JPS59213016A - Magnetic recording device - Google Patents

Magnetic recording device

Info

Publication number
JPS59213016A
JPS59213016A JP8500883A JP8500883A JPS59213016A JP S59213016 A JPS59213016 A JP S59213016A JP 8500883 A JP8500883 A JP 8500883A JP 8500883 A JP8500883 A JP 8500883A JP S59213016 A JPS59213016 A JP S59213016A
Authority
JP
Japan
Prior art keywords
current
magnetic head
erasing
magnetic
circuit
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.)
Pending
Application number
JP8500883A
Other languages
Japanese (ja)
Inventor
Shinichiro Wataya
和田谷 伸一郎
Kunihiro Hashimoto
邦弘 橋本
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.)
Y II DATA KK
Original Assignee
Y II DATA KK
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 Y II DATA KK filed Critical Y II DATA KK
Priority to JP8500883A priority Critical patent/JPS59213016A/en
Publication of JPS59213016A publication Critical patent/JPS59213016A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/465Arrangements for demagnetisation of heads

Landscapes

  • Digital Magnetic Recording (AREA)

Abstract

PURPOSE:To execute recording with a high density on a flexible disk by providing a self-degaussing circuit consisting of an LC resonance circuit on a magnetic head driving circuit. CONSTITUTION:When a driving current is made to flow to a driving coil of a magnetic head, a magnetic energy stored in the driving coil is utilized, and after de-energizing is completed, an AC current which is attenuated together with a time generated by a self-degaussing circuit 2 added newly is made to flow to the driving coil, and degaussing of the magnetic head is executed so as to improve a degaussing operation of the magnetic head to a recording medium. When a switch SW is closed, namely, when an erasing magnetic head 1 is operated, an erasing current iE is equal to a current of a DC constant-current source E. Accordingly, when the AC current, which is attenuated as oscillating, is made to flow to an erasing coil LE, a residual magnetic flux density can be reduced by its AC degaussing operation.

Description

【発明の詳細な説明】 本発明の第1の目的は一般の磁気記録装置としては勿論
のこと5%に可撓性ディスクに高密度に記録する磁気記
録装置として有用な磁気記録装置を提供するにある。
DETAILED DESCRIPTION OF THE INVENTION The first object of the present invention is to provide a magnetic recording device which is useful not only as a general magnetic recording device but also as a magnetic recording device for recording at a high density of 5% on a flexible disk. It is in.

他の目的は磁気ヘッド駆動回路に比較的簡単な回路を付
加するだけで性能向上を図ることのできるものを提供す
るにある。
Another object of the present invention is to provide a magnetic head drive circuit that can improve performance by simply adding a relatively simple circuit.

近時、その使い勝手の良さから事務能率向上用に可撓性
ディスクを用いた磁気記録装置が、盛んに用いられてい
ることは周知の通シであるが、更に高記録密度化並びに
小型化全目的とする研究が進められている。
It is well known that magnetic recording devices using flexible disks have recently been widely used to improve office efficiency due to their ease of use. Research aimed at this purpose is underway.

本発明もこの目的を達成する一手段として成されたもの
である。   ゛ 現在一般に用いられている可撓性ディスク用磁気記録装
置の磁気ヘッド用磁性体としては抗磁力が約300エル
ステツドのものが用いられている。
The present invention has also been made as a means to achieve this objective. ``The magnetic material for the magnetic head of the magnetic recording device for flexible disks currently in general use has a coercive force of about 300 oersteds.

これに対し、高記録密度用の磁性体としては抗磁力が約
600エルステツドと云う大きなものが用いられている
On the other hand, magnetic materials with a large coercive force of about 600 oersteds are used as magnetic materials for high recording density.

このように抗磁力が大きいことは減磁に対する抵抗力か
強い事を意味する反面、記録及び消去の為の磁界の強さ
が大きいことが必要となシ%仁の為磁気ヘッドの残留磁
気も大きくなってしまうので、それによる不都合を生じ
ることになる。
Although a large coercive force means a strong resistance to demagnetization, it also reduces the residual magnetism of the magnetic head because it requires a large magnetic field strength for recording and erasing. Since it becomes larger, it causes inconvenience.

即ち、消去磁気ヘッドの残留磁気が大きいと、磁気媒体
に記録されたデータ上を消去磁気ヘッドが摺動すること
によシ、その減磁作用によって記録データの再生出力振
幅が減小せしめられることになるので、再生性能に影響
を及ぼすことになる。
That is, if the residual magnetism of the erasing magnetic head is large, the reproduction output amplitude of the recorded data will be reduced due to the demagnetizing effect of the erasing magnetic head as it slides over the data recorded on the magnetic medium. Therefore, the playback performance will be affected.

そこで1本発明は、磁気ヘッドの残留磁気が少い優れた
磁気記録装置を提供しようとするものである。
Therefore, one object of the present invention is to provide an excellent magnetic recording device in which the residual magnetism of the magnetic head is small.

即ち5本発明は磁気ヘッドの駆動コイルに駆動電流を流
している時に駆動コイルに蓄えられた磁気エネルギーを
利用し、消勢完了後、新たに付加した自己消磁回路によ
って生じる時間と共に減衰する交流電流を駆動コイルに
流して磁気ヘッドの消磁を行なって記録媒体に対する磁
気ヘッドの減磁作用を改善するようにしたものである。
In other words, the present invention utilizes the magnetic energy stored in the drive coil when the drive current is flowing through the drive coil of the magnetic head, and after the deenergization is completed, the alternating current that decays over time is generated by the newly added self-demagnetization circuit. is applied to the drive coil to demagnetize the magnetic head, thereby improving the demagnetizing effect of the magnetic head on the recording medium.

第1図は本発明の原理説明因で、横軸は磁界の強さの強
さH1縦軸は磁束密度Bを示している。
FIG. 1 is an explanation of the principle of the present invention, in which the horizontal axis shows the strength of the magnetic field H1, and the vertical axis shows the magnetic flux density B.

従来の磁気記録装置では、駆動コイルに流す直流電流を
切ると、駆動中11点にあった磁気ヘッドの磁束密度は
矢印方向に減磁し、残留磁束密度はBlとなるが、それ
以下には減小しないのでこれが問題を起すのである。
In a conventional magnetic recording device, when the direct current flowing through the drive coil is cut off, the magnetic flux density of the magnetic head at 11 points during drive is demagnetized in the direction of the arrow, and the residual magnetic flux density becomes Bl, but below that This causes a problem because it does not decrease.

本発明は、駆動電流rBを切った後、第2図に示すよう
に自己減衰する交流消磁電流を流すことにより、磁束密
度が0に収斂するようにしたものである。
In the present invention, after the drive current rB is cut off, a self-attenuating AC demagnetizing current is caused to flow as shown in FIG. 2, so that the magnetic flux density converges to zero.

ここで第1図と第2図を対応させると、第1図に示すB
−H1ill@!上の21点は、第2図におけ゛る消去
電流INに対応し、22点は■2に対応する。
If we compare Figures 1 and 2, we can see that B shown in Figure 1 is
-H1ill@! The 21 points above correspond to the erase current IN in FIG. 2, and the 22 points correspond to 2.

駆動コイルに流す電流が第2図に示すように変化すると
、B−H特性は第1図に示したB−H曲線上をP1→P
2→Ps・・・と変化し、残留磁束密度がB1→B2→
Bs→・・・と小さくなる。
When the current flowing through the drive coil changes as shown in Figure 2, the B-H characteristic changes from P1 to P on the B-H curve shown in Figure 1.
2 → Ps... and the residual magnetic flux density changes from B1 → B2 →
It becomes smaller as Bs→...

本発明はこのような働きをするLO共振回路から成る自
己消磁回路を磁気ヘッド駆動回路に設けたものである。
The present invention provides a magnetic head drive circuit with a self-demagnetizing circuit composed of an LO resonance circuit that functions as described above.

以下消去磁気ヘッドに木兄BAを適用した場合の実施例
について説明すれば次の通シである。
The following is a description of an embodiment in which the Kinei BA is applied to an erasing magnetic head.

第3図は本発明の実施例を示すもので1は消去磁気ヘッ
ド、2は消去電流コントロール用スイッチSWと消去磁
気ヘッド1の間に設けたLOR共振回路、Eは直流定電
流源b LBは消去コイル、r鱒消去コイルLllの内
部抵抗である。
FIG. 3 shows an embodiment of the present invention, in which 1 is an erase magnetic head, 2 is an LOR resonant circuit provided between the erase current control switch SW and the erase magnetic head 1, E is a DC constant current source b, and LB is a This is the internal resistance of the erasing coil, r-trout erasing coil Lll.

ここで消去電流をiB、固有角周波数をωn、角度をφ
とし、消去コイルLBのインダクタンスをIF3〔H3
、消去コイルの内部抵抗rHの抵抗値’fc rncΩ
〕。
Here, the erase current is iB, the natural angular frequency is ωn, and the angle is φ
and the inductance of the erasing coil LB is IF3 [H3
, the resistance value of the internal resistance rH of the erasing coil 'fc rncΩ
].

(但しγB#0)h消去コイルに直列に接続されたコイ
ルLのインダクタンスをL[HJ &電源に対し並列に
接続したコンデンサCと抵抗凡の値を夫々0FF) %
几〔Ω〕とすると、スイッチSWが閉じている時。
(However, γB #0) h The inductance of the coil L connected in series to the erase coil is L [HJ & the values of the capacitor C and the resistor connected in parallel to the power supply are each 0FF) %
When it is 几〔Ω〕, when the switch SW is closed.

即ち、消去磁気ヘッド1が働いている時の消去電流1B
は直流定電流源Eの電流に等しい。
That is, when the erasing magnetic head 1 is working, the erasing current is 1B.
is equal to the current of the DC constant current source E.

この状態でスイッチSWを第2図におけるt=0点で開
いた時の消去電流3F+(t )は、下記(1)式で表
・・・(1) φ−t a n−”凸:で         ・・・(
旬ζ である。
In this state, the erase current 3F+(t) when the switch SW is opened at the t=0 point in Fig. 2 is expressed by the following equation (1)... (1) φ-t a n-" convex: ...(
It is season ζ.

上式においてζく1となる様に几、0.Lを選ぶと、(
1式は第2図に示すような減殺振動となる。
In the above formula, set 几, 0. so that ζ becomes 1. If you choose L, (
Type 1 produces attenuated vibration as shown in Figure 2.

従って、この様に振動しながら減衰する交流電流を消去
コイルLHに流せばその交流消磁作用により残留磁束密
度を小さくすることができる。
Therefore, by flowing an alternating current that oscillates and attenuates in this way through the erasing coil LH, the residual magnetic flux density can be reduced by the alternating current demagnetizing effect.

なお、第3図の実施例において、抵抗几は省略する場合
もある。
In the embodiment shown in FIG. 3, the resistor may be omitted in some cases.

第4図は異なる実施例を示すもので、第3図に示すもの
が、コンデンサと抵抗几を直流定電流源Eに対して去列
に接続したものに対し、直列に接続した場合T、L、O
,几の値を適当に選ぶことによシ、同様の働きをさせる
ことができる。
FIG. 4 shows a different embodiment. In contrast to the one shown in FIG. 3 in which a capacitor and a resistor are connected in series with respect to a DC constant current source E, when they are connected in series, T, L , O
A similar function can be achieved by appropriately selecting the values of , and .

以上ここでは可続性ディスク使用の磁気記録装置の消去
磁気ヘッドに適用した場合の実施例について説明したが
、一般の磁気記録装置の消去磁気ヘッドに対しても適用
が可能である。
Although an embodiment has been described above in which the present invention is applied to an erasing magnetic head of a magnetic recording device using a continuous disk, the present invention can also be applied to an erasing magnetic head of a general magnetic recording device.

一般の消去磁気ヘッドへの適用に関しての注意点は消去
終了後の減衰振動喧流にょシ媒体に記録が残る。仁れは
本発明の適用を制限するものではない。
A point to note regarding application to a general erasing magnetic head is that the recording remains on the medium due to the damped vibration turbulence after erasing. The grain does not limit the application of the present invention.

またここでは消去磁気ヘッドに直流電流を流した時の説
明をしたが1本発明の原理は消去コイルに蓄えられた磁
気エネルギを消磁に利用するものであることから解る様
に、消去電流をオフした時の消去電流にのみ関係する為
、交流電流を流す消去磁気ヘッドにも適用可能である。
Also, here we have explained the case where a direct current is passed through the erasing magnetic head, but the principle of the present invention is to use the magnetic energy stored in the erasing coil for demagnetization, so the erasing current is turned off. Since it is related only to the erasing current when the current is applied, it can also be applied to erasing magnetic heads that flow alternating current.

また、データの書き込み用ヘッドにも適用可能である。It is also applicable to a data writing head.

なお消去コイルに直列に接続したインダクタンスLは1
本質的なものではなく消去ヘッドのインダクタンスの値
によって不要となる場合がある。
Note that the inductance L connected in series with the erasing coil is 1
This is not essential and may be unnecessary depending on the inductance value of the erase head.

従って、本発明はここに例示したもののみに限定される
ものでないことを諒承すべきである。
Therefore, it should be understood that the present invention is not limited to only those exemplified herein.

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

第1図は本発明の詳細な説明するためのB−H曲線図、
第2図は本発明における消去電流特性囚。 第3図及び第4図は夫々本発明の実施例の電気回路図で
ちる。
FIG. 1 is a B-H curve diagram for detailed explanation of the present invention;
Figure 2 shows the erase current characteristics in the present invention. 3 and 4 are electrical circuit diagrams of embodiments of the present invention, respectively.

Claims (1)

【特許請求の範囲】[Claims] (1)  消去用磁気ヘッド駆動回路にLO共振回路か
ら成る自己消磁回路を設けたことを%徴とする磁気記録
装置。 ■) 書込用磁気ヘッド駆動回路に共振周波数〃;曹き
込み信号と共振を起さない周波数としたLO共振回路か
ら成る自己消磁回路を設けたことを特徴とする磁気記録
装置。
(1) A magnetic recording device characterized by providing a self-demagnetizing circuit consisting of an LO resonance circuit in the erasing magnetic head drive circuit. (2) A magnetic recording device characterized in that a write magnetic head drive circuit is provided with a self-demagnetizing circuit consisting of an LO resonant circuit having a resonant frequency that does not cause resonance with the fill-in signal.
JP8500883A 1983-05-17 1983-05-17 Magnetic recording device Pending JPS59213016A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8500883A JPS59213016A (en) 1983-05-17 1983-05-17 Magnetic recording device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8500883A JPS59213016A (en) 1983-05-17 1983-05-17 Magnetic recording device

Publications (1)

Publication Number Publication Date
JPS59213016A true JPS59213016A (en) 1984-12-01

Family

ID=13846712

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8500883A Pending JPS59213016A (en) 1983-05-17 1983-05-17 Magnetic recording device

Country Status (1)

Country Link
JP (1) JPS59213016A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5038230A (en) * 1988-08-30 1991-08-06 Kabushiki Kaisha Toshiba Method of accurately executing read access and magnetic recording/reproducing apparatus therefor
CN100377213C (en) * 2004-12-28 2008-03-26 株式会社东芝 Head amplifier circuit with function for degaussing residual magnetism of recording head
JP2008543230A (en) * 2005-06-03 2008-11-27 センサーマティック・エレクトロニクス・コーポレーション Deactivation technology for electronic article surveillance labels using energy recovery
JP2015161327A (en) * 2014-02-26 2015-09-07 不二ラテックス株式会社 Control method and control device for electromagnetic clutch

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5351724A (en) * 1976-10-21 1978-05-11 Toshiba Corp Demagnetizing device for magnetic head
JPS566033B2 (en) * 1973-07-25 1981-02-09

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS566033B2 (en) * 1973-07-25 1981-02-09
JPS5351724A (en) * 1976-10-21 1978-05-11 Toshiba Corp Demagnetizing device for magnetic head

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5038230A (en) * 1988-08-30 1991-08-06 Kabushiki Kaisha Toshiba Method of accurately executing read access and magnetic recording/reproducing apparatus therefor
CN100377213C (en) * 2004-12-28 2008-03-26 株式会社东芝 Head amplifier circuit with function for degaussing residual magnetism of recording head
US7460324B2 (en) 2004-12-28 2008-12-02 Kabushiki Kaisha Toshiba Head amplifier circuit with function for degaussing residual magnetism of recording head
JP2008543230A (en) * 2005-06-03 2008-11-27 センサーマティック・エレクトロニクス・コーポレーション Deactivation technology for electronic article surveillance labels using energy recovery
JP2015161327A (en) * 2014-02-26 2015-09-07 不二ラテックス株式会社 Control method and control device for electromagnetic clutch

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