JPS59124015A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPS59124015A
JPS59124015A JP22959382A JP22959382A JPS59124015A JP S59124015 A JPS59124015 A JP S59124015A JP 22959382 A JP22959382 A JP 22959382A JP 22959382 A JP22959382 A JP 22959382A JP S59124015 A JPS59124015 A JP S59124015A
Authority
JP
Japan
Prior art keywords
core
magnetic
erasing
erase
gap
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
JP22959382A
Other languages
Japanese (ja)
Inventor
Tsutomu Imai
勉 今井
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.)
Seiko Epson Corp
Suwa Seikosha KK
Original Assignee
Seiko Epson Corp
Suwa Seikosha 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 Seiko Epson Corp, Suwa Seikosha KK filed Critical Seiko Epson Corp
Priority to JP22959382A priority Critical patent/JPS59124015A/en
Publication of JPS59124015A publication Critical patent/JPS59124015A/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
    • G11B5/127Structure or manufacture of heads, e.g. inductive

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Magnetic Heads (AREA)

Abstract

PURPOSE:To improve the coercive force of a magnetic head by providing a shield core adjacently to an erasing core. CONSTITUTION:The shield core 4 is provided adjacently to the erasing core 1. When an external magnetic field is applied, the major part of it flows into the shield core 6 and magnetic flux flowing in the erasing core 1 is reduced greatly. The magnetic flux flowing in the shield core 6 flows directly to the erasing core 2 from a back core 3 partially, and the remainder flows to the erasing core 2 through the shield gap 7, erasing core 1, and an erasing gap 4. The magnetic path of the latter, however, has magnetic resistance far larger than that of the latter and the majority of the magnetic flux flowing in the core 6 flows through the erasing core 2. Consequently, the magnetic flux flowing through the gap 4 is reduced and a magnetic field established at the circumference is also reduced. Thus, the coercive force of the magnetic head is improved.

Description

【発明の詳細な説明】 本発明は、磁気ヘッドの磁気じゃへいに関するものでる
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic jacket for a magnetic head.

従来の磁気ヘッドの構造の例を第1図に示す。An example of the structure of a conventional magnetic head is shown in FIG.

1.2は消去コア、3はバックコア、4は消去ギャップ
、5は記録再生コア、6は消去コイルである。現任磁−
A記憶装置は小型化される傾向にあり、そのために装置
内外の磁界発生源が磁気ヘッドに近接し、an気ヘッド
に外部の磁界が加わり易くなっている。
1.2 is an erase core, 3 is a back core, 4 is an erase gap, 5 is a recording/reproducing core, and 6 is an erase coil. Current position
As storage devices tend to be smaller, magnetic field sources inside and outside the device are brought closer to the magnetic head, making it easier for external magnetic fields to be applied to the magnetic head.

バックコア3′(Il″持たない)[有]気ヘッドに、
第1図に示す矢印の方°回の磁界が加わると、磁束はコ
ア1に流入した鏝、消去ギヤラグ4會通過し、コア2に
流入する。消去コア1.2に比べて、消去ギャップ4は
断面積が小さいため、この部分に磁束が集中し、消去ギ
ャップ4周辺に諸うB界ffxA生する。
Back core 3' (does not have Il'') [has] Qi head,
When a magnetic field is applied in the direction of the arrow shown in FIG. Since the erase gap 4 has a smaller cross-sectional area than the erase core 1.2, magnetic flux concentrates in this portion, and a B field ffxA is generated around the erase gap 4.

このような状態で、磁気ヘッド?記録媒体にφ融させた
11移動すると、消去ギャップ4周辺の高磁界により、
記録媒体が磁1ヒされ、すてに書き込1れた清報を壊し
てしま9ことになる。また消去コイル6に電流を流し、
消去I′11′勤全行9際には、磁路の一部が非磁性体
となるため、所定の消去団界を得るための電流値が大き
くなる。
Magnetic head in this condition? When the recording medium is moved by φ11, due to the high magnetic field around the erase gap 4,
The recording medium was magnetically damaged and the information written on it was destroyed. Also, a current is passed through the erasing coil 6,
During erasing I'11', part of the magnetic path becomes non-magnetic, so the current value for obtaining a predetermined erasing field becomes large.

次にバックコア52ft:待つ磁気ヘッドでは、前列と
同様な磁界が加わると、消去コア1 [流入した磁束は
、バックコア6と消去ギャップ4に分が九で流れるため
、消去ギャップ4を通過する磁束は、バンクコアがない
場合に比べると少なくなるが、バンクコア5及びバック
コア3と消去コア1.2の接置部分の磁気抵抗が消去ギ
キップ4の磁気抵抗に比べて十分小姑くはならないため
、消去ギャップ4周辺に鍋磁界が発生し、同様に、記録
され大情報を壊してし1ワ。
Next, back core 52ft: In the waiting magnetic head, when the same magnetic field as in the front row is applied, erase core 1 [The inflowing magnetic flux flows through back core 6 and erase gap 4 at a rate of 9, so it passes through erase gap 4. Although the magnetic flux is smaller than when there is no bank core, the magnetic resistance of the part where the bank core 5 and back core 3 are in contact with the erase core 1.2 is not sufficiently smaller than the magnetic resistance of the erase core 4. A pot magnetic field is generated around the erase gap 4, and similarly destroys a large amount of recorded information.

本発明は、こうした問題点を解決するために。The present invention aims to solve these problems.

消去コアて隣接し:化しゃへいコアを設けたものでその
目的は、′dB気ヘッドの耐磁性全向上することにある
A shielding core is provided adjacent to the erase core, and its purpose is to completely improve the magnetic resistance of the head by 100 dB.

以下、図面f(よって詳訓に説明する。Below, drawing f (therefore, detailed explanation will be given).

第2図に、本発明の実施例である。1,2Vよ消55j
7.3はバックコア、4は消去(ヤツフ、5は記録再生
コア、6はしやへいコア、7はしやへいギーヤツプ、8
は消去コイルである。
FIG. 2 shows an embodiment of the present invention. 1,2V 55j
7.3 is the back core, 4 is the eraser, 5 is the recording/reproducing core, 6 is the fast core, 7 is the fast gear, 8
is the cancellation coil.

第2図において、図中矢印の方向ニジ外部磁界が加わる
と、しやへいコア6周辺の磁束は、しや・\いコア6〕
5二ない場合には、消去コア1に流入するが、−シやへ
いコア6がある場合には、しやへいコアAVc大述分が
流入し、消去コア1に流入する磁束はかfXシ減少する
。しやへいコア6に流入した磁束は、バンクコア3から
、直接消去コア2へ流れるものと、しやへいギャップノ
、消去コア1゜消去ギャップ4を通っで消去コア2へ流
れるものとの2つに分かすする。しかし、後者の経路に
はしやへいギャップ7と消去ギャップ402つの非磁性
体が磁路となっているため、前者の磁路に比べて磁気抵
抗が十分商くなシ、しやへいコア6にηε人しfe (
1411束の大部分はバックコア3全介して消去コア2
へ流れる。したがって、(肖去ギャップ4ケ通過する磁
束は減少し、消去ギャップ4周辺に発生する磁界も減少
する。この結果%磁気ヘッドが移動しても、すでに書き
込1れた情報全壊す危険性が少なくなり、磁気ヘッドの
耐磁性が噌す。
In FIG. 2, when an external magnetic field is applied in the direction of the arrow in the figure, the magnetic flux around the thin core 6 changes to the thin core 6.
If there is no 52, the magnetic flux flows into the erase core 1, but if there is a -shi or hei core 6, the magnetic flux from the hei core AVc flows in, and the magnetic flux flowing into the erasure core 1 becomes the fX series. Decrease. The magnetic flux that has flowed into the blank core 6 is divided into two parts: one that flows directly from the bank core 3 to the erase core 2, and the other that flows through the blank gap, the erase core 1° and the erase gap 4 to the erase core 2. I'll share it. However, since the latter path includes two non-magnetic materials, the magnetic gap 7 and the erase gap 40, the magnetic resistance is not sufficiently reduced compared to the former magnetic path. ηε人しfe (
Most of the 1411 bundles are sent to erased core 2 via all back cores 3.
flows to Therefore, the magnetic flux passing through the erase gap 4 decreases, and the magnetic field generated around the erase gap 4 also decreases.As a result, even if the magnetic head moves, there is no risk of destroying all the information that has already been written. This decreases the magnetic head's magnetic resistance.

次に、消去コイルに電かCを流し、消去動作を行う場合
には、磁路としては、消去コア1から、しやへいギャッ
プ7、バックコア3、消去コア2を経て、消去ギャップ
4から消去コアへ戻る経路と、消去コア1から、しやへ
いギャップ7、バックコア 5 、 L’?”イコ“ア
ロ全経て、しやへいコア6と消去コア10間の空間全通
って消去コア1へ戻る経路がめるが、後者の経路ではし
やへいコア6と消去コア1の空間が非磁性体であり、両
者の間隔も、消去ギャップ4の間隔よりも十分大きくと
っであるため、前者のaFMK比較して、磁気抵抗が十
分大きくなり、磁束の大部分は前者の経w1を通過する
。したがって、消去動作においてハ、シやへいコア6は
ほとんど影響なく、従来と1eI3様の動作を行うこと
ができる。さらに、〕(ツクコア5゜しやへいコア6の
ないものと比べると、磁路の磁気抵抗がかなり低くなる
ので、消去′亀流力濫少なくなる。
Next, when an electric current is applied to the erase coil to perform an erase operation, the magnetic path starts from erase core 1, passes through Shiyahei gap 7, back core 3, erase core 2, and then from erase gap 4. The path back to the erased core, from erased core 1 to Shiyahei gap 7, back core 5, L'? After going through the "Ico" arrow, a path is created that passes through the entire space between the shy core 6 and the erase core 10 and returns to the erase core 1, but in the latter route, the space between the strong core 6 and the erase core 1 is made of non-magnetic material. Since the distance between the two is also sufficiently larger than the distance between the erase gaps 4, the magnetic resistance is sufficiently large compared to the former aFMK, and most of the magnetic flux passes through the former's warp w1. Therefore, in the erasing operation, the C, H, and H cores 6 are hardly affected, and can perform operations similar to the conventional 1eI3 type. Furthermore, since the magnetic resistance of the magnetic path is considerably lower than that of the case where the core is 5° and there is no core 6, the erase current force is reduced.

以上のように、消去コア1に隣接して、しやへいコア4
を設けることにより、消去の動作に影響を与えることな
く、外部から流入する磁界による消去ギャップ5周辺の
磁界を小さくすること力玉でき、磁気ヘッドの耐磁性全
高めることができる。
As described above, adjacent to the erased core 1, the quiet core 4
By providing this, it is possible to reduce the magnetic field around the erase gap 5 due to the magnetic field flowing in from the outside without affecting the erase operation, and the magnetic resistance of the magnetic head can be completely improved.

また、消去電流も少なくなる。したがって%磁気記憶装
置の磁気ヘッド周辺の磁気的な設ば1を容易にする。
Furthermore, the erase current also decreases. Therefore, the magnetic arrangement around the magnetic head of the magnetic storage device is facilitated.

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

第1図は、従来の磁気ヘッドの一実施例の図1であり、
第2図は、本発明による磁気へ〕ノドの一実施例て゛お
る。 1.2・・・・・C肖去コア 5・・・・・・バックコア 4・・・・・・ζ肖去ギャツフ” 5・・・・・・記録再生コア 6・・・・・・シャへいコア 7・・・・・・L−?へいギャップ 8・・・・・・消去コイル ツ上 出願人 抹式会仕 諏訪絹工舎 代理人 弁琥士最上  楊 第1図 第2図
FIG. 1 shows an example of a conventional magnetic head.
FIG. 2 shows an embodiment of the magnetic throat according to the present invention. 1.2・・・・・・C death core 5・・・・・・Back core 4・・・・・・ζDepression Gatsfu” 5・・・・・・Recording/playback core 6・・・・・・Shahei Core 7...L-?Hei Gap 8...Erase Koilz Upper Applicant Mashishiki Kaishi Suwa Silk Industry Agent Benkoji Mogami Yang Figure 1 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 消去コアに隣接したしや′\いコアを持つこと全特徴と
した飾気ヘッド。
An elegant head characterized by having a thin core adjacent to an erased core.
JP22959382A 1982-12-29 1982-12-29 Magnetic head Pending JPS59124015A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22959382A JPS59124015A (en) 1982-12-29 1982-12-29 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22959382A JPS59124015A (en) 1982-12-29 1982-12-29 Magnetic head

Publications (1)

Publication Number Publication Date
JPS59124015A true JPS59124015A (en) 1984-07-18

Family

ID=16894610

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22959382A Pending JPS59124015A (en) 1982-12-29 1982-12-29 Magnetic head

Country Status (1)

Country Link
JP (1) JPS59124015A (en)

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