JPS61296515A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPS61296515A JPS61296515A JP13813785A JP13813785A JPS61296515A JP S61296515 A JPS61296515 A JP S61296515A JP 13813785 A JP13813785 A JP 13813785A JP 13813785 A JP13813785 A JP 13813785A JP S61296515 A JPS61296515 A JP S61296515A
- Authority
- JP
- Japan
- Prior art keywords
- working gap
- head body
- magnetic
- gap
- boundaries
- 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
Links
Abstract
Description
【発明の詳細な説明】 産業上の利用分野 この発明は、磁気記録装置の磁気ヘッドに関する。[Detailed description of the invention] Industrial applications The present invention relates to a magnetic head for a magnetic recording device.
従来の技術
従来、第10図、第11図に示すように、磁性材により
形成したヘッド本体50の媒体対接面51に作動ギャッ
プ52を形成し、この作動ギヤツブ52め面側にヘッド
本体50より飽和磁束密度の高い磁性膜53.54を形
成し、ヘッド本体50に磁気コイル55を巻回した磁気
ヘッドが存する。2. Description of the Related Art Conventionally, as shown in FIGS. 10 and 11, an operating gap 52 is formed in a medium contacting surface 51 of a head body 50 formed of a magnetic material, and a working gap 52 is formed on the inner surface of the operating gear 52. There is a magnetic head in which magnetic films 53 and 54 having a higher saturation magnetic flux density are formed and a magnetic coil 55 is wound around the head body 50.
第12図、第13図に示すように作動ギャップ52の一
側に飽和磁束密度の高い磁性膜53を形成したものも存
する。As shown in FIGS. 12 and 13, there is also a device in which a magnetic film 53 with a high saturation magnetic flux density is formed on one side of the working gap 52.
発明が解決しようとする問題点
従来は、ヘッド本体50と磁性膜53.54との境界5
6が本来の記録再生用の作動ギャップ52に対して平行
である。境界5Gは微小なギャップが形成される。した
がって、磁気記録媒体に記録された信号が作動ギャップ
52と境界56との両方で再生されるにれらの再生信号
は記録波長に対応した位相差を生じる。したがって、磁
気記録媒体の保磁力Hcを10000 e 、ヘッド本
体50と磁気記録媒体との相対速度を2 m / sと
した場合の再生特性は第14図に示すようになる。Problems to be Solved by the Invention Conventionally, the boundary 5 between the head body 50 and the magnetic films 53 and 54
6 is parallel to the actual working gap 52 for recording and reproducing. A minute gap is formed at the boundary 5G. Therefore, when a signal recorded on the magnetic recording medium is reproduced at both the working gap 52 and the boundary 56, the reproduced signals generate a phase difference corresponding to the recording wavelength. Therefore, when the coercive force Hc of the magnetic recording medium is 10,000 e and the relative speed between the head body 50 and the magnetic recording medium is 2 m/s, the reproduction characteristics are as shown in FIG. 14.
すなわち、その周波数が高くなるにともない再生出力が
低下する傾向は現在の技術ではやむを火ないものである
が、このような再生出力の状態では前述の作動ギャップ
52と境界56との寸法及び周波数の条件により波打ち
現象が生ずる欠点を有する。In other words, the tendency for the playback output to decrease as the frequency increases is unavoidable in the current technology, but in such a state of playback output, the dimensions of the above-mentioned operating gap 52 and the boundary 56 and the frequency It has the disadvantage that a waving phenomenon occurs depending on the conditions.
この発明はこのような点に鑑みなされたもので、記録信
号を周波数に影響されることなく再生しうる磁気ヘッド
をうろことを目的とする。The present invention has been made in view of these points, and an object thereof is to provide a magnetic head that can reproduce recorded signals without being affected by frequency.
問題点を解決するための手段。A means to solve problems.
この発明は、第1図、第2図に代表して示すように、ヘ
ッド本体1の媒体対接面2に作動ギャップ3を形成し、
ヘッド本体1より飽和磁束密度の高い磁性膜4,5を少
なくとも作動ギャップ3の一側に位置させて形成し、ヘ
ッド本体1と磁性膜4.5との境界6,7を作動ギャッ
プ3と平行な直線8,9に対して傾斜させる。As typically shown in FIGS. 1 and 2, this invention forms an operating gap 3 in the medium contacting surface 2 of the head body 1,
The magnetic films 4 and 5 having a higher saturation magnetic flux density than the head body 1 are formed to be located at least on one side of the working gap 3, and the boundaries 6 and 7 between the head body 1 and the magnetic films 4 and 5 are parallel to the working gap 3. It is inclined with respect to the straight lines 8 and 9.
作用
したがって、作動ギャップ3により記録した信号に対し
て、作動ギャップ3は忠実に再生信号を出力するが、境
界6,7ではアジマス損失のため再生効率が低下し、作
動ギャップ3による再生出力が有効に作用する。Therefore, with respect to the signal recorded by the working gap 3, the working gap 3 faithfully outputs a reproduction signal, but at the boundaries 6 and 7, the reproduction efficiency decreases due to azimuth loss, and the reproduction output by the working gap 3 becomes effective. It acts on
実施例
この発明の第一の実施例を第1図ないし第3図に基づい
て説明する。フェライトにより形成されたヘッド本体1
の媒体対接面2に直線の作動ギャップ3が形成され、作
動ギャップ3の両側にフェライトより飽和磁束密度の高
いセンダストによる磁性膜4,5が形成されている。ヘ
ッド本体1と磁性膜4,5との境界6,7はヘッド本体
1の両側と平行であるが、作動ギャップ3と平行な直線
8.9に対してはθなるアジマス角をもって傾斜する。Embodiment A first embodiment of the present invention will be described with reference to FIGS. 1 to 3. Head body 1 made of ferrite
A linear working gap 3 is formed on the medium contacting surface 2 of the working gap 3, and magnetic films 4 and 5 made of sendust, which has a higher saturation magnetic flux density than ferrite, are formed on both sides of the working gap 3. The boundaries 6, 7 between the head body 1 and the magnetic films 4, 5 are parallel to both sides of the head body 1, but are inclined at an azimuth angle θ with respect to a straight line 8.9 parallel to the working gap 3.
そして、ヘッド本体1には磁気コイル1゜が巻回されて
いる。A magnetic coil 1° is wound around the head body 1.
このような構成において、磁気記録媒体とヘッド本体1
とを相対的に移動させてデータの記録又は再生を行う。In such a configuration, the magnetic recording medium and the head body 1
Data is recorded or reproduced by moving the two relative to each other.
作動ギャップ3により記録した信号は作動ギャップ3と
境界6,7から再生されるが、境界は6,7は作動ギャ
ップ3に対してアジマス角をもっているため再生信号の
読み取り幅が広く再生効率が極度に低下する。したがっ
て、作動ギャップ3による再生出力が有効に作用する。The signal recorded by the working gap 3 is reproduced from the working gap 3 and the boundaries 6 and 7, but since the boundaries 6 and 7 have an azimuth angle with respect to the working gap 3, the reading width of the reproduced signal is wide and the reproduction efficiency is extremely high. decreases to Therefore, the reproduction output by the actuation gap 3 acts effectively.
ちなみに、磁気記録媒体の保磁力Hcを10000e、
ヘッド本体1と磁気記録媒体との相対速度を2m/sと
した場合、再生出力と記録周波数との関係は第3図の通
りである。By the way, the coercive force Hc of the magnetic recording medium is 10000e,
When the relative speed between the head body 1 and the magnetic recording medium is 2 m/s, the relationship between the reproduction output and the recording frequency is as shown in FIG.
ついで、作動ギャップ3と平行な直線8又は9に対する
境界6又は7のアジマス角の付けかたの第二、第三、第
四の実施例について説明する。前記実施例と同一部分は
同一符号を用いる。作用に付いては前記実施例と同様の
ため説明を省略する。Next, second, third and fourth embodiments of how to set the azimuth angle of the boundary 6 or 7 with respect to the straight line 8 or 9 parallel to the working gap 3 will be described. The same parts as in the previous embodiment use the same reference numerals. Since the operation is similar to that of the previous embodiment, the explanation will be omitted.
第二の実施例は、第4図、第5図に示すように、作動ギ
ャップ3をヘッド本体1の両側に対して平行にし、境界
6,7を作動ギャップ3と平行な直線8,9に対して傾
斜させたものである。In the second embodiment, as shown in FIGS. 4 and 5, the working gap 3 is made parallel to both sides of the head body 1, and the boundaries 6 and 7 are made into straight lines 8 and 9 parallel to the working gap 3. It is tilted to the opposite direction.
第三の実施例は、第6図、第7図に示すように、両側の
境界6,7を作動ギャップ3に対して対称的に傾斜させ
たものである。In the third embodiment, as shown in FIGS. 6 and 7, the boundaries 6 and 7 on both sides are symmetrically inclined with respect to the working gap 3.
第四の実施例は、第8図、第9図に示すように、作動ギ
ャップ3の一側に磁性膜4を形成したもので、作動ギャ
ップ3に対する境界6の傾けがたは第一の実施例と同様
である。In the fourth embodiment, as shown in FIGS. 8 and 9, a magnetic film 4 is formed on one side of the working gap 3, and the inclination of the boundary 6 with respect to the working gap 3 is different from that of the first embodiment. Similar to the example.
発明の効果
この発明は上述のように、データの記録再生のための本
来の作動ギャップに対して、ヘッド本体と飽和磁束密度
の高い磁性膜との境界を傾けたことにより、作動ギャッ
プにより記録した信号に対して、境界の再生効率を極端
に低下させることができ、したがって、再生特性の優れ
た作動ギャップを主体に正確に再生することができる効
果を有する。Effects of the Invention As described above, this invention enables recording using the working gap by tilting the boundary between the head body and the magnetic film with high saturation magnetic flux density with respect to the original working gap for recording and reproducing data. With respect to the signal, it is possible to extremely reduce the reproduction efficiency at the boundary, and therefore, it has the effect of accurately reproducing mainly the operating gap with excellent reproduction characteristics.
第1図はこの発明の第一の実施例を示す斜視図、第2図
はその正面図、第3図はその再生特性を示すグラフ、第
4図はこの発明の第二の実施例を示す斜視図、第5図は
その正面図、第6図はこの発明の第三の実施例を示す斜
視図、第7図はその正面図、第8図はこの発明の第四の
実施例を示す斜視図、第9図はその正面図、第10図は
従来の−例を示す斜視図、第11図はその正面図、第1
2図は従来の他の実施例を示す斜視図、第、13図はそ
の正面図、第14図は従来の再生特性を示すグラフであ
る。Fig. 1 is a perspective view showing a first embodiment of this invention, Fig. 2 is a front view thereof, Fig. 3 is a graph showing its reproduction characteristics, and Fig. 4 shows a second embodiment of this invention. A perspective view, FIG. 5 is a front view, FIG. 6 is a perspective view showing a third embodiment of the invention, FIG. 7 is a front view, and FIG. 8 is a fourth embodiment of the invention. 9 is a front view thereof, FIG. 10 is a perspective view showing a conventional example, FIG. 11 is a front view thereof, and
2 is a perspective view showing another conventional example, FIGS. 13 and 13 are front views thereof, and FIG. 14 is a graph showing the conventional reproduction characteristics.
Claims (1)
ギャップを形成し、前記ヘッド本体より飽和磁束密度の
高い磁性膜を少なくとも前記作動ギャップの一側に位置
させて前記媒体対接面に形成し、前記ヘッド本体と前記
磁性膜との境界を前記作動ギャップに対して傾斜させた
ことを特徴とする磁気ヘッド。A working gap is formed on a medium contacting surface of a head main body formed of a magnetic material, and a magnetic film having a higher saturation magnetic flux density than the head main body is positioned on at least one side of the working gap and formed on the medium contacting surface. A magnetic head characterized in that a boundary between the head main body and the magnetic film is inclined with respect to the working gap.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13813785A JPS61296515A (en) | 1985-06-25 | 1985-06-25 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13813785A JPS61296515A (en) | 1985-06-25 | 1985-06-25 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61296515A true JPS61296515A (en) | 1986-12-27 |
Family
ID=15214858
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13813785A Pending JPS61296515A (en) | 1985-06-25 | 1985-06-25 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61296515A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5001588A (en) * | 1989-06-30 | 1991-03-19 | Ampex Corporation | Composite core magnetic transducer having a wedge shaped core portion |
-
1985
- 1985-06-25 JP JP13813785A patent/JPS61296515A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5001588A (en) * | 1989-06-30 | 1991-03-19 | Ampex Corporation | Composite core magnetic transducer having a wedge shaped core portion |
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