JPH10275437A - Magnetic transducer - Google Patents
Magnetic transducerInfo
- Publication number
- JPH10275437A JPH10275437A JP11645698A JP11645698A JPH10275437A JP H10275437 A JPH10275437 A JP H10275437A JP 11645698 A JP11645698 A JP 11645698A JP 11645698 A JP11645698 A JP 11645698A JP H10275437 A JPH10275437 A JP H10275437A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- magnetic transducer
- transducer
- rail
- airflow
- 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
Landscapes
- Adjustment Of The Magnetic Head Position Track Following On Tapes (AREA)
Abstract
Description
【発明の詳細な説明】
【0001】
【発明の属する技術分野】発明は、磁気変換器に係り、
特に磁気デイスク装置の磁気ヘツドなどに用いられる磁
気変換器に関するものである。
【0002】
【従来の技術】気記録において、例えば磁気デイスクの
ような磁気記憶媒体(以下単に磁気媒体という)に磁気
変換器の磁気ギヤツ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触を避けるために、特開
昭49−121514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。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。ここに第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磁気媒体に垂直方向からみ
た説明図である。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。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ぴる3本のレール
部l,2,3が形成されている。これらのレール部l,
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1a,2a,3aがあり、それらの後方にレール
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つている。中央のレール部2
の後方には、磁気コア4と磁気ギヤツプ5が設けられて
いる。そして、この磁気ギヤツプ5は、磁気媒体上の所
定の記憶トラツク上に精度よく保持されていなければな
らない。通常、このような磁気変換器9は、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つてアクセ
ス機構に違設されるもので、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61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。
【0003】磁気媒体表面と微小間隔を保つて磁気変換
器が浮上する動作状態では、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る。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る
と、第3図に示すように、磁気変換器の両側面の前縁
7,8で剥離する流れ11,12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。
【0004】このようなカルマン渦列13が生じる場合
には周知のように、磁気変換器9に、空気の流れに直角
方向の、時間的にその大きさと方向が変化する力、すな
わち変動揚カが作用するものである。
【0005】
【発明が解決しようとする課題】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つて、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、磁気ギヤツプ5は磁気変換器9の
後流端に設置されているため、その揺動運動によつて磁
気媒体、例えば磁気デイスクの記録トラツクからの位置
ずれを起すという問題があつた。本発明は、前述の従来
技術の間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、従って磁気ギヤツプ
が位置ずれを起しにくい浮動形の磁気変換器の提供を、
その自的としている。
【0006】
【課題を解決するための手段】前述の間題点を解決する
ための手段として、本発明は、磁気媒体の表面との間に
空気滑動膜を形成する平面状のレール面を少なくとも両
側部に有するレール部と、このレール部間に形成され、
底面が前記レール面と平行な平面であって空気流の流入
端から流出端まで連続する溝部とを備えた磁気変換器に
おいて、前記磁気変換器への空気流れの上流側から見た
前記磁気変換器の前記レール面からの高さhに対する幅
wの比を、空気流によって前記磁気変換器に作用する変
動揚力を抑制する値、すなわち3.8から6に設定した
ものである。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。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。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。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。本発明者らは、磁気媒体20に係る磁気
デイ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。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つた。これは、第3図に示したカル
マン渦列の発生と関違しているものである。
【0007】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カ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。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
のビーク周波数成分の振幅を指数化したものをとつたも
ので、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l/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つ
た。したがつて、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3.8以上にすれば、
変動揚力による磁気ギヤツプの位置ずれを低滅できるこ
とがわかった。さらに良好な効果を得るためには、w/
hを4以上に設定することによりが好ましい。
【0008】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。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。左右対称の渦列1
4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l,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
れの影響が強まつたために、両前縁7,8からの剥離の
相互干渉が弱まつたためと考えられる。
【0009】
【発明の実施の形態】以下、本発明の一実施例を第l図
を参照して説明する。第l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。第l図に示す磁気変換器l 0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l,2,3が形成されており、そ
れぞれレール面l b,2b,3bを僧えて磁気媒体表
面との間で空気滑動面を形成するようになつている。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
接する方向から前記磁気変換器l0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3.8に形成されている。全体形状が
薄形となつているため、アクセス機構に連設される支持
手段を取付ける溝部6は浅くなつているが、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。したがつて、中央レール部2の後方に設け
られた磁気コア4と磁気ギヤツプ5は、磁気媒体20、
例えば磁気デイスクの記億トラツク上に精度よく保持さ
れる。磁気媒体20の表面と微小間隔を保つて磁気変換
器10が浮上する動作状態では、磁気変換器l0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l0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抑制され
る。したがつて、本実施例の磁気変換器10によれば、
磁気コア4、磁気ギヤツプ5部の揺動運動が抑制され、
磁気媒体、例えば磁気デイスクの記録トラツクの記録ト
ラツクからの位置ずれが少なくなり、位置決め誤差を従
来のl/2以下に低減する効果が得られる。
【0010】なお、本発明は、当然、ここに示した巻線
形の磁気変換器に限定されるものではなく、薄膜形の磁
気変換器にも適用できる。また、支持ばねを接着するた
めの溝部6a’の有無にも限定されず適用できるもので
あることは言うまでもない。
【0011】
【発明の効果】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動揚力の小さい、したがつて磁気
ギヤツ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。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnetic transducer,
In particular, the present invention relates to a magnetic transducer used for a magnetic head of a magnetic disk device. 2. Description of the Related Art In magnetic recording, a magnetic gap of a magnetic transducer is brought as close as possible to a magnetic storage medium (hereinafter, simply referred to as a magnetic medium) such as a magnetic disk, while a direct connection between the magnetic medium and the magnetic transducer is made possible. In order to avoid contact, an air levitation type magnetic transducer using an air bearing as described in Japanese Patent Application Laid-Open No. 49-121514 has been developed. Such a conventional magnetic transducer will be described with reference to FIGS. 2 and 3. FIG. FIG. 2 is a perspective view of a conventional magnetic transducer, and FIG. 3 is an explanatory view of a flow of air around the conventional magnetic transducer as viewed from a direction perpendicular to a magnetic medium. The magnetic transducer shown in FIG. 2 is a perspective view seen from the magnetic medium side, and the magnetic medium (not shown) approaches the magnetic transducer from the lower left of the figure and leaves at the upper right. On the surface of the magnetic transducer 9 facing the surface of the magnetic medium, there are formed three rails 1, 2, 3 extending in parallel at intervals in the direction of relative movement with the magnetic medium. These rails l,
Each of the tapes 2 and 3 has tapered portions 1a, 2a and 3a on the near side of the magnetic medium, and has rail surfaces 1b, 2b and 3b behind the tapered portions 1a, 2b and 3b to provide an air sliding surface with the magnetic medium surface. To form. Central rail part 2
A magnetic core 4 and a magnetic gap 5 are provided at the rear of the head. The magnetic gap 5 must be accurately held on a predetermined storage track on a magnetic medium. Normally, such a magnetic transducer 9 is provided on the access mechanism by a support means (not shown) including a gimbal and a spring member. This is performed by a known means in which a gimbal is bonded to the bottom surface 6a 'of a groove 61 provided substantially at the center in the longitudinal direction on the back side of the container 9. In an operating state in which the magnetic transducer floats with a small distance from the surface of the magnetic medium, the magnetic transducer is exposed to the flow of air from the direction of relative movement. When the flow of air around the magnetic transducer at this time is viewed from the direction perpendicular to the surface of the magnetic medium, as shown in FIG. 3, the flows 11, 12 that separate at the front edges 7, 8 on both side surfaces of the magnetic transducer. The so-called Karman vortex street 13 is generated behind the right and left peeling alternately. [0004] When such a Karman vortex street 13 is generated, as is well known, a magnetic force is applied to the magnetic transducer 9 in a direction perpendicular to the flow of air, the force of which changes in size and direction over time, that is, a fluctuating lift. Works. As described above, since the magnetic transducer 9 shown in FIG. 2 is adhered to the supporting means at substantially the center thereof, the magnetic transducer 9 is subjected to the above-mentioned fluctuating lift. Rotational vibration (oscillating motion) occurs around the support means bonding portion.
Further, as described above, since the magnetic gap 5 is provided at the downstream end of the magnetic transducer 9, there is a problem that the rocking motion causes a displacement of a magnetic medium, for example, a magnetic disk from a recording track. There was. SUMMARY OF THE INVENTION The present invention has been made in order to solve the above-mentioned problem of the prior art, and provides a floating type magnetic transducer which has a small fluctuation lift received from an air flow, and therefore, a magnetic gap is hardly displaced. To
It is selfish. [0006] As a means for solving the above-mentioned problems, the present invention provides at least a flat rail surface for forming an air sliding film with a surface of a magnetic medium. A rail portion on both sides and formed between the rail portions,
A bottom surface being a plane parallel to the rail surface and having a groove portion continuous from an inflow end to an outflow end of the airflow, wherein the magnetic conversion as viewed from the upstream side of the airflow to the magnetic converter is provided. The ratio of the width w to the height h of the vessel from the rail surface is set to a value that suppresses the fluctuating lift acting on the magnetic transducer by the air flow, that is, from 3.8 to 6. Here, the concept of developing the present invention will be described with reference to FIG. 4 to FIG. FIG. 4 is a front view of the magnetic transducer of FIG. 2, FIG. 5 is a frequency distribution diagram of the variable lift, and FIG. 6 is a diagram showing the amplitude of the peak frequency component of the variable lift and the cross-sectional shape of the magnetic converter. FIG. 4th
The figure is a front view of the conventional magnetic transducer 9 viewed from the upstream side of the air flow. In other words, the magnetic transducer 9 is viewed from the direction in which the magnetic medium approaches the magnetic transducer 9. This corresponds to a diagram showing a projected shape of the converter. Assuming that 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, w / h is 2.8. The present inventors have proposed a magnetic transducer 9 held at a small distance from the magnetic disk of the magnetic medium 20.
Was measured and the frequency was analyzed. As a result, the results shown in FIG. 5 were obtained. FIG.
The horizontal axis shows the frequency and the vertical axis shows the fluctuating lift. As is clear from this figure, it was found that the fluctuating lift fluctuated at a specific frequency. This is different from the occurrence of the Karman vortex street shown in FIG. [0007] Then, the present inventors next measured the peak value of the variable lift using w / h as a parameter, and obtained the results shown in FIG. In FIG. 6, the horizontal axis represents w / h representing the cross-sectional shape of the magnetic transducer, and the vertical axis represents the amplitude of the beak frequency component of the variable lift as an index, as shown in FIG. In addition, it was found that when w / h is 3.8, the amplitude becomes about l / 2 when w / h is small, and when w / h exceeds 4, the fluctuation of the specific frequency is not observed. Therefore, if w / h in the projected shape of the relative motion direction formed by the magnetic transducer with the magnetic medium is set to 3.8 or more,
It was found that the displacement of the magnetic gap due to the fluctuating lift could be reduced. To obtain a better effect, w /
It is preferable to set h to 4 or more. Next, FIG. 7 is an explanatory view showing the flow of air around the magnetic transducer of the present invention.
In this case, the flow of air at the time of (1) is shown as a vortex shape in comparison with FIG. As shown in FIG. 7, from the leading edges 7 and 8 on both sides of the magnetic transducer, a vortex street 14 in which the flow is symmetrical in the left and right direction (up and down in the figure) is generated, so that the fluctuating lift is reduced. It is considered something. Symmetric vortex street 1
The reason for the occurrence of 4 is that the distance between the left and right front edges 7 and 8 of the magnetic transducer is large, and because of this, between the rails 1 and 2 and between the rails 2 and 3, the upstream and downstream in the relative movement direction. Separation from both leading edges 7 and 8 due to the strong influence of the flow flowing into the wake from the flow of air through the groove formed in the air flow and the flow of air passing behind the magnetic transducer It is considered that the mutual interference weakened. An embodiment of the present invention will be described below with reference to FIG. FIG. 1 is a perspective view of a magnetic transducer according to one embodiment of the present invention, in which the same reference numerals as in FIG. 2 denote the same parts as in the conventional example, and a description thereof will be omitted. The magnetic transducer 10 shown in FIG. 1 is formed with three rails 1, 2, 3 extending in parallel with each other at intervals in the direction of relative movement with the magnetic medium, as in FIG. The air sliding surface is formed between the rail surfaces lb, 2b, and 3b and the surface of the magnetic medium. The magnetic transducer 10 has a thin overall shape, and is used when the magnetic medium 20 (see FIG. 4) views the magnetic transducer 10 from a direction approaching the magnetic transducer 10. The ratio w / h 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 in the projected shape of the container is formed to be 3.8. Since the overall shape is thin, the groove 6 for attaching the support means connected to the access mechanism is shallow, but the gimbal is adhered to the bottom surface 6a, and the function of the support is different from that of the related art. There is no. Accordingly, the magnetic core 4 and the magnetic gap 5 provided behind the central rail portion 2 are connected to the magnetic medium 20,
For example, it is accurately held on a storage track of a magnetic disk. In an operating state in which the magnetic transducer 10 floats with a small distance from the surface of the magnetic medium 20, the magnetic transducer 10 is exposed to the flow of air from the direction of relative motion. As described earlier with reference to FIG. 7, the vortex streets 14 symmetrical to the left and right (up and down in FIG. 7) of the air flow are generated from the front edges 7 and 8 on both sides of the magnetic transducer 10.
The fluctuating lift acting on the magnetic transducer 10 is suppressed to a small value. Therefore, according to the magnetic transducer 10 of the present embodiment,
The oscillating motion of the magnetic core 4 and the magnetic gap 5 is suppressed,
The positional deviation of the recording track of the magnetic medium, for example, the magnetic disk from the recording track is reduced, and the effect of reducing the positioning error to less than 1/2 of the conventional one can be obtained. It should be noted that the present invention is not limited to the wound type magnetic transducer shown here, but can be applied to a thin film type magnetic transducer. Further, it goes without saying that the present invention is not limited to the presence or absence of the groove 6a 'for bonding the support spring, and can be applied. As described above, according to the present invention, there is provided a floating type magnetic transducer which has a small fluctuation lift received from the flow of air, and is therefore less likely to cause a magnetic gap displacement. can do.
【図面の簡単な説明】
【図1】本発明の一実施例に係る磁気変換器の斜視図で
ある。
【図2】従来の磁気変換器の斜視図である。
【図3】従来の磁気変換器まわりの空気の流れを説明す
る図である。
【図4】従来の磁気変換器を空気の流れの上流側からみ
た投影図である。
【図5】変動揚力の周波数分布を示す図である。
【図6】変動揚力のピーク局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図である。
【図7】本発明における磁気変換器まわりの空気の流れ
を説明する図である。
【符号の説明】
l,2,3・・・レール部、lb,2b,3b・・・レ
ール面、4・・・磁気コア、5・・・磁気ギヤツプ、1
0・・・磁気変換器。BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a perspective view of a magnetic transducer according to one embodiment of the present invention. FIG. 2 is a perspective view of a conventional magnetic transducer. FIG. 3 is a diagram illustrating the flow of air around a conventional magnetic transducer. FIG. 4 is a projection view of a conventional magnetic transducer viewed from an upstream side of an air flow. FIG. 5 is a diagram showing a frequency distribution of a variable lift. FIG. 6 is a diagram showing the relationship between the amplitude of the peak local wave number component of the variable lift and the cross-sectional shape of the magnetic transducer. FIG. 7 is a diagram illustrating the flow of air around the magnetic transducer according to the present invention. [Description of Signs] 1, 2, 3 ... rail section, lb, 2b, 3b ... rail surface, 4 ... magnetic core, 5 ... magnetic gap, 1
0: magnetic transducer.
Claims (1)
状のレール面を少なくとも両側部に有するレール部と、
このレール部間に形成され、底面が前記レール面と平行
な平面であって空気流の流入端から流出端まで連続する
溝部とを備えた磁気変換器において、前記磁気変換器へ
の空気流れの上流側から見た前記磁気変換器の前記レー
ル面からの高さhに対する幅wの比を、空気流によって
前記磁気変換器に作用する変動揚力を抑制する値、すな
わち3.8から6に設定したことを特徴とする磁気変換
器。[Claims] 1. A rail portion having a flat rail surface on at least both sides forming an air sliding film between the surface of the magnetic medium,
A groove formed between the rails and having a bottom surface that is a plane parallel to the rail surface and that is continuous from an inflow end to an outflow end of the airflow. The ratio of the width w to the height h of the magnetic transducer from the rail surface as viewed from the upstream side is set to a value that suppresses the fluctuating lift acting on the magnetic transducer by the airflow, that is, from 3.8 to 6. A magnetic transducer, characterized in that:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11645698A JPH10275437A (en) | 1998-04-27 | 1998-04-27 | Magnetic transducer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11645698A JPH10275437A (en) | 1998-04-27 | 1998-04-27 | Magnetic transducer |
Related Parent Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61023807A Division JPH06103585B2 (en) | 1986-02-07 | 1986-02-07 | Magnetic transducer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH10275437A true JPH10275437A (en) | 1998-10-13 |
Family
ID=14687577
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11645698A Pending JPH10275437A (en) | 1998-04-27 | 1998-04-27 | Magnetic transducer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH10275437A (en) |
-
1998
- 1998-04-27 JP JP11645698A patent/JPH10275437A/en active Pending
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