JPS62183020A - Magnetic transducer - Google Patents

Magnetic transducer

Info

Publication number
JPS62183020A
JPS62183020A JP2380786A JP2380786A JPS62183020A JP S62183020 A JPS62183020 A JP S62183020A JP 2380786 A JP2380786 A JP 2380786A JP 2380786 A JP2380786 A JP 2380786A JP S62183020 A JPS62183020 A JP S62183020A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic transducer
transducer
magnetic medium
medium
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.)
Granted
Application number
JP2380786A
Other languages
Japanese (ja)
Other versions
JPH06103585B2 (en
Inventor
Yuzo Yamaguchi
雄三 山口
Yoshinori Takeuchi
芳徳 竹内
Mikio Tokuyama
幹夫 徳山
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP61023807A priority Critical patent/JPH06103585B2/en
Publication of JPS62183020A publication Critical patent/JPS62183020A/en
Publication of JPH06103585B2 publication Critical patent/JPH06103585B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Adjustment Of The Magnetic Head Position Track Following On Tapes (AREA)

Abstract

PURPOSE:To make the occurrence of position deviation of a magnetic gap difficult by forming a ratio of a width in parallel with the magnetic medium surface to a height perpendicular to the magnetic medium surface in a projected shape of a magnetic transducer to be >=4. CONSTITUTION:Three rails 1, 2, 3 prolonged in parallel are formed to the magnetic transducer 10 at an interval in the relative moving direction from the magnetic medium and provided with rail faces 1b, 2b, 3b to form an air sliding face with the magnetic medium surface. The profile of the magnetic transducer 10 is made thin and the width (w) in parallel with the surface of the magnetic medium 20 to the height (h) perpendicular to the surface of the magnetic medium 20 in the projected shape of the magnetic transducer viewing the magnetic transducer 10 from a direction where the magnetic medium 20 approaches the magnetic transducer 10 is formed to be 4 or over. Since the profile is made thin, although a slot 6 fitting a support means provided side by side to the access mechanism is shallow, a gimbal is adhered to a bottom face 6a and the function of a support does not differ from that of a conventional system.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、磁気変換器に係り、例えば磁気ディスク装置
の磁気ヘッドなどに用いられる磁気変換器の、特にその
長手方向の中央部にアクセス機構との連接部があり、長
手方向の最後尾に磁気ギャップが設けられているものに
好適な磁気変換器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 transducer, and particularly relates to a magnetic transducer used in a magnetic head of a magnetic disk device, etc., in which an access mechanism is provided in the longitudinal center of the transducer. The present invention relates to a magnetic transducer suitable for a magnetic transducer having a connecting portion with a magnetic transducer and a magnetic gap provided at the rearmost end in the longitudinal direction.

〔従来の技術〕[Conventional technology]

磁気記録においては1例えば磁気ディスクのような磁気
記憶媒体(以下単に磁気媒体という)に磁気変換器の磁
ギャップをできるだけ近付ける一方で、磁気媒体と磁気
変換器との直接接燗を避けるために、特開昭49−12
1514号公報に記載されているような空気ベアリング
を適用した空気浮上方式の磁気変換器が開発されている
In magnetic recording, 1. For example, in order to make the magnetic gap of a magnetic transducer as close as possible to a magnetic storage medium (hereinafter simply referred to as a magnetic medium) such as a magnetic disk, and to avoid direct contact between the magnetic medium and the magnetic transducer, Japanese Unexamined Patent Publication No. 49-12
An air levitation type magnetic transducer using an air bearing as described in Japanese Patent No. 1514 has been developed.

そのような従来の磁気変換器について第2図および第3
図を参照して説明する。
2 and 3 for such conventional magnetic transducers.
This will be explained with reference to the figures.

ここに第2図は、従来の磁気変換器の斜視図。FIG. 2 is a perspective view of a conventional magnetic transducer.

第3図は、従来の磁気変換器まわりの空気の流れを磁気
媒体に垂直方向からみた説明図である。
FIG. 3 is an explanatory diagram of the air flow around a conventional magnetic transducer viewed from a direction perpendicular to the magnetic medium.

第2図に示す磁気変換器は磁気媒体側からみた斜視図で
、磁気媒体(図示せず)は図の左下から磁気変換器に近
付き、右上に去るものである。
The magnetic transducer shown in FIG. 2 is a perspective view seen from the magnetic medium side, with the magnetic medium (not shown) approaching the magnetic transducer from the bottom left of the figure and leaving the top right.

磁気変換器9の磁気媒体表面と相対する面には、磁気媒
体との相対運動方向に間隔をおいて平行に伸びる;3本
のレール部1,2.3が形成されている。これらのレー
ル部1,2.3には、いずれも磁気媒体の近寄り側にそ
れぞれテーパ部1 a +2a、3aがあり、それらの
後方にレール面】b。
On the surface of the magnetic transducer 9 facing the surface of the magnetic medium, three rail portions 1, 2.3 are formed that extend parallel to each other at intervals in the direction of relative movement with the magnetic medium. Each of these rail parts 1, 2.3 has a tapered part 1a+2a, 3a, respectively, on the side closer to the magnetic medium, and a rail surface [b] behind them.

2b、3bを備えて磁気媒体表面との間で空気滑動面を
形成するようになっている。
2b and 3b to form an air sliding surface with the surface of the magnetic medium.

中央のレール部2の後方には、磁気コア4と磁気ギャッ
プ5が設けられている。そして、この磁気ギャップ5は
、磁気媒体上の所定の記憶トラック上に精度よく保持さ
れていなければならない。
A magnetic core 4 and a magnetic gap 5 are provided behind the central rail portion 2. This magnetic gap 5 must be maintained precisely on a predetermined storage track on the magnetic medium.

通常、このような磁気変換器9は1図示しないがジンバ
ルとばね部材からなる支持手段によってアクセス機構に
連設されるもので、その支持手段と磁気変換器9との取
り付けは、磁気変換器9の背面側で長手方向のほぼ中央
部に設けられている溝部6′の底面6a’ にジンバル
を接着するという公知の手段で行われている。
Normally, such a magnetic transducer 9 is connected to the access mechanism by a support means (not shown) consisting of a gimbal and a spring member, and the attachment of the support means and the magnetic transducer 9 is done by This is accomplished by a known method of bonding a gimbal to the bottom surface 6a' of a groove 6' provided at approximately the center in the longitudinal direction on the rear side.

磁気媒体表面と微小間隔を保って磁気変換器が浮上する
作動状態では、その磁気変換器は相対運動方向からの空
気の流れに曝されろ。このときの磁気変換器まわりの空
気の流れを磁気媒体面の垂直方向から見ろと、第3図に
示すように、磁気変換器の両側面の前縁7,8で剥1離
する流れ】1゜12が左、右交互に剥離して、後方に、
いわゆるカルマン渦列13が発生している。
In the operating state in which the magnetic transducer floats at a small distance from the surface of the magnetic medium, the magnetic transducer is exposed to air flow from the direction of relative motion. If we look at the air flow around the magnetic transducer at this time from the direction perpendicular to the surface of the magnetic medium, we can see that the flow separates at the front edges 7 and 8 on both sides of the magnetic transducer, as shown in Figure 3.゜12 peels off alternately on the left and right, backwards,
A so-called Karman vortex street 13 is generated.

このようなカルマン渦列13が生じる場合には。When such a Karman vortex street 13 occurs.

周知のように、磁気変換器9に、空気の流れに直角方向
の1時間的にその大きさと方向が変化する力、すなわち
変1)+揚力を作用するものである。
As is well known, a force whose magnitude and direction change over time in a direction perpendicular to the air flow, that is, a lift force is applied to the magnetic transducer 9.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

前述のように、第2図に示す磁気変換器9は、そのほぼ
中央部で支持手段に接着されているため、上記の変動揚
力によって、支持手段接着部を中心とする回転振動(揺
動運動)が発生する。また、前述のように、磁気ギャッ
プ5は磁気変換器9の後流端に設置されているため、そ
の揺動運動によって磁気媒体、例えば磁気ディスクの記
録トラックからの位置ずれを起すという問題があった。
As mentioned above, since the magnetic transducer 9 shown in FIG. 2 is bonded to the support means at approximately the center thereof, the above-mentioned fluctuating lift causes rotational vibration (oscillating motion) centered on the bonded portion of the support means. ) occurs. Furthermore, as described above, since the magnetic gap 5 is installed at the downstream end of the magnetic transducer 9, there is a problem in that its oscillating motion causes a positional shift from the recording track of the magnetic medium, for example, a magnetic disk. Ta.

本発明は、前述の従来技術の問題点を解決するためにな
されたもので、空気の流れから受ける変動揚力の小さい
、したがって磁気ギャップが位置ずれを起しにくい浮動
形の磁気変換器の提供を、その目的としている。
The present invention has been made in order to solve the above-mentioned problems of the prior art, and aims to provide a floating magnetic transducer that receives little fluctuating lift from airflow and is therefore less likely to cause misalignment of the magnetic gap. , that purpose.

〔問題点を解決するための手段〕[Means for solving problems]

前述の問題点を解決するための手段として、本発明に係
る磁気変換器の構成は、磁気媒体表面と相対運動をなす
磁気変換器であって、磁気媒体表面と相対する面に相対
運動方向に間隔をおいて形成され、前記磁気媒体表面と
の間に空気滑動膜を形成すべきレール面を有する複数の
レール部を備えた磁気変換器において、前記磁気媒体が
前記磁気変換器に近寄、る方向から前記磁気変換器を見
るときの当該磁気変換器の投影形状における、前記磁気
媒体表面に垂直な高さに対する前記磁気媒体表面に平行
な幅の比が4以上に形成されているものである。
As a means for solving the above-mentioned problems, the configuration of a magnetic transducer according to the present invention is a magnetic transducer that moves relative to the surface of a magnetic medium, and has a magnetic transducer that moves relative to the surface of the magnetic medium in the direction of the relative movement. In the magnetic transducer, the magnetic transducer includes a plurality of rail portions that are formed at intervals and have rail surfaces that form an air sliding film between the magnetic medium and the magnetic medium surface. In the projected shape of the magnetic transducer when looking at the magnetic transducer from the direction, the ratio of the width parallel to the magnetic medium surface to the height perpendicular to the magnetic medium surface is 4 or more. .

ここで、本発明を開発した考え方を第4図ないし第6図
を参照して説明する。
The concept behind the development of the present invention will now be explained with reference to FIGS. 4 to 6.

第4図は、第2図の磁気変換器の正面図、第5図は、変
動揚力の周波数分布図、第6図は、変動揚力のピーク周
波数成分の振幅と磁気変換器の横断面形状との関係を示
す線図である。
Figure 4 is a front view of the magnetic transducer shown in Figure 2, Figure 5 is a frequency distribution diagram of fluctuating lift, and Figure 6 shows the amplitude of the peak frequency component of fluctuating lift and the cross-sectional shape of the magnetic transducer. FIG.

第4図は、従来の磁気変換器9を空気の流れの上流側か
ら見た正面図であるが、換言すれば、磁気媒体が磁気変
換器9に近寄る方向から前記磁気変換器を見るときの当
該磁気変換器の投影形状を示す図に相当する。
FIG. 4 is a front view of the conventional magnetic transducer 9 seen from the upstream side of the air flow. In other words, when looking at the magnetic transducer 9 from the direction in which the magnetic medium approaches the magnetic transducer 9 This corresponds to a diagram showing the projected shape of the magnetic transducer.

第4図に示す従来の磁気変換器9の、磁気媒体20に垂
直な高さをh、磁気媒体20に平行な幅をWとすると、
w/hは2.8である。
If the height perpendicular to the magnetic medium 20 of the conventional magnetic transducer 9 shown in FIG. 4 is h, and the width parallel to the magnetic medium 20 is W, then
w/h is 2.8.

本発明者らは、磁気媒体20に係る磁気ディスクと微小
間隔をなすように保持した磁気変換器9に作用する変動
揚力を測定し、その周波数を分析したところ、第5図に
示すような結果が得られた。
The present inventors measured the fluctuating lift force acting on the magnetic transducer 9 held at a minute distance from the magnetic disk related to the magnetic medium 20, and analyzed its frequency, and found the results shown in FIG. was gotten.

第5図は、横軸に周波数、縦軸に変動揚力を示したもの
で、本図から明らかなように、変動揚力はある特定の周
波数で変動していることがわかった。これは、第3図に
示したカルマン渦列の発生と関連しているものである。
FIG. 5 shows the frequency on the horizontal axis and the variable lift force on the vertical axis. As is clear from this figure, it was found that the variable lift force fluctuates at a specific frequency. This is related to the generation of the Karman vortex street shown in FIG.

そこで、本発明者らは、次にw/hをパラメータとして
変動揚力のピーク値を測定したところ、第6図に示す結
果が得られた。
Therefore, the inventors next measured the peak value of the fluctuating lift using w/h as a parameter, and obtained the results shown in FIG. 6.

第6図は、横軸に磁気変換器の横断面形状を表わすw/
hをとり、縦軸に変動揚力のピーク周波数成分の振幅を
指数化したものをとったもので。
In Figure 6, the horizontal axis represents the cross-sectional shape of the magnetic transducer w/
h, and the amplitude of the peak frequency component of the fluctuating lift is plotted as an index on the vertical axis.

本図に示すように、w/hが3.8ではw / hが小
さいときの約1/2の振幅となり、w/hが4を越すと
特定の周波数の変動は見られなくなることがわかった。
As shown in this figure, when w/h is 3.8, the amplitude is approximately 1/2 of that when w/h is small, and when w/h exceeds 4, fluctuations in specific frequencies are no longer observed. Ta.

したがって、磁気変換器が磁気媒体となす相対運動方向
の投影形状におけるw / hを4以上にすれば、変動
揚力による磁気ギャップの位置ずれを低減できる見込み
が得られた。
Therefore, if w/h in the projected shape of the relative motion direction made by the magnetic transducer with the magnetic medium is set to 4 or more, it is possible to reduce the positional deviation of the magnetic gap due to the fluctuating lift force.

〔作用〕[Effect]

次に、第7図は、本発明の磁気変換器まわりの空気の流
れを示す説明図であり、前述のw/hが6のときの空気
の流れを、先の第3図に対比する渦形状として示したも
のである。
Next, FIG. 7 is an explanatory diagram showing the air flow around the magnetic transducer of the present invention. It is shown as a shape.

第7図に示すように、磁気変換器の両側面の前縁7,8
から、流れの左右(図では上下)が対称の渦列14が発
生しており、このために変動揚力が小さくなるものと考
えられる。
As shown in FIG. 7, the front edges 7, 8 on both sides of the magnetic transducer
Therefore, a vortex row 14 that is symmetrical on the left and right sides of the flow (up and down in the figure) is generated, and it is thought that this causes the fluctuating lift force to become small.

左右対称の渦列14が発生する理由は、磁気変換器の左
右の前縁7,8の間隔が離れたためと、そのためにレー
ル部1,2間、およびレール部2゜3間に、相対運動方
向に上流から下流に形設されている溝部を通る空気の流
れ、および磁気変換器の背面を越す空気の流れから、後
流中に流入する流れの影響が強まったために、両前縁7
,8からの剥離の相互干渉が弱まったためと考えられる
The reason why the left-right symmetrical vortex row 14 is generated is that the left and right front edges 7 and 8 of the magnetic transducer are spaced apart, and because of this, there is a relative movement between the rail parts 1 and 2 and between the rail parts 2 and 3. Due to the air flow through the groove formed in the direction from upstream to downstream and the air flow over the back side of the magnetic transducer, the influence of the flow flowing into the wake is strengthened, so that both leading edges 7
This is thought to be due to the weakening of the mutual interference of peeling from , 8.

〔実施例〕〔Example〕

以下、本発明の一実施例を第1図を参照して説明する。 An embodiment of the present invention will be described below with reference to FIG.

第1図は、本発明の一実施例に係る磁気変換器の斜視図
であり、図中、第2図と同一符号のものは従来例と同等
部分であるから、その説明を省略する。
FIG. 1 is a perspective view of a magnetic transducer according to an embodiment of the present invention. In the figure, the same reference numerals as those in FIG. 2 are the same parts as in the conventional example, and therefore the explanation thereof will be omitted.

第1図に示す磁気変換器10は、先の第2図と同様、磁
気媒体との相対運動方向に間隔をおいて平行に伸びる3
本のレール部1,2.3が形成されており、それぞれレ
ール面1b、2b、3bを備えて磁気媒体表面との間で
空気滑動面を形成するようになっている。そして、この
磁気変換器10は、全体の形状を薄形に形成し、磁気媒
体20(第4図参照)が磁気変換器10に近寄する方向
から前記磁気変換器10を見るときの当該磁気変換器の
投影形状におけろ、前記磁気媒体20表面に垂直な高さ
hに対する前記磁気媒体20表面に平行な幅Wの比、w
/hが4.2 に形成されている。
The magnetic transducer 10 shown in FIG. 1, as in FIG.
Book rail portions 1, 2.3 are formed, each having a rail surface 1b, 2b, 3b so as to form an air sliding surface with the magnetic medium surface. The magnetic transducer 10 has a thin overall shape, and the magnetic transducer 10 when viewed from the direction in which the magnetic medium 20 (see FIG. 4) approaches the magnetic transducer 10 In the projected shape of the container, the ratio of the width W parallel to the surface of the magnetic medium 20 to the height h perpendicular to the surface of the magnetic medium 20, w
/h is set to 4.2.

全体形状が薄形となっているため、アクセス機構に連設
される支持手段を取付けろ溝部6は浅くなっているが、
底面6aにジンバルを接着して、支持部の機能は従来と
相違するところはない。
Since the overall shape is thin, the groove 6 is shallow for attaching the support means connected to the access mechanism.
A gimbal is bonded to the bottom surface 6a, and the function of the support section is no different from the conventional one.

したがって、中央レール部2の後方に設けられた磁気コ
ア4と磁気ギャップ5は、磁気媒体20、例えば磁気デ
ィスクの記憶トラック上に精度よく保持される。
Therefore, the magnetic core 4 and the magnetic gap 5 provided at the rear of the central rail portion 2 are accurately held on the storage track of the magnetic medium 20, for example, a magnetic disk.

磁気媒体20の表面と微小間隔を保って磁気変換器10
が浮上する作動状態では、磁気変換器10は相対運動方
向からの空気の流れに曝されるが、本実施例の磁気変換
器10では、先に第7図で説明したように、磁気変換器
10の両側面の前縁7,8から、空気の流れの左右(第
7図では上下)対称の渦列14が発生するので、磁気変
換器10に作用する変動揚力は小さく7抑制される。
The magnetic transducer 10 is placed at a small distance from the surface of the magnetic medium 20.
In the operating state in which the magnetic transducer 10 floats, the magnetic transducer 10 is exposed to air flow from the direction of relative motion. Since vortex rows 14 are generated from the front edges 7 and 8 on both side surfaces of the magnetic transducer 10, which are symmetrical in the left and right directions (up and down in FIG. 7) of the air flow, the fluctuating lift acting on the magnetic transducer 10 is suppressed to a small level.

したがって、本実施例の磁気変換器10によれば、磁気
コア4、磁気ギャップ5部の揺動運動が抑制され、磁気
媒体、例えば磁気ディスクの記録トラックの記録トラッ
クからの位置ずれが少なくなり、位置決め誤差を従来の
1/2J’J、下に低減する効果が得られる。
Therefore, according to the magnetic transducer 10 of this embodiment, the swinging motion of the magnetic core 4 and the magnetic gap 5 is suppressed, and the positional deviation of the recording track of the magnetic medium, for example, a magnetic disk, from the recording track is reduced. The effect of reducing the positioning error to 1/2 J'J of that of the conventional method can be obtained.

〔発明の効果〕〔Effect of the invention〕

以上述べたように、本発明によれば、空気の流れから受
ける変!l!lJ揚力の小さい、したがって磁気ギャッ
プが位置ずれを起しにくい浮動形の磁気変換器を提供す
ることができる。
As described above, according to the present invention, changes caused by air flow can be reduced. l! It is possible to provide a floating magnetic transducer that has a small lJ lift force and is therefore less likely to cause misalignment of the magnetic gap.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は、本発明の一実施例に係る磁気変換器の斜視図
、第2図は、従来の磁気変換器の斜視図、第3図は、従
来の磁気変換器まわりの空気の流れを示す説明図、第4
図は、従来の磁気変換器を空気の流れの上流側からみた
投影図、第5図は、変動揚力の周波数分布図、第6図は
、変動揚力のピーク周波数成分の振幅と磁気変換器の横
断面形状との関係を示す線図、第7図は、本発明の磁気
変換器まわりの空気の流れを示す説明図である。 1.2.3・・・レール部、lb、2b、3b ・・レ
ール面、4・・・磁気コア、5・・・磁気ギャップ、1
0・・・磁気変換器。
Fig. 1 is a perspective view of a magnetic transducer according to an embodiment of the present invention, Fig. 2 is a perspective view of a conventional magnetic transducer, and Fig. 3 shows the air flow around the conventional magnetic transducer. Explanatory diagram showing, No. 4
The figure shows a projection of a conventional magnetic transducer viewed from the upstream side of the air flow, Figure 5 is a frequency distribution diagram of fluctuating lift, and Figure 6 shows the amplitude of the peak frequency component of fluctuating lift and the magnetic transducer. FIG. 7, a diagram showing the relationship with the cross-sectional shape, is an explanatory diagram showing the flow of air around the magnetic transducer of the present invention. 1.2.3...Rail part, lb, 2b, 3b...Rail surface, 4...Magnetic core, 5...Magnetic gap, 1
0...Magnetic transducer.

Claims (1)

【特許請求の範囲】[Claims] 1、磁気媒体表面と相対運動をなす磁気変換器であつて
、磁気媒体表面と相対する面に相対運動方向に間隔をお
いて形成され、前記磁気媒体表面との間に空気滑動膜を
形成すべきレール面を有する複数のレール部を備えた磁
気変換器において、前記磁気媒体が前記磁気変換器に近
寄る方向から前記磁気変換器を見るときの当該磁気変換
器の投影形状における、前記磁気媒体表面に垂直な高さ
に対する前記磁気媒体表面に平行な幅の比が4以上に形
成されていることを特徴とする磁気変換器。
1. A magnetic transducer that moves relative to the surface of a magnetic medium, which is formed on a surface facing the surface of the magnetic medium at intervals in the direction of relative movement, and forms an air sliding film between it and the surface of the magnetic medium. In a magnetic transducer equipped with a plurality of rail parts having a symmetrical rail surface, the surface of the magnetic medium in the projected shape of the magnetic transducer when the magnetic transducer is viewed from a direction in which the magnetic medium approaches the magnetic transducer. A magnetic transducer characterized in that the ratio of the width parallel to the surface of the magnetic medium to the height perpendicular to the magnetic medium is 4 or more.
JP61023807A 1986-02-07 1986-02-07 Magnetic transducer Expired - Lifetime JPH06103585B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61023807A JPH06103585B2 (en) 1986-02-07 1986-02-07 Magnetic transducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61023807A JPH06103585B2 (en) 1986-02-07 1986-02-07 Magnetic transducer

Related Child Applications (1)

Application Number Title Priority Date Filing Date
JP11645698A Division JPH10275437A (en) 1998-04-27 1998-04-27 Magnetic transducer

Publications (2)

Publication Number Publication Date
JPS62183020A true JPS62183020A (en) 1987-08-11
JPH06103585B2 JPH06103585B2 (en) 1994-12-14

Family

ID=12120595

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61023807A Expired - Lifetime JPH06103585B2 (en) 1986-02-07 1986-02-07 Magnetic transducer

Country Status (1)

Country Link
JP (1) JPH06103585B2 (en)

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS48109919U (en) * 1972-03-23 1973-12-18
JPS5278416A (en) * 1975-12-24 1977-07-01 Fujitsu Ltd Thin-film integrated multiplex magnetic head
JPS52151016A (en) * 1976-06-10 1977-12-15 Nec Corp Floating head slider
US4081846A (en) * 1976-06-07 1978-03-28 Applied Magnetics Corporation Magnetic head-slider assembly

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS48109919U (en) * 1972-03-23 1973-12-18
JPS5278416A (en) * 1975-12-24 1977-07-01 Fujitsu Ltd Thin-film integrated multiplex magnetic head
US4081846A (en) * 1976-06-07 1978-03-28 Applied Magnetics Corporation Magnetic head-slider assembly
JPS52151016A (en) * 1976-06-10 1977-12-15 Nec Corp Floating head slider

Also Published As

Publication number Publication date
JPH06103585B2 (en) 1994-12-14

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