JP2008241368A - Magnet structure for angle sensor and angle sensor using the same - Google Patents

Magnet structure for angle sensor and angle sensor using the same Download PDF

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JP2008241368A
JP2008241368A JP2007080274A JP2007080274A JP2008241368A JP 2008241368 A JP2008241368 A JP 2008241368A JP 2007080274 A JP2007080274 A JP 2007080274A JP 2007080274 A JP2007080274 A JP 2007080274A JP 2008241368 A JP2008241368 A JP 2008241368A
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permanent magnet
magnetic flux
angle
angle sensor
magnet
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JP5012130B2 (en
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Nobuyuki Shinpo
信之 眞保
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TDK Corp
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a magnet structure for an angle sensor and an angle sensor, used for extensive angle detection with the linearity of a synthetic magnetic field enhanced in an intra-magnetic pole domain. <P>SOLUTION: This magnet structure comprises a cylindrical permanent magnet 1 having a plurality of magnetized poles (for example, two poles comprising an N pole and an S pole). A boundary domain 4A of the permanent magnet 1 is formed obliquely with respect to the moving direction (the circumferential direction of the permanent magnet 1) of a magnetic flux detection means 5 at a position where the detection means 5 crosses the boundary domain 4A. The inclination angle θ of the boundary domain 4A is 3° to 45°. Angle detection is performed by the detection means 5 (for example, a hall element) 5 in an enlarged rectilinear change domain of magnetic flux density. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

本発明は、角度センサ用磁石構造体及びこれを用いた角度センサに関するものであり、特に、円筒形状を有し多極着磁された永久磁石の隣接する磁極の境界領域における合成磁界の直線性(リニアリティ)を改善するための技術に関する。   The present invention relates to a magnet structure for an angle sensor and an angle sensor using the same, and in particular, linearity of a composite magnetic field in a boundary region between adjacent magnetic poles of a cylindrical magnet having multiple poles. The present invention relates to a technique for improving (linearity).

相対運動する物体の運動を適当な信号に変換してその位置制御を正確に行う位置センサ(位置検出装置)の開発が進められており、例えば磁気検出手段(GMRセンサ)と磁石とを用いて回転角度検出を行う角度センサが提案されている(例えば、特許文献1等を参照)。   The development of a position sensor (position detection device) that accurately converts the movement of a relatively moving object into an appropriate signal and accurately controls its position has been developed. For example, using a magnetic detection means (GMR sensor) and a magnet An angle sensor for detecting a rotation angle has been proposed (see, for example, Patent Document 1).

特許文献1記載の回転角度検出装置は、磁界の強度を検出するGMRセンサと、GMRセンサに対してN極が対向する磁石と、GMRセンサに対してS極が対向する磁石とを備えており、各磁石はロータの回転方向に沿ってGMRセンサとの対向面積がロータの回転角度に比例して変化するように形成されている。GMRセンサは、N極とS極との境界線に沿うように磁石に対して相対移動する。   The rotation angle detection device described in Patent Document 1 includes a GMR sensor that detects the strength of a magnetic field, a magnet that has an N pole facing the GMR sensor, and a magnet that has an S pole that faces the GMR sensor. Each magnet is formed such that the area facing the GMR sensor changes in proportion to the rotation angle of the rotor along the rotation direction of the rotor. The GMR sensor moves relative to the magnet along the boundary line between the north and south poles.

すなわち、前述の特許文献1記載の回転角度検出装置では、ロータの回転方向に対して幅が変化する磁石体が付加されており、回転に伴って磁力が変化し、その変化量をGMRセンサで検出するようにしている。したがって、磁力の変化量を捉えて角度検出を行うことが可能であるが、磁石が非常に複雑な非対称形状となり、例えば1つの永久磁石を多極着磁して形成することは難しい。また、複数の磁石を用いて前記着磁状態を実現しようとした場合、個々の永久磁石の形状の加工が難しく、固定も困難であるという問題がある。   That is, in the rotation angle detection device described in Patent Document 1 described above, a magnet body whose width changes with respect to the rotation direction of the rotor is added, the magnetic force changes with rotation, and the amount of change is detected by the GMR sensor. I try to detect it. Therefore, it is possible to detect the angle by detecting the amount of change in the magnetic force, but the magnet has a very complicated asymmetric shape, and it is difficult to form one permanent magnet by multipolar magnetization, for example. Moreover, when it is going to implement | achieve the said magnetized state using a some magnet, there exists a problem that the process of the shape of each permanent magnet is difficult and fixation is also difficult.

磁石構成を簡略化して回転検出等を可能とする角度センサとしては、単純に2極着磁した永久磁石を用いた位置検出装置も知られている(例えば、特許文献2等を参照)。特許文献2には、隣接して配置されたS極とN極の磁石と、これら磁石に対して相対的に移動可能な部材に、初期状態で前記各磁石の間に位置するように固定され、前記部材の相対位置を検出する為の少なくとも1個以上の磁気検出手段とを備え、前記S極とN極の磁石の間には、これら磁石と前記部材の相対位置検出保証範囲に応じた大きさを持つ無磁極部分が設けられることを特徴とする位置検出装置が開示されている。特許文献2記載の位置検出装置では、2極着磁された永久磁石に対向してホール素子を回転体に固定することにより角度検出を可能としており、簡単な構成により角度検出を可能とするとともに、アクチュエータとしての機能も付与している。   As an angle sensor that makes it possible to detect rotation by simplifying the magnet configuration, a position detection device using a permanent magnet that is simply two-pole magnetized is also known (see, for example, Patent Document 2). In Patent Document 2, the S-pole and N-pole magnets arranged adjacent to each other and a member that can move relative to the magnets are fixed so as to be positioned between the magnets in the initial state. And at least one magnetic detection means for detecting the relative position of the member, and according to the relative position detection guarantee range between the magnet and the member between the S-pole and N-pole magnets. There is disclosed a position detecting device characterized in that a non-magnetic pole portion having a size is provided. In the position detection device described in Patent Document 2, angle detection is possible by fixing the Hall element to the rotating body so as to face a permanent magnet magnetized with two poles, and angle detection can be performed with a simple configuration. Also, it has a function as an actuator.

あるいは、磁極を斜めに配置することで、比較的長いストロークでの位置検出を可能とする技術も提案されている(例えば、特許文献3を参照)。特許文献3記載の発明では、2つのS極の間に長方形のN極領域を斜めに配置し、ホール素子をN極領域の長手方向に移動することによりN極領域の幅方向での位置が変化し、前記2つのS極の影響が変化することによる磁界強度の変化に基づいて位置検出を行うようにしている。
特開2005−195471号公報 特開平8−136207号公報 特開平6−11303号公報
Or the technique which enables the position detection with a comparatively long stroke by arrange | positioning a magnetic pole diagonally is proposed (for example, refer patent document 3). In the invention described in Patent Document 3, a rectangular N-pole region is diagonally disposed between two S-poles, and the Hall element is moved in the longitudinal direction of the N-pole region so that the position of the N-pole region in the width direction is changed. The position is detected based on the change in the magnetic field strength due to the change in the influence of the two south poles.
JP 2005-195471 A JP-A-8-136207 JP-A-6-11303

ところで、前述の特許文献2記載の発明では、S極とN極の間に相対的位置検出保証範囲に応じた大きさを持つ無磁極部分を設けるとともに、S極とN極の間の無磁極部分を広げることで、磁気検出手段の出力の直線的変化部分の範囲を広げるようにしている。しかしながら、無磁極部分を広げるだけでは、検出可能な範囲には自ずと限界があり、例えば角度センサにおいて広範な角度範囲での角度検出はほとんど不可能である。   By the way, in the invention described in Patent Document 2, a non-magnetic pole portion having a size corresponding to the relative position detection guarantee range is provided between the S pole and the N pole, and a non-magnetic pole between the S pole and the N pole. By expanding the portion, the range of the linear change portion of the output of the magnetic detection means is expanded. However, there is a limit to the detectable range simply by widening the non-magnetic pole part, and for example, angle detection in a wide angle range is almost impossible in an angle sensor.

一方、特許文献3記載の発明のように、2つのS極の間に長方形のN極領域を斜めに配置し、磁束ガイドで磁極面に平行な方向へ磁束をホール素子に誘導し、当該ホール素子をN極領域の幅内で相対移動することで位置検出を行う構造では、3つの磁気媒体を用意する必要または3極の着磁が必要となり着磁操作が煩雑になるばかりか、2つのS極をバランス良く着磁する必要があり、また、磁束ガイドを別途必要とする等、やはり装置構成の煩雑化によるコスト上昇等が問題になる。また、角度検出については、何ら考慮されていない。   On the other hand, as in the invention described in Patent Document 3, a rectangular N-pole region is obliquely disposed between two S-poles, and a magnetic flux is guided to the Hall element in a direction parallel to the magnetic pole surface by a magnetic flux guide. In the structure in which position detection is performed by relatively moving the element within the width of the N-pole region, it is not only necessary to prepare three magnetic media or three-pole magnetization, which complicates the magnetizing operation. It is necessary to magnetize the south pole in a well-balanced manner, and a separate magnetic flux guide is required, which also raises a problem of cost increase due to complicated apparatus configuration. In addition, no consideration is given to angle detection.

本発明は、このような従来の実情に鑑みて提案されたものであり、簡単な構造でありながら、互いに異なる磁極が隣接する磁極の境界領域において合成磁界の直線性(リニアリティ)を高めることが可能で、広範な角度検出が可能な角度センサ用磁石構造体及び角度センサを提供することを目的とする。   The present invention has been proposed in view of such a conventional situation, and can improve the linearity of the combined magnetic field in the boundary region of magnetic poles adjacent to each other with different magnetic poles while having a simple structure. An object of the present invention is to provide a magnet structure for an angle sensor and an angle sensor capable of detecting a wide range of angles.

前述の目的を達成するために、本発明の角度センサ用磁石構造体は、複数極に着磁された円筒形状を有する永久磁石を備え、前記永久磁石に対向配置された磁束検出手段が前記永久磁石の互いに異なる磁極が隣接する境界領域を横切って周方向に相対的に移動し、前記永久磁石の磁極面に垂直な磁束密度成分を検出することによって角度検出が行われる角度センサ用磁石構造体であって、前記境界領域は、少なくとも前記磁束検出手段が横切る位置において永久磁石の周方向に対して斜めに形成されていることを特徴とする。   In order to achieve the above-mentioned object, a magnet structure for an angle sensor according to the present invention comprises a permanent magnet having a cylindrical shape magnetized in a plurality of poles, and a magnetic flux detection means arranged to face the permanent magnet is the permanent magnet. Magnet structure for angle sensor in which angle detection is performed by detecting magnetic flux density components perpendicular to the magnetic pole surface of the permanent magnet, in which different magnetic poles of the magnet move relative to each other in the circumferential direction across adjacent boundary regions. And the said boundary area | region is formed diagonally with respect to the circumferential direction of a permanent magnet at least in the position which the said magnetic flux detection means crosses.

また、本発明の角度センサは、複数極に着磁された円筒形状を有する永久磁石と、前記永久磁石に対向配置され前記永久磁石の互いに異なる磁極が隣接する境界領域を横切って周方向に相対的に移動し、前記永久磁石の磁極面に垂直な磁束密度成分を検出することによって角度検出を行う磁束検出手段とを備えた角度センサであって、前記境界領域は、少なくとも前記磁束検出手段が横切る位置において永久磁石の周方向に対して斜めに形成されていることを特徴とする。   In addition, the angle sensor of the present invention has a cylindrical permanent magnet magnetized with a plurality of poles and a circumferential direction across a boundary region where the permanent magnets are arranged opposite to each other and different magnetic poles of the permanent magnet are adjacent to each other. And a magnetic flux detecting means for detecting an angle by detecting a magnetic flux density component perpendicular to the magnetic pole surface of the permanent magnet, wherein the boundary region is at least provided by the magnetic flux detecting means. It is characterized in that it is formed obliquely with respect to the circumferential direction of the permanent magnet at the crossing position.

本発明の角度センサ用磁石構造体及び角度センサにおいては、互いに異なる磁極が隣接する磁極の境界領域が磁束検出手段の移動方向に対して斜めに形成されていることが大きな特徴点である。境界領域を斜めに形成することで、直線性(リニアリティ)の向上が実現され、検出可能な角度範囲が大幅に拡大される。検出可能な角度範囲を拡大するための構成としては、前記境界領域の方向の変更のみで済み、着磁も容易で着磁治具も簡単なもので済む。また、例えば傾斜角度を調整することにより、磁束検出素子の出力調整も容易に行える。   A major feature of the angle sensor magnet structure and the angle sensor according to the present invention is that the boundary region of magnetic poles adjacent to different magnetic poles is formed obliquely with respect to the moving direction of the magnetic flux detection means. By forming the boundary region diagonally, the linearity is improved and the detectable angular range is greatly expanded. As a configuration for expanding the detectable angle range, it is only necessary to change the direction of the boundary region, the magnetization is easy, and the magnetizing jig is simple. Further, for example, by adjusting the tilt angle, the output of the magnetic flux detection element can be easily adjusted.

なお、磁極を斜めに配置する例としては、先の特許文献3記載の位置センサ装置を挙げることができるが、前述の通り、特許文献3記載の発明では、斜めに配置されるN極の両側にS極を配置することが必要であり、磁束ガイドで磁極面に平行な方向へ磁束をホール素子に誘導し、当該ホール素子をN極領域の長手方向に移動することによりN極領域の幅方向での位置が変化し、前記2つのS極の影響が変化することによる磁束ガイドで誘導される磁束密度の変化に基づいて位置検出を行うというのが基本原理である。これに対して、本発明では、互いに異なる磁極が隣接する磁極の境界領域を横切って磁束検出手段が移動し、永久磁石の磁極面に垂直な磁束密度成分を検出することが前提で、境界領域を挟んだ2極間の磁界変化を利用するというのが基本原理であり、本質的な技術思想が大きく異なる。   In addition, as an example of arranging the magnetic poles diagonally, the position sensor device described in Patent Document 3 can be given. As described above, in the invention described in Patent Document 3, both sides of the N pole arranged diagonally are provided. It is necessary to arrange the S pole at the center, and the magnetic flux is guided to the Hall element in the direction parallel to the magnetic pole surface by the magnetic flux guide, and the Hall element is moved in the longitudinal direction of the N pole area, thereby moving the width of the N pole area. The basic principle is that the position is detected based on the change in magnetic flux density induced by the magnetic flux guide due to the change in the position in the direction and the influence of the two south poles. On the other hand, in the present invention, it is assumed that the magnetic flux detecting means moves across the boundary area between adjacent magnetic poles and different magnetic poles detect the magnetic flux density component perpendicular to the magnetic pole surface of the permanent magnet. The basic principle is to use the change in the magnetic field between two poles with a gap between them.

本発明の角度センサ用磁石構造体においては、互いに異なる磁極が隣接する境界領域を斜めに形成しているので、当該境界領域において合成磁界の直線性(リニアリティ)を高め、検出可能な角度範囲を拡大することが可能である。したがって、本発明の磁石構造体を用いることで、広範な角度範囲に亘って角度検出が可能な角度センサを提供することが可能である。また、本発明によれば、装置構成を簡略化することが可能であり、コストの低減を図ることも可能である。   In the magnet structure for an angle sensor according to the present invention, the boundary region where the different magnetic poles are adjacent to each other is formed obliquely, so that the linearity (linearity) of the combined magnetic field is enhanced in the boundary region and the detectable angle range is increased. It is possible to enlarge. Therefore, it is possible to provide an angle sensor capable of detecting an angle over a wide range of angles by using the magnet structure of the present invention. In addition, according to the present invention, the device configuration can be simplified and the cost can be reduced.

以下、本発明を適用した角度センサ用磁石構造体及びこれを用いた角度センサについて、図面を参照して詳細に説明する。   Hereinafter, a magnet structure for an angle sensor to which the present invention is applied and an angle sensor using the same will be described in detail with reference to the drawings.

図1は、本実施形態の角度センサ用磁石構造体(永久磁石1)における着磁状態を示すものである。角度センサ用磁石構造体を構成する永久磁石1は、ここでは円筒形状を有する永久磁石であり、上下に分割される形で多極着磁(2極着磁)されている。すなわち、図中上側部分の表面がN極2となるように着磁されるとともに、図中下側部分の表面がS極3となるように着磁されている。   FIG. 1 shows a magnetized state in the magnet structure for an angle sensor (permanent magnet 1) of the present embodiment. The permanent magnet 1 constituting the magnet structure for the angle sensor is a permanent magnet having a cylindrical shape here, and is multipolarly magnetized (bipolar magnetized) so as to be divided vertically. That is, the surface of the upper part in the figure is magnetized so as to be the N pole 2 and the surface of the lower part in the figure is magnetized so as to be the S pole 3.

多極着磁(2極着磁)の場合、前記N極2とS極3の境界部分には、いわゆるニュートラルゾーン(無着磁領域4)が発生するが、これはN極2とS極3の境界において不可避なものである。なお、前記N極2とS極3を複数個(2個)の永久磁石を組み合わせて構成することで、無着磁領域4を実質的に発生させなくすることも可能である。本実施形態の角度センサ用磁石構造体(永久磁石1)においては、後述の磁束検出手段が横切る位置において、前記無着磁領域4が永久磁石1の周方向(図中、矢印X方向)に対して斜めに形成されている。   In the case of multipolar magnetization (bipolar magnetization), a so-called neutral zone (non-magnetized region 4) is generated at the boundary between the N pole 2 and the S pole 3, which is the N pole 2 and the S pole. It is inevitable at the boundary of three. The non-magnetized region 4 can be substantially prevented from being generated by combining the N pole 2 and the S pole 3 by combining a plurality (two) of permanent magnets. In the angle sensor magnet structure (permanent magnet 1) of the present embodiment, the non-magnetized region 4 extends in the circumferential direction of the permanent magnet 1 (in the direction of the arrow X in the figure) at a position crossed by a magnetic flux detection means described later. On the other hand, it is formed obliquely.

具体的には、本実施形態において、前記無着磁領域4は、円筒形状を有する永久磁石1の斜め切断面の外周に沿って永久磁石1の周面を1周する形で形成されている。また、互いに異なる前記N極2とS極3が前記無着磁領域4を挟んで隣接し、境界領域4Aを構成している。図2は、前記永久磁石1の展開図である。前記境界領域4Aを斜め切断面の外周に沿って形成することにより、磁束検出手段5が横切る位置において、境界領域4Aが永久磁石1の周方向X(すなわち、磁束検出手段5の移動方向)に対して斜めに形成されることになる。   Specifically, in the present embodiment, the non-magnetized region 4 is formed so as to make one round of the peripheral surface of the permanent magnet 1 along the outer periphery of the oblique cut surface of the permanent magnet 1 having a cylindrical shape. . Further, the N pole 2 and the S pole 3 which are different from each other are adjacent to each other with the non-magnetized region 4 interposed therebetween, thereby forming a boundary region 4A. FIG. 2 is a development view of the permanent magnet 1. By forming the boundary area 4A along the outer periphery of the oblique cut surface, the boundary area 4A is arranged in the circumferential direction X of the permanent magnet 1 (that is, the moving direction of the magnetic flux detection means 5) at the position where the magnetic flux detection means 5 crosses. On the other hand, it is formed obliquely.

前記磁束検出手段5による角度検出においては、磁束密度の直線変化領域の範囲が広いほど検出可能角度範囲γが広くなる。また、磁束密度の直線変化領域の直線性(以下、リニアリティと称する。)が優れるほど、簡単な演算処理で正確な角度検出が可能になる。磁束密度の直線変化領域のリニアリティが低い場合、表面磁束密度波形に応じた煩雑な演算をしなければ正確な角度検出は難しい。   In the angle detection by the magnetic flux detecting means 5, the detectable angle range γ becomes wider as the range of the magnetic flux density linear change region is wider. In addition, as the linearity of the linear change region of magnetic flux density (hereinafter referred to as linearity) is improved, more accurate angle detection can be performed with simple arithmetic processing. When the linearity of the linear change region of the magnetic flux density is low, accurate angle detection is difficult unless a complicated calculation according to the surface magnetic flux density waveform is performed.

そこで本実施形態においては、図1及び図2に示すように、前記永久磁石1において、境界領域4Aを磁束検出手段5の移動方向に対して斜めに形成することで、永久磁石1の各磁極(N極2及びS極3)における発生磁界を低下させずに、磁束密度の直線変化領域の幅を広げ、検出可能角度範囲γを広げるようにしている。   Therefore, in the present embodiment, as shown in FIGS. 1 and 2, in the permanent magnet 1, the boundary region 4 </ b> A is formed obliquely with respect to the moving direction of the magnetic flux detection means 5, thereby allowing each magnetic pole of the permanent magnet 1. Without reducing the generated magnetic field at (N pole 2 and S pole 3), the width of the linear change region of the magnetic flux density is widened to widen the detectable angle range γ.

ここで、前記境界領域4Aの傾斜角度θは、前記永久磁石の外径をDとした場合、前記磁束検出手段5の移動方向(図2中、水平方向)に対して0.5≦D・tanθ≦5.0を満たすとすることが好ましく、1.0≦D・tanθ≦2.0とすることがより好ましい。D・tanθが0.5未満であると、境界領域4A上での磁束密度が低くなり、検出が困難になるおそれがある。逆に、前記D・tanθが5.0を越えると、リニアリティの向上が不十分なものとなり、検出可能角度範囲γが狭くなる。   Here, the inclination angle θ of the boundary region 4A is 0.5 ≦ D · with respect to the moving direction of the magnetic flux detecting means 5 (horizontal direction in FIG. 2), where D is the outer diameter of the permanent magnet. It is preferable to satisfy tan θ ≦ 5.0, and it is more preferable to satisfy 1.0 ≦ D · tan θ ≦ 2.0. If D · tan θ is less than 0.5, the magnetic flux density on the boundary region 4A becomes low, which may make detection difficult. On the other hand, when D · tan θ exceeds 5.0, the linearity is not sufficiently improved, and the detectable angle range γ is narrowed.

前記無着磁領域4の幅wは、任意に設計することができるが、0.0mm〜2.5mmとすることが好ましく、0.5mm〜2.0mmとすることがより好ましい。前記無着磁領域4の幅wが2.5mmを越えると、発生する磁束が低下するおそれがある。   The width w of the non-magnetized region 4 can be arbitrarily designed, but is preferably 0.0 mm to 2.5 mm, and more preferably 0.5 mm to 2.0 mm. If the width w of the non-magnetized region 4 exceeds 2.5 mm, the generated magnetic flux may be reduced.

本発明者らは、種々検討を重ねた結果、境界領域4Aを斜めに形成することが、磁束密度の直線変化領域の幅を広げ、検出可能角度範囲γを拡大する上で極めて有効であることを見出すに至った。具体的には、以下に記載するような実験を行い、前記境界領域4Aを斜めに形成することの効果を確認した。   As a result of various studies, the present inventors have found that forming the boundary region 4A diagonally is extremely effective in expanding the width of the linear change region of the magnetic flux density and expanding the detectable angle range γ. I came to find. Specifically, an experiment as described below was performed, and the effect of forming the boundary region 4A obliquely was confirmed.

実験に際しては、永久磁石として円筒状のNdFeB系ボンド磁石を用い、これを2極着磁した。用いた永久磁石は、外径32mm、内径30mm、高さ6mm、厚さが1mmである。前記2極着磁に際しては、無着磁領域の幅を0.8mm〜4.0mm、傾斜角度θを5°〜45°とし、ホール素子を磁束検出手段として回転に伴う磁束密度の変化を調べた。結果を図3〜図5に示す。図3〜図5において、比較のため、傾斜角度θを90°(磁束検出手段の移動方向と境界領域を構成する無着磁領域が直交)とした場合についての測定結果も併せて示す。また、傾斜角度θに対するD・tanθの値を表1に示す。   In the experiment, a cylindrical NdFeB-based bond magnet was used as a permanent magnet, and this was two-pole magnetized. The used permanent magnet has an outer diameter of 32 mm, an inner diameter of 30 mm, a height of 6 mm, and a thickness of 1 mm. When the two-pole magnetization is performed, the width of the non-magnetized region is set to 0.8 mm to 4.0 mm, the inclination angle θ is set to 5 ° to 45 °, and the change in the magnetic flux density due to the rotation is examined using the Hall element as the magnetic flux detection means. It was. The results are shown in FIGS. In FIG. 3 to FIG. 5, for comparison, the measurement results when the inclination angle θ is 90 ° (the direction of movement of the magnetic flux detection means and the non-magnetized region constituting the boundary region are orthogonal) are also shown. Table 1 shows the values of D · tan θ with respect to the inclination angle θ.

Figure 2008241368
Figure 2008241368

図3では、本発明に基づいて無着磁領域の幅w=1.5mm、傾斜角度θ=3°、D・tanθ=1.68とした場合における磁束密度の変化を、従来例に相当する傾斜角度θ=90°とした場合の磁束密度の変化と比較することができる。図3から明らかなように、境界領域を斜めに形成した場合に直線性(リニアリティ)が格段に向上しており、広範囲に亘って直線性が維持されている。これに対して、境界領域を磁束検出手段の移動方向と略直交して形成した場合には、直線性が低下し、且つ検出可能角度範囲γが狭い。したがって、境界領域を斜めに形成することが、検出角度範囲γを拡大する上で有利であることが実証された。   In FIG. 3, the change in the magnetic flux density when the width w of the non-magnetized region is 1.5 mm, the tilt angle θ is 3 °, and D · tan θ is 1.68 according to the present invention corresponds to the conventional example. This can be compared with the change in magnetic flux density when the tilt angle θ is 90 °. As is apparent from FIG. 3, when the boundary region is formed obliquely, the linearity is remarkably improved and the linearity is maintained over a wide range. On the other hand, when the boundary region is formed substantially orthogonal to the moving direction of the magnetic flux detection means, the linearity is lowered and the detectable angle range γ is narrow. Therefore, it has been proved that forming the boundary region diagonally is advantageous in expanding the detection angle range γ.

図4では、本発明に基づく無着磁領域の幅wを変えた場合を比較している。図4から明らかなように、無着磁領域の幅wが大きくなると発生する磁束が小さくなっており、無着磁領域の幅wをある範囲に設定することが発生する磁束を確保する上で有利であることが実 証された。さらに、図5では、本発明に基づくD・tanθを変えた場合を比較している。図5から明らかなように、D・tanθが小さくなると発生する磁束が小さくなっており、D・tanθをある範囲に設定することが発生する磁束を確保する上で有利であることが実証された。   FIG. 4 compares the case where the width w of the non-magnetized region according to the present invention is changed. As is clear from FIG. 4, when the width w of the non-magnetized region increases, the generated magnetic flux decreases, and in order to secure the magnetic flux generated by setting the width w of the non-magnetized region within a certain range. It proved to be advantageous. Furthermore, in FIG. 5, the case where D * tan (theta) based on this invention is changed is compared. As is clear from FIG. 5, the generated magnetic flux decreases as D · tan θ decreases, and it has been demonstrated that setting D · tan θ within a certain range is advantageous in securing the generated magnetic flux. .

前述のように境界領域4Aが斜めに形成された永久磁石1は、1つの円筒状の磁石を多極着磁(2極着磁)することによって実現することができる。例えば、図6に示すように着磁コイル6を巻回し、当該着磁コイル6に電流を流して着磁を行うことで、図1及び図2に示すような着磁を行うことが可能である。あるいは、複数枚(2枚)の永久磁石を組み合わせて構成することも可能である。この場合には、組み合わされる永久磁石間のギャップが前記無着磁領域4に相当し、その幅wは実質的に0mmになる。   As described above, the permanent magnet 1 in which the boundary region 4A is formed obliquely can be realized by performing multipolar magnetization (bipolar magnetization) on one cylindrical magnet. For example, the magnetizing coil 6 is wound as shown in FIG. 6, and a current is passed through the magnetizing coil 6 to perform the magnetizing, whereby the magnetizing as shown in FIGS. 1 and 2 can be performed. is there. Alternatively, a plurality (two) of permanent magnets can be combined. In this case, the gap between the combined permanent magnets corresponds to the non-magnetized region 4 and its width w is substantially 0 mm.

本実施形態の角度センサ用磁石構造体(永久磁石1)を角度センサに用いる場合、発生する磁束をなるべく大きくして検出感度を向上させる必要がある。したがって、使用する永久磁石1は、発生する磁力が大きい希土類磁石により形成されていることが好ましい。特に、高磁気特性であるR−T−B系(Rは希土類元素、Tは遷移金属元素、Bはホウ素である。)ボンド磁石及び焼結磁石や、Sm−Co系焼結磁石等が好ましい。また、本発明には、円筒形状の磁石を使用するため、上記組成系の磁石であり、且つ、等方性磁石またはラジアルリング磁石を用いることが好ましい。前記磁石は着磁に対する自由度が高いため、本発明のようにニュートラル傾斜部または複数のニュートラル傾斜部を有する場合に有効である。   When the angle sensor magnet structure (permanent magnet 1) of this embodiment is used for an angle sensor, it is necessary to increase the generated magnetic flux as much as possible to improve the detection sensitivity. Therefore, it is preferable that the permanent magnet 1 to be used is formed of a rare earth magnet that generates a large magnetic force. In particular, an R-T-B system (R is a rare earth element, T is a transition metal element, and B is boron) having a high magnetic property, a bonded magnet and a sintered magnet, an Sm-Co-based sintered magnet, and the like are preferable. . Further, in the present invention, since a cylindrical magnet is used, it is preferable to use an isotropic magnet or a radial ring magnet which is a magnet of the above composition system. Since the magnet has a high degree of freedom for magnetization, it is effective when it has a neutral inclined portion or a plurality of neutral inclined portions as in the present invention.

図7は、前述の角度センサ用磁石構造体(永久磁石1)を用いた角度センサの構成例を示すものである。角度センサは、前述の永久磁石1と、永久磁石1の周面に沿って移動し永久磁石1の磁界を検出する磁束検出手段5から構成される。前記磁束検出手段5としては、ホール素子の他、MRセンサ等も用いることができる。ホール素子による検出では、直流電流を印加することで、磁束密度に比例した電圧を出力することができるため、回路が簡単になり、また、停止された位置でも永久磁石1からの磁束によって検出が可能となる。   FIG. 7 shows a configuration example of an angle sensor using the above-described angle sensor magnet structure (permanent magnet 1). The angle sensor includes the aforementioned permanent magnet 1 and magnetic flux detection means 5 that moves along the peripheral surface of the permanent magnet 1 and detects the magnetic field of the permanent magnet 1. As the magnetic flux detection means 5, an MR sensor or the like can be used in addition to a Hall element. In the detection by the Hall element, since a voltage proportional to the magnetic flux density can be output by applying a direct current, the circuit is simplified, and the detection is performed by the magnetic flux from the permanent magnet 1 even at the stopped position. It becomes possible.

図7に示す角度センサにおいて、前記磁束検出手段5は、前記境界領域4Aを横切る方向(円筒状の永久磁石1の周方向)に移動し、検出された磁界に基づいて位置を検出する。したがって、図8に示すように、回転角αを検出することが可能であり、角度センサとして機能する。例えば、前記永久磁石1を回転軸に装着し、前記磁束検出手段5によって角度検出を行えば、回転軸の回転角度を検出することが可能である。この時、永久磁石1と磁束検出手段5が平行に相対的に回転するため、可動手段が一軸であることから簡易な角度センサとすることが可能なる。   In the angle sensor shown in FIG. 7, the magnetic flux detection means 5 moves in a direction crossing the boundary region 4A (a circumferential direction of the cylindrical permanent magnet 1), and detects a position based on the detected magnetic field. Therefore, as shown in FIG. 8, the rotation angle α can be detected and functions as an angle sensor. For example, if the permanent magnet 1 is mounted on a rotating shaft and the angle is detected by the magnetic flux detection means 5, the rotation angle of the rotating shaft can be detected. At this time, since the permanent magnet 1 and the magnetic flux detection means 5 rotate relatively in parallel, the movable means is uniaxial, so that a simple angle sensor can be obtained.

前記角度センサにおいては、磁束検出手段5が永久磁石1に対して相対移動し、各角度位置において検出される磁束密度に基づいて回転角αを算出する。この場合、前記永久磁石1を固定し磁束検出手段5を移動するようにしても良いし、逆に磁束検出手段5を固定し永久磁石1を移動するようにしてもよい。   In the angle sensor, the magnetic flux detection means 5 moves relative to the permanent magnet 1 and calculates the rotation angle α based on the magnetic flux density detected at each angular position. In this case, the permanent magnet 1 may be fixed and the magnetic flux detection means 5 may be moved. Conversely, the magnetic flux detection means 5 may be fixed and the permanent magnet 1 may be moved.

また、磁束検出手段5を複数配置して永久磁石1の全周に亘り角度検出を行うことも可能である。この場合、例えば、図9に示すように、第1の磁束検出手段5Aと第2の磁束検出手段5Bの間に90°の位相差を持たせる。すなわち、第1の磁束検出手段5Aと第2の磁束検出手段5Bが90°の角度差を維持したまま一体的に移動するように設置する。   It is also possible to arrange a plurality of magnetic flux detection means 5 and perform angle detection over the entire circumference of the permanent magnet 1. In this case, for example, as shown in FIG. 9, a 90 ° phase difference is provided between the first magnetic flux detection means 5A and the second magnetic flux detection means 5B. That is, the first magnetic flux detection means 5A and the second magnetic flux detection means 5B are installed so as to move integrally while maintaining an angle difference of 90 °.

このように第1の磁束検出手段5Aと第2の磁束検出手段5Bを設置して、図9の矢印方向に永久磁石1の周囲を1回転させた場合、各磁束検出手段5A,5Bからは図10に示すような出力が得られる。図10において、出力Aは第1の磁束検出手段5Aからの出力、出力Bは第2の磁束検出手段5Bからの出力である。ここで、例えばいずれか一方の磁束検出手段5A,5Bの出力が所定の閾値を越えた場合、他方の磁束検出手段5A,5Bからの出力に基づいて角度検出を行うようにすれば、360°全てについて角度検出が可能である。図10に示す例では、0°〜45°、135°〜225°、315°〜360°については、磁束検出手段5Aからの出力に基づいて角度検出を行う。45°〜135°、225°〜315°については、磁束検出手段5Bからの出力に基づいて角度検出を行う。なお、ここでは検出手段が2つ設置されている場合について説明したが、必要に応じて、複数の傾斜部を持つように着磁し、2つ以上の検出手段を用いて360°角度検出とすることも可能である。   In this way, when the first magnetic flux detection means 5A and the second magnetic flux detection means 5B are installed and the periphery of the permanent magnet 1 is rotated once in the direction of the arrow in FIG. 9, the magnetic flux detection means 5A, 5B An output as shown in FIG. 10 is obtained. In FIG. 10, an output A is an output from the first magnetic flux detection means 5A, and an output B is an output from the second magnetic flux detection means 5B. Here, for example, when the output of one of the magnetic flux detection means 5A, 5B exceeds a predetermined threshold, if angle detection is performed based on the output from the other magnetic flux detection means 5A, 5B, 360 ° Angle detection is possible for all. In the example shown in FIG. 10, for 0 ° to 45 °, 135 ° to 225 °, and 315 ° to 360 °, angle detection is performed based on the output from the magnetic flux detection means 5A. For 45 ° to 135 ° and 225 ° to 315 °, angle detection is performed based on the output from the magnetic flux detection means 5B. Here, the case where two detection means are installed has been described. However, if necessary, the detector is magnetized so as to have a plurality of inclined portions, and two or more detection means are used to detect the 360 ° angle. It is also possible to do.

以上の構成を有する角度センサ用磁石構造体及び角度センサにおいては、磁極間の境界領域4Aを斜めに形成しているので、境界領域4Aを挟んだ磁極間領域において合成磁界の直線性(リニアリティ)を高めることが可能であり、検出可能な角度範囲γを大幅に拡大することが可能である。また、円筒状の永久磁石1を斜め断面を境に2極着磁するだけで良いので、装置構成も簡便なもので済み、装置コストを低減する上でも有利である。   In the angle sensor magnet structure and angle sensor having the above-described configuration, the boundary region 4A between the magnetic poles is formed obliquely, and thus the linearity of the combined magnetic field (linearity) in the region between the magnetic poles across the boundary region 4A. And the detectable angular range γ can be greatly expanded. In addition, since the cylindrical permanent magnet 1 need only be two-pole magnetized with an oblique cross section as a boundary, the apparatus configuration is simple, which is advantageous in reducing the apparatus cost.

なお、本発明の角度センサ用磁石構造体及び角度センサは、前記実施形態に限られるものではなく、種々の変更が可能である。例えば、先の実施形態においては、境界領域4Aを円筒状の永久磁石1の斜め切断面の外周に沿う形で形成したが、図11に示すように、境界領域4Aを螺旋状に形成することも可能である。この場合には、螺旋状の無着磁領域4aの他、永久磁石1の周方向と直交する無着磁領域4bも形成されることになるが、角度検出を行う上で、前記無着磁領域4bの存在はほとんど影響が無い。図11に示すような着磁は、一括して行うことは難しいが、例えばN極部分とS極部分をラバー磁石等により個別に形成し、これを組み合わせることで作製することが可能である。   In addition, the magnet structure for angle sensors and angle sensor of this invention are not restricted to the said embodiment, A various change is possible. For example, in the previous embodiment, the boundary region 4A is formed along the outer periphery of the oblique cut surface of the cylindrical permanent magnet 1, but the boundary region 4A is formed in a spiral shape as shown in FIG. Is also possible. In this case, in addition to the spiral non-magnetized region 4a, a non-magnetized region 4b orthogonal to the circumferential direction of the permanent magnet 1 is also formed. The presence of the region 4b has almost no effect. Although it is difficult to perform magnetization as shown in FIG. 11 in a lump, for example, the N pole portion and the S pole portion can be individually formed with a rubber magnet or the like, and can be manufactured by combining them.

本発明を適用した角度センサ用磁石構造体(永久磁石)の一例を示す概略斜視図である。It is a schematic perspective view which shows an example of the magnet structure (permanent magnet) for angle sensors to which this invention is applied. 図1に示す永久磁石の展開図である。It is an expanded view of the permanent magnet shown in FIG. 無着磁領域の幅w=1.5mm、傾斜角度θ=3°、D・tanθ=1.68とした場合における磁束密度の変化を、従来例に相当する傾斜角度θ=90°(w=0.8mm〜4.0mm)とした場合の磁束密度の変化と比較して示す特性図である。The change in magnetic flux density when the width w of the non-magnetized region is 1.5 mm, the tilt angle θ is 3 °, and D · tan θ is 1.68. The tilt angle θ is equal to 90 ° (w = It is a characteristic diagram shown in comparison with the change of the magnetic flux density in the case of 0.8 mm to 4.0 mm). 無着磁領域の傾斜角度θを3°に固定し、幅wを0.8mm〜4.0mmとした場合における磁束密度の変化を示す特性図である。FIG. 6 is a characteristic diagram showing changes in magnetic flux density when the tilt angle θ of the non-magnetized region is fixed at 3 ° and the width w is 0.8 mm to 4.0 mm. 無着磁領域の幅wを1.5mmに固定し、傾斜角度θを1°〜45°とした場合における磁束密度の変化を示す特性図である。It is a characteristic view showing a change in magnetic flux density when the width w of the non-magnetized region is fixed to 1.5 mm and the inclination angle θ is 1 ° to 45 °. 円筒形状を有する永久磁石を2極着磁するための着磁方法の一例を示す模式的な斜視図である。It is a typical perspective view which shows an example of the magnetization method for carrying out 2 pole magnetization of the permanent magnet which has a cylindrical shape. 本発明を適用した角度センサの一例を示す概略斜視図である。It is a schematic perspective view which shows an example of the angle sensor to which this invention is applied. 図7に示す角度センサにおける磁束検出手段の移動状態を示す概略平面図である。It is a schematic plan view which shows the movement state of the magnetic flux detection means in the angle sensor shown in FIG. 2つの磁束検出手段の設置状態の一例を永久磁石を展開して示す図である。It is a figure which expands and shows an example of the installation state of two magnetic flux detection means. 2つの磁束検出手段からの出力を示す図である。It is a figure which shows the output from two magnetic flux detection means. 角度センサ用磁石構造体(永久磁石)の他の例を示す概略斜視図である。It is a schematic perspective view which shows the other example of the magnet structure (permanent magnet) for angle sensors.

符号の説明Explanation of symbols

1 永久磁石、2 N極、3 S極、4 無着磁領域、4A 境界領域、5,5A,5B 磁束検出手段、6 着磁コイル DESCRIPTION OF SYMBOLS 1 Permanent magnet, 2 N pole, 3 S pole, 4 Non-magnetization area | region, 4 A boundary area | region, 5, 5 A, 5 B Magnetic flux detection means, 6 Magnetization coil

Claims (7)

複数極に着磁された円筒形状を有する永久磁石を備え、前記永久磁石に対向配置された磁束検出手段が前記永久磁石の互いに異なる磁極が隣接する境界領域を横切って周方向に相対的に移動し、前記永久磁石の磁極面に垂直な磁束密度成分を検出することによって角度検出が行われる角度センサ用磁石構造体であって、
前記境界領域は、少なくとも前記磁束検出手段が横切る位置において永久磁石の周方向に対して斜めに形成されていることを特徴とする角度センサ用磁石構造体。
A permanent magnet having a cylindrical shape magnetized with a plurality of poles, and a magnetic flux detecting means arranged opposite to the permanent magnet relatively moves in a circumferential direction across a boundary region where different magnetic poles of the permanent magnet are adjacent to each other. An angle sensor magnet structure in which angle detection is performed by detecting a magnetic flux density component perpendicular to the magnetic pole surface of the permanent magnet,
The boundary structure is formed at an angle with respect to the circumferential direction of the permanent magnet at least at a position crossed by the magnetic flux detection means.
前記境界領域が円筒形状の永久磁石の斜め切断面の外周に沿う形で永久磁石の周面に形成されていることを特徴とする請求項1記載の角度センサ用磁石構造体。   2. The magnet structure for an angle sensor according to claim 1, wherein the boundary region is formed on the peripheral surface of the permanent magnet so as to follow the outer periphery of the oblique cut surface of the cylindrical permanent magnet. 前記境界領域の傾斜角度θが前記永久磁石の外径Dに対して0.5≦D・tanθ≦5なる関係を満たすことを特徴とする請求項1または2記載の角度センサ用磁石構造体。   3. The magnet structure for an angle sensor according to claim 1, wherein an inclination angle θ of the boundary region satisfies a relationship of 0.5 ≦ D · tan θ ≦ 5 with respect to an outer diameter D of the permanent magnet. 複数極に着磁された円筒形状を有する永久磁石と、前記永久磁石に対向配置され前記永久磁石の互いに異なる磁極が隣接する境界領域を横切って周方向に相対的に移動し、前記永久磁石の磁極面に垂直な磁束密度成分を検出することによって角度検出を行う磁束検出手段とを備えた角度センサであって、
前記境界領域は、少なくとも前記磁束検出手段が横切る位置において永久磁石の周方向に対して斜めに形成されていることを特徴とする角度センサ。
A permanent magnet having a cylindrical shape magnetized with a plurality of poles, and different permanent magnetic poles of the permanent magnet, which are opposed to the permanent magnet, move relative to each other in a circumferential direction across an adjacent boundary region. An angle sensor including magnetic flux detection means for detecting an angle by detecting a magnetic flux density component perpendicular to the magnetic pole surface,
The angle sensor, wherein the boundary region is formed obliquely with respect to a circumferential direction of the permanent magnet at least at a position crossed by the magnetic flux detection means.
前記境界領域が円筒形状の永久磁石の斜め切断面の外周に沿う形で永久磁石の周面に形成されていることを特徴とする請求項4記載の角度センサ。   The angle sensor according to claim 4, wherein the boundary region is formed on the peripheral surface of the permanent magnet so as to follow the outer periphery of the oblique cut surface of the cylindrical permanent magnet. 前記境界領域の傾斜角度θが前記永久磁石の外径Dに対して0.5≦D・tanθ≦5なる関係を満たすことを特徴とする請求項4または5記載の角度センサ。   6. The angle sensor according to claim 4, wherein an inclination angle θ of the boundary region satisfies a relationship of 0.5 ≦ D · tan θ ≦ 5 with respect to an outer diameter D of the permanent magnet. 前記磁束検出手段がホール素子であることを特徴とする請求項4から6のいずれか1項記載の角度センサ。   The angle sensor according to any one of claims 4 to 6, wherein the magnetic flux detection means is a Hall element.
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JP2017161365A (en) * 2016-03-09 2017-09-14 Tdk株式会社 Magnet and displacement detector
CN110048529A (en) * 2018-01-15 2019-07-23 江门市中磁机电有限公司 It is a kind of tiltedly to polar diameter to p-m rotor, preparation method and its motor

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JPH08136207A (en) * 1994-11-08 1996-05-31 Canon Inc Position detector
JP2005195471A (en) * 2004-01-07 2005-07-21 Tokai Rika Co Ltd Rotation angle detecting device

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JPH0611303A (en) * 1992-02-27 1994-01-21 Philips Gloeilampenfab:Nv Position sensor device
JPH08136207A (en) * 1994-11-08 1996-05-31 Canon Inc Position detector
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JP2017161365A (en) * 2016-03-09 2017-09-14 Tdk株式会社 Magnet and displacement detector
CN110048529A (en) * 2018-01-15 2019-07-23 江门市中磁机电有限公司 It is a kind of tiltedly to polar diameter to p-m rotor, preparation method and its motor
CN110048529B (en) * 2018-01-15 2024-05-14 汉宇集团股份有限公司 Oblique-pole radial permanent magnet rotor, preparation method and motor thereof

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