JPH02220209A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPH02220209A JPH02220209A JP4063089A JP4063089A JPH02220209A JP H02220209 A JPH02220209 A JP H02220209A JP 4063089 A JP4063089 A JP 4063089A JP 4063089 A JP4063089 A JP 4063089A JP H02220209 A JPH02220209 A JP H02220209A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- magnetic flux
- recording
- core
- 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
Links
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、高飽和磁束密度を必要とする磁気記録再生
装置に用いる磁気ヘッドに関するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a magnetic head used in a magnetic recording/reproducing device that requires high saturation magnetic flux density.
従来、フェライトヘッドより高い飽和磁束密度を必要と
する磁気ヘッドは、大別すると第3図に示すようにコア
全体を高飽和磁束密度の金属磁性体から構成するタイプ
と、第4図に示すようにコアの一部、特にギャンブ近傍
を同じ金属磁性体で構成するタイプとがある。第3図に
おいて、1は高飽和磁束密度の金i磁性体、2はギャッ
プを構成する非磁性体からなるギャップ材、4は金属磁
性体lを接合する接合材、5は信号の記録、再生を行な
う巻線コイルである。また第4図において、1は高飽和
磁束密度の金属磁性体、2はギャップを構成する非磁性
体からなるギャップ材、3はフェライトコア材、4は金
属磁性体lおよびコア材3を接合する接合材、5は信号
の記録、再生を行なう@線コイルである。Conventionally, magnetic heads that require a higher saturation magnetic flux density than ferrite heads can be roughly divided into two types, as shown in Figure 3, in which the entire core is made of a metallic magnetic material with a high saturation magnetic flux density, and two types, as shown in Figure 4. There is a type in which a part of the core, especially the vicinity of the gamb, is made of the same metallic magnetic material. In Fig. 3, 1 is a gold i magnetic material with high saturation magnetic flux density, 2 is a gap material made of a non-magnetic material constituting the gap, 4 is a bonding material for joining the metal magnetic material l, and 5 is a signal recording and reproducing material. This is a winding coil that performs. Further, in Fig. 4, 1 is a metal magnetic material with high saturation magnetic flux density, 2 is a gap material made of a non-magnetic material constituting the gap, 3 is a ferrite core material, and 4 is a material for joining the metal magnetic material l and the core material 3. The bonding material 5 is an @ wire coil for recording and reproducing signals.
上記した磁気ヘッドを用いて13号を記録する場合、巻
線コイル5に電流を通電し、その起磁力で発生した磁束
が金属磁性体l (第3図)若しくは金属磁性体1とフ
ェライトコア材3(第4図)およびギャップ材2を通る
。このとき、ギャップ材2は非磁性体のため磁束がギャ
ップ部分で外側にはみ出す、このはみ出した磁束がギャ
ップ部に対向して配置した磁気テープを磁化し、テープ
上に信号を記録する。一方、再生時は磁気テープ上の記
録磁化からの磁束が金属磁性体1を°通り、巻線コイル
5に起電力を生しる。これが再生信号として取出される
。When recording No. 13 using the magnetic head described above, a current is passed through the wire-wound coil 5, and the magnetic flux generated by the magnetomotive force is transmitted between the metal magnetic material 1 (Fig. 3) or the metal magnetic material 1 and the ferrite core material. 3 (FIG. 4) and gap material 2. At this time, since the gap material 2 is a non-magnetic material, the magnetic flux protrudes outward at the gap portion, and this protruding magnetic flux magnetizes the magnetic tape placed facing the gap portion, thereby recording a signal on the tape. On the other hand, during reproduction, the magnetic flux from the recorded magnetization on the magnetic tape passes through the metal magnetic body 1 and generates an electromotive force in the wire-wound coil 5. This is extracted as a reproduced signal.
従来の磁気ヘッドは以上のように構成されているので、
コア全体を金属磁性体で構成するタイプは、金属磁性体
1とフェライトコア材3との間に透磁率の変曲点(面)
が存在し、再生時に擬似的にギャップの作用をする。こ
の擬似ギャップ現象を軽減するため、従来は擬似ギャッ
プ面を本来のギャップ材2面と非平行になるようにして
いる。Since the conventional magnetic head is configured as described above,
In the type where the entire core is made of a metal magnetic material, there is an inflection point (plane) of magnetic permeability between the metal magnetic material 1 and the ferrite core material 3.
exists and acts as a pseudo gap during playback. In order to reduce this pseudo-gap phenomenon, conventionally the pseudo-gap surface is made non-parallel to the two surfaces of the original gap material.
つまり、金属磁性体lを接合面が非平行になるのに充分
なだけ厚く、しかも両側コアに形成するため、やはりコ
スト的に不利であるという課題があった。In other words, since the metal magnetic material l is thick enough to make the bonding surfaces non-parallel and is formed on both cores, there is still a problem in that it is disadvantageous in terms of cost.
この発明は上記のような課題を解消するためになされた
もので、磁気ヘッド製造時の金属磁性体形成を少な(抑
えるようにした磁気ヘッドを得ることを目的とする。The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to obtain a magnetic head in which the amount of metal magnetic material formed during manufacturing of the magnetic head is reduced (suppressed).
この発明に係る磁気ヘッドは、高透磁率フェライトから
なる磁気コアと、同じく高透磁率フェライトからなりギ
ャップ面に高飽和磁束密度の金属磁性体を付加した磁気
コアとをギャップ材を挾んで対向させ、上記磁気コアに
信号の記録、再生を行なう巻線コイルを備えたものであ
る。The magnetic head according to the present invention has a magnetic core made of high magnetic permeability ferrite and a magnetic core made of high magnetic permeability ferrite with a magnetic metal material having a high saturation magnetic flux density added to the gap surface, facing each other with a gap material in between. , the magnetic core is equipped with a wire-wound coil for recording and reproducing signals.
この発明においては、上記のように構成したので記録過
程においては、巻線コイルに流れる信号電流から発生し
た磁束が金属磁性体および磁気コアを通り、ギャップ部
分ではテープ内を通る。また、再生過程は金属磁性体で
テープ記録磁化から発生する磁束を磁気コア内に引込ん
で再生効率を確保することができる。In this invention, with the above configuration, during the recording process, the magnetic flux generated from the signal current flowing through the winding coil passes through the metal magnetic material and the magnetic core, and passes through the tape at the gap portion. Furthermore, during the reproduction process, the magnetic flux generated from tape recording magnetization is drawn into the magnetic core using a metal magnetic material, thereby ensuring reproduction efficiency.
以下、この発明の一実施例を図について説明する。第1
図はこの発明による磁気ヘッドの構成図と要部の拡大図
を示すもので、1はテープ走行方向後側のコアに形成さ
れた高飽和磁束密度の金属磁性体で、この金属磁性体l
の膜厚は磁気テープ上の信号記録波長のA−zである。An embodiment of the present invention will be described below with reference to the drawings. 1st
The figure shows a configuration diagram and an enlarged view of the main parts of a magnetic head according to the present invention. 1 is a metal magnetic material with a high saturation magnetic flux density formed in the core on the rear side in the tape running direction;
The film thickness is A-z of the signal recording wavelength on the magnetic tape.
ただし、この場合、膜厚とは金属膜のうち、高飽和磁束
密度の磁性体として有効な部分の厚み寸法をいう、2は
ギヤ、プを構成する非磁性体からなるギャップ材で、一
般には記録波長のA以下の厚みに形成されている。3は
磁気ヘッドを構成する高透磁率のフェライトコア、4は
これらコア3を接合する接合材、5は信号の記録再生を
行なう巻線コイルであって、コイル端子には図示しない
記録アンプや再生アンプが接続される。However, in this case, the film thickness refers to the thickness of the part of the metal film that is effective as a magnetic material with high saturation magnetic flux density. 2 is the gap material made of non-magnetic material that constitutes the gear, It is formed to have a thickness equal to or less than the recording wavelength A. 3 is a ferrite core with high magnetic permeability that constitutes the magnetic head, 4 is a bonding material that joins these cores 3, and 5 is a wound coil for recording and reproducing signals, and the coil terminals are connected to a recording amplifier and a reproducing device (not shown). Amplifier is connected.
第2図にこの発明による磁気ヘッドの記録再生過程の模
式図を示す、なお、図中6は記録媒体の磁気テープであ
る。FIG. 2 shows a schematic diagram of the recording and reproducing process of the magnetic head according to the present invention. In the figure, reference numeral 6 indicates a magnetic tape as a recording medium.
まず、記録過程においては、巻線コイル5に流れる信号
電流から発生した磁束がフェライトコア3および金属磁
性体lを遺り、ギャップ2部分ではテープ内を通過する
。このとき、テープ走行方向の前側はフェライトコア3
のため磁束は分散するが、後側は高飽和磁束密度の金属
磁性体lのため磁束は集中する。また、テープ走行に伴
ない磁気テープ6上に残る磁化部分は図に示すようにテ
ープ走行の後側で形成された扇形の磁束集中部分の磁化
である。First, in the recording process, the magnetic flux generated from the signal current flowing through the winding coil 5 leaves the ferrite core 3 and the metal magnetic material 1, and passes through the tape in the gap 2 portion. At this time, the front side in the tape running direction is the ferrite core 3.
Therefore, the magnetic flux is dispersed, but because the rear side is a metal magnetic material l with a high saturation magnetic flux density, the magnetic flux is concentrated. Further, the magnetized portion remaining on the magnetic tape 6 as the tape runs is the magnetization of a fan-shaped magnetic flux concentration portion formed at the rear side of the tape run, as shown in the figure.
一方、再生過程は金属磁性体lでテープ記録磁化から発
生する磁束をコア内に引込へことにより再生効率を確保
する。再生磁束の一部はオーブンループとなり、フェラ
イトコア3の形成時よりやや劣るものの使用上の問題は
生じない。特にこの発明の磁気ヘッドを用いて記録した
テープに対しては全く問題はなく充分な再生効率が得ら
れる。On the other hand, in the reproduction process, reproduction efficiency is ensured by drawing the magnetic flux generated from tape recording magnetization into the core using the metal magnetic material l. A part of the reproduced magnetic flux becomes an oven loop, and although it is slightly inferior to that when forming the ferrite core 3, there is no problem in use. In particular, there are no problems with tapes recorded using the magnetic head of the present invention, and sufficient playback efficiency can be obtained.
また、金属磁性体lとフェライトコア3との間に発生す
る擬似ギャップ現象も本来のギャップからの距離が波長
のA以下であるため、はぼ同一の信号を再生する形とな
り、信号成分として再生信号に悪影響を及ぼすことはな
い。In addition, since the pseudo gap phenomenon that occurs between the metal magnetic material l and the ferrite core 3 is less than the wavelength A from the original gap, almost the same signal is reproduced, and it is reproduced as a signal component. It will not adversely affect the signal.
なお、この発明による磁気ヘッドは、磁気テープ用へラ
ドについて説明したが、その他、面内記録タイプの磁気
ディスク装置用ヘッドについても上記と同様の作用を得
ることができる。Although the magnetic head according to the present invention has been described with respect to a magnetic tape head, the same effect as described above can also be obtained with a head for a longitudinal recording type magnetic disk device.
以上説明したようにこの発明によれば、高透磁率のフェ
ライトコアと、同じく高透磁率からなりギャップ面に飽
和磁束密度の高い金属磁性体を付加したフェライトコア
とをギャップ材を挟んで対向させたことにより、磁気ヘ
ッド製造時の金属磁性体の形成を少なく抑えろことがで
き、これによって、製造コストおよび装置コストが安価
にできる。As explained above, according to the present invention, a ferrite core with high magnetic permeability and a ferrite core which also has high magnetic permeability and has a magnetic metal material with high saturation magnetic flux density added to the gap surface are opposed to each other with a gap material in between. As a result, the amount of metal magnetic material formed during the manufacture of the magnetic head can be kept to a minimum, thereby reducing manufacturing costs and device costs.
第1図はこの発明の一実施例による磁気ヘッドの構成図
と要部の拡大図、第2図は磁気ヘッドの記録、再生過程
の説明図、第3図および第4図は従来のタイプの異なる
磁気ヘッドの構成図である。
1・・・高飽和磁束密度の金属磁性体、2・・・ギャッ
プ材、3・・・フェライトコア。
なお、図中同一符号は同−又は相当部分を示す。
代理人 大 岩 増 雄
第2図
第1
第3
第4図Fig. 1 is a block diagram and an enlarged view of the main parts of a magnetic head according to an embodiment of the present invention, Fig. 2 is an explanatory diagram of the recording and reproducing process of the magnetic head, and Figs. 3 and 4 are of a conventional type. FIG. 3 is a configuration diagram of a different magnetic head. 1... Metal magnetic material with high saturation magnetic flux density, 2... Gap material, 3... Ferrite core. Note that the same reference numerals in the figures indicate the same or equivalent parts. Agent Masuo Oiwa Figure 2 Figure 1 Figure 3 Figure 4
Claims (1)
率フェライトからなり、そのギャップ面に相当する面に
これより飽和磁束密度の高い金属磁性体を付加した磁気
コアとを有し、両磁気コアはそれらの間にギャップ材を
挟んで対向させ、上記磁気コアに信号の記録、再生を行
なう巻線コイルを備えたことを特徴とする磁気ヘッド。It has a magnetic core made of high magnetic permeability ferrite, and a magnetic core made of high magnetic permeability ferrite, with a magnetic metal material having a higher saturation magnetic flux density added to the surface corresponding to the gap surface. A magnetic head comprising a wire-wound coil which is opposed to each other with a gap material interposed therebetween and which records and reproduces signals on the magnetic core.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4063089A JPH02220209A (en) | 1989-02-20 | 1989-02-20 | Magnetic head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4063089A JPH02220209A (en) | 1989-02-20 | 1989-02-20 | Magnetic head |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02220209A true JPH02220209A (en) | 1990-09-03 |
Family
ID=12585867
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4063089A Pending JPH02220209A (en) | 1989-02-20 | 1989-02-20 | Magnetic head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02220209A (en) |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58105422A (en) * | 1981-12-17 | 1983-06-23 | Sony Corp | Magnetic head |
| JPS60209906A (en) * | 1984-04-02 | 1985-10-22 | Nec Corp | Ring head for vertical magnetic recording |
| JPS62223807A (en) * | 1986-03-25 | 1987-10-01 | Hitachi Metals Ltd | Composite magnetic head |
| JPH01124106A (en) * | 1987-11-06 | 1989-05-17 | Sharp Corp | Core for magnetic head |
-
1989
- 1989-02-20 JP JP4063089A patent/JPH02220209A/en active Pending
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58105422A (en) * | 1981-12-17 | 1983-06-23 | Sony Corp | Magnetic head |
| JPS60209906A (en) * | 1984-04-02 | 1985-10-22 | Nec Corp | Ring head for vertical magnetic recording |
| JPS62223807A (en) * | 1986-03-25 | 1987-10-01 | Hitachi Metals Ltd | Composite magnetic head |
| JPH01124106A (en) * | 1987-11-06 | 1989-05-17 | Sharp Corp | Core for magnetic head |
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