JPS58169318A - Magnetic head and its manufacture - Google Patents
Magnetic head and its manufactureInfo
- Publication number
- JPS58169318A JPS58169318A JP5012182A JP5012182A JPS58169318A JP S58169318 A JPS58169318 A JP S58169318A JP 5012182 A JP5012182 A JP 5012182A JP 5012182 A JP5012182 A JP 5012182A JP S58169318 A JPS58169318 A JP S58169318A
- Authority
- JP
- Japan
- Prior art keywords
- rectangular parallelepiped
- gap
- magnetic head
- groove
- substantially rectangular
- 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
- 238000004519 manufacturing process Methods 0.000 title claims description 11
- 125000006850 spacer group Chemical group 0.000 claims abstract description 19
- 239000000463 material Substances 0.000 claims abstract description 12
- 239000000853 adhesive Substances 0.000 claims abstract description 11
- 230000001070 adhesive effect Effects 0.000 claims abstract description 11
- 238000004804 winding Methods 0.000 claims abstract description 5
- 239000000696 magnetic material Substances 0.000 claims description 18
- 238000009792 diffusion process Methods 0.000 claims description 8
- 238000005520 cutting process Methods 0.000 claims description 4
- 239000011521 glass Substances 0.000 abstract description 26
- 239000010409 thin film Substances 0.000 abstract description 19
- 238000002844 melting Methods 0.000 abstract description 6
- 229910000859 α-Fe Inorganic materials 0.000 abstract description 6
- 230000008018 melting Effects 0.000 abstract description 4
- 239000011195 cermet Substances 0.000 abstract description 2
- 239000000758 substrate Substances 0.000 abstract 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 3
- CPLXHLVBOLITMK-UHFFFAOYSA-N Magnesium oxide Chemical compound [Mg]=O CPLXHLVBOLITMK-UHFFFAOYSA-N 0.000 description 2
- GWEVSGVZZGPLCZ-UHFFFAOYSA-N Titan oxide Chemical compound O=[Ti]=O GWEVSGVZZGPLCZ-UHFFFAOYSA-N 0.000 description 2
- 239000002131 composite material Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 238000005498 polishing Methods 0.000 description 2
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 1
- 238000005299 abrasion Methods 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 230000006835 compression Effects 0.000 description 1
- 238000007906 compression Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 239000010432 diamond Substances 0.000 description 1
- 229910003460 diamond Inorganic materials 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000010408 film Substances 0.000 description 1
- 239000000395 magnesium oxide Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 238000007517 polishing process Methods 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
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
- G11B5/1272—Assembling or shaping of elements
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は磁気ヘッド及びその製造法に係り、コア半休同
士を接着剤によって接合した磁気ヘッドにおいて、磁気
ヘッドのギャップ部をコア半休同士の接着剤と接着時に
相互拡散現象の起きにくい非磁性材で構成することによ
り、ギャップ寸法、特にギャップ幅の精度が極めて高い
ものとなり、又磁気へラドコアの磁気特性が低下しない
ものとなり、さらには製造歩留りが著しく向上したもの
となる磁気ヘッド及びその製造法を提供することを目的
とする。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic head and a method for manufacturing the same, and relates to a magnetic head in which core half-holes are bonded to each other with an adhesive, in which a mutual diffusion phenomenon occurs when the gap portion of the magnetic head is bonded to the adhesive between the core half-holes. By using a non-magnetic material that is difficult to cause, the accuracy of the gap dimensions, especially the gap width, is extremely high, and the magnetic properties of the magnetic helad core are not deteriorated, and the manufacturing yield is significantly improved. The purpose of the present invention is to provide a magnetic head and a method for manufacturing the same.
従来、例えば高密度記録ビデオテープレコーダ用の磁気
ヘッドは、その磁性材として単結晶フェライト又は多結
晶フェライト等を用い、ギャップスペーサにギャップ幅
を規定する高軟化点の石英ガラスを用い、コア半休同士
を接合する為に後部ギャップ部に低融点ガラスの薄膜を
形成し、加熱圧着してコア半休同士を接合したものであ
る。そして、狭トラツク化の為に、トラック幅を規定す
る凹部にガラスを熔融充填している。この為、凹部にガ
ラス電充填すると共に低融点ガラスで構成された後部を
熔融接合する為に加熱すると、凸部に充填したガラスと
ギャップスペーサとして用いた石英ガラスとの間で相互
に拡散する現象が生じ、ギャップスペーサが本来の石英
ガラス質とは異なった低融点の混合ガラスに変質し、コ
ア半休同士の圧着度によってギャップ幅が微妙に変動し
、ギャップ幅の寸法が正確に決められず、ギャップ幅の
精度向上が図りにくく、又磁気ヘッドの特性が低下した
ものとなる。さらには、均一なギャップ幅のものが出来
にくいので、製造歩留りも悪い。Conventionally, magnetic heads for high-density recording video tape recorders, for example, have used single-crystal ferrite or polycrystalline ferrite as the magnetic material, used quartz glass with a high softening point to define the gap width for the gap spacer, and placed the cores half-half apart. A thin film of low-melting glass is formed in the rear gap, and the core halves are joined together by heat and pressure bonding. In order to narrow the track, the recesses that define the track width are melted and filled with glass. For this reason, when the concave part is filled with glass and the rear part made of low-melting point glass is heated to melt and bond, a phenomenon occurs in which the glass filled in the convex part and the quartz glass used as a gap spacer mutually diffuse. As a result, the gap spacer changes into a mixed glass with a low melting point different from the original silica glass, and the gap width varies slightly depending on the degree of compression between the half-core cores, making it impossible to determine the gap width accurately. It is difficult to improve the accuracy of the gap width, and the characteristics of the magnetic head deteriorate. Furthermore, since it is difficult to produce a material with a uniform gap width, the manufacturing yield is also poor.
又1.フエライト等のコア半休とギャップスペーサの混
合ガラスとの間で、加熱圧着時に相互拡散現象が生じ、
ギャップ部近傍のフェライト等の磁気特性が低下したも
のとなる。Also 1. A mutual diffusion phenomenon occurs between the core semicircular material such as ferrite and the mixed glass of the gap spacer during heat and pressure bonding.
The magnetic properties of ferrite and the like near the gap are degraded.
本発明は上記欠点を除去したものであり、以下その実施
例について説明する。The present invention eliminates the above-mentioned drawbacks, and examples thereof will be described below.
第1図〜第6図は、本発明に係る磁気ヘッド製造工程説
明図である。1 to 6 are explanatory diagrams of the manufacturing process of the magnetic head according to the present invention.
まず、第1図に示す如く、例えばMn−Znフェライト
等の高透磁率磁性材料を切断研削して直方体ブロック1
を形成し、この直方体ブロック1の上面を鏡面研磨した
後、この鏡面研磨面とテープ走行面側の面の角に切り欠
きとなる溝2を長手方向に沿って形成し、又、この溝2
と略平行に巻線用の窓となる溝3を研削加工して形成す
る。又、直方体ブロック1の溝2,3に対して直交方向
に一定間隔毎に複数個の凹部4を溝2,3につながるよ
う薄肉のダイヤモンドブレードを使用したダイシングソ
ー等で形成する。尚、この凹部4の形状は、その深さが
直方体ブロックの端部、すなわち溝2側の部分が深く、
溝3側の部分が浅くなるようテーパー状に形成されてお
り、又、その幅ははぼ一定のものである。First, as shown in FIG.
After mirror-polishing the upper surface of this rectangular parallelepiped block 1, a groove 2 serving as a notch is formed along the longitudinal direction at the corner of this mirror-polished surface and the surface on the tape running surface side.
A groove 3, which will serve as a winding window, is formed by grinding substantially parallel to the groove 3. Further, a plurality of recesses 4 are formed at regular intervals in a direction orthogonal to the grooves 2 and 3 of the rectangular parallelepiped block 1 so as to connect to the grooves 2 and 3 using a dicing saw or the like using a thin diamond blade. Note that the shape of this recess 4 is such that its depth is deep at the end of the rectangular parallelepiped block, that is, the part on the groove 2 side.
It is formed in a tapered shape so that the portion on the groove 3 side is shallower, and its width is approximately constant.
又、第2図に示す如く、例えばMn−Znフェライト等
の高透磁率磁性材料を切断研削して直方体ブロック1と
同形状の直方体ブロック5を形成し、この直方体ブロッ
ク5の上面を鏡面研磨した後、直方体ブロック1の溝2
と同様な溝6を形成し、又直方体ブロック1の凹部4と
同様な凹部7を形成する。Further, as shown in FIG. 2, a rectangular parallelepiped block 5 having the same shape as the rectangular parallelepiped block 1 was formed by cutting and grinding a high permeability magnetic material such as Mn-Zn ferrite, and the upper surface of this rectangular parallelepiped block 5 was mirror-polished. Back, groove 2 of rectangular parallelepiped block 1
A groove 6 similar to the above is formed, and a recess 7 similar to the recess 4 of the rectangular parallelepiped block 1 is formed.
次に、第3図に示す如く、例えば直方体ブロック1の上
面の凹部4間の平担面に、ギャップスペーサとなる、例
えば8i0−Or等のサーメット、クロム金属、8i0
等のカーノ(イド系化合物、混合酸化物のマグネシア、
アルミナ、チタニア等のガラス質以外の比較的高融点で
高硬度の非磁性材料でスパッタリング等によって磁気ヘ
ッドのギャップ幅となる厚さgの薄膜層8を形成する。Next, as shown in FIG. 3, a gap spacer such as a cermet such as 8i0-Or, chromium metal, 8i0
etc. (ideal compounds, mixed oxide magnesia, etc.)
A thin film layer 8 having a thickness g corresponding to the gap width of the magnetic head is formed by sputtering or the like using a non-magnetic material with a relatively high melting point and high hardness other than glass such as alumina or titania.
又、溝3を境に薄膜層8を形成した平担面と反対側の直
方体ブロック1の上面の平担面に、厚さがg以下の低軟
化点のガラス薄膜層9をスノ(ツタリング等によって形
成する。伺、このガラス薄膜層9は、直方体ブロック1
と直方体ブロック5とを接合する接着剤としての役割を
もつものでもある。Further, on the flat surface of the upper surface of the rectangular parallelepiped block 1, which is opposite to the flat surface on which the thin film layer 8 is formed with the groove 3 as a boundary, a glass thin film layer 9 having a thickness of g or less and having a low softening point is applied by slatting, etc. This glass thin film layer 9 is formed by a rectangular parallelepiped block 1.
It also has the role of an adhesive for bonding the rectangular parallelepiped block 5 and the rectangular parallelepiped block 5 together.
そして、上記第2図及び第3図のように構成された直方
体ブロック1と5とを、各直方体ブロックに形成されて
いる凹部4と7とが正確に一致するよう突き合わせ、第
4図に示す如く、これら突き合わされた直方体ブロック
1と5との溝2と6とによって構成される溝に、ガラス
薄膜層9の低軟化点ガラスの軟化点より例えば約100
℃位高い比較的低軟化点の棒状ガラス10を配し、直方
体ブロックの両側から矢印方向に加圧しながら不活性ガ
ス中で棒状ガラス10の作業点付近の温度に加熱する。Then, the rectangular parallelepiped blocks 1 and 5 configured as shown in FIG. 2 and FIG. As shown in FIG.
A rod-shaped glass 10 having a relatively low softening point, which is about .degree.
そうすると、棒状ガラス10が、溝2と6とによって構
成される溝に充填すると共に、凹部4と7とによって構
成さ、れる空隙部にも充填してゆき、この軟化充填した
ガラスによって直方体ブロック1と5とは接着されると
共に、軟化したガラス薄膜層9によっても直方体ブロッ
ク1と5とが接着されるようになる。Then, the rod-shaped glass 10 fills the groove formed by the grooves 2 and 6, and also fills the gap formed by the recesses 4 and 7, and this softened and filled glass fills the rectangular parallelepiped block 1. and 5 are bonded together, and the rectangular parallelepiped blocks 1 and 5 are also bonded together by the softened glass thin film layer 9.
この直方体ブロック1と5との加熱圧着時には、棒状ガ
ラス10が軟化して凹部4と7とによって構成される空
隙部に流れ込んでゆくのであるが、この比較的低軟化点
の軟化したガラスによって薄膜層8は侵されず、薄膜層
8とガラスとの間には相互拡散現象はなく1例えば薄膜
層8の厚さが変化してギャップ幅が薄膜層形成時の厚さ
gからずれてしまうものとなるといった悪影響は起きず
、ギャップ寸法を高精度に形成できるものである。又、
直方体ブロックと薄膜層との接合面部において、ギャッ
プスペーサ材として非ガラス質の高融点非磁性材を用い
たので、ギャップ近傍の磁性材が侵されず、磁気特性を
劣下させるようなこともない。When the rectangular parallelepiped blocks 1 and 5 are bonded together under heat and pressure, the rod-shaped glass 10 softens and flows into the gap formed by the recesses 4 and 7, and this softened glass with a relatively low softening point forms a thin film. The layer 8 is not attacked, and there is no interdiffusion phenomenon between the thin film layer 8 and the glass.1For example, the thickness of the thin film layer 8 changes and the gap width deviates from the thickness g when the thin film layer was formed. The gap dimension can be formed with high precision without causing any adverse effects such as. or,
Since a non-vitreous high melting point non-magnetic material is used as the gap spacer material at the joint surface between the rectangular parallelepiped block and the thin film layer, the magnetic material near the gap will not be attacked and the magnetic properties will not deteriorate. .
次に、ガラスによって接合された直方体ブロック1と5
との複合ブロック11を、第5図に示す如く、一点鎖線
及び二点鎖線で示す仮想面で切断し。Next, rectangular parallelepiped blocks 1 and 5 joined by glass
As shown in FIG. 5, the composite block 11 is cut along an imaginary plane shown by a dashed line and a dashed double dotted line.
その後所定の切削研磨加工を施して第6図に示すような
磁気ヘッド12を構成する。伺、第6図中、13.14
は、直方体ブロック1と5より形成されたコア半休、1
5は、溝3より形感された巻線用窓、1 16は、薄膜
層8より形成されたギャップスペーサである。Thereafter, a predetermined cutting and polishing process is performed to form the magnetic head 12 as shown in FIG. 13.14 in Figure 6
is a half core formed by rectangular parallelepiped blocks 1 and 5, 1
5 is a winding window formed from the groove 3, and 116 is a gap spacer formed from the thin film layer 8.
上記のように構成された磁気ヘッドは、ギャップ部を、
ギャップ幅を決める部分には比較的高軟化点で非ガラス
質の非磁性材で構成し、ギャップ幅の決定に寄与しない
部分において、すなわち比較的高軟化点で非ガラス質の
非磁性材よりなるギャップスペーサ挟持面以外の部分に
おいて低軟化点のガラス材を用いて磁気へラドコア半休
同士を接合した構成であるので、コア半休同士の接着に
際してあらかじめギャップ幅は決まっており、しかもこ
のギャップ幅には変動が生じないものであるから、極め
て正確にギャップ幅寸法を構成でき、ギャップ寸法の測
定が容易であり、又加熱接着時にギャップスペーサとコ
ア半休との挟持面において相互拡散現象は起きず、ギャ
ップスペーサ接合面付近の磁性材の磁気特性は劣下せず
、磁気ヘッドの例えば高周波特性は優れたものである。In the magnetic head configured as above, the gap portion is
The part that determines the gap width is made of a non-vitreous non-magnetic material with a relatively high softening point, and the part that does not contribute to determining the gap width is made of a non-vitreous non-magnetic material with a relatively high softening point. Since the magnetic herad core halves are bonded together using a glass material with a low softening point in the area other than the gap spacer sandwiching surface, the gap width is predetermined when the core halves are bonded together. Since no fluctuations occur, it is possible to configure the gap width dimension extremely accurately, and measurement of the gap dimension is easy.Also, there is no mutual diffusion phenomenon at the sandwiching surface between the gap spacer and the core half-hole during heat bonding, and the gap width is The magnetic properties of the magnetic material near the spacer joint surface are not degraded, and the magnetic head has excellent high frequency properties, for example.
又、コア半休のギャップスペーサ挟持部の両側に形成さ
れた凹部に充填したガラスとギャップスペーサ材との間
で混合相互拡散が生じることもないので、ギャップスペ
ーサ材の組成が変化することもなく、例えば極めて高精
度なギャップ幅のギャップが構成されるものとなる。In addition, since mixing and mutual diffusion does not occur between the gap spacer material and the glass filled in the recesses formed on both sides of the gap spacer holding portion of the core half-closed, the composition of the gap spacer material does not change. For example, a gap with an extremely high precision gap width can be constructed.
さらに、ギャップスペーサ挾持面においてコア半休同士
が結合されていなくても、ギャップスペーサの両側にお
いて形成された凹部に低軟化点のガラスが充填され強固
に結合されたものであるので、切削研磨加工時に破損し
に<<、製造歩留りは著しく向上したものであり、さら
にはテープ走行時における耐摩耗性にも優れたものであ
る。Furthermore, even if the core half-holes are not bonded to each other on the gap spacer clamping surface, the recesses formed on both sides of the gap spacer are filled with low softening point glass and are firmly bonded, so during cutting and polishing. The production yield has been significantly improved, and the abrasion resistance during tape running is also excellent.
同、上記実施例においては、薄膜層8は直方体ブロック
1のみにしか形成しなかったが、これは直方体ブロック
5にも形成してもよく、このような場合にはそれぞれの
直方体ブロックに形成した薄膜層の厚さの和がギャップ
幅となるようにしておけばよく、又、ガラス薄膜層につ
いても同様である。Similarly, in the above embodiment, the thin film layer 8 was formed only on the rectangular parallelepiped block 1, but it may also be formed on the rectangular parallelepiped block 5, and in such a case, the thin film layer 8 was formed on each rectangular parallelepiped block. The gap width may be the sum of the thicknesses of the thin film layers, and the same applies to the glass thin film layers.
上述の如く、本発明に係る磁気ヘッドは、コア半休同士
を接着剤によって接合した磁気ヘッドにおいて、磁気ヘ
ッドのギャップスペーサ材をコア半休同士を接合する接
着剤と相互拡散現象の生じにくい非磁性材で構成したの
で、ギャップ寸法、特にギャップ幅の寸法精度が極めて
高いものとなり、又磁性材コアの磁気特性の低下もなく
、例えば高周波特性等に優れたものであり、又、本発明
に係る磁気ヘッド製造法は、2個の磁性材の略直方体ブ
ロックのうち少なくとも1個の略直方体ブロックの所定
位置に巻線用窓となる溝を、かつこの溝に対して略直交
方向に所定間隔毎に複数個の略凹部を2個の略直方体ブ
ロックに形成すると共に、少なくとも1個の略直方体ブ
ロックのギャップ形成位置となる所定位置に略直方体ブ
ロック同士の接着時に接着剤と相互拡散現象の生じにく
い非磁性材で所定厚の膜を形成した後、これらの略直方
体ブロックの突き合わせ面同士を向かい合わせて突き合
わせ、その後略直方体ブロック同士の突き合わせ面の空
隙に接着剤を配して略直方体ブロック同士を接合した後
、前記略凹部位置を通る所定の仮想面に沿って接合した
略直方体ブロックを切断して所定形状にするので、高精
度の寸法のギャップの磁気ヘッドを製造歩留りよく低コ
ストで作れ、しかもギャップ形成時にギャップ近傍の磁
性材の磁気特性を劣下させることもなく1例えば高周波
特性等に優れた磁気特性のものが得られ。As described above, in the magnetic head according to the present invention, the gap spacer material of the magnetic head is made of a non-magnetic material that does not easily cause the mutual diffusion phenomenon with the adhesive that joins the core halves. As a result, the dimensional accuracy of the gap dimension, especially the gap width, is extremely high, and there is no deterioration in the magnetic properties of the magnetic material core, for example, it is excellent in high frequency properties, etc., and the magnetic material according to the present invention The head manufacturing method includes forming grooves to serve as winding windows at a predetermined position in at least one of the two substantially rectangular blocks made of magnetic material, and forming grooves at predetermined intervals in a direction substantially orthogonal to the grooves. A plurality of substantially concave portions are formed in two substantially rectangular parallelepiped blocks, and at least one of the substantially rectangular parallelepiped blocks is provided at a predetermined position, which is a gap formation position, with a non-stick material that is unlikely to cause mutual diffusion with the adhesive when the substantially rectangular parallelepiped blocks are bonded together. After forming a film of a predetermined thickness with a magnetic material, the abutting surfaces of these approximately rectangular parallelepiped blocks are butted against each other, and then an adhesive is placed in the gap between the abutting surfaces of the approximately rectangular parallelepiped blocks to join the approximately rectangular parallelepiped blocks together. After that, the joined substantially rectangular parallelepiped blocks are cut into a predetermined shape along a predetermined virtual plane passing through the substantially concave portion position, so that a magnetic head with a gap of highly accurate dimensions can be manufactured at a high manufacturing yield and at low cost. When the gap is formed, magnetic properties of the magnetic material near the gap are not deteriorated, and magnetic properties excellent in, for example, high frequency properties can be obtained.
又耐摩耗性に優れたものが得られる等の特長を有する。It also has the advantage of being able to provide products with excellent wear resistance.
第1図〜第6図は、本発明に係る磁気ヘッドの製造工程
説明図である。
1.5・・・直方体ブロック、2.3.6・・・溝、4
.7・・・凹部、8・・・薄膜層、9・・・ガラス薄膜
層、10・・・棒状ガラス、11・・・複合ブロック、
12・・・磁気ヘッド、13.14・・・コア半休、1
6・・・ギャップスゝ−サ。
特許出願人 日本ビクター株式会社
代 理 人 宇 高 克 入侵。
騙。
才I Ll
!
才3I乙
一才!5図
1′2 ゾ
Σ
才6し11 to 6 are explanatory diagrams of the manufacturing process of the magnetic head according to the present invention. 1.5... Rectangular parallelepiped block, 2.3.6... Groove, 4
.. 7... Concave portion, 8... Thin film layer, 9... Glass thin film layer, 10... Rod-shaped glass, 11... Composite block,
12...Magnetic head, 13.14...Core half-off, 1
6...Gap spacer. Patent applicant: Japan Victor Co., Ltd. Agent: Katsu Uko Intrusion. Deception. Talented I Ll! Sai 3 I Otsu Ichi sai! 5 figure 1'2 zo Σ year 6 year 1
Claims (1)
にわいて、磁気ヘッドのギャップスペーサ材をコア半休
同士を接合する接着剤と相互拡散現象の生じにくい非磁
性材で構成したことを特徴とする磁気ヘッド。 ■ 2個の磁性材の略直方体ブロックのうち少なくとも
1個の略直方体ブロックの所定位置に巻線用窓となる溝
を、かつこの溝に対して略直交方向に所定間隔毎に複数
個の略凹部を2個の略直方体ブロックに形成すると共に
、少なくとも1個の略直方体ブロックのギャップ形成位
置となる所定位置に略直方体ブロック同士の接着時に接
着剤と相互拡散現象の生じにくい非磁性材で所定厚の膜
を形成した後、これらの略直方体ブロックの突き合わせ
面同士を向かい合わせて突き合わせ、その後略直方体ブ
ロック同士の突き合わせ面の空隙に接着剤を配して略直
方体ブロック同士を接合した後、前記略凹部位置を通る
所定の仮想面に沿って接合した略直方体ブロックを切断
して所定形状にすることを特徴とする磁気ヘッド製造法
。[Claims] ■ In a magnetic head in which core halves are bonded to each other with an adhesive, the gap spacer material of the magnetic head is made of an adhesive that joins the core halves and a non-magnetic material that is unlikely to cause mutual diffusion. A magnetic head characterized by: ■ A groove serving as a winding window is provided at a predetermined position in at least one of the two substantially rectangular blocks made of magnetic material, and a plurality of grooves are provided at predetermined intervals in a direction substantially orthogonal to the groove. Concave portions are formed in two substantially rectangular parallelepiped blocks, and at least one of the substantially rectangular parallelepiped blocks is formed at a predetermined position where a gap is formed using a non-magnetic material that is unlikely to cause mutual diffusion with adhesive when the substantially rectangular parallelepiped blocks are bonded together. After forming a thick film, the abutting surfaces of these substantially rectangular parallelepiped blocks are faced and butted together, and then an adhesive is placed in the gap between the abutting surfaces of the substantially rectangular parallelepiped blocks to join the substantially rectangular parallelepiped blocks. 1. A method of manufacturing a magnetic head, which comprises cutting a substantially rectangular parallelepiped block joined together along a predetermined imaginary plane passing substantially through a recessed portion position to form a predetermined shape.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5012182A JPS58169318A (en) | 1982-03-30 | 1982-03-30 | Magnetic head and its manufacture |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5012182A JPS58169318A (en) | 1982-03-30 | 1982-03-30 | Magnetic head and its manufacture |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS58169318A true JPS58169318A (en) | 1983-10-05 |
Family
ID=12850284
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5012182A Pending JPS58169318A (en) | 1982-03-30 | 1982-03-30 | Magnetic head and its manufacture |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58169318A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2562304A1 (en) * | 1984-03-29 | 1985-10-04 | Sony Corp | MAGNETIC TRANSDUCER HEAD |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS51141609A (en) * | 1975-06-02 | 1976-12-06 | Hitachi Denshi Ltd | Magnetic head |
JPS55125526A (en) * | 1979-03-22 | 1980-09-27 | Pioneer Electronic Corp | Magnetic head |
JPS5613511A (en) * | 1979-07-11 | 1981-02-09 | Hitachi Denshi Ltd | Magnetic head |
-
1982
- 1982-03-30 JP JP5012182A patent/JPS58169318A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS51141609A (en) * | 1975-06-02 | 1976-12-06 | Hitachi Denshi Ltd | Magnetic head |
JPS55125526A (en) * | 1979-03-22 | 1980-09-27 | Pioneer Electronic Corp | Magnetic head |
JPS5613511A (en) * | 1979-07-11 | 1981-02-09 | Hitachi Denshi Ltd | Magnetic head |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2562304A1 (en) * | 1984-03-29 | 1985-10-04 | Sony Corp | MAGNETIC TRANSDUCER HEAD |
US4819113A (en) * | 1984-03-29 | 1989-04-04 | Sony Corporation | Magnetic transducer head with inclined magnetic gap |
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