JPH0793708A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPH0793708A
JPH0793708A JP25637193A JP25637193A JPH0793708A JP H0793708 A JPH0793708 A JP H0793708A JP 25637193 A JP25637193 A JP 25637193A JP 25637193 A JP25637193 A JP 25637193A JP H0793708 A JPH0793708 A JP H0793708A
Authority
JP
Japan
Prior art keywords
magnetic
tape
magnetic head
sliding surface
magnetic tape
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
JP25637193A
Other languages
Japanese (ja)
Other versions
JP3590644B2 (en
Inventor
Toshio Kawakita
敏夫 川北
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.)
Maxell Ltd
Original Assignee
Hitachi Maxell 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 Maxell Ltd filed Critical Hitachi Maxell Ltd
Priority to JP25637193A priority Critical patent/JP3590644B2/en
Publication of JPH0793708A publication Critical patent/JPH0793708A/en
Application granted granted Critical
Publication of JP3590644B2 publication Critical patent/JP3590644B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

(57)【要約】 【目的】 厚さの異なる磁気テ―プで互換性があり、薄
い磁気テ―プでも良好なエンベロ―プ出力を得ることが
でき、しかもテ―プ摺動面での接合部材の強度や耐摩耗
性を十分に確保することができる磁気ヘツドを提供す
る。 【構成】 磁気ヘツド1のテ―プ摺動面9における幅方
向ロの両端側に、磁気テ―プの摺動方向イに沿う一対の
溝10a,10bを形成するとともに、その深さを、磁
気テ―プの入側位置Xの深さよりも、出側位置Yの深さ
の方が小さくなるように、設計する。
(57) [Summary] [Purpose] Compatible with magnetic tapes of different thicknesses, good envelope output can be obtained even with thin magnetic tapes, and the tape sliding surface Provided is a magnetic head capable of sufficiently securing the strength and wear resistance of a joining member. [Structure] A pair of grooves 10a, 10b along the sliding direction a of the magnetic tape are formed at both ends of the tape sliding surface 9 of the magnetic head 1 in the width direction b, and the depth thereof is The magnetic tape is designed so that the depth at the outlet side position Y is smaller than the depth at the inlet side position X.

Description

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

【0001】[0001]

【産業上の利用分野】この発明は、ビデオテ―プレコ―
ダ(VTR)などの磁気記録再生装置に装備される磁気
ヘツドに関し、主に回転ヘツド型ヘリキヤルスキヤン方
式の磁気記録再生装置に使用する磁気ヘツドに関する。
BACKGROUND OF THE INVENTION This invention is a video tape recorder.
The present invention relates to a magnetic head equipped in a magnetic recording / reproducing apparatus such as a VTR (VTR), and mainly relates to a magnetic head used in a rotary head type helikyalskian type magnetic recording / reproducing apparatus.

【0002】[0002]

【従来の技術】回転ヘツド型ヘリキヤルスキヤン方式の
磁気記録再生装置では、シリンダの周面に磁気ヘツドが
数10μm突き出した状態で固定され、このシリンダに
磁気テ―プを一定角度で巻き付け、シリンダの回転によ
り磁気ヘツドを磁気テ―プに摺動させて、記録,再生を
行うものである。磁気ヘツドは、テ―プ摺動面の形状
が、摺動方向および幅方向ともに滑らかな楕円曲面に形
成されており、ヘツドギヤツプはテ―プ摺動面の中心に
形成されている。
2. Description of the Related Art In a rotary head type helikyalskian type magnetic recording / reproducing apparatus, a magnetic head is fixed to a circumferential surface of a cylinder in a state of protruding by several tens of μm, and a magnetic tape is wound around the cylinder at a constant angle. The magnetic head is slid on the magnetic tape by the rotation of, and recording and reproducing are performed. The magnetic head has a tape sliding surface formed in a smooth elliptic curved surface in both the sliding direction and the width direction, and the head gear tape is formed at the center of the tape sliding surface.

【0003】このような磁気記録再生装置により、磁気
特性が同じで厚さの異なる磁気テ―プを用いて、テ―プ
張力を一定条件にして記録,再生を行うと、薄い磁気テ
―プでは再生出力が低下し、とくにエンベロ―プ出力波
形でみると、図7の破線(曲線−β)に示すように、シ
リンダの回転方向前方側での磁気テ―プの張力が大きく
なる区間Aにおいて、再生出力が低下する欠点がある。
With such a magnetic recording / reproducing apparatus, when magnetic tapes having the same magnetic characteristics but different thicknesses are used for recording / reproducing under a constant tape tension, a thin magnetic tape is obtained. In the section A where the tension of the magnetic tape on the front side in the direction of rotation of the cylinder is large, as shown by the broken line (curve -β) in FIG. However, there is a drawback in that the reproduction output decreases.

【0004】これは、図8のように、厚い磁気テ―プT
1 は、磁気ヘツド20のテ―プ摺動面21の幅方向のほ
ぼ全面に接触するが、薄い磁気テ―プT2 は、図9の如
く、剛性の低下によるテ―プ変形が大きく、テ―プ摺動
面21の幅方向の両端部21a,21b位置で接触し、
ギヤツプ中心21c位置での磁気テ―プと磁気ヘツドと
の間のスペ―シング、とくに磁気テ―プの張力が増大す
る前記Aの区間での上記スペ―シングが大きくなるた
め、と推定される。
This is a thick magnetic tape T as shown in FIG.
1 contacts almost the entire width direction of the tape sliding surface 21 of the magnetic head 20, but the thin magnetic tape T 2 has a large tape deformation due to a decrease in rigidity as shown in FIG. The tape sliding surface 21 comes into contact with both widthwise end portions 21a and 21b,
It is estimated that the spacing between the magnetic tape and the magnetic head at the position of the gear center 21c, especially the spacing in the section A where the tension of the magnetic tape increases, becomes large. .

【0005】このため、従来より、磁気テ―プ側の改良
として、ポリエチレンナフタレ―トや芳香族ポリアミド
樹脂などの高ヤング率のベ―スフイルムを用いて、磁気
テ―プの剛性を高めることが行われている。しかし、そ
の効果には限度があるため、磁気記録再生装置側の改良
についても、種々検討されている。
Therefore, conventionally, as an improvement on the magnetic tape side, the rigidity of the magnetic tape is increased by using a base film having a high Young's modulus such as polyethylene naphthalate or aromatic polyamide resin. Is being done. However, since the effect is limited, various improvements on the magnetic recording / reproducing apparatus side have been studied.

【0006】この装置側の改良として、たとえば、磁気
テ―プの張力を低くしたり、シリンダ周面での磁気ヘツ
ドの突き出し量を下げるなどの改良が試みられている
が、薄い磁気テ―プに最適にすると、厚い磁気テ―プの
出力が逆に低下し、厚い磁気テ―プと薄い磁気テ―プと
の互換性をとれないという問題があつた。
[0006] As an improvement on this device side, for example, an attempt has been made to reduce the tension of the magnetic tape or to reduce the protrusion amount of the magnetic head on the circumferential surface of the cylinder, but a thin magnetic tape is used. However, the optimum output of the thick magnetic tape is reduced, and there is a problem that the compatibility between the thick magnetic tape and the thin magnetic tape cannot be obtained.

【0007】また、図10および図11に示すように、
磁気ヘツド30(40)におけるテ―プ摺動面31(4
1)の幅方向の両端部31a,31b(41a,41
b)を面取りした構造とすることにより、テ―プ摺動面
の幅を狭くして摺動面積を小さくし、磁気テ―プと磁気
ヘツドとの間の面圧を増加する方法も知られているが、
この方法によると、テ―プ摺動面の幅が一定値以下とな
ると、ギヤツプ幅を規制している接合部材の強度が低下
する問題がある。
Further, as shown in FIGS. 10 and 11,
Tape sliding surface 31 (4) on the magnetic head 30 (40)
1) Both ends 31a, 31b (41a, 41) in the width direction
It is also known that the chamfered structure of b) reduces the width of the tape sliding surface to reduce the sliding area and increases the surface pressure between the magnetic tape and the magnetic head. However,
According to this method, when the width of the tape sliding surface becomes a certain value or less, there is a problem that the strength of the joining member that regulates the width of the gear tape decreases.

【0008】さらに、特開昭62−192907号、同
60−101706号などの公報には、テ―プ摺動面の
幅を部分的に狭くする方法も提案されているが、狭トラ
ツク化に対応して摺動面の幅を狭くしていくと、磁気テ
―プとの接触面積が著しく小さくなるため、上記幅が一
定値以下となると、磁気ヘツドの局部的な摩耗量が極め
て大きくなり、磁気ヘツドの耐摩耗性の点で問題が生じ
る。
Further, Japanese Patent Laid-Open Nos. 62-192907 and 60-101706 also propose a method of partially narrowing the width of the tape sliding surface. Correspondingly, if the width of the sliding surface is reduced, the contact area with the magnetic tape will be significantly reduced, so if the width is below a certain value, the amount of local wear of the magnetic head will become extremely large. However, there is a problem in the wear resistance of the magnetic head.

【0009】[0009]

【発明が解決しようとする課題】このように、従来の改
良技術では、厚い磁気テ―プと薄い磁気テ―プとの互換
性をとれなかつたり、磁気ヘツドのテ―プ摺動面での接
合部材の強度や耐摩耗性を確保しにくいという難点があ
つた。
As described above, in the conventional improved technique, the compatibility between the thick magnetic tape and the thin magnetic tape cannot be obtained, and the tape sliding surface of the magnetic head is not compatible. However, it is difficult to secure the strength and wear resistance of the joining member.

【0010】この発明は、上記の事情に鑑み、厚さの異
なる磁気テ―プで互換性があり、薄い磁気テ―プでも良
好なエンベロ―プ出力を得ることができ、しかもテ―プ
摺動面での接合部材の強度や耐摩耗性を十分に確保する
ことができる磁気ヘツドを提供することを目的としてい
る。
In view of the above circumstances, the present invention is compatible with magnetic tapes having different thicknesses, and a good envelope output can be obtained even with a thin magnetic tape, and a tape slide is also possible. It is an object of the present invention to provide a magnetic head capable of sufficiently securing the strength and wear resistance of the joining member on the moving surface.

【0011】[0011]

【課題を解決するための手段】この発明者らは、上記の
目的を達成するために、鋭意検討した結果、磁気ヘツド
のテ―プ摺動面の特定位置に特定の溝を形成すると、薄
い磁気テ―プを用いたときのテ―プ摺動面における幅方
向両端部での接触が防がれて、ギヤツプ中心位置での磁
気テ―プと磁気ヘツドとの間のスペ―シングが低減さ
れ、良好なエンベロ―プ出力が得られることを知り、こ
の発明を完成するに至つた。
Means for Solving the Problems The inventors of the present invention have made earnest studies in order to achieve the above-mentioned object. As a result, when a specific groove is formed at a specific position on a tape sliding surface of a magnetic head, it is thin. When a magnetic tape is used, contact at both widthwise ends on the tape sliding surface is prevented, reducing the spacing between the magnetic tape and the magnetic head at the center position of the gear tape. It was discovered that a good envelope output was obtained, and the invention was completed.

【0012】すなわち、この発明は、テ―プ摺動面の幅
方向の両端側に、磁気テ―プの摺動方向に沿う一対の溝
を、その深さが磁気テ―プの入側位置よりも出側位置で
小さくなるように形成したことを特徴とする磁気ヘツド
に係るものである。
That is, according to the present invention, a pair of grooves along the sliding direction of the magnetic tape are provided at both ends of the tape sliding surface in the width direction, and the depth of the groove is at the entrance side of the magnetic tape. The magnetic head is characterized in that it is formed so as to be smaller at the exit side position.

【0013】[0013]

【作 用】この発明において、テ―プ摺動面の幅方向の
両端部に形成された溝内には、空気が流入する。溝の深
さが磁気テ―プの入側位置よりも出側位置で小さくされ
ているので、流入空気は出側付近で外部に圧出され、こ
の圧出で走行テ―プに対して内方からの押圧力が生じ
る。この押圧力により、薄い磁気テ―プを用いたときで
も、従来のような幅方向の両端部側での磁気テ―プの接
触が防がれて、ギヤツプ中心位置での磁気テ―プと磁気
ヘツドとの間のスペ―シングが低減され、これにより良
好なエンベロ―プ出力が得られる。
[Operation] In this invention, air flows into the grooves formed at both ends of the tape sliding surface in the width direction. Since the depth of the groove is smaller at the outlet side than at the inlet side of the magnetic tape, the inflowing air is extruded to the outside near the outlet side, and this expulsion causes the inside of the running tape. A pressing force from one side is generated. With this pressing force, even when using a thin magnetic tape, the contact of the magnetic tape on both ends in the width direction as in the past is prevented, and the magnetic tape at the center position of the gear tape is prevented. Spacing to and from the magnetic head is reduced, which results in better envelope output.

【0014】[0014]

【実施例】以下、この発明の磁気ヘツドの一実施例を図
面に基づいて説明する。図1はこの発明の回転ヘツド型
ヘリキヤルスキヤン方式のVTR用磁気ヘツドの斜視
図、図2は上記磁気ヘツドのテ―プ摺動面の正面図、図
3は同側面図で、(A)は磁気テ―プの入側位置、
(B)は出側位置である。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the magnetic head of the present invention will be described below with reference to the drawings. FIG. 1 is a perspective view of a magnetic head for a VTR of a rotary head type helicopter scan method of the present invention, FIG. 2 is a front view of a tape sliding surface of the magnetic head, and FIG. 3 is a side view of the same. Is the entry position of the magnetic tape,
(B) is the exit position.

【0015】図1〜図3において、磁気ヘツド1は、磁
気コア半体2A,2Bおよび両半体の対向面に配した磁
性合金薄膜3A,3Bで形成された磁気ギヤツプ4と、
この磁気ギヤツプ4を保持するために配された接合部材
5とにより構成され、磁気ギヤツプ4の対向面の近傍に
切欠部を設けてトラツク幅6を規制している。7は、磁
気コア半体2A,2Bにコイル8を巻き付けるための巻
線窓である。
1 to 3, a magnetic head 1 comprises a magnetic core half 2A, 2B and a magnetic gear 4 formed of magnetic alloy thin films 3A, 3B arranged on the opposing surfaces of both halves.
It is constituted by a joining member 5 arranged to hold the magnetic gear 4 and a notch is provided in the vicinity of the facing surface of the magnetic gear 4 to regulate the track width 6. Reference numeral 7 is a winding window for winding the coil 8 around the magnetic core halves 2A and 2B.

【0016】磁気コア半体2A,2Bには、Mn−Zn
系フエライトのような酸化物系磁性材料が用いられ、磁
性合金薄膜3A,3Bには、Fe−Al−Si系合金、
Co−Nb−Zr系アモルフアス合金などからなる高飽
和磁束密度および高透磁率を有する結晶質または非晶質
の合金材料が用いられる。また、接合部材5には、通常
PbO2 を主成分とする鉛系ガラスなどが用いられる。
The magnetic core halves 2A and 2B contain Mn-Zn.
An oxide magnetic material such as a system ferrite is used, and the magnetic alloy thin films 3A and 3B are made of a Fe-Al-Si alloy,
A crystalline or amorphous alloy material having a high saturation magnetic flux density and a high magnetic permeability, such as a Co—Nb—Zr-based amorphous alloy, is used. The joining member 5 is usually made of lead-based glass containing PbO 2 as a main component.

【0017】この磁気ヘツド1のテ―プ摺動面9の形状
としては、たとえばHi8VTR用としては摺動方向(つ
まり長手方向)イの長さが1〜2mm程度、幅方向の長さ
が50〜100μm程度であつて、摺動方向のア―ル
(曲率半径)が5〜10mm、幅方向のア―ルが1〜2mm
の滑らかな楕円曲面に形成されており、前記の磁気ギヤ
ツプ4はこのテ―プ摺動面9の中心に形成されている。
As the shape of the tape sliding surface 9 of the magnetic head 1, for example, for Hi8 VTR, the length in the sliding direction (that is, the longitudinal direction) is about 1 to 2 mm, and the length in the width direction is 50 mm. Approximately -100 μm, sliding direction arm (curvature radius) is 5-10 mm, width direction arm is 1-2 mm
Is formed into a smooth elliptic curved surface, and the magnetic gear 4 is formed at the center of the tape sliding surface 9.

【0018】このようなテ―プ摺動面9の幅方向ロの両
端側には、磁気テ―プの摺動方向イに沿う一対の溝10
a 10bが形成されており、その深さは、図3の
(A)に示す磁気テ―プの入側位置Xでの深さd1 より
も、図3の(B)に示す磁気テ―プの出側位置Yでの深
さd2 が小さくなるようにされている。この溝10a,
10bの幅としては、磁気テ―プの巻き込みによるテ―
プ損傷を防止するために、通常10μm以下であるのが
よい。上記の深さd1 ,d2 は、磁気ギヤツブ4の深さ
0 以下の1〜10μm程度であるのが望ましい。
At both ends of the tape sliding surface 9 in the width direction b, a pair of grooves 10 are formed along the magnetic tape sliding direction a.
a 10b is formed, and the depth thereof is larger than the depth d 1 at the entrance side position X of the magnetic tape shown in FIG. 3 (A), as shown in FIG. 3 (B). The depth d 2 at the outlet side position Y of the cup is set to be small. This groove 10a,
The width of 10b is a tape formed by winding a magnetic tape.
In order to prevent damage to the ridge, the thickness is usually 10 μm or less. The depths d 1 and d 2 are preferably about 1 to 10 μm, which is less than the depth d 0 of the magnetic gear tube 4.

【0019】上記構成の磁気ヘツドは、磁気コア半体へ
の磁性合金薄膜のスパツタリング、磁気ギヤツプ部のボ
ンデイング、磁気コアの切り出し、研削加工、ラツピン
グテ―プによるテ―プ摺動面の研磨などの通常の磁気ヘ
ツドの作製手順を経て、規定トラツク幅および所定ア―
ルのテ―プ摺動面としたのち、イオンミリング、スライ
サなどの回転砥石、化学エツチング、超音波加工などの
手段により、テ―プ摺動面の幅方向の両端側に一対の溝
を形成することにより、作製される。
The magnetic head having the above-mentioned structure is used for sputtering the magnetic alloy thin film onto the magnetic core half, bonding the magnetic gear part, cutting out the magnetic core, grinding, polishing the tape sliding surface by lapping tape, etc. After a normal magnetic head manufacturing procedure, the specified track width and specified
After making the tape sliding surface of the tape, a pair of grooves are formed on both ends in the width direction of the tape sliding surface by means such as ion milling, rotating grindstone such as slicer, chemical etching, ultrasonic machining, etc. It is produced by

【0020】この磁気ヘツドを回転ヘツド型ヘリキヤル
スキヤン方式のVTR(Hi8VTR;SONY CCD-V90
0 )に装備して、磁気テ―プと磁気ヘツドとの間のスペ
―シングを調べた。図5は厚い磁気テ―プ(総厚13μ
m)を、図6は薄い磁気テ―プ(総厚9μm)を用いた
場合で、両図中、実線(曲線−a,曲線−c)がこの発
明の上記構成の磁気ヘツド、破線(曲線−b,曲線−
d)が溝10a,10bを形成しない以外は上記と同様
構成とした比較用の磁気ヘツドである。
This magnetic head is a rotary head type helicopter scanning VTR (Hi8VTR; Sony CCD-V90).
Equipped with 0), we investigated the spacing between the magnetic tape and the magnetic head. Figure 5 shows a thick magnetic tape (total thickness 13μ
m) and FIG. 6 shows the case where a thin magnetic tape (total thickness 9 μm) is used. In both figures, the solid line (curve-a, curve-c) is the magnetic head and the broken line (curve) of the above-mentioned configuration of this invention. -B, curve-
The magnetic head for comparison has the same configuration as that described above except that d) does not form the grooves 10a and 10b.

【0021】この両図から明らかなように、厚い磁気テ
―プを用いた場合は、この発明の上記構成の磁気ヘツド
と比較用の磁気ヘツドとの間にほとんど差はないが、薄
い磁気テ―プを用いた場合、比較用の磁気ヘツドでは、
テ―プ摺動面の幅方向の両端側で接触して、ギヤツプ中
心位置のスペ―シングが著しく大きくなつているのに対
して、この発明の上記構成の磁気ヘツドによると、上記
両端側での接触が防がれて、ギヤツプ中心位置のスペ―
シングが低減されている。
As is clear from these figures, when a thick magnetic tape is used, there is almost no difference between the magnetic head having the above-mentioned structure of the present invention and the magnetic head for comparison, but a thin magnetic tape is used. -If a magnetic head for comparison is used,
While the spacing at the center position of the gear is significantly increased due to the contact on both widthwise sides of the tape sliding surface, according to the magnetic head having the above-mentioned structure of the present invention, the spacing at both ends is increased. Contact with the gear is prevented,
Thing is reduced.

【0022】また、薄い磁気テ―プを用いる場合に、こ
の発明の上記構成の磁気ヘツドと比較用の磁気ヘツドと
について、再生出力のエンベロ―プ波形、つまりエンベ
ロ―プ出力を調べたところ、図7に示す結果が得られ
た。図中、実線(曲線−α)がこの発明の上記構成の磁
気ヘツド、破線(曲線−β)が比較用の磁気ヘツドで、
この図から、この発明の上記構成の磁気ヘツドによれ
ば、比較用の磁気ヘツドの欠点である再生出力の低下を
防げることがわかる。
When a thin magnetic tape is used, the reproduction output envelope waveform, that is, the envelope output, is examined for the magnetic head having the above-described structure of the present invention and the magnetic head for comparison. The results shown in FIG. 7 were obtained. In the figure, the solid line (curve-α) is the magnetic head having the above-described configuration of the present invention, and the broken line (curve-β) is the magnetic head for comparison.
From this figure, it can be seen that the magnetic head having the above-described structure according to the present invention can prevent a reduction in reproduction output, which is a drawback of the comparative magnetic head.

【0023】なお、上記の実施例では、溝10a 10
bを磁気テ―プの入側端部より出側端部にかけて、つま
りテ―プ摺動面の全面にわたつて形成しているが、図4
に示すように、磁気テ―プの入側端部より磁気ギヤツプ
4を少し超えるあたりまで、つまりテ―プ摺動面の一部
に形成してもよく、この場合でも上記と同様の効果が得
られる。図4中の符号は、図1〜3の場合と同じであ
る。
In the above embodiment, the grooves 10a 10
b is formed from the entrance end to the exit end of the magnetic tape, that is, over the entire tape sliding surface.
As shown in FIG. 5, it may be formed from the entrance end of the magnetic tape to a portion slightly beyond the magnetic gear 4, that is, on a part of the tape sliding surface. can get. Reference numerals in FIG. 4 are the same as those in FIGS.

【0024】[0024]

【発明の効果】以上のように、この発明の磁気ヘツドに
よると、テ―プ摺動面の幅方向の両端部に形成した一対
の溝内に空気を流入させ、この流入空気に基づく圧出力
を利用することにより、薄い磁気テ―プでも良好なエン
ベロ―プ出力が得られるから、薄い磁気テ―プと厚い磁
気テ―プとの互換性にすぐれており、しかもテ―プ摺動
面は幅方向の長さを十分にとれるので、従来のような接
合部材の強度や耐摩耗性の点で問題を生じる心配がな
い。
As described above, according to the magnetic head of the present invention, air is caused to flow into a pair of grooves formed at both ends of the tape sliding surface in the width direction, and a pressure output based on the inflow air is produced. By using, good envelope output can be obtained even with a thin magnetic tape, so compatibility between thin magnetic tape and thick magnetic tape is excellent, and the tape sliding surface is also excellent. Since a sufficient width in the width direction can be obtained, there is no fear of causing a problem in the strength and wear resistance of the joining member as in the conventional case.

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

【図1】この発明の回転ヘツド型ヘリキヤルスキヤン方
式のVTR用磁気ヘツドの一例を示す斜視図である。
FIG. 1 is a perspective view showing an example of a magnetic head for a VTR of a rotary head type helicopter scan system of the present invention.

【図2】上記磁気ヘツドのテ―プ摺動面の正面図であ
る。
FIG. 2 is a front view of a tape sliding surface of the magnetic head.

【図3】上記磁気ヘツドのテ―プ摺動面の側面図で、
(A)は磁気テ―プの入側位置、(B)は出側位置であ
る。
FIG. 3 is a side view of the tape sliding surface of the magnetic head,
(A) is the entrance side position of the magnetic tape, and (B) is the exit side position.

【図4】テ―プ摺動面の一対の溝の形成態様が異なる例
を示す正面図である。
FIG. 4 is a front view showing an example in which a pair of grooves on a tape sliding surface are formed differently.

【図5】厚い磁気テ―プと磁気ヘツドとの間のスペ―シ
ングと、テ―プ摺動面の幅方向の変位との関係を示す特
性図である。
FIG. 5 is a characteristic diagram showing the relationship between the spacing between a thick magnetic tape and a magnetic head and the widthwise displacement of the tape sliding surface.

【図6】薄い磁気テ―プと磁気ヘツドとの間のスペ―シ
ングと、テ―プ摺動面の幅方向の変位との関係を示す特
性図である。
FIG. 6 is a characteristic diagram showing the relationship between the spacing between a thin magnetic tape and a magnetic head and the displacement of the tape sliding surface in the width direction.

【図7】薄い磁気テ―プを用いた場合の、再生出力のエ
ンベロ―プ波形を示す特性図である。
FIG. 7 is a characteristic diagram showing an envelope waveform of reproduction output when a thin magnetic tape is used.

【図8】従来の磁気ヘツドにおいて、厚い磁気テ―プと
磁気ヘツドのテ―プ摺動面との接触状態を示す側面図で
ある。
FIG. 8 is a side view showing a contact state between a thick magnetic tape and a tape sliding surface of the conventional magnetic head.

【図9】従来の磁気ヘツドにおいて、薄い磁気テ―プと
磁気ヘツドのテ―プ摺動面との接触状態を示す側面図で
ある。
FIG. 9 is a side view showing a contact state between a thin magnetic tape and a tape sliding surface of the conventional magnetic head.

【図10】従来の磁気ヘツドのひとつとして、テ―プ摺
動面の幅方向の両端部を面取りした状態を示す側面図で
ある。
FIG. 10 is a side view showing a state in which both widthwise ends of a tape sliding surface are chamfered as one of conventional magnetic heads.

【図11】従来の磁気ヘツドのひとつとして、テ―プ摺
動面の幅方向の両端部を上記とは異なる態様で面取りし
た状態を示す側面図である。
FIG. 11 is a side view showing, as one of the conventional magnetic heads, a state in which both widthwise end portions of a tape sliding surface are chamfered in a manner different from the above.

【符号の説明】[Explanation of symbols]

1 磁気ヘツド 2A,2B 磁気コア半体 3A,3B 磁性合金薄膜 4 磁気ギヤツプ 5 接合部材 9 テ―プ摺動面 イ テ―プ摺動面の摺動方向(長手方向) ロ テ―プ摺動面の幅方向 10a,10b 一対の溝 X 磁気テ―プの入側位置 Y 磁気テ―プの出側位置 d1 一対の溝の磁気テ―プの入側位置の深さ d2 一対の溝の磁気テ―プの出側位置の深さ d0 磁気ギヤツプの深さ 実線(曲線−a,c,α) この発明の磁気ヘツド 破線(曲線−b,d,β) 比較用の磁気ヘツド T1 厚い磁気テ―プ T2 薄い磁気テ―プ1 Magnetic head 2A, 2B Magnetic core half 3A, 3B Magnetic alloy thin film 4 Magnetic gear 5 Joining member 9 Tape sliding surface Sliding direction of tape sliding surface (longitudinal direction) Tape sliding Width direction of surface 10a, 10b Pair of grooves X Magnetic tape entry side position Y Magnetic tape exit side position d 1 Depth of pair of grooves magnetic tape entry side d 2 Pair of grooves magnetic tape - the depth of the exit side position of the flop d 0 magnetic Giyatsupu depth solid (curve -a, c, α) magnetic head dashed present invention (curve -b, d, β) the magnetic head T for comparison 1 thick magnetic tape T 2 thin magnetic tape

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 テ―プ摺動面の幅方向の両端側に、磁気
テ―プの摺動方向に沿う一対の溝を、その深さが磁気テ
―プの入側位置よりも出側位置で小さくなるように形成
したことを特徴とする磁気ヘツド。
1. A pair of grooves extending along the sliding direction of the magnetic tape on both ends of the tape sliding surface in the width direction, the depth of which is greater than the entrance side of the magnetic tape on the exit side. A magnetic head characterized in that it is formed so as to become smaller in position.
【請求項2】 回転ヘツド型ヘリキヤルスキヤン方式の
磁気記録再生装置に使用する請求項1に記載の磁気ヘツ
ド。
2. The magnetic head according to claim 1, wherein the magnetic head is used in a rotary head type helical recording / reproducing system.
JP25637193A 1993-09-20 1993-09-20 Magnetic head Expired - Fee Related JP3590644B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP25637193A JP3590644B2 (en) 1993-09-20 1993-09-20 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP25637193A JP3590644B2 (en) 1993-09-20 1993-09-20 Magnetic head

Publications (2)

Publication Number Publication Date
JPH0793708A true JPH0793708A (en) 1995-04-07
JP3590644B2 JP3590644B2 (en) 2004-11-17

Family

ID=17291765

Family Applications (1)

Application Number Title Priority Date Filing Date
JP25637193A Expired - Fee Related JP3590644B2 (en) 1993-09-20 1993-09-20 Magnetic head

Country Status (1)

Country Link
JP (1) JP3590644B2 (en)

Also Published As

Publication number Publication date
JP3590644B2 (en) 2004-11-17

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