JPH04110725A - Magnetic sensor and its manufacturing method - Google Patents
Magnetic sensor and its manufacturing methodInfo
- Publication number
- JPH04110725A JPH04110725A JP2231750A JP23175090A JPH04110725A JP H04110725 A JPH04110725 A JP H04110725A JP 2231750 A JP2231750 A JP 2231750A JP 23175090 A JP23175090 A JP 23175090A JP H04110725 A JPH04110725 A JP H04110725A
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- magnetic
- tracks
- drum
- ferromagnetic
- magnetized
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Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、ロボット、NC装置等に広く使用されている
アブソリュート型の磁気センサおよびその製造方法に関
するものである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an absolute type magnetic sensor widely used in robots, NC devices, etc., and a method for manufacturing the same.
従来の技術
インクリメンタル型の磁気エンコーダは第8図のように
、ソヤフト15に固着された磁気ドラムの外周に着磁を
施し、その磁界を磁気抵抗素子(以下MR素子と称す)
により検出する構造が開発されている。第8図に示す如
く、磁気ドラム11には2トラツクの外周着磁がされて
おり、1つは多極着磁部12であり、所定の磁極を着磁
する。他は1回転に1対の磁極を着磁する原点着磁部1
3となる。Conventional technology Incremental magnetic encoders, as shown in FIG. 8, magnetize the outer periphery of a magnetic drum fixed to a soyaft 15, and apply the magnetic field to a magnetoresistive element (hereinafter referred to as an MR element).
A detection structure has been developed. As shown in FIG. 8, the magnetic drum 11 is magnetized on the outer periphery of two tracks, one of which is a multi-pole magnetized section 12, which magnetizes a predetermined magnetic pole. The other is the origin magnetization part 1 that magnetizes one pair of magnetic poles per rotation.
It becomes 3.
以上のように構成された磁気ドラム11について以下に
説明する。磁気ドラムは樹脂マグネットやステンレスヘ
ースの外周に磁性粉を塗布することにより構成する。そ
の外周部に2トラックの着磁を行なう。第8図中、多極
着磁部12は1回転に1000パルスの出力が必要な場
合は1000極の着磁を行なう。磁気ドラムの外径が8
On+mであれば着磁幅は0.25am+程度となる原
点着磁部13はほぼ同し着磁幅で着磁したもので、回転
の原点を示す原点着磁部13となっている。磁気ドラム
11に近接配置したMR素子14により信号検出をする
。その信号を第9図に示す。信号16は原点着磁部13
からの信号、信号17.18は多極着磁部12からの信
号で信号1718は相互に90°の位相差のある2信号
である。このような3信号により磁気ドラム11の回転
位置情報を得る方式をインクリメンタル型のエンコーダ
といわれている。The magnetic drum 11 configured as described above will be explained below. The magnetic drum is constructed by applying magnetic powder to the outer periphery of a resin magnet or stainless steel heath. Two tracks of magnetization are performed on the outer periphery. In FIG. 8, the multi-pole magnetization section 12 performs magnetization of 1000 poles when an output of 1000 pulses per rotation is required. The outer diameter of the magnetic drum is 8
If On+m, the magnetization width is approximately 0.25 am+.The origin magnetized portion 13 is magnetized with approximately the same magnetization width, and serves as the origin magnetization portion 13 that indicates the origin of rotation. Signals are detected by an MR element 14 placed close to the magnetic drum 11. The signal is shown in FIG. Signal 16 is the origin magnetized section 13
Signals 17 and 18 are signals from the multi-pole magnetization section 12, and signals 1718 are two signals with a phase difference of 90 degrees. A method of obtaining rotational position information of the magnetic drum 11 using these three signals is called an incremental encoder.
発明が解決しようとする課題
上記インクリメンタル型のエンコーダの場合、電源が切
れるとその位置情報が失われてしまうので、必ず原点復
帰が必要となる。一方、アブソリュート型では円周を多
段のトラックに分けて、それぞれ2. 4. 8.16
.32・・・・・・2″分割してその絶対位置を検出す
る方式が光を媒体としたエンコダとしである。これを磁
気で行なうと多段の着磁トラックが必要となり、また着
磁も複雑なものとなり、大形化、高価格となる失点があ
った。着磁トラックを減らして、例えば2,16.12
8.1024分割したトラックを用いて4.8 、32
.64.256512、2048.4096分割は電気
回路処理によって作る方法を取ると、12トラツク必要
なものが4トラツクで作ることができる。このように電
気回路処理により分割する場合は元の2.16.128
.1024の検出波形は歪の少ない相互に90°の位相
差を持つ正弦波が必要であるといわれている。一方外径
80mmのように大形磁気ドラムになると、128.1
024分割では正弦波で検出することが可能であるが、
2.16分割では着磁ピッチが125+on、 15.
7mmとなり、このように大きいピンチでは円周方向に
磁界を発生させる従来の着磁とMR素子の構成では正弦
波の信号波形が得られなかった。Problems to be Solved by the Invention In the case of the above-mentioned incremental type encoder, when the power is turned off, the position information is lost, so it is always necessary to return to the origin. On the other hand, in the absolute type, the circumference is divided into multiple tracks, each with 2 tracks. 4. 8.16
.. An encoder that uses light as a medium divides the 32... This resulted in a larger size and higher price.By reducing the number of magnetized tracks, for example, 2, 16, 12
8. 4.8, 32 using 1024 divided tracks
.. If the 64.256512 and 2048.4096 divisions are created by electrical circuit processing, what would require 12 tracks can be created with 4 tracks. When dividing by electrical circuit processing like this, the original 2.16.128
.. It is said that the detection waveform of 1024 requires a sine wave with little distortion and a phase difference of 90 degrees. On the other hand, if it is a large magnetic drum with an outer diameter of 80 mm, it will be 128.1
Although it is possible to detect with a sine wave in 0.024 division,
2. In 16 division, the magnetization pitch is 125+on, 15.
7 mm, and in such a large pinch, a sinusoidal signal waveform could not be obtained with the conventional magnetization and MR element configuration that generates a magnetic field in the circumferential direction.
課題を解決するための手段
上記問題点を解決するために本発明では、円周に沿って
は磁界強さがsinで変化し、その磁界方向は軸方向と
した磁気トラックを少なくとも2本作り、かつその磁気
トラックは相互に磁界強さが逆に変化する構成とし、こ
の磁気トラックをMR素子でsin波信号として検出す
るものである。Means for Solving the Problems In order to solve the above problems, in the present invention, at least two magnetic tracks are created in which the magnetic field strength changes at a sin along the circumference, and the direction of the magnetic field is in the axial direction. The magnetic tracks are configured such that the magnetic field strength changes inversely to each other, and the magnetic tracks are detected as a sine wave signal by an MR element.
作用
この構成により、円周に沿って磁界強さがsinで変化
する磁気ドラムに対向したMR素子が、その磁界強さを
sin波信号として検出する。Effect: With this configuration, the MR element facing the magnetic drum, whose magnetic field strength varies sinically along the circumference, detects the magnetic field strength as a sine wave signal.
実施例
以下本発明の一実施例を添付図面にもとづいて説明する
。第1図において、磁気ドラム1にシャフト2を取付け
る。シャフト2には回転に伴い回転と同期したsin波
信号を発生する信号発生器3を取付ける。EXAMPLE Hereinafter, an example of the present invention will be described based on the accompanying drawings. In FIG. 1, a shaft 2 is attached to a magnetic drum 1. A signal generator 3 is attached to the shaft 2 to generate a sine wave signal synchronized with the rotation as the shaft 2 rotates.
信号発生器3から出た信号はアンプ4で増幅され磁気ヘ
ッド5A、5B、5C,5D (陰となるので図示せず
)により磁気トラ、り6A、686C,6Dとして着磁
される。磁気トラック6A6B、6C,6Dの磁界強さ
は信号発生器からのsin波信号と同期したものとなり
、sin状で磁界強さが変化する磁気トラック6A、6
B。The signal output from the signal generator 3 is amplified by an amplifier 4 and magnetized by magnetic heads 5A, 5B, 5C, and 5D (not shown because they are shaded) as magnetic tracks 6A, 686C, and 6D. The magnetic field strength of the magnetic tracks 6A, 6B, 6C, and 6D is synchronized with the sinusoidal signal from the signal generator, and the magnetic field strength of the magnetic tracks 6A, 6 changes in a sinusoidal manner.
B.
6C,6Dとなる。They become 6C and 6D.
磁気トラック6A、6B、6C,6Dの位相関係は6A
と6Bは180度、6Cと6Dは180度、6Aと60
は90度の位相差となるように着磁する。The phase relationship of magnetic tracks 6A, 6B, 6C, and 6D is 6A.
and 6B are 180 degrees, 6C and 6D are 180 degrees, 6A and 60
are magnetized to have a phase difference of 90 degrees.
例えば1回転IH2の信号の場合は相互に機械角度で磁
気ヘッドAとBは180度、CとDは180度6Aと6
0は90度となるように取付け、直列に接続して同し電
流で着磁する。なお51A、 51851C,51Dは
磁気ヘッド5A、5B、5C,5Dのヨーク開口部で、
磁気ドラム1の軸方向と合致しており、磁気トラックは
上下方向に磁極が設けられる。For example, in the case of a signal of 1 rotation IH2, the mechanical angle between magnetic heads A and B is 180 degrees, and magnetic heads C and D are 180 degrees.
0 is 90 degrees, connected in series, and magnetized with the same current. Note that 51A, 51851C, and 51D are the yoke openings of the magnetic heads 5A, 5B, 5C, and 5D.
It coincides with the axial direction of the magnetic drum 1, and the magnetic track is provided with magnetic poles in the vertical direction.
ここで、1回転16Hzの場合はその角度を磁気ヘンド
5Aと5Bおよび5Cと5Dは11.25度又は等価な
11.25+ n X22.5度(n≧1の整数)とし
、5Aと50は5,625度または等価な5,625
十n X22.5度(n≧1の整数)に取付ける。Here, if one rotation is 16Hz, the angle for magnetic hands 5A and 5B and 5C and 5D is 11.25 degrees or equivalently 11.25 + n x 22.5 degrees (an integer of n≧1), and 5A and 50 are 5,625 degrees or equivalent 5,625
Install at 10n x 22.5 degrees (n≧1 integer).
なお、磁気トラック6A、6B、6C,6Dを同一電流
で同時に着磁することで説明したが、磁気トラック6A
、6B、6C,6Dを別々の着磁電流としてその位相を
所定の位相差としてもよい。Although the explanation was given by magnetizing the magnetic tracks 6A, 6B, 6C, and 6D at the same time with the same current, the magnetic tracks 6A
, 6B, 6C, and 6D may be separate magnetizing currents, and their phases may be set to have a predetermined phase difference.
このように着磁した磁気ドラム1にMR素子7を磁気ト
ラック6A、6B、6C,6Dに一定のギャップgで近
接配置する。The MR element 7 is placed close to the magnetic tracks 6A, 6B, 6C, and 6D with a constant gap g on the magnetic drum 1 magnetized in this manner.
MR素子7の内部には磁界により抵抗値の変化する強磁
性の磁気抵抗M R+ とMR2、MR。Inside the MR element 7 are ferromagnetic magnetoresistances M R+ , MR2, and MR whose resistance value changes depending on the magnetic field.
MR,を配置する。磁気抵抗MR,,MR。Place MR. Magnetoresistive MR,,MR.
MR3、MRa 、MRs 、MRb 、MRq、MR
eは第2図に示すようにそれぞれ磁気トラックの6A
6B、6C,6Dに対向して配置する。MR3, MRa, MRs, MRb, MRq, MR
e is 6A of each magnetic track as shown in Figure 2.
It is arranged facing 6B, 6C, and 6D.
この磁気抵抗MR1,MR2、MRi 、MRaMRs
、MRb 、MR? 、MRs 、は同一基板上に同
時に作られたもので、第3図に示す等価回路のようにM
R+ とMR2をMR3とMR,を、MR5とMR,
を、MR,とMR,をそれぞれ直列に接続し、その接続
点から出力信号VA、VAをVB、VBをそれぞれ取り
出し、他端側を電源上に接続する。These magnetic resistances MR1, MR2, MRi, MRaMRs
, MRb , MR? , MRs , were made simultaneously on the same substrate, and as shown in the equivalent circuit shown in Figure 3, M
R+ and MR2, MR3 and MR, MR5 and MR,
, MR, and MR are connected in series, and the output signals VA, VA and VB are taken out from the connection point, respectively, and the other end is connected to the power source.
より具体的なMR素子と磁気トラックとの関係を第4図
により説明する。A more specific relationship between the MR element and the magnetic track will be explained with reference to FIG.
磁気抵抗MR,,MR2、MR3、MR。Magnetoresistive MR,, MR2, MR3, MR.
MRs 、MRb 、MRv 、MRsはNiFe又は
NiCo等の強磁性の合金薄膜からなる磁界によって抵
抗が変化する抵抗で、図に示すように、それぞれの抵抗
は同一基板上に同し形状で作る。この強磁性磁気抵抗は
薄膜の面と同し面で、電流の流れる方向と直角方向の磁
界に対して最大に抵抗変化があるので、図に示すように
磁気トラック6A、6Bの磁界方向(図では上から下)
と直角に電流が流れるように磁界を感知する磁気抵抗M
R,,MR,,MR,,MR,を配置する。MRs, MRb, MRv, and MRs are resistors whose resistances change depending on the magnetic field and are made of ferromagnetic alloy thin films such as NiFe or NiCo, and as shown in the figure, each resistor is made in the same shape on the same substrate. This ferromagnetic magnetoresistance has a maximum resistance change in the direction of the magnetic field in the direction perpendicular to the direction of current flow in the same plane as the thin film. (from top to bottom)
A magnetic resistance M that senses a magnetic field so that a current flows at right angles to
Arrange R,,MR,,MR,,MR,.
そして、MR,とMR,を接続し、その接続点から出力
VAをM R3とMR,を接続し、その接続点から出力
VAを取り出す。一方、それぞれの他端子側は電flE
に接続する。このとき図に示すようにMR,とMR,に
対してMR,とMR,は逆極性となるように電源Eに接
続する。Then, MR3 and MR are connected, and the output VA is taken out from the connection point.MR3 and MR are connected, and the output VA is taken out from the connection point. On the other hand, the other terminal side of each
Connect to. At this time, as shown in the figure, MR and MR are connected to the power source E so that they have opposite polarities.
このように構成することによりMR素子7の抵抗は第5
図aのようにMR,とMR,およびMR。With this configuration, the resistance of the MR element 7 becomes the fifth
MR, and MR, and MR as shown in figure a.
とMR3は互いに逆の関係でSinで増減する。and MR3 are inversely related to each other and increase or decrease with Sin.
したがって出力電圧VAは第5b図および第5図Cに示
すように、はぼ電源電圧の%を中心にVAのように出力
電圧として取りだせる。仮に片側MR,だけの動作の場
合は第5図すの点線のようにVAの2の出力となる。逆
極性の電源に接続したMR:1.MR4からは同様に第
5図Cの点線で示すVAのようにVAとは逆相の出力電
圧として取りだせる。このように、はぼ電源電圧の2を
中心にVAとVAは位相が180度ずれた出力となり、
この差(VA−VA)を取ると出力電圧が2倍となる。Therefore, as shown in FIGS. 5b and 5C, the output voltage VA can be obtained as an output voltage centered around % of the power supply voltage. If only one side MR is operated, the output of VA will be 2 as shown by the dotted line in FIG. MR connected to a power supply with opposite polarity: 1. Similarly, from the MR4, an output voltage having the opposite phase to VA as indicated by the dotted line in FIG. 5C can be obtained. In this way, VA and VA output with a phase difference of 180 degrees centered on the power supply voltage 2,
Taking this difference (VA-VA) doubles the output voltage.
また、第6図に示すような差動アンプで出力電圧を増幅
するとMR+ 、MR2、MR3、MR4に入ってくる
ノイズは差動アンプの同相除去により大幅に減少するこ
とができ、大幅な耐ノイズ性が向上する。Furthermore, when the output voltage is amplified by a differential amplifier as shown in Figure 6, the noise entering MR+, MR2, MR3, and MR4 can be significantly reduced by the common mode rejection of the differential amplifier, resulting in significant noise resistance. Improves sex.
同しようにして90度位相差のある磁気トラック6C2
6DおよびMRs 、MR−、MRl、MRsからはV
A、VAに対して90度位相差のあるVBVBが得られ
る。Similarly, magnetic track 6C2 with a 90 degree phase difference
6D and MRs, MR-, MRl, MRs from V
VBVB with a 90 degree phase difference with respect to A and VA is obtained.
なお強磁性の磁気抵抗は磁極のN、S両磁極に対して対
称に抵抗変化するので1回転1)1zを得るときは第7
図に示すように直流が重畳した着M1電流で着磁し、磁
気トラックの極性が反転しないようにする。(極性が反
転すると1回転2Hzの出力信号となってしまう)。Note that the magnetic resistance of ferromagnetism changes symmetrically with respect to both the N and S magnetic poles, so when obtaining 1) 1z per rotation, the 7th
As shown in the figure, the magnetic track is magnetized by the M1 current superimposed with a direct current to prevent the polarity of the magnetic track from being reversed. (If the polarity is reversed, the output signal will be 2Hz per revolution).
]回転に2Hz以上の場合は直流を重畳してもしなくて
もよい。] If the rotation is 2Hz or more, direct current may or may not be superimposed.
発明の効果
このような構成とすることにより、1回転IHzあるい
は1回転16H2というような低周波なsin波検出が
高出力で、ノイズの少ない信号として検出することがで
き、アブソリュート型でも少ない磁気トラックと少ない
MR素子で構成することができ、小型で安価なエンコー
ダを作ることができる。Effects of the Invention With this configuration, low-frequency sine wave detection such as IHz per revolution or 16H2 per revolution can be detected as a high-output, low-noise signal, and even with an absolute type, it is possible to detect a low-frequency sine wave with a small number of magnetic tracks. The encoder can be constructed with a small number of MR elements, and a small and inexpensive encoder can be manufactured.
第1図は本発明の一実施例において、磁気ドラムと着磁
ヘッドの関係を示す概略図、第2図は本発明の磁気ドラ
ムとMR素子の関係を示す概略l、第3図は本発明のM
R素子の接続を示す等価回路図、第4図は本発明の磁気
トラックとMR素子の磁気抵抗との関係を示す概略図、
第5図a −cは第4図のMR素子の磁気抵抗の変化と
実施例における出力電圧の変化を示す波形図、第6図は
第4図の実施例におけるアンプ回路の接続を示す回路図
、第7図は1回転IHz時の着磁電流を示す波形図、第
8図は従来例の磁気トラックとMR素子のαb
関係を示す概略図、第9図は従来例での出力電圧を示す
波形図である。
1・・・・・・磁気ドラム、2・・・・・・シャフト、
3・・・・・・信号発生器、4・・・・・・アンプ、5
A、5B、5C,5D・・・・・・磁気ヘッド、51A
51B 51C,51D・・・・・・磁気ヨーク
開口部、6A、6B、6C16D・・・・・・磁気トラ
ック、7・・・・・・MR素子、MR,、MR。
MR3MR,MR5MR,、MR,、MR。
・・・・・・強磁性の磁気抵抗。
代理人の氏名 弁理士 小鍜治 明 ほか2名1図
第2図
47レデ
第
図
第6図
第7図
回斡絢
第
図
第
第
図
図
@転角
@転角
目に角
1、へFIG. 1 is a schematic diagram showing the relationship between the magnetic drum and the magnetized head in an embodiment of the present invention, FIG. 2 is a schematic diagram showing the relationship between the magnetic drum and the MR element of the present invention, and FIG. 3 is a schematic diagram showing the relationship between the magnetic drum and the MR element of the present invention. M of
An equivalent circuit diagram showing the connection of the R element, FIG. 4 is a schematic diagram showing the relationship between the magnetic track of the present invention and the magnetic resistance of the MR element,
Figures 5a-c are waveform diagrams showing changes in the magnetic resistance of the MR element in Figure 4 and changes in output voltage in the example, and Figure 6 is a circuit diagram showing the connection of the amplifier circuit in the example in Figure 4. , Fig. 7 is a waveform diagram showing the magnetizing current during one revolution at IHz, Fig. 8 is a schematic diagram showing the αb relationship between the magnetic track and the MR element in the conventional example, and Fig. 9 shows the output voltage in the conventional example. FIG. 1...magnetic drum, 2...shaft,
3...signal generator, 4...amplifier, 5
A, 5B, 5C, 5D...Magnetic head, 51A
51B 51C, 51D...Magnetic yoke opening, 6A, 6B, 6C16D...Magnetic track, 7...MR element, MR, MR. MR3MR, MR5MR, MR, MR. ...Ferromagnetic magnetic resistance. Name of agent: Patent attorney Akira Odaji and 2 others 1 Figure 2 Figure 47 Rede Figure 6 Figure 7 Turning Aya Figure Figure Figure 1
Claims (5)
の磁気トラックに対向して強磁性磁気抵抗素子を配置し
、かつ前記磁気トラックは、着磁方向を磁気ドラムの一
周に亘り軸方向とするとともに、磁気ドラムの回転に伴
い強磁性磁気抵抗素子に対してsin状に磁界強さが変
化する磁気トラックとし、かつ少なくとも2本の磁気ト
ラックは相互に磁界強さが逆に変化するように構成した
磁気センサ。(1) A ferromagnetic magnetoresistance element is arranged opposite to at least two magnetic tracks that are magnetized around one circumference of the magnetic drum, and the magnetic tracks are magnetized in the axial direction around one circumference of the magnetic drum. At the same time, the magnetic track is such that the magnetic field strength changes in a sinusoidal manner with respect to the ferromagnetic magnetoresistive element as the magnetic drum rotates, and the magnetic field strength of at least two magnetic tracks changes in the opposite direction. The configured magnetic sensor.
磁方向と直角に配置するとともに、前記2個の強磁性磁
気抵抗を直列に接続して強磁性磁気抵抗素子を構成し、
かつ直列接続した端子を信号検出端とし、他端側を電源
に接続した請求項1記載の磁気センサ。(2) arranging two ferromagnetic magnetoresistances at right angles to the magnetization direction of the two magnetic tracks, and connecting the two ferromagnetic magnetoresistances in series to form a ferromagnetic magnetoresistive element;
2. The magnetic sensor according to claim 1, wherein the terminals connected in series are used as signal detection ends, and the other end is connected to a power source.
も2組用い、かつそれぞれの組の強磁性磁気抵抗素子を
互いに逆位相とした請求項1記載の磁気センサ。(3) The magnetic sensor according to claim 1, wherein at least two sets of two ferromagnetic magnetoresistive elements are used, and the ferromagnetic magnetoresistive elements of each set have phases opposite to each other.
れぞれ1組とし、前記磁気トラックは、磁気ドラムに相
互に90度の位相差を設けて2組設け、前記強磁性磁気
抵抗を2組設けて相互に90度の位相差の出力を得るよ
うに構成した請求項1記載の磁気センサ。(4) Each set includes two magnetic tracks and two ferromagnetic magnetoresistances, and the magnetic tracks are provided in two sets with a phase difference of 90 degrees from each other on the magnetic drum, and the ferromagnetic magnetoresistive 2. The magnetic sensor according to claim 1, wherein two sets are provided so as to obtain outputs with a phase difference of 90 degrees from each other.
ラックを4本作るにあたり、磁気ドラムに対向する4個
の着磁用磁気ヘッドを相互に所定の角度離れた位置に設
けるとともに、着磁用磁気ヘッドには磁気ドラムの回転
と同期した着磁電流を4個の着磁用磁気ヘッドに同時に
流すようにした請求項1記載の磁気センサの製造方法。(5) When creating four magnetic tracks with a predetermined phase difference from each other on the magnetic drum, four magnetic heads for magnetization facing the magnetic drum are provided at positions separated by a predetermined angle from each other, and 2. The method of manufacturing a magnetic sensor according to claim 1, wherein a magnetizing current synchronized with the rotation of the magnetic drum is simultaneously applied to the four magnetizing magnetic heads.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2231750A JPH04110725A (en) | 1990-08-31 | 1990-08-31 | Magnetic sensor and its manufacturing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2231750A JPH04110725A (en) | 1990-08-31 | 1990-08-31 | Magnetic sensor and its manufacturing method |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH04110725A true JPH04110725A (en) | 1992-04-13 |
Family
ID=16928451
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2231750A Pending JPH04110725A (en) | 1990-08-31 | 1990-08-31 | Magnetic sensor and its manufacturing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH04110725A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6391269B1 (en) | 1997-08-21 | 2002-05-21 | Takeshiro Yoshimatsu | Deodorizing/sterilizing device |
| US6620224B1 (en) | 2002-08-12 | 2003-09-16 | Kabushiki Kaisha Circland | Air purification device with a needle-shaped electrode having a protective cover thereon |
-
1990
- 1990-08-31 JP JP2231750A patent/JPH04110725A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6391269B1 (en) | 1997-08-21 | 2002-05-21 | Takeshiro Yoshimatsu | Deodorizing/sterilizing device |
| US6620224B1 (en) | 2002-08-12 | 2003-09-16 | Kabushiki Kaisha Circland | Air purification device with a needle-shaped electrode having a protective cover thereon |
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