JPH06309607A - Magnetic field modulation overwrite system magnetic head - Google Patents

Magnetic field modulation overwrite system magnetic head

Info

Publication number
JPH06309607A
JPH06309607A JP10129793A JP10129793A JPH06309607A JP H06309607 A JPH06309607 A JP H06309607A JP 10129793 A JP10129793 A JP 10129793A JP 10129793 A JP10129793 A JP 10129793A JP H06309607 A JPH06309607 A JP H06309607A
Authority
JP
Japan
Prior art keywords
magnetic head
power consumption
coil
magnetic field
winding
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
JP10129793A
Other languages
Japanese (ja)
Other versions
JP3268058B2 (en
Inventor
Atsushi Akiyama
淳 秋山
Tomoyuki Miyake
知之 三宅
Kazuhiko Ueda
和彦 上田
Kunio Kojima
邦男 小嶋
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.)
Sharp Corp
Original Assignee
Sharp 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 Sharp Corp filed Critical Sharp Corp
Priority to JP10129793A priority Critical patent/JP3268058B2/en
Publication of JPH06309607A publication Critical patent/JPH06309607A/en
Application granted granted Critical
Publication of JP3268058B2 publication Critical patent/JP3268058B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To suppress unnecessary power consumption and to prevent the deterioration of a magnetic head by forming the winding wire of a coil with a winding wire whose diameter is specified within + or -30% or below of the wire diameter where the power consumption of the magnetic head becomes minimum. CONSTITUTION:The magnetic head consists of a core 1 and a coil 2, and the core 1 is formed out of a ferrite material having a low electric conductivity in order to reduce loss by suppressing an eddy current caused by a transmission magnetic field. Further, round the coil 2, the winding wire whose diameter within + or -30% or below of the wire diameter where the power consumption of the magnetic head becomes minimum is wound in many numbers of winding of e.g. about 30-60 turns for reducing a driving current. Therefor, a multilayer winding wire structure is constituted by about four to six layers. Thus, the unnecessary power consumption is suppressed, and also heat generation is reduced to prevent the deterioration of the magnetic head.

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、磁界変調オーバーライ
ト方式の、光磁気ディスク駆動装置やハードディスク装
置等に使用される記録用磁気ヘッドの改良に関するもの
である。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an improvement of a magnetic head for recording used in a magneto-optical disk drive device, a hard disk device or the like of a magnetic field modulation overwrite type.

【0002】[0002]

【従来の技術】近年、消去動作なしに書込が可能な磁界
変調オーバーライト技術が開発されてきた。
2. Description of the Related Art In recent years, a magnetic field modulation overwrite technique has been developed which enables writing without erasing operation.

【0003】従来の光磁気ディスク駆動装置では、書込
時には、まず、直流磁界を加えた状態で、光ピックアッ
プから出射される高出力のレーザ光を光磁気ディスクの
記録膜に照射し、一旦以前のデータを消去した後、逆向
きの直流磁界を加えた状態で、高出力のレーザ光をON
/OFFすることにより書込を行なっていた。
In the conventional magneto-optical disk drive, at the time of writing, a high-power laser beam emitted from an optical pickup is first radiated to a recording film of the magneto-optical disk in a state in which a direct current magnetic field is applied, and the recording film of the magneto-optical disk is temporarily erased. After erasing the data of, the high output laser light is turned on in the condition that the reverse DC magnetic field is applied.
Writing was performed by turning it off.

【0004】一方、磁界変調オーバーライト方式では、
光ピックアップから出射される高出力のレーザ光によ
り、光磁気ディスクの記録膜を加熱すると同時に、磁気
ヘッドにより高速で反転する磁界を与えデータを書込
む。このため、消去動作が不要となり、データ書込時間
の短縮や、リアルタイムでのデジタル音声記録が可能と
なるなど大きな利点がある。
On the other hand, in the magnetic field modulation overwrite system,
The high-power laser beam emitted from the optical pickup heats the recording film of the magneto-optical disk, and at the same time, a magnetic field is applied at high speed by the magnetic head to write data. Therefore, there is a great advantage that the erasing operation becomes unnecessary, the data writing time can be shortened, and digital voice recording can be performed in real time.

【0005】以下、磁界変調オーバーライト方式磁気ヘ
ッド(以下磁気ヘッドという)の駆動回路の動作につい
て説明する。
The operation of the drive circuit of the magnetic field modulation overwrite type magnetic head (hereinafter referred to as the magnetic head) will be described below.

【0006】図4は、その駆動回路の一例の回路図であ
る。磁界変調オーバーライトにおいては、前述のごとく
高速で磁界を反転させる必要があるため、図4に示され
るように、電界効果トランジスタ(以下トランジスタと
いう)Q1 〜Q4 をHブリッジ接続し、直列のトランジ
スタQ1 ,Q3 およびQ2 ,Q4 の間にそれぞれダイオ
ードD1 およびD2 によるスイッチを付加し、トランジ
スタQ3 とQ4 との間に磁気ヘッドのコイルLを接続し
た構成の磁気ヘッド駆動回路が、たとえば特開平1−1
30302号公報に開示されている。
FIG. 4 is a circuit diagram of an example of the drive circuit. In the magnetic field modulation overwrite, it is necessary to reverse the magnetic field at a high speed as described above, and therefore, as shown in FIG. 4, field effect transistors (hereinafter referred to as transistors) Q 1 to Q 4 are connected in H bridge and connected in series. A magnetic head having a configuration in which switches by diodes D 1 and D 2 are added between the transistors Q 1 , Q 3 and Q 2 , Q 4 , respectively, and a coil L of the magnetic head is connected between the transistors Q 3 and Q 4. The drive circuit is, for example, Japanese Patent Laid-Open No. 1-1.
It is disclosed in Japanese Patent No. 30302.

【0007】トランジスタQ1 ,Q4 およびトランジス
タQ2 ,Q3 の2組のトランジスタには、それぞれ交互
にON,OFFを繰り返すように制御信号が与えられ
る。すなわち、トランジスタQ1 ,Q4 がONのときに
は、トランジスタQ2 ,Q3 はOFFに、トランジスタ
1 ,Q4 がOFFのときには、トランジスタQ2 ,Q
3 がオンになる。このため、コイルLに流れる電流は反
転し、結果として磁界も反転する。また、トランジスタ
1 ,Q4 がONの状態からOFFに反転した直後は、
コイルLが発生する逆起電圧により、ダイオードD2
カソードには、数十Vの高電圧がかかるため、ダイオー
ドD2 はOFF状態となる。これにより、トランジスタ
3 ,Q4 およびコイルLのループが形成される。この
ループは、コイルLのインダクタンスおよび抵抗ならび
にトランジスタQ3 およびQ4 のキャパシタンスおよび
オン抵抗等からなるLCRの共振回路をなしており、L
CRの値により決まる時定数で電流が反転する。
Transistor Q1, QFourAnd Transis
Q2, Q3The two sets of transistors are alternately
Is given a control signal to repeat ON and OFF
It That is, the transistor Q1, QFourWhen is ON
Is the transistor Q2, Q3Off, transistor
Q1, QFourIs off, transistor Q2, Q
3Turns on. Therefore, the current flowing through the coil L is
And, as a result, the magnetic field is also reversed. Also transistors
Q1, QFourImmediately after turning from ON to OFF,
Due to the counter electromotive voltage generated by the coil L, the diode D2of
Since a high voltage of several tens of volts is applied to the cathode,
De D2Is turned off. This allows the transistor
Q3, QFourAnd the loop of the coil L is formed. this
The loop consists of the inductance and resistance of the coil L and
Transistor Q3And QFourCapacitance and
It forms an LCR resonance circuit consisting of on-resistance, etc.
The current is inverted with a time constant determined by the value of CR.

【0008】このように、この構成の磁気ヘッド駆動回
路では、電流反転時におけるLCRの共振現象を利用す
るため、比較的大きなインダクタンスを持つ磁気ヘッド
でも、CとRの値を適切に選ぶことにより高速で磁界反
転が可能となる。
As described above, in the magnetic head drive circuit having this configuration, the resonance phenomenon of LCR at the time of current reversal is utilized, so that even if the magnetic head has a relatively large inductance, the values of C and R can be appropriately selected. Magnetic field reversal becomes possible at high speed.

【0009】磁界変調オーバーライト方式では、前述の
ごとく、高速の電流反転を行ない、また、記録周波数も
数百KHz〜数MHzと高いため、磁気ヘッドにおける
電力損失が大きくなる。このため、従来より、磁気ヘッ
ドの電力損失を低減するための研究が行なわれてきた。
たとえば、「磁界変調光磁気記録用磁気ヘッド」(電子
情報通信学会、磁気記録研究会資料、MR87−52
13〜20頁)に詳細に開示されている。
In the magnetic field modulation overwrite method, as described above, high-speed current reversal is performed, and the recording frequency is as high as several hundred KHz to several MHz, so that the power loss in the magnetic head becomes large. For this reason, research has been conventionally conducted to reduce the power loss of the magnetic head.
For example, "magnetic head for magnetic field modulation magneto-optical recording" (The Institute of Electronics, Information and Communication Engineers, Magnetic Recording Research Group material, MR87-52).
13-20).

【0010】[0010]

【発明が解決しようとする課題】ところで、従来は磁気
ヘッドのコアの形状や材質等については、前述の開示に
も示されるように検討が行なわれてきたが、磁気ヘッド
のコイルの巻線径については検討が不十分なため、低消
費電力化に最適な巻線径が明確になっておらず、その結
果、巻線径が不適切であり消費電力が大きくなってしま
っていた。前述の開示においても、巻線径40μm以下
の場合(16頁)および30μmの場合(18頁)につ
いて述べているにすぎない。
By the way, the shape and material of the core of the magnetic head have been conventionally examined as shown in the above disclosure, but the winding diameter of the coil of the magnetic head has been studied. However, due to insufficient studies, the optimum winding diameter for low power consumption has not been clarified, and as a result, the winding diameter is inappropriate and power consumption has increased. Also in the above disclosure, only the case where the winding diameter is 40 μm or less (page 16) and the case where the winding diameter is 30 μm (page 18) are described.

【0011】本発明は、このような従来の問題点を解決
し、消費電力を少なくし、また、磁気ヘッドの発熱を抑
える記録用磁気ヘッドを提供することを目的とする。
SUMMARY OF THE INVENTION It is an object of the present invention to solve the above-mentioned conventional problems, to provide a recording magnetic head which consumes less power and suppresses heat generation of the magnetic head.

【0012】[0012]

【課題を解決するための手段】本発明の磁界変調オーバ
ーライト方式磁気ヘッドにおいては、磁気ヘッドのコイ
ルの巻線を、使用する記録信号帯域の中で平均して磁気
ヘッドの電力消費が最小となる線径の±30%以内の線
径を有する巻線により構成するようにした。
In the magnetic field modulation overwrite type magnetic head of the present invention, the winding of the coil of the magnetic head is averaged in the recording signal band to be used and the power consumption of the magnetic head is minimized. The wire diameter is within ± 30% of the wire diameter.

【0013】[0013]

【作用】本発明によれば、巻線径が、記録周波数帯によ
って決まる電力消費最小の線径付近とされるため、低消
費電力化が図れる。また、磁気ヘッドでの発熱が減少
し、磁気ヘッドの劣化が抑えられる。
According to the present invention, the winding diameter is set to be near the minimum power consumption wire diameter determined by the recording frequency band, so that the power consumption can be reduced. Further, heat generation in the magnetic head is reduced, and deterioration of the magnetic head is suppressed.

【0014】[0014]

【実施例】図1(a)は本発明の一実施例の磁気ヘッド
の平面図であり、同図(b)はそのA−A′断面図であ
る。
1 (a) is a plan view of a magnetic head according to an embodiment of the present invention, and FIG. 1 (b) is a sectional view taken along line AA '.

【0015】磁気ヘッドは、コア1およびコイル2から
なる。コア1は、透過磁界により発生する渦電流を抑制
し、損失を低減するため、導電率の低い(たとえば30
0〜700Ω・cm)フェライト材料からなる。また、
コイル2は駆動電流を低減するため、巻数が多く(たと
えば30〜60ターン)巻かれており、そのため、4〜
6層程度の多層巻線構造となっている。図1(b)で
は、4層の場合を示している。
The magnetic head comprises a core 1 and a coil 2. The core 1 suppresses the eddy current generated by the transmission magnetic field and reduces the loss, so that the core 1 has a low conductivity (for example, 30
0 to 700 Ω · cm) made of ferrite material. Also,
The coil 2 has a large number of turns (for example, 30 to 60 turns) to reduce the drive current, and therefore 4 to 4 turns.
It has a multi-layer winding structure of about 6 layers. FIG. 1B shows the case of four layers.

【0016】図2は、図1(a),(b)に示される磁
気ヘッドについて、線径(50μm,60μm,90μ
mの3種類)および記録周波数(200KHz〜1MH
z)を変えて消費電力を測定した結果のグラフである。
図2に示されるように、低い周波数では線径が太い方が
消費電力は小さく、高い周波数では、線径が細い方が消
費電力は小さい。また、中間の周波数では、中くらいの
線径の磁気ヘッドが一番消費電力が少ない。このよう
に、記録周波数によって消費電力が最小となる線径は異
なる。このため、消費電力を抑えるためには、使用され
る記録信号帯域の中で平均して電力消費が最小となるよ
うに、記録周波数に応じて線径を選択することが重要で
ある。
FIG. 2 shows the wire diameter (50 μm, 60 μm, 90 μm) of the magnetic head shown in FIGS. 1 (a) and 1 (b).
m) and recording frequency (200 KHz to 1 MH)
It is a graph of the result of having measured power consumption by changing z).
As shown in FIG. 2, the power consumption is smaller when the wire diameter is thicker at low frequencies, and the power consumption is smaller when the wire diameter is thinner at high frequencies. Further, at the intermediate frequency, the magnetic head having the medium diameter has the lowest power consumption. In this way, the wire diameter that minimizes the power consumption varies depending on the recording frequency. Therefore, in order to suppress the power consumption, it is important to select the wire diameter according to the recording frequency so that the power consumption is averaged minimum in the recording signal band used.

【0017】図3は、一例として、コンパクトディスク
(CD)等で用いられるEFM(Eight Fourteen Modul
ation )信号(周波数帯域200KHz〜720KH
z)を磁気ヘッドに加えたときの消費電力測定結果のグ
ラフである。この場合、線径が70μm近傍のとき消費
電力が最も低いことがわかる。また、50〜85μmの
範囲では、70μmに比べ消費電力の差は20mW程度
で比較的小さいが、その範囲を超えると急激に消費電力
が増える。したがって、線径は70μmを中心として±
30%程度の範囲内であれば、使用に耐える。よって、
光磁気ディスクを用いた磁界変調オーバーライト方式の
書換可能型CD装置の記録用磁気ヘッドには、約50〜
85μmの線径のコイルを使用するのがよい。
FIG. 3 shows, as an example, an EFM (Eight Fourteen Modul) used in a compact disc (CD) or the like.
ation) signal (frequency band 200 KHz to 720 KH
7 is a graph of power consumption measurement results when z) is added to the magnetic head. In this case, it can be seen that the power consumption is lowest when the wire diameter is around 70 μm. Further, in the range of 50 to 85 μm, the difference in power consumption is about 20 mW, which is relatively small compared to 70 μm, but if it exceeds the range, the power consumption increases rapidly. Therefore, the wire diameter is centered around 70 μm ±
If it is within the range of about 30%, it can be used. Therefore,
The recording magnetic head of a rewritable CD device of the magnetic field modulation overwrite type using a magneto-optical disk has about 50
It is preferable to use a coil having a wire diameter of 85 μm.

【0018】記録信号帯域が増加したときも、同様の傾
向があるものと類推さる。
It is assumed that there is a similar tendency when the recording signal band increases.

【0019】[0019]

【発明の効果】以上のように、本発明によれば、記録信
号の周波数帯域により磁気ヘッドでの消費電力が最小と
なるように線径を選ぶことができるので、不要な電力消
費を抑え、同時に発熱も少なくなり、磁気ヘッドの劣化
を防ぐことができる。
As described above, according to the present invention, the wire diameter can be selected so that the power consumption in the magnetic head is minimized depending on the frequency band of the recording signal, so that unnecessary power consumption can be suppressed. At the same time, less heat is generated, and deterioration of the magnetic head can be prevented.

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

【図1】(a)は本発明の一実施例による磁気ヘッドの
平面図、(b)は(a)のA−A′断面図である。
1A is a plan view of a magnetic head according to an embodiment of the present invention, and FIG. 1B is a sectional view taken along line AA ′ of FIG.

【図2】線径による周波数と消費電力の関係を示すグラ
フである。
FIG. 2 is a graph showing the relationship between frequency and power consumption according to wire diameter.

【図3】EFM信号帯域におけるコイル線径と消費電力
の関係を示すグラフである。
FIG. 3 is a graph showing a relationship between a coil wire diameter and power consumption in an EFM signal band.

【図4】磁気ヘッドの駆動回路の一例の回路図である。FIG. 4 is a circuit diagram of an example of a drive circuit of a magnetic head.

【符号の説明】[Explanation of symbols]

1 コア 2 コイル Q1 ,Q2 ,Q3 ,Q4 トランジスタ D1 ,D2 ダイオード1 core 2 coil Q 1 , Q 2 , Q 3 , Q 4 transistor D 1 , D 2 diode

───────────────────────────────────────────────────── フロントページの続き (72)発明者 小嶋 邦男 大阪府大阪市阿倍野区長池町22番22号 シ ャープ株式会社内 ─────────────────────────────────────────────────── ─── Continued Front Page (72) Inventor Kunio Kojima 22-22 Nagaike-cho, Abeno-ku, Osaka-shi, Osaka

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 コアとコイルとよりなり、 コイルの巻線は、使用する記録信号帯域の中で平均して
磁気ヘッドの電力消費が最小となる線径の±30%以内
の線径を有する巻線により構成されていることを特徴と
する磁界変調オーバーライト方式磁気ヘッド。
1. A core and a coil, wherein a winding of the coil has a wire diameter within ± 30% of a wire diameter at which the power consumption of the magnetic head is minimum on average in a recording signal band to be used. A magnetic field modulation overwrite type magnetic head comprising a winding.
【請求項2】 使用する記録信号帯域が200KHz〜
720KHzのEFM信号のとき、巻線の線径は50〜
85μmであることを特徴とする請求項1記載の磁界変
調オーバーライト方式磁気ヘッド。
2. The recording signal band used is from 200 KHz to
When the EFM signal is 720 KHz, the wire diameter of the winding is 50 ~
The magnetic field modulation overwrite type magnetic head according to claim 1, wherein the magnetic head has a thickness of 85 μm.
JP10129793A 1993-04-27 1993-04-27 Magnetic field modulation overwrite type magnetic head Expired - Fee Related JP3268058B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10129793A JP3268058B2 (en) 1993-04-27 1993-04-27 Magnetic field modulation overwrite type magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10129793A JP3268058B2 (en) 1993-04-27 1993-04-27 Magnetic field modulation overwrite type magnetic head

Publications (2)

Publication Number Publication Date
JPH06309607A true JPH06309607A (en) 1994-11-04
JP3268058B2 JP3268058B2 (en) 2002-03-25

Family

ID=14296898

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10129793A Expired - Fee Related JP3268058B2 (en) 1993-04-27 1993-04-27 Magnetic field modulation overwrite type magnetic head

Country Status (1)

Country Link
JP (1) JP3268058B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR19990056215A (en) * 1997-12-29 1999-07-15 윤종용 Coil winding method of magnetic head
US6529448B1 (en) 1998-05-07 2003-03-04 Canon Kabushiki Kaisha High speed magnetic coil for magneto-optical head

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR19990056215A (en) * 1997-12-29 1999-07-15 윤종용 Coil winding method of magnetic head
US6529448B1 (en) 1998-05-07 2003-03-04 Canon Kabushiki Kaisha High speed magnetic coil for magneto-optical head

Also Published As

Publication number Publication date
JP3268058B2 (en) 2002-03-25

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