JPH08147917A - Magnetic storage device and its slider - Google Patents

Magnetic storage device and its slider

Info

Publication number
JPH08147917A
JPH08147917A JP28167894A JP28167894A JPH08147917A JP H08147917 A JPH08147917 A JP H08147917A JP 28167894 A JP28167894 A JP 28167894A JP 28167894 A JP28167894 A JP 28167894A JP H08147917 A JPH08147917 A JP H08147917A
Authority
JP
Japan
Prior art keywords
air
magnetic recording
slider
outflow end
air outflow
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
Application number
JP28167894A
Other languages
Japanese (ja)
Inventor
Hidekazu Kodaira
英一 小平
Masaaki Matsumoto
真明 松本
Yasuo Kojima
康生 小島
Hiromitsu Tokisue
裕充 時末
Shuichi Sugawara
秀一 菅原
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 JP28167894A priority Critical patent/JPH08147917A/en
Publication of JPH08147917A publication Critical patent/JPH08147917A/en
Pending legal-status Critical Current

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

Abstract

PURPOSE: To substantially make the mim. floating gap of a slider conform to a magnetic recording gap by satisfying an expression as shown in the figure, where a distance from an air outflow end of the slider to an air outflow end side of a tapered surface is denoted as 1x, and a distance from the air outflow end to the magnetic recording/reproducing gap as 1g, etc. CONSTITUTION: The distance from the air outflow end of the slider to the air outflow end side of the tapered surface is denoted as 1x, while the distance from the air outflow end to the magnetic recording/reproducing gap as 1g, a floating height at the air outflow end as hr, a floating height on the air outflow end side of the tapered surface as hin and a crown height δx. The slider is provided to satisfy the conditions of the expression including the above factors. Thus, the magnetic recording gap and the min. floating height can substantially be made to conform to each other. Then, the capacity of the magnetic storage device can be increased while the reliability is maintained.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は磁気記憶装置及びそのス
ライダに関わり、特に、スライダの最小浮上すきまと磁
気記録すきまを実質的に一致させることで、浮上信頼性
を保ちながら大容量化を実現しうる磁気記憶装置及びそ
のスライダに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic storage device and a slider thereof, and in particular, by substantially matching the minimum flying clearance of the slider with the magnetic recording clearance, a large capacity is realized while maintaining the flying reliability. Magnetic storage device and its slider.

【0002】[0002]

【従来の技術】磁気記録媒体に磁気情報を記録したり、
また磁気記録媒体上に記録された磁気情報を再生するこ
とを目的とした磁気記憶装置では、磁気変換器の磁気記
録/再生ギャップと磁気記録媒体間の距離である磁気記
録すきまをできる限り狭く保つ必要がある。そこで、磁
気変換器を備えたスライダを空気ベアリング効果を利用
して、磁気記録媒体上に微小なすきまで浮上させてい
る。
2. Description of the Related Art Recording magnetic information on a magnetic recording medium,
Further, in a magnetic storage device intended to reproduce magnetic information recorded on a magnetic recording medium, the magnetic recording gap which is the distance between the magnetic recording / reproducing gap of the magnetic converter and the magnetic recording medium is kept as narrow as possible. There is a need. Therefore, a slider provided with a magnetic converter is levitated to a minute gap on the magnetic recording medium by utilizing the air bearing effect.

【0003】磁気記録媒体とスライダ間の浮上すきまを
狭小化するために、磁気記録媒体は平滑であることが望
ましい。しかし、磁気記録媒体が平滑になるほど、磁気
記憶装置が停止中に、スライダの浮上面と磁気記録媒体
が粘着しやすくなり、磁気記憶装置の起動時にスライダ
と磁気記録媒体間に大きな粘着力が働いて装置が起動で
きなくなったり、支持バネが破壊されることがある。そ
こで、特公昭58−21329では、浮上面の長手方向
にクラウンを設けることでスライダと磁気記録媒体の粘
着を防ぎ、さらに空気流出端側にテーパ面を設けること
で、空気流出端が最小浮上すきまとなるようにしてい
る。また、USP4285019では、スライダの長手
方向あるいは短手方向にクラウンを形成して粘着を防ぐ
と共に、磁気記録/再生ギャップ位置で最小浮上すきま
にならないようにして、磁気変換器に対するダストの悪
影響を防いでいる。
In order to narrow the flying clearance between the magnetic recording medium and the slider, it is desirable that the magnetic recording medium be smooth. However, as the magnetic recording medium becomes smoother, the air bearing surface of the slider and the magnetic recording medium are more likely to adhere to each other while the magnetic storage device is stopped, and a large adhesive force is exerted between the slider and the magnetic recording medium when the magnetic storage device is activated. This may cause the device to fail to start or the support spring to break. Therefore, in Japanese Patent Publication No. 58-21329, a crown is provided in the longitudinal direction of the air bearing surface to prevent sticking between the slider and the magnetic recording medium, and a taper surface is provided on the air outlet end side to provide a minimum clearance for the air outlet end. I am trying to become. Further, in USP 4285019, a crown is formed in a longitudinal direction or a lateral direction of a slider to prevent adhesion, and a minimum floating clearance is not provided at a magnetic recording / reproducing gap position to prevent an adverse effect of dust on a magnetic converter. There is.

【0004】[0004]

【発明が解決しようとする課題】磁気記憶装置の大容量
化を進めるために、スライダの浮上すきまの狭小化は必
須である。浮上すきまの狭小化を信頼性高く実現するに
は、磁気記録媒体上のあるトラックから他のトラックへ
の移動動作であるシーク位置決め時に、スライダに作用
するモーメント力や、磁気記録媒体のうねりに起因する
加振力、環境温度変化等、各種外乱による動的な浮上す
きま変化をできる限り小さくする必要がある。また、ス
ライダの加工誤差に起因する静的な浮上すきま変化もで
きる限り小さくする必要がある。
In order to increase the capacity of the magnetic storage device, it is essential to narrow the flying clearance of the slider. In order to realize the narrowing of the floating clearance with high reliability, the moment force acting on the slider and the waviness of the magnetic recording medium during seek positioning, which is the movement from one track to another on the magnetic recording medium, are required. It is necessary to minimize the dynamic change in the floating clearance due to various disturbances such as the applied excitation force and environmental temperature changes. Also, it is necessary to minimize the static change in the floating clearance due to the machining error of the slider.

【0005】磁気記録媒体のうねりに起因する浮上すき
まの変化を小さくするために磁気記録媒体を平滑化する
必要があるが、スライダと磁気記録媒体との粘着力が大
きくなり、支持バネや磁気記録媒体を破壊する可能性が
高くなるという問題点がある。
Although it is necessary to smooth the magnetic recording medium in order to reduce the change in the floating clearance caused by the undulation of the magnetic recording medium, the adhesive force between the slider and the magnetic recording medium becomes large, and the supporting spring and the magnetic recording are increased. There is a problem that the possibility of destroying the medium increases.

【0006】前記特公昭58−21329は粘着力を低
減するためにスライダの長手方向にクラウンを形成し
て、スライダと磁気記録媒体との接触面積を減らし粘着
力を低減している。さらにスライダの空気流入端にテー
パ面を設け空気流出端が最小浮上すきまになるようにし
ている。磁気記憶装置の記憶容量を増加させるためには
磁気記録/再生ギャップと磁気記録媒体間の距離である
磁気記録すきまをできるだけ狭小化した方がよいが、逆
に、磁気記憶装置の信頼性を向上させるためには、スラ
イダと磁気記録媒体間の最小浮上すきまはできるだけ大
きな方がよい。従来の一般的なスライダでは、前記特公
昭58−21329で開示されているようにスライダの
空気流出端近傍に磁気変換器を備えており、磁気記録/
再生ギャップは空気流出端ではなく、そこから空気流入
端側にわずかにずれた位置に形成されている。また空気
流入端側にはテーパ面が形成されているのでスライダ
は、空気流入端側の浮上すきまは大きく、空気流出端位
置において最小浮上すきまとなるような姿勢で浮上して
いる。このような浮上姿勢の下では、磁気記録/再生ギ
ャップ位置における磁気記録すきまは、空気流出端にお
ける最小浮上すきまより必ず大きくなってしまう。先に
述べたように、磁気記憶装置の記憶容量を大きくするた
めには磁気記録すきまはできるだけ小さく、また浮上信
頼性を保つためには最小浮上すきまはできるだけ大きく
したい。スライダの浮上すきまの狭小化が進むほど、磁
気記録すきまと最小浮上すきまの差が記憶容量と浮上信
頼性の面から問題となってくる。スライダの最小浮上す
きま位置はスライダの浮上姿勢、およびクラウン高さ等
によって大きく変わり、前記公知例に述べられているよ
うに必ずしもテーパ面を設けたからといって空気流出端
が最小浮上すきまになるわけではなく、最小浮上すきま
と磁気記録すきまを一致させるためには、適切な浮上姿
勢とクラウン高さを規定する必要がある。さらに近年普
及してきた半導体プロセスを利用して薄膜磁気変換器を
形成する場合には、スライダ浮上面の任意の位置に精度
良く磁気記録/再生ギャップを形成することができ、空
気流出端近傍に磁気記録/再生ギャップを形成すること
にとらわれる必要もなくなる。
In Japanese Patent Publication No. 58-21329, a crown is formed in the longitudinal direction of the slider in order to reduce the adhesive force and the contact area between the slider and the magnetic recording medium is reduced to reduce the adhesive force. Furthermore, a taper surface is provided on the air inflow end of the slider so that the air outflow end has a minimum floating clearance. In order to increase the storage capacity of the magnetic storage device, it is better to make the magnetic recording gap, which is the distance between the magnetic recording / reproducing gap and the magnetic recording medium, as narrow as possible. On the contrary, the reliability of the magnetic storage device is improved. For this purpose, the minimum floating clearance between the slider and the magnetic recording medium should be as large as possible. In a conventional general slider, a magnetic transducer is provided near the air outflow end of the slider as disclosed in Japanese Patent Publication No. 58-21329, and magnetic recording / recording is performed.
The regeneration gap is formed not at the air outflow end but at a position slightly displaced from the air outflow end toward the air inflow end. Further, since the taper surface is formed on the air inflow end side, the slider has a large floating clearance on the air inflow end side, and is floated in such a posture as to have the minimum floating clearance at the air outflow end position. Under such a flying posture, the magnetic recording clearance at the magnetic recording / reproducing gap position is always larger than the minimum floating clearance at the air outflow end. As described above, the magnetic recording clearance should be as small as possible in order to increase the storage capacity of the magnetic storage device, and the minimum floating clearance should be as large as possible in order to maintain the floating reliability. As the slider flying clearance becomes narrower, the difference between the magnetic recording clearance and the minimum flying clearance becomes a problem in terms of storage capacity and flying reliability. The minimum floating clearance of the slider greatly changes depending on the flying posture of the slider, the height of the crown, etc., and as described in the above-mentioned known example, the taper surface does not necessarily mean that the air outflow end has the minimum floating clearance. Instead, in order to match the minimum flying clearance with the magnetic recording clearance, it is necessary to specify an appropriate flying posture and crown height. Further, when a thin film magnetic transducer is formed by utilizing a semiconductor process which has been widely used in recent years, a magnetic recording / reproducing gap can be formed with high accuracy at an arbitrary position on the slider air bearing surface, and the magnetic recording / reproducing gap can be formed near the air outflow end. There is no need to be obsessed with forming the recording / playback gap.

【0007】USP4285019ではスライダの長手
方向及び短手方向にクラウンを設け磁気変換器の位置が
あえて最小浮上すきまとならないようにして、磁気記憶
装置内に存在するダストが磁気変換器に悪影響を与えな
いような構成としている。この公知例では最小浮上すき
まと磁気記録すきまが異なるので、磁気記憶装置の大容
量化が難しくなる。
According to USP 4285019, a crown is provided in the longitudinal direction and the lateral direction of the slider so that the position of the magnetic transducer does not intentionally become the minimum floating clearance, so that dust existing in the magnetic storage device does not adversely affect the magnetic transducer. It has such a configuration. In this known example, since the minimum floating clearance is different from the magnetic recording clearance, it is difficult to increase the capacity of the magnetic storage device.

【0008】本発明は、上記従来技術の問題点を解決す
るためになされたものであり、その目的は、スライダの
最小浮上すきまと磁気記録すきまを実質的に一致させ、
磁気記憶装置を信頼性を維持したまま、大容量化するこ
とにある。
The present invention has been made to solve the above-mentioned problems of the prior art, and its purpose is to make the minimum flying clearance of the slider substantially coincide with the magnetic recording clearance.
It is to increase the capacity of a magnetic storage device while maintaining its reliability.

【0009】[0009]

【課題を解決するための手段】上記目的を達成するため
に本発明の特徴は、空気流入端、空気流出端及び浮上面
を有し、前記浮上面は前記空気流入端側に形成したテー
パ面と、前記浮上面の長手方向に形成したクラウン高さ
δxの正クラウンからなり、前記浮上面の任意の位置に
磁気記録/再生ギャップが形成された磁気変換器を備
え、磁気記録媒体上を浮上するスライダにおいて、前記
正クラウン高さδxと、前記磁気記憶装置が記録/再生
中に、前記空気流出端と前記磁気記録媒体間にベアリン
グ効果で生じる浮上すきまhfと、前記テーパ面の空気
流出端側と前記磁気記録媒体間にベアリング効果で生じ
る浮上すきまhinと、前記空気流出端と前記テーパ面
の空気流出端側の距離lxと、前記空気流出端と前記磁
気記録/再生ギャップ間の距離lgとの間に、 (hf-hin)・lx/{6(2lg-lx)} ≦ δx ≦ (hin+hf)/4+1
/2・(hin・hf)1/2 の関係式が成り立つようなスライダとし、またそのスラ
イダを備えた磁気記憶装置とした。
To achieve the above object, a feature of the present invention is that it has an air inflow end, an air outflow end, and an air bearing surface, and the air bearing surface is a tapered surface formed on the air inflow end side. And a magnetic transducer having a crown height δx formed in the longitudinal direction of the air bearing surface and having a magnetic recording / reproducing gap formed at an arbitrary position on the air bearing surface and flying over a magnetic recording medium. In the slider, the positive crown height δx, the flying clearance hf generated by the bearing effect between the air outflow end and the magnetic recording medium during recording / reproducing by the magnetic storage device, and the air outflow end of the taper surface. Side clearance between the magnetic recording medium and the magnetic recording medium, the distance lx between the air outflow end and the air outflow end side of the tapered surface, the air outflow end and the magnetic recording / reproducing gap. Between the distance lg and (hf-hin) lx / {6 (2lg-lx)} ≤ δx ≤ (hin + hf) / 4 + 1
The slider is such that the relational expression of / 2 · (hin · hf) 1/2 is satisfied, and the magnetic storage device is provided with the slider.

【0010】[0010]

【作用】上記構成によれば、スライダの磁気記録/再生
ギャップ位置における浮上すきまが最小浮上すきまとな
り、最小浮上すきまと磁気記録すきまを実質的に一致さ
せることができ、磁気記憶装置の大容量化を信頼性を保
ちながら達成できる。
According to the above structure, the floating clearance at the magnetic recording / reproducing gap position of the slider becomes the minimum floating clearance, and the minimum floating clearance and the magnetic recording clearance can be substantially matched with each other, thus increasing the capacity of the magnetic storage device. Can be achieved while maintaining reliability.

【0011】[0011]

【実施例】以下、本発明の第1実施例について、図1〜
図4を用いて詳細に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A first embodiment of the present invention will be described below with reference to FIGS.
This will be described in detail with reference to FIG.

【0012】図1は本発明の第1実施例に関わるスライ
ダの浮上時の側面図である。スライダ1は空気流入端
2、空気流出端3、浮上面4を有し、浮上面4は空気流
入端側にテーパ面5と、テーパ面5の空気流出端側から
空気流出端4までの距離lxにわたりクラウン高さδx
のクラウンが形成されている。空気流出端3から距離l
gの位置に半導体プロセスを利用して形成した薄膜磁気
変換器6が備えられており、薄膜磁気変換器6の記録/
再生ギャップ7の位置において、磁気記録媒体8に磁気
情報を記録したり、あるいは磁気記録媒体8上に記録さ
れた磁気情報を再生している。スライダ1は磁気記録媒
体8の回転によって生じる空気流をテーパ面5および浮
上面4で受け、空気ベアリング効果により、磁気記録媒
体8上を極微小なすきまを保って浮上する。磁気記憶装
置の大容量化を実現するためには、磁気記録/再生ギャ
ップと磁気記録媒体8間の距離である磁気記録すきまを
できる限り狭小化する必要があり、それに伴いスライダ
の浮上面の任意の位置でとりうる最小浮上すきまをでき
る限り狭小化することが必要となる。現在、その最小浮
上すきまは100nm以下になっている。スライダ1を
磁気記録媒体8に接触させることなく、信頼性を保ちな
がら最小浮上すきまを低減するためには、磁気記録媒体
8の平滑性を向上させ、スライダ1の磁気記録媒体8に
対する追従性を向上させる必要がある。ところが磁気記
録媒体8の平滑性を向上させると、磁気記憶装置の停止
中にスライダ1と磁気記録媒体8が粘着し、装置を起動
させようとした際に、装置が起動しなかったり、スライ
ダ1の支持バネが破損したりすることがある。そこで、
従来は粘着を防ぐ目的で浮上面4の長手方向に正クラウ
ンを形成し、さらにスライダ1の空気流出端3の位置で
最小浮上すきまとなるように空気流入端側にテーパ面5
が形成されている。
FIG. 1 is a side view of a slider according to a first embodiment of the present invention when the slider is flying. The slider 1 has an air inflow end 2, an air outflow end 3, and an air bearing surface 4, and the air bearing surface 4 has a taper surface 5 on the air inflow end side and a distance from the air outflow end side of the taper surface 5 to the air outflow end 4. Crown height δx over lx
The crown is formed. Distance l from the air outflow end 3
A thin film magnetic converter 6 formed by using a semiconductor process is provided at the position of g, and recording / recording of the thin film magnetic converter 6 is performed.
At the position of the reproducing gap 7, magnetic information is recorded on the magnetic recording medium 8 or the magnetic information recorded on the magnetic recording medium 8 is reproduced. The slider 1 receives the air flow generated by the rotation of the magnetic recording medium 8 on the tapered surface 5 and the air bearing surface 4, and floats above the magnetic recording medium 8 with an extremely small clearance due to the air bearing effect. In order to realize a large capacity of the magnetic storage device, it is necessary to make the magnetic recording gap, which is the distance between the magnetic recording / reproducing gap and the magnetic recording medium 8, as narrow as possible, and accordingly, the air bearing surface of the slider is arbitrarily set. It is necessary to narrow the minimum floating clearance that can be taken at the position of as much as possible. Currently, the minimum floating clearance is 100 nm or less. In order to reduce the minimum flying clearance while maintaining reliability without contacting the slider 1 with the magnetic recording medium 8, the smoothness of the magnetic recording medium 8 is improved and the followability of the slider 1 to the magnetic recording medium 8 is improved. Need to improve. However, if the smoothness of the magnetic recording medium 8 is improved, the slider 1 and the magnetic recording medium 8 adhere to each other while the magnetic storage device is stopped, and the device does not start when the device is started, or the slider 1 The support spring of may be damaged. Therefore,
Conventionally, a positive crown is formed in the longitudinal direction of the air bearing surface 4 for the purpose of preventing sticking, and a taper surface 5 is provided on the air inflow end side so that the air bearing end has a minimum floating clearance at the position of the air outflow end 3.
Are formed.

【0013】近年、磁気変換器6は半導体プロセスを利
用して形成される薄膜磁気変換器が主流となっている。
この場合、例えばスライダ1の母材であるAlTiCな
どのセラミック基板の上に薄膜素子が多層膜として形成
されるため、図1に示すように空気流出端3の位置と磁
気記録/再生ギャップ7の位置を完全に一致させること
は困難である。
In recent years, a thin film magnetic converter formed by utilizing a semiconductor process has become the mainstream of the magnetic converter 6.
In this case, since the thin film element is formed as a multi-layered film on the ceramic substrate such as AlTiC which is the base material of the slider 1, the position of the air outflow end 3 and the magnetic recording / reproducing gap 7 as shown in FIG. It is difficult to match the positions perfectly.

【0014】図2は浮上面4にクラウンが形成されてい
ない場合のスライダ1の浮上状態を説明する側面図であ
る。空気流入端側にテーパ面5を有し、しかも空気流出
端3の位置と磁気記録/再生ギャップ7の位置が一致し
ていないので、空気流出端3における浮上すきまhfが
最小浮上すきまhminとなり、磁気記録/再生ギャッ
プ7の位置における浮上すきまである磁気記録すきまh
gは、hfより大きくなる。従来のようにスライダの浮
上すきまが大きな場合には、このhminとhgの差は
あまり重要でなかったが、今後益々低浮上化が進むと、
この差は記憶容量の損失と浮上信頼性の両面から非常に
重要になってくる。例えば、lx=1.1mm、lg=
40μm、hf=hmin=35nm、hin=210
nmという条件でスライダが浮上していると、磁気記録
すきまhgと最小浮上すきまhminの差Δhは約6.
4nmとなり、最小浮上すきまhminの約18%もの
値となってしまう。
FIG. 2 is a side view for explaining the flying state of the slider 1 when no crown is formed on the flying surface 4. Since the taper surface 5 is provided on the air inflow end side and the position of the air outflow end 3 and the position of the magnetic recording / reproducing gap 7 do not match, the floating clearance hf at the air outflow end 3 becomes the minimum floating clearance hmin, Magnetic recording clearance h with a floating clearance at the position of the magnetic recording / reproducing gap 7
g becomes larger than hf. When the flying clearance of the slider is large as in the past, the difference between hmin and hg was not so important, but if the flying height is further reduced in the future,
This difference becomes very important in terms of storage capacity loss and floating reliability. For example, lx = 1.1 mm, lg =
40 μm, hf = hmin = 35 nm, hin = 210
When the slider flies under the condition of nm, the difference Δh between the magnetic recording clearance hg and the minimum flying clearance hmin is about 6.
It becomes 4 nm, which is about 18% of the minimum floating clearance hmin.

【0015】図3は浮上面4にクラウンが形成されてい
るが、図1と比べて空気流入端2側の浮上すきまが大き
な場合のスライダの浮上状態を説明する側面図である。
空気流入端2側の浮上すきまが大きな姿勢で浮上してい
ることにより最小浮上すきまhminと磁気記録すきま
hgの差が大きくなってしまう。例えば、lx=1.1
mm、lg=40μm、hf=hmin=35nm、h
in=300nm、δx=15nmの場合、磁気記録す
きまhgと最小浮上すきまhminの差Δhは約7.5
nmとなり、最小浮上すきまhminの約21%もの値
となってしまう。
FIG. 3 is a side view for explaining a flying state of the slider when a crown is formed on the air bearing surface 4 but the flying clearance on the air inflow end 2 side is larger than that in FIG.
Since the levitation clearance on the air inflow end 2 side is large, the difference between the minimum levitation clearance hmin and the magnetic recording clearance hg becomes large. For example, lx = 1.1
mm, lg = 40 μm, hf = hmin = 35 nm, h
When in = 300 nm and δx = 15 nm, the difference Δh between the magnetic recording clearance hg and the minimum flying clearance hmin is about 7.5.
nm, which is about 21% of the minimum floating clearance hmin.

【0016】図4は浮上面4にクラウンがなく、しかも
磁気記録/再生ギャップ7が図1、図2および図3と比
較して空気流入端側に形成された場合のスライダの浮上
状態を説明する側面図である。磁気記録/再生ギャップ
7が最小浮上すきまhminとなる空気流出端3から離
れるほど、磁気記録すきまhgと最小浮上すきまhfの
差が大きくなることが分かる。例えば、lx=1.1m
m、lg=400μm、hf=35nm、hin=21
0nmの場合、磁気記録すきまhgと最小浮上すきまh
fの差Δhは約63.6nmとなり、最小浮上すきまh
fの約182%もの値となってしまう。
FIG. 4 illustrates the flying state of the slider when the air bearing surface 4 has no crown and the magnetic recording / reproducing gap 7 is formed on the air inflow end side as compared with FIGS. 1, 2 and 3. FIG. It can be seen that the difference between the magnetic recording clearance hg and the minimum floating clearance hf increases as the magnetic recording / reproducing gap 7 moves away from the air outflow end 3 where the minimum floating clearance hmin is reached. For example, lx = 1.1m
m, lg = 400 μm, hf = 35 nm, hin = 21
In the case of 0 nm, the magnetic recording clearance hg and the minimum floating clearance h
The difference Δh in f is about 63.6 nm, and the minimum floating clearance h
The value is about 182% of f.

【0017】図1から図4の比較より、最小浮上すきま
hminと磁気記録すきまhgとの大小関係はスライダ
の空気流出端における浮上すきまhfの大きさ、テーパ
面の空気流出端側における浮上すきまhinの大きさ、
空気流出端からテーパ面の空気流出端側までの距離l
x、クラウンの大きさδx、そして空気流出端から磁気
記録/再生ギャップまでの距離lgとから決定され、こ
の5つの変数を適当な値に設計することで、最小浮上す
きまと磁気記録すきまを実質的に一致させることができ
る。その結果、スライダの浮上すきまを信頼性を保ちな
がら狭小化することができ、磁気記憶装置の大容量化を
実現できる。
From comparison of FIGS. 1 to 4, the magnitude relationship between the minimum flying clearance hmin and the magnetic recording clearance hg is as follows: the size of the flying clearance hf at the air outflow end of the slider, and the flying clearance hin at the air outflow end of the taper surface. The size of
Distance l from the air outflow end to the air outflow end side of the tapered surface
x, the size of the crown δx, and the distance lg from the air outflow end to the magnetic recording / reproducing gap, and by designing these five variables to appropriate values, the minimum floating clearance and the magnetic recording clearance can be substantially Can be matched. As a result, the flying clearance of the slider can be reduced while maintaining reliability, and the capacity of the magnetic storage device can be increased.

【0018】ここで、上記5つの変数を用いて、磁気記
録すきまhgを表すと次式になる。
Here, the magnetic recording clearance hg is expressed by the following equation using the above five variables.

【0019】 hg = hf + (hin-hf-4δx)・lg/lx + 4δx・x2/lx2 (1) ただし、クラウン形状は、空気流出端とテーパ面の空気
流出端側を両端とする2次曲線で定義した。
[0019] hg = hf + (hin-hf -4δx) · lg / lx + 4δx · x 2 / lx 2 (1) where the crown shape, and both ends of air outflow end side of the air outflow end and the tapered surface It was defined by a quadratic curve.

【0020】磁気記録すきまhgが最小浮上すきまhm
inと一致するための条件式は、(1)式より、 δx = (hf-hin)/{4(2lg/lx-1)} (2) となる。
The magnetic recording clearance hg is the minimum floating clearance hm
The conditional expression for matching with in is δx = (hf-hin) / {4 (2lg / lx-1)} (2) from the expression (1).

【0021】上記(2)式を満たすようなクラウン高さ
δx、浮上すきまhinおよびhf、スライダ長lx、
磁気記録/再生ギャップ位置lgとなるようなスライダ
を設計することで、磁気記録すきまhgと最小浮上すき
まhminを完全に一致させることができる。
Crown height δx, flying clearances h in and h f, slider length lx, which satisfy the above equation (2),
By designing the slider so that the magnetic recording / reproducing gap position lg is set, the magnetic recording clearance hg and the minimum floating clearance hmin can be perfectly matched.

【0022】ところで、浮上すきまの計測法としては、
ガラスディスク上でスライダを浮上させ、ガラスディス
クの背面から白色光あるいは単色光を照射し、スライダ
表面からの反射光とガラスディスクからの反射光の干渉
縞から浮上すきまを求める光干渉法が一般的である。ク
ラウン高さも同様に光干渉法を利用して計測することが
できる。
By the way, as a method of measuring the floating clearance,
The optical interference method is generally used in which the slider is levitated on the glass disk, white light or monochromatic light is emitted from the back surface of the glass disk, and the floating clearance is obtained from the interference fringes of the light reflected from the slider surface and the light reflected from the glass disk. Is. Similarly, the crown height can be measured by using the optical interference method.

【0023】この計測法では、浮上すきまの測定精度は
2nmから4nm程度であり、浮上すきまの計測にその
ような誤差が含まれていることを考慮すれば、以下の式
で表されるようなクラウン高さであれば、実質的に磁気
記録すきまhgが最小浮上すきまhminと一致してい
ると考えられる。
In this measuring method, the measurement accuracy of the floating clearance is about 2 nm to 4 nm, and considering that such an error is included in the measurement of the floating clearance, it is expressed by the following equation. At the crown height, it is considered that the magnetic recording clearance hg substantially matches the minimum floating clearance hmin.

【0024】 δx ≧ (hf-hin)/{6(2lg/lx-1)} (3) となる。Δx ≧ (hf-hin) / {6 (2lg / lx-1)} (3)

【0025】(3)式より小さなクラウン高さδxなら
ば、磁気記録すきまhgと最小浮上すきまhminの差
が無視できないほど大きくなってしまう。
If the crown height δx is smaller than the expression (3), the difference between the magnetic recording clearance hg and the minimum floating clearance hmin becomes too large to be ignored.

【0026】ここで具体的な計算例を示す。lx=1.
25mm、lg=30μm、hf=40nm、hin=
100nmとすれば、(2)式よりクラウン高さはδx
=15.8nmとなる。この時、磁気記録/再生ギャッ
プ位置、すなわち空気流出端から空気流入端側へ30μ
mの位置における浮上すきまである磁気記録すきまはh
g=39.96nmとなり、ここで浮上すきまは極小値
をとり、磁気記録すきまhgと最小浮上すきまhmin
が完全に一致する。同条件で(3)式よりクラウン高さ
を求めるとδx=10.5nmとなる。この場合、最小
浮上すきまとなる位置は空気流出端となり、最小浮上す
きまはhf=hmin=40nmとなる。一方、磁気記
録すきまはhg=40.45nmとなる。従って、hg
とhminの差はたかだか0.45nm程度であり、浮
上測定の誤差を考慮すれば実質的に等しいと考えて差し
支えない。
Here, a concrete calculation example will be shown. lx = 1.
25 mm, lg = 30 μm, hf = 40 nm, hin =
If the thickness is 100 nm, the crown height is δx from equation (2).
= 15.8 nm. At this time, the magnetic recording / reproducing gap position, that is, 30 μ from the air outflow end to the air inflow end side
The magnetic recording clearance up to the floating clearance at the m position is h
g = 39.96 nm, where the floating clearance has a minimum value, and the magnetic recording clearance hg and the minimum floating clearance hmin
Is an exact match. Under the same conditions, when the crown height is calculated from the equation (3), δx = 10.5 nm. In this case, the position of the minimum floating clearance is the air outflow end, and the minimum floating clearance is hf = hmin = 40 nm. On the other hand, the magnetic recording gap is hg = 40.45 nm. Therefore, hg
The difference between hmin and hmin is at most about 0.45 nm, and it may be considered that they are substantially equal in consideration of the error in the flying measurement.

【0027】次に浮上姿勢が上記例よりも大きな場合の
計算例を示す。lx=1.25mm、lg=30μm、
hf=40nm、hin=500nmとすれば、(2)
式よりδx=120.8nmとなる。この時、磁気記録
/再生ギャップ位置、すなわち空気流出端から空気流入
端側へ30μmの位置における浮上すきまである磁気記
録すきまはhg=39.72nmとなり、ここで浮上す
きまは極小値をとり、磁気記録すきまhgと最小浮上す
きまhminが完全に一致する。同条件で(3)式より
クラウン高さを求めるとδx=80.53nmとなる。
この場合、最小浮上すきまとなる位置は空気流出端とな
り最小浮上すきまはhf=hmin=40nmとなる。
一方、磁気記録すきまはhg=43.49nmとなる。
従って、hgとhminの差はたかだか3.49nm程
度であり、浮上測定の誤差を考慮すれば実質的に等しい
と考えて差し支えない。
Next, a calculation example when the flying posture is larger than the above example will be shown. lx = 1.25 mm, lg = 30 μm,
If hf = 40 nm and hin = 500 nm, (2)
From the formula, δx = 120.8 nm. At this time, the magnetic recording / reproducing gap position, that is, the magnetic recording clearance from the air outflow end to the air inflow end side at the position of 30 μm to the floating clearance is hg = 39.72 nm, where the floating clearance has a minimum value and The recording clearance hg and the minimum flying clearance hmin completely match. Under the same conditions, when the crown height is calculated from the equation (3), δx = 80.53 nm.
In this case, the position of the minimum floating clearance is the air outflow end, and the minimum floating clearance is hf = hmin = 40 nm.
On the other hand, the magnetic recording clearance is hg = 43.49 nm.
Therefore, the difference between hg and hmin is at most about 3.49 nm, and it can be considered that they are substantially equal in consideration of an error in levitation measurement.

【0028】次に、磁気記録/再生ギャップ位置の影響
を明らかにする計算例を示す。lx=1.25mm、l
g=300μm、hf=40nm、hin=100nm
とすれば、(2)式よりδx=28.8nmとなる。こ
の時、磁気記録/再生ギャップ位置、すなわち空気流出
端から空気流入端側へ300μmの位置における浮上す
きまである磁気記録すきまはhg=33.35nmとな
り、ここで浮上すきまは極小値をとり、磁気記録すきま
hgと最小浮上すきまhminが完全に一致する。同条
件で(3)式よりクラウン高さを求めるとδx=19.
23nmとなる。この場合、最小浮上すきま位置は空気
流出端から150μm空気流入端側にずれた位置とな
り、最小浮上すきまはhmin=39.08nmとな
る。磁気記録すきまはhg=40.37nmとなり、h
gとhminの差はたかだか1.29nm程度であり、
浮上測定の誤差を考慮すれば実質的に等しいと考えて差
し支えない。
Next, a calculation example for clarifying the influence of the magnetic recording / reproducing gap position will be shown. lx = 1.25 mm, l
g = 300 μm, hf = 40 nm, hin = 100 nm
Then, δx = 28.8 nm from the equation (2). At this time, the magnetic recording / reproducing gap position, that is, the magnetic recording clearance from the air outflow end to the air inflow end side at a position of 300 μm to the floating clearance is hg = 33.35 nm, where the floating clearance has a minimum value and The recording clearance hg and the minimum flying clearance hmin completely match. Under the same conditions, the crown height is calculated from equation (3), and δx = 19.
23 nm. In this case, the minimum floating clearance is a position displaced from the air outflow end to the air inflow end side by 150 μm, and the minimum floating clearance is hmin = 39.08 nm. The magnetic recording clearance is hg = 40.37 nm,
The difference between g and hmin is at most about 1.29 nm,
Considering the error of the levitation measurement, it can be considered that they are substantially equal.

【0029】以上のように、スライダの空気流出端にお
ける浮上すきまhf、テーパ面の空気流出端側の位置に
おける浮上すきまhin、空気流出端からテーパ面の空
気流出端側までの距離lx、空気流出端から磁気記録/
再生ギャップまでの距離lg、そしてクラウン高さδx
の値を(3)式を満たすように規定することで、磁気記
録すきまhgと最小浮上すきまhminを実質的に一致
させることができる。これは磁気記録媒体の径や周速に
よらず成り立つ条件式である。しかし、一般にスライダ
の浮上姿勢は周速によって変わるので設計の際には、磁
気記憶装置の記憶容量が最大となるように、スライダが
磁気記録媒体の記録領域の最外周位置で浮上していると
きの姿勢が(3)式を満足するようにするのが好まし
い。
As described above, the floating clearance hf at the air outflow end of the slider, the floating clearance h in at the air outflow end side of the tapered surface, the distance lx from the air outflow end to the air outflow end side of the tapered surface, the air outflow Magnetic recording from the edge /
Distance to reproduction gap lg, and crown height δx
By defining the value of to satisfy the expression (3), the magnetic recording clearance hg and the minimum floating clearance hmin can be substantially matched. This is a conditional expression that holds regardless of the diameter and peripheral speed of the magnetic recording medium. However, since the flying posture of the slider generally changes depending on the peripheral speed, when the slider is flying at the outermost peripheral position of the recording area of the magnetic recording medium, the maximum storage capacity of the magnetic storage device is designed. It is preferable that the posture of 3 satisfies the expression (3).

【0030】(3)式の条件を満たすと実質的にhgと
hminを一致させることができるが、図5に示すよう
にhinとhfの差が小さな姿勢で浮上し、しかも磁気
記録/再生ギャップ7が浮上面4の中程にあり、クラウ
ン高さδxが大きな場合には、計算上、浮上すきまが負
となることがある。しかし、実際には負の浮上すきまと
いうのはあり得ず、これは浮上面4のどこかが接触して
いることを意味している。
When the condition of the expression (3) is satisfied, hg and hmin can be substantially matched with each other. However, as shown in FIG. When 7 is in the middle of the air bearing surface 4 and the crown height δx is large, the flying clearance may be negative in calculation. However, in reality, there is no negative floating clearance, which means that somewhere on the air bearing surface 4 is in contact.

【0031】そこで、スライダ1と磁気記録媒体8の接
触が生じないようにするための条件式を求める。
Therefore, a conditional expression for preventing contact between the slider 1 and the magnetic recording medium 8 will be determined.

【0032】スライダ浮上面の任意の位置xにおける、
浮上すきまをh(x)とすれば、 h(x) = hf + (hin-hf-4δx)・x/lx + 4δx・x2/lx2 (4) となる。浮上面4が磁気記録媒体8に接触しないための
条件は、(4)式の極値が正であればよいので、結局、 δx < (hin+hf)/4 + 1/2・(hin/hf)1/2 (5) となる。
At an arbitrary position x on the air bearing surface of the slider,
If the floating clearance is h (x), then h (x) = hf + (hin-hf-4δx) · x / lx + 4δx · x 2 / lx 2 (4). The condition for the air bearing surface 4 not to come into contact with the magnetic recording medium 8 is that the extreme value of the expression (4) is positive, so that δx <(hin + hf) / 4 + 1/2 · (hin / hf) 1/2 (5)

【0033】従って、(3)式及び(5)式から (hf-hin)/{6(2lg/lx-1)} ≦ δx < (hin+hf)/4 + 1/2・(hin/hf)1/2 (6 ) とすることで、実質的にhgとhminを一致させられ
るばかりでなく、浮上面4と磁気記録媒体8の接触を防
ぐことができる。
Therefore, from equations (3) and (5), (hf-hin) / {6 (2lg / lx-1)} ≤ δx <(hin + hf) / 4 + 1/2 · (hin / hf By setting 1/2 (6), not only can hg and hmin be substantially matched, but also contact between the air bearing surface 4 and the magnetic recording medium 8 can be prevented.

【0034】図6から図8を用いて第2の実施例の詳細
な説明を行う。
The second embodiment will be described in detail with reference to FIGS. 6 to 8.

【0035】本実施例においては図6(b)のスライダ
浮上図に示すようにスライダ1は空気流入端2、空気流
出端3、浮上面4を有する。図6(a)に示す様に第2
の実施例のスライダ1を媒体対向面から見ると、浮上面
4はテーパ面5、一対のサイドレール10、一対のサイ
ドレールを空気流入端側で結ぶクロスレール9、クロス
レール9と一対のサイドレールで囲まれた負圧溝部1
1、空気流出端近傍に磁気変換器6を備えたセンタレー
ル12からなる。一対のサイドレール10はテーパ面5
の空気流出端側から延び、空気流出端3に到達する前に
カットされ、センタレール12はサイドレール10とは
逆に空気流出端3まで到達する形状となっている。この
ような形状のスライダの利点の一つとして、サイドレー
ルを空気流出端に到達する前にカットし、しかも空気流
入端2側が空気流出端3側より大きな浮上すきまとなる
ような姿勢で浮上しているので、仮にスライダの浮上姿
勢が幅方向に傾いてもサイドレール10がセンタレール
12より先に磁気記録媒体8に接触することが無く、必
ずセンタレール12の空気流出端近傍が最小浮上すきま
となり、結果としてスライダのロール剛性を見かけ上大
きくできることにある。ところが、第1実施例で述べた
ような条件でスライダを設計すると、センタレール12
上に形成された磁気記録/再生ギャップ7の位置におけ
る磁気記録すきまhgが最小浮上すきまhminと実質
的に一致した上に、サイドレール10の空気流出端側の
浮上すきまhsとhminの値が近づいてしまう。スラ
イダ1は磁気記録媒体8の全周にわたり浮上するので、
浮上している位置によって、スライダに対する空気の流
入方向が変わり、浮上すきまにスライダ幅方向の浮上ア
ンバランスΔhyが生じる。先に述べたようにhsとh
minの差が小さな場合に、Δhyが大きいとhsとh
minの大小関係が逆転し、hsの方が小さくなる場合
も起こりうる。そうなるとセンタレール12に磁気変換
器6を搭載して、その位置が必ず最小浮上すきまとなる
ことで達成していた利点を失うことになる。これを避け
るためには、サイドレール10のカット量をさらに大き
くし、スライダが傾いてもサイドレールが先に接触しな
いようにするか、あるいは空気流入端2側の浮上すきま
を大きくし、サイドレール10の空気流出端側における
浮上すきまを大きくする方法が考えられる。しかし、前
者はスライダのロール剛性が小さくなるという問題、後
者は磁気記録すきまhgと最小浮上すきまhminの差
が大きくなるという問題があり好ましくない。そこで、
本実施例では、スライダの長手方向には第1実施例で述
べたようなクラウン高さδxを形成し、その上で、短手
方向にもキャンバ高さδyの正キャンバを形成する。
In this embodiment, the slider 1 has an air inflow end 2, an air outflow end 3, and an air bearing surface 4, as shown in the slider flying view of FIG. 6B. As shown in FIG. 6A, the second
When the slider 1 of the embodiment is viewed from the medium facing surface, the air bearing surface 4 has a taper surface 5, a pair of side rails 10, a cross rail 9 connecting the pair of side rails at the air inflow end side, and a pair of side rails with the cross rail 9. Negative pressure groove 1 surrounded by rails
1. A center rail 12 having a magnetic converter 6 near the air outflow end. The pair of side rails 10 has a tapered surface 5
The center rail 12 has a shape that extends from the air outflow end side of the above, is cut before reaching the air outflow end 3, and reaches the air outflow end 3 contrary to the side rail 10. One of the advantages of the slider having such a shape is that the side rails are cut before reaching the air outflow end, and the slider is floated in a posture such that the air inflow end 2 side has a larger floating clearance than the air outflow end 3 side. Therefore, even if the flying posture of the slider is tilted in the width direction, the side rail 10 does not come into contact with the magnetic recording medium 8 before the center rail 12, and the vicinity of the air outflow end of the center rail 12 always has the minimum floating clearance. As a result, the roll rigidity of the slider can be apparently increased. However, when the slider is designed under the conditions described in the first embodiment, the center rail 12
The magnetic recording clearance hg at the position of the magnetic recording / reproducing gap 7 formed above substantially matches the minimum floating clearance hmin, and the values of the floating clearances hs and hmin on the air outflow end side of the side rail 10 approach each other. Will end up. Since the slider 1 flies over the entire circumference of the magnetic recording medium 8,
The inflow direction of air to the slider changes depending on the flying position, and a flying unbalance Δhy in the slider width direction occurs in the flying clearance. As mentioned above, hs and h
If the difference in min is small and Δhy is large, hs and h
It is possible that the magnitude relationship of min is reversed and hs becomes smaller. In that case, the magnetic converter 6 is mounted on the center rail 12, and the advantage that the position is always the minimum floating clearance is lost. In order to avoid this, the side rail 10 is further cut so that the side rail does not come into contact with the slider even if the slider is tilted, or the floating clearance on the air inflow end 2 side is increased to increase the side rail. A method of increasing the floating clearance on the air outflow end side of 10 can be considered. However, the former is not preferable because it has a problem that the roll rigidity of the slider becomes small, and the latter has a problem that the difference between the magnetic recording clearance hg and the minimum floating clearance hmin becomes large. Therefore,
In this embodiment, the crown height δx as described in the first embodiment is formed in the longitudinal direction of the slider, and then the positive camber having the camber height δy is formed also in the lateral direction.

【0036】この短手方向のキャンバ高さδyは図7及
び図8に示すようにスライダ1が磁気記録媒体8上で最
も傾いた状態における一対のサイドレール10の空気流
出端側の浮上すきまをそれぞれhs1、hs2とおけ
ば、 Δhy = | hs1 - hs2 | /2 < δy (7) となるように形成すれば、必ず磁気記録すきまhgが最
小浮上すきまhminと実質的に一致した上で、サイド
レール側が最小浮上すきまとることもなく、センタレー
ル方式のスライダの利点を失うことがない。
As shown in FIGS. 7 and 8, the camber height δy in the lateral direction is the floating clearance of the pair of side rails 10 on the air outflow end side when the slider 1 is most inclined on the magnetic recording medium 8. If hs1 and hs2 are written so that Δhy = | hs1-hs2 | / 2 <δy (7), the magnetic recording clearance hg will always be substantially the same as the minimum floating clearance hmin, and the side There is no minimum floating clearance on the rail side, and the advantages of the center rail type slider are not lost.

【0037】例えば図6で示したようなスライダ形状を
考えた場合、lx=1.25mm、lg=30μm、h
f=40nm、hin=500nm、δx=120.8
nmならば、磁気記録/再生ギャップ位置すなわち空気
流出端から30μmの位置における磁気記録すきまhg
は、最小浮上すきまhminと一致し、hg=hmin
=39.72nmとなるが、サイドレールがカットされ
ている位置が空気流出端から150μmの位置とすれ
ば、ここでの浮上すきまはhs=44.17nmとな
る。この浮上状態では、磁気記録すきまhgが最小浮上
すきまhminとなり、本発明の利点およびセンタレー
ル方式の利点が生かされる。ところが、もしスライダが
磁気記録媒体のある半径位置で、例えばスライダの全幅
にわたりΔhy=10nm傾けば、サイドレールの空気
流出端側が最小浮上すきまとなってしまう。スライダ幅
方向に10nm程度の傾きは容易に起こりうる。そこ
で、例えばスライダにキャンバ高さδy=5nmの正キ
ャンバをスライダの短手方向に形成することで、サイド
レール流出端の浮上すきまはほぼ5nm大きくなり、ス
ライダがキャンバを設ける前と同じだけ傾いてもサイド
レールの空気流出端が最小浮上すきまとなることはな
く、本発明の効果とセンタレールに磁気変換器を備えた
ことの利点の両方を満足することができる。
For example, considering a slider shape as shown in FIG. 6, lx = 1.25 mm, lg = 30 μm, h
f = 40 nm, hin = 500 nm, δx = 120.8
nm, the magnetic recording gap hg at the magnetic recording / reproducing gap position, that is, the position 30 μm from the air outflow end.
Is equal to the minimum floating clearance hmin, and hg = hmin
= 39.72 nm, but if the position where the side rail is cut is 150 μm from the air outflow end, the floating clearance here is hs = 44.17 nm. In this floating state, the magnetic recording clearance hg becomes the minimum floating clearance hmin, and the advantages of the present invention and the center rail system are utilized. However, if the slider is tilted at a certain radial position of the magnetic recording medium, for example, Δhy = 10 nm over the entire width of the slider, the air outflow end side of the side rail becomes the minimum floating clearance. A tilt of about 10 nm in the slider width direction can easily occur. Therefore, for example, by forming a positive camber with a camber height δy = 5 nm on the slider in the lateral direction of the slider, the flying clearance at the outflow end of the side rail is increased by about 5 nm, and the slider is inclined as much as before the camber is provided. However, the air outflow end of the side rail does not have the minimum floating clearance, and both the effect of the present invention and the advantage of providing the center rail with the magnetic converter can be satisfied.

【0038】図9は本発明の第3の実施例を表すスライ
ダの浮上時の側面図を表している。本実施例においては
スライダの空気流出端3をある適当な角度を持って面取
りすることで第1実施例、第2実施例と同様な効果を得
ることができる。
FIG. 9 is a side view of the slider of the third embodiment of the present invention when the slider is flying. In this embodiment, the same effect as in the first and second embodiments can be obtained by chamfering the air outflow end 3 of the slider at an appropriate angle.

【0039】スライダ1の空気流出端3からテーパ面の
空気流出端までの距離をlx、空気流出端3から磁気記
録/再生ギャップ7までの距離をlg、空気流出端3に
おける浮上すきまをhf、テーパ面の空気流出端側の浮
上すきまをhinとすれば、 sin-1{(hin-hf)/(lx-lg)} ≦ θ (8) なる角度θを持って、磁気記録/再生ギャップ7近傍を
面取りすれば、磁気記録すきまhgと最小浮上すきまh
minを実質的に等しくすることができる。特に、スラ
イダ長手方向のクラウン高さδxが (hf-hin)/{6(2lg/lx-1)} < δx (9) の場合にはhgとhminの差が無視できなくなってく
るので、(8)式で定義される面取りを施すことの効果
が顕著になる。
The distance from the air outflow end 3 of the slider 1 to the air outflow end of the tapered surface is lx, the distance from the air outflow end 3 to the magnetic recording / reproducing gap 7 is lg, and the floating clearance at the air outflow end 3 is hf. Assuming that the floating clearance on the air outflow end side of the tapered surface is h in, the magnetic recording / reproducing gap 7 has an angle θ of sin −1 {(hin-hf) / (lx-lg)} ≦ θ (8). By chamfering the vicinity, the magnetic recording clearance hg and the minimum floating clearance h
min can be made substantially equal. Particularly, when the crown height δx in the slider longitudinal direction is (hf-hin) / {6 (2lg / lx-1)} <δx (9), the difference between hg and hmin cannot be ignored, so ( The effect of chamfering defined by the equation (8) becomes remarkable.

【0040】図10は本発明によるスライダを備えた磁
気記憶装置の斜視図である。本発明によるスライダを備
えたことで、スライダの浮上すきまを信頼性を保ちなが
ら狭小化することができ、磁気記憶装置の大容量化を実
現できる。
FIG. 10 is a perspective view of a magnetic memory device having a slider according to the present invention. By providing the slider according to the present invention, the floating clearance of the slider can be narrowed while maintaining reliability, and the capacity of the magnetic storage device can be increased.

【0041】[0041]

【発明の効果】上記のとおり本発明によれば、スライダ
の浮上すきまを信頼性を保ちながら狭小化することがで
き、磁気記憶装置の大容量化を実現できる。
As described above, according to the present invention, the floating clearance of the slider can be narrowed while maintaining reliability, and the capacity of the magnetic storage device can be increased.

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

【図1】本発明の第1実施例に関するスライダの側面
図。
FIG. 1 is a side view of a slider according to a first embodiment of the present invention.

【図2】本発明の第1実施例のクラウンの影響を説明す
るスライダの側面図。
FIG. 2 is a side view of the slider for explaining the influence of the crown of the first embodiment of the present invention.

【図3】本発明の第1実施例の浮上姿勢の影響を説明す
るスライダの側面図。
FIG. 3 is a side view of the slider for explaining the influence of the flying posture according to the first embodiment of the present invention.

【図4】本発明の第1実施例の磁気変換器の位置の影響
を説明するスライダの側面図。
FIG. 4 is a side view of the slider for explaining the influence of the position of the magnetic converter according to the first embodiment of the present invention.

【図5】スライダと磁気記憶媒体の接触状態を説明する
側面図。
FIG. 5 is a side view illustrating a contact state between a slider and a magnetic storage medium.

【図6】本発明の第2実施例に関するスライダの正面図
(a)と本発明の第2実施例に関するスライダの側面図
(b)。
FIG. 6A is a front view of the slider according to the second embodiment of the present invention, and FIG. 6B is a side view of the slider according to the second embodiment of the present invention.

【図7】本発明の第2実施例に関するスライダを後方か
ら見た斜視図。
FIG. 7 is a perspective view of a slider according to a second embodiment of the present invention as viewed from the rear.

【図8】本発明の第2実施例に関するスライダを後端か
ら見た図。
FIG. 8 is a diagram of a slider according to a second embodiment of the present invention viewed from the rear end.

【図9】本発明の第3実施例に関するスライダの側面
図。
FIG. 9 is a side view of the slider according to the third embodiment of the present invention.

【図10】本発明のスライダを備えた磁気記憶装置の斜
視図。
FIG. 10 is a perspective view of a magnetic storage device including the slider of the present invention.

【符号の説明】[Explanation of symbols]

1…スライダ、 2…空気流入端、 3…空気
流出端、4…浮上面、 5…テーパ面、
6…磁気変換器、7…磁気記録/再生ギャップ、
8…磁気記録媒体、9…クロスレール、 10…サイ
ドレール、 11…負圧溝、12…センタレール。
1 ... Slider, 2 ... Air inflow end, 3 ... Air outflow end, 4 ... Air bearing surface, 5 ... Tapered surface,
6 ... Magnetic converter, 7 ... Magnetic recording / reproducing gap,
8 ... Magnetic recording medium, 9 ... Cross rail, 10 ... Side rail, 11 ... Negative pressure groove, 12 ... Center rail.

フロントページの続き (72)発明者 時末 裕充 神奈川県小田原市国府津2880番地 株式会 社日立製作所ストレージシステム事業部内 (72)発明者 菅原 秀一 神奈川県小田原市国府津2880番地 株式会 社日立製作所ストレージシステム事業部内Front Page Continuation (72) Inventor Hiromitsu Togue 2880 Kunizu, Odawara, Kanagawa Stock Storage Company Hitachi Storage Systems Division (72) Inventor Shuichi Sugawara 2880, Kozu, Odawara, Kanagawa Hitachi Storage System Business Department

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】磁気変換器と、前記磁気変換器を備えたス
ライダと、前記スライダに所定の荷重を付与する支持バ
ネと、磁気情報を蓄える磁気記録媒体とからなる磁気記
憶装置において、 前記磁気記憶装置が記録/再生中に前記スライダと前記
磁気記録媒体間にベアリング効果で生じる最小浮上すき
まと、前記磁気変換器の磁気記録/再生ギャップと前記
磁気記録媒体間の距離である磁気記録すきまが実質的に
等しいことを特徴とする磁気記憶装置。
1. A magnetic storage device comprising a magnetic converter, a slider provided with the magnetic converter, a support spring for applying a predetermined load to the slider, and a magnetic recording medium for storing magnetic information. The minimum floating clearance generated by the bearing effect between the slider and the magnetic recording medium during recording / reproduction by the storage device, and the magnetic recording clearance that is the distance between the magnetic recording / reproducing gap of the magnetic converter and the magnetic recording medium are A magnetic storage device characterized by being substantially equal.
【請求項2】磁気変換器と、前記磁気変換器を備えたス
ライダと、前記スライダに所定の荷重を付与する支持バ
ネと、磁気情報を蓄える磁気記録媒体とからなる磁気記
憶装置において、 前記スライダは、空気流入端、空気流出端及び浮上面を
有し、 前記浮上面は前記空気流入端側に形成したテーパ面と、
前記浮上面の長手方向に形成したクラウン高さδxの正
クラウンを有し、 前記正クラウン高さδxと、前記磁気記憶装置が記録/
再生中に前記スライダの空気流出端と前記磁気記録媒体
間にベアリング効果で生じる浮上すきまhfと、前記テ
ーパ面の空気流出端側と前記磁気記録媒体間にベアリン
グ効果で生じる浮上すきまhinと、 前記空気流出端と前記テーパ面の空気流出端側の距離l
xと、前記空気流出端と前記磁気変換器の磁気記録/再
生ギャップ間の距離lgとの間に、 (hf-hin)・lx/{6(2lg-lx)} ≦ δx の関係式が成り立つことを特徴とする磁気記憶装置。
2. A magnetic storage device comprising a magnetic converter, a slider provided with the magnetic converter, a support spring for applying a predetermined load to the slider, and a magnetic recording medium for storing magnetic information, wherein the slider is provided. Has an air inflow end, an air outflow end, and an air bearing surface, and the air bearing surface is a tapered surface formed on the air inflow end side,
A positive crown having a crown height δx formed in the longitudinal direction of the air bearing surface, the positive crown height δx, and
A floating clearance hf generated by a bearing effect between the air outflow end of the slider and the magnetic recording medium during reproduction, and a floating clearance hin generated by a bearing effect between the air outflow end side of the tapered surface and the magnetic recording medium, Distance l between the air outflow end and the air outflow end side of the tapered surface
The relational expression of (hf-hin) · lx / {6 (2lg-lx)} ≤ δx holds between x and the distance lg between the air outflow end and the magnetic recording / reproducing gap of the magnetic transducer. A magnetic storage device characterized by the above.
【請求項3】空気流入端、空気流出端及び浮上面を有
し、 前記浮上面は前記空気流入端側に形成したテーパ面と、
前記浮上面の長手方向に形成したクラウン高さδxの正
クラウンからなり、前記浮上面の任意の位置に磁気記録
/再生ギャップが形成された磁気変換器を備え、磁気記
録媒体上を浮上するスライダにおいて、 前記正クラウン高さδxと、前記磁気記憶装置が記録/
再生中に前記空気流出端と前記磁気記録媒体間にベアリ
ング効果で生じる浮上すきまhfと、前記テーパ面の空
気流出端側と前記磁気記録媒体間にベアリング効果で生
じる浮上すきまhinと、 前記空気流出端と前記テーパ面の空気流出端側の距離l
xと、前記空気流出端と前記磁気記録/再生ギャップ間
の距離lgとの間に、 (hf-hin)・lx/{6(2lg-lx)} ≦ δx の関係式が成り立つことを特徴とするスライダ。
3. An air inflow end, an air outflow end, and an air bearing surface, wherein the air bearing surface is a tapered surface formed on the air inflow end side,
A slider, which is composed of a positive crown having a crown height δx formed in the longitudinal direction of the air bearing surface and has a magnetic recording / reproducing gap formed at an arbitrary position on the air bearing surface, and which floats on a magnetic recording medium. At the positive crown height δx,
A floating clearance hf generated by a bearing effect between the air outflow end and the magnetic recording medium during reproduction, a floating clearance hin generated by a bearing effect between the air outflow end side of the tapered surface and the magnetic recording medium, and the air outflow The distance l between the end and the taper surface on the air outflow end side
The relational expression of (hf-hin) · lx / {6 (2lg-lx)} ≤ δx is established between x and the distance lg between the air outflow end and the magnetic recording / reproducing gap. The slider to do.
【請求項4】空気流入端、空気流出端及び浮上面を有
し、 前記浮上面は前記空気流入端側に形成したテーパ面と、
前記浮上面の長手方向に形成したクラウン高さδxの正
クラウンからなり、前記浮上面の任意の位置に磁気記録
/再生ギャップが形成された磁気変換器を備え、磁気記
録媒体上を浮上するスライダにおいて、 前記正クラウン高さδxと、前記磁気記憶装置が記録/
再生中に前記空気流出端と前記磁気記録媒体間にベアリ
ング効果で生じる浮上すきまhfと、前記テーパ面の空
気流出端側と前記磁気記録媒体間にベアリング効果で生
じる浮上すきまhinと、 前記空気流出端と前記テーパ面の空気流出端側の距離l
xと、前記空気流出端と前記磁気記録/再生ギャップ間
の距離lgとの間に、 (hf-hin)・lx/{6(2lg-lx)} ≦ δx ≦ (hin+hf)/4+1
/2・(hin・hf)1/2 の関係式が成り立つことを特徴とするスライダ。
4. An air inflow end, an air outflow end, and an air bearing surface, wherein the air bearing surface is a tapered surface formed on the air inflow end side.
A slider, which is composed of a positive crown having a crown height δx formed in the longitudinal direction of the air bearing surface and has a magnetic recording / reproducing gap formed at an arbitrary position on the air bearing surface, and which floats on a magnetic recording medium. At the positive crown height δx,
A floating clearance hf generated by a bearing effect between the air outflow end and the magnetic recording medium during reproduction, a floating clearance hin generated by a bearing effect between the air outflow end side of the tapered surface and the magnetic recording medium, and the air outflow The distance l between the end and the taper surface on the air outflow end side
between x and the distance lg between the air outflow end and the magnetic recording / reproducing gap, (hf-hin) · lx / {6 (2lg-lx)} ≤ δx ≤ (hin + hf) / 4 + 1
A slider characterized in that the relational expression of / 2 · (hin · hf) 1/2 holds.
【請求項5】空気流入端、空気流出端及び浮上面を有
し、 前記浮上面は前記空気流入端側に形成したテーパ面と、
前記空気流入端側から前記空気流出端側に延び、かつ前
記空気流出端まで到達しない一対のサイドレールと、前
記空気流入端側から前記空気流出端側に延び、かつ前記
空気流出端に到達する一つのセンタレールと、前記浮上
面の長手方向に形成されたクラウン高さδxの正クラウ
ンと、前記浮上面の短手方向に形成されたキャンバ高さ
δyの正ギャンバとからなり、前記センタレールの前記
空気流出端近傍に磁気変換器が備えられ、磁気記録媒体
上を浮上するスライダにおいて、 前記正クラウン高さδxと、前記スライダを備えた磁気
記憶装置が記録/再生中に、前記空気流出端と前記磁気
記録媒体間にベアリング効果で生じる浮上すきまhf
と、前記テーパ面の空気流出端側と前記磁気記録媒体間
にベアリング効果で生じる浮上すきまhinと、 前記空気流出端と前記テーパ面の空気流出端側の距離l
xと、前記スライダの空気流出端と前記磁気記録/再生
ギャップ間の距離lgとの間に、 (hf-hin)・lx/{6(2lg-lx)} ≦ δx ≦ (hin+hf)/4+1
/2・(hin・hf)1/2 の関係式が成り立ち、かつ前記正キャンバ高さδyと、
前記スライダを備えた磁気記憶装置が記録/再生中に、
前記スライダが短手方向に最も傾いた場合の傾き量Δh
yとの間に、 Δhy/2 ≦ δy の関係式が成り立つことを特徴とするスライダ。
5. An air inflow end, an air outflow end, and an air bearing surface, wherein the air bearing surface is a tapered surface formed on the air inflow end side,
A pair of side rails extending from the air inflow end side to the air outflow end side and not reaching the air outflow end, and a pair of side rails extending from the air inflow end side to the air outflow end side and reaching the air outflow end. The center rail comprises one center rail, a positive crown having a crown height δx formed in the longitudinal direction of the air bearing surface, and a positive gamba having a camber height δy formed in the lateral direction of the air bearing surface. A magnetic converter is provided in the vicinity of the air outflow end of the slider, and the slider floats above the magnetic recording medium. The air outflow is generated during the recording / reproducing of the positive crown height δx and the magnetic storage device including the slider. The floating clearance hf between the edge and the magnetic recording medium due to the bearing effect
And a floating clearance h in between the air outflow end side of the tapered surface and the magnetic recording medium due to a bearing effect, and a distance l between the air outflow end and the air outflow end side of the tapered surface.
x and the distance lg between the air outflow end of the slider and the magnetic recording / reproducing gap, (hf-hin) · lx / {6 (2lg-lx)} ≤ δx ≤ (hin + hf) / 4 + 1
The relational expression of / 2 · (hin · hf) 1/2 holds, and the positive camber height δy,
During recording / reproduction by the magnetic storage device having the slider,
Inclination amount Δh when the slider is most inclined in the lateral direction
A slider having a relational expression of Δhy / 2 ≤ δy with y.
【請求項6】空気流入端、空気流出端及び浮上面を有
し、 前記浮上面は前記空気流入端側に形成したテーパ面と、
前記浮上面の長手方向に形成したクラウン高さδxの正
クラウンからなり、前記浮上面の任意の位置に磁気記録
/再生ギャップが形成された磁気変換器を備え、磁気記
録媒体上を浮上するスライダにおいて、 前記クラウン高さδxと、前記スライダを備えた磁気記
憶装置が記録/再生中に、前記空気流出端と前記磁気記
録媒体間にベアリング効果で生じる浮上すきまhfと、
前記テーパ面の空気流出端側と前記磁気記録媒体間にベ
アリング効果で生じる浮上すきまhinと、前記空気流
出端と前記テーパ面の空気流出端側の距離lxと、前記
空気流出端と前記磁気記録/再生ギャップ間の距離lg
との間に、 0 < δx < (hf-hin)・lx/{6(2lg-lx)} の関係式が成り立ち、かつ前記空気流出端を前記磁気記
録/再生ギャップ近傍において sin-1{(hin-hf)/(lx-lg)} ≦ θ の角度θを持って面取りしたことを特徴とするスライ
ダ。
6. An air inflow end, an air outflow end, and an air bearing surface, wherein the air bearing surface is a tapered surface formed on the air inflow end side,
A slider, which is composed of a positive crown having a crown height δx formed in the longitudinal direction of the air bearing surface and has a magnetic recording / reproducing gap formed at an arbitrary position on the air bearing surface, and which floats on a magnetic recording medium. In the above, the crown height δx, and a flying clearance hf generated by a bearing effect between the air outflow end and the magnetic recording medium during recording / reproduction by the magnetic storage device including the slider,
A floating clearance h in between the air outflow end side of the tapered surface and the magnetic recording medium, a distance lx between the air outflow end and the air outflow end side of the tapered surface, the air outflow end and the magnetic recording. / Distance between playback gaps lg
, And the relational expression of 0 <δx <(hf-hin) · lx / {6 (2lg-lx)} holds, and the air outflow end is located near the magnetic recording / reproducing gap by sin −1 {(( (hin-hf) / (lx-lg)} ≤ θ The chamfer with an angle θ.
JP28167894A 1994-11-16 1994-11-16 Magnetic storage device and its slider Pending JPH08147917A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28167894A JPH08147917A (en) 1994-11-16 1994-11-16 Magnetic storage device and its slider

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28167894A JPH08147917A (en) 1994-11-16 1994-11-16 Magnetic storage device and its slider

Publications (1)

Publication Number Publication Date
JPH08147917A true JPH08147917A (en) 1996-06-07

Family

ID=17642465

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28167894A Pending JPH08147917A (en) 1994-11-16 1994-11-16 Magnetic storage device and its slider

Country Status (1)

Country Link
JP (1) JPH08147917A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6349018B2 (en) 1998-09-28 2002-02-19 Fujitsu Limited Negative pressure air bearing slider
US6351345B1 (en) 1999-01-12 2002-02-26 Fujitsu Limited Air bearing slider and method of producing the same

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6349018B2 (en) 1998-09-28 2002-02-19 Fujitsu Limited Negative pressure air bearing slider
US6396664B2 (en) 1998-09-28 2002-05-28 Fujitsu Limited Negative pressure air bearing slider
US6351345B1 (en) 1999-01-12 2002-02-26 Fujitsu Limited Air bearing slider and method of producing the same

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