JPS6394406A - Magnetic head driving circuit - Google Patents

Magnetic head driving circuit

Info

Publication number
JPS6394406A
JPS6394406A JP23867986A JP23867986A JPS6394406A JP S6394406 A JPS6394406 A JP S6394406A JP 23867986 A JP23867986 A JP 23867986A JP 23867986 A JP23867986 A JP 23867986A JP S6394406 A JPS6394406 A JP S6394406A
Authority
JP
Japan
Prior art keywords
coil
magnetic head
current
switching element
inductance
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
JP23867986A
Other languages
Japanese (ja)
Other versions
JPH0743805B2 (en
Inventor
Tadao Yoshida
忠雄 吉田
Kazuhiko Fujiie
和彦 藤家
Akira Ando
亮 安藤
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.)
Sony Corp
Original Assignee
Sony Corp
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 Sony Corp filed Critical Sony Corp
Priority to JP23867986A priority Critical patent/JPH0743805B2/en
Publication of JPS6394406A publication Critical patent/JPS6394406A/en
Publication of JPH0743805B2 publication Critical patent/JPH0743805B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B11/00Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor
    • G11B11/10Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field
    • G11B11/105Recording on or reproducing from the same record carrier wherein for these two operations the methods are covered by different main groups of groups G11B3/00 - G11B7/00 or by different subgroups of group G11B9/00; Record carriers therefor using recording by magnetic means or other means for magnetisation or demagnetisation of a record carrier, e.g. light induced spin magnetisation; Demagnetisation by thermal or stress means in the presence or not of an orienting magnetic field using a beam of light or a magnetic field for recording by change of magnetisation and a beam of light for reproducing, i.e. magneto-optical, e.g. light-induced thermomagnetic recording, spin magnetisation recording, Kerr or Faraday effect reproducing

Landscapes

  • Recording Or Reproducing By Magnetic Means (AREA)

Abstract

PURPOSE:To shorten sufficiently the rise time of a current and to cause a driving power to be sufficient even when it is small by turning alternately on and off two switching elements and changing over the direction of a current to flow at a magnetic head. CONSTITUTION:A head coil to execute the magneto-optical recording has an inductance Lx. One edge of the coil 1 is connected through an auxiliary coil 2 to a direct current power source 3 and grounded through a switching element S11. Other edge of the coil 1 is connected through an auxiliary coil 4 to a direct current power source 5 and grounded through a switching element S12. Coils 2 and 4 have an inductance Ld sufficiently larger than the inductance Lx of the coil 1. Switching elements S11 and S12 are turned on and off based on the recoding signal and controlled so as to be turned on and off alternately. Thus, the rise time of the current can be sufficiently shortened and the driving power can be made sufficient even when it is small.

Description

【発明の詳細な説明】 A、産業上の利用分野 本発明は光磁気記録を行う磁気ヘッドを駆動するだめの
磁気ヘッド駆動回路に関する。
DETAILED DESCRIPTION OF THE INVENTION A. Field of Industrial Application The present invention relates to a magnetic head drive circuit for driving a magnetic head that performs magneto-optical recording.

B0発明の概要 本発明は光磁気記録を行う磁気ヘッドを駆動するだめの
磁気ヘッド駆動回路において、少なくとも2つのスイッ
チング素子を交互にオン/オフさせ、磁気ヘッドのコイ
ルに流れる電流の向きを切換えるようにしたことにより
、該電流の立上り時間を充分に短かくすることができ、
また、省電力化を実現することができるようにしたもの
である。
B0 Summary of the Invention The present invention is a magnetic head drive circuit for driving a magnetic head that performs magneto-optical recording. By doing so, the rise time of the current can be made sufficiently short,
Furthermore, it is possible to realize power saving.

C1従来の技術 従来より、情報の書換えが可能な光磁気ディスクが知ら
れている。この光磁気ディスクに情報を記録する方法と
して、例えば第5図に示すような、いわゆる重ね書き(
オーバーライド)が可能な磁場変調による方法が提案さ
れている。すなわち、光磁気ディスク101の垂直磁化
膜101aに光学ピックアップ102による一定のレー
ザー光を照射し、垂直磁化膜101aの温度をキュリ一
点以上に上げておき、磁気ヘッド103による磁場を記
録信号で変調して、垂直磁化膜101aに該磁場の変化
のパターンに対応した磁気パターンを残すことにより、
情報の記録を行うものである。
C1 Prior Art Magneto-optical disks on which information can be written are conventionally known. As a method of recording information on this magneto-optical disk, for example, the so-called overwriting (
A method using magnetic field modulation that allows for override has been proposed. That is, the perpendicularly magnetized film 101a of the magneto-optical disk 101 is irradiated with a constant laser beam from the optical pickup 102, the temperature of the perpendicularly magnetized film 101a is raised to one Curie point or above, and the magnetic field produced by the magnetic head 103 is modulated with a recording signal. By leaving a magnetic pattern corresponding to the pattern of change in the magnetic field on the perpendicularly magnetized film 101a,
It records information.

このような磁場変調方式により記録を行う場合には、例
えば、第6図(A)に示すような矩形波状の記録信号に
対して、磁気ヘッド103のコイル103aに流れる電
流は第6図(B)に示すようなある時定数を有する積分
波形となる。また、磁気ヘッド103による磁場は、第
6図(C)に示すように、上記電流波形と略等しい積分
波形となる。ここで、工dは駆動電流であり、出はこれ
に対応する磁場の強さである。
When recording is performed using such a magnetic field modulation method, for example, the current flowing through the coil 103a of the magnetic head 103 is as shown in FIG. ) is an integral waveform with a certain time constant. Further, the magnetic field generated by the magnetic head 103 has an integral waveform substantially equal to the current waveform described above, as shown in FIG. 6(C). Here, d is the driving current, and d is the strength of the corresponding magnetic field.

D8発明が解決しようとする問題点 ところで、一般に、磁場変調方式による記録においては
、磁気ヘッドによる磁場を記録に必要な強さにし、また
磁場の立上り時間すなわち電流の立上り時間を充分に速
くする必要がある。−例として、磁場の強さHdを20
00e、立上り時間tを0.1μsecとし、駆動電流
IdをIA、また磁気ヘッドのコイルのインダクタンス
を5μHとして、第7図に示すような駆動回路を用いる
場合を考える。いま、磁気ヘッドのコイル104のイン
ダクタンスをり、抵抗105の抵抗値をRとすると、立
上り時間tは次式 により与えられる。但し、ここでは、立上り時間tを時
定数に等しいものとしている。
D8 Problems to be Solved by the Invention In general, in recording using the magnetic field modulation method, it is necessary to make the magnetic field by the magnetic head as strong as necessary for recording, and to make the rise time of the magnetic field, that is, the rise time of the current, sufficiently fast. There is. - As an example, the magnetic field strength Hd is 20
00e, the rise time t is 0.1 μsec, the drive current Id is IA, and the inductance of the magnetic head coil is 5 μH, and a drive circuit as shown in FIG. 7 is used. Now, assuming that the inductance of the coil 104 of the magnetic head is R and the resistance value of the resistor 105 is R, the rise time t is given by the following equation. However, here, the rise time t is assumed to be equal to the time constant.

ここで、上式に前述した条件t = 0.1μsec 
Here, the condition t = 0.1 μsec mentioned above in the above equation
.

L=5μHを代入して抵抗値Rを求めると、R−50Ω
となる。よって電圧源106による駆動電圧VdはVd
=1(A)X50(Ω)=50(V)となり、駆動電力
は50Wにもなってしまう。
Substituting L=5μH to find the resistance value R, we get R-50Ω.
becomes. Therefore, the driving voltage Vd by the voltage source 106 is Vd
= 1 (A) x 50 (Ω) = 50 (V), and the driving power becomes 50 W.

このように、立上り時間を充分短かくしようとすると、
駆動電力が非常に大きくなってしまうという問題点があ
った。
In this way, if you try to shorten the rise time sufficiently,
There was a problem in that the driving power became extremely large.

そこで、本発明は上述した問題点に鑑みて提案されたも
のであり、磁気ヘッドのコイルに流れる電流の立上り時
間が充分に短かく、かつ駆動電力の小さな磁気ヘッド駆
動回路を提供することを目的とする。
The present invention was proposed in view of the above-mentioned problems, and it is an object of the present invention to provide a magnetic head drive circuit in which the rise time of the current flowing through the coil of the magnetic head is sufficiently short and the drive power is low. shall be.

E0問題点を解決するだめの手段 本発明に係る磁気ヘッド駆動回路は、前述した問題点を
解決するために、光磁気記録を行う磁気ヘッドのコイル
に電流を供給するための直流電源と、記録信号に基づい
てオン/オフされる少なくとも2つのスイッチング素子
と、上記直流電源と上記磁気ヘッドのコイルとの間に設
けられ、上記磁気ヘッドのコイルのインダクタンスより
も充分大なるインダクタンスを有する補助コイルとを備
え、上記スイッチング素子を交互にオン/オフさせ、上
記磁気ヘッドのコイルに流れる電流の向きを切換えるよ
うにしたことを特徴としている。
Means for Solving the E0 Problem In order to solve the above-mentioned problems, the magnetic head drive circuit according to the present invention includes a DC power supply for supplying current to the coil of a magnetic head that performs magneto-optical recording, and a recording at least two switching elements that are turned on and off based on signals; and an auxiliary coil that is provided between the DC power supply and the coil of the magnetic head and has an inductance that is sufficiently larger than the inductance of the coil of the magnetic head. The magnetic head is characterized in that the switching element is alternately turned on and off to switch the direction of the current flowing through the coil of the magnetic head.

F1作用 本発明によれば、スイッチング素子のスイッチング時間
程度のごく短時間で、磁気ヘッドのコイルに流れる電流
の向きが瞬間的に切換えられる。
F1 action According to the present invention, the direction of the current flowing through the coil of the magnetic head can be instantaneously switched in a very short period of time equivalent to the switching time of the switching element.

G、実施例 以下、本発明の実施例について図面を参照しながら詳細
に説明する。
G. EXAMPLES Hereinafter, examples of the present invention will be described in detail with reference to the drawings.

G−1,第1の実施例 第1図に第1の実施例の磁気ヘッド駆動回路を示す。こ
の第1図において、ヘッドコイル1は、磁場変調方式に
より光磁気記録を行うだめの磁気ヘッドのコイルであり
、インダクタンスLxを有している。上記ヘッドコイル
1の一端は補助コイル2を介して直流電源3に接続され
ていると共に、スイッチング素子S11を介して接地さ
れている。また、上記ヘッドコイル1の他端は補助コイ
ル4を介して直流電源5に接続されていると共に、スイ
ッチング素子S1□を介して接地されている。上記補助
コイル2,4は、上記ヘッドコイル1のインダクタンス
Lxよりも充分大なるインダクタンスLdをそれぞれ有
している(La>Lx)。また、上記直流電源3,5は
、記録に必要な電流(定電流)を上記ヘッドコイル1に
供給するためのものである。
G-1, First Embodiment FIG. 1 shows a magnetic head drive circuit of a first embodiment. In FIG. 1, a head coil 1 is a coil of a magnetic head for performing magneto-optical recording using a magnetic field modulation method, and has an inductance Lx. One end of the head coil 1 is connected to a DC power source 3 via an auxiliary coil 2, and is also grounded via a switching element S11. The other end of the head coil 1 is connected to a DC power source 5 via an auxiliary coil 4, and is also grounded via a switching element S1□. The auxiliary coils 2 and 4 each have an inductance Ld that is sufficiently larger than the inductance Lx of the head coil 1 (La>Lx). Further, the DC power supplies 3 and 5 are for supplying the head coil 1 with a current (constant current) necessary for recording.

また、上記スイッチング素子So + 812は、記録
信号に基づいてオン/オフされるようになっており、交
互にオン/オフされるよう釦なっている。すなわち、一
方がオンの時、他方はオフとなるように制御される。な
お、上記スイッチング素子S、1゜S1□には、実際に
は、トランジスタあるいはFET(電界効果トランジス
タ)等が用いられる。
Further, the switching element So + 812 is turned on/off based on the recording signal, and has a button so that it can be turned on/off alternately. That is, when one is on, the other is controlled to be off. Note that a transistor or a FET (field effect transistor) or the like is actually used for the switching element S, 1°S1□.

続いて、このように構成された磁気ヘッド駆動回路の動
作について説明する。なお、ヘッドコイル1に流れる電
流をIxとする。
Next, the operation of the magnetic head drive circuit configured as described above will be explained. Note that the current flowing through the head coil 1 is assumed to be Ix.

いま、スイッチング素子Sllがオンであり、スイッチ
ング素子S1□がオフの場合を考える。この時、補助コ
イル2には電源3による電流I、が流れ、補助コイル4
およびヘッドコイル1には電源5による電流工2が流れ
(IX=I2)、よって、スイッチング素子Sttには
これらの総和電流が流れる。ここで、I、=I、とする
と、補助コイル4およびヘッドコイル1に蓄えられるエ
ネルギーは、それぞれとなる。
Now, consider a case where switching element Sll is on and switching element S1□ is off. At this time, a current I from the power source 3 flows through the auxiliary coil 2, and the auxiliary coil 4
A current 2 from the power source 5 flows through the head coil 1 (IX=I2), and therefore, the sum of these currents flows through the switching element Stt. Here, if I,=I, the energy stored in the auxiliary coil 4 and the head coil 1 will be respectively.

次に、第2図に示すように、スイッチング素子Sllが
オフとなり、スイッチング素子S12がオンとなると、
この瞬間に補助コイル2とヘッドコイル1との接続点P
に高電圧(瞬間的には例えば数百V程度)が発生する。
Next, as shown in FIG. 2, when the switching element Sll is turned off and the switching element S12 is turned on,
At this moment, the connection point P between the auxiliary coil 2 and the head coil 1
A high voltage (instantaneously, for example, about several hundred volts) is generated.

そして、その後、補助コイル2およびヘッドコイル1に
流れる電流は同一となる。この電流を工、とすると次式
に示す関係が成立する。
After that, the current flowing through the auxiliary coil 2 and the head coil 1 becomes the same. If this current is expressed as , then the relationship shown in the following equation holds true.

この(1)式は、補助コイル2およびヘントコイル1に
それぞれ蓄えられるエネルギーの総和は、スイッチング
素子811 + s、tの切換の前後で等しくなるとい
うことを示している。上記(1)式を工、について解く
と、 となる。ここで、前述したように、L(1:>Lxであ
ることから、 工3 ”e II            °−(3)
となり、ヘッドコイル1には向きが逆でほぼ同一の値の
電流を流すことができる。また、時間の概念はどこにも
なく、スイッチング素子S1□、Sl、のスイッチング
時間程度のごく短時間で、ヘッドコイル1に流れる電流
の向きを瞬間的に切換えることができる。この様子を第
3図のタイムチャートに示す。すなわち、例えば、第3
図(A)に示すような矩形波状の記録信号に基づいて、
スイッチング素子So + 812は第3図(B)およ
び第3図(C)に示すように交互にオン/オフされる。
This equation (1) indicates that the total sum of energy stored in the auxiliary coil 2 and the hent coil 1 is equal before and after the switching elements 811 + s and t are switched. Solving the above equation (1) for engineering gives the following. Here, as mentioned above, since L(1:>Lx)
Therefore, currents of approximately the same value can be passed through the head coil 1 in opposite directions. Further, there is no concept of time, and the direction of the current flowing through the head coil 1 can be instantaneously switched in a very short time, such as the switching time of the switching elements S1□ and Sl. This situation is shown in the time chart of FIG. That is, for example, the third
Based on the rectangular waveform recording signal as shown in figure (A),
The switching element So + 812 is alternately turned on and off as shown in FIG. 3(B) and FIG. 3(C).

そして、この結果、ヘッドコイル1に流れる電流Ixは
、第3図(D)に示すように、はとんど鈍りのない矩形
波状の波形となり、スイッチング素子So + SI2
が切換わる度に電流Ixの向きが瞬間的に切換えられる
ことになる。
As a result, the current Ix flowing through the head coil 1 has a rectangular waveform with almost no dullness, as shown in FIG. 3(D), and the current Ix flows through the switching element So + SI2.
Each time the current Ix is switched, the direction of the current Ix is instantaneously switched.

また、この実施例の磁気ヘッド駆動回路には、素子とし
ての抵抗がなく、電源3,5は各コイル1.2.4の抵
抗弁に対して電流を流せば良いため、駆動電力は小さく
て済み、省電力化を実現することができる。
In addition, the magnetic head drive circuit of this embodiment has no resistance as an element, and the power supplies 3 and 5 only need to send current to the resistance valves of each coil 1, 2, and 4, so the drive power is small. It is possible to realize power saving.

なお、現実には、記録信号の周波数をfとすると、 で示されるエネルギーが、スイッチング素子S、1゜S
12の切換えの度に損失される。そこで、例えばLx=
5μHt Ix=IA、 f=500KHzとして(4
)式の値を算出すると、1.25Wのエネルギー損失が
発生することになるが、このエネルギー損失を加味して
も、充分な省電力化が図られていることになる。
In reality, if the frequency of the recording signal is f, then the energy shown by the switching element S, 1°S
It is lost every time 12 switches. So, for example, Lx=
5μHt Ix=IA, f=500KHz (4
) Calculating the value of the equation results in an energy loss of 1.25 W, but even when this energy loss is taken into consideration, sufficient power saving is achieved.

G−2,第2の実施例 第4図に第2の実施例の磁気ヘッド駆動回路を示す。こ
の第4図において、磁気ヘッドのコイルであるヘッドコ
イル6の一端はスイッチング素子S21を介して、直流
電源7に接続された補助コイル8に接続されていると共
に、スイッチング素子S2□を介して接地されている。
G-2, Second Embodiment FIG. 4 shows a magnetic head drive circuit of a second embodiment. In FIG. 4, one end of the head coil 6, which is the coil of the magnetic head, is connected to an auxiliary coil 8 connected to a DC power supply 7 via a switching element S21, and is also grounded via a switching element S2□. has been done.

また、上記ヘッドコイル6の他端はスイッチング素子8
23を介して上記補助コイル8に接続されていると共に
、スイッチング素子S2.を介して接地されている。上
記補助コイル8は、ヘッドコイル6のインダクタンスL
x’よりも充分大なるインダクタンスLd’を有してい
る。また、スイッチング素子Sttとスイッチング素子
S21、およびスイッチング素子S22とスイッチング
素子S23は、それぞれ連動して切換えられる。また、
各スイッチング素子対は、記録信号に基づいて交互にオ
ン/オフされるようになっている。
The other end of the head coil 6 is connected to a switching element 8.
23 to the auxiliary coil 8, and the switching element S2. is grounded through. The auxiliary coil 8 has an inductance L of the head coil 6.
It has an inductance Ld' that is sufficiently larger than x'. Further, the switching element Stt and the switching element S21, and the switching element S22 and the switching element S23 are respectively switched in conjunction with each other. Also,
Each pair of switching elements is alternately turned on and off based on a recording signal.

このように構成された第2の実施例の磁気ヘッド駆動回
路は、前述した第1の実施例のものと同様の動作原理に
基づいて駆動される。よって、動作の説明を省略する。
The magnetic head drive circuit of the second embodiment thus configured is driven based on the same operating principle as that of the first embodiment described above. Therefore, the explanation of the operation will be omitted.

また、第1の実施例のものと同様の効果が得られること
は勿論である。
Moreover, it goes without saying that the same effects as those of the first embodiment can be obtained.

H0発明の効果 上述した実施例の説明から明らかなように、本発明の磁
気ヘッド駆動回路によれば、少なくとも2つのスイッチ
ング素子を交互にオン/オフさせ、磁気ヘッドのコイル
に流れる電流の向きを切換えるようにしており、該電流
の立上り時間を充分に短かくすることができる。また、
素子としての抵抗を用いておらず、直流電源はコイルの
抵抗分に対して電流を流せば良いため、駆動電力は小さ
くて済み、省電力化を実現することができる。
H0 Effects of the Invention As is clear from the description of the embodiments described above, the magnetic head drive circuit of the present invention alternately turns on and off at least two switching elements to control the direction of the current flowing through the coil of the magnetic head. The current rise time can be made sufficiently short. Also,
Since no resistance is used as an element, and the DC power supply only needs to flow a current corresponding to the resistance of the coil, the driving power is small, and power saving can be achieved.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明に係る磁気ヘッド駆動回路の第1の実施
例を示す回路図、第2図は上記第1の実施例の動作を説
明するだめの回路図、第3図は同じくタイムチャート、
第4図は本発明に係る磁気ヘッド駆動回路の第2の実施
例を示す回路図である。 第5図は磁場変調方式を説、明するための模式図、第6
図は従来例を説明するためのタイムチャート、第7図は
磁気ヘッド駆動回路の従来例を示す回路図である。 1.6・・・ヘッドコイル 2.4.8・・・補助コイル 3.5.7・・・直流電源 S++ + SI2* S21 + 52215231
 S24 ・・・ス(yfン”素子
FIG. 1 is a circuit diagram showing a first embodiment of the magnetic head drive circuit according to the present invention, FIG. 2 is a circuit diagram for explaining the operation of the first embodiment, and FIG. 3 is a time chart. ,
FIG. 4 is a circuit diagram showing a second embodiment of the magnetic head drive circuit according to the present invention. Figure 5 is a schematic diagram for explaining the magnetic field modulation method, Figure 6
The figure is a time chart for explaining a conventional example, and FIG. 7 is a circuit diagram showing a conventional example of a magnetic head drive circuit. 1.6... Head coil 2.4.8... Auxiliary coil 3.5.7... DC power supply S++ + SI2* S21 + 52215231
S24...S(yfn" element)

Claims (1)

【特許請求の範囲】 光磁気記録を行う磁気ヘッドのコイルに電流を供給する
ための直流電源と、 記録信号に基づいてオン/オフされる少なくとも2つの
スイッチング素子と、 上記直流電源と上記磁気ヘッドのコイルとの間に設けら
れ、上記磁気ヘッドのコイルのインダクタンスよりも充
分大なるインダクタンスを有する補助コイルとを備え、 上記スイッチング素子を交互にオン/オフさせ、上記磁
気ヘッドのコイルに流れる電流の向きを切換えるように
したことを特徴とする磁気ヘッド駆動回路。
[Claims] A DC power source for supplying current to a coil of a magnetic head that performs magneto-optical recording, at least two switching elements that are turned on/off based on recording signals, the DC power source and the magnetic head. and an auxiliary coil provided between the coil of the magnetic head and having an inductance sufficiently larger than the inductance of the coil of the magnetic head, the switching element is alternately turned on and off to control the current flowing through the coil of the magnetic head. A magnetic head drive circuit characterized by switching the direction.
JP23867986A 1986-10-07 1986-10-07 Magnetic head drive circuit Expired - Fee Related JPH0743805B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23867986A JPH0743805B2 (en) 1986-10-07 1986-10-07 Magnetic head drive circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23867986A JPH0743805B2 (en) 1986-10-07 1986-10-07 Magnetic head drive circuit

Publications (2)

Publication Number Publication Date
JPS6394406A true JPS6394406A (en) 1988-04-25
JPH0743805B2 JPH0743805B2 (en) 1995-05-15

Family

ID=17033694

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23867986A Expired - Fee Related JPH0743805B2 (en) 1986-10-07 1986-10-07 Magnetic head drive circuit

Country Status (1)

Country Link
JP (1) JPH0743805B2 (en)

Cited By (18)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0304298A2 (en) * 1987-08-19 1989-02-22 Sony Corporation Magnetic head drive circuit
WO1992001285A1 (en) * 1990-07-13 1992-01-23 Deutsche Thomson-Brandt Gmbh Circuit for reversing a magnetic field
EP0519729A2 (en) * 1991-06-21 1992-12-23 Sharp Kabushiki Kaisha Magnetic head driving circuit
EP0540275A2 (en) * 1991-10-31 1993-05-05 Canon Kabushiki Kaisha A circuit apparatus for driving a magnetic head
EP0545579A1 (en) * 1991-11-18 1993-06-09 Sharp Kabushiki Kaisha External magnetic field generation apparatus and a magneto-optical recording apparatus
JPH0555302U (en) * 1991-12-24 1993-07-23 ティアック株式会社 Digital recording circuit
EP0576286A2 (en) * 1992-06-26 1993-12-29 Canon Kabushiki Kaisha Magnetic head driving device and magnetooptical recording apparatus
US5278809A (en) * 1990-01-17 1994-01-11 Olympus Optical Co., Ltd. Photomagnetic recording apparatus recording with alternating magnetic field and D.C. magnetic field
US5329408A (en) * 1991-07-10 1994-07-12 Sharp Kabushiki Kaisha Magnetic field modulation magnet-optical recording apparatus in which an FM modulator and a magnetic head driving circuit are used in common
US5351155A (en) * 1991-12-24 1994-09-27 Sharp Kabushiki Kaisha Magnetic head driving device with pre-recording energization with two inductors sharing a common magnetic core
US5444688A (en) * 1991-08-02 1995-08-22 Sharp Kabushiki Kaisha Information reproducing circuit
US5477509A (en) * 1993-10-26 1995-12-19 Tdk Corporation Magneto-optical head circuit for minimizing the overshoot reversing current
US5559763A (en) * 1992-03-06 1996-09-24 Canon Kabushiki Kaisha Magnetic head driving device and magnetooptical recording apparatus with acceleration coil for shortening current inversion time
US5574702A (en) * 1993-08-06 1996-11-12 Canon Kabushiki Kaisha Magnetic head current control circuit for use in a magnetic head drive device, and magnetic/magnetooptical recording apparatus using the same
US5579293A (en) * 1993-03-26 1996-11-26 Canon Kabushiki Kaisha Magnetic head driving circuit for controlling switching operations in a magnetooptical recording apparatus
US5587851A (en) * 1991-12-24 1996-12-24 Sharp Kabushiki Kaisha Magnetic head driving device with prerecording energization
US6477119B2 (en) 1999-12-16 2002-11-05 Canon Kabushiki Kaisha Magnetic head drive circuit including paired auxiliary coils, paired switching elements, and switch element control circuit, and magneto-optical recording device using the same
US6570725B1 (en) 1999-07-12 2003-05-27 Fujitsu Limited Drive circuit for magnetic head and winding configuration of magnetic head suitable for the drive circuit

Cited By (25)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0304298A2 (en) * 1987-08-19 1989-02-22 Sony Corporation Magnetic head drive circuit
US5278809A (en) * 1990-01-17 1994-01-11 Olympus Optical Co., Ltd. Photomagnetic recording apparatus recording with alternating magnetic field and D.C. magnetic field
WO1992001285A1 (en) * 1990-07-13 1992-01-23 Deutsche Thomson-Brandt Gmbh Circuit for reversing a magnetic field
EP0519729A2 (en) * 1991-06-21 1992-12-23 Sharp Kabushiki Kaisha Magnetic head driving circuit
US5359466A (en) * 1991-06-21 1994-10-25 Sharp Kabushiki Kaisha Magnetic head driving circuit with impedance elements to balance auxiliary coil loads
US5329408A (en) * 1991-07-10 1994-07-12 Sharp Kabushiki Kaisha Magnetic field modulation magnet-optical recording apparatus in which an FM modulator and a magnetic head driving circuit are used in common
US5444688A (en) * 1991-08-02 1995-08-22 Sharp Kabushiki Kaisha Information reproducing circuit
EP0540275A2 (en) * 1991-10-31 1993-05-05 Canon Kabushiki Kaisha A circuit apparatus for driving a magnetic head
US5377055A (en) * 1991-10-31 1994-12-27 Canon Kabushiki Kaisha Circuit apparatus for driving a magnetic head
EP0545579A1 (en) * 1991-11-18 1993-06-09 Sharp Kabushiki Kaisha External magnetic field generation apparatus and a magneto-optical recording apparatus
US5313444A (en) * 1991-11-18 1994-05-17 Sharp Kabushiki Kaisha External magnetic field generation apparatus capable of light intensity modulation and magnetic field modulation
EP0855704A3 (en) * 1991-12-24 2000-08-16 Sharp Kabushiki Kaisha A magnetic head driving device
US5351155A (en) * 1991-12-24 1994-09-27 Sharp Kabushiki Kaisha Magnetic head driving device with pre-recording energization with two inductors sharing a common magnetic core
JPH0555302U (en) * 1991-12-24 1993-07-23 ティアック株式会社 Digital recording circuit
US5587851A (en) * 1991-12-24 1996-12-24 Sharp Kabushiki Kaisha Magnetic head driving device with prerecording energization
EP0855704A2 (en) * 1991-12-24 1998-07-29 SHARP Corporation A magnetic head driving device
US5559763A (en) * 1992-03-06 1996-09-24 Canon Kabushiki Kaisha Magnetic head driving device and magnetooptical recording apparatus with acceleration coil for shortening current inversion time
EP0576286A2 (en) * 1992-06-26 1993-12-29 Canon Kabushiki Kaisha Magnetic head driving device and magnetooptical recording apparatus
US5661612A (en) * 1992-06-26 1997-08-26 Canon Kabushiki Kaisha Magnetic head driving device and magnetooptical recording apparatus
EP0576286A3 (en) * 1992-06-26 1994-08-10 Canon Kk Magnetic head driving device and magnetooptical recording apparatus
US5579293A (en) * 1993-03-26 1996-11-26 Canon Kabushiki Kaisha Magnetic head driving circuit for controlling switching operations in a magnetooptical recording apparatus
US5574702A (en) * 1993-08-06 1996-11-12 Canon Kabushiki Kaisha Magnetic head current control circuit for use in a magnetic head drive device, and magnetic/magnetooptical recording apparatus using the same
US5477509A (en) * 1993-10-26 1995-12-19 Tdk Corporation Magneto-optical head circuit for minimizing the overshoot reversing current
US6570725B1 (en) 1999-07-12 2003-05-27 Fujitsu Limited Drive circuit for magnetic head and winding configuration of magnetic head suitable for the drive circuit
US6477119B2 (en) 1999-12-16 2002-11-05 Canon Kabushiki Kaisha Magnetic head drive circuit including paired auxiliary coils, paired switching elements, and switch element control circuit, and magneto-optical recording device using the same

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