JPS60202502A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPS60202502A JPS60202502A JP5837684A JP5837684A JPS60202502A JP S60202502 A JPS60202502 A JP S60202502A JP 5837684 A JP5837684 A JP 5837684A JP 5837684 A JP5837684 A JP 5837684A JP S60202502 A JPS60202502 A JP S60202502A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic head
- magnetic
- permeability
- gap
- alloy film
- 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
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
- G11B5/127—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
Description
【発明の詳細な説明】 〔技術分野〕 この発明は、磁気ヘッドに関するものである。[Detailed description of the invention] 〔Technical field〕 The present invention relates to a magnetic head.
磁気ヘッドの再生時の出力特性の1つにフンター効果に
よる出力のうねりがあるが、これを引き起こす要因は、
磁気ヘッドのコア幅りと波長λによるもので、その一般
式状、
で表わされる。第1図は(11式による計算結果を示し
た亀のであシ、第2図祉そのときの磁気ヘッドh1と磁
気記録媒体tの関係を模式的に示したものである。One of the output characteristics of a magnetic head during playback is output undulation due to the Hunter effect, and the factors that cause this are:
It depends on the core width of the magnetic head and the wavelength λ, and is expressed by the general formula: FIG. 1 shows the results of calculations using Equation 11, and FIG. 2 schematically shows the relationship between the magnetic head h1 and the magnetic recording medium t at that time.
このよう表関係から、従来のバルク状磁気コアに対して
捲線を施したタイプ(以下バルク捲線型)の磁気ヘッド
であれば、例えば、第4図(イ)の磁気ヘッドh、の磁
気記録媒体との摺接面の背部を45度の角度をもってカ
ットして、同図(ロ)の磁気ヘッドh、のように摺接面
の形状を改善すれば、コンタ−効果による影響を軽減す
ることができる。第3図はこれを比較例とともに示した
ものである。From this table relationship, if it is a conventional magnetic head of the type in which a bulk magnetic core is wound (hereinafter referred to as bulk-wound type), for example, the magnetic recording medium of magnetic head h in FIG. The influence of the contour effect can be reduced by cutting the back part of the sliding contact surface at a 45 degree angle and improving the shape of the sliding contact surface as shown in the magnetic head h shown in Figure (b). can. FIG. 3 shows this together with a comparative example.
すなわち、第3図におけるカーブD1とカーブD、は、
それぞれ第4図(イ)の磁気ヘッドh、で、コア幅りが
6m++のものと、同図(ロ)の磁気ヘッドh。That is, curve D1 and curve D in FIG.
The magnetic head h shown in FIG. 4(a) has a core width of 6 m++, and the magnetic head h shown in FIG. 4(b).
で、両肩部を45変にカットしてコア幅りを3■とした
ものについてのコンタ−効果を比較したものである。こ
れから明らかなように、磁気記録媒体がギャップから遠
ざかるにつれて、磁気ヘッドから除々に離れるようにす
れば、第3図のようにフンター効果による出力のうねり
の振幅を小さくすることができる。This is a comparison of the contour effect when both shoulders are cut at 45 degrees and the core width is 3 mm. As is clear from this, by making the magnetic recording medium gradually move away from the magnetic head as it moves away from the gap, the amplitude of the output undulation due to the Hunter effect can be reduced as shown in FIG.
こうした事実から、従来は磁気ヘッドのテープとの摺動
面形状をどのように変えれば、コンタ−効果による影響
を少なくできるか、を検討することが必要であった。バ
ルク捲線型の磁気ヘッドに於いて、磁気ヘッドのテープ
との摺接面に面取りを施すことによシコンヨー効果によ
る影響の改善をはかつているのは、このような検討の結
果によるものである。Based on these facts, it has been necessary to consider how to change the shape of the sliding surface of the magnetic head with the tape in order to reduce the influence of the contour effect. It is as a result of such studies that in bulk-wound magnetic heads, the influence of the shikon-yaw effect is improved by chamfering the sliding surface of the magnetic head with the tape.
ところが、第5図に示すような高透磁率磁性合金膜2,
2′を形成した一対の非磁性基板1.1′を、向合金膜
2.2′の間にギャップ材3を設けて有機または無機接
着剤で接着して形成した磁気ヘッドにあっては、磁性合
金膜2,2′が極めて薄いため、上述した従来技術では
コンタ−効果の影響による出力のうねりの振幅を小さく
するととができないという問題があった。なお、4は巻
線である。However, the high permeability magnetic alloy film 2 as shown in FIG.
In a magnetic head formed by bonding a pair of non-magnetic substrates 1.1' with a metal alloy film 2' formed thereon with an organic or inorganic adhesive with a gap material 3 provided between the opposing alloy film 2.2', Since the magnetic alloy films 2 and 2' are extremely thin, the above-mentioned prior art has a problem in that it is not possible to reduce the amplitude of output waviness due to the influence of the contour effect. Note that 4 is a winding wire.
すなわち、第5図に示す磁気ヘッドは、ギャップ3を挟
んだ合金膜2,2′部分(以下コアという。)の厚さD
が極めて小さいため、つt、b磁気記録媒体であるテー
プとの摺接面の長さが極めて小さいため、この部分に面
取シを施しても、コア形状は微視的に見掛は上平坦であ
シ、コンタ−効果による影響の改善ははとんど期待でき
ない、といの問題があった、
そこで、このような問題を解決するために、例えば次の
ような手法が採られている。この手法線従来技術による
手法の延長線上のものである。That is, in the magnetic head shown in FIG.
Since the length of the sliding contact surface with the tape, which is a magnetic recording medium, is extremely small, even if this part is chamfered, the core shape will not look microscopically good. There was a problem that the contour effect could hardly be expected to be improved due to the flat surface.Therefore, in order to solve this problem, the following methods have been adopted, for example. . This method is an extension of the prior art method.
(1)、磁気ヘッドのテープとの摺接面に於けるコアの
厚さDを大きくシ、このテープ摺接面とテープ間の間隔
がギャップから遠ざかるにつれて除々に大きくなるよう
な形状にする。(1) The thickness D of the core at the sliding surface of the magnetic head with the tape is increased, and the distance between the tape sliding surface and the tape gradually increases as the distance from the gap increases.
(2)、第6図(第5図と同−表いし相当部分には同符
号が付しである。)に示すように、磁気ヘッドの上記コ
アの肩部をカットして鋭角状とし、そのカット面を非磁
性金属5,5′で覆い、コアが見掛は上テープから除々
に離れるようにする。(2) As shown in FIG. 6 (same representation as in FIG. 5, and corresponding parts are given the same reference numerals), the shoulder of the core of the magnetic head is cut to form an acute angle, The cut surface is covered with non-magnetic metals 5 and 5' so that the core appears to gradually separate from the upper tape.
しかし、(1)の場合は、蒸着またはスパッタ等で成膜
してコア厚りを少なくとも1w以上にしなければならな
いが、膜はがれ等が生じて事実上不可能である。(2;
の場合は、数μ割しかたいコアをカットしたカット面に
非磁性金属5,5′を貼シ合わせるさい、コアのテープ
との摺接面を僅かに露出させるように施す必要がある。However, in the case of (1), it is necessary to make the core thickness at least 1 W by forming a film by vapor deposition or sputtering, but this is practically impossible because film peeling occurs. (2;
In this case, when pasting the non-magnetic metals 5 and 5' onto the cut surface of a core that is only a few microns thick, it is necessary to slightly expose the sliding surface of the core with the tape.
このため、作業に正確性が要求され、精度の均一なもの
を安定して製造することが困難である0したがって、歩
留シが悪く、量産性に欠ける。For this reason, precision is required in the work, and it is difficult to stably manufacture products with uniform precision.Therefore, the yield is poor and mass productivity is lacking.
この発明は、このような従来の問題点を解決するために
なされたもので、コンタ−効果による影響を軽減できる
だけでなく、製造容易であり、かつ安価で信頼性の高い
磁気ヘッドを提供するものである。This invention was made to solve these conventional problems, and provides a magnetic head that not only can reduce the influence of the contour effect, but also is easy to manufacture, inexpensive, and highly reliable. It is.
以下、この発明の実施例を第7図によって説明する。 Hereinafter, an embodiment of the present invention will be described with reference to FIG.
図において、第5図と同符号は同一ないし相当部分を示
す。7,7′及び8,8′は磁性合金膜2.2′と基板
1,1′との間に積層した他の磁性合金膜である。後者
8,8′は前者7,7′よシ透磁率の大きい層にしてあ
って、この透磁率の大きい方の合金膜層8,8′が透磁
率の小さい方の合金膜層7.T′より外側、つまりギャ
ップ3側へ積層しである。In the figure, the same reference numerals as in FIG. 5 indicate the same or corresponding parts. 7, 7' and 8, 8' are other magnetic alloy films laminated between the magnetic alloy film 2.2' and the substrates 1, 1'. The latter 8, 8' are layers with higher magnetic permeability than the former 7, 7', and the alloy film layers 8, 8' with higher magnetic permeability are the alloy film layers 7, 8' with lower magnetic permeability. It is laminated on the outside of T', that is, on the gap 3 side.
このような構成の磁気ヘッドについて、コンタ−効果に
よる出方のうねシを示したものが第8図であり、これと
比較するために示したのが第9図の従来の磁気ヘッド(
第1図)におけるそれである。両図から、明らかなよう
に、この発明の磁気ヘッドによれば、コンタ−効果によ
る影響を大きく改善し得ることが判る。これは、磁気ヘ
ッドのコア部分の近傍に、さらに2ケの磁気回路が形成
され、これがコア部分に従来のいわゆるカット面を入れ
たのと実質的に同じ効果をもたらすためと考えられる。Figure 8 shows the ridges of the magnetic head with such a configuration due to the contour effect, and for comparison, Figure 9 shows the conventional magnetic head (Figure 9).
This is the case in Figure 1). As is clear from both figures, according to the magnetic head of the present invention, it is possible to greatly improve the influence of the contour effect. This is thought to be because two more magnetic circuits are formed near the core portion of the magnetic head, which produces substantially the same effect as when a conventional so-called cut surface is provided in the core portion.
また、この磁気ヘッドの場合は、各合金膜T。In addition, in the case of this magnetic head, each alloy film T.
7’、8.8’を形成するだけで、格別の加工技術を要
せず簡単に製造できるので、造シ易く、コストもか\ら
ない。しかも、従来のように、特殊の加工を施す必要が
ないので、製品としての信頼性が向上する。Since it can be easily manufactured by simply forming 7' and 8.8' without requiring special processing techniques, it is easy to manufacture and inexpensive. Moreover, unlike conventional products, there is no need for special processing, which improves the reliability of the product.
なお、上記実施例は、その他の磁性合金膜7゜8を2層
設けた場合の例であるが、単層3層、4層と層数はいく
つでも構わない。この場合、各層は、それらの透磁率が
基板側からギャップ側へ順次大きくなるように積層する
ことは言うまでもない。得られる作用効果は、上記実施
例の場合と同様である。Although the above embodiment is an example in which two layers of other magnetic alloy films 7.8 are provided, the number of layers may be any number, such as three or four single layers. In this case, it goes without saying that the layers are stacked such that their magnetic permeability increases sequentially from the substrate side to the gap side. The obtained effects are the same as in the above embodiment.
以上説明したように、この発明によれば、従来の磁気ヘ
ッドにおける基板と磁性合金膜との間に、さらに他の磁
性合金膜を積層し、かつそれら各層を、それらの透磁率
が基板側からギャップ側へ順次大きくなるように積層し
たから、フンター効果による出力のうねりを軽減できる
だけでなく、製造容易で、かつ安価であり、しかも信頼
性の高い磁気ヘッドを提供することができる。As explained above, according to the present invention, another magnetic alloy film is further laminated between the substrate and the magnetic alloy film in a conventional magnetic head, and the magnetic permeability of each layer is different from the substrate side. Since the layers are stacked so as to increase in size toward the gap side, it is possible not only to reduce output fluctuations caused by the Hunter effect, but also to provide a magnetic head that is easy to manufacture, inexpensive, and highly reliable.
第1図は従来のバルク捲線型の磁気ヘッドのコンタ−効
果による出力の計算値を示すグラフ、第2図は第1図の
計算における磁気ヘッドの幅と磁気記録媒体との関係を
模式的に示した図、第3図は従来のバルク捲線型の磁気
ヘッドと、その形状に改善を加えた磁気ヘッドとのコン
タ−効果による出力を比較をしたグラフ、第4図(イ)
は第3図における従来の磁気ヘッド、同図(→は第3図
における形状を改善した磁気ヘッドを示す正面図、第5
図は従来の磁性合金薄膜を設けた磁気ヘッドの側面図、
第6図は第5図の磁気ヘッドを従来技術で改良した磁気
ヘッドの側面図、第7図はこの発明による磁気ヘッドの
側面図、第8図は第7図の磁気ヘッドにおけるコンタ−
効果による出力を示すグラフ、第9図は第5図の従来の
磁気ヘッドのコンタ−効果による出力を示すグラフであ
る。
1・・・・・・基 板
2 ・・・・・・ 磁性合金薄膜
3 ・・・・・・ ギャップ
7、B ・・・ 他の磁性合金薄膜
第1図
一牧
第2図
−判
第3図
第4図
(イ) (ロ)
第5図Figure 1 is a graph showing the calculated value of the output due to the contour effect of a conventional bulk-wound magnetic head, and Figure 2 schematically shows the relationship between the width of the magnetic head and the magnetic recording medium in the calculation of Figure 1. The figure shown in Figure 3 is a graph comparing the output due to the contour effect between a conventional bulk-wound magnetic head and a magnetic head whose shape has been improved, and Figure 4 (A).
3 is a conventional magnetic head, the same figure (→ is a front view showing a magnetic head with an improved shape in FIG. 3, and 5.
The figure shows a side view of a magnetic head equipped with a conventional magnetic alloy thin film.
6 is a side view of a magnetic head that is an improved version of the magnetic head shown in FIG. 5 using conventional technology, FIG. 7 is a side view of a magnetic head according to the present invention, and FIG.
Graph showing the output due to the effect. FIG. 9 is a graph showing the output due to the contour effect of the conventional magnetic head of FIG. 1... Substrate 2... Magnetic alloy thin film 3... Gap 7, B... Other magnetic alloy thin film Figure 1 Ichimaki Figure 2 - Size 3 Figure 4 (a) (b) Figure 5
Claims (1)
両会金膜をギャップ材を介して接合して成る磁気ヘッド
において、前記一対の基板と磁性合金膜との間に、さら
に他の磁性合金膜を、それら各膜の透磁率が基板側から
ギャップ側へ順次大きくなるように夫々積層した仁とを
特徴とする磁気ヘッド。 (2)基板を、非磁性基板とした特許請求の範囲第1項
記載の磁気ヘッド。[Claims] (11) A magnetic head comprising a pair of substrates each having a magnetic alloy film provided on the 11-plane, and a metal film bonded between the two substrates through a gap material, wherein the pair of substrates and the magnetic alloy film are (2) The substrate is made of a non-magnetic material. A magnetic head according to claim 1, which is used as a substrate.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5837684A JPS60202502A (en) | 1984-03-28 | 1984-03-28 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5837684A JPS60202502A (en) | 1984-03-28 | 1984-03-28 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS60202502A true JPS60202502A (en) | 1985-10-14 |
Family
ID=13082603
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5837684A Pending JPS60202502A (en) | 1984-03-28 | 1984-03-28 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS60202502A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4764832A (en) * | 1986-05-21 | 1988-08-16 | U.S. Philips Corporation | Magnetic transducing head having clad core faces |
US5157570A (en) * | 1990-06-29 | 1992-10-20 | Digital Equipment Corporation | Magnetic pole configuration for high density thin film recording head |
US5325254A (en) * | 1991-12-18 | 1994-06-28 | Hewlett-Packard Company | Thin film inductive transducer having improved yoke and pole tip structure |
-
1984
- 1984-03-28 JP JP5837684A patent/JPS60202502A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4764832A (en) * | 1986-05-21 | 1988-08-16 | U.S. Philips Corporation | Magnetic transducing head having clad core faces |
US5157570A (en) * | 1990-06-29 | 1992-10-20 | Digital Equipment Corporation | Magnetic pole configuration for high density thin film recording head |
US5325254A (en) * | 1991-12-18 | 1994-06-28 | Hewlett-Packard Company | Thin film inductive transducer having improved yoke and pole tip structure |
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