JPH0439736B2 - - Google Patents
Info
- Publication number
- JPH0439736B2 JPH0439736B2 JP60281585A JP28158585A JPH0439736B2 JP H0439736 B2 JPH0439736 B2 JP H0439736B2 JP 60281585 A JP60281585 A JP 60281585A JP 28158585 A JP28158585 A JP 28158585A JP H0439736 B2 JPH0439736 B2 JP H0439736B2
- Authority
- JP
- Japan
- Prior art keywords
- erase
- magnetic head
- erasing
- gap
- current
- 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.)
- Expired - Lifetime
Links
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- Magnetic Heads (AREA)
Description
【発明の詳細な説明】
(イ) 産業上の利用分野
本発明は磁気ヘツドに関するものであり、特に
8ミリVTR等において回転型に用いられる消去
ヘツドに関する。DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to a magnetic head, and particularly to an erasing head used in a rotary manner in an 8 mm VTR or the like.
(ロ) 従来の技術
フエライトコア半体が記録媒体への当接面で作
動ギヤツプおよび金属磁性層を挾んで対向すると
共に、そのギヤツプサイドにおける擬似ギヤツプ
部が前記作動ギヤツプから外側へ行くに従つて広
がる形式の磁気ヘツドは例えば特開昭60−89807
号に記載されている。このような形式の磁気ヘツ
ドを8ミリVTRの回転消去型ヘツドとして用い
る場合の記録媒体(磁気テープ)への当接面形態
として第6図の構造のものが提案されている。(b) Prior art The ferrite core halves face each other with the working gap and the metal magnetic layer sandwiched between them at the surfaces that contact the recording medium, and the pseudo-gap portion on the side of the gap widens as it goes outward from the working gap. For example, the type of magnetic head is disclosed in Japanese Patent Application Laid-Open No. 60-89807.
It is stated in the number. When a magnetic head of this type is used as a rotary erasing head for an 8 mm VTR, the structure shown in FIG. 6 has been proposed as a contact surface configuration for a recording medium (magnetic tape).
第6図において、1,2は第1、第2フエライ
トコア半体であり、3はガラス材料よりなる作動
ギヤツプである。4は第2フエライトコア半体2
に予め被膜形成されたセンダスト膜である。この
センダスト膜4の代りにアモルフアスやパーマロ
イなどの金属磁性材料膜も可能である。両サイド
のトラツク幅規制溝5には前記作動ギヤツプ3を
形成するガラス6が同時に充填されている。この
トラツク幅規制溝5のガラスはテープ当接面積の
確保と作動ギヤツプ部の保護を与える。例えば
VTRに使用される回転型の消去ヘツドは、きれ
いな継ぎ撮りを実現するために任意の1フレーム
を消去できることが必要である。この消去ヘツド
に要求されることは充分な消去率と安定な消去幅
であるが、充分な消去率を得るためには第5図か
ら分るように少くとも150mA以上の電流(通常
の記録電流に比べて10倍程度の大きな消費電流)
を流す必要がある。第5図で横軸は磁気ヘツドに
流す6MHzの消去電流を示し、縦軸は消去率を示
す。そして図中、Yは輝度信号Cは色信号、Pは
トラツクキング用のパイロツト信号の消去特性を
それぞれ示す。 In FIG. 6, 1 and 2 are first and second ferrite core halves, and 3 is an operating gap made of glass material. 4 is the second ferrite core half 2
This is a sendust film that is coated in advance on the Instead of the sendust film 4, a metal magnetic material film such as amorphous or permalloy may be used. The track width regulating grooves 5 on both sides are filled with glass 6 forming the working gap 3 at the same time. The glass in the track width regulating groove 5 ensures a tape contact area and protects the operating gap. for example
The rotary erasing head used in VTRs needs to be able to erase any single frame in order to achieve clear transition shots. What is required of this erase head is a sufficient erasing rate and a stable erasing width, but in order to obtain a sufficient erasing rate, as shown in Figure 5, a current of at least 150 mA (normal recording current (approximately 10 times larger current consumption compared to
It is necessary to flow. In FIG. 5, the horizontal axis shows the 6MHz erasing current applied to the magnetic head, and the vertical axis shows the erasing rate. In the figure, Y indicates the luminance signal C indicates the color signal, and P indicates the erasing characteristic of the pilot signal for tracking.
(ハ) 発明が解決しようとする問題点
しかしながら、上記第6図の如き構造の磁気ヘ
ツド、即ちギヤツプ長Gが略一定で、第1フエラ
イトコア半体1側のトラツク幅TFに対しセンダ
スト膜4側のトラツク側TSが少許大きくなつて
いる構造の消去ヘツドでは通常の記録電流の10倍
程度の大きな消費電流を流した場合、漏れ磁界が
大きくなり、見掛け上のトラツク幅(前記TF)
に比べ実際に消去された幅(消去幅)が大きくな
るという問題があつた。この消去幅はTFよりも
TSに依存し、しかも電流値に応じて変化しやす
いという問題もある。即ち、第2図において実線
aで示すように前記従来構造では消去電流が
400mA以上では消去幅の広がりは略一定になる
が、特に150mA〜300mAにかけては直線的に変
化する。従つて、記録電流の10倍程度の大きさの
消去電流(250mA〜300mA)では消去幅の広が
り(従つて消去幅)は消去電流値の変化に応答し
て大きく変化してしまう。一方、消去電流回路は
消去ヘツドのコイルを利用した共振回路を採用し
ている場合が多く、磁気ヘツドのインダクタンス
や共振回路のQの僅かな変化に伴ない消去電流が
変化し、このため消去幅も変化するという問題が
あつた。この問題が生じないようにするためには
前記インダクタンスやQの規格が厳しくして、そ
のバラツキを少なくすればよいが、歩留りや生産
性などの面で困難である。また消去電流を大きく
することも考えられるが、電気回路の信頼性およ
び消費電力の面から好ましくない。(c) Problems to be Solved by the Invention However, in a magnetic head having a structure as shown in FIG. 6, the gap length G is approximately constant, and the sendust film is In an erase head with a structure in which the track side T S on the 4th side is slightly larger, when a large current consumption of about 10 times the normal recording current is applied, the leakage magnetic field becomes large and the apparent track width (T F )
There was a problem that the actual erased width (erased width) was larger than that of the original. This erasure width is larger than T F
There is also the problem that it depends on T S and is likely to change depending on the current value. That is, as shown by the solid line a in FIG. 2, in the conventional structure, the erase current is
At 400 mA or more, the spread of the erase width becomes approximately constant, but it changes linearly especially from 150 mA to 300 mA. Therefore, when the erase current is about 10 times as large as the recording current (250 mA to 300 mA), the spread of the erase width (therefore, the erase width) changes greatly in response to changes in the erase current value. On the other hand, erase current circuits often employ a resonant circuit using the coil of the erase head, and the erase current changes with slight changes in the inductance of the magnetic head or the Q of the resonant circuit. There was also the problem that things were changing. In order to prevent this problem from occurring, the standards for the inductance and Q may be made stricter to reduce their variations, but this is difficult in terms of yield and productivity. It is also conceivable to increase the erase current, but this is not preferable from the viewpoint of reliability of the electric circuit and power consumption.
(ニ) 問題点を解決するための手段
本発明では、フエライトコア半体が記録媒体へ
の当接面で作動ギヤツプおよび金属磁性層を挾ん
で対向すると共に、そのギヤツプサイドにおける
トラツク幅規制溝が前記作動ギヤツプから外側へ
行くに従つて広がる形式の磁気ヘツドにおいて、
前記金属磁性層の前記作動ギヤツプに面する角度
を切欠いている。(d) Means for Solving the Problems In the present invention, the ferrite core halves face each other with the actuating gap and the metal magnetic layer sandwiched between them at the surfaces that contact the recording medium, and the track width regulating grooves on the side of the gap are arranged as described above. In a magnetic head that widens outward from the working gap,
The metal magnetic layer is notched at an angle facing the working gap.
(ホ) 作 用
前記の構成によれば消去幅の広がりが一定のヘ
ツドを得ることができる。即ち、150mA以上の
消費電流の場合は200mA程度でもトラツクTS1の
両端部に漏れ磁界を生じ、300mA、400mAにな
つても消去幅は殆んど変化しない。(e) Effect According to the above configuration, a head with a constant spread of erase width can be obtained. That is, in the case of a current consumption of 150 mA or more, a leakage magnetic field is generated at both ends of the track T S1 even at about 200 mA, and the erase width hardly changes even when the current is 300 mA or 400 mA.
(ヘ) 実施例
第1図は本発明を実施した磁気ヘツドのテープ
への当接面を示しており、第6図と同一部分には
同一の符号を付してある。本発明の特徴とすると
ころはセンダスト膜4(センダスト膜の代りに他
の金属磁性膜でもよい)の前記第1フエライトコ
ア半体1および作動ギヤツプ3へ面する部分の角
部7,8に切欠き9を設けた点である。第1図の
ように切欠き9によつて、その部分と相手の第1
フエライトコア半体1との間のギヤツプは漸次大
きくなり、2倍程度にまでなる。その結果、この
切欠き9からは磁界が漏れ、消去幅は大きくな
る。この消去ヘツドの消去電流に対する消去幅の
広がりは第2図の破線bで示すようになり、
200mA〜300mAの消去電流でも消去幅は殆んど
変化しないことになる。即ち、消去幅はセンダス
ト膜4側のトラツク幅TS1とギヤツプ長Gの和と
なり、略一定となる。切欠き9の形状については
適当な漏れ磁界を生じさせるためにθの値は30゜
θ60゜が望ましく、特にTS2−TS1=Gの関係
を充足するθ=45゜のときが最適であつた。第3
図と第4図はそれぞれ本発明の他の実施例を示し
ており、第3図はセンダスト膜形成前に第2フエ
ライトコア半体2の角部10,11を予め加工し
ておいて、その上にセンダスト膜を形成すること
によつて自動的にセンダスト膜4の角部に切欠き
9を設けたものである。一方、第4図はセンダス
ト膜4を形成した後にダイシングソー等で同時加
工して得たものである。以上において、8ミリ
VTR用の回転型消去ヘツドを例に挙げて説明し
たが、通常の1/2インチ型VTR用の回転消去
ヘツドにも同様に適用できる。また、上述の実施
例で第1フエライトコア半体1側にもセンダスト
等の金属膜を形成した磁気ヘツドに対しても本発
明が適用できることはいうまでもない。(F) Embodiment FIG. 1 shows the contact surface of a magnetic head embodying the present invention against a tape, and the same parts as in FIG. 6 are given the same reference numerals. A feature of the present invention is that the corners 7 and 8 of the sendust film 4 (another metal magnetic film may be used instead of the sendust film) facing the first ferrite core half 1 and the working gap 3 are cut. This is because the notch 9 is provided. As shown in Figure 1, the notch 9 allows you to
The gap between the ferrite core half body 1 gradually increases and becomes about twice as large. As a result, the magnetic field leaks from this notch 9, and the erase width increases. The expansion of the erase width with respect to the erase current of this erase head is shown by the broken line b in FIG.
Even with an erase current of 200 mA to 300 mA, the erase width hardly changes. That is, the erase width is the sum of the track width T S1 on the sendust film 4 side and the gap length G, and is substantially constant. Regarding the shape of the notch 9, in order to generate an appropriate leakage magnetic field, the value of θ is preferably 30° θ60°, and in particular, θ = 45°, which satisfies the relationship T S2 - T S1 = G, is optimal. Ta. Third
4 and 4 respectively show other embodiments of the present invention, and FIG. 3 shows that the corners 10 and 11 of the second ferrite core half 2 are processed in advance before forming the sendust film. Notches 9 are automatically provided at the corners of the sendust film 4 by forming the sendust film thereon. On the other hand, FIG. 4 is obtained by simultaneously processing with a dicing saw or the like after forming the sendust film 4. In the above, 8 mm
Although the explanation has been given using a rotary erasing head for a VTR as an example, the present invention can be similarly applied to a rotary erasing head for a normal 1/2 inch VTR. It goes without saying that the present invention can also be applied to the magnetic head in which a metal film such as sendust is formed on the first ferrite core half 1 side in the above embodiment.
(ト) 発明の効果
本発明によれば消去電流を著しく大きくするこ
となしに、消去電流の値如何に拘わらず消去幅の
一定な消去ヘツドを実現できるという効果があ
る。従つて、磁気ヘツドのインダクタンスや共振
回路のQの規格を広げることができ、歩留りも大
きく向上する。(G) Effects of the Invention According to the present invention, an erase head with a constant erase width regardless of the value of the erase current can be realized without significantly increasing the erase current. Therefore, the specifications for the inductance of the magnetic head and the Q of the resonant circuit can be expanded, and the yield can be greatly improved.
第1図は本発明を実施した磁気ヘツドの要部正
面図であり、第2図はその説明図である。第3図
および第4図はそれぞれ本発明の他の実施例の要
部正面図である。第5図は消去ヘツドの消去特性
図であり、第6図は従来の磁気ヘツドの要部正面
図である。
1,2…第1、第2フエライトコア半体、5…
トラツク幅規制溝、9…切欠き。
FIG. 1 is a front view of essential parts of a magnetic head embodying the present invention, and FIG. 2 is an explanatory diagram thereof. 3 and 4 are front views of essential parts of other embodiments of the present invention, respectively. FIG. 5 is a diagram showing the erasing characteristics of the erasing head, and FIG. 6 is a front view of the main parts of a conventional magnetic head. 1, 2...first and second ferrite core halves, 5...
Track width regulation groove, 9...notch.
Claims (1)
ライトコア半体に金属磁性層を設け、前記一対の
フエライトコア半体が記録媒体への当接面で作動
ギヤツプおよび前記金属磁性層を挟んで対向する
と共に、前記作動ギヤツプの側方にトラツク幅規
制溝を有する構造の消去磁気ヘツドにおいて、前
記金属磁性層のうち前記作動ギヤツプと前記トラ
ツク幅規制溝との間に位置する角部を切欠いたこ
とを特徴とする消去磁気ヘツド。 2 前記角部の切欠きの長さを作動ギヤツプ長の
略半分としたことを特徴とする特許請求の範囲第
1項に記載の消去磁気ヘツド。[Scope of Claims] 1 A metal magnetic layer is provided on one of the pair of ferrite core halves, and the pair of ferrite core halves form an operating gap and the metal magnetic layer on the surface that contacts the recording medium. In an erasing magnetic head having a structure in which track width regulating grooves are located on sides of the working gap and are opposed to each other with a layer in between, a corner of the metal magnetic layer located between the working gap and the track width regulating groove is provided. An erasing magnetic head characterized by having a notched portion. 2. The erasing magnetic head according to claim 1, wherein the length of the notch in the corner is approximately half the length of the working gap.
Priority Applications (6)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60281585A JPS62140210A (en) | 1985-12-13 | 1985-12-13 | Magnetic head |
| DE86115344T DE3688971T2 (en) | 1985-11-13 | 1986-11-05 | Magnetic recording device. |
| EP86115344A EP0227920B1 (en) | 1985-11-13 | 1986-11-05 | Magnetic recording apparatus |
| US06/927,487 US4772967A (en) | 1985-11-13 | 1986-11-06 | Magnetic recording apparatus in a helical scan system |
| CA000522595A CA1292309C (en) | 1985-11-13 | 1986-11-10 | Magnetic recording apparatus |
| KR868609523A KR930008777B1 (en) | 1985-11-13 | 1986-11-12 | Magnetic recording apparatus in a helical scan system |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60281585A JPS62140210A (en) | 1985-12-13 | 1985-12-13 | Magnetic head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62140210A JPS62140210A (en) | 1987-06-23 |
| JPH0439736B2 true JPH0439736B2 (en) | 1992-06-30 |
Family
ID=17641205
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60281585A Granted JPS62140210A (en) | 1985-11-13 | 1985-12-13 | Magnetic head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62140210A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2591009B2 (en) * | 1988-01-30 | 1997-03-19 | ソニー株式会社 | Magnetic head |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5496013A (en) * | 1978-01-13 | 1979-07-30 | Matsushita Electric Ind Co Ltd | Compound magnetic head |
| JPS56169214A (en) * | 1980-06-02 | 1981-12-25 | Nippon Hoso Kyokai <Nhk> | Magnetic head |
| JPS5715217A (en) * | 1980-06-30 | 1982-01-26 | Hitachi Ltd | Magnetic head and its manufacture |
| JPS5819698U (en) * | 1981-08-01 | 1983-02-07 | 下川 清 | Sized cutting and drooping device for toilet paper rolls |
| JPS5880124A (en) * | 1981-11-07 | 1983-05-14 | Sanyo Electric Co Ltd | Forming method of track width control groove of magnetic head |
-
1985
- 1985-12-13 JP JP60281585A patent/JPS62140210A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62140210A (en) | 1987-06-23 |
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