手段の第2の例を示したもので、巻線56及びギ
ヤツプ63を有し高透磁性体から成るコア55
と、前記巻線56へ交流バイアス電流iを流す発
振器54とで形成され磁気抵抗効果素子12,1
3,14,15は前記ギヤツプ63中に設置され
ている。巻線56に流れる交流バイアス電流iに
よりコア55のギヤツプ63に生じる漏洩磁界が
交流バイアス磁界として磁気抵抗効果素子12,
13,14,15のストライプ幅方向に印加され
る。交流バイアス磁界の大きさはコア55のギヤ
ツプ63の大きさや、交流バイアス電流値により
適宜設定される。コア55としては、パーマロイ
やフエライト等の高透磁率磁性体を適当な大きさ
に加工したものが適する。 FIG. 6 shows a second example of the AC bias magnetic field applying means according to the present invention, in which a core 55 made of a highly permeable material has a winding 56 and a gap 63.
and an oscillator 54 that flows an alternating current bias current i to the winding 56.
3, 14, and 15 are installed in the gap 63. A leakage magnetic field generated in the gap 63 of the core 55 due to the AC bias current i flowing through the winding 56 is used as an AC bias magnetic field in the magnetoresistive element 12,
It is applied in the width direction of stripes 13, 14, and 15. The magnitude of the AC bias magnetic field is appropriately set depending on the size of the gap 63 of the core 55 and the value of the AC bias current. As the core 55, a material obtained by processing a high permeability magnetic material such as permalloy or ferrite into an appropriate size is suitable.
第7図は、本発明における微小振幅交流バイア
ス印加手段の第3の例を示したもので、一定速度
で回転し磁気信号が円周に沿つて等間隔のビツト
長L2を有する磁化58の形で記録されている。
磁気記憶媒体59を有する円柱60から成り、こ
の磁気記憶媒体59から生じるバイアス磁界64
が、磁気抵抗効果素子12,13,14,15の
ストライプ幅方向に印加される様に配置されてい
る。交流バイアス磁界の大きさ及び周波数は、円
柱60の径の大きさ、磁気記憶体59の厚さ、ビ
ツト長L2、円柱60が磁気抵抗効果素子12,
13,14,15に対する設置位置及び回転軸5
7の回転速度を調節することにより所望の値に設
定される。この交流バイアス磁界発生源の材料及
び構成は、前述した磁気信号発生源とほぼ同様の
ものが適する。 FIG. 7 shows a third example of the minute amplitude alternating current bias applying means according to the present invention, in which the magnetization 58 rotates at a constant speed and the magnetic signal has a bit length L 2 equally spaced along the circumference. recorded in the form.
It consists of a cylinder 60 with a magnetic storage medium 59 and a bias magnetic field 64 generated from this magnetic storage medium 59.
is applied in the stripe width direction of the magnetoresistive elements 12, 13, 14, and 15. The magnitude and frequency of the AC bias magnetic field are determined by the diameter of the cylinder 60, the thickness of the magnetic storage body 59, the bit length L 2 , the magnetoresistive element 12 of the cylinder 60,
Installation position and rotation axis 5 for 13, 14, 15
The desired value is set by adjusting the rotation speed of 7. The material and structure of this alternating current bias magnetic field generation source are suitably similar to those of the magnetic signal generation source described above.
第8図は、本発明における微小振幅交流バイア
ス印加手段の第4の例を示したもので、一定速度
で走行し磁気信号が走行方向に沿つて、等間隔の
ビツト長L3を有する磁化66の形で記録されて
いる磁気記憶媒体65を有する磁気テープ62か
ら成り、この磁気記憶媒体65から生じるバイア
ス磁界67が磁気抵抗効果素子12,13,1
4,15のストライプ幅方向に印加される様に配
置されている。交流バイアス磁界の大きさ及び周
波数、磁気記憶媒体65の厚さ、ビツト長L3、
磁気テープ62が磁気抵抗効果素子12,13,
14,15に対する設置位置及び磁気テープ62
の走向速度を調節することにより所望の値に設定
される。この交流バイアス磁界の発生源には、通
常の磁気テープが適する。 FIG. 8 shows a fourth example of the minute amplitude alternating current bias applying means according to the present invention, in which magnetization 66 which travels at a constant speed and has a magnetic signal having equally spaced bit lengths L 3 along the traveling direction is shown in FIG. It consists of a magnetic tape 62 having a magnetic storage medium 65 recorded in the form of
The voltage is applied in the width direction of stripes 4 and 15. The magnitude and frequency of the AC bias magnetic field, the thickness of the magnetic storage medium 65, the bit length L 3 ,
The magnetic tape 62 has magnetoresistive elements 12, 13,
Installation position for 14, 15 and magnetic tape 62
It is set to a desired value by adjusting the strike speed of . An ordinary magnetic tape is suitable as a source of this AC bias magnetic field.
以上説明した様に本発明によれば、角度位置情
報発生源としての磁気記憶媒体と、この位置情報
の磁気センサーとしての強磁性磁気抵抗効果素子
とを組み合わせた角度検出器において、上記構成
要素のほかに、磁気センサーへの微小振幅交流バ
イアス磁界印加手段と振幅復調回路とを設けて、
角度位置信号磁界を前記微小振幅交流バイアス磁
界を搬送波として、振幅変調された形で交流的に
検出し復調することにより、従来の直流的な信号
磁界検出方式で最大の問題となつていた直流オフ
セツト電圧に起因する種々の欠点を克服できる効
果がある。 As explained above, according to the present invention, in an angle detector that combines a magnetic storage medium as an angular position information generation source and a ferromagnetic magnetoresistive element as a magnetic sensor for this position information, the above-mentioned components are combined. In addition, means for applying a minute amplitude AC bias magnetic field to the magnetic sensor and an amplitude demodulation circuit are provided,
By detecting and demodulating the angular position signal magnetic field in an AC manner in an amplitude-modulated form using the minute amplitude AC bias magnetic field as a carrier wave, it is possible to eliminate DC offset, which has been the biggest problem with conventional DC signal magnetic field detection methods. This has the effect of overcoming various drawbacks caused by voltage.
第1図は、本発明の再生原理を説明するための
図、第2図は、本発明の一実施例の基本構成を模
式的に示した図、第3図は第2図に示した磁気抵
抗効果素子と駆動回路及び再生回路の具体的な一
例を示す回路図、第4図は本発明の検出過程を示
す図で、aは磁気記憶媒体の磁化の繰り返し状態
を示す図、bは磁気記憶媒体から磁気抵抗効果素
子に加わる信号磁界を示す図、cは増幅器出力波
形を示す図、dは整流回路出力波形を示す図、e
は振幅復調回路出力波形を示す図、fはA相出力
波形を示す図、gはB相出力波形を示す図であ
る。第5図、第6図、第7図および第8図はそれ
ぞれ本発明における交流バイアス磁界印加手段の
例を示す概略斜視図である。
1……強磁性磁気抵抗効果素子の静特性曲線、
2……微小振幅交流バイアス磁界、3,4,5…
…交流的なΔRの変化、6,57,68……回転
軸、7,58,66……磁化、8,64,67…
…磁性媒体から生じる信号磁界及びバイアス磁
界、9,59,65……磁気記憶媒体、10……
円板、11……磁気センサー、12,13,1
4,15……強磁性磁気抵抗効果素子、16……
微小交流バイアス磁界、17……微小交流バイア
ス磁界印加手段、18……駆動回路、19,2
0,21,22……磁気抵抗効果素子の出力端
子、23……再生回路、24……交流増幅回路、
25……振幅復調回路、26……コンパレータ、
27……A相出力端子、28……B相出力端子、
29……コンデンサ、30……増幅器、31……
ダイオード、32……積分回路、33,34,3
5,36……交流増幅回路出力端子、37,3
8,39,40……整流回路出力端子、41,4
2,43,44……振幅復調回路出力端子、45
……回転軸の回転方向、46……信号磁界、47
……増幅回路出力波形、48……整流回路出力波
形、49,50……振幅復調回路出力波形、51
……A相出力波形、52……B相出力波形、53
……導電体層、54……発振器、55……コア、
56……巻線、61……モータ、62……磁気テ
ープ、63……コアのギヤツプ、69……コンデ
ンサ。
FIG. 1 is a diagram for explaining the reproduction principle of the present invention, FIG. 2 is a diagram schematically showing the basic configuration of an embodiment of the present invention, and FIG. 3 is a diagram for explaining the reproduction principle of the present invention. FIG. 4 is a circuit diagram showing a specific example of a resistive effect element, a drive circuit, and a reproducing circuit, and FIG. 4 is a diagram showing the detection process of the present invention. A diagram showing the signal magnetic field applied to the magnetoresistive element from the storage medium, c is a diagram showing the amplifier output waveform, d is a diagram showing the rectifier circuit output waveform, e
is a diagram showing an amplitude demodulation circuit output waveform, f is a diagram showing an A-phase output waveform, and g is a diagram showing a B-phase output waveform. 5, 6, 7, and 8 are schematic perspective views showing examples of alternating current bias magnetic field applying means in the present invention, respectively. 1... Static characteristic curve of ferromagnetic magnetoresistive element,
2...Minute amplitude AC bias magnetic field, 3, 4, 5...
...Change in AC-like ΔR, 6,57,68...Rotation axis, 7,58,66...Magnetization, 8,64,67...
...Signal magnetic field and bias magnetic field generated from magnetic medium, 9,59,65...Magnetic storage medium, 10...
Disc, 11... Magnetic sensor, 12, 13, 1
4, 15...Ferromagnetic magnetoresistive element, 16...
Minute alternating current bias magnetic field, 17...Minute alternating current bias magnetic field applying means, 18... Drive circuit, 19,2
0, 21, 22...Output terminal of magnetoresistive element, 23...Reproduction circuit, 24...AC amplifier circuit,
25...amplitude demodulation circuit, 26...comparator,
27...A phase output terminal, 28...B phase output terminal,
29...Capacitor, 30...Amplifier, 31...
Diode, 32...Integrator circuit, 33, 34, 3
5, 36... AC amplifier circuit output terminal, 37, 3
8, 39, 40... Rectifier circuit output terminal, 41, 4
2, 43, 44...amplitude demodulation circuit output terminal, 45
...Rotation direction of the rotating shaft, 46...Signal magnetic field, 47
... Amplifier circuit output waveform, 48 ... Rectifier circuit output waveform, 49, 50 ... Amplitude demodulation circuit output waveform, 51
...A phase output waveform, 52...B phase output waveform, 53
... Conductor layer, 54 ... Oscillator, 55 ... Core,
56...Winding, 61...Motor, 62...Magnetic tape, 63...Core gap, 69...Capacitor.
1 計測室内に回転自在のロータを配置し、この
ロータにロータ軸を挟んで対向して位置するブレ
ードを配置し、このブレードの後退端の上、下部
それぞれに切欠部を設けて外顎部およびこれより
も突出する内顎部を形成し、この内、外顎部にロ
ーラが回転自在に保持されたローラ軸を配置する
一方、
前記計測室の上、下蓋の内側中心に板カムを固
定し、この板カムを収納するカム収納穴を前記ロ
ータの両側に設けて前記ブレードの上、下部のロ
ーラを板カムのカム面に沿つて回転するように配
置した摺動式ブレード流量計において、
対向するブレードの上、下部それぞれをロータ
軸を貫通して配置された連結ロツドにより所定間
隔をおいて連結し、ブレードの上、下部のローラ
を板カムのカム面に接触させたことを特徴とする
摺動式ブレード流量計。
1. A rotatable rotor is placed in the measurement chamber, and blades are placed on the rotor to face each other across the rotor shaft, and cutouts are provided at the top and bottom of the retracted end of the blades to form external jaws and An inner jaw is formed that protrudes beyond this, and a roller shaft with a rotatably held roller is placed in the inner and outer jaw, while a plate cam is fixed at the center of the inner side of the lower lid above the measurement chamber. In a sliding blade flowmeter, in which cam storage holes for storing the plate cam are provided on both sides of the rotor, and rollers at the upper and lower parts of the blade are arranged to rotate along the cam surface of the plate cam, The upper and lower parts of the opposing blades are connected at a predetermined interval by connecting rods that pass through the rotor shaft, and the rollers on the upper and lower parts of the blades are brought into contact with the cam surface of the plate cam. Sliding blade flow meter.
Claims (1)
転し磁気信号が円周に沿つて等間隔のビツト長を
有する磁化の形で記録されている磁気記憶媒体を
有する円板もしくは円柱から成る特許請求の範囲
第1項に記載の角度検出器。 5 交流バイアス磁界印加手段が、一定速度で走
行し磁気信号が走行方向に沿つて等間隔のビツト
長を有する磁化の形で記録されている磁気記憶媒
体を有する磁気テープから成る特許請求の範囲第
1項に記載の角度検出器。4. A patent claim in which the alternating current bias magnetic field applying means consists of a disk or cylinder having a magnetic storage medium that rotates at a constant speed and in which magnetic signals are recorded in the form of magnetization with equally spaced bit lengths along the circumference. An angle detector according to range 1. 5. The alternating current bias magnetic field applying means comprises a magnetic tape having a magnetic storage medium running at a constant speed and in which magnetic signals are recorded in the form of magnetization having bit lengths equally spaced along the running direction. Angle detector according to item 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2920879A JPS55121110A (en) | 1979-03-13 | 1979-03-13 | Angle detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2920879A JPS55121110A (en) | 1979-03-13 | 1979-03-13 | Angle detector |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS55121110A JPS55121110A (en) | 1980-09-18 |
| JPH022086B2 true JPH022086B2 (en) | 1990-01-16 |
Family
ID=12269770
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2920879A Granted JPS55121110A (en) | 1979-03-13 | 1979-03-13 | Angle detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS55121110A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS586565A (en) * | 1981-07-02 | 1983-01-14 | Nec Corp | Angle detector for magnetic disc recorder and reproducer |
| US5144231A (en) * | 1988-09-30 | 1992-09-01 | Jeffrey Tenenbaum | Eddy current detector for detecting an object with offset compensation |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6020802B2 (en) * | 1976-04-26 | 1985-05-23 | 日本電気株式会社 | magnetic head |
| JPS5357810A (en) * | 1976-11-04 | 1978-05-25 | Mitsubishi Electric Corp | Magnetic head device |
-
1979
- 1979-03-13 JP JP2920879A patent/JPS55121110A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS55121110A (en) | 1980-09-18 |
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