JPS62164204A - floating head slider - Google Patents
floating head sliderInfo
- Publication number
- JPS62164204A JPS62164204A JP492486A JP492486A JPS62164204A JP S62164204 A JPS62164204 A JP S62164204A JP 492486 A JP492486 A JP 492486A JP 492486 A JP492486 A JP 492486A JP S62164204 A JPS62164204 A JP S62164204A
- Authority
- JP
- Japan
- Prior art keywords
- head slider
- floating head
- floating
- magnetic disk
- angle
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 230000007423 decrease Effects 0.000 claims description 5
- 238000005339 levitation Methods 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000004904 shortening Methods 0.000 description 2
- 238000000034 method Methods 0.000 description 1
- 238000005096 rolling process Methods 0.000 description 1
- 230000000087 stabilizing effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/48—Disposition or mounting of heads or head supports relative to record carriers ; arrangements of heads, e.g. for scanning the record carrier to increase the relative speed
- G11B5/58—Disposition or mounting of heads or head supports relative to record carriers ; arrangements of heads, e.g. for scanning the record carrier to increase the relative speed with provision for moving the head for the purpose of maintaining alignment of the head relative to the record carrier during transducing operation, e.g. to compensate for surface irregularities of the latter or for track following
- G11B5/60—Fluid-dynamic spacing of heads from record-carriers
- G11B5/6005—Specially adapted for spacing from a rotating disc using a fluid cushion
Landscapes
- Adjustment Of The Magnetic Head Position Track Following On Tapes (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は浮動ヘッドスライダに係り、特にYAW角特性
を持ったスイングアーム方式磁気ディスク装置において
浮上高さの低下と変動を低減させるに好適な浮動ヘッド
スライダに関する。[Detailed Description of the Invention] [Field of Application of the Invention] The present invention relates to a floating head slider, and in particular, a floating head slider suitable for reducing the drop and fluctuation of flying height in a swing arm type magnetic disk drive having YAW angle characteristics. Regarding the head slider.
磁気ディスク装置用の浮動ヘッドスライダを磁気ディス
クと微少空隙を保って浮上させる方法のスイングアーム
方式の従来のスライダは、例えば特開昭60−2278
2号に示されている。この浮動ヘッドスライダ1は、第
4図に示すように、浮上用レール面2a、2b、空気流
入用勾配面3a、3bから構成されている。A conventional slider using a swing arm method for floating a floating head slider for a magnetic disk device while maintaining a small gap with the magnetic disk is disclosed in, for example, Japanese Patent Laid-Open No. 60-2278.
It is shown in No. 2. As shown in FIG. 4, the floating head slider 1 is composed of floating rail surfaces 2a, 2b and air inflow slope surfaces 3a, 3b.
磁気ディスクの回転で生ずる空気流の圧力分布は、スラ
イダの前後に2つの正圧発生部が得られるために、かな
り安定した浮上高さとなる。しかし、スイングアームの
移動によって、スライダ1のYAW角が変わり、流入空
気の圧力損失が大きくなり、スライダ1の浮上高さは、
第3図中曲線■で示すように、磁気ディスクの半径位置
に応じて変化する。スライダ1のYAW角とスライダ1
の浮上高さとは、YAW角O度の位置で浮上高さが最も
大きく、YAW角が例く内周位nで浮上高さが最も小ざ
くなる関係にある。The pressure distribution of the air flow generated by the rotation of the magnetic disk has two positive pressure generating parts before and after the slider, resulting in a fairly stable flying height. However, as the swing arm moves, the YAW angle of the slider 1 changes, the pressure loss of the incoming air increases, and the flying height of the slider 1 changes.
As shown by the curve ■ in FIG. 3, it changes depending on the radial position of the magnetic disk. YAW angle of slider 1 and slider 1
The relationship is such that the flying height is greatest at a YAW angle of 0 degrees, and the flying height is smallest at a YAW angle of, for example, the inner circumferential position n.
このように従来のスライダ1では、スイングア−ムの移
動によって浮上高さは放物線を描ぎ、浮上高さの変動を
生ずる。なお、浮上高さが変動力るど、スライダの浮上
状況が不安定となり、スライダが磁気ディスクに接触し
て磁気ディスクの磁性膜を破壊し、磁気ディスクの寿命
を短くしてしまう。As described above, in the conventional slider 1, the flying height draws a parabola due to the movement of the swing arm, causing fluctuations in the flying height. Note that as the flying height fluctuates, the flying condition of the slider becomes unstable, and the slider comes into contact with the magnetic disk, destroying the magnetic film of the magnetic disk and shortening the life of the magnetic disk.
本発明の目的はスイングアームの移動によって、浮動ヘ
ッドスライダにYAW角が何き、これににる流入空気の
圧力損失によって生ずる磁気ディスクの内周位置での浮
上高さの低下を少なくし、磁気ディスクの半径位置によ
る浮上高さ変動を抑えるに好適な浮動ヘッドスライダを
提供することにある。An object of the present invention is to reduce the drop in flying height at the inner circumferential position of the magnetic disk caused by the YAW angle of the floating head slider due to the movement of the swing arm, and the pressure loss of the incoming air. An object of the present invention is to provide a floating head slider suitable for suppressing fluctuations in flying height depending on the radial position of a disk.
本発明は、浮上用レールを空気流入端に垂直な線に対し
て角度を刊けて形成し、このJ:うに形成された浮上用
レールにより浮上高さの変動を抑えるように構成したも
のである。In the present invention, the levitation rail is formed at an angle to a line perpendicular to the air inflow end, and the levitation rail is configured to suppress fluctuations in the levitation height. be.
以下、本発明の一実施例を第1図乃至第3図により説明
する。An embodiment of the present invention will be described below with reference to FIGS. 1 to 3.
第1図は浮動ヘッドスライダ10を示す。スライダ10
は、空気流入端11に対して垂直な線2に対して角度α
を持った一対の浮上用レール面12と、空気流入勾配面
13及び書込、読出ができるギャップ部14を有するセ
ンターレール15で構成されている。FIG. 1 shows a floating head slider 10. FIG. slider 10
is the angle α with respect to the line 2 perpendicular to the air inflow end 11
The center rail 15 includes a pair of floating rail surfaces 12 having an air inflow slope surface 13 and a gap portion 14 that allows writing and reading.
第2図は第1図で用いた浮動ヘッドスライダ10がスイ
ングアーム16の軸17を中心とする回動によって、磁
気ディスク18上に描く軌跡19とスライダ10のYA
W角を表わしたモデル図である。FIG. 2 shows a trajectory 19 drawn on a magnetic disk 18 by the floating head slider 10 used in FIG.
It is a model diagram showing the W angle.
第1図で浮動ヘッドスライダ10の中央部に押付筒1i
Fが働き、スライダ10のピッチング及びローリング運
動を許容する。第2図で磁気ディスク18の矢印六方向
の回転により浮上用レール面12と磁気ディスク18と
の間に空気が引込まれて圧力を発生させ、スライダ10
を浮上させる。In FIG. 1, a cylinder 1i is pressed into the center of the floating head slider 10.
F acts to permit pitching and rolling motion of the slider 10. In FIG. 2, as the magnetic disk 18 rotates in the six directions of arrows, air is drawn between the floating rail surface 12 and the magnetic disk 18 to generate pressure, and the slider 10
surface.
スイングアーム16は従来と同様の構成であり、浮動ヘ
ッドスライダ10は、従来の浮動ヘッドスライダと同様
にスイングアーム16に取りイ(1けである。浮動ヘッ
ドスライダ10は、第2図中、P+ (磁気ディスク
18の内周位置)、β3 (外周位置)で示す位置の間
を往復移動する。β2はPlとβ3との中間の位置を示
す。β2を通る磁気ディスク18の中心線を1で示す。The swing arm 16 has the same configuration as the conventional one, and the floating head slider 10 has only one attachment point on the swing arm 16 like the conventional floating head slider. (inner circumferential position of the magnetic disk 18) and β3 (outer circumferential position). β2 indicates the intermediate position between Pl and β3. The center line of the magnetic disk 18 passing through β2 is show.
上記の浮動ヘッドスライダ10によれば、浮上用レール
面12の中心線CLは、浮動ヘッドスライダ10がPl
に位置するときには、ディスク中心線りに対する角度は
β1であり、浮動ヘッドスライダ10がβ2に到ると上
記角度はβ2となり更に浮動ヘッドスライダ10がβ3
に到ると上記角度β3となる。こ)で、β1〈β2〈β
3の関係にある。また、上記角度αは、浮動ヘッドスラ
イダ10がPlに位置するときに、上記角度β1が90
度となるように定めてあり、β1は90度である。また
角度β1 (β2.β3)より90度を減算した角度を
YAW角θというとすると、Y△W角は、浮動ヘッドス
ライダ10′h<P+に位置するとぎに零となり、β2
、β3と移動するにつれて増す。According to the above floating head slider 10, the center line CL of the floating rail surface 12 is
When the floating head slider 10 is located at β2, the angle with respect to the disk center line is β1, and when the floating head slider 10 reaches β2, the angle becomes β2, and the floating head slider 10 is at β3.
When the angle β3 is reached, the angle β3 is reached. ), β1〈β2〈β
There is a relationship of 3. Further, the angle α is such that when the floating head slider 10 is located at Pl, the angle β1 is 90°.
β1 is 90 degrees. Also, if the angle obtained by subtracting 90 degrees from the angle β1 (β2.β3) is the YAW angle θ, then the Y△W angle becomes zero when the floating head slider 10'h<P+, and β2
, β3.
こ)でYAW角θと流入空気の圧力損失及び圧力発生効
率との関係についてみると、YAW角が零のとき、圧力
損失が最小となり、圧力発生効率が最大となり、YAW
角が増えるにつれて圧力損失が増え、圧力発生効率が減
る。Looking at the relationship between the YAW angle θ and the pressure loss and pressure generation efficiency of the incoming air, when the YAW angle is zero, the pressure loss is the minimum, the pressure generation efficiency is the maximum, and the YAW
As the angle increases, pressure loss increases and pressure generation efficiency decreases.
本実施例によれば、浮動ヘッドスライダ10が磁気ディ
スク18の内周側に位置しているとぎに、流入空気の圧
力発生効率が最大となり、浮上高さは従来より増し、第
3図中点m1からnlに移る。According to this embodiment, when the floating head slider 10 is located on the inner circumferential side of the magnetic disk 18, the pressure generation efficiency of the incoming air becomes maximum, and the flying height is increased compared to the conventional one, and the midpoint in FIG. Move from m1 to nl.
スライダ10がPlに位置するときに、上記角度β1が
90度となるように定めてあり、β1は90度である。The angle β1 is set to be 90 degrees when the slider 10 is located at Pl, and β1 is 90 degrees.
また角度β1 (β2.β3)より90度を減算した角
度をYAW角θというとすると、YAW角は、浮動ヘッ
ドスライダ10がPlに位置するときに零となり、β2
、β3と移動するにつれて増す。Furthermore, if the angle obtained by subtracting 90 degrees from the angle β1 (β2.β3) is the YAW angle θ, the YAW angle becomes zero when the floating head slider 10 is located at Pl, and β2
, β3.
こ)でYAW角θと流入空気の圧力損失及び圧力発生効
率との関係についてみると、YΔW角が−〇 −
零のどき、圧ツノ損失が最小となり、圧力発生効率が最
大どなり、Y A W角が増えるにつれて圧力損失が増
え、圧力発生効率が減る。Looking at the relationship between the YAW angle θ and the pressure loss and pressure generation efficiency of the incoming air, we see that when the YΔW angle is -〇 - zero, the pressure horn loss is at its minimum and the pressure generation efficiency is at its maximum. As the angle increases, pressure loss increases and pressure generation efficiency decreases.
本実施例によれば、浮動ヘッドスライダ10が磁気ディ
スク18の内周側に位置しているとぎに、流入空気の圧
力発生効率が最大となり、浮上高さは従来より増し、第
3図中点m1からnlに移る。According to this embodiment, when the floating head slider 10 is located on the inner circumferential side of the magnetic disk 18, the pressure generation efficiency of the incoming air becomes maximum, and the flying height is increased compared to the conventional one, and the midpoint in FIG. Move from m1 to nl.
浮動ヘッドスライダ101J<11気デイスク18の外
周側に移動するにつれで、流入空気の圧力発生効率は低
下し、約145mの磁気ディスク半径位置で従来と略同
程瓜となり、浮動ヘッドスライダ10の浮上高さは従来
と略等しくなる。浮動ヘッドスライダ10が更に外周側
に移動すると、流入空気の圧力発生効率は更に低下し、
浮動ヘッドスライダ10の浮上高さは従来より減り、第
3図中点m2からnlに移る。Floating head slider 101J The height will be approximately the same as before. As the floating head slider 10 moves further toward the outer circumference, the pressure generation efficiency of the incoming air further decreases.
The flying height of the floating head slider 10 is reduced compared to the conventional one, and moves from the midpoint m2 in FIG. 3 to nl.
このように、浮動ヘッドスライダ10の浮上高さは、従
来に比べて、磁気ディスク18の内周側では増し、外周
側では減り、第3図中曲線■で示寸如くになる。同図よ
り分かるように、スイングアーム16の移動による浮上
ヘッドスライダ10の浮上高さ変動が小さくなり、浮上
ヘッドスライダ10は安定に動作し、浮動ヘッドスライ
ダ10が磁気ディスク18に不要に接触して磁性膜を壊
ずにうな不都合は確実に回避出来、磁気ディスク18の
寿命が不当に短くなってしまうようなことは無くなる。As described above, the flying height of the floating head slider 10 increases on the inner circumferential side of the magnetic disk 18 and decreases on the outer circumferential side, as shown by the curve 3 in FIG. 3, compared to the conventional one. As can be seen from the figure, fluctuations in the flying height of the flying head slider 10 due to movement of the swing arm 16 are reduced, the flying head slider 10 operates stably, and the floating head slider 10 is prevented from unnecessary contact with the magnetic disk 18. Such inconveniences can be reliably avoided without damaging the magnetic film, and the life of the magnetic disk 18 will not be unduly shortened.
本発明によれば、浮上用レールに作用する流入空気の圧
力発生効率が、浮動ヘッドスライダが磁気ディスク内周
側に位置するときに、最大となり、浮動ヘッドスライダ
が磁気ディスクの外周側に移動するにつれて減する構成
であるため、磁気ディスクの内周位置での浮上高さの低
下を少なくでき1つ磁気ディスクの外周位置での浮上高
さを抑えることができ、然して、浮動ヘッドスライダの
移動範囲に亘って浮上高さが略一定となり、浮上高さの
変動を抑えることが出来、浮動ヘッドスライダの動作が
安定化し、浮動ヘッドスライダが磁気ディスクに接触し
て磁性面を破壊して磁気ディスクの寿命を不当に短くし
てしまうという不都合を回避出来るという効果がある。According to the present invention, the pressure generation efficiency of the incoming air acting on the floating rail is maximized when the floating head slider is located on the inner circumferential side of the magnetic disk, and the floating head slider moves toward the outer circumferential side of the magnetic disk. Since it is configured to reduce the flying height at the inner circumferential position of the magnetic disk, it is possible to suppress the flying height at the outer circumferential position of the magnetic disk, thereby reducing the movement range of the floating head slider. The flying height remains approximately constant over the period of time, suppressing fluctuations in the flying height, and stabilizing the operation of the floating head slider. This has the effect of avoiding the inconvenience of unduly shortening the lifespan.
第1図は本発明の浮動ヘッドスライダの一実施例を上下
反転して示す斜視図、第2図は第1図の浮動ヘッドスラ
イダの実装状態を拡大して表わすモデル図、第3図は第
1図の浮動ヘッドスライダの浮上高さの特性を従来の浮
動ヘッドスライダの浮上高さの特性と併せて示す図、第
4図は従来の浮動ヘッドスライダの1例の斜視図である
。
10・・・浮動ヘッドスライダ、11・・・空気流入端
、12・・・浮上用レール面、13・・・空気流入勾配
面、14・・・ギャップ部、15・・・センターレール
、16・・・スイングアーム、18・・・磁気ディスク
、19・・・軌跡。
第1図FIG. 1 is a perspective view showing an embodiment of the floating head slider of the present invention upside down, FIG. 2 is an enlarged model diagram showing the mounted state of the floating head slider of FIG. 1, and FIG. FIG. 4 is a perspective view of an example of the conventional floating head slider. DESCRIPTION OF SYMBOLS 10... Floating head slider, 11... Air inflow end, 12... Rail surface for floating, 13... Air inflow slope surface, 14... Gap part, 15... Center rail, 16... ...Swing arm, 18...Magnetic disk, 19...Trajectory. Figure 1
Claims (1)
流入用勾配面と浮上用レール面より成る浮動ヘッドスラ
イダにおいて、該浮動ヘッドスライダが上記磁気ディス
クの内周側に位置するときに流入空気の圧力発生効率が
最大となり、該浮動ヘッドスライダが上記磁気ディスク
の外周側に移動するにつれて、上記流入空気の圧力効率
が減ずるように、浮上用レールを、空気流入端に対して
垂直な線に対して角度をもたせて設けてなることを特徴
とする浮動ヘッドスライダ。In a floating head slider consisting of an air inflow slope surface and a floating rail surface for maintaining a minute air gap with a magnetic disk and floating the disk, when the floating head slider is located on the inner circumferential side of the magnetic disk, the pressure of the inflowing air increases. The floating rail is aligned with a line perpendicular to the air inflow end so that the generation efficiency is maximized and the pressure efficiency of the inflow air decreases as the floating head slider moves toward the outer periphery of the magnetic disk. A floating head slider characterized by being provided at an angle.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP492486A JPS62164204A (en) | 1986-01-16 | 1986-01-16 | floating head slider |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP492486A JPS62164204A (en) | 1986-01-16 | 1986-01-16 | floating head slider |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62164204A true JPS62164204A (en) | 1987-07-20 |
Family
ID=11597152
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP492486A Pending JPS62164204A (en) | 1986-01-16 | 1986-01-16 | floating head slider |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62164204A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01320690A (en) * | 1988-06-13 | 1989-12-26 | Internatl Business Mach Corp <Ibm> | Magnetic disc driver |
US5086360A (en) * | 1990-09-06 | 1992-02-04 | Applied Magnetics Corporation | Constant flying height slider |
US5625513A (en) * | 1994-11-14 | 1997-04-29 | Nec Corporation | Floating head slider having uniform spacing from recording medium surface |
US6128162A (en) * | 1997-06-26 | 2000-10-03 | Fujitsu Limited | Head slider with constant flying height over sliding range |
-
1986
- 1986-01-16 JP JP492486A patent/JPS62164204A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01320690A (en) * | 1988-06-13 | 1989-12-26 | Internatl Business Mach Corp <Ibm> | Magnetic disc driver |
US5086360A (en) * | 1990-09-06 | 1992-02-04 | Applied Magnetics Corporation | Constant flying height slider |
US5625513A (en) * | 1994-11-14 | 1997-04-29 | Nec Corporation | Floating head slider having uniform spacing from recording medium surface |
US6128162A (en) * | 1997-06-26 | 2000-10-03 | Fujitsu Limited | Head slider with constant flying height over sliding range |
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