JPH06338003A - Magnetic field application device - Google Patents

Magnetic field application device

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Publication number
JPH06338003A
JPH06338003A JP12702893A JP12702893A JPH06338003A JP H06338003 A JPH06338003 A JP H06338003A JP 12702893 A JP12702893 A JP 12702893A JP 12702893 A JP12702893 A JP 12702893A JP H06338003 A JPH06338003 A JP H06338003A
Authority
JP
Japan
Prior art keywords
magnetic field
magnetic
exciting coil
overcurrent
magneto
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP12702893A
Other languages
Japanese (ja)
Other versions
JP3137501B2 (en
Inventor
Takashi Ogawa
隆 小川
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Ricoh Co Ltd
Original Assignee
Ricoh Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP05127028A priority Critical patent/JP3137501B2/en
Publication of JPH06338003A publication Critical patent/JPH06338003A/en
Application granted granted Critical
Publication of JP3137501B2 publication Critical patent/JP3137501B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

(57)【要約】 【目的】 大容量の電源を必要とすることなく、磁界印
加装置の発熱量を大幅に低減することができる。 【構成】 光磁気ディスク装置等に用いられる磁界印加
装置において、磁芯の極性反転時、励磁コイルに過電流
を流すことにより、磁芯に残留磁界を発生させ、通電時
の電流値を小さくする。
(57) [Summary] [Purpose] The heat generation amount of the magnetic field application device can be significantly reduced without requiring a large-capacity power supply. In a magnetic field applying device used in a magneto-optical disk device or the like, a residual magnetic field is generated in the magnetic core by flowing an overcurrent when the polarity of the magnetic core is reversed, and the current value when energized is reduced. .

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、光磁気ディスク装置等
の光磁気記録装置に用いられる磁界印加装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic field applying device used in a magneto-optical recording device such as a magneto-optical disk device.

【0002】[0002]

【従来の技術】従来より、光磁気ディスク装置等に用い
られる磁界印加装置としては、永久磁石を用いるもの
と、電磁石を用いるものとが知られている。永久磁石を
用いるものは、その極性を切り換える時間が長くかか
り、また装置も大型化するという欠点を有している。
2. Description of the Related Art Conventionally, as a magnetic field applying device used in a magneto-optical disk device or the like, one using a permanent magnet and one using an electromagnet are known. The one using a permanent magnet has a drawback that it takes a long time to switch the polarity and the device becomes large.

【0003】そこで、電磁石を用いた磁界印加装置とし
ては、例えば、特公平4−56362号公報に示される
ものがある。即ち、半導体レーザ等の光源からの光ビー
ムを光学レンズで集光してその光スポットをバイアス磁
界を印加した光磁気ディスクに投射して情報を記録ある
いは消去するようにした光学的情報記録再生装置におい
て、前記バイアス磁界印加手段が半硬質磁性材料より形
成され十分なN極とS極間の距離を有する磁芯と前記磁
極の極性を反転し得る励磁コイルおよびパルス励磁電流
電源より構成されたことを特徴とするバイアス磁界印加
装置である。
Therefore, as a magnetic field applying device using an electromagnet, there is, for example, a device disclosed in Japanese Patent Publication No. 4-56362. That is, an optical information recording / reproducing apparatus adapted to record or erase information by condensing a light beam from a light source such as a semiconductor laser with an optical lens and projecting the light spot on a magneto-optical disk to which a bias magnetic field is applied. The bias magnetic field applying means is composed of a magnetic core formed of a semi-hard magnetic material and having a sufficient distance between the N and S poles, an exciting coil capable of reversing the polarities of the magnetic poles, and a pulse exciting current power supply. Is a bias magnetic field applying device.

【0004】[0004]

【発明が解決しようとする課題】しかしながら、上記従
来の磁界印加装置は、電流を加えてコイルを一旦磁化さ
せた後、電流を0にし、半硬質磁性材料による保磁力に
より光磁気ディスクに磁界を印加するので、消費電流は
小さくなるという利点はあるものの、保磁力を大きくす
るために瞬間的に大量の電流を流す必要があり、磁界印
加用電源が大型化し、部品実装上好ましくないという問
題点がある。
However, in the above-mentioned conventional magnetic field applying device, a current is applied to magnetize the coil once, and then the current is set to 0, and the magnetic field is applied to the magneto-optical disk by the coercive force of the semi-hard magnetic material. Since it is applied, there is an advantage that the current consumption is small, but it is necessary to momentarily supply a large amount of current in order to increase the coercive force, and the magnetic field application power source becomes large, which is not preferable for component mounting. There is.

【0005】本発明は上記の点に鑑みてなされたもので
あり、大容量の電源を必要とすることなく、磁界印加装
置の発熱量を大幅に減少することを目的とする。
The present invention has been made in view of the above points, and it is an object of the present invention to significantly reduce the amount of heat generated by a magnetic field applying device without requiring a large-capacity power source.

【0006】[0006]

【課題を解決するための手段】本発明は上記の目的を達
成するためになされたもので、光源からの光ビームを対
物レンズで集光してその光磁気記録媒体にスポットを形
成し、この光磁気記録媒体に情報を記録または消去する
ために前記光磁気記録媒体にバイアス磁界を印加するた
めの磁界印加装置において、半硬質磁性材料または軟質
磁性材料より形成される磁芯と、前記磁芯の極性を反転
し得る励磁コイルと、この励磁コイルに通常電流を供給
する通常電流供給手段と、極性反転時に前記励磁コイル
に過電流を供給する過電流供給手段とを具備することを
特徴とする磁界印加装置である。また、前記過電流供給
手段は、前記磁芯の磁気飽和電流値より小さい過電流を
励磁コイルに供給する。そして、光磁気記録媒体の近傍
に配置される磁気センサーと、この磁気センサーからの
出力信号に基づいて前記励磁コイルに流す電流を制御す
る制御回路を有する。
The present invention has been made to achieve the above-mentioned object, and a light beam from a light source is condensed by an objective lens to form a spot on the magneto-optical recording medium. In a magnetic field applying device for applying a bias magnetic field to the magneto-optical recording medium for recording or erasing information on the magneto-optical recording medium, a magnetic core formed of a semi-hard magnetic material or a soft magnetic material, and the magnetic core. Is provided with an exciting coil capable of reversing the polarity, a normal current supplying means for supplying a normal current to the exciting coil, and an overcurrent supplying means for supplying an overcurrent to the exciting coil at the time of polarity reversal. It is a magnetic field applying device. Further, the overcurrent supply means supplies an overcurrent smaller than the magnetic saturation current value of the magnetic core to the exciting coil. Further, it has a magnetic sensor arranged in the vicinity of the magneto-optical recording medium, and a control circuit for controlling a current flowing through the exciting coil based on an output signal from the magnetic sensor.

【0007】[0007]

【作用】本発明によれば、極性反転時、励磁コイルに瞬
間的に通電時より大きい電流、すなわち過電流を流すこ
とにより残留磁界が発生し、所定の磁界を得るのに必要
な通電時の電流値を低下することが可能となる。また、
励磁コイルに飽和電流値より小さい過電流を供給するこ
とにより、電源の負荷は低減される。さらに、磁気セン
サーにより磁芯の残留磁界が検出され、この検出された
信号に基づいて励磁コイルに流す電流量が精度よく制御
される。
According to the present invention, at the time of polarity reversal, a residual magnetic field is generated by causing a current larger than that during energization, that is, an overcurrent, to be momentarily applied to the exciting coil. It is possible to reduce the current value. Also,
By supplying an overcurrent smaller than the saturation current value to the exciting coil, the load on the power supply is reduced. Further, the residual magnetic field of the magnetic core is detected by the magnetic sensor, and the amount of current flowing through the exciting coil is accurately controlled based on the detected signal.

【0008】[0008]

【実施例】以下、本発明の一実施例を添付図面に基づい
て具体的に説明する。図中1は、断面H字状(横向き)
のボビンで、このボビン1の中央部1aには励磁コイル
2が巻かれており、またボビン1の中央部1aには穴部
が形成されている。この穴部には磁芯3が挿入されてお
り、前記ボビン1の外周を覆うカバー4が前記磁芯3と
連続して形成されている。これらより構成される磁界発
生手段Aは、メディア5の上方に所定の間隔をおいて配
置されている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be specifically described below with reference to the accompanying drawings. 1 in the figure is H-shaped in cross section (sideways)
In this bobbin, the exciting coil 2 is wound around the central portion 1a of the bobbin 1, and the central portion 1a of the bobbin 1 is formed with a hole. A magnetic core 3 is inserted into this hole, and a cover 4 covering the outer periphery of the bobbin 1 is formed continuously with the magnetic core 3. The magnetic field generating means A composed of these is arranged above the medium 5 at a predetermined interval.

【0009】ここで、前記磁芯3の材質としては、保磁
力Hcが1〜10[Oe]くらいの軟質磁性材料(例え
ば、純鉄、軟鋼、鋳鉄、けい素鋼等)か、あるいは半硬
質材料(Hcが10〜100[Oe]程度)がよい。も
し、硬質材料にすると保磁力Hcは大きくなるが、透磁
率が小さいため、所定の磁界を得るために必要な電流を
非常に大きくする必要があり、また、ヒステリシスルー
プの面積が大きいため、磁極の反転時のエネルギー損失
も大となるからである。
Here, as the material of the magnetic core 3, a soft magnetic material having a coercive force Hc of about 1 to 10 [Oe] (for example, pure iron, mild steel, cast iron, silicon steel, etc.) or semi-hard material is used. A material (Hc of about 10 to 100 [Oe]) is preferable. If a hard material is used, the coercive force Hc will increase, but since the magnetic permeability is small, the current required to obtain a predetermined magnetic field must be extremely large, and the area of the hysteresis loop is large. This is because the energy loss at the time of reversing is also large.

【0010】前記磁界発生手段Aには、磁芯3を磁化さ
せておくために励磁コイル2に電流を供給する磁界発生
手段駆動回路8が接続されている。ここで、励磁コイル
2に発生する磁界を図2及び図3に基づいて説明する。
図2はコイルに流れる電流と時間との関係を示す図で、
図中aは通常電流IAを流す時の特性を示す曲線であ
り、bは本発明でいう過電流IBを流す時の特性を示す
曲線である。図3は、コイル磁界(H)と磁束密度
(B)との関係を示す図で、前記通常電流IAを励磁コ
イル2に流すことによりコイル磁界HAが発生し、それ
により磁束密度BAが生じる。また、前記過電流IBを
励磁コイル2に流すことによりコイル磁界HBが発生
し、それにより磁束密度BBが生じる。
The magnetic field generating means A is connected to a magnetic field generating means drive circuit 8 which supplies a current to the exciting coil 2 in order to magnetize the magnetic core 3. Here, the magnetic field generated in the exciting coil 2 will be described with reference to FIGS. 2 and 3.
FIG. 2 is a diagram showing the relationship between the current flowing through the coil and time,
In the figure, a is a curve showing the characteristic when the normal current IA is passed, and b is a curve showing the characteristic when the overcurrent IB is passed according to the present invention. FIG. 3 is a diagram showing the relationship between the coil magnetic field (H) and the magnetic flux density (B). When the normal current IA is passed through the exciting coil 2, a coil magnetic field HA is generated, which causes a magnetic flux density BA. Further, the coil magnetic field HB is generated by causing the overcurrent IB to flow through the exciting coil 2, thereby generating the magnetic flux density BB.

【0011】従って、その磁界の向きを反転させる瞬間
あるいは磁界を立ち上げる瞬間に、図2に示すbのよう
に、一時的に過電流IBを流すようにすれば、図3に示
すように、残留磁気(BA’−BA)の分だけ磁芯3に
発生する磁界を強くすることができる。つまり所定の磁
界を得るために必要な電流を図2に示すaのような立上
り方をした場合に比べて、結局小さくすることができ
る。なお、図2のcに示すような過電流を励磁コイル2
に流せば、bに比べて静定時間が長くなり、より好まし
い。
Therefore, if the overcurrent IB is temporarily made to flow at the moment of reversing the direction of the magnetic field or at the moment of raising the magnetic field, as shown in FIG. 2B, as shown in FIG. The magnetic field generated in the magnetic core 3 can be strengthened by the amount of the residual magnetism (BA'-BA). That is, the current required to obtain the predetermined magnetic field can be reduced as compared with the case where the rising manner as shown in FIG. In addition, an overcurrent as shown in FIG.
It is more preferable to let it flow to (1) because the settling time becomes longer than that of (b).

【0012】前記磁界発生手段駆動回路8は、例えば図
4に示すような既知の電流制御回路を用いることがで
き、後述する演算処理装置12より磁界発生手段駆動回
路8へステップ入力を入れることにより、励磁コイル2
に、図2に示すbのような過電流IBを流すことができ
る。
The magnetic field generating means drive circuit 8 can use a known current control circuit as shown in FIG. 4, for example. By inputting a step input from the arithmetic processing unit 12 described later to the magnetic field generating means drive circuit 8. , Excitation coil 2
In addition, an overcurrent IB such as b shown in FIG. 2 can flow.

【0013】ところで、一般に磁性材料は無限に磁化で
きるものではなく、ある点で飽和が起こる。従って、残
留磁気を大きくしようとしてたくさんの電流を流して
も、ある限度以上には残留磁気を大きくすることはでき
ない。また、過電流を多く流し過ぎると、電流が定常値
に戻るまでの時間が長くなり、その間、情報をメディア
5に書き込むタイミングを半導体レーザ駆動回路11に
よって遅らせなければならないので、ドライブ装置とし
ての性能上好ましくない。
By the way, generally, magnetic materials cannot be magnetized infinitely, and saturation occurs at a certain point. Therefore, even if a large amount of current is passed to increase the remanence, the remanence cannot be increased beyond a certain limit. Further, if too much overcurrent is passed, the time until the current returns to a steady value becomes long, and the timing for writing information to the medium 5 must be delayed by the semiconductor laser drive circuit 11 during that time, so the performance as a drive device is improved. It is not preferable.

【0014】そこで、図5に示すように、先に図4で示
した磁界発生手段駆動回路8における抵抗R1、R2に
ボリューム等の調整手段8a,8bを設けた駆動回路を
用いることにより、励磁コイル2に流す電流は、磁芯3
が飽和するのに必要な電流値より小さくするように、回
路の定数を調整することが可能となる。
Therefore, as shown in FIG. 5, by using the drive circuit in which the adjusting means 8a, 8b such as the volume is provided to the resistors R1, R2 in the magnetic field generating means drive circuit 8 shown in FIG. The current flowing through the coil 2 is the magnetic core 3
It is possible to adjust the constant of the circuit so that the current value is smaller than the current value required for saturation.

【0015】一方、メディア5の下方には、前記磁界発
生手段Aに対向して、対物レンズ6等を搭載したキャリ
ッジ7が配置されている。このキャリッジ7には、対物
レンズ位置検出手段9が接続されており、また対物レン
ズ6を移動させるための駆動回路10に接続されてい
る。そして、半導体レーザ駆動回路11と、上述した磁
界発生手段駆動回路8、対物レンズ位置検出手段9、駆
動回路10はそれぞれ演算処理装置12に接続されてお
り、これら各回路等はこの演算処理装置12により制御
される。
On the other hand, below the medium 5, a carriage 7 having an objective lens 6 and the like mounted thereon is arranged so as to face the magnetic field generating means A. The objective lens position detecting means 9 is connected to the carriage 7, and is also connected to a drive circuit 10 for moving the objective lens 6. The semiconductor laser drive circuit 11, the magnetic field generation means drive circuit 8, the objective lens position detection means 9, and the drive circuit 10 described above are connected to an arithmetic processing unit 12, and these respective circuits and the like are connected to the arithmetic processing unit 12. Controlled by.

【0016】次に、本実施例にかかる装置の実施例につ
いて説明する。メディア5に情報を書き込む場合には、
指定された目標トラック情報を演算処理装置12が受け
取ると、演算処理装置12は駆動回路10に駆動信号を
与える。それにより、該駆動回路10はキャリッジ7を
目標トラックへ移動させる。そして、目標トラックに到
達したことを対物レンズ位置検出手段9によって検出す
ると、その検出信号が演算処理装置12に伝えられる。
この演算処理装置12より磁界発生手段駆動回路8へ駆
動命令が送られる。すると、磁界発生手段駆動回路8は
励磁コイル2に、上述した図2に示すbのような過電流
IBを供給し、この過電流によってメディア5にかかる
磁界Bは、図3に示すようにBBからBA’へ変動す
る。このタイミングを見計らって演算処理装置12は半
導体レーザ駆動回路11へ点灯命令を送り、情報がメデ
ィア5に記録されることになる。
Next, an embodiment of the apparatus according to this embodiment will be described. When writing information to media 5,
When the arithmetic processing unit 12 receives the designated target track information, the arithmetic processing unit 12 gives a drive signal to the drive circuit 10. Thereby, the drive circuit 10 moves the carriage 7 to the target track. Then, when the objective lens position detecting means 9 detects that the target track has been reached, the detection signal is transmitted to the arithmetic processing unit 12.
A drive command is sent from the arithmetic processing unit 12 to the magnetic field generating means drive circuit 8. Then, the magnetic field generator driving circuit 8 supplies the exciting coil 2 with the overcurrent IB as shown in FIG. 2B, and the magnetic field B applied to the medium 5 by this overcurrent is BB as shown in FIG. To BA '. In consideration of this timing, the arithmetic processing unit 12 sends a lighting command to the semiconductor laser drive circuit 11, and the information is recorded on the medium 5.

【0017】次に、図6に基づいて他の実施例を説明す
る。図6に示す実施例は、前述した図1に示す実施例と
同一の部分については同一の番号が付してある。先の実
施例と異なるところは、メディア5の近傍に磁気を検知
するためのホール素子等からなる磁気センサー13が配
置されていることと、この磁気センサー13から得られ
る信号が入力されるゲイン可変アンプ14が演算処理装
置12と磁界発生手段駆動回路8との間に介在されてい
ることである。
Next, another embodiment will be described with reference to FIG. In the embodiment shown in FIG. 6, the same parts as those in the embodiment shown in FIG. 1 described above are designated by the same reference numerals. The difference from the previous embodiment is that a magnetic sensor 13 including a Hall element for detecting magnetism is arranged in the vicinity of the medium 5, and a gain variable to which a signal obtained from the magnetic sensor 13 is input. That is, the amplifier 14 is interposed between the arithmetic processing unit 12 and the magnetic field generating means drive circuit 8.

【0018】従って、前記磁気センサー13からの出力
は、ゲイン可変アンプ14を介して磁界発生手段駆動回
路8へ送られる。前記ゲイン可変アンプ14は、磁気セ
ンサー13の出力に基づいて、磁界発生手段駆動回路8
へ入力するゲインを変え、そのゲインによって励磁コイ
ル2に流れる電流の波形を変える。このような構成にす
ることにより、磁芯3の残留磁界を磁気センサー13で
検知して常に最適な電流波形を作りだすことができる。
Therefore, the output from the magnetic sensor 13 is sent to the magnetic field generating means drive circuit 8 via the variable gain amplifier 14. The variable gain amplifier 14 uses the output of the magnetic sensor 13 to drive the magnetic field generating means 8
The gain input to is changed, and the waveform of the current flowing through the exciting coil 2 is changed according to the gain. With such a configuration, the residual magnetic field of the magnetic core 3 can be detected by the magnetic sensor 13 and an optimum current waveform can always be created.

【0019】[0019]

【発明の効果】以上説明したように、本発明によれば、
極性反転時に瞬間的に通電時よりも多くの電流を流して
いるので、所定の磁界を作るのに必要な通電時の電流値
が残留磁気の分だけ少なくて済む。従って、消費電流が
少なくなり、また装置内の発熱を押さえることができ
る。また、残留磁気を発生させるための最低限の電流し
か流さないので、電源を小型化、低コスト化できる。さ
らに、磁芯に残っている残留磁気の量を検知して励磁コ
イルに流す電流量を制御するので、電流設定値の精度が
向上する。
As described above, according to the present invention,
Since more current is instantaneously applied when the polarity is reversed than when the current is applied, the current value required when the current is applied to create a predetermined magnetic field can be reduced by the amount of residual magnetism. Therefore, current consumption is reduced, and heat generation in the device can be suppressed. Moreover, since only the minimum current for generating the residual magnetism is passed, the power supply can be downsized and the cost can be reduced. Furthermore, since the amount of residual magnetism remaining in the magnetic core is detected and the amount of current flowing through the exciting coil is controlled, the accuracy of the current set value is improved.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の1実施例を示す装置説明図である。FIG. 1 is an explanatory diagram of an apparatus showing one embodiment of the present invention.

【図2】励磁コイルに流れる電流の特性を示す説明図で
ある。
FIG. 2 is an explanatory diagram showing characteristics of a current flowing through an exciting coil.

【図3】コイル磁界と磁束密度との関係を示す説明図で
ある。
FIG. 3 is an explanatory diagram showing a relationship between a coil magnetic field and a magnetic flux density.

【図4】磁界発生手段駆動回路を示す説明図である。FIG. 4 is an explanatory diagram showing a magnetic field generation unit drive circuit.

【図5】他の磁界発生手段駆動回路を示す説明図であ
る。
FIG. 5 is an explanatory diagram showing another magnetic field generating means drive circuit.

【図6】他の実施例を示す装置説明図である。FIG. 6 is an explanatory view of an apparatus showing another embodiment.

【符号の説明】[Explanation of symbols]

1 ボビン 2 励磁コイル 3 磁芯 4 カバー 5 メディア 6 対物レンズ 7 キャリッジ 8 磁界発生手段駆動回路 8a,8b 調整手段 9 対物レンズ位置検出手段 10 駆動回路 11 半導体レーザ駆動回路 12 演算処理装置 13 磁界センサー 14 ゲイン可変アンプ 1 Bobbin 2 Excitation Coil 3 Magnetic Core 4 Cover 5 Media 6 Objective Lens 7 Carriage 8 Magnetic Field Generation Means Driving Circuit 8a, 8b Adjusting Means 9 Objective Lens Position Detecting Means 10 Driving Circuit 11 Semiconductor Laser Driving Circuit 12 Arithmetic Processor 13 Magnetic Field Sensor 14 Variable gain amplifier

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 光源からの光ビームを対物レンズで集光
してその光磁気記録媒体にスポットを形成し、この光磁
気記録媒体に情報を記録または消去するために前記光磁
気記録媒体にバイアス磁界を印加するための磁界印加装
置において、半硬質磁性材料または軟質磁性材料より形
成される磁芯と、前記磁芯の極性を反転し得る励磁コイ
ルと、この励磁コイルに通常電流を供給する通常電流供
給手段と、極性反転時に前記励磁コイルに過電流を供給
する過電流供給手段とを具備することを特徴とする磁界
印加装置。
1. A light beam from a light source is condensed by an objective lens to form a spot on the magneto-optical recording medium, and a bias is applied to the magneto-optical recording medium to record or erase information on the magneto-optical recording medium. In a magnetic field applying device for applying a magnetic field, a magnetic core formed of a semi-hard magnetic material or a soft magnetic material, an exciting coil capable of reversing the polarity of the magnetic core, and a normal current usually supplied to this exciting coil A magnetic field applying device comprising: a current supply means; and an overcurrent supply means for supplying an overcurrent to the exciting coil when the polarity is reversed.
【請求項2】 前記過電流供給手段は、前記磁芯の磁気
飽和電流値より小さい過電流を励磁コイルに供給するこ
とを特徴とする請求項1記載の磁界印加装置。
2. The magnetic field applying apparatus according to claim 1, wherein the overcurrent supplying means supplies an overcurrent smaller than a magnetic saturation current value of the magnetic core to the exciting coil.
【請求項3】 光磁気記録媒体の近傍に配置される磁気
センサーと、この磁気センサーからの出力信号に基づい
て前記励磁コイルに流す電流を制御する制御回路を有す
ることを特徴とする請求項1または請求項2記載の磁界
印加装置。
3. A magnetic sensor arranged near the magneto-optical recording medium, and a control circuit for controlling a current flowing through the exciting coil based on an output signal from the magnetic sensor. Alternatively, the magnetic field applying device according to claim 2.
JP05127028A 1993-05-28 1993-05-28 Magnetic field application device Expired - Fee Related JP3137501B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP05127028A JP3137501B2 (en) 1993-05-28 1993-05-28 Magnetic field application device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP05127028A JP3137501B2 (en) 1993-05-28 1993-05-28 Magnetic field application device

Publications (2)

Publication Number Publication Date
JPH06338003A true JPH06338003A (en) 1994-12-06
JP3137501B2 JP3137501B2 (en) 2001-02-26

Family

ID=14949891

Family Applications (1)

Application Number Title Priority Date Filing Date
JP05127028A Expired - Fee Related JP3137501B2 (en) 1993-05-28 1993-05-28 Magnetic field application device

Country Status (1)

Country Link
JP (1) JP3137501B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
RU2289094C1 (en) * 2005-07-12 2006-12-10 ООО Опытно-механический завод Центра "Транспорт" Method and device for measuring distortion of actual rolling circle of railway wheel

Also Published As

Publication number Publication date
JP3137501B2 (en) 2001-02-26

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