JPS6089806A - Magnetic erasure head - Google Patents
Magnetic erasure headInfo
- Publication number
- JPS6089806A JPS6089806A JP19893383A JP19893383A JPS6089806A JP S6089806 A JPS6089806 A JP S6089806A JP 19893383 A JP19893383 A JP 19893383A JP 19893383 A JP19893383 A JP 19893383A JP S6089806 A JPS6089806 A JP S6089806A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- thin film
- erasing
- magnetic material
- tape
- 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
Links
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/02—Recording, reproducing, or erasing methods; Read, write or erase circuits therefor
- G11B5/024—Erasing
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/187—Structure or manufacture of the surface of the head in physical contact with, or immediately adjacent to the recording medium; Pole pieces; Gap features
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Magnetic Heads (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、磁気記録媒体に磁気記録さnた信号全交流消
去する磁気消去ヘッドに関し、特に消去効率の向上を図
った磁気消去ヘッドに関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magnetic erasing head for erasing all AC signals magnetically recorded on a magnetic recording medium, and particularly to a magnetic erasing head with improved erasing efficiency.
従来、たとえばビデオテープレコーダ(以下■TRとい
う)用の消去ヘッドとして用いら九でいる回転型磁気消
去ヘッドは、゛フライングイレーズへクドと称さ几、磁
気記録媒体である磁気テープに磁気記録さ几た信号を記
録トランク毎に交流消去している。このような磁気消去
ヘッドは、一般的に、第1図Aに示す工9に、非磁性拐
料のギャップスペーサ1を介して、金属酸化物磁性材料
であるフェライトコア素片2,3が接合さ九ることで形
成さ九ている。スパクタ等の手段にxD配されるこのギ
ャップスペーサ1は、消去ヘッドのギャップ間隔tを与
えるものである。また、消去ヘッドには、トラノキンダ
動作全行なう消去ヘッドに対する矢印Xの磁気テープ相
対移動方向の逃げ側に、巻線穴4が形成さnている。こ
の巻線穴ヰに巻線さ九るコイルには、たとえば5MHz
程度の消去周波数の信号が供給さ九る。そして、ギヤン
グ部に飽和磁界が発生し、磁気テープの相対移動に伴い
、磁気テープに加わる磁界が飽和磁界よシ徐々に小さく
なってゆくことにより、磁気テープ上の残留磁化がゼロ
に収斂さ九、磁気テープに磁気記録さ几た信号の交流消
去が行なわ九る。ところで、コア素片2,3として用い
ら九でいる金属酸化物磁性材料のフェライトは、電気抵
抗は太きいが、飽和磁束密度Bsが5000ガウス程度
であり、ギヤング部よシ発生し得る磁界強度が、メタル
テープ等の高い抗磁力He’(5有する磁気テープに記
録さ几ている信号を消去するには不充分である。Conventionally, the rotary magnetic erase head, which has been used as an erase head for video tape recorders (hereinafter referred to as TR), is called a "flying erase head" and is used to record magnetically on magnetic tape, which is a magnetic recording medium. The filtered signals are erased for each recording trunk. In general, such a magnetic erasing head has ferrite core pieces 2 and 3 made of a metal oxide magnetic material joined to a workpiece 9 shown in FIG. 1A through a gap spacer 1 made of a non-magnetic material. It is formed by s9. This gap spacer 1, which is disposed xD on a means such as a spactor, provides a gap distance t of the erase head. Further, the erasing head has a winding hole 4 formed on the escape side in the direction of relative movement of the magnetic tape as indicated by the arrow X with respect to the erasing head that performs all of the tranokinder operations. For example, the coil that is wound in this winding hole is 5MHz.
A signal with a cancellation frequency of about 9 is supplied. Then, a saturation magnetic field is generated in the gearing part, and as the magnetic tape moves relative to each other, the magnetic field applied to the magnetic tape gradually becomes smaller than the saturation magnetic field, so that the residual magnetization on the magnetic tape converges to zero. , alternating current erasure of signals magnetically recorded on magnetic tape is performed. By the way, the metal oxide magnetic material ferrite used as the core pieces 2 and 3 has a high electrical resistance, but the saturation magnetic flux density Bs is about 5000 Gauss, and the magnetic field strength that can be generated in the young part is low. However, it is insufficient to erase signals recorded on a magnetic tape having a high coercive force He' (5) such as a metal tape.
第1図Bは、第1図Aの磁気消去ヘッドのギヤツブ部周
辺での磁界強度分布を、テープ相対移動方向距離ケ横軸
に取シ示したものである。FIG. 1B shows the magnetic field strength distribution around the gear part of the magnetic erasing head of FIG. 1A, plotted on the horizontal axis of distance in the tape relative movement direction.
ところで、磁気テープに記録される信号の高密度化が要
求されてくるに従い、残留磁束密度Brの高いメタルテ
ープ等の磁気テープが使用されるLうになハそ12とと
も咳消去効率の高い磁気消去ヘッドが必要となってきて
いる。そこで、磁気消去ヘッドを構成する一対のコア素
片に飽和磁束密度B8の高い材料であるセンダスト等ケ
用いて、ギャップ部より発生する磁界強度を高めること
も考えら九る。このセンダストは飽和磁束密度Bs75
Z9000ガウス程度と高い。しかし、センダストは電
気抵抗が小さいことにXシ、コア素片に士ンダストヶ用
いたとしても渦電流損が太き(発熱が多いため、消去効
率が上がらないという問題点がある。By the way, as there is a demand for higher density signals recorded on magnetic tapes, magnetic tapes such as metal tapes with high residual magnetic flux density Br are used, as well as magnetic tapes with high cough eradication efficiency. Eraser heads are becoming necessary. Therefore, it is conceivable to use sendust or the like, which is a material with a high saturation magnetic flux density B8, for the pair of core pieces constituting the magnetic erasing head to increase the strength of the magnetic field generated from the gap portion. This Sendust has a saturation magnetic flux density of Bs75
It is high, about Z9000 Gauss. However, Sendust has a low electrical resistance, and even if Sendust is used in the core piece, there is a problem in that the eddy current loss is large (it generates a lot of heat, so the erasing efficiency cannot be improved).
このように、たとえばVTRの回転型消去ヘッドとして
用いらnる従来の磁気消去ヘッドは、高い抗磁力Hcを
有するメタルテープ等の磁気テープに記録さ九ている信
号音消去するには消去効率が不充分であるという問題点
があった。In this way, conventional magnetic erasing heads used, for example, as rotary erasing heads for VTRs, have insufficient erasing efficiency to erase signal sounds recorded on magnetic tapes such as metal tapes having high coercive force Hc. The problem was that it was insufficient.
そこで、本発明はこのような実情に鑑み提案さ′t′し
たものであシ、高い抗磁力Heを有する磁気記録媒体で
あるたとえばメタルテープ等の磁気テープに磁気記録さ
nfC信号を消去するのに適した高い消去効率を持つ磁
気消去ヘッドを提供することを目的とする。The present invention was proposed in view of the above circumstances, and is a method for erasing nfC signals magnetically recorded on a magnetic recording medium having a high coercive force He, such as a magnetic tape such as a metal tape. The purpose of the present invention is to provide a magnetic erasing head with high erasing efficiency suitable for
この目的を達成するために本発明の磁気消去ヘッドは、
軟磁性材料、!、シ成る一対のコア素片の磁気ギャップ
形成面側に、上記軟磁性材料よシ高い飽和磁束密度を有
する軟磁性材料薄膜をそれぞ几形成し、この一対のコア
素片を非磁性材料のギャップスペーサを介して接合する
磁気消去ヘッドにおいて、磁気記録媒体進入側のコア素
片に形成された上記磁性材料薄膜の膜厚は磁気記録媒体
逃げ側のコア素片に形成さT′した上記磁性材料薄膜の
膜厚ニジ厚いことを特徴とする。To achieve this objective, the magnetic erase head of the present invention comprises:
Soft magnetic material! A thin film of a soft magnetic material having a higher saturation magnetic flux density than the above-mentioned soft magnetic material is formed on the magnetic gap forming surface side of a pair of core pieces consisting of In the magnetic erasing head that is joined via a gap spacer, the thickness of the magnetic material thin film formed on the core piece on the side where the magnetic recording medium enters is the same as the thickness of the magnetic material thin film formed on the core piece on the side where the magnetic recording medium escapes. It is characterized by a thicker material thin film.
まず、本発明の一実施例の説明に先立ち本発明の前提と
なる技術の説明を行なう。First, prior to explaining one embodiment of the present invention, the technology on which the present invention is based will be explained.
第2図Aばこの技術によって構成さ几る磁気消去ヘッド
を示している。この磁気消去ヘッドは、フェライトコア
素片2,3で形成される消去ヘッドに対して、ギャップ
スペーサ1の両9111部分にのみ、センダスト等の高
飽和磁束密度あるいは高透磁率?有する互いに等しい膜
厚aの磁性膜を接着あるいはスバクタ等にニジ配してい
る。FIG. 2A shows a magnetic erase head constructed according to tobacco technology. In this magnetic erase head, unlike the erase head formed of the ferrite core pieces 2 and 3, only the both 9111 portions of the gap spacer 1 are made of high saturation magnetic flux density or high magnetic permeability such as sendust. Magnetic films having the same thickness a are bonded or arranged on a substrate or the like.
第2図Aに示す構成とすることで、第2図Bにその特性
を示すようにキャンプ部よシは充分な磁界強度を得るこ
とができる。しかし、第2図Bに示すようにこの消去へ
ンドは、磁界強度の分布が域)が急峻であることによシ
、消去ヘッドのコイルに供給さ九る消去周波数の信号が
磁気テープに記録さfしたり、磁気テープ上に磁気記録
さ九ている消去さ几るべき信号がこの消去周波数成分全
バイアスとして再記録さnてしまうという欠点上布して
いる。By adopting the configuration shown in FIG. 2A, the camping portion can obtain sufficient magnetic field strength, as shown in FIG. 2B. However, as shown in Figure 2B, this erase head has a steep distribution of magnetic field strength, so that the signal at the erase frequency supplied to the coil of the erase head is recorded on the magnetic tape. The disadvantage is that the signal to be erased, which is magnetically recorded on the magnetic tape, is re-recorded as the entire bias of the erased frequency component.
つぎに、上述の技術の問題点を解決する本発明の一実施
例を図面に基づき説明する。Next, an embodiment of the present invention that solves the above-mentioned technical problems will be described based on the drawings.
第3図は、本発明に係る磁気消去ヘッドの外観斜視図ケ
示し、また第4図は、その要部斜視図ケ示している。こ
の磁気消去へクドは、たとえばVTR用の回転型消去ヘ
ッドとして用いら九、磁気記録媒体であるたとえば磁気
テープに磁気記録された信号を記録トラクク毎に、たと
えば5 M Hzの消去周波数の信号によシ交流消去し
ている。ところで、上記磁気消去ヘッドは、一対のコア
素片10.11が軟磁性材料であるたとえばマンガンジ
ンクフェライト(Mn=Znフェライト)で構成さ九、
またトラッキング動作全行なう消去ヘッドに対する矢印
Xの磁気テープ相対移動方向の逃げ側のコア素片11に
は巻線穴12が形成されている。この巻線穴12には、
消去用の信号が供給さ九るコイルが巻線さnる。FIG. 3 shows a perspective view of the external appearance of the magnetic erasing head according to the present invention, and FIG. 4 shows a perspective view of the main parts thereof. This magnetic erasing head is used, for example, as a rotary erasing head for a VTR, and records signals magnetically recorded on a magnetic recording medium, such as a magnetic tape, for each recording track, at an erasing frequency of, for example, 5 MHz. I am erasing the current. By the way, in the magnetic erase head, the pair of core pieces 10 and 11 are made of a soft magnetic material, for example, manganese zinc ferrite (Mn=Zn ferrite).
Further, a winding hole 12 is formed in the core piece 11 on the escape side in the direction of relative movement of the magnetic tape as indicated by the arrow X with respect to the erasing head that performs the entire tracking operation. In this winding hole 12,
A coil to which a signal for erasing is supplied is wound.
丑た、一対のコア素片10,11の磁気ギヤツブ形成面
111jには、コア素片10.llk構成するたとえば
Mn−Znフェライトよシも高い飽和磁束密度Bsある
いは高い透磁率を有する軟磁性材料のたとえばいわゆる
センダストエフなる磁性材料薄膜13.14がスパッタ
等の手段上用いて形成さnている。磁気テープ相対移動
方向の進入側のコア素片10側に形成さ九る上記薄膜1
3の膜厚eは、磁気テープ相対移動方向の逃げ側のコア
素片11側に形成さnる上記薄膜14の膜厚fニジも厚
くすなわちe>fに形成さ几ている。この実施例では、
膜厚eをたとえば3μmに、膜厚fをたとえが1μmと
している。ところで、磁性材料薄膜13.14が形成さ
れた上記コア素片10゜11は、非磁性材料のたとえば
二酸化シリコンSiO2のスパッタ膜ニジなるギャップ
スペーサ15ケ介して、非磁性材料のガラス16ケ用い
融着接合さ九る。このギャップスペーサ15 ij:、
磁気ギャップのギャップ間隔t’(r与えるものであり
、このギヤング部より消去磁界が発生する。Moreover, on the magnetic gear forming surface 111j of the pair of core pieces 10 and 11, there is a core piece 10. A magnetic thin film 13.14 of a soft magnetic material having a high saturation magnetic flux density Bs or high magnetic permeability, such as Mn-Zn ferrite, for example, so-called SendustF, is formed using a method such as sputtering. . The thin film 1 formed on the core piece 10 side on the entry side in the direction of relative movement of the magnetic tape.
The film thickness e of No. 3 is such that the film thickness f of the thin film 14 formed on the core piece 11 side on the escape side in the direction of relative movement of the magnetic tape is also thicker, that is, e>f. In this example,
For example, the film thickness e is 3 μm, and the film thickness f is 1 μm. By the way, the core pieces 10 and 11 on which the magnetic material thin films 13 and 14 are formed are fused using 16 pieces of glass made of non-magnetic material via 15 gap spacers made of sputtered films of non-magnetic material such as silicon dioxide SiO2. Attachment is completed. This gap spacer 15 ij:,
The gap distance t'(r) of the magnetic gap is given, and an erasing magnetic field is generated from this gigantic portion.
このように構成さf′した上記磁気消去ヘッドは、ギャ
ップ部よ多発生する消去磁界の磁界強度が高く、またこ
の磁界の強度分布が第5図Aに示さ几る↓9になシ、磁
気テープ相対移動方向距離についてのこの磁界強度分布
がギャップ形成位置に対して非対称となっている。すな
わち、磁気テープ相対移動方向の逃げ側方向での強度分
布(図中りで示す領域)が、緩やかな傾斜を描くような
分布となっている。この第5図Aは、縦軸に磁界強度を
、横軸にテープ相対移動方向距離を取っている。In the above magnetic erasing head having f' configured in this way, the magnetic field strength of the erasing magnetic field generated more often than the gap portion is high, and the intensity distribution of this magnetic field is shown in FIG. 5A. This magnetic field strength distribution with respect to the distance in the tape relative movement direction is asymmetrical with respect to the gap forming position. That is, the intensity distribution in the escape side direction of the relative movement direction of the magnetic tape (the region shown in the figure) has a gentle slope. In FIG. 5A, the vertical axis represents the magnetic field strength, and the horizontal axis represents the distance in the tape relative movement direction.
また、第5図Aと対応するような位置関係にある第5図
Bは、第4図のI−I線断面図である。ところで、磁界
強度が上記逃げ側において緩やかなスロープを描くよう
な分布となるのは、ギャップスペーサ15の両側に配さ
れる上記磁性材料薄膜13.14の内、上記逃げ側に配
さ几る薄膜14の膜厚fが進入側の薄膜13の膜厚eニ
ジも薄く形成さnていることによシ、高飽和磁束密度材
料のこの薄膜14が先に磁気飽和奮起こすことに起因し
ている。Further, FIG. 5B, which has a positional relationship corresponding to FIG. 5A, is a sectional view taken along the line II in FIG. 4. Incidentally, the reason why the magnetic field strength has a gentle slope distribution on the escape side is because of the magnetic material thin films 13 and 14 disposed on both sides of the gap spacer 15, the thin film disposed on the escape side is This is due to the fact that the film thickness f of the thin film 14 on the entry side is also thinner than the thin film 14 made of a high saturation magnetic flux density material, causing magnetic saturation to occur first. .
このように、本発明によれば、コア素片10゜110も
高飽和磁束密度iする磁性材料薄膜13.14’にギャ
ップスペーサ150両側に配し磁気ギャップ部よ多発生
する磁界強度?高くするとともに、磁気テープ相対移動
方向逃げ側に配さ九る薄膜14の膜厚を薄膜13に比べ
て薄く形成することによシ、磁界強度の分布を上記逃げ
側方向に緩や〃為なスロープを描くようにしている0こ
のため、メタルテープのような高い抗磁力■IC′(l
l−有する磁気テープに磁気記録さ:f’L fc 4
i号を消去するのに充分な磁界強度を得ることができる
とともに、↓シ逃げ側に延在する磁界強度分布によって
、消去周波数の信号が磁気テープに記録さ几るようなこ
とはなく、消去周波数成分をバイアスとして磁気テープ
上に磁気記録さnた消去さ几るべき信号が再記録さnる
ようなことはない。すなわち、緩やかな傾斜状の磁界強
度分布によって、磁気テープに加えられる磁界が、テー
プの相対移動に伴って飽和磁界xD徐々に小さくなって
ゆき、磁気テープ上の残留磁化が徐々にゼロに収斂さ几
るようになる。As described above, according to the present invention, the core pieces 10° 110 are also arranged on both sides of the gap spacer 150 in the magnetic material thin films 13 and 14' having a high saturation magnetic flux density i, so that the magnetic field strength generated at the magnetic gap portion is large. In addition, by forming the thin film 14 disposed on the relief side in the direction of relative movement of the magnetic tape to be thinner than the thin film 13, the distribution of magnetic field strength can be made gentler in the relief side direction. 0 For this reason, it has a high coercive force like metal tape ■IC' (l
l - magnetically recorded on a magnetic tape with: f'L fc 4
In addition to being able to obtain a magnetic field strength sufficient to erase the number i, the magnetic field strength distribution extending to the ↓ edge side prevents the signal at the erasing frequency from being recorded on the magnetic tape. A signal that was magnetically recorded on the magnetic tape using the frequency component as a bias will not be re-recorded to be erased. In other words, due to the gently sloped magnetic field strength distribution, the magnetic field applied to the magnetic tape gradually becomes smaller as the tape moves relative to the saturation magnetic field xD, and the residual magnetization on the magnetic tape gradually converges to zero. It starts to cool down.
ところで、コア素片10,11の磁性材料としてMn−
Zn フェライトの他に、ニッケルジンクフェライト(
Ni−Znフェライト)等を用いてもよい。また、磁性
材料薄膜13.14の高飽和磁束密度材料としては、鉄
−アルミニウム−シリコン系(Fe−AJ−8t系)の
上述のいわゆるセンダストの他に、M−Xで示さ几る非
晶質材料ケ用いてもよい。ここで、MはF e t−C
o (コバルト)、Niであシ、XはたとえばSi、B
(Itう素)P〔リン〕、C(カーボン)等であシ、具
体的には上記非晶質材料として、Fe−Co−8i−B
系の磁性材料が上げら几る〇
丑た、上記磁性材料薄膜13,14の膜厚は、上記進入
側に配さ汎る薄膜13t1μmから5μmとするのがよ
く、−上嗜゛4、。By the way, as the magnetic material of the core pieces 10 and 11, Mn-
In addition to Zn ferrite, nickel zinc ferrite (
Ni--Zn ferrite) or the like may also be used. In addition to the above-mentioned so-called sendust of the iron-aluminum-silicon system (Fe-AJ-8t system), examples of the high saturation magnetic flux density material for the magnetic material thin film 13.14 include the amorphous material shown by M-X. Materials may also be used. Here, M is Fet-C
o (cobalt), Ni, X is for example Si, B
(It boron) P [phosphorus], C (carbon), etc. Specifically, as the above amorphous material, Fe-Co-8i-B
Since the magnetic material of the system is increased, the thickness of the magnetic material thin films 13 and 14 is preferably set to 1 to 5 μm for the thin film 13 disposed on the entrance side.
一喝゛
上6己逃げ側に配さ几る薄膜14を薄膜13の一以下と
し、0゜1μm以上とするのがよい。こ九は、薄膜13
の膜厚が5μm以上であると、コア素片10.11であ
るフェライトと融着結合用のガラス16との熱膨張係数
の違いにょシ接合時に割れが生じたシ、膜の剥離が生じ
てしまうためであ勺、1μm以下であるとギャップ形成
部分に高飽和磁束密度材料を配する効果が失わnる。ま
た、薄膜14の膜厚全薄膜13の百以下とするのは、上
述の磁界強度分布に非対称性を待たせるためであシ、o
、 iμm以上とするのは磁気テープ相対移動方向逃げ
側での磁界強度分布全綴やたなスロープ状にするため必
要である。゛
なお、本発明の磁気消去ヘッドは、VTR用の回転型消
去ヘッドとして用いるのみならず、固定型消去ヘッドと
して用いるよりにしてもよい。It is preferable that the thin film 14 disposed on the relief side be less than one part of the thin film 13 and 0°1 μm or more. This is thin film 13
If the film thickness is 5 μm or more, cracks may occur during bonding or peeling of the film may occur due to the difference in thermal expansion coefficient between the ferrite core piece 10.11 and the glass 16 for fusion bonding. However, if the thickness is less than 1 μm, the effect of placing the high saturation magnetic flux density material in the gap forming portion will be lost. Moreover, the reason why the thickness of the thin film 14 is set to be less than 100 of the total thickness of the thin film 13 is to avoid asymmetry in the above-mentioned magnetic field strength distribution.
, i .mu.m or more is necessary in order to make the magnetic field strength distribution on the escape side in the direction of relative movement of the magnetic tape full-length or in the form of a vertical slope. Note that the magnetic erasing head of the present invention may be used not only as a rotary erasing head for a VTR, but also as a fixed erasing head.
以上の説明から明らかなように、本発明によ几ば、一対
のコア素片を構成する磁性材料の飽和磁束密度よシも高
い飽和磁束密度を有する磁性材料薄膜を、ギャップスペ
ーサの両側に配し、磁気記録媒体であるたとえば磁気テ
ープ相対移動方向の逃げ側の上記薄膜の膜厚全進入側の
薄膜の膜厚ニジも薄く形成するよりにしている。これに
よシ、たとえばメタルテープのような高い抗磁力Hck
有する磁気テープに記憶さ几ている信号を消去するのに
充分な磁界強度2得ることができるとともに、1勺逃げ
側に傾斜を持つような磁界強度分布によって、消去周波
数の信号が磁気テープに記録さ九るようなことはなく、
この消去周波数成分がバイアスとなシ消去さ几るべき信
号が再び磁気テープ上に記録さ几る再記録が起こるよう
なことはない。As is clear from the above description, according to the present invention, thin films of magnetic material having a saturation magnetic flux density higher than that of the magnetic material constituting the pair of core pieces are disposed on both sides of the gap spacer. However, the thickness of the thin film on the escape side of the magnetic recording medium, for example, the magnetic tape in the direction of relative movement, is also made thinner. In addition, for example, high coercive force Hck such as metal tape
It is possible to obtain a magnetic field strength 2 sufficient to erase the signals stored on the magnetic tape, and the signal at the erasing frequency is recorded on the magnetic tape due to the magnetic field strength distribution having a slope on the side of the escape. There is no need to worry,
If this erasing frequency component is used as a bias, the signal to be erased will not be recorded again on the magnetic tape, thereby preventing re-recording.
このJ:うに、本発明によって、高い消去効率ケ持つ磁
気消去ヘッドを実現することができる。According to the present invention, a magnetic erasing head with high erasing efficiency can be realized.
第1図Aは従来の磁気消去ヘッドの概略断面図、第1図
Bは第1図Aの磁気消去ヘッドの磁界強度分布金示す特
性図、第2図Aは本発明の前提となる技術によって構成
さnる消去ヘッドの概略断面図、第2図Bは第2図Aの
磁気消去ヘッドの磁界強度分布を示す特性図、第3図は
本発明に係る磁気消去ヘッドの外観斜視図、第4図は第
3図の磁気消去ヘッドの要部斜視図、第5図Aは第3図
の磁気消去ヘッドの磁界強度分布7示す特性図、第5図
13は第4図のI−I線断面図である。
to、ii−・・ コア素片
12・・・巻線穴
13 、14 、、、磁性材料薄膜
15−−− ギャップスペーサ
16・會・ガラス
X・・・磁気テープ相対移動方向
特許出願人 ン二一株式会社
代理人 弁理士 小 池 見
間 1) 村 榮 −
第1 図(A)
−4゜
第1図(B)
テープ担刻e動力伺円邑高1 −
第2図(A)
第2図(B)
テーア柑対物゛動力匈巨# −
第3図
第4図
6
第5 図(A)
第5 図(B)FIG. 1A is a schematic cross-sectional view of a conventional magnetic erasing head, FIG. 1B is a characteristic diagram showing the magnetic field strength distribution of the magnetic erasing head of FIG. 1A, and FIG. FIG. 2B is a characteristic diagram showing the magnetic field strength distribution of the magnetic erase head of FIG. 2A, and FIG. 3 is an external perspective view of the magnetic erase head according to the present invention. 4 is a perspective view of the main parts of the magnetic erasing head in FIG. 3, FIG. 5A is a characteristic diagram showing the magnetic field strength distribution 7 of the magnetic erasing head in FIG. 3, and FIG. 5 13 is a line I-I in FIG. 4. FIG. to, ii-- Core piece 12... Winding holes 13, 14,..., Magnetic material thin film 15-- Gap spacer 16, Ai, Glass X... Direction of relative movement of magnetic tape Patent applicant N2 1 Co., Ltd. Agent Patent Attorney Koike Mima 1) Sakae Mura - Figure 1 (A) -4゜Figure 1 (B) Tape engraving e-Dyokuryokuenmura High School 1 - Figure 2 (A) 2 Figure (B) Thea's objective: power force # - Figure 3 Figure 4 Figure 6 Figure 5 (A) Figure 5 (B)
Claims (1)
面側に、上記軟磁性材料よシ高い飽和磁束密度を有する
軟磁性材料薄膜上そnぞれ形成し、この一対のコア素片
を非磁性材料のギャップスペーサケ介して接合する磁気
消去ヘッドにおいて、磁気記録媒体進入側のコア木片に
形成さnた上記磁性材料薄膜の膜厚は磁気記録媒体逃げ
側のコア素片に形成さ−nた上記磁性材料薄膜の膜厚よ
シ厚いことを特徴とする磁気消去ヘッド。A thin film of a soft magnetic material having a higher saturation magnetic flux density than the above-mentioned soft magnetic material is formed on the magnetic gap forming surface side of a pair of core pieces made of a soft magnetic material, and the pair of core pieces are In a magnetic erasing head that is joined via a gap spacer made of non-magnetic material, the thickness of the thin film of magnetic material formed on the core piece on the side where the magnetic recording medium enters is the same as that formed on the core piece on the side where the magnetic recording medium escapes. A magnetic erasing head characterized in that the film thickness is greater than that of the above-mentioned thin film of magnetic material.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19893383A JPS6089806A (en) | 1983-10-24 | 1983-10-24 | Magnetic erasure head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19893383A JPS6089806A (en) | 1983-10-24 | 1983-10-24 | Magnetic erasure head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6089806A true JPS6089806A (en) | 1985-05-20 |
| JPH0467245B2 JPH0467245B2 (en) | 1992-10-27 |
Family
ID=16399379
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19893383A Granted JPS6089806A (en) | 1983-10-24 | 1983-10-24 | Magnetic erasure head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6089806A (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60160008A (en) * | 1984-01-17 | 1985-08-21 | エヌ・ベー・フイリツプス・フルーイランペンフアブリケン | Magnetic head |
| JPS63167407A (en) * | 1986-12-27 | 1988-07-11 | Sony Corp | Magnetic erasing head |
| US4772967A (en) * | 1985-11-13 | 1988-09-20 | Sanyo Electric Co., Ltd. | Magnetic recording apparatus in a helical scan system |
| US5448425A (en) * | 1991-11-29 | 1995-09-05 | Nec Corporation | Method for erasing information recorded on magnetic tape with reduced residual magnetization |
-
1983
- 1983-10-24 JP JP19893383A patent/JPS6089806A/en active Granted
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60160008A (en) * | 1984-01-17 | 1985-08-21 | エヌ・ベー・フイリツプス・フルーイランペンフアブリケン | Magnetic head |
| US4772967A (en) * | 1985-11-13 | 1988-09-20 | Sanyo Electric Co., Ltd. | Magnetic recording apparatus in a helical scan system |
| JPS63167407A (en) * | 1986-12-27 | 1988-07-11 | Sony Corp | Magnetic erasing head |
| US5448425A (en) * | 1991-11-29 | 1995-09-05 | Nec Corporation | Method for erasing information recorded on magnetic tape with reduced residual magnetization |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0467245B2 (en) | 1992-10-27 |
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