JPS5918780B2 - Adsorption floating magnetic head - Google Patents
Adsorption floating magnetic headInfo
- Publication number
- JPS5918780B2 JPS5918780B2 JP6950275A JP6950275A JPS5918780B2 JP S5918780 B2 JPS5918780 B2 JP S5918780B2 JP 6950275 A JP6950275 A JP 6950275A JP 6950275 A JP6950275 A JP 6950275A JP S5918780 B2 JPS5918780 B2 JP S5918780B2
- Authority
- JP
- Japan
- Prior art keywords
- floating
- magnetic head
- suction
- air
- attack
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Landscapes
- Adjustment Of The Magnetic Head Position Track Following On Tapes (AREA)
- Supporting Of Heads In Record-Carrier Devices (AREA)
Description
【発明の詳細な説明】
この発明は、磁気ディスクの回転の起動、停止において
、磁気ディスクに接触して離着陸する浮動形磁気ヘッド
に係る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a floating magnetic head that takes off and lands in contact with a magnetic disk when starting and stopping the rotation of the magnetic disk.
磁気ディスクに離着陸する浮動形磁気ヘッドをコンタク
トスタートストップ(constactstartst
op;C、S−S)形磁気ヘッドと呼び、従来の浮動形
磁気ヘッドのごとき、空気ベアリングを発生させるため
の荷重が大きいためC、S、Sが出来ず、磁気ディスク
が高速定常回転に達してから磁気ヘッドを磁気ディスク
に近づける複雑な荷重機構がないため、装置価格、信頼
度を改善する上で優れた利点を持つている。接触して離
陸するので、スライダおよびディスクの摺動摩耗を少な
くするためには摺動距離をなるべく少なくすることが必
要である。このためにはC、S、Sにおける離着陸速度
がなるべく低いことも必要である。磁気ディスクの低速
時におけるスライダ浮力が大きいことは離着陸速度が低
いことを意味するが、磁気ディスクが高速定常速度にな
つた時は大きな浮力を発生することになり、一定の荷重
ではこれと釣合うための浮上量すなわち、磁気ディスク
とスライダのスペーシングは非常に大きくなる。A floating magnetic head that takes off and lands on a magnetic disk is connected to a contact start/stop.
It is called a C, S-S) type magnetic head, and unlike conventional floating magnetic heads, the load to generate air bearings is large, so C, S, and S cannot be performed, and the magnetic disk cannot rotate at high speed and steady. Since there is no complicated loading mechanism that brings the magnetic head closer to the magnetic disk after reaching the magnetic disk, it has excellent advantages in terms of improving device cost and reliability. Since they make contact and take off, it is necessary to reduce the sliding distance as much as possible in order to reduce the sliding wear on the slider and disk. For this purpose, it is also necessary that the takeoff and landing speeds in C, S, and S be as low as possible. A large slider buoyancy force when the magnetic disk is at low speed means that takeoff and landing speeds are low, but when the magnetic disk reaches a high steady speed, it generates a large buoyant force, which is balanced by a constant load. Therefore, the flying height, that is, the spacing between the magnetic disk and the slider becomes very large.
所望のスペーシングを得ようとすると大きな荷重を必要
とし、C、S、S時のスライダの磁気ディスクに対する
接触圧力が多くなり摺動摩耗量を増す。したがつてC、
S、Sにおける離着陸時には大きな浮力を生じて離着陸
速度が下がり、磁気ディスクの高速回転時にも浮力は増
大せず、荷重を大きくしないでも所定のスペーシングが
得られることが望ましい。この発明の目的は、磁気ディ
スクの回転速度が低い範囲では大きな浮力を有し、回転
速度が高い時も浮力が大きくならず、所定のスペーシン
グを荷重を変えることなく得られるような吸着浮動形磁
気ヘッドを得ることである。In order to obtain the desired spacing, a large load is required, and the contact pressure of the slider against the magnetic disk during C, S, and S increases, increasing the amount of sliding wear. Therefore C,
During takeoff and landing at S and S, a large buoyant force is generated to reduce the takeoff and landing speed, and it is desirable that the buoyant force not increase even when the magnetic disk rotates at high speed, and that a predetermined spacing can be obtained without increasing the load. The purpose of this invention is to provide a suction floating type that has a large buoyancy when the rotational speed of the magnetic disk is low, does not increase the buoyancy even when the rotational speed is high, and can obtain a predetermined spacing without changing the load. The objective is to obtain a magnetic head.
本発明の特徴とするところは、記録媒体の移動により生
じる空気粘性層流から浮力を受ける浮動部と、この浮動
部の空気流出端部に支持された磁気ヘッド部とからなる
浮動形磁気ヘッドにおいて、浮動部の空気流入端に形成
された迎え角と、浮動部の記録媒体対向面に正の浮力が
発生するように形成された浮動面と、浮動部の少なくと
も迎え角と浮動面の交点より空気流入端寄りの部分から
浮動部の後端に向つて負の浮力が発生するようテーパ付
けられた吸着面とを具備するところにある。The present invention is characterized by a floating magnetic head consisting of a floating part that receives buoyancy from the air viscous laminar flow generated by the movement of a recording medium, and a magnetic head part supported by the air outflow end of this floating part. , an angle of attack formed at the air inflow end of the floating section, a floating surface formed so as to generate a positive buoyancy force on the surface of the floating section facing the recording medium, and at least the intersection of the angle of attack and the floating surface of the floating section. It has a suction surface that is tapered to generate negative buoyancy from a portion near the air inflow end toward the rear end of the floating section.
以下図面にしたがつてこの発明の実施例を説明する。第
1図において、フェライトなどの磁性材料で作られた磁
気ヘツド部1の磁気回路の一部を司るスライダ2に迎え
角部3、多数の浮動面4を形成し浮動時に正の浮力を持
つ浮動面とする。さらに浮動面4のそれぞれの間に、浮
動時に負の迎え角をもちしたがつて、負の浮力すなわち
吸着力を持つ多数の吸着面5を設ける。吸着面5は迎え
角3と浮動面4との交点13(迎え角4の頂点)より空
気流入端寄りの部分から空気流出端に向けてテーパ付け
られて形成される。このようなスライダ2を、第2図の
ごとくジンバル6に作られた爪7の弾力を用いて、スラ
イダ2に設けた溝8に固定し、かつ支持する。第2図に
は具体的に示してないが、スプリングなどの撓みによる
圧力を荷重9としてスライダ2に加えておく。磁気デイ
スク10を矢印11の方向に回転させると、磁気デイス
ク上に塗布された磁気記録媒体であるコーテイング12
の土をスライダ2の浮動面4が摺動し始める。Embodiments of the present invention will be described below with reference to the drawings. In Fig. 1, a slider 2, which controls a part of the magnetic circuit of a magnetic head part 1 made of a magnetic material such as ferrite, has an angle of attack part 3 and a number of floating surfaces 4, and has a positive buoyancy when floating. Make it a face. Further, between each of the floating surfaces 4, a large number of suction surfaces 5 are provided which have a negative angle of attack when floating and therefore have a negative buoyancy, that is, a suction force. The suction surface 5 is tapered from a portion closer to the air inflow end than an intersection 13 between the attack angle 3 and the floating surface 4 (the apex of the attack angle 4) toward the air outflow end. Such a slider 2 is fixed and supported in a groove 8 provided in the slider 2 by using the elasticity of a claw 7 formed in a gimbal 6 as shown in FIG. Although not specifically shown in FIG. 2, pressure due to deflection of a spring or the like is applied to the slider 2 as a load 9. When the magnetic disk 10 is rotated in the direction of the arrow 11, a coating 12 which is a magnetic recording medium applied on the magnetic disk
The floating surface 4 of the slider 2 begins to slide on the soil.
次第に周速が上り、浮動面4に生ずる空気粘性層流によ
る圧力分布は第3図のようになる。圧力はスライダ2の
先端の大気圧から始まつて、迎え角部3の頂点13で空
気が圧縮されることによつて最大になり、浮動面4に入
ると一旦減少し、後端14で再び最大になることが知ら
れている。As the circumferential speed gradually increases, the pressure distribution due to the air viscous laminar flow generated on the floating surface 4 becomes as shown in FIG. The pressure starts from atmospheric pressure at the tip of the slider 2, reaches a maximum at the apex 13 of the angle of attack 3 due to air being compressed, decreases once entering the floating surface 4, and then returns to the rear end 14. known to be the largest.
磁気デイスク10の周速が上がり、スライダ2が浮動し
スペーシング15が遂にコーテイング12における最大
凸起量以上になり離陸する。この時のスペーシングおよ
び最大凸起量は0.025μ程度である。離陸時圧力分
布16に対して吸着面4の吸着圧力分布17は第3図に
示す通りで、負の圧力であるため、離陸時圧力分布16
の正平均値18と吸着圧力分布17の負平均値19の差
による和平均値20と浮動面4、迎え角部3の面積を掛
けたものが浮上刃となり、第2図における荷重と釣合う
。磁気デイスク10が高速定常回転に達すると、圧力分
布は第4図のようになる。The circumferential speed of the magnetic disk 10 increases, the slider 2 floats, and the spacing 15 finally exceeds the maximum convexity of the coating 12 and takes off. The spacing and maximum protrusion amount at this time are approximately 0.025μ. The suction pressure distribution 17 of the suction surface 4 is as shown in FIG. 3 with respect to the take-off pressure distribution 16, which is negative pressure,
The floating blade is obtained by multiplying the sum average value 20 resulting from the difference between the positive average value 18 of the adsorption pressure distribution 17 and the negative average value 19 of the adsorption pressure distribution 17 by the area of the floating surface 4 and the angle of attack part 3, which balances the load in Figure 2. . When the magnetic disk 10 reaches steady rotation at high speed, the pressure distribution becomes as shown in FIG.
浮上刃は定常圧力分布21、定常吸着圧力分布22とな
り、正平均値18と負平均値19の差である和平均値2
0に浮動面積を掛けたものである。ここで和平均値20
は正平均値が大きくなつても吸着面5による吸着圧力分
布17力状きくなり、負平均値19も大きく差である和
平均値20は離陸時の正平均値18とほとんど同じにな
り、所定のスペーシングが得られる。この場合、もし吸
着面5がないとすると浮上刃は極めて大きくなり、大き
な荷重9が必要となることは明かであり、したがつて吸
着面5を設けることによつて、所定のスペーシングを得
るのに荷重を変える必要はない。また吸着面5が迎え角
3の途中から形成されていることにより、吸着面5の最
小すき間は浮動面4の最小すき間に比べて常に十分大き
いため、浮動面4の浮土量の変動に対して吸着面5のす
き間の変動割合は小さい。The floating blade has a steady pressure distribution 21, a steady adsorption pressure distribution 22, and a sum average value 2 which is the difference between the positive average value 18 and the negative average value 19.
0 times the floating area. Here, the sum average value is 20
Even if the positive average value increases, the suction pressure distribution 17 by the suction surface 5 becomes stronger, and the negative average value 19 also has a large difference.The sum average value 20 is almost the same as the positive average value 18 at the time of takeoff, and the predetermined spacing is obtained. In this case, it is clear that if there is no suction surface 5, the floating blade will be extremely large and a large load 9 will be required. Therefore, by providing the suction surface 5, a predetermined spacing can be obtained. There is no need to change the load. In addition, since the suction surface 5 is formed from the middle of the angle of attack 3, the minimum gap of the suction surface 5 is always sufficiently larger than the minimum gap of the floating surface 4, so that it can withstand fluctuations in the amount of floating soil on the floating surface 4. The rate of change in the gap between the suction surfaces 5 is small.
従つて浮上量の変動に対して浮上刃は大きく変動して復
元力を生ずるのに対して、吸着力はほとんど一定の力を
生じ、高い空気膜剛姓が得られる。Therefore, the floating blade fluctuates greatly in response to fluctuations in the flying height, producing a restoring force, whereas the suction force produces a nearly constant force, resulting in high air film rigidity.
第1図はこの発明による吸着浮動形磁気ヘツドを浮動面
から見た斜視図、第2図は浮動状態側面断面図、第3図
は離陸時浮動面、吸着面圧力分布、第4図は定常時浮動
面、吸着面圧力分布である。Fig. 1 is a perspective view of the suction floating type magnetic head according to the present invention as seen from the floating surface, Fig. 2 is a side sectional view of the floating state, Fig. 3 is the floating surface at takeoff, pressure distribution on the adsorption surface, and Fig. 4 is the fixed Constantly floating surface and adsorption surface pressure distribution.
Claims (1)
を受ける浮動部と、該浮動部の空気流出端部に支持され
た磁気ヘッド部とからなる浮動形磁気ヘッドにおいて、
前記浮動部の空気流入端に形成された迎え角と、浮動部
の記録媒体対向面に正の浮力が発生するように形成され
た浮動面と、浮動部の少なくとも前記迎え角と浮動面の
交点より空気流入端寄りの部分から浮動部の後端に向つ
て負の浮力が発生するようテーパ付けられた吸着面とを
具備することを特徴とする吸着浮動形磁気ヘッド。1. A floating magnetic head consisting of a floating part that receives buoyancy from the air viscous laminar flow generated by the movement of a recording medium, and a magnetic head part supported by the air outflow end of the floating part,
An angle of attack formed at an air inflow end of the floating section, a floating surface formed so as to generate a positive buoyancy on a surface of the floating section facing the recording medium, and an intersection of at least the angle of attack and the floating surface of the floating section. What is claimed is: 1. A suction floating magnetic head comprising a suction surface tapered to generate negative buoyancy from a portion closer to an air inlet end toward a rear end of the floating section.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6950275A JPS5918780B2 (en) | 1975-06-11 | 1975-06-11 | Adsorption floating magnetic head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6950275A JPS5918780B2 (en) | 1975-06-11 | 1975-06-11 | Adsorption floating magnetic head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS51146215A JPS51146215A (en) | 1976-12-15 |
| JPS5918780B2 true JPS5918780B2 (en) | 1984-04-28 |
Family
ID=13404556
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6950275A Expired JPS5918780B2 (en) | 1975-06-11 | 1975-06-11 | Adsorption floating magnetic head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5918780B2 (en) |
-
1975
- 1975-06-11 JP JP6950275A patent/JPS5918780B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS51146215A (en) | 1976-12-15 |
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