JP2003084007A - Rotation direction detecting device - Google Patents
Rotation direction detecting deviceInfo
- Publication number
- JP2003084007A JP2003084007A JP2001279431A JP2001279431A JP2003084007A JP 2003084007 A JP2003084007 A JP 2003084007A JP 2001279431 A JP2001279431 A JP 2001279431A JP 2001279431 A JP2001279431 A JP 2001279431A JP 2003084007 A JP2003084007 A JP 2003084007A
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- Prior art keywords
- magnet
- magnetic
- rotation
- detected
- detection element
- Prior art date
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- Transmission And Conversion Of Sensor Element Output (AREA)
Abstract
Description
【0001】[0001]
【発明が属する技術分野】本発明は、磁石と磁気検出素
子とを組み合わせた簡単な構成によって種々の回転体の
回転方向を検出する回転方向検出に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to rotation direction detection for detecting rotation directions of various rotating bodies with a simple structure in which a magnet and a magnetic detection element are combined.
【0002】[0002]
【発明の背景】従来、磁石と、この磁石による磁界の磁
束密度を電気信号に変換するホール素子などの磁気検出
素子とを組み合わせた構成は、機械的な変位量や変形量
などを非接触で検出できる簡易な検出手段として広く用
いられており、例えば、被検出回転体の回転角検出装置
(特開2001−59702号公報参照)や被検出移動
体のポジションセンサ(特開2001−74409号公
報参照)などが知られている。しかし、前記検出手段
は、被検出回転体の回転方向を検出することはできな
い。BACKGROUND OF THE INVENTION Conventionally, a structure in which a magnet and a magnetic detection element such as a Hall element for converting the magnetic flux density of a magnetic field generated by the magnet into an electric signal are combined has been used in a non-contact manner such as a mechanical displacement amount or a deformation amount. It is widely used as a simple detection means capable of detecting, for example, a rotation angle detection device for a rotating body to be detected (see JP 2001-59702 A) or a position sensor for a moving body to be detected (JP 2001-74409 A). (See) is known. However, the detection means cannot detect the rotation direction of the detected rotating body.
【0003】そこで、回転方向を検出できる磁石とし
て、図6(a)に示す磁石1が考えられる。この図にお
いて、磁石1は、長手方向の反転部を境界として磁極が
反転しており、その一方がN極の磁性部分1aで、他方
がS極の磁性部分1bとなるように着磁されている。磁
気検出素子2は磁石1の回転軌跡に近接して対向する位
置に配置され、被検出回転体の回転に伴って磁石1が同
図(a)の矢印方向に移動した場合には、磁気検出素子
2が磁石1によって生じた磁界の磁束密度を電気信号に
変換して、同図(b)に示すようなホール電圧を出力す
る。Therefore, a magnet 1 shown in FIG. 6A can be considered as a magnet capable of detecting the rotation direction. In this figure, the magnet 1 has its magnetic poles reversed with a longitudinal reversal portion as a boundary, and one of them is magnetized so that it is an N-pole magnetic portion 1a and the other is an S-pole magnetic portion 1b. There is. The magnetic detection element 2 is arranged at a position close to and facing the rotation locus of the magnet 1, and when the magnet 1 moves in the direction of the arrow in FIG. The element 2 converts the magnetic flux density of the magnetic field generated by the magnet 1 into an electric signal, and outputs a Hall voltage as shown in FIG.
【0004】磁気検出素子2のホール電圧は、両磁性部
分1a,1bの境界部分でゼロとなって極性が急激に反
転する。換言すると、磁石1における磁束密度が変化す
る部分、つまり、磁気検出素子2のホール電圧が変化す
る部分は、前記境界に対し両側の僅かな区間Aのみであ
る。そのため、被検出回転体の回転方向は、前記区間A
に相当する小さな回転角度の間でのみ検出できるだけで
あるから、この磁石1と磁気検出素子2とを組み合わせ
た構成は、被検出回転体の回転方向の検出手段として用
いることは難しい。なお、磁石1を長手方向に沿って磁
束密度が連続的に変化する分布に着磁することは、極め
て困難であって、実用化できない。The Hall voltage of the magnetic detection element 2 becomes zero at the boundary between the magnetic portions 1a and 1b, and the polarity is rapidly inverted. In other words, the portion where the magnetic flux density in the magnet 1 changes, that is, the portion where the Hall voltage of the magnetic detection element 2 changes is only a small section A on both sides of the boundary. Therefore, the rotation direction of the detected rotating body is the same as in the section A
Therefore, it is difficult to use the configuration in which the magnet 1 and the magnetic detection element 2 are combined as a means for detecting the rotational direction of the detected rotating body. It is extremely difficult to magnetize the magnet 1 in a distribution in which the magnetic flux density changes continuously along the longitudinal direction, which cannot be put to practical use.
【0005】そこで、本発明においては、被検出回転体
の回転方向を比較的広い回転角度の範囲にわたり回転す
る毎に確実に検出することのできる回転方向検出装置を
提供することを目的とする。SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a rotation direction detecting device capable of surely detecting the rotation direction of a rotating body to be detected each time it rotates over a relatively wide range of rotation angles.
【0006】[0006]
【課題を解決するための手段】前記目的を達成するため
に、本発明の回転方向検出装置は、所定の軸線の回りに
回転する被検出回転体の回転方向を検出する回転方向検
出装置であって、前記被検出回転体に固定されて前記被
検出回転体と一体に回転する磁石と、前記磁石の回転軌
跡に近接する位置に配置されて前記磁石により生じる磁
界の磁束密度を検出する磁気検出素子とを備え、前記磁
石は、前記被検出回転体の回転軌跡に対応して湾曲され
た帯状であって、円周方向の中間部分で磁極が反転する
反転部を有するように着磁されていると共に前記反転部
から前記円周方向の両端部に向かってそれぞれ前記磁気
検出素子に検出される磁束密度が連続的に増大するよう
に設定されていることを特徴とするIn order to achieve the above object, the rotation direction detecting device of the present invention is a rotation direction detecting device for detecting the rotation direction of a rotating body to be detected which rotates around a predetermined axis. And a magnet that is fixed to the detected rotating body and rotates integrally with the detected rotating body, and a magnetic detector that is arranged in a position close to the rotation locus of the magnet and detects the magnetic flux density of the magnetic field generated by the magnet. The magnet is magnetized so as to have a reversing portion in which a magnetic pole is reversed at an intermediate portion in a circumferential direction, the magnet being a strip shape curved corresponding to a rotation locus of the detected rotating body. In addition, the magnetic flux density detected by the magnetic detection element is set to continuously increase from the reversal portion toward both ends in the circumferential direction.
【0007】[0007]
【発明の実施の形態】以下、本発明の好ましい実施形態
について、図面を参照しながら説明する。図1および図
2は本発明の第1実施形態の回転方向検出装置を示す。
回転方向の検出対象となる被検出回転体3としては、回
転軸4と、この回転軸4に軸着されて軸線Cの回りに一
体に回転する回転円板7とを備えたものを例示してあ
る。回転方向検出装置は、回転円板7に接着手段などで
固着されて回転円板7と一体に回転する磁石8と、磁石
8に対し被検出回転体3の軸線C方向において磁石8の
回転軌跡に近接して相対向する配置でフレーム(図示せ
ず)に取り付けられた磁気検出素子2とを備えている。
なお、磁石8は、回転円板7に代えて、例えば、回転軸
4に軸着されたプレートなどに取り付けてもよい。つま
り、磁石8は被検出回転体3の所定の軸線Cの回りに一
体に回転するように取り付ければよい。BEST MODE FOR CARRYING OUT THE INVENTION Preferred embodiments of the present invention will be described below with reference to the drawings. 1 and 2 show a rotation direction detecting device according to a first embodiment of the present invention.
An example of the detected rotating body 3 to be detected in the rotating direction is one including a rotating shaft 4 and a rotating disk 7 that is attached to the rotating shaft 4 and integrally rotates around an axis C. There is. The rotation direction detecting device includes a magnet 8 fixed to the rotating disk 7 by an adhesive means or the like and rotating integrally with the rotating disk 7, and a rotation locus of the magnet 8 with respect to the magnet 8 in the direction of the axis C of the detected rotating body 3. And a magnetic detection element 2 attached to a frame (not shown) so as to closely face and face each other.
The magnet 8 may be attached to, for example, a plate axially attached to the rotary shaft 4 instead of the rotary disc 7. That is, the magnet 8 may be attached so as to integrally rotate around the predetermined axis C of the rotating body to be detected 3.
【0008】前記磁気検出素子2は、磁界の変化量を電
気的な変化量に変換することにより、磁石により生じる
磁界の磁束密度を検出する。磁気検出素子2としては、
たとえば、磁界の磁束密度に対応したホール電圧を出力
するホール素子または磁界の変化に応じて抵抗値が変化
するMR素子などを用いることができる。この実施形態
では、ホール素子と増幅回路とを一体化したホールIC
を用いる場合について説明する。したがって、磁気検出
素子2は、磁石8により生じる磁界の磁束密度を検出し
てホール電圧を出力する。The magnetic detection element 2 detects the magnetic flux density of the magnetic field generated by the magnet by converting the amount of change in the magnetic field into the amount of electrical change. As the magnetic detection element 2,
For example, a Hall element that outputs a Hall voltage corresponding to the magnetic flux density of the magnetic field or an MR element whose resistance value changes according to the change of the magnetic field can be used. In this embodiment, a Hall IC in which a Hall element and an amplifier circuit are integrated
The case of using will be described. Therefore, the magnetic detection element 2 detects the magnetic flux density of the magnetic field generated by the magnet 8 and outputs the Hall voltage.
【0009】前記磁石8は、回転方向に沿った角棒状の
第1および第2の磁性部分8a,8bからなる。前記両
磁性部分8a,8bは、円周方向(長手方向)に直交す
る前記軸線C方向に沿って着磁されており、一方の側面
がS極に他方の側面がN極に着磁されている。前記磁石
8は一対の前記磁性部分8a,8bを突き合せ部8cに
おいて互いに付き合せ接合して形成されている。ここ
で、前記第1の磁性部分8aと第2の磁性部分8bと
は、互いに反対方向に極性が設定されている。したがっ
て、前記突き合せ部8cにおいて、極性が反転してい
る。図2において、前記磁石8は、回転円板7における
90度の角度範囲の周縁部に沿った形状に湾曲された帯
状(回転方向に沿った角棒状)であって、長手方向の中
間の突き合せ部(反転部)8cで磁極が反転するように
着磁され、前記反転部8cを境界として、両側に第1お
よび第2の磁性部分8a,8bが形成されている。この
実施形態では、両磁性部分8a,8bにそれぞれ生じる
平行な磁力線の向きが中央の反転部8cで反転するよう
に着磁した場合を例示してある。但し、第1および第2
の磁性部分8a,8bは互いに相反する極性に着磁させ
ればよく、この点については、後述する第2ないし第4
実施形態についても同様である。なお、両磁性部分8
a,8bを一体とした(接合していない)1つの磁石で
磁石8を形成してもよい。The magnet 8 is composed of first and second rectangular rod-shaped magnetic portions 8a and 8b along the direction of rotation. The both magnetic portions 8a and 8b are magnetized along the axis C direction orthogonal to the circumferential direction (longitudinal direction), and one side surface is magnetized as an S pole and the other side surface is magnetized as an N pole. There is. The magnet 8 is formed by abutting and joining a pair of the magnetic portions 8a and 8b at a butting portion 8c. Here, the polarities of the first magnetic portion 8a and the second magnetic portion 8b are set in mutually opposite directions. Therefore, the polarity is reversed in the abutting portion 8c. In FIG. 2, the magnet 8 has a strip shape (a rectangular bar shape along the rotation direction) curved in a shape along the peripheral edge portion of the rotating disk 7 in the angle range of 90 degrees, and has an intermediate protrusion in the longitudinal direction. The magnetic poles are magnetized so that the magnetic poles are inverted at the matching portion (reversing portion) 8c, and first and second magnetic portions 8a and 8b are formed on both sides with the reversing portion 8c as a boundary. In this embodiment, a case is illustrated in which the directions of the parallel magnetic lines of force generated in both the magnetic portions 8a and 8b are magnetized so as to be inverted at the central inversion portion 8c. However, the first and second
The magnetic portions 8a and 8b of the above may be magnetized to have polarities opposite to each other.
The same applies to the embodiment. Both magnetic parts 8
The magnet 8 may be formed by one magnet in which a and 8b are integrated (not joined).
【0010】前記磁石8は、軸線C方向の厚みが反転部
8cで最も小さく、且つ反転部8cから磁石8の両端部
に向かってそれぞれ連続的に増大する形状を有してい
る。したがって、この磁石8では、両磁性部分8a,8
bが全体にわたり均一な密度に着磁されているが、厚み
が最も大きい両端部によって生じる磁界の強さが最も大
きくなって磁束密度が最も高くなり、両端部から反転部
8cに向けて磁束密度が連続的に低くなっている。磁気
検出素子2は、磁石8に対して軸線C方向側に配置され
ているので、磁石8の第2の磁性部分8bの端部(この
点を回転角度0°とする)から第1の磁性部分8aの端
部(この点を回転角度90°とする)までの全体につい
て、つまり、広い角度の範囲にわたって、図2(b)に
示すように、磁気検出素子2から出力するホール電圧が
負電圧から正電圧に向けて増大する。The magnet 8 has a shape in which the thickness in the direction of the axis C is the smallest at the reversing portion 8c and increases continuously from the reversing portion 8c toward both ends of the magnet 8. Therefore, in this magnet 8, both magnetic parts 8a, 8
b is magnetized to a uniform density throughout, but the strength of the magnetic field generated by both ends having the largest thickness becomes the highest and the magnetic flux density becomes the highest. Is continuously low. Since the magnetism detecting element 2 is arranged on the side of the magnet 8 in the direction of the axis C, the magnetism detecting element 2 moves from the end of the second magnetic portion 8b of the magnet 8 (this point is defined as a rotation angle of 0 °) to the first magnetism. As shown in FIG. 2B, the Hall voltage output from the magnetic detection element 2 is negative over the entire range up to the end of the portion 8a (this point is the rotation angle 90 °), that is, over a wide angle range. Voltage increases from positive voltage.
【0011】本実施形態では、磁石8の軸線C方向の厚
みが、反転部8cでもっとも小さく、且つ反転部8cか
ら両磁性部分8a,8bの両端部に向かってそれぞれ連
続的に増大する形状を有しているのに加えて、図2
(b)に明示するように、磁石8の両端部が最も小さな
間隙で磁気検出素子2に近接対向し、両端部から反転部
8cにいくに従って徐々に大きな間隙で磁気検出素子2
に対向するようになっているので、磁気検出素子2から
出力するホール電圧は、負電圧から正電圧に向けて比較
的大きな変化率で直線的に増大する。なお、磁石8は、
その長手方向の全体にわたり同一の間隙で磁気検出素子
2に対向するとともに、厚みが反転部8cでもっとも小
さく、且つ反転部8cから両磁性部分8a,8bの両端
部に向かってそれぞれ連続的に増大する形状を有してい
るだけでも、磁気検出素子2からは、負電圧から正電圧
に向けて直線的に増大するホール電圧を取り出すことが
できる。In this embodiment, the magnet 8 has a shape in which the thickness in the direction of the axis C is the smallest at the reversing portion 8c and continuously increases from the reversing portion 8c toward both ends of both the magnetic portions 8a and 8b. In addition to having FIG.
As clearly shown in (b), both ends of the magnet 8 closely oppose the magnetic detecting element 2 with the smallest gap, and the magnetic detecting element 2 gradually increases with a gap from both ends toward the reversing portion 8c.
The Hall voltage output from the magnetic detection element 2 linearly increases from the negative voltage to the positive voltage at a relatively large rate of change. The magnet 8 is
The magnetism detecting element 2 is opposed to the magnetic detecting element 2 with the same gap over the entire longitudinal direction, and the thickness is the smallest at the reversing portion 8c, and continuously increases from the reversing portion 8c to both ends of both the magnetic portions 8a and 8b. The Hall voltage that linearly increases from the negative voltage to the positive voltage can be taken out from the magnetic detection element 2 only by having the shape.
【0012】図2(a)に示すように、磁気検出素子2
から出力されるホール電圧は、演算部9のサンプリング
回路10においてサンプリングパルスによる一定周期で
サンプリングされる。増減検出部11は、サンプリング
回路10からのサンプリング値が増大または減少の何れ
であるかを判別して、回転方向検出信号を出力する。し
たがって、この実施形態の回転方向検出装置では、磁石
8と磁気検出素子2とを組み合わせた簡単な構成としな
がらも、帯状の磁石8の一端から他端の全体にわたり磁
束密度が連続して直線的に変化する磁界を発生させるこ
とができるので、磁石8の長さに対応した比較的大きな
回転角の範囲において、被検出回転体3が回転する毎に
その回転方向を確実に検出することができる。ここで、
図6(c)に示すように、1つの磁石1Aのみで、つま
り、極性を反転させないことも考えられる。しかし、こ
うすると、最大厚さTが本実施形態の2倍程度になる。
これに対し、図2(a)の本実施形態の磁石8は極性を
反転させているので、磁石8の最大厚さTmが薄くなる
から、装置のコンパクト化を図ることができる。なお、
この実施形態では、磁石8の厚みが、両端部から反転部
8cに向けて連続的に薄くなっていることから、図4の
実施形態よりも、トータルとしての厚みを薄く形成で
き、装置をコンパクト化できる利点がある。As shown in FIG. 2A, the magnetic detection element 2
The Hall voltage output from is sampled in the sampling circuit 10 of the calculation unit 9 at a constant cycle by a sampling pulse. The increase / decrease detector 11 determines whether the sampling value from the sampling circuit 10 is increasing or decreasing, and outputs a rotation direction detection signal. Therefore, in the rotation direction detection device of this embodiment, the magnetic flux density is continuous and linear from one end to the other end of the strip-shaped magnet 8 even though the magnet 8 and the magnetic detection element 2 are combined in a simple configuration. Since it is possible to generate a magnetic field that changes with time, it is possible to reliably detect the rotation direction of the detected rotating body 3 each time it rotates in a range of a relatively large rotation angle corresponding to the length of the magnet 8. . here,
As shown in FIG. 6 (c), it is also possible to use only one magnet 1A, that is, not reverse the polarity. However, in this case, the maximum thickness T becomes about twice as large as that in this embodiment.
On the other hand, since the polarity of the magnet 8 of the present embodiment shown in FIG. 2A is reversed, the maximum thickness Tm of the magnet 8 becomes thin, so that the device can be made compact. In addition,
In this embodiment, since the thickness of the magnet 8 is continuously reduced from both ends toward the reversal portion 8c, the total thickness can be made smaller than that of the embodiment of FIG. 4, and the device is compact. There is an advantage that can be realized.
【0013】図3は本発明の第2実施形態を示す。この
実施形態は、第1実施形態の変形例であって、磁気検出
素子2が磁石8に対し被検出回転体3の回転円板7の径
方向外側で近接して相対向する位置に配置されている。
前記磁石8は、回転円板7の回転方向に沿った角棒状の
第1および第2の磁性部分8a,8bからなる。前記磁
性部分8a,8bは、回転円板7の径方向に沿ってそれ
ぞれ着磁されている。たとえば、第1の磁性部分8aは
外周縁側がS極に中心C側がN極に着磁されており、第
2の磁性部分8bは外周縁側がN極に中心C側がS極に
着磁されている。前記磁石8は、一対の前記磁性部分8
a,8bにおいて、互いに付き合せ接合して形成されて
おり、したがって、第1の磁性部分8aと第2の磁性部
分8bとは、長手方向の中間の反転部8cで互いに反対
方向に極性が設定されている。図3(b)に示すよう
に、磁石8は、前記磁気検出素子2の配設位置の変更に
伴って、径方向の厚みが反転部8cでもっとも小さく、
且つ反転部8cから両磁性部分8a,8bの両端部に向
かってそれぞれ連続的に増大する形状を有している。な
お、磁石8の反転部8cは、磁石8の両端部よりも中心
C側に近づいており、前記磁気検出素子2との距離が磁
石8の両端部から反転部8cにかけて次第に大きくなる
ように設定されている。その他の構成は、第1実施形態
と同様であり、同一部分または相当部分に同一符号を付
して、その詳しい説明および図示を省略する。FIG. 3 shows a second embodiment of the present invention. This embodiment is a modification of the first embodiment, in which the magnetic detection element 2 is arranged at a position facing the magnet 8 on the outer side in the radial direction of the rotating disk 7 of the rotating body to be detected 3 and facing each other. ing.
The magnet 8 is composed of first and second rectangular rod-shaped magnetic portions 8a and 8b along the rotation direction of the rotating disk 7. The magnetic portions 8a and 8b are magnetized along the radial direction of the rotary disc 7. For example, the first magnetic portion 8a is magnetized so that the outer peripheral edge side is the S pole and the center C side is the N pole, and the second magnetic portion 8b is the outer peripheral edge side is the N pole and the center C side is the S pole. There is. The magnet 8 includes a pair of the magnetic parts 8
a and 8b are formed by butt-joining each other, and therefore, the first magnetic portion 8a and the second magnetic portion 8b have opposite polarities set in opposite directions at the middle inversion portion 8c in the longitudinal direction. Has been done. As shown in FIG. 3 (b), the magnet 8 has the smallest radial thickness in the reversing portion 8 c as the arrangement position of the magnetic detection element 2 is changed,
In addition, it has a shape that continuously increases from the reversal portion 8c toward both ends of both magnetic portions 8a and 8b. The inversion part 8c of the magnet 8 is closer to the center C side than both ends of the magnet 8, and the distance from the magnetism detecting element 2 is set to gradually increase from both ends of the magnet 8 to the inversion part 8c. Has been done. Other configurations are similar to those of the first embodiment, and the same portions or corresponding portions will be denoted by the same reference numerals and detailed description and illustration thereof will be omitted.
【0014】したがって、前述の第1実施形態と同様
に、被検出回転体3の回転に伴って磁石8がその一端か
ら他端に向けて磁気検出素子2に順次近接した場合に
は、負電圧から正電圧に向けて直線的に増大するホール
電圧が磁気検出素子2から出力されるので、第1実施形
態で説明したのと同様の効果を得られる。Therefore, as in the case of the first embodiment described above, when the magnet 8 sequentially approaches the magnetic detection element 2 from one end to the other end as the detected rotating body 3 rotates, a negative voltage is applied. Since the Hall voltage linearly increasing from 0 to positive voltage is output from the magnetic detection element 2, the same effect as described in the first embodiment can be obtained.
【0015】図4は本発明の第3実施形態を示す。この
実施形態では、磁気検出素子2が磁石8に対し被検出回
転体3の軸線C方向で近接して相対向する位置に配置さ
れている点において第1実施形態と同様であるが、帯状
の磁石8が、厚みが長手方向の全体にわたりほぼ同一
で、極性が反転する長手方向の反転部8cを屈曲点とし
て、両側が軸線C方向における磁気検出素子2の配置位
置に向けて屈曲された形状を有している。すなわち、磁
石8を構成する第1および第2の磁性部分8a,8b
は、回転円板7の回転方向に沿った角棒状に形成されて
おり、該磁性部分8a,8bは軸線C方向に沿って着磁
されている。一方、前記磁石8は、2つのスペーサ部材
12を介在して回転円板7に固着されている。FIG. 4 shows a third embodiment of the present invention. This embodiment is similar to the first embodiment in that the magnetic detection element 2 is arranged at a position close to and opposed to the magnet 8 in the direction of the axis C of the rotating body 3 to be detected. A shape in which the magnet 8 has substantially the same thickness over the entire length in the longitudinal direction, and both sides are bent toward the arrangement position of the magnetic detection element 2 in the direction of the axis C with the longitudinal reversal portion 8c where the polarity is reversed as the bending point. have. That is, the first and second magnetic portions 8a and 8b forming the magnet 8 are formed.
Are formed in a rectangular rod shape along the rotation direction of the rotating disk 7, and the magnetic portions 8a and 8b are magnetized along the axis C direction. On the other hand, the magnet 8 is fixed to the rotating disc 7 with two spacer members 12 interposed therebetween.
【0016】前記磁石8が回転に伴って磁気検出素子2
に対し一端から他端に向けて近接したときの磁石8と磁
気検出素子2との間隙は、極性が反転する長手方向の反
転部8cにおいて最も大きく、且つ反転部8cから両側
にいくにしたがって連続的に小さくなる。磁石8から磁
気検出素子2に作用する磁界の強さは前記間隙が小さい
程大きいので、第1実施形態と同様に、被検出回転体3
の回転に伴って磁石8がその一端から他端に向けて磁気
検出素子2に順次近接した場合には、負電圧から正電圧
に向けて直線的に増大するホール電圧が磁気検出素子2
から出力し、これにより、第1実施形態で説明したのと
同様の効果を得られる。それに加えて、この実施形態で
は、磁石8を全体にわたり同一の厚みとすることができ
るので、磁石8の成形が容易となる利点がある。As the magnet 8 rotates, the magnetic detection element 2
On the other hand, the gap between the magnet 8 and the magnetic detection element 2 when approaching from one end to the other end is the largest in the longitudinal reversing portion 8c where the polarity is reversed, and is continuous as going from the reversing portion 8c to both sides. Becomes smaller. The strength of the magnetic field acting on the magnetic detection element 2 from the magnet 8 is larger as the gap is smaller. Therefore, similarly to the first embodiment, the rotating body to be detected 3 is detected.
When the magnet 8 sequentially approaches the magnetic detection element 2 from its one end to the other end as the magnet rotates, the Hall voltage linearly increasing from the negative voltage to the positive voltage is applied to the magnetic detection element 2.
And the same effect as described in the first embodiment can be obtained. In addition to this, in this embodiment, since the magnet 8 can be made to have the same thickness throughout, there is an advantage that the magnet 8 can be easily molded.
【0017】図5は本発明の第4実施形態を示す。この
実施形態は、第3実施形態の変形例であって、磁気検出
素子2が磁石8に対し被検出回転体3の回転円板7の径
方向外側で近接して相対向する位置に配置されている点
において第3実施形態と相違する。この磁気検出素子2
の配設位置の変更に伴って、磁石8は、厚みが長手方向
の全体にわたりほぼ同一である点において第3実施形態
と同様であるが、極性が反転する長手方向の反転部8c
が回転円板7の外周縁から最も離間し、その反転部8c
から両端部に向けて回転円板7の外周縁に徐々に近接
し、両端部が外周縁に接した形状になっている。磁石8
は回転円板7の外周縁に近接した位置に配置されている
ので、回転に伴って磁気検出素子2に対し一端から他端
に向けて近接したときの磁石8と磁気検出素子2との間
隙は、極性が反転する長手方向の反転部8cにおいて最
も大きく、且つ反転部8cから両側にいくにしたがって
連続的に小さくなる。FIG. 5 shows a fourth embodiment of the present invention. This embodiment is a modification of the third embodiment, in which the magnetic detection element 2 is arranged at a position facing the magnet 8 on the outer side in the radial direction of the rotating disk 7 of the detected rotating body 3 and facing each other. It is different from the third embodiment in the point. This magnetic detection element 2
The magnet 8 is similar to the third embodiment in that the thickness is substantially the same in the entire longitudinal direction with the change of the arrangement position of the magnet, but the polarity is reversed.
Is the farthest from the outer peripheral edge of the rotating disk 7, and its reversal portion 8c
To gradually approach the outer peripheral edge of the rotating disk 7 toward both end portions, and both end portions are in contact with the outer peripheral edge. Magnet 8
Is disposed at a position close to the outer peripheral edge of the rotating disk 7, and therefore, the gap between the magnet 8 and the magnetic detection element 2 when the magnetic detection element 2 approaches from the one end to the other end with rotation. Is the largest at the inversion portion 8c in the longitudinal direction in which the polarity is inverted, and continuously decreases from the inversion portion 8c to both sides.
【0018】この実施形態では、被検出回転体3の回転
に伴って磁石8がその一端から他端に向けて磁気検出素
子2に順次近接した場合に、磁気検出素子2から出力す
るホール電圧が負電圧から正電圧に向けて直線的に増大
して、第1実施形態で説明した同様の効果を得られる。
それに加えて、この第4実施形態では、前述の第3実施
形態と同様に磁石8を全体にわたり同一の厚みとするこ
とができるので、磁石8の成形が容易となる利点があ
り、さらに、磁石8を第3実施形態のようなスペーサ部
材12を用いることなく回転円板7に直接固着できる。In this embodiment, when the magnet 8 sequentially approaches the magnetic detection element 2 from one end to the other end as the detected rotating body 3 rotates, the Hall voltage output from the magnetic detection element 2 is By linearly increasing from the negative voltage to the positive voltage, the same effect as described in the first embodiment can be obtained.
In addition to this, in the fourth embodiment, since the magnet 8 can be made to have the same thickness throughout as in the third embodiment, there is an advantage that the magnet 8 can be easily molded. 8 can be directly fixed to the rotating disk 7 without using the spacer member 12 as in the third embodiment.
【0019】なお、前記第2および第4実施形態では、
磁気検出素子2を回転円板7の径方向外側に配置する場
合を例示して説明したが、磁気検出素子2を径方向内側
に配置しても、上述したと同様の効果を得ることができ
る。また、反転部(突き合せ部)8cは、磁石8の長手
方向の中間部分に設定すればよく、たとえば磁石8の何
れか一方の端部に片寄った位置に設定してもよい。さら
に、磁石8は2つの磁性部分8a,8bの間に微小な隙
間が設けられていてもよい。また、本発明は、前記回転
方向の検出に加え、ホール電圧の変動に基づいて回転角
度の検出を行ってもよい。In the second and fourth embodiments,
The case where the magnetic detection element 2 is arranged on the outer side in the radial direction of the rotating disk 7 has been described as an example, but the same effect as described above can be obtained even if the magnetic detection element 2 is arranged on the inner side in the radial direction. . Further, the reversal portion (butting portion) 8c may be set at an intermediate portion in the longitudinal direction of the magnet 8, and may be set at a position deviated to either one end of the magnet 8, for example. Furthermore, the magnet 8 may be provided with a minute gap between the two magnetic portions 8a and 8b. Further, in the present invention, in addition to the detection of the rotation direction, the rotation angle may be detected based on the fluctuation of the Hall voltage.
【0020】[0020]
【発明の効果】以上説明したように、本発明の回転方向
検出装置によれば、磁石と磁気検出素子とを組み合わせ
た簡単な構成としながらも、被検出回転体における帯状
磁石の長さに相当する比較的広い回転角度の範囲内にお
いて、被検出回転体が回転する毎にその回転方向を確実
に検出することができる。しかも、長手方向の中間部分
において、磁性が反転するように着磁されているので、
磁石の厚みが薄くなる。As described above, according to the rotation direction detecting device of the present invention, although it has a simple structure in which the magnet and the magnetic detecting element are combined, it corresponds to the length of the strip magnet in the rotating body to be detected. It is possible to reliably detect the rotation direction of the detected rotating body each time it rotates within a relatively wide range of rotation angle. Moreover, because the magnetism is reversed in the middle portion in the longitudinal direction,
The magnet becomes thinner.
【0021】また、請求項2の発明によれば、磁石の厚
みを、反転部から両端部に向って軸線方向に連続的に増
大する形状に設定することにより、更に磁石の厚みが薄
くなり、コンパクト化を図り得る。さらに、請求項6の
発明によれば、磁石と磁気検出素子との間隙を反転部か
ら円周方向の両端部に向って連続的に小さくなるように
設定することにより、回転角に対する出力の変化が大き
くなり、検出精度がより一層向上する。また、同一の厚
みに形成した磁石を、磁石と磁気検出素子との間隙を反
転部から円周方向の両端部に向って連続的に小さくなる
ように設ければ、磁石の成形が容易になる。Further, according to the invention of claim 2, the thickness of the magnet is set to a shape which continuously increases in the axial direction from the reversing portion toward both ends, whereby the thickness of the magnet is further reduced. Can be made compact. Further, according to the invention of claim 6, by setting the gap between the magnet and the magnetic detection element so as to be continuously reduced from the reversal portion toward both ends in the circumferential direction, the change of the output with respect to the rotation angle is changed. Becomes larger and the detection accuracy is further improved. Further, if the magnets formed to have the same thickness are provided so that the gap between the magnet and the magnetic detection element is continuously reduced from the reversal portion toward both ends in the circumferential direction, the magnet can be easily molded. .
【図1】本発明の第1実施形態の回転方向検出装置を示
す要部の斜視図である。FIG. 1 is a perspective view of essential parts showing a rotation direction detection device according to a first embodiment of the present invention.
【図2】(a)は同実施形態の概略構成図、(b)は被
検出回転体の回転角と磁気検出素子の出力との関係を示
す特性図である。FIG. 2A is a schematic configuration diagram of the same embodiment, and FIG. 2B is a characteristic diagram showing a relationship between a rotation angle of a detected rotating body and an output of a magnetic detection element.
【図3】(a)は第2実施形態に係る回転方向検出装置
を示す要部の斜視図、(b)は正面図である。FIG. 3A is a perspective view of a main part of a rotation direction detection device according to a second embodiment, and FIG. 3B is a front view.
【図4】(a)は第3実施形態に係る回転方向検出装置
を示す要部の斜視図、(b)は正面図である。FIG. 4A is a perspective view of a main part of a rotation direction detecting device according to a third embodiment, and FIG. 4B is a front view.
【図5】(a)は第4実施形態に係る回転方向検出装置
を示す要部の斜視図、(b)は正面図である。FIG. 5A is a perspective view of an essential part showing a rotation direction detecting device according to a fourth embodiment, and FIG. 5B is a front view.
【図6】(a),(b)は本発明に含まれない回転方向
検出装置の概略平面図および回転角と磁気検出素子の出
力ホール電圧との関係図、(c)は同側面図である。6 (a) and 6 (b) are schematic plan views of a rotation direction detection device not included in the present invention and a relationship diagram between a rotation angle and an output Hall voltage of a magnetic detection element, and FIG. 6 (c) is a side view thereof. is there.
2:磁気検出素子 3:被検出回転体 8:磁石 9:演算部 C:軸線 8c:反転部(突き合せ部) 2: Magnetic detection element 3: Detected rotating body 8: Magnet 9: Calculation unit C: axis 8c: Inversion part (butt part)
Claims (6)
体の回転方向を検出する回転方向検出装置であって、 前記被検出回転体に固定されて前記被検出回転体と一体
に回転する磁石と、 前記磁石の回転軌跡に近接する位置に配置されて前記磁
石により生じる磁界の磁束密度を検出する磁気検出素子
とを備え、 前記磁石は、前記被検出回転体の回転軌跡に対応して湾
曲された帯状であって、円周方向の中間部分で磁極が反
転する反転部を有するように着磁されていると共に前記
反転部から前記円周方向の両端部に向かってそれぞれ前
記磁気検出素子に検出される磁束密度が連続的に増大す
るように設定されていることを特徴とする回転方向検出
装置。1. A rotation direction detecting device for detecting a rotation direction of a detected rotary body that rotates around a predetermined axis, wherein the rotational direction detection device is fixed to the detected rotary body and rotates integrally with the detected rotary body. A magnet and a magnetic detection element that is disposed in a position close to the rotation locus of the magnet to detect the magnetic flux density of the magnetic field generated by the magnet, and the magnet corresponds to the rotation locus of the detected rotating body. It has a curved strip shape, and is magnetized so as to have an inversion portion in which a magnetic pole is inverted at an intermediate portion in the circumferential direction, and the magnetic detection elements are respectively provided from the inversion portion toward both ends in the circumferential direction. 2. A rotation direction detecting device, characterized in that the magnetic flux density detected by is set so as to continuously increase.
方向の厚みがそれぞれ連続的に増大する形状を有してい
る回転方向検出装置。2. The rotation direction detecting device according to claim 1, wherein the magnet has a shape in which the thickness in the axial direction continuously increases from the reversal portion toward the both ends.
記軸線方向に近接して相対向する位置に配置されている
回転方向検出装置。3. The rotation direction detecting device according to claim 2, wherein the magnetic detection element is arranged at a position facing the magnet in the axial direction of the rotating body to be detected so as to face each other and face each other.
向の厚みがそれぞれ連続的に増大する形状を有している
回転方向検出装置。4. The rotation direction detecting device according to claim 1, wherein the magnet has a shape in which the thickness in the radial direction continuously increases from the reversal portion toward the both ends.
方向に近接して相対向する位置に配置されている回転方
向検出装置。5. The rotation direction detection device according to claim 4, wherein the magnetic detection element is arranged at a position that is close to and opposes the magnet in the radial direction of the rotating body to be detected.
て、 前記磁石は、回転に伴い前記磁気検出素子に近接すると
きの間隙が前記反転部から円周方向の前記両端部に向か
って連続的に小さくなるように設定されている回転方向
検出装置。6. The magnet according to any one of claims 1 to 5, wherein a gap when the magnet approaches the magnetic detection element due to rotation is continuous from the reversal portion toward both ends in the circumferential direction. Direction detection device that is set to be smaller in size.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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JP2001279431A JP2003084007A (en) | 2001-09-14 | 2001-09-14 | Rotation direction detecting device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2001279431A JP2003084007A (en) | 2001-09-14 | 2001-09-14 | Rotation direction detecting device |
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JP2003084007A true JP2003084007A (en) | 2003-03-19 |
Family
ID=19103623
Family Applications (1)
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Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004317486A (en) * | 2003-03-31 | 2004-11-11 | Denso Corp | Device for detecting rotation angle |
JP2007071641A (en) * | 2005-09-06 | 2007-03-22 | Nsk Ltd | State quantity measuring apparatus |
JP2007132710A (en) * | 2005-11-08 | 2007-05-31 | Tokai Rika Co Ltd | Position detector |
JP2008286588A (en) * | 2007-05-16 | 2008-11-27 | Alps Electric Co Ltd | Position detection device |
JP2009025317A (en) * | 2003-03-31 | 2009-02-05 | Denso Corp | Rotation angle detecting device |
EP1998147A3 (en) * | 2007-05-29 | 2013-01-23 | Robert Bosch Gmbh | Measuring device for contactless calculation of a rotation angle with radially polarised magnets |
KR101874606B1 (en) * | 2015-10-07 | 2018-07-04 | 캄텍주식회사 | A magnet for sensing rotation state |
CN112888951A (en) * | 2018-09-19 | 2021-06-01 | 哈姆林电子(苏州)有限公司 | Speed sensor assembly |
-
2001
- 2001-09-14 JP JP2001279431A patent/JP2003084007A/en active Pending
Cited By (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004317486A (en) * | 2003-03-31 | 2004-11-11 | Denso Corp | Device for detecting rotation angle |
JP2009025317A (en) * | 2003-03-31 | 2009-02-05 | Denso Corp | Rotation angle detecting device |
JP2007071641A (en) * | 2005-09-06 | 2007-03-22 | Nsk Ltd | State quantity measuring apparatus |
JP2007132710A (en) * | 2005-11-08 | 2007-05-31 | Tokai Rika Co Ltd | Position detector |
JP2008286588A (en) * | 2007-05-16 | 2008-11-27 | Alps Electric Co Ltd | Position detection device |
EP1998147A3 (en) * | 2007-05-29 | 2013-01-23 | Robert Bosch Gmbh | Measuring device for contactless calculation of a rotation angle with radially polarised magnets |
KR101874606B1 (en) * | 2015-10-07 | 2018-07-04 | 캄텍주식회사 | A magnet for sensing rotation state |
CN112888951A (en) * | 2018-09-19 | 2021-06-01 | 哈姆林电子(苏州)有限公司 | Speed sensor assembly |
US11796556B2 (en) | 2018-09-19 | 2023-10-24 | Suzhou Littelfuse Ovs Co., Ltd. | Speed sensor assembly |
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