JPS63166007A - Head for magnetic recording and reproducing device - Google Patents

Head for magnetic recording and reproducing device

Info

Publication number
JPS63166007A
JPS63166007A JP31319886A JP31319886A JPS63166007A JP S63166007 A JPS63166007 A JP S63166007A JP 31319886 A JP31319886 A JP 31319886A JP 31319886 A JP31319886 A JP 31319886A JP S63166007 A JPS63166007 A JP S63166007A
Authority
JP
Japan
Prior art keywords
head
disk
gap
outflow
sliding part
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP31319886A
Other languages
Japanese (ja)
Other versions
JP2606833B2 (en
Inventor
Toyofumi Tani
谷 豊文
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP61313198A priority Critical patent/JP2606833B2/en
Publication of JPS63166007A publication Critical patent/JPS63166007A/en
Application granted granted Critical
Publication of JP2606833B2 publication Critical patent/JP2606833B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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

Abstract

PURPOSE:To prevent spacing loss due to the increase of relative velocity from being increased, by setting the position of a read/write gap in a specific range on the outflow end of a sliding part assuming the length of the sliding part in the inflow/outflow direction of gas as one. CONSTITUTION:When a disk 1 is rotated and is moved in a direction of arrow head G for a head, the head 10 floats by a dynamic pressure effect due to air compression generated between the head 10 and the disk. At this time, a gap quantity between the head and the disk is distributed in a state where the quantity on the inflow side of the head is larger than that on the outflow side. And relation (h1<h) always exists between the gap quantities (h) and (h1), and relation p1<=1/4 is set, therefore, it goes to h1<=1/2h. In such way, the value of the (h1) goes to the value less than the surface coarseness of a medium and almost negligible, and the spacing loss due to the (h1) can be almost neglected.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は70ツビーデイスクに対して情報を記録(蓄
き込み)、かつこの70ツビーデイスクよシ情報を再生
(読み出す)するための磁気記録再生装置用ヘッドに関
するものである。
[Detailed Description of the Invention] [Field of Industrial Application] This invention relates to magnetic recording for recording (storing) information on a 70-tube disc and reproducing (reading) information from the 70-tube disc. This invention relates to a head for a playback device.

〔従来の技術〕[Conventional technology]

従来の70ツビーデイスク用ヘツドとしては。 As a conventional 70-tube disk head.

例えば第9図の要部斜視図で示されるフロッピーディス
クドライブ(以下、FDDと略す)装置に使用されるも
のがあった。図において、(1)はフロッピーディスク
(以下、単にFDという)i2)はFDII)に情報を
書き込みまた読み出すヘッドを搭載したキャリッジであ
る。(3)はキャリッジ(2)を支持するとともにキャ
リッジ(2)のX軸(FDの半径方向)の移動を案内し
、かつY軸(FDの周方向)の移動が固定されている一
対のガイドバーである。
For example, there is one used in a floppy disk drive (hereinafter abbreviated as FDD) device shown in the perspective view of the main part in FIG. In the figure, (1) is a carriage equipped with a head for writing and reading information on a floppy disk (hereinafter simply referred to as FD) (i2) and FDII). (3) is a pair of guides that support the carriage (2), guide the movement of the carriage (2) in the X axis (radial direction of the FD), and are fixed in movement in the Y axis (circumferential direction of the FD). It's a bar.

この種の装置では、第10図のヘッドの断面部分につい
ては八ツチングを省略して示すPDD装置のヘッド部分
の断面図に示すように、キャリッジ(2a)(2b)に
搭載されているヘッド(4a)(4b)はFD(1)を
はさんで一対ある。このヘッドのギャップのあるコア部
(6a)(6b)は谷ヘッド(4a)(4b)がFD(
1)に摺接する側の2つの平端面(摺動部X7aX7b
)及び(7c)(7a)のうち各々片側(7a)及び(
7C)にアシ。
In this type of device, the head (2a) (2b) mounted on the carriage (2a) (2b) is shown in the cross-sectional view of the head portion of the PDD device in which the cross-section of the head is omitted in Figure 10. There is a pair of 4a) and (4b) with FD (1) in between. The core portions (6a) (6b) of this head with gaps are such that the valley heads (4a) (4b) are FD (
1) Two flat end surfaces on the side that slide into contact with (sliding part X7aX7b
) and (7c) (7a), one side (7a) and (7a) respectively.
7C) reeds.

対向するヘッドとはディスク上の半径位置が若干異なっ
ている。(この量は規格で決められており。
The opposing head has a slightly different radial position on the disk. (This amount is determined by the standard.

通常8トラック分ずれている。) (5a)(5b)は
ジンバル板でおる。
Usually there is a shift of 8 tracks. ) (5a) (5b) are covered by gimbal plates.

第11図(a)は第10図における従来のヘッドを示す
側面図、同(b)はFD(1)との摺動部側から見た平
面図である。この種のヘッド(4)ではそのリードライ
トギャップ(以下、R/WGと示す)(8)の位置は5
g11図(a)に示すようにヘッド長さ10半分の位置
(C)9図中流入端(4)よシ長さmの一点鎖線で示し
た位置(C)よシ長さpだけ流入端(N側に形成されて
いた。この長さpはアジマスロスがほぼ0になるように
考慮して決められておシ2通常数百μm以下に設定され
ておシ1のほぼ1Aの位置にあった。上記でアジマスロ
スとは記録トラックに対して再生ヘッドギャップがある
角式θをもつことに起因して発生するロスでロシ、波長
をλ、トラツとはFDの回転に伴ってFDが移動するこ
とによ1)vDとヘッド(4)の間に動圧効果によシ形
成される空気流がヘッド(4)に流入する位置を意味し
、流出端(B)とは空気流が流出する位置を意味してい
る(以下、流入端込)、流出端(B)は上記の意味で用
いる)。(9)はイレーズギャップ(以下、EGと略す
)で、ヘッド長さlの半分の位置(C)よシ長さqだけ
流出端(BJ側に形成されていた。なお矢印(G)はF
Dの移動方向を示す。
FIG. 11(a) is a side view showing the conventional head in FIG. 10, and FIG. 11(b) is a plan view seen from the sliding part side with the FD (1). In this type of head (4), the read/write gap (hereinafter referred to as R/WG) (8) is located at 5
g11 As shown in Figure (a), the position (C) is 10-half the head length; 9 The position shown by the dashed line (C) is the length p from the inlet end (4) in Figure 9; (It was formed on the N side. This length p was determined in consideration of the azimuth loss being almost 0. The length p is usually set to several hundred μm or less and is located at a position of approximately 1A of the shaft 1. In the above, azimuth loss is the loss that occurs due to the angle θ of the playback head gap with respect to the recording track, and azimuth loss is the loss caused by the angle θ, where the wavelength is λ, and the azimuth loss is the loss that occurs when the FD moves as the FD rotates. Particularly 1) means the position where the air flow formed by the dynamic pressure effect between vD and the head (4) enters the head (4), and the outflow end (B) means the position from which the air flow exits; (Hereinafter, the inflow end is included) and the outflow end (B) is used in the above meaning). (9) is the erase gap (hereinafter abbreviated as EG), which is formed at the outflow end (BJ side) by a length q from the position (C) that is half of the head length l.
The direction of movement of D is shown.

このような従来のヘッド装置では9例えば特開昭55−
45105.同59−48867及び同59−9427
4号公報に開示されているように、ヘッドとFDは常に
接触しておシ、ヘッドとFD間のスペーシング(すきま
)はほぼ0と考えられていた。つま9第12図のヘッド
の動作状態における説明図に示すように、ヘッド(4)
とPDtl1間のすきまは、ヘッド(4)とFD(11
間の空気流によって発生する圧力が小さいため、ヘッド
(4)上の任意の位置で変わらず常に一定でほぼ0とみ
なされていた。
In such a conventional head device, for example,
45105. 59-48867 and 59-9427
As disclosed in Publication No. 4, it was thought that the head and the FD were always in contact with each other, and that the spacing between the head and the FD was almost zero. Head (4)
The clearance between the head (4) and the FD (11) is
Since the pressure generated by the air flow between them is small, it is always considered to be constant and approximately zero at any position on the head (4).

このような条件下ではヘッドギャップ位置はスペーシン
グロスの観点からは、ヘッド上のどの位置にあってもよ
いことになる。すなわちスペーシングロスL、S ハg
F2録ttl長λ、ヘッドFDiJ]スペーシング(ヘ
ッドギャップ位置にて)dによシ一般にLll = x
7(aaXここに、には常数)で表わされる。
Under such conditions, the head gap position can be located anywhere on the head from the standpoint of spacing loss. In other words, spacing loss L, S
F2 record ttl length λ, head FDiJ] spacing (at head gap position) according to d Generally Lll = x
7 (aaX is a constant here).

これまではこのdがほぼ0で変化しないので出力の減シ
方は、ギャップがヘッド上のどの位置にあっても、変わ
らずほぼ0とみなされていた。
Until now, this d was approximately 0 and did not change, so the reduction in output was considered to be approximately 0 regardless of the position of the gap on the head.

さらに、41!開昭50−34213号公報によれば信
号損失を減少させるために、送風器や送風管他のものを
余分に装置に備え付け、FDに空気を吹きつけることが
必要で装置のコストアップとなる欠点があった。
Furthermore, 41! According to JP-A No. 50-34213, in order to reduce signal loss, it is necessary to equip the device with an extra device such as a blower or air pipe to blow air to the FD, which increases the cost of the device. was there.

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

上記のように従来のヘッド装置では、スペーシング量は
ヘッドの位置によらず、はぼ一定で0とみなされていた
。またスペーシング0とするために余分な装置が必要だ
った。しかしながら、高稍贋な(測定種度±103μr
IL)すきま計測装置によシ実副を行なったところ、F
Dが回転している状態では第13図の説明図に示すよう
に、空気流(矢印W)による動圧効果によシヘッド(4
1F D (11間のすきまはヘッド(4)の流入側で
大きく、R,出側で小さいスペーシング分布となってい
ることが判明した。図中、  (A’) (B’) (
C’) (B)は各々ヘッド(4)の流入端内、流出端
(B)、形状中心位置(C) 、  1%/W G +
8)に対向するFD+1)の位置である。(h)はn/
wots+でのすきま量である。このすきま発生の条件
としては通常ヘッド(4) F D (0間の大きい相
対速度が必要であると予想されたにもかかわらず、  
1.2 m/Sというごく低速の場合にも11μm程度
生じていることが判明した(ヘッド押圧荷重1519f
の条件)。この量はヘッドギャップ位置換算で約0.0
5μmに相当し。
As described above, in conventional head devices, the spacing amount is considered to be approximately constant and zero regardless of the position of the head. Also, extra equipment was required to achieve zero spacing. However, it is highly fake (measurement degree ±103μr)
IL) When the clearance measurement device was used to perform actual subtraction, F
When D is rotating, as shown in the explanatory diagram of Fig. 13, the head (4) is
It was found that the spacing distribution between 1F D (11) was large on the inlet side of the head (4), and small on the R and outlet sides.In the figure, (A') (B') (
C') (B) is the inflow end, outflow end (B), and shape center position (C) of the head (4), respectively, 1%/W G +
This is the position of FD+1) opposite to 8). (h) is n/
This is the amount of clearance at wots+. Although it was predicted that the condition for this gap to occur would normally require a large relative speed between the head (4) F D (0),
It was found that approximately 11 μm was generated even at a very low speed of 1.2 m/S (head pressing load 1519 f).
conditions). This amount is approximately 0.0 when calculated by head gap position substitution.
Equivalent to 5 μm.

線記録密度30KFRPIの場合で約3dBのスペーシ
ングロスに相当し、出力の低下が大きい。この出力低下
量は線記録密度に比例するため、よシ高密度の記録にお
いては、出力劣化はさ1らに増大し。
In the case of a linear recording density of 30 KFRPI, this corresponds to a spacing loss of about 3 dB, resulting in a large decrease in output. Since this amount of output reduction is proportional to the linear recording density, the output deterioration increases even more when recording at a higher density.

大きな問題となる。なお、このすきま量の流入端と流出
端での差は、第14図のFDの回転速度とすきまとの関
係の実測例を表わす特性図に示すように、相対速度が増
すにつれて、これに比例して増大する。このためスペー
シングロスも相対速度が大きくなるほど大きくなること
は明らかでおる。
It becomes a big problem. Note that the difference in the amount of clearance between the inflow end and the outflow end becomes proportional to this as the relative speed increases, as shown in the characteristic diagram in Figure 14, which shows an actual measurement example of the relationship between the rotational speed of the FD and the clearance. and increase. Therefore, it is clear that the spacing loss increases as the relative speed increases.

図において、縦軸はすきま(h)(μrIL)を、横軸
はヘッドにおける位置を表わしており、特性曲線)→は
相対速& v = 1.3 rn/8 、  O−Oは
v = 1.0 m/8 。
In the figure, the vertical axis represents the clearance (h) (μrIL), the horizontal axis represents the position in the head, the characteristic curve) → is the relative speed & v = 1.3 rn/8, O-O is v = 1 .0 m/8.

Δ−イはv=0.6m/S、  E→はv = OyX
/8の場合を表わしている。なお、これは押圧Ogfす
なわちヘッドの自重のみを支える空気圧がヘッドディス
ク間に発生している場合の実測例である。
Δ-I is v=0.6m/S, E→ is v = OyX
/8 is shown. Note that this is an actual measurement example where the pressure Ogf, that is, the air pressure that supports only the head's own weight, is generated between the head and disk.

この発明は上記のような問題点を解消するためになされ
たもので、線記録密度が大きくなっても。
This invention was made to solve the above-mentioned problems, even when the linear recording density increases.

またフロッピーディスクの回転数が増して、相対速度が
大きくなってもスペーシングロスの少ない磁気記録再生
装置用ヘッドを得ることを目的とする。
Another object of the present invention is to obtain a head for a magnetic recording/reproducing device that exhibits less spacing loss even when the rotational speed of a floppy disk increases and the relative speed increases.

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

この発明の磁気記録再生装置用ヘッドは、フロッピーデ
ィスクと対向する摺動部との間に上記ディスクの回転に
伴なって気体が流入し、流出するとともに、上記摺動部
にリードライトギャップを設け上記ディスクに情報を記
録し、再生するものにおいて、上記摺動部における気体
の流入出方向の長さを1としたとき、上記リードライト
ギャップの位置を上記摺動部の流出端側T1の範囲に設
けたものである。
In the head for a magnetic recording/reproducing device of the present invention, gas flows in and out between the floppy disk and the opposing sliding portion as the disk rotates, and a read/write gap is provided in the sliding portion. In the disk for recording and reproducing information, when the length of the sliding portion in the gas inflow and outflow direction is 1, the position of the read/write gap is within the range T1 on the outflow end side of the sliding portion. It was established in

〔作用〕[Effect]

この発明におけるヘッドは、R/WG位置を摺動部の流
出端%1/4lの範囲、すなわちヘッド流出端によシ近
い位置に設けているので、高線密度記録や、相対速度の
増大に伴うスペーシングロスの影響を受は難くなる。
The head in this invention has the R/WG position in the range of 1/4 liter of the outflow end of the sliding part, that is, in a position close to the head outflow end, so it is suitable for high linear density recording and increase in relative speed. This makes it difficult to be affected by the accompanying spacing loss.

〔実施例〕〔Example〕

以ド、この発明を図について説明する。 The invention will now be explained with reference to the drawings.

第1図(aJはこの発明の一実施例の磁気記録再生装置
用ヘッドを示す側面図、同(b)はFDとの摺動部側か
ら見た平面図である。図において、 uttはこの実施
例のヘッド、aJはR/W Gで、ヘッドaOの形状中
心線つまシ摺動面における空気流入方向(ディスク回転
方向)の中心線(C)よV) plだけヘッド流出端(
B)側に配置したものであシ、ギャップ位置でのすきま
量がディスク面粗さ程度になるよう。
FIG. 1 (aJ is a side view showing a head for a magnetic recording/reproducing device according to an embodiment of the present invention, and FIG. 1(b) is a plan view seen from the side of the sliding part with the FD. In the figure, utt is In the head of the embodiment, aJ is R/W G, and the shape center line of the head aO is the center line (C) in the air inflow direction (disk rotation direction) on the sliding surface of the head (V).
It is placed on the B) side so that the amount of clearance at the gap position is about the same as the disc surface roughness.

相対速度の最大値が、  1.2m78程度ではp1之
′−1[71に設定している。また(1りはトラック幅
を決めるイレーズギャップでありtqlの値が数百μ馬
でR/WGよりさらに流出端(B)側に位置させたもの
である。
When the maximum value of relative velocity is about 1.2m78, it is set to p1'-1[71. Further, (1) is an erase gap that determines the track width, and the value of tql is several hundred microhorses, and it is located further toward the outflow end (B) side than the R/WG.

第2図はこの実施例のヘッド11(IのFD(1)回転
中の状態を示す説明図で、FD(11上のA1点がヘッ
ド0上の空気が流入する流入端(4)に相当し B7点
が流出端(B)に相当する。また07点はヘッド住〔の
形状中心線(C)に対応する点である。V点はこの実施
例におけるR/WGQI)位置に対応する点でちゃ9図
中。
FIG. 2 is an explanatory diagram showing the rotating state of the FD (1) of the head 11 (I) of this embodiment, where point A1 on the FD (11) corresponds to the inflow end (4) into which the air above the head 0 flows. Point B7 corresponds to the outflow end (B). Point 07 corresponds to the center line (C) of the shape of the head. Point V corresponds to the R/WGQI) position in this example. Decha 9 figures in the middle.

この点に示したhlがこの場合のヘッドσ・とFD(1
)間のすきまである。なお B1点は従来のR7’wa
位置に対応し、hがすきまである。
The hl shown at this point is the head σ・and FD(1
) There is a gap between. Note that B1 point is the conventional R7'wa
Corresponding to the position, h is the gap.

次に動作について説明する。Next, the operation will be explained.

第2図に示すようにディスク(1)が回転して、ヘッド
に対して矢印Q)方向に移動すると、ヘッドαQとディ
スク間に発生する空気圧による動圧効果にり、ヘッド+
11は浮上する。この時、ヘッドとディスク間のすきま
量はヘッドの流入側が流出側より。
As shown in Fig. 2, when the disk (1) rotates and moves in the direction of arrow Q with respect to the head, the head +
11 rises to the surface. At this time, the amount of clearance between the head and the disk is larger on the inflow side of the head than on the outflow side.

よシ大きい分布となっている。このため、上記すきま量
りとhlの間には常にhl<hの関係がある。しかもp
1≦土の関係よF) ht≦+hである。
The distribution is quite large. Therefore, there is always a relationship of hl<h between the clearance measurement and hl. Moreover, p
The relationship is 1≦earth F) ht≦+h.

よってhlの値は媒体表面粗さ以下のほとんど無視でき
る値となりp  hlによるスペーシングロスはほとん
ど無視できる。
Therefore, the value of hl is an almost negligible value that is less than the medium surface roughness, and the spacing loss due to phl can be almost ignored.

ところで、実際の系においては再生出力の劣化はスペー
シングロスだけではなく、前述した記録トラックに対す
る再生ヘッド軌跡の角度誤差であるアジマスロスも無く
すようにする必要がある。
Incidentally, in an actual system, deterioration of the reproduction output is caused not only by the spacing loss, but also by eliminating the azimuth loss, which is the angular error of the trajectory of the reproduction head with respect to the recording track.

これに関する工夫を次に述べる。Next, we will discuss some ideas regarding this.

第3図は従来のヘッドのギャップ線Q3のディスク上で
の対応位置を記録トラックα4.ディスク回転中心(i
s等と照らし合わせる形で示す説明図であり、ギヤツブ
線値譜の延長線がディスク回転中心a$を通る形になシ
ワヘッドの取付角度誤差や位置オフセット誤差(ギャッ
プ線0の平行移動する形でのズレによる誤差)がない限
り、アジマスロスがない。なおこの時、ヘッド(4)の
ギャップ線はほぼヘッドの形状中心に位置しておシ、キ
ャリッジ(2)の線対称線に対してヘッドも同様の位置
に配設されている。なお、矢印(R)はディスクの回転
方向を示している。
FIG. 3 shows the corresponding position of the gap line Q3 of the conventional head on the recording track α4. Disk rotation center (i
It is an explanatory diagram shown in comparison with s, etc., and the extension line of the gear line value passes through the disk rotation center a$, and the installation angle error and position offset error of the wrinkle head (in the form of parallel movement of the gap line 0) There is no azimuth loss unless there is an error due to the deviation of At this time, the gap line of the head (4) is located approximately at the center of the shape of the head, and the head is also disposed at the same position with respect to the line of symmetry of the carriage (2). Note that the arrow (R) indicates the rotation direction of the disk.

一方、第4図の説明図に示すように、この実施例のヘッ
ドαlはそのギャップ線0がヘッドの形状中心線よシ流
出端側に位置しているため、キャリッジ上にヘッドを取
付ける際、キャリッジの形状中心線にヘッドの形状中心
線(即ち、摺動面における空気流入方向ディスク回転方
向の中心)を合わせて配設した場合9図中に示すθだけ
の角度誤差が発生するため、アジマスロスが生じる。
On the other hand, as shown in the explanatory diagram of FIG. 4, in the head αl of this embodiment, the gap line 0 is located on the outflow end side of the head shape center line, so when the head is mounted on the carriage, If the shape center line of the head is aligned with the shape center line of the carriage (i.e., the center of the sliding surface in the air inflow direction and the disk rotation direction), an angular error of θ shown in Figure 9 will occur, resulting in azimuth loss. occurs.

そこで、この実施例のヘッドをキャリッジ上に配設する
場合には、第5図の説明図に示すように。
Therefore, when the head of this embodiment is disposed on a carriage, as shown in the explanatory diagram of FIG.

ヘッドのギャップ+!iα罎がディスクの回転中心a5
を通るように配設すればアジマスロスは無くなる。
Head gap +! iα is the center of rotation of the disk a5
If it is arranged so that it passes through, azimuth loss will be eliminated.

すなわち、ヘッド員の形状中心線(C)をmだけ流入端
側にずらせてキャリッジ(2)上に配設する。このよう
にヘッドをキャリッジ上に配設することは容易である。
That is, the head member is disposed on the carriage (2) with its shape center line (C) shifted by m toward the inflow end. It is easy to arrange the head on the carriage in this way.

もう少し具体的には、第6図の説明図に示すようにする
ことである。この図はヘッドを含むキャリッジ部を摺動
面側から見た平面図で。
More specifically, it is as shown in the explanatory diagram of FIG. This figure is a plan view of the carriage section including the head, viewed from the sliding surface side.

(5)はヘッドαGを支持するジンバル板であり、α〔
はヘッド、 (13はこのヘッドのギャップ線である。
(5) is a gimbal plate that supports head αG;
is the head, (13 is the gap line of this head.

なお、上記実施例では相対速度1.2F7!/S以下程
度(この値は大きさ15インチディスクを30゜rpm
で回転させた場合の外周での速度に相当する)の条件下
でギャップ位置をずらせたヘッドの例を示したが、ヘッ
ドの押圧が一定であれば相対速反の大きさに対応してス
ペーシング量は変化するので、このスペーシング量に合
わせてスペーシングロスが無視できる位置までギヤツブ
位Itをヘッドの形状中心位置からずらせることはもち
ろんである。当然スペーシングが大きい程、ずらせる童
もふえる。
In addition, in the above example, the relative speed is 1.2F7! /S or less (this value is for a 15-inch disc at 30° rpm)
We have shown an example of a head in which the gap position is shifted under the condition (corresponding to the speed at the outer circumference when rotating at Since the amount of pacing changes, it is of course necessary to shift the gear position It from the center position of the head shape to a position where the spacing loss can be ignored in accordance with the amount of spacing. Naturally, the larger the spacing, the more children will be shifted.

さらに、上記実施例ではヘッドがFDと摺動する側の平
端面(摺動部)がほぼ矩形のヘッドについて示したが、
これに限らず、第7図(a)の側面図。
Furthermore, in the above embodiment, the flat end surface (sliding part) on the side where the head slides on the FD is shown as a head that is approximately rectangular.
The side view of FIG. 7(a) is not limited to this.

同(b)の摺動部側から見た平面図、51g8図のFD
回転状態の説明図に示すような形状を持つヘッドでも同
様の効果を奏する。第7図(b)において点模様で示し
た部分がヘッドσηがディスク(1)と摺動する側の平
端面(摺動部)であり、これが流入端側と流出端側で8
状の丸味を帯びた形になっており。
Plan view from the sliding part side in (b), FD in Figure 51g8
A similar effect can be achieved even with a head having a shape as shown in the explanatory diagram of the rotating state. In Fig. 7(b), the dotted part is the flat end surface (sliding part) on the side where the head ση slides on the disk (1), and this is the flat end surface (sliding part) on the side where the head ση slides on the disk (1).
It has a rounded shape.

いわば楕円の半分のような形のものになっている。It is shaped like half an ellipse, so to speak.

このような形状のものも上記と同様の効果を有する。な
お、この形状のヘッドα乃の場合、R/WGαυとB、
Gd2の距1lliq1は・B、Gが上記平端面内に来
るように配設されていることはもちろんである。
A device having such a shape also has the same effect as above. In addition, in the case of head α of this shape, R/WGαυ and B,
Of course, the distance 1lliq1 of Gd2 is arranged such that B and G are within the flat end surface.

以上において、FDのヘッドと対向する面は。In the above, the surface of the FD facing the head is as follows.

実際には例えば0.03μm〜0.1μmRmax程度
の面粗さを持っているが1図には示していない。一方。
In reality, it has a surface roughness of, for example, about 0.03 μm to 0.1 μmRmax, but it is not shown in FIG. on the other hand.

ヘッドの面粗さは例えば0,01μm Rmax以下の
鏡面であり、少なくともディスクよシは面粗さは良い。
The surface roughness of the head is, for example, a mirror surface of 0.01 μm or less Rmax, and at least the surface roughness of the disk is good.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によれば、フロッピーディスク
と対向する摺動部との間に上記ディスクの回転に伴なっ
て気体が流入し、流出するとともに、上記摺動部にリー
ドライトギャップを設け上記ディスクに情報を記録し、
再生するものにおいて、上記摺動部における気体の流入
出方向の長さを1としたとき、上記リードライトギャッ
プの位置を上記摺動部の流出端側11の範囲に設けたこ
とによシ、線記録密度が上がシ、ディスクの回転数が増
して相対速度が大きくなってもスペーシングロスが殆ど
無視できるため、よシ高い密度の記録が可能となシ装置
の小形化に寄与でき一゛る磁気記録再生装置用ヘッドが
得られる効果がある。
As described above, according to the present invention, gas flows in and out between the floppy disk and the opposing sliding portion as the disk rotates, and a read/write gap is provided in the sliding portion. Record information on the above disk,
In the regenerating device, when the length of the sliding portion in the direction of inflow and outflow of gas is 1, the position of the read/write gap is provided within the range of the outflow end side 11 of the sliding portion, As the linear recording density increases, the spacing loss can be almost ignored even when the disk rotational speed increases and the relative speed increases, so it can contribute to the miniaturization of devices that can perform higher density recording. This has the effect of providing a head for a magnetic recording/reproducing device.

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

第1図(a)はこの発明の一実施例のヘッドを示す側面
図、同(b)は摺動部側から見た平面図、第2図は第1
図に示すヘッドの動作状態を示す説明図。 W、3図はアジマスロスが無い場合のヘッドギャップ配
置を示す説明図、第4図はアジマスロスがある場合の説
明図、第5図はこの発明の一実施例によるキャリッジへ
のヘッド取付状態を示す説明図。 第60図は第5図の詳細説明図、第7図はこの発明の他
の実施例のヘッドを示す側面図、同(b)は摺動部側か
ら見た平面図、第8図は第7図のヘッドの動作状態を示
す説明図、第9図は従来例に関わるFDD装置の要部斜
視図、第10図は従来例に関わるFDDのヘッド近傍の
断面図、第11図(=)は従来例のヘッドの側面図、同
(b)は摺動部側から見た平面図、第12図は従来想定
されていたヘッドの動作状態を示す説明図、第13図は
従来例のヘッドの動作状態を示す説明図、第14図はF
Dの回転速度とすきまとの関係を示す実測特性図である
。 図において、(1)はフロッピーディスク、αQ、αη
はヘッド、αυはリードライトギャップ、αJはリード
ライトギャップ線、(1!19はディスク回転中心、(
A)は流入端、(B)は流出端である。 なお2図中、同一符号は同−又は相当部分を示す。
FIG. 1(a) is a side view showing a head according to an embodiment of the present invention, FIG. 1(b) is a plan view seen from the sliding part side, and FIG.
FIG. 3 is an explanatory diagram showing the operating state of the head shown in the figure. W, Figure 3 is an explanatory diagram showing the head gap arrangement when there is no azimuth loss, Figure 4 is an explanatory diagram when there is azimuth loss, and Figure 5 is an explanatory diagram showing the head attachment state to the carriage according to an embodiment of the present invention. figure. 60 is a detailed explanatory diagram of FIG. 5, FIG. 7 is a side view showing a head according to another embodiment of the present invention, FIG. 60 is a plan view seen from the sliding part side, and FIG. Fig. 7 is an explanatory diagram showing the operating state of the head, Fig. 9 is a perspective view of the main parts of the FDD device related to the conventional example, Fig. 10 is a sectional view of the vicinity of the head of the FDD related to the conventional example, and Fig. 11 (=) is a side view of the head of the conventional example, (b) is a plan view seen from the sliding part side, FIG. 12 is an explanatory diagram showing the conventionally assumed operating state of the head, and FIG. 13 is the head of the conventional example. An explanatory diagram showing the operating state of F
It is an actually measured characteristic diagram showing the relationship between the rotational speed of D and the clearance. In the figure, (1) is a floppy disk, αQ, αη
is the head, αυ is the read/write gap, αJ is the read/write gap line, (1!19 is the center of disk rotation, (
A) is the inflow end, and (B) is the outflow end. Note that in the two figures, the same reference numerals indicate the same or equivalent parts.

Claims (2)

【特許請求の範囲】[Claims] (1)フロッピーディスクと対向する摺動部との間に上
記ディスクの回転に伴なつて気体が流入し、流出すると
ともに、上記摺動部にリードライトギャップを設け上記
ディスクに情報を記録し、再生するものにおいて、上記
摺動部における気体の流入出方向の長さをlとしたとき
、上記リードライトギャップの位置を上記摺動部の流出
端側1/4lの範囲に設けたことを特徴とする磁気記録
再生装置用ヘッド。
(1) Gas flows in and out between the floppy disk and the opposing sliding portion as the disk rotates, and a read/write gap is provided in the sliding portion to record information on the disk; In the regenerating device, the read/write gap is located within a range of 1/4 l on the outflow end side of the sliding portion, where l is the length of the sliding portion in the gas inflow and outflow direction. A head for a magnetic recording/reproducing device.
(2)リードライトギャップの延長線がディスクの回転
中心を通つていることを特徴とする特許請求の範囲第1
項記載の磁気記録再生装置用ヘッド。
(2) Claim 1, characterized in that the extension line of the read/write gap passes through the center of rotation of the disk.
A head for a magnetic recording/reproducing device as described in 1.
JP61313198A 1986-12-26 1986-12-26 Magnetic recording / reproducing device Expired - Lifetime JP2606833B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61313198A JP2606833B2 (en) 1986-12-26 1986-12-26 Magnetic recording / reproducing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61313198A JP2606833B2 (en) 1986-12-26 1986-12-26 Magnetic recording / reproducing device

Publications (2)

Publication Number Publication Date
JPS63166007A true JPS63166007A (en) 1988-07-09
JP2606833B2 JP2606833B2 (en) 1997-05-07

Family

ID=18038283

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61313198A Expired - Lifetime JP2606833B2 (en) 1986-12-26 1986-12-26 Magnetic recording / reproducing device

Country Status (1)

Country Link
JP (1) JP2606833B2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57103173A (en) * 1980-12-19 1982-06-26 Ricoh Co Ltd Flexible disk device
JPS6055509A (en) * 1983-09-05 1985-03-30 Nec Corp Magnetic head

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57103173A (en) * 1980-12-19 1982-06-26 Ricoh Co Ltd Flexible disk device
JPS6055509A (en) * 1983-09-05 1985-03-30 Nec Corp Magnetic head

Also Published As

Publication number Publication date
JP2606833B2 (en) 1997-05-07

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