JPS6346482B2 - - Google Patents
Info
- Publication number
- JPS6346482B2 JPS6346482B2 JP54151062A JP15106279A JPS6346482B2 JP S6346482 B2 JPS6346482 B2 JP S6346482B2 JP 54151062 A JP54151062 A JP 54151062A JP 15106279 A JP15106279 A JP 15106279A JP S6346482 B2 JPS6346482 B2 JP S6346482B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- block
- core
- atmosphere
- track
- 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
Links
Landscapes
- Magnetic Heads (AREA)
Description
【発明の詳細な説明】
本発明は強磁性体酸化物を磁心とした磁気ヘツ
ドの製造方法に関するものであり、特に記録の高
密度化に伴う磁気ヘツドの狭トラツク化における
加工の際の加工歪を除去し、高性能の狭トラツク
磁気ヘツドの製造方法を提供することを目的とし
たものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing a magnetic head using a ferromagnetic oxide as a magnetic core, and in particular, it relates to a method for manufacturing a magnetic head with a magnetic core made of ferromagnetic oxide. The object of the present invention is to provide a method for manufacturing a high performance narrow track magnetic head.
従来、強磁性体酸化物を磁心とする磁気ヘツド
の製造方法においては、素材を切断、研削して直
方体ブロツクに成形したのち、上記直方体ブロツ
クの長手方向と直交する方向に所定幅のトラツク
を形成すべく一定間隔のノツチ溝を形成し、その
後上記ノツチ溝にガラス等の非磁性充填物を充填
し、空隙形成面を研削、研削した後、所定厚の非
磁性体よりなるスペーサを介して対向コアブロツ
クと突合せ、ガラス等で固定することによりギヤ
ツプドバーを形成する方法が一般的である。上記
一連の工程の中で、トラツク部を形成する溝加工
は砥石加工によるのが一般的である。しかし、最
近の記録密度の向上は著るしく、従つて磁気ヘツ
ドに要求されるトラツク幅は年々小さくなり、現
在では30μm程度のものが実用化されており、更
に将来的にはもつと狭いものが要求されている。
一般にフエライトのような硬脆材料は機械的にも
ろい性質を有しており、研削、切断といつた加工
に対し、その表面層にはかなり深いクラツク層及
び加工変質層を形成し、磁気特性が大きく劣化す
る。第1図にMn−Znフエライトをリング状に切
断した場合の透磁率の周波数特性を示してある
が、リングの厚みを50μmで切断した場合は200μ
mで切断した場合に較べて10MHz以下のほぼ全域
で大きく劣化している。リングの厚みが50μm以
下になれば更に透磁率が劣化することは容易に相
像される。厚みが薄くなればなる程フエライトに
加わる応力大きくなり、クラツクは増長し、表面
の加工変質層による影響が大きくなる。更に一般
に耐摩耗性向上の為、上記ノツチ溝はガラス等で
充填するのが普通であるが、前述のようなクラツ
クの存在及び加工変質層の存在は溶融したガラス
による浸透、浸食を助長し、更にフエライトコア
の磁気特性を劣化させる。又、厚みが厚い場合は
溝加工後のエツチング等の除歪効果が磁気特性回
復の為に有効であるが、厚みが薄くなるとクラツ
クによる浸食が無視できなくなり有効な手段とは
ならなくなる。このように極めて狭トラツクの磁
気ヘツドを製造しようとする場合、現状のフエラ
イト−砥石工という組合せでは性能の良好な磁気
ヘツドを製造する事は困難である。 Conventionally, in the manufacturing method of a magnetic head using a ferromagnetic oxide as a magnetic core, a material is cut and ground to form a rectangular parallelepiped block, and then a track of a predetermined width is formed in a direction perpendicular to the longitudinal direction of the rectangular parallelepiped block. After that, the notched grooves are filled with a non-magnetic filler such as glass, and the gap-forming surfaces are ground and ground, and then the notched grooves are faced with a spacer made of a non-magnetic material of a predetermined thickness interposed therebetween. A common method is to form a gapped bar by butting it against a core block and fixing it with glass or the like. In the above series of steps, the grooves forming the track portions are generally processed by grinding. However, recent improvements in recording density have been remarkable, and the track width required for magnetic heads has become smaller year by year.Currently, track widths of about 30 μm are in practical use, and in the future, track widths of about 30 μm are in practical use. is required.
In general, hard and brittle materials such as ferrite have mechanical brittle properties, and when subjected to processing such as grinding and cutting, they form a fairly deep crack layer and a process-altered layer on their surface layer, which impairs their magnetic properties. Significantly deteriorates. Figure 1 shows the frequency characteristics of magnetic permeability when Mn-Zn ferrite is cut into a ring shape.
Compared to the case of cutting at m, there is a large deterioration in almost the entire range below 10 MHz. It is easy to see that when the thickness of the ring becomes 50 μm or less, the magnetic permeability deteriorates further. As the thickness becomes thinner, the stress applied to the ferrite increases, the cracks increase, and the effect of the processed layer on the surface increases. Furthermore, in order to generally improve wear resistance, the above-mentioned notch grooves are usually filled with glass, etc., but the presence of cracks and the presence of a damaged layer as described above promotes penetration and erosion by molten glass. Furthermore, it deteriorates the magnetic properties of the ferrite core. Further, when the thickness is large, strain removal effects such as etching after groove processing are effective for restoring magnetic properties, but when the thickness becomes thin, erosion due to cracks cannot be ignored and is no longer an effective means. When attempting to manufacture a magnetic head with such a very narrow track, it is difficult to manufacture a magnetic head with good performance using the current combination of ferrite and grindstone.
本発明は上記欠点を除去するものであり、トラ
ツク構成部を再結晶させることにより該トラツク
構成部のマイクロクラツク、加工変質層を消失せ
しめることを特徴とするものである。 The present invention is intended to eliminate the above-mentioned drawbacks, and is characterized by recrystallizing the track component to eliminate microcracks and process-affected layers in the track component.
前述したように第1図においてMn−Znフエラ
イトの透磁率は例えば切断加工においてコアの厚
みが薄くなる程劣化し、更に劣化範囲が高周波域
まで拡大してくる。本発明者の実験によると、
200μm厚の切断リングに対して50μm厚の切断リ
ングの透磁率は低域で約1/4であり、ビデオ周波
数帯域でもかなり劣化している。しかし、この両
者を例えば酸素1%、1100℃で1時間熱処理を施
してやると図中に示したように両者共ほぼバルク
の透磁率状態にまで回復する。参考までに同様の
リングを化学エツチングあるいは700℃程度の熱
焼鈍を施すとある程度の回復はみられるがいずれ
もバルク状態の透磁率までは回復せず、又薄いも
の程回復度合いが少なくなる。このように再結晶
熱処理は加工によつてフエライト内に生じたマイ
クロクラツクや加工変質層を消失しほぼ完全なバ
ルク状態に復帰させるのに極めて有効な方法であ
る。 As mentioned above, in FIG. 1, the magnetic permeability of Mn--Zn ferrite deteriorates as the thickness of the core becomes thinner, for example, during cutting, and the range of deterioration further expands to the high frequency range. According to the inventor's experiments,
The magnetic permeability of a 50 μm thick cutting ring is about 1/4 of that of a 200 μm thick cutting ring in the low range, and is considerably degraded even in the video frequency band. However, when both are subjected to heat treatment at 1100° C. in 1% oxygen for 1 hour, as shown in the figure, both recover to almost the bulk magnetic permeability state. For reference, when a similar ring is subjected to chemical etching or thermal annealing at about 700°C, some recovery can be seen, but neither of these recovers the magnetic permeability to the bulk state, and the thinner the ring, the less the degree of recovery. As described above, recrystallization heat treatment is an extremely effective method for eliminating microcracks and process-altered layers generated in ferrite due to processing and returning the ferrite to an almost perfect bulk state.
以下本発明の一実施例を図面とともに説明す
る。まず強磁性体酸化物の素材を切断研削して直
方体ブロツク1を形成して(第2図a)、次に上
記直方体ブロツクの長手方向と直交する方向に所
定幅のトラツク部を形成すべく一定間隔のノツチ
溝2をダイシング・ソーあるいはワイヤー・ソー
等の手段で形成する(第2図b)。その後、不活
性雰囲気もしくは強磁性体酸化物磁心と炉内雰囲
気の酸素分圧濃度が略平衡状態にある酸化性雰囲
気中で900〜1300℃の範囲で熱処理を施す(第2
図c)。なお第2図cにおいて、3は炉であり、
4は炉心管、5は処理ボートである。再結晶速度
は処理温度に依存することが大きく高温程短時間
で十分再結晶させることができるが、900℃程度
の低温でも処理時間の延長により同様の効果が得
られる。しかし900℃以下になると処理時間の延
長と共にコア形状が大きな凸状に変化するように
なり、又1300℃以上になると逆に大きな凹状に変
化するようになり以降の加工工程で不都合を生じ
るし、又狭トラツクをねらう上で精度が出なくな
る。従つて熱処理温度はコア形状が安定している
900℃〜1300℃の温度範囲が望ましい。又酸素分
圧濃度も大切であり、炉内雰囲気中の酸素分圧濃
度がコアブロツク内の酸素濃度との平衡状態から
大きくずれていると、コアブロツクが酸化あるい
は還元されてかえつて磁気特性が劣化するように
なる。例えば酸素分圧1%、1100℃、1時間保持
するとトラツク部はほぼ完全にバルク状態に再結
晶させられる。また1300℃の場合は酸素分圧1〜
20%、900℃の場合は0.001〜0.1%の範囲が再結
晶に適した雰囲気であるが900℃程度の場合は不
活性雰囲気中でもほぼ同様の効果が得られる。こ
のように温度によつて、最適な酸素分圧濃度は変
わる。すなわちコアブロツク内の酸素分圧濃度と
炉内雰囲気中の酸素分圧濃度が略等しい状態で熱
処理を行なう。その後例えばガラス等の非磁性充
填物6を上記ノツチ溝2に充填し空隙形成面7を
研削、研摩し(第2図d)巻線用溝加工を施した
後所定厚の非磁性ギヤツプスペーサ8を介して対
向ブロツク1′と当接させて加熱、接合しギヤツ
プドバーを形成する(第2図e)。然る後所定の
トラツク位置、コア厚にて切断し、巻線を施して
1ケのヘツドが完成する。 An embodiment of the present invention will be described below with reference to the drawings. First, a ferromagnetic oxide material is cut and ground to form a rectangular parallelepiped block 1 (Fig. 2a), and then a track portion of a predetermined width is formed in a direction perpendicular to the longitudinal direction of the rectangular parallelepiped block. Notch grooves 2 at intervals are formed by a means such as a dicing saw or a wire saw (FIG. 2b). After that, heat treatment is performed in the range of 900 to 1300°C in an inert atmosphere or an oxidizing atmosphere in which the oxygen partial pressure concentration of the ferromagnetic oxide core and the furnace atmosphere are approximately in equilibrium (second stage).
Figure c). In addition, in Fig. 2c, 3 is a furnace;
4 is a furnace tube, and 5 is a processing boat. The recrystallization rate depends on the processing temperature, and the higher the temperature, the more sufficient recrystallization can be achieved in a shorter time, but the same effect can be obtained even at a lower temperature of about 900°C by extending the processing time. However, if the temperature is below 900℃, the core shape will change to a large convex shape as the processing time increases, and if the temperature exceeds 1300℃, it will change to a large concave shape, causing problems in subsequent processing steps. Also, accuracy is lost when aiming at narrow tracks. Therefore, the core shape is stable at the heat treatment temperature.
A temperature range of 900°C to 1300°C is desirable. The oxygen partial pressure concentration is also important; if the oxygen partial pressure concentration in the furnace atmosphere deviates significantly from the equilibrium state with the oxygen concentration in the core block, the core block will be oxidized or reduced, and the magnetic properties will deteriorate. It becomes like this. For example, if the track portion is held at 1100° C. for 1 hour at an oxygen partial pressure of 1%, the track portion is almost completely recrystallized into a bulk state. In addition, in the case of 1300℃, the oxygen partial pressure is 1~
When the temperature is 20% and 900°C, an atmosphere suitable for recrystallization is in the range of 0.001 to 0.1%, but when the temperature is about 900°C, almost the same effect can be obtained even in an inert atmosphere. In this way, the optimal oxygen partial pressure concentration changes depending on the temperature. That is, the heat treatment is performed in a state where the oxygen partial pressure concentration in the core block and the oxygen partial pressure concentration in the atmosphere in the furnace are approximately equal. Thereafter, the notch groove 2 is filled with a non-magnetic filler 6 such as glass, and the gap forming surface 7 is ground and polished (FIG. 2d) to form a winding groove, and then a non-magnetic gear spacer 8 of a predetermined thickness is formed. The gapped bar is formed by contacting the opposed block 1' through the gap and heating and bonding it (FIG. 2e). After that, it is cut at a predetermined track position and core thickness, and a wire is wound to complete one head.
以上のように本発明によれば加工の影響によつ
て磁気特性の劣化した狭トラツク部の磁気特性を
ほぼバルク状態の特性に回復させ、又結晶的にも
マイクロクラツクや加工変質部を消失させる為
に、例えばガラス充填によるコア内部への浸透、
浸食も少なく、高性能及び高精度の狭トラツクヘ
ツドが得られる。 As described above, according to the present invention, the magnetic properties of the narrow track portion where the magnetic properties have deteriorated due to the influence of processing can be restored to almost the properties of the bulk state, and microcracks and processing-altered parts can also be eliminated from the crystallographic perspective. For example, penetration into the core by glass filling,
A narrow track head with low erosion, high performance and high accuracy is obtained.
第1図はMn−Znフエライトの透磁率の周波数
特性を示した図、第2図は本発明による一実施例
の磁気ヘツドの製造工程を示す図である。
1……直方体ブロツク、2……ノツチ溝、7…
…空隙形成面、8……スペーサ。
FIG. 1 is a diagram showing the frequency characteristics of magnetic permeability of Mn--Zn ferrite, and FIG. 2 is a diagram showing the manufacturing process of a magnetic head according to an embodiment of the present invention. 1... Rectangular parallelepiped block, 2... Notch groove, 7...
...Gap forming surface, 8...Spacer.
Claims (1)
し、上記直方体ブロツクの長手方向と直交する方
向にトラツクを形成すべく一定間隔のノツチ溝を
形成した後、不活性雰囲気もしくは強磁性体酸化
物磁心と炉内雰囲気の酸素分圧濃度が略平衡状態
にある酸化性雰囲気中で900〜1300℃で熱処理を
行ない上記ノツチ溝によつて形成されるトラツク
部を再結晶化させ、然る後上記ブロツクの空隙形
成面を研摩し、所定厚の非磁性ギヤツプスペーサ
を介し、対向ブロツクと当接させて接合すること
を特徴とする磁気ヘツドの製造方法。1. After forming notch grooves at regular intervals to form tracks in a direction perpendicular to the longitudinal direction of the rectangular parallelepiped block made of ferromagnetic oxide, the notch grooves are placed in an inert atmosphere or with a ferromagnetic oxide core. Heat treatment is performed at 900 to 1300°C in an oxidizing atmosphere in which the oxygen partial pressure concentration in the furnace atmosphere is in a substantially equilibrium state to recrystallize the track portion formed by the notch groove, and then the block is re-crystallized. 1. A method of manufacturing a magnetic head, which comprises polishing a gap forming surface and joining the head to an opposing block through a non-magnetic gear spacer of a predetermined thickness.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15106279A JPS5674814A (en) | 1979-11-20 | 1979-11-20 | Production of magnetic head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP15106279A JPS5674814A (en) | 1979-11-20 | 1979-11-20 | Production of magnetic head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5674814A JPS5674814A (en) | 1981-06-20 |
| JPS6346482B2 true JPS6346482B2 (en) | 1988-09-16 |
Family
ID=15510460
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP15106279A Granted JPS5674814A (en) | 1979-11-20 | 1979-11-20 | Production of magnetic head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5674814A (en) |
-
1979
- 1979-11-20 JP JP15106279A patent/JPS5674814A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5674814A (en) | 1981-06-20 |
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