JPH065172B2 - Magnetoresistive sensor for magnetic encoder - Google Patents
Magnetoresistive sensor for magnetic encoderInfo
- Publication number
- JPH065172B2 JPH065172B2 JP61134464A JP13446486A JPH065172B2 JP H065172 B2 JPH065172 B2 JP H065172B2 JP 61134464 A JP61134464 A JP 61134464A JP 13446486 A JP13446486 A JP 13446486A JP H065172 B2 JPH065172 B2 JP H065172B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- detection
- recording medium
- detection signal
- magnetic recording
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
- 230000005291 magnetic effect Effects 0.000 title claims description 104
- 238000001514 detection method Methods 0.000 claims description 81
- 238000006073 displacement reaction Methods 0.000 description 8
- 239000000758 substrate Substances 0.000 description 7
- 238000010586 diagram Methods 0.000 description 4
- 230000000694 effects Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 230000005415 magnetization Effects 0.000 description 2
- 239000005360 phosphosilicate glass Substances 0.000 description 2
- 230000001681 protective effect Effects 0.000 description 2
- 230000008961 swelling Effects 0.000 description 2
- 229910017709 Ni Co Inorganic materials 0.000 description 1
- 229910003267 Ni-Co Inorganic materials 0.000 description 1
- 229910003271 Ni-Fe Inorganic materials 0.000 description 1
- 229910003262 Ni‐Co Inorganic materials 0.000 description 1
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- QXZUUHYBWMWJHK-UHFFFAOYSA-N [Co].[Ni] Chemical compound [Co].[Ni] QXZUUHYBWMWJHK-UHFFFAOYSA-N 0.000 description 1
- WATWJIUSRGPENY-UHFFFAOYSA-N antimony atom Chemical compound [Sb] WATWJIUSRGPENY-UHFFFAOYSA-N 0.000 description 1
- 239000005385 borate glass Substances 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- WPYVAWXEWQSOGY-UHFFFAOYSA-N indium antimonide Chemical compound [Sb]#[In] WPYVAWXEWQSOGY-UHFFFAOYSA-N 0.000 description 1
- 238000007689 inspection Methods 0.000 description 1
- UGKDIUIOSMUOAW-UHFFFAOYSA-N iron nickel Chemical compound [Fe].[Ni] UGKDIUIOSMUOAW-UHFFFAOYSA-N 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 230000010363 phase shift Effects 0.000 description 1
- 229910052698 phosphorus Inorganic materials 0.000 description 1
- 239000011574 phosphorus Substances 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 229910052814 silicon oxide Inorganic materials 0.000 description 1
Landscapes
- 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】 「産業上の利用分野」 この発明は、例えば磁気ロータリーエンコーダ等に適用
され、磁気記録媒体に記録された磁気情報を、固有抵抗
が磁界の強さに応じて変化する磁気抵抗素子を用いて検
出することにより、磁気記録媒体の相対的変位を検出す
る磁気エンコーダ用磁気抵抗センサに関する。DETAILED DESCRIPTION OF THE INVENTION "Industrial field of application" The present invention is applied to, for example, a magnetic rotary encoder and the like, and the specific resistance of magnetic information recorded on a magnetic recording medium changes according to the strength of a magnetic field. The present invention relates to a magnetic resistance sensor for a magnetic encoder, which detects a relative displacement of a magnetic recording medium by detecting the magnetic resistance element.
「従来の技術」 周知のように、磁気ロータリーエンコーダは、シャフト
に固定された円盤状の磁気記録媒体と、この磁気記録媒
体と所定のギャップを隔てて対向配置された磁気抵抗セ
ンサとから構成されているが、これらは、従来、一般に
第3図(イ)〜(ニ)に示すように構成されている。"Prior Art" As is well known, a magnetic rotary encoder is composed of a disk-shaped magnetic recording medium fixed to a shaft, and a magnetoresistive sensor that is opposed to the magnetic recording medium with a predetermined gap. However, these are generally configured as shown in FIGS. 3 (A) to 3 (D).
これらの図において、1は磁気記録媒体、2は磁気抵抗
センサである。この磁気記録媒体1には、磁気抵抗セン
サ2と対向する円軌道に沿って波長λの正弦波を磁化記
録することにより、等間隔の磁化ピッチ1a,1a,…からな
る磁気情報(着磁パターン)が記録されている。一方、
磁気抵抗センサ2は、ガラス基板3と、このガラス基板
3上に蒸着された磁気抵抗素子4とから構成されてい
る。この磁気抵抗素子4は、磁界中に置かれた場合、そ
の磁界の強さに応じて固有抵抗が変化する現象、いわゆ
る磁気抵抗効果が生じる素子材料によって構成されてお
り、この磁気抵抗効果を利用して、磁気記録媒体1が図
に示す矢印M方向に相対変位した場合に、磁気記録媒体
1上に記録された着磁パターンが読み取られ、これによ
り、磁気記録媒体1と共に回転するシャフトの回転量が
検出されるようになっている。In these figures, 1 is a magnetic recording medium, and 2 is a magnetoresistive sensor. By magnetically recording a sinusoidal wave having a wavelength λ along a circular orbit facing the magnetoresistive sensor 2, magnetic information (magnetization pattern 1a, 1a, ... ) Is recorded. on the other hand,
The magnetoresistive sensor 2 is composed of a glass substrate 3 and a magnetoresistive element 4 deposited on the glass substrate 3. The magnetoresistive element 4 is composed of an element material that produces a phenomenon in which the specific resistance changes according to the strength of the magnetic field when placed in a magnetic field, so-called magnetoresistive effect. Then, when the magnetic recording medium 1 is relatively displaced in the direction of the arrow M shown in the figure, the magnetization pattern recorded on the magnetic recording medium 1 is read, whereby the rotation of the shaft that rotates together with the magnetic recording medium 1 is rotated. The amount is to be detected.
この場合、磁気抵抗素子4は、磁気記録媒体1の変位方
向Mと直交する方向に延びる検出部S1〜S16と、これ
ら各検出部S1〜S16の間を各々接続し、変位方向Mと平
行に延びる接続部C1〜C16とから構成され、櫛形状に
形成されている。ここで、各検出部S1〜S16の相対的
位置関係について述べると、検出部S1〜S4は各々λず
つ離間し、検出部S5は検出部S4とλ/2離間し、検出
部S5〜S8は各々λずつ離間し、検出部S9は検出部S8
と5/4λ離間し、検出部S9〜S12は各々λずつ離間
し、検出部S13は検出部S12とλ/2離間し、検出部S
13〜S16は各々λずつ離間している。また、検出部S1
の端部は端子T1に、接続部C4は端子T2に、接続部C8
およびC9は端子T3に、接続部C13は端子T4に、検出
部S16の端部は端子T5に各々接続されている。In this case, the magnetoresistive element 4 connects the detection units S 1 to S 16 extending in the direction orthogonal to the displacement direction M of the magnetic recording medium 1 and the detection units S 1 to S 16 respectively, and It is composed of connecting portions C 1 to C 16 extending in parallel with M and is formed in a comb shape. Here, the relative positional relationship between the detection units S 1 to S 16 will be described. The detection units S 1 to S 4 are separated from each other by λ, and the detection unit S 5 is separated from the detection unit S 4 by λ / 2. The detectors S 5 to S 8 are separated from each other by λ, and the detector S 9 detects the detector S 8
And the detectors S 9 to S 12 are separated from each other by λ, the detector S 13 is separated from the detector S 12 by λ / 2, and the detector S 9 is separated from the detector S 12.
13 to S 16 are separated by λ. In addition, the detection unit S 1
End of the terminal is connected to the terminal T 1 , the connecting portion C 4 is connected to the terminal T 2 , and the connecting portion C 8
And C 9 are connected to the terminal T 3 , the connecting portion C 13 is connected to the terminal T 4 , and the end portion of the detecting portion S 16 is connected to the terminal T 5 .
そして、端子T3を接地して、端子T1とT5に+VCCを
印加すると、磁気記録媒体1の変位に伴って、端子T2
から正弦波の検出信号SinOUTが出力されると共に、
端子T4から余弦波の検出信号CosOUTが出力され
る。すなわち、検出部S1〜S8と接続部S1〜S8と接続
部C1〜C8からなる正弦波検出用磁気抵抗素子Aによっ
て検出される検出信号SinOUTは、検出部S9〜S16
と接続部C9〜C16からなる余弦波検出用磁気抵抗素子
Bによって検出される検出信号CosOUTと、位相がλ
/4(90゜)ずれていることになる。これにより、これら
の検出信号SinOUTとCosOUTに基づいて、磁気記
録媒体1の変位方向および変位量が求められる。Then, when the terminal T 3 is grounded and + VCC is applied to the terminals T 1 and T 5 , the terminal T 2 is moved along with the displacement of the magnetic recording medium 1.
The sine wave detection signal SinOUT is output from
The cosine wave detection signal CosOUT is output from the terminal T 4 . That is, the detection signal SinOUT detected by the sine wave detecting magnetoresistive element A including the detection units S 1 to S 8 , the connection units S 1 to S 8 and the connection units C 1 to C 8 is detected by the detection units S 9 to S 8. 16
And the detection signal CosOUT detected by the cosine wave detecting magnetoresistive element B including the connecting portions C 9 to C 16 and the phase is λ.
It is / 4 (90 °) offset. As a result, the displacement direction and displacement amount of the magnetic recording medium 1 are obtained based on these detection signals SinOUT and CosOUT.
「発明が解決しようとする問題点」 ところで、上述した磁気抵抗センサ2の正弦波検出用磁
気抵抗素子Aの中心と余弦波検出用磁気抵抗素子Bの中
心間の距離は、約1mm(約8λ分)前後に設定されてい
る。この中心間の距離は微少ではあるが、このような微
少距離であっても、磁気記録媒体1側に物理的な歪が発
生している確率は高く、これが、高精度の位置検出がで
きない原因となっていた。以下、その理由を詳細に説明
する。[Problems to be Solved by the Invention] By the way, the distance between the center of the sine wave detecting magnetic resistance element A and the center of the cosine wave detecting magnetic resistance element B of the magnetic resistance sensor 2 is about 1 mm (about 8λ). Minutes) before and after. Although the distance between the centers is very small, even with such a small distance, there is a high probability that physical distortion occurs on the magnetic recording medium 1 side, which is the reason why highly accurate position detection cannot be performed. It was. The reason will be described in detail below.
まず、第3図(ハ)に示すように、正弦波検出用磁気抵
抗素子Aと余弦波検出用磁気抵抗素子Bとは磁気記録媒
体1の変位方向Mに沿って直列に設けられている。ここ
で、磁気記録媒体1が図上右方向に移動しているものと
考えると、磁気記録媒体1のうち正弦波検出用磁気抵抗
素子Aに対向する部分は、所定時間経過後に余弦波検出
用磁気抵抗素子Bに対向することになる。ところで、磁
気記録媒体1のうち正弦波検出用磁気抵抗素子Aに対向
する部分に歪が生じているとすると、検出信号SinOU
Tにうねりが生じる。次に、所定時間経過後、その部分
が右方向に移動し余弦波検出用磁気抵抗素子Bに対向す
ると、検出信号CosOUTにうねりが生じる。このよう
に、磁気記録媒体1に歪が存在する場合には、検出信号
SinOUTおよびCosOUTの双方にうねりが生ずるの
であるが、両検出信号においてうねりの生ずるタイミン
グは異なり、最悪の場合、第4図(ロ)および(ハ)に
示すように検出信号SinOUTおよびCosOUTに相互
に逆相のうねりが重畳することとなる。First, as shown in FIG. 3C, the sine wave detecting magnetic resistance element A and the cosine wave detecting magnetic resistance element B are provided in series along the displacement direction M of the magnetic recording medium 1. Here, assuming that the magnetic recording medium 1 is moving to the right in the figure, a portion of the magnetic recording medium 1 facing the sine wave detecting magnetoresistive element A is for detecting a cosine wave after a predetermined time has elapsed. It faces the magnetoresistive element B. By the way, if there is distortion in the portion of the magnetic recording medium 1 facing the sine wave detecting magnetic resistance element A, the detection signal SinOU
Swelling occurs at T. Next, after a lapse of a predetermined time, when the portion moves to the right and faces the cosine wave detecting magnetoresistive element B, the detection signal CosOUT is undulated. As described above, when the magnetic recording medium 1 is distorted, undulations occur in both the detection signals SinOUT and CosOUT, but the undulations occur at different timings in both detection signals, and in the worst case, FIG. As shown in (b) and (c), undulations of opposite phase are superimposed on the detection signals SinOUT and CosOUT.
さて、ロータリエンコーダ等に適用される磁気抵抗セン
サは、第5図に示すような検出回路とともに用いられ
る。図において、正弦波検出用磁気抵抗素子Aから出力
された検出信号SinOUTは、コンパレータ12におい
て基準電圧V0と比較され、両者の大小関係に基づいて
第6図(a)に示すような方形波aに変換される。同様
に、検出信号CosOUTは、コンパレータ14により第
6図(b)に示すような方形波bに変換される。ここ
で、基準電圧コントローラ15は、方形波aのデューテ
ィ比が50%になるように基準電圧V0を制御する。す
なわち、仮に方形波aのデューティ比が50%よりも大
であれば基準電圧V0のレベルを上げ、デューティ比が
50%よりも小であれば基準電圧V0のレベルを下げ
る。この結果、基準電圧V0は、第4図(ロ)に示す検
出信号SinOUTの上下の包絡線の中央部を通るように
変化する。また、基準電圧V0は余弦波検出用磁気抵抗
素子B用のコンパレータ14の基準電圧としても用いら
れる。Now, the magnetoresistive sensor applied to a rotary encoder or the like is used together with a detection circuit as shown in FIG. In the figure, the detection signal SinOUT output from the sine wave detecting magnetic resistance element A is compared with the reference voltage V0 in the comparator 12, and the square wave a as shown in FIG. Is converted to. Similarly, the detection signal CosOUT is converted by the comparator 14 into a square wave b as shown in FIG. 6 (b). Here, the reference voltage controller 15 controls the reference voltage V0 so that the duty ratio of the square wave a is 50%. That is, if the duty ratio of the square wave a is larger than 50%, the level of the reference voltage V0 is raised, and if the duty ratio is smaller than 50%, the level of the reference voltage V0 is lowered. As a result, the reference voltage V0 changes so as to pass through the central portion of the upper and lower envelopes of the detection signal SinOUT shown in FIG. The reference voltage V0 is also used as the reference voltage of the comparator 14 for the cosine wave detecting magnetic resistance element B.
しかしながら、従来の磁気抵抗センサの場合、検出信号
SinOUTと検出信号CosOUTとにおいて、うねりの
生ずるタイミングが異なるため、基準電圧V0は検出信
号CosOUTの包絡線の中央から外れることになる。従
って、方形波bのデューティ比は大きく上下することと
なり、正確な位置検出を行うことが困難になる。However, in the case of the conventional magnetoresistive sensor, the detection signal SinOUT and the detection signal CosOUT have different swelling timings, so that the reference voltage V0 deviates from the center of the envelope of the detection signal CosOUT. Therefore, the duty ratio of the square wave b greatly fluctuates, and it becomes difficult to perform accurate position detection.
この発明は上述した事情に鑑みてなされたもので、磁気
記録媒体に微妙な物理的歪が生じている場合において
も、正弦波検出用磁気抵抗素子と余弦波検出用磁気抵抗
素子から各々出力される各検出信号のうねりを同相化す
ることができ、これにより検出誤差を低減することがで
きる磁気エンコーダ用磁気抵抗センサを提供することを
目的としている。The present invention has been made in view of the above-mentioned circumstances, and even when a slight physical distortion occurs in the magnetic recording medium, the magnetic resistance elements for sine wave detection and the cosine wave detection are output respectively. It is an object of the present invention to provide a magnetoresistive sensor for a magnetic encoder that can make the undulations of the respective detection signals in phase with each other and thereby reduce the detection error.
「問題点を解決するための手段」 この発明は、所定の軌道に沿って所定の波長で交番する
磁気情報が記録された磁気記録媒体上から、前記磁気情
報を、固有抵抗が磁界の強さに応じて変化する磁気抵抗
素子を用いて検出する磁気エンコーダ用磁気抵抗センサ
において、 一波長、一波長半および一波長の間隔を隔てて順次配置
された第1、第2,第3および第4の磁気検出部と、方
形波をなすようにこれら第1,第2,第3および第4の
磁気検出部を順次接続する第1,第2および第3の接続
部とから成り、両端に電圧が印加されるとともに前記磁
気記録媒体が変位すると前記第2の接続部から第1の検
出信号を出力する第1の磁気抵抗素子と、 二波長、半波長および二波長の間隔を隔てて順次配置さ
れた第5,第6,第7および第8の磁気検出部と、方形
波をなすようにこれら第5,第6,第7および第8の磁
気検出部を順次接続する第4,第5および第6の接続部
とから成り、両端に電圧が印加されるとともに前記磁気
記録媒体が変位すると前記第5の接続部から第2の検出
信号を出力する第2の磁気抵抗素子と を具備し、前記第1の磁気抵抗素子と前記第2の磁気抵
抗素子とを入れ子状に配置し、前記第1の検出信号およ
び前記第2の検出信号のうち一方は正弦波であり他方は
余弦波であることを特徴としている。"Means for Solving the Problems" The present invention provides the magnetic information from a magnetic recording medium on which magnetic information alternating at a predetermined wavelength along a predetermined orbit is recorded. In a magnetoresistive sensor for a magnetic encoder for detecting using a magnetoresistive element that changes in accordance with, a first wavelength, a half wavelength, and a first wavelength, a second wavelength, a third wavelength, and a fourth wavelength that are sequentially arranged at intervals of one wavelength. And a first, a second, and a third connection part for sequentially connecting these first, second, third, and fourth magnetic detection parts so as to form a square wave, and a voltage is applied across the both ends. Is applied and the magnetic recording medium is displaced and a first magnetoresistive element that outputs a first detection signal from the second connection portion and a second magnetoresistive element are sequentially arranged at intervals of two wavelengths, a half wavelength, and two wavelengths. 5th, 6th, 7th and 8th magnetism The output part and the fourth, fifth, and sixth connection parts that sequentially connect the fifth, sixth, seventh, and eighth magnetic detection parts so as to form a square wave, and a voltage is applied to both ends. And a second magnetoresistive element that outputs a second detection signal from the fifth connection portion when the magnetic recording medium is displaced, the first magnetoresistive element and the second magnetoresistive element. The elements are arranged in a nested manner, and one of the first detection signal and the second detection signal is a sine wave and the other is a cosine wave.
「作用」 正弦波検出用磁気抵抗素子と余弦波検出用磁気抵抗素子
が、入れ子状に重畳的に配置されているので、磁気記録
媒体の軌道の同一部分から正弦波の磁気情報が検出さ
れ、これにより、磁気記録媒体に微少な物理的歪が生じ
ている場合においても、正弦波検出用磁気抵抗素子と余
弦波検出用磁気抵抗素子から各々出力される両検出信号
のうねりが同相化され、これにより検出誤差が低減され
る。"Operation" Since the magnetic resistance element for detecting the sine wave and the magnetic resistance element for detecting the cosine wave are arranged in a superimposed manner in a nested manner, the magnetic information of the sine wave is detected from the same portion of the track of the magnetic recording medium, Thereby, even when a slight physical distortion occurs in the magnetic recording medium, the swell of both detection signals respectively output from the sine wave detection magnetic resistance element and the cosine wave detection magnetic resistance element is in-phase, This reduces the detection error.
「実施例」 以下、図面を参照し、この発明の実施例について説明す
る。[Embodiment] An embodiment of the present invention will be described below with reference to the drawings.
第1図(イ)および(ロ)はこの発明の一実施例の構成を示す
図である。なお、第1図(イ)においては、磁気抵抗素子
4のパターン以外の部分の図示が省略されている。1 (a) and 1 (b) are diagrams showing the configuration of an embodiment of the present invention. In addition, in FIG. 1 (a), the illustration of the portion other than the pattern of the magnetoresistive element 4 is omitted.
これらの図において、10は、例えばホウ酸ガラスから
なる絶縁性、平滑性の高い基板であり、この基板10上
には検出部S1〜S8と接続部C1〜C8からなる正弦波検
出用磁気抵抗素子Aと、検出S9〜S16と接続部C9〜C
16からなる余弦波検出用磁気抵抗素子Bとが蒸着されて
いる。これら正弦波検出用磁気抵抗素子Aと余弦波検出
用磁気抵抗素子Bが蒸着された基板10上には、例えば
PSG膜(phospho-silicate-glass;りんをドープした
シリコン酸化膜)からなる保護膜14が形成されてい
る。上記正弦波検出用磁気抵抗素子Aおよび余弦波検出
用磁気抵抗素子Bからなる磁気抵抗素子4はNi-Fe(ニ
ッケル−鉄),Ni-Co(ニッケル-コバルト)などの強磁性材料、ま
たはInSb(アンチモン化シンジウム)などの半導体に
よって構成されている。In these figures, 10 is a substrate made of, for example, borate glass and having a high insulating property and smoothness, and a sine wave composed of detection units S 1 to S 8 and connection units C 1 to C 8 is provided on the substrate 10. Magnetic resistance element A for detection, detection S 9 to S 16 and connecting portions C 9 to C
A cosine wave detecting magnetoresistive element B consisting of 16 is deposited. On the substrate 10 on which the sine wave detecting magnetic resistance element A and the cosine wave detecting magnetic resistance element B are vapor-deposited, for example, a protective film formed of a PSG film (phospho-silicate-glass; silicon oxide film doped with phosphorus) 14 is formed. The magnetoresistive element 4 including the sine wave detecting magnetic resistance element A and the cosine wave detecting magnetic resistance element B is a ferromagnetic material such as Ni-Fe (nickel-iron), Ni-Co (nickel-cobalt), or InSb. (Cindium antimonide) and other semiconductors.
また、正弦波検出用磁気抵抗素子Aと余弦波検出用磁気
抵抗素子Bは基板10上に、重畳的に配置され、正弦波
検出用磁気抵抗素子Aの櫛形のパターンが、余弦波検出
用磁気抵抗素子Bの櫛形のパターンに対して入れ子状に
配置されている。Further, the sine wave detecting magnetic resistance element A and the cosine wave detecting magnetic resistance element B are arranged in a superposed manner on the substrate 10, and the comb-shaped pattern of the sine wave detecting magnetic resistance element A has a cosine wave detecting magnetic resistance. The resistance elements B are arranged in a nested manner with respect to the comb-shaped pattern.
ここで、各検出部S1〜S16の相対的位置関係について
述べると、検出部S2は検出部S1とλ離間し、検出部S
3は検出部S2と2λ離間し、検出部S4は検出部S3とλ
離間し、検出部S5は検出部S4と3/2λ離間し、検出
部S6は検出部S5とλ離間し、検出部S7は検出部S6と
2λ離間し、検出部S8は検出部S7とλ離間している。
また検出部S15は検出部S16と2λ離間し、検出部S14
は検出部S15とλ離間し、検出部S13は検出部S14と2
λ離間し、検出部S12は検出部S13とλ/2離間し、検
出部S11は検出部S12と2λ離間し、検出部S10は検出
部S11とλ離間し、検出部S9は検出S10と2λ離間し
て配置されている。さらに、各検出部S1,S3,S5,S7は、
各検出部S16,S14,S12,S10に対して各々λ/4ずつ離間
して配置されている。Here, the relative positional relationship between the detection units S 1 to S 16 will be described. The detection unit S 2 is separated from the detection unit S 1 by λ, and the detection unit S 1 is separated from the detection unit S 1.
3 is separated from the detector S 2 by 2λ, and the detector S 4 is separated from the detector S 3 by λ.
The detector S 5 is separated from the detector S 4 by 3 / 2λ, the detector S 6 is separated from the detector S 5 by λ, and the detector S 7 is separated from the detector S 6 by 2λ. 8 is separated from the detection section S 7 by λ.
Further, the detection unit S 15 is separated from the detection unit S 16 by 2λ, and the detection unit S 14
Is separated from the detecting section S 15 by λ, and the detecting section S 13 is separated from the detecting sections S 14 and 2.
The detector S 12 is separated from the detector S 13 by λ / 2, the detector S 11 is separated from the detector S 12 by 2λ, and the detector S 10 is separated from the detector S 11 by λ. S 9 is placed 2λ away from the detection S 10 . Furthermore, each detection unit S 1 , S 3 , S 5 , S 7 ,
The detectors S 16 , S 14 , S 12 , and S 10 are arranged with a distance of λ / 4.
以上によって、正弦波検出用磁気抵抗素子Aと余弦波検
出用磁気抵抗素子Bが、磁気記録媒体1(第3図参照)
に記録された正弦波の波長λに対して位相が90°ずれ
るように、入れ子状に、かつ重畳的に配置されている。As described above, the magnetic resistance element A for detecting the sine wave and the magnetic resistance element B for detecting the cosine wave are arranged in the magnetic recording medium 1 (see FIG. 3).
They are arranged in a nested manner and in a superposed manner so that the phase shifts by 90 ° with respect to the wavelength λ of the sine wave recorded in 1.
次に、上述した一実施例による磁気抵抗センサを用い
て、第4図(イ)に示すような歪が生じている磁気記録媒
体1に記録された正弦波の磁気情報を検出する場合につ
いて説明する。Next, a case will be described where the magnetic resistance sensor according to the above-described embodiment is used to detect the magnetic information of the sine wave recorded on the magnetic recording medium 1 in which the distortion as shown in FIG. To do.
この場合、端子T3を接地して、端子T1とT5に+VCC
を印加すると、磁気記録媒体1の変位に伴って、端子T
2およびT4から第2図(イ)および(ロ)に示すような検出信
号SinOUTおよびCosOUTが各々出力される。すな
わち、正弦波検出用磁気抵抗素子Aと余弦波検出用磁気
抵抗素子Bが、入れ子状に、重畳的に配置されているの
で、磁気記録媒体1の軌道の同一部分から正弦波の磁気
情報が検出され、これにより、磁気記録媒体1に微少な
物理的歪が生じている場合においても、第2図(イ)およ
び(ロ)に示すように、正弦波検出用磁気抵抗素子Aと余
弦波検出用磁気抵抗素子Bから各々出力される検出信号
SinOUTとCosOUTのうねりU1およびU2が同相化
される。したがって、上述した各実施例の磁気抵抗セン
サを用いることにより、検出誤差を低減することができ
る。In this case, connect terminal T 3 to ground and connect terminals T 1 and T 5 to + VCC
Is applied, the terminal T is moved along with the displacement of the magnetic recording medium 1.
Detection signals SinOUT and CosOUT as shown in FIGS. 2A and 2B are output from 2 and T 4, respectively. That is, since the sine wave detecting magnetic resistance element A and the cosine wave detecting magnetic resistance element B are arranged in a nested manner so as to overlap each other, magnetic information of the sine wave is transmitted from the same portion of the track of the magnetic recording medium 1. Even if a slight physical distortion is generated in the magnetic recording medium 1 due to the detection, the sine wave detecting magnetic resistance element A and the cosine wave are detected as shown in FIGS. The swells U 1 and U 2 of the detection signals SinOUT and CosOUT respectively output from the detection magnetic resistance element B are made in phase. Therefore, the detection error can be reduced by using the magnetoresistive sensor of each of the above-described embodiments.
第7図は本実施例に係る磁気抵抗センサから得られた検
出信号の実測波形を示すものであり、図中、(a)が検
出信号SinOUTの波形、(b)が検出信号CosOU
Tの波形を示すものである。同図に示す通り、各検出信
号SinOUTおよびCosOUTにはほぼ同相の低周
波のうむりが重畳しているのが分かる。従来の磁気抵抗
センサにおいては、これらの低周波のうねりがずれたタ
イミングで重畳していたため、上述の通り正確な位置検
出の障害となっていた。しかし、本実施例によれば、第
7図に示す通り、各検出信号SinOUTおよびCos
OUTには重畳するうねりはほぼ同相であるため、正確
な位置検出を行うことができる。FIG. 7 shows measured waveforms of the detection signal obtained from the magnetoresistive sensor according to the present embodiment. In the figure, (a) is the waveform of the detection signal SinOUT, and (b) is the detection signal CosOU.
It shows a waveform of T. As shown in the figure, it can be seen that low-frequency swells of substantially the same phase are superimposed on the detection signals SinOUT and CosOUT. In the conventional magnetoresistive sensor, these low-frequency undulations are superimposed at the shifted timing, which is an obstacle to accurate position detection as described above. However, according to the present embodiment, as shown in FIG. 7, the respective detection signals SinOUT and Cos are
Since the undulations superimposed on OUT are almost in phase, accurate position detection can be performed.
「発明の効果」 以上説明したように、この発明によれば、所定の軌道に
沿って正弦波の磁気情報が記録された磁気記録媒体上か
ら、前記磁気情報を、固有抵抗が磁界の強さに応じて変
化する磁気抵抗素子を用いて検出する磁気エンコーダ用
磁気抵抗センサにおいて、前記磁気記録媒体の変位に伴
って、正弦波の検出信号を出力する正弦波検出用磁気抵
抗素子と、余弦波の検出信号を出力する余弦波検出用磁
気抵抗素子とを、入れ子状に重畳的に配置したので、磁
気記録媒体の軌道の同一部分から前記正弦波の磁気情報
が検出され、これにより、磁気記録媒体に微少な物理的
歪が生じている場合においても、正弦波検出用磁気抵抗
素子と余弦波検出用磁気抵抗素子から各々出力される各
検出信号のうねりを同相化することができ、これにより
検出誤差を低減することができるという効果が得られ
る。[Advantages of the Invention] As described above, according to the present invention, the magnetic information is recorded on a magnetic recording medium on which sinusoidal magnetic information is recorded along a predetermined orbit, and the specific resistance indicates the strength of the magnetic field. In a magnetoresistive sensor for a magnetic encoder that detects using a magnetoresistive element that changes in accordance with, a sine wave detecting magnetoresistive element that outputs a sine wave detection signal with displacement of the magnetic recording medium, and a cosine wave. The magnetic resistance element for detecting a cosine wave for outputting the detection signal of is arranged in a nested manner so that the magnetic information of the sine wave is detected from the same portion of the orbit of the magnetic recording medium, and thereby the magnetic recording is performed. Even when a slight physical distortion occurs in the medium, it is possible to make the swell of each detection signal output from the sine wave detection magnetic resistance element and the cosine wave detection magnetic resistance element in phase, thereby Inspection The effect that the output error can be reduced is obtained.
さらに、この発明によれば、第1および第2の磁気抵抗
素子のうち入れ子状配置の内側に位置する一方の素子の
間隔を正弦波の半波長に設定した区間を設け、かつ、入
れ子状配置の外側に位置する他方の素子の間隔を正弦波
の一波長半に設定した区間を設けたから、装置をきわめ
て小型に構成することが可能である。Further, according to the present invention, the interval between the one of the first and second magnetoresistive elements located inside the nested arrangement is set to a half wavelength of the sine wave, and the nested arrangement is provided. Since the interval in which the other element located outside is set to one and a half wavelength of the sine wave is provided, the device can be made extremely small.
第1図(イ)はこの発明の一実施例の構成を示す概略平面
図、第1図(ロ)は同図(イ)のB−B線視断面図、第2図
(イ)および(ロ)はこの発明の一実施例の動作を説明するた
めの波形図、第3図(イ)〜(ニ)は従来の磁気ロータリーエ
ンコーダの磁気記録媒体1と磁気抵抗センサ2の構成を
示す図、第4図(イ)〜(ハ)は従来の磁気抵抗センサ2を用
いた場合の問題点を説明するための図、第5図はロータ
リエンコーダ等において磁気抵抗センサと共に用いられ
る検出回路の構成を例示する回路図、第6図は同検出回
路から得られる方形波信号を示す波形図、第7図は本発
明の実施例による磁気抵抗センサから得られた検出信号
の実測例を示す波形図である。 A……正弦波検出用磁気抵抗素子、B……余弦波検出用
磁気抵抗素子、S1〜S16……検出部、C1〜C16……接
続部、T1〜T5……端子、1……磁気記録媒体、4……
磁気抵抗素子、10……基板、12……絶縁膜、14…
…保護膜。FIG. 1 (a) is a schematic plan view showing the configuration of an embodiment of the present invention, FIG. 1 (b) is a sectional view taken along line BB of FIG. 1 (a), and FIG.
(A) and (B) are waveform charts for explaining the operation of the embodiment of the present invention, and FIGS. 3A to 3D are the magnetic recording medium 1 and the magnetoresistive sensor 2 of the conventional magnetic rotary encoder. 4A to 4C are views for explaining problems when the conventional magnetoresistive sensor 2 is used, and FIG. 5 is used with a magnetoresistive sensor in a rotary encoder or the like. 6 is a circuit diagram illustrating the configuration of a detection circuit that is used, FIG. 6 is a waveform diagram showing a square wave signal obtained from the detection circuit, and FIG. 7 is an actual measurement of detection signals obtained from a magnetoresistive sensor according to an embodiment of the present invention. It is a wave form diagram which shows an example. A: sine wave detecting magnetic resistance element, B ... cosine wave detecting magnetic resistance element, S 1 to S 16 ...... detecting section, C 1 to C 16 ...... connecting section, T 1 to T 5 ...... terminal 1 ... Magnetic recording medium, 4 ...
Magnetoresistive element, 10 ... Substrate, 12 ... Insulating film, 14 ...
…Protective film.
フロントページの続き (72)発明者 林 好典 静岡県浜松市中沢町10番1号 日本楽器製 造株式会社内 (56)参考文献 特開 昭59−166812(JP,A) 特開 昭59−179321(JP,A) 特開 昭55−59314(JP,A)Front page continued (72) Inventor Yoshinori Hayashi 10-1 Nakazawa-machi, Hamamatsu-shi, Shizuoka Nihon Gakki Co., Ltd. (56) Reference JP 59-166812 (JP, A) JP 59- 179321 (JP, A) JP-A-55-59314 (JP, A)
Claims (1)
磁気情報が記録された磁気記録媒体上から、前記磁気情
報を、固有抵抗が磁界の強さに応じて変化する磁気抵抗
素子を用いて検出する磁気エンコーダ用磁気抵抗センサ
において、 一波長、一波長半および一波長の間隔を隔てて順次配置
された第1、第2,第3および第4の磁気検出部と、方
形波をなすようにこれら第1,第2,第3および第4の
磁気検出部を順次接続する第1,第2および第3の接続
部とから成り、両端に電圧が印加されるとともに前記磁
気記録媒体が変位すると前記第2の接続部から第1の検
出信号を出力する第1の磁気抵抗素子と、 二波長、半波長および二波長の間隔を隔てて順次配置さ
れた第5,第6,第7および第8の磁気検出部と、方形
波をなすようにこれら第5,第6,第7および第8の磁
気検出部を順次接続する第4,第5および第6の接続部
とから成り、両端に電圧が印加されるとともに前記磁気
記録媒体が変位すると前記第5の接続部から第2の検出
信号を出力する第2の磁気抵抗素子と を具備し、前記第1の磁気抵抗素子と前記第2の磁気抵
抗素子とを入れ子状に配置し、前記第1の検出信号およ
び前記第2の検出信号のうち一方は正弦波であり他方は
余弦波であることを特徴とする磁気エンコーダ用磁気抵
抗センサ。1. A magnetoresistive element whose specific resistance changes in accordance with the strength of a magnetic field from a magnetic recording medium on which magnetic information alternating with a predetermined wavelength along a predetermined trajectory is recorded. In a magnetoresistive sensor for a magnetic encoder for detecting by using, a first, a second, a third and a fourth magnetic detection section sequentially arranged at intervals of one wavelength, one and a half wavelength and one wavelength, and a square wave The magnetic recording medium is composed of first, second and third connecting portions for sequentially connecting the first, second, third and fourth magnetic detecting portions so that a voltage is applied to both ends thereof. Is displaced, a first magnetoresistive element that outputs a first detection signal from the second connection portion and fifth, sixth, and sixth elements sequentially arranged at intervals of two wavelengths, a half wavelength, and two wavelengths. Make a square wave with the 7th and 8th magnetic detectors. And the fifth, sixth, seventh and eighth magnetic detectors are sequentially connected, and the fourth, fifth and sixth connecting portions are connected. When a voltage is applied to both ends and the magnetic recording medium is displaced, A second magnetoresistive element that outputs a second detection signal from the fifth connection portion, wherein the first magnetoresistive element and the second magnetoresistive element are arranged in a nested manner, and One of the first detection signal and the second detection signal is a sine wave, and the other is a cosine wave.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61134464A JPH065172B2 (en) | 1986-06-10 | 1986-06-10 | Magnetoresistive sensor for magnetic encoder |
| KR1019870005799A KR920008235B1 (en) | 1986-06-10 | 1987-06-08 | Magneto-resistance sensor for magnetic encoder |
| GB8713364A GB2191589B (en) | 1986-06-10 | 1987-06-08 | Sensor |
| US07/059,941 US4806860A (en) | 1986-06-10 | 1987-06-09 | Overlapped magnetoresistive displacement detecting transducers having closely spaced longitudinal centers |
| DE19873719328 DE3719328A1 (en) | 1986-06-10 | 1987-06-10 | MAGNETORESISTIVE SENSOR FOR AN ENCODER |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61134464A JPH065172B2 (en) | 1986-06-10 | 1986-06-10 | Magnetoresistive sensor for magnetic encoder |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62289724A JPS62289724A (en) | 1987-12-16 |
| JPH065172B2 true JPH065172B2 (en) | 1994-01-19 |
Family
ID=15128937
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61134464A Expired - Fee Related JPH065172B2 (en) | 1986-06-10 | 1986-06-10 | Magnetoresistive sensor for magnetic encoder |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH065172B2 (en) |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5559314A (en) * | 1978-10-27 | 1980-05-02 | Sony Corp | Magnetic scale signal detector |
| JPS59166812A (en) * | 1983-03-14 | 1984-09-20 | Fanuc Ltd | One rotation detecting system of motor |
| JPS59179321A (en) * | 1983-03-30 | 1984-10-11 | Nissan Motor Co Ltd | Product made of foamed plastic |
-
1986
- 1986-06-10 JP JP61134464A patent/JPH065172B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62289724A (en) | 1987-12-16 |
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| LAPS | Cancellation because of no payment of annual fees |