JPS63213106A - Magnetic head - Google Patents

Magnetic head

Info

Publication number
JPS63213106A
JPS63213106A JP4642287A JP4642287A JPS63213106A JP S63213106 A JPS63213106 A JP S63213106A JP 4642287 A JP4642287 A JP 4642287A JP 4642287 A JP4642287 A JP 4642287A JP S63213106 A JPS63213106 A JP S63213106A
Authority
JP
Japan
Prior art keywords
magnetic
depth
gap
magnetic gap
head
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
Application number
JP4642287A
Other languages
Japanese (ja)
Inventor
Yoshiyuki Kunito
国頭 義之
Heikichi Sato
平吉 佐藤
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.)
Sony Corp
Original Assignee
Sony 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 Sony Corp filed Critical Sony Corp
Priority to JP4642287A priority Critical patent/JPS63213106A/en
Publication of JPS63213106A publication Critical patent/JPS63213106A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a high output by reducing the adverse effect of magnetic resistance and leakage at a part in the neighborhood of a magnetic gap and to improve reliability and workability, by forming the cutting plane of a winding groove on a magnetic gap side in curved structure, and selecting a tilt angle, etc., appropriately. CONSTITUTION:The cutting plane on the magnetic gap (g) side is constituted of first and second cutting planes 5a and 5b out of the cutting planes formed in the winding groove 5, and the tilt angle thetaH is set between 80-90 deg. and thetaW between 20-70 deg., and the length LH of the plane 5a is set at 0.3-1.5 times the depth DP of the magnetic gap. Therefore, it is possible to reduce the leakage keeping the core capacity of the part in the neighborhood of the gap (g), and to obtain the high output, and also, to obtain the high picture quality of a reproducing image, etc. Also, since the plane 5a is notched in a prescribed length LH in a direction almost orthogonal to a coupling plane 6, the depth DP can be measured with high accuracy in the range of the length LH even when an opaque part is generated on welding glass 8 in the neighborhood of the gap (g). Therefore, it is possible to perform the measuring work of the DP rapidly and with high accuracy. In such a way, the reliability and the workability can be improved.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、ビデオテープレコーダ(VTR)等の磁気記
録再生装置に搭載される磁気ヘッドに関し、詳細には磁
気ギャップのデプスを規制する巻線溝の形状に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a magnetic head installed in a magnetic recording/reproducing device such as a video tape recorder (VTR), and in particular, a winding that regulates the depth of a magnetic gap. Regarding the shape of the groove.

〔発明の概要〕[Summary of the invention]

本発明は、一対の磁気コア半体を突き合わせて磁気ギャ
ップを形成してなる。所謂バルク構造の磁気ヘッドにお
いて、 磁気ギャップのデプスを規制する巻線溝の磁気ギャップ
側の切削面のうち、前記デプスを規制する磁気ギャップ
側の切削面を前記接合面に対して80″〜90@傾斜さ
せ、その磁気記録媒体走行方向の長さを前記デプスの0
.3〜1.5倍とするとともに、これよりも離れた位置
での接合面に対する傾斜角度を20”〜70@とし、前
記磁気ギャップ側の切削面を屈曲させることにより、磁
気ギャップ近傍部における磁気的な各種損失を低減し、
磁気ヘッドの高出力化を実現しようとするものである。
In the present invention, a pair of magnetic core halves are butted against each other to form a magnetic gap. In a magnetic head with a so-called bulk structure, among the cut surfaces on the magnetic gap side of the winding groove that regulates the depth of the magnetic gap, the cut surface on the magnetic gap side that regulates the depth is 80" to 90" with respect to the bonding surface. @ Incline the magnetic recording medium, and set the length of the magnetic recording medium in the running direction to 0 of the depth.
.. 3 to 1.5 times, and the inclination angle to the joint surface at a position further away from this is set to 20" to 70@, and by bending the cut surface on the magnetic gap side, the magnetic field in the vicinity of the magnetic gap is reduced. reduce various types of losses,
This is an attempt to realize high output of a magnetic head.

〔従来の技術〕[Conventional technology]

一般に、テープレコーダやビデオテープレコーダ等の磁
気記録再生装置には、電気信号を磁気信号に変換して記
録し、また磁気信号を電気信号として再生する電磁変換
素子として磁気ヘッドが搭載されている。
Generally, a magnetic recording/reproducing device such as a tape recorder or a video tape recorder is equipped with a magnetic head as an electromagnetic transducer element that converts an electric signal into a magnetic signal for recording and reproduces the magnetic signal as an electric signal.

この種の磁気ヘッドは、例えば第5図(A)及び第5図
(B)に示すように、一対の磁気コア半体(101) 
、 (102)をギャップスペーサ(103)を介して
突き合わせ、融着用ガラス(105)にて接合し磁気ギ
ャップgを形成している。そして、一方の磁気コア半体
(101)には、コイル導線(104)を巻回するため
に巻線溝(106)が穿設され、当該巻線溝(106)
の切削面のうち、磁気ギヤツブg側の切削面(106a
)にてデプスDρを規制する構成となっている。
This type of magnetic head includes a pair of magnetic core halves (101), as shown in FIGS. 5(A) and 5(B), for example.
, (102) are butted together with a gap spacer (103) interposed therebetween and bonded with a fusing glass (105) to form a magnetic gap g. A winding groove (106) is formed in one magnetic core half (101) in order to wind the coil conductor (104), and the winding groove (106)
Among the cutting surfaces, the cutting surface on the side of the magnetic gear g (106a
) is configured to regulate the depth Dρ.

ここで従来、上記切削面(106a)と磁気コア半体の
接合面(107)とがなす角度αは、コイル導線(10
4)の巻回作業等を考慮し略55°に設定している。
Conventionally, the angle α between the cutting surface (106a) and the joining surface (107) of the magnetic core half is
The angle is set to approximately 55° in consideration of the winding work etc. in 4).

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

ところで近年では、再生画像等の一層の高品質化が望ま
れ、その対策として磁気ヘッドの高出力化を図るために
、ヘッド効率の向上を目的とした研究が盛んに進められ
ている。
Incidentally, in recent years, there has been a desire for higher quality of reproduced images, etc., and as a countermeasure to this, research aimed at improving head efficiency has been actively conducted in order to increase the output of magnetic heads.

しかしながら、従前の磁気ヘッドにおいては、上記切削
面(106a)と接合面(107)とが近接した構造と
なっているため、リーケージと称される洩れ磁束(第5
図CB)中符号Aで示す〕が顕著に現れる。特に、上記
リーケージはデプスop近傍部分で大きく、ヘッド効率
の低下を招いている。
However, in the conventional magnetic head, since the cut surface (106a) and the bonding surface (107) are close to each other, leakage magnetic flux called leakage (fifth
(Fig. CB)) marked with the symbol A] appears prominently. In particular, the leakage is large in the vicinity of the depth op, leading to a decrease in head efficiency.

また、磁気コア半体(101)、 (102)をガラス
融着する際に、この融着用ガラス(105) と磁気コ
ア材あるいはギャップ材とが反応し、この結果磁気ギャ
ップg近傍に充填された融着用ガラス(105)は不透
明となってしまう。したがって、ヘッドの性能に重要で
あるデプスOpを高精度に測定することが困難となり、
ヘッドの信頼性あるいは作業性の点で問題となっている
Furthermore, when glass fusing the magnetic core halves (101) and (102), the fusing glass (105) reacts with the magnetic core material or the gap material, and as a result, the vicinity of the magnetic gap g is filled. The glass for fusing (105) becomes opaque. Therefore, it becomes difficult to measure the depth Op, which is important for head performance, with high precision.
This poses a problem in terms of head reliability or workability.

そこで本発明は、かかる従来の実情に鑑みて提案された
ものであり、磁気ギャップ近傍部の磁気抵抗が小さく且
つリーケージの悪影響も少なく、高出力化が可能で、し
かも信頼性1作業性に優れた磁気ヘッドを提供すること
を目的とする。
Therefore, the present invention has been proposed in view of the conventional situation, and has a structure in which the magnetic resistance near the magnetic gap is small, the negative effects of leakage are small, high output is possible, and the reliability and workability are excellent. The purpose of the present invention is to provide a magnetic head with improved characteristics.

(問題点を解決するための手段) 上述の目的を達成するために、本発明の磁気ヘッドは、
一対の磁気コア半体を突き合わせて磁気ギャップを形成
するとともに、前記磁気コア半体の少な(とも一方の接
合面に設けられた巻線溝によって前記磁気ギャップのデ
プスを規制してなる磁気ヘッドにおいて、前記S線溝の
磁気ギャップ側の切削面のうち、前記デプスを規制する
磁気ギャップ近傍部分の傾斜角度を前記接合面に対して
80″〜90″とし、その磁気記録媒体走行方向の長さ
を前記デプスの0.3〜1.5倍とするとともに、これ
よりも離れた位置での傾斜角度を前記接合面に対して2
0°〜70″とし、前記磁気ギャップ側の切削面を屈曲
させたことを特徴とするものである。
(Means for solving the problems) In order to achieve the above-mentioned object, the magnetic head of the present invention has the following features:
In a magnetic head in which a pair of magnetic core halves are butted against each other to form a magnetic gap, and the depth of the magnetic gap is regulated by a winding groove provided on the joint surface of one of the magnetic core halves. , of the cut surface on the magnetic gap side of the S-line groove, the inclination angle of the portion near the magnetic gap that regulates the depth is 80'' to 90'' with respect to the bonding surface, and the length thereof in the running direction of the magnetic recording medium. is 0.3 to 1.5 times the depth, and the angle of inclination at a position further away than this is 2 to the joining surface.
0° to 70″, and is characterized in that the cut surface on the side of the magnetic gap is bent.

〔作用〕[Effect]

本発明では、巻線溝の磁気ギャップ側の切削面を屈曲構
造とし、デプスを規制する切削面の接合面に対する傾斜
角度を80″〜90″とし、その磁気記録媒体走行方向
の長さをデプスの0.3〜1゜5倍とし、これよりも離
れた位置でのtlJI斜角度を20°〜70″としてい
るので、これら切削面と接合面との間の距離が確保され
る。特に、磁気ギャップ近傍部において、上記切削面と
接合面間の距離が確保できることより、リーケージによ
るー・ラド効率の低下は大幅に減少する。したがって、
ヘッドの高出力化が実現される。
In the present invention, the cut surface on the magnetic gap side of the winding groove has a bent structure, the inclination angle of the cut surface that regulates the depth with respect to the bonding surface is 80'' to 90'', and the length in the running direction of the magnetic recording medium is the depth. Since the tlJI slope angle at a position further away from this is set to 0.3 to 1°5 times the angle of 20° to 70'', the distance between these cutting surfaces and the joint surface is secured.In particular, Since the distance between the cutting surface and the bonding surface can be secured in the vicinity of the magnetic gap, the decrease in Rad efficiency due to leakage is significantly reduced.
High output of the head is realized.

〔実施例〕〔Example〕

以下、本発明を適用した実施例について図面を参照しな
がら説明する。
Embodiments to which the present invention is applied will be described below with reference to the drawings.

本実施例の磁気ヘッドは、第1図(A)及び第1図(B
)に示すように、磁気コア半体(1) 、 (2)が例
えばMn−Znフェライト等の軟磁性材料で構成され、
これら磁気コア半体(1) 、 (2)の所定の接合面
同士をギャップスペーサ(3)を介して突き合わせ融着
用ガラス(8)にて固定し、記録再生に関与する磁気ギ
ャップgを形成してなるものである。また、上記磁気ギ
ャップgが露出する磁気記録媒体摺動面(7)には円筒
研磨が施され、磁気記録媒体と良好な摺接が得られる構
成となっている。
The magnetic head of this example is shown in FIGS. 1(A) and 1(B).
), the magnetic core halves (1) and (2) are made of a soft magnetic material such as Mn-Zn ferrite,
The predetermined joint surfaces of these magnetic core halves (1) and (2) are butted together via a gap spacer (3) and fixed with a glass for fusing (8) to form a magnetic gap g involved in recording and reproduction. This is what happens. Further, the magnetic recording medium sliding surface (7) where the magnetic gap g is exposed is subjected to cylindrical polishing, so that good sliding contact with the magnetic recording medium can be obtained.

そして、上記磁気コア半体(1) 、 (2)のうち、
一方の磁気コア半体(1)の接合面には、磁気ギャップ
gのデプスDpを規制するとともに、コイル導線(4)
を巻装するだめの巻線溝(5)が穿設され、他方の磁気
コア半体(2)の接合面(6) は平坦な構造となって
いる。
Of the magnetic core halves (1) and (2),
On the joint surface of one magnetic core half (1), the depth Dp of the magnetic gap g is regulated, and a coil conductor (4) is provided.
A winding groove (5) for winding the magnetic core is formed, and the joint surface (6) of the other magnetic core half (2) has a flat structure.

本実施例では上記巻線溝(5)が、磁気ギヤツブg側に
位置しデプスOpを規制する第1の切削面(5a)と、
該第1の切削面(5a)よりも磁気ギャップgから離れ
て位置する第2の切削面(5b)と、接合面(6)と対
向配置される第3の切削面(5c)と、バックギャップ
側に位置する第4の切削面(5d)とで構成され、全体
的にみたときにその外観が略々台形の構造となっている
In this embodiment, the winding groove (5) has a first cutting surface (5a) located on the side of the magnetic gear g and regulating the depth Op;
a second cutting surface (5b) located further from the magnetic gap g than the first cutting surface (5a); a third cutting surface (5c) disposed opposite to the bonding surface (6); and a fourth cutting surface (5d) located on the gap side, and has a substantially trapezoidal appearance when viewed as a whole.

ここで、上記巻線溝(5)により形成される切削面のう
ち、磁気ギヤツブg側に位置する第1の切削面(5a)
及び第2の切削面(5b)は、それぞれ接合面(6)に
対す傾斜角度θ□、θ1が、80”≦08≦90″ 20°≦01≦70″ なる範囲内に設定され、同時に上記第1の切削面(5a
)の磁気記録媒体走行方向Xの長さし、Iが、0.3X
op≦L++≦1.5Xop となるように設定されている。
Here, among the cutting surfaces formed by the winding groove (5), the first cutting surface (5a) located on the magnetic gear g side
and the second cutting surface (5b) have inclination angles θ□ and θ1 with respect to the joint surface (6), respectively, set within the ranges of 80"≦08≦90"20°≦01≦70", and at the same time the above-mentioned First cutting surface (5a
) is the length of the magnetic recording medium in the running direction X, and I is 0.3X
It is set so that op≦L++≦1.5Xop.

すなわち本実施例では、上記巻線溝(5)の磁気ギヤツ
ブg側の切削面を第1及び第2の切削面(5a) 、 
(5b)とで構成し、第1の切削面(5a)を接合面(
6)に対し略直交する方向に所定長さり、たけ切欠き、
同時に第2の切削面(5b)の傾斜角度θ8を制御する
ことに大きな特徴を有している。上記巻線溝(5)を上
述のように設定すれば、これら切削面(5a) 、 (
5b)と接合面(6)との距離が確保されるので、磁気
ギャップ近傍部のり一ケージが減少しヘッド効率が向上
する。たとえ第2の切削面(5b)の傾斜角度θ1が従
前のへラド(α=55’)よりも小さくリーケージが従
来と同程度であっても、この場合には磁気ギヤツブg近
傍のコア容積が増加し磁気抵抗が低下することより、ヘ
ッド効率は向上する。
That is, in this embodiment, the cut surface of the winding groove (5) on the magnetic gear g side is the first and second cut surfaces (5a),
(5b), and the first cutting surface (5a) is the joint surface (
6) a predetermined length and a tall notch in a direction substantially perpendicular to
A major feature is that the inclination angle θ8 of the second cutting surface (5b) is controlled at the same time. If the winding groove (5) is set as described above, these cutting surfaces (5a), (
5b) and the bonding surface (6), the glue cage in the vicinity of the magnetic gap is reduced and the head efficiency is improved. Even if the inclination angle θ1 of the second cutting surface (5b) is smaller than that of the conventional helad (α=55') and the leakage is about the same as the conventional one, in this case, the core volume near the magnetic gear g As the magnetic resistance increases and the magnetic resistance decreases, the head efficiency improves.

ここで、上記第1の切削面(5a)の傾斜角度θ。Here, the inclination angle θ of the first cutting surface (5a).

が80°未満では、接合面(6)と該切削面(5a)と
が近接し、この部分でのり一ケージが顕著となりヘッド
効率の改善が難しい。逆に、上記傾斜角度θ、が90@
を越えた場合には、デプスopの減少に対して第1及び
第2の切削面で形成される屈曲部(5^)での磁気抵抗
が大きくなり、ヘッドの性能上問題がある。したがって
、上記傾斜角度θ8は80″〜90”の範囲内に設定す
ることが好ましい。なお、デプスDlpの精度や巻線溝
の加工性等の観点からは、上記傾斜角度θイは90″と
することがより好ましい。
When the angle is less than 80°, the joint surface (6) and the cutting surface (5a) are close to each other, and the glue cage becomes noticeable in this part, making it difficult to improve the head efficiency. Conversely, the above inclination angle θ is 90@
If the depth OP is exceeded, the magnetic resistance at the bent portion (5^) formed by the first and second cutting surfaces increases as the depth OP decreases, causing a problem in terms of head performance. Therefore, it is preferable that the inclination angle θ8 is set within the range of 80'' to 90''. In addition, from the viewpoint of the accuracy of the depth Dlp, the workability of the winding groove, etc., it is more preferable that the above-mentioned inclination angle θa is 90''.

また、上記第1の切削面(5a)の長さ−L9がデプス
opの0.3倍未満では、この切削面(5a)を形成し
た効果が薄れ、第2の切削面(5b)と接合面(6)と
が近接することにょろり一ケージが顕著となって、誘起
磁束が減少する。逆に、上記長さり、がデプス[11)
の1.5倍を越えると、磁気ギヤツブg近傍のコア容積
が減少することより、ヘッド効率が低下する。したがっ
て、上記長さし□はデプスOpの0゜3〜1.5倍に設
定する。
Furthermore, if the length -L9 of the first cut surface (5a) is less than 0.3 times the depth op, the effect of forming this cut surface (5a) will be weakened, and it will be bonded to the second cut surface (5b). As the surface (6) approaches, the cage becomes more noticeable and the induced magnetic flux decreases. Conversely, the above length is the depth [11]
If it exceeds 1.5 times, the core volume near the magnetic gear g decreases, resulting in a decrease in head efficiency. Therefore, the length □ is set to 0.3 to 1.5 times the depth Op.

さらに、上記第2の切削面(5b)の傾斜角度θ。Furthermore, the inclination angle θ of the second cutting surface (5b).

が20″未満では、該切削面(5b)と接合面(6)と
が近接して向かい合った構造となり、リーケージの悪影
響が顕著となり、逆に70°を越えると磁気ギヤツブg
近傍のコア容積が小さくなり、何れの場合にもヘッド効
率の改善が困難となる。したがって、上記傾斜角度θ8
は20”〜70@に設定する。
If the angle is less than 20", the cut surface (5b) and the joint surface (6) will face each other in close proximity, and the adverse effects of leakage will be significant. On the other hand, if it exceeds 70 degrees, the magnetic gear g
The volume of the core in the vicinity becomes smaller, making it difficult to improve head efficiency in either case. Therefore, the above inclination angle θ8
is set to 20” to 70@.

このように本実施例では、巻線溝(5)にて形成される
切削面のうち、磁気ギヤツブg側の切削面を第1及び第
2の切削面(5a) 、 (5b)で構成し、これら切
削面(5a) 、 (5b)の傾斜角度θ1110−及
び第1の切削面(5a)の長さLHを上記範囲内に設定
しているので、磁気ギヤツブg近傍部のコア容積を確保
したまま、リーケージを低減することができる。
As described above, in this embodiment, among the cutting surfaces formed by the winding groove (5), the cutting surface on the side of the magnetic gear g is composed of the first and second cutting surfaces (5a) and (5b). , since the inclination angle θ1110- of these cutting surfaces (5a) and (5b) and the length LH of the first cutting surface (5a) are set within the above range, the core volume near the magnetic gear g is secured. Leakage can be reduced while maintaining the

したがって、本実施例の磁気ヘッドにおいては、巻線溝
(5)の形状に起因するリーケージ等の磁気的な各種損
失を最小限に抑えることができるので、より一層の高出
力化が実現される。この結果、再生画像等の高品位化に
好適な磁気ヘッドが提供できる。
Therefore, in the magnetic head of this embodiment, various magnetic losses such as leakage caused by the shape of the winding groove (5) can be minimized, and even higher output can be achieved. . As a result, a magnetic head suitable for improving the quality of reproduced images and the like can be provided.

また、第1の切削面(5a)を接合面(6)に対して略
直交方向に所定長さLSIに切欠いているので、磁気ギ
ヤツブg近傍の融着用ガラス(8)に不透明部が発生し
ても、デプスopは上記長さL工の範囲内で精度良く測
定できる。したがって、デプスの測定作業を迅速かつ高
精度に行えるので、ヘッドの信頼性や作業性が大幅に向
上する。
In addition, since the first cut surface (5a) is cut out to a predetermined length LSI in a direction substantially perpendicular to the joint surface (6), an opaque portion is not generated in the fusion glass (8) near the magnetic gear g. However, the depth op can be measured accurately within the range of the length L described above. Therefore, the depth measurement work can be performed quickly and with high precision, and the reliability and workability of the head are greatly improved.

以上、本発明の一実施例について説明したが、本発明は
この実施例に限定されず、本発明の趣旨を逸脱しない範
囲内で種々の構造をとり得る。なお、以下の説明で引用
する第2図(A)及び第2図(B)、第3図(A)及び
第3図(B)、第4図(A)及び第4図(B)に示す磁
気ヘッドにおいて、第1図(A)及び第1図(B)に示
す磁気ヘッドと同一部材には同−符号付しその詳細な説
明は省略する。
Although one embodiment of the present invention has been described above, the present invention is not limited to this embodiment, and can take various structures without departing from the spirit of the present invention. In addition, in Figure 2 (A) and Figure 2 (B), Figure 3 (A) and Figure 3 (B), Figure 4 (A) and Figure 4 (B) cited in the following explanation. In the magnetic head shown, the same members as those of the magnetic heads shown in FIGS. 1(A) and 1(B) are given the same reference numerals, and detailed explanation thereof will be omitted.

例えば、第2図(A)及び第2図(B)に示すように、
先の実施例における巻線溝(5)が穿設された磁気コア
半体(1)を2個用意し、これら磁気コア半体(1) 
、 (1)をギャップスペーサ(3)を介して接合一体
化した磁気ヘッドとしてもよい。このように両磁気コア
半体に巻線溝を設ければ、対向する切削面(5b) 、
 (5b)間の距離が大きくなり、リーケージの悪影響
をより低減できる。
For example, as shown in FIG. 2(A) and FIG. 2(B),
Prepare two magnetic core halves (1) in which the winding grooves (5) in the previous embodiment are perforated, and
, (1) may be integrated into a magnetic head via a gap spacer (3). If winding grooves are provided in both magnetic core halves in this way, the opposing cutting surfaces (5b),
(5b) becomes larger, and the adverse effects of leakage can be further reduced.

この場合、第1の切削面(5a) 、 (5a)が必ず
しも一直線状に連なるように構成する必要はなく、第2
図(B)示すようにデプス方向で多少ズレるよに配置さ
せても、デプスopを規制する磁気コア半体の巻線溝が
上記要件を満足していればリーケージは改善される。
In this case, the first cutting surfaces (5a) and (5a) do not necessarily need to be configured in a straight line, and the second
Even if the magnetic core halves are arranged with some deviation in the depth direction as shown in Figure (B), leakage can be improved if the winding grooves of the magnetic core halves that regulate the depth OP satisfy the above requirements.

あるいは、第3図(A)及び第3図(B)に示すように
、一対の磁気コア半体(1) 、 (2)が、それぞれ
Mn−Znフェライト等の酸化物磁性材料よりなる磁気
コア部(la) 、 (2a) と、この磁気コア部(
La) 、 (2a)の当接面に配設された強磁性金属
薄膜(lb) 、 (2b)との複合磁性材料で構成さ
れ、これら強磁性金属薄膜(lb) 、 (2b)同士
の突き合わせ面を磁気ギヤツブgとした所謂複合型の磁
気ヘッドにも本発明は適用される。
Alternatively, as shown in FIGS. 3(A) and 3(B), the pair of magnetic core halves (1) and (2) are each made of an oxide magnetic material such as Mn-Zn ferrite. parts (la), (2a), and this magnetic core part (
It is composed of a composite magnetic material with ferromagnetic metal thin films (lb) and (2b) arranged on the contact surfaces of La) and (2a), and these ferromagnetic metal thin films (lb) and (2b) are butted against each other. The present invention is also applicable to a so-called composite type magnetic head whose surface is a magnetic gear g.

ただし、上述の如く磁気コア半体(1) 、 (2)を
複合磁性材料で構成した場合、第1の切削面(5a)の
媒体走行方向Xの長さり、は、’A磁性金属薄膜(11
)の膜厚を含んで、第1及び第2の切削面(5a) 。
However, when the magnetic core halves (1) and (2) are made of a composite magnetic material as described above, the length of the first cutting surface (5a) in the medium running direction X is 'A magnetic metal thin film ( 11
) of the first and second cutting surfaces (5a).

(5b)による屈曲部(5A)までの長さとする。(5b) to the bent part (5A).

さらには、第4図(A)及び第4図(B)示すように、
第2図(A>及び第2図(B)に示す磁気へラドのコア
材として上述の複合磁性材料を用いた複合型の磁気ヘッ
ドとしてもよい。
Furthermore, as shown in FIGS. 4(A) and 4(B),
A composite magnetic head may be used in which the above-described composite magnetic material is used as the core material of the magnetic helad shown in FIGS. 2(A> and 2(B)).

このように磁気コア半体(1) 、 (2)に複合磁性
材料を用いた磁気ヘッドに本発明を適用すれば、巻線溝
(5)の形状に起因する各種損失が低減されることは勿
論のこと、高密度記録に対応したメタルテープ等の高抗
磁力磁気記録媒体に対して優れた記録特性及び再生特性
が発揮できる磁気ヘッドが提供される。
As described above, if the present invention is applied to a magnetic head using a composite magnetic material for the magnetic core halves (1) and (2), various losses caused by the shape of the winding groove (5) can be reduced. Needless to say, a magnetic head is provided that can exhibit excellent recording and reproducing characteristics for high coercive force magnetic recording media such as metal tapes that are compatible with high-density recording.

なお、上記複合型の磁気ヘッドにおいて、磁気記録媒体
摺接面(7)の構造、すなわち強磁性金属薄膜(Ib)
 、 (2b)の配置構造は、この種の複合磁気ヘッド
として従来から公知である種々の構造をとり得ることが
できる。
In addition, in the above composite magnetic head, the structure of the magnetic recording medium sliding contact surface (7), that is, the ferromagnetic metal thin film (Ib)
, (2b) can take various conventionally known structures for this type of composite magnetic head.

ここで、上記強磁性金属薄膜(lb) 、 (2b)と
しては、高飽和磁束密度を有し軟磁気特性に優れた合金
が使用され、具体的にはアモルファス合金等の非晶質系
の磁性材料、あるいはFe−A(1−3i系合金。
Here, as the ferromagnetic metal thin film (lb), (2b), an alloy having a high saturation magnetic flux density and excellent soft magnetic properties is used. Specifically, an amorphous magnetic material such as an amorphous alloy is used. material or Fe-A (1-3i alloy).

Fe−Al−Ge系合金+  F e  G a  S
 i系合金。
Fe-Al-Ge alloy + Fe Ga S
i-based alloy.

Fe−Ga−Ge系合金+  F a  G e  S
 i系合金等の結晶系の磁性材料が用いられる。
Fe-Ga-Ge alloy + F a G e S
A crystalline magnetic material such as an i-based alloy is used.

本発明者等は、上述の各磁気ヘッドについて、磁気コア
半体をM n −Z nフェライトで構成し、トラック
幅を25μm、デプスopを25μm、ギャップ長を0
.25μmに統一し、同条件のもとてそれぞれ磁気ヘッ
ドを作成した。なお、第3図(A)及び第4図(A)に
示す磁気ヘッドにおいては、強磁性金属薄膜(lb) 
、 (2b)として膜厚が3μmのFe−Ga−3i系
合金薄膜を形成した。
The present inventors constructed each magnetic head described above by constructing a magnetic core half of Mn-Zn ferrite, having a track width of 25 μm, a depth op of 25 μm, and a gap length of 0.
.. The thickness was unified to 25 μm, and magnetic heads were manufactured under the same conditions. Note that in the magnetic heads shown in FIGS. 3(A) and 4(A), a ferromagnetic metal thin film (lb)
As (2b), a Fe-Ga-3i alloy thin film having a thickness of 3 μm was formed.

次いで、これら各磁気ヘッドの5MHzにおけるインダ
クタンス、Q、再生出力をそれぞれ測定した。
Next, the inductance, Q, and reproduction output of each of these magnetic heads at 5 MHz were measured.

なお、第1図(A)及び第2図(A)に示すヘッドと比
較するために第5図(A)に示す磁気ヘッドについても
前記磁気特性を測定し、第3図(A)及び第4図(A)
に示すヘッドと比較するために第5図(A)と同一構造
で磁気コア半体を上記複合磁性材料で構成した磁気ヘッ
ドを作成し、この磁気ヘッドについても前記各磁気特性
を測定した。これらの測定結果を第1表にまとめて示す
In addition, in order to compare with the heads shown in FIGS. 1(A) and 2(A), the magnetic properties of the magnetic head shown in FIG. 5(A) were also measured, and the magnetic characteristics shown in FIGS. Figure 4 (A)
In order to compare with the head shown in FIG. 5A, a magnetic head having the same structure as that shown in FIG. 5(A) and having a magnetic core half made of the above-mentioned composite magnetic material was prepared, and the above-mentioned magnetic properties were also measured for this magnetic head. These measurement results are summarized in Table 1.

但し、表中の測定値は、各磁気ヘッドをそれぞれ10個
作成しこれらの平均値を示す。
However, the measured values in the table are the average values obtained by producing 10 magnetic heads of each type.

第1表 この第1表から明らかなように、本発明を適用した磁気
ヘッドは、リーケージが減少することより、再生出力(
5MHz)が0.6〜1.0 d B程度向上すること
が確認された。また、ヘッドのQ(5MHz)が3〜1
0%向上することがわかった。したがって、本゛発明を
適用することにより、磁気ヘッドの高出力化が実現され
、高品位の再生画像が得られることがわかった。
Table 1 As is clear from Table 1, the magnetic head to which the present invention is applied has a reduction in leakage, which improves the playback output (
5MHz) was confirmed to be improved by about 0.6 to 1.0 dB. Also, the Q (5MHz) of the head is 3 to 1.
It was found that the improvement was 0%. Therefore, it has been found that by applying the present invention, a high output magnetic head can be realized and a high quality reproduced image can be obtained.

〔発明の効果〕〔Effect of the invention〕

以上の説明からも明らかなように、本発明では巻線溝の
切削面のうち磁気ギャップ側の切削面を屈曲構造とし、
これら切削面の接合面に対する傾斜角度を規制するとと
もに、デプスを規制する磁気ギャップ近傍部分の切削面
の磁気記録媒体走行方向の長さを当該デプスの0.3〜
1.5倍に設定しているので、磁気ギャップ側の切削面
と接合面との距離が確保される。この結果、リーケージ
が減少する等、巻線溝の形状に起因する磁気的な各種損
失が低減されるので、ヘッドの高出力化が実現できる。
As is clear from the above description, in the present invention, among the cut surfaces of the winding groove, the cut surface on the magnetic gap side has a bent structure,
In addition to regulating the inclination angle of these cut surfaces with respect to the bonding surface, the length of the cut surface near the magnetic gap that regulates the depth in the running direction of the magnetic recording medium is set to 0.3 to 0.3 of the depth.
Since it is set to 1.5 times, the distance between the cut surface on the magnetic gap side and the bonding surface is ensured. As a result, leakage is reduced and various magnetic losses due to the shape of the winding grooves are reduced, so that high output of the head can be realized.

また、デプスを規制する切削面の傾斜角度を上記接合面
に対して略直交方向としているので、デプスの測定が迅
速かつ高精度に行え、ヘッドの偉績性や作業性も同時に
改善される。
Furthermore, since the angle of inclination of the cutting surface that regulates the depth is approximately perpendicular to the joint surface, the depth can be measured quickly and with high precision, and the performance and workability of the head are improved at the same time.

さらに本発明は、従来のヘッド製造工程の大幅な変更を
伴うことなく、現状の装置を用いて容易に実現でき、こ
の実用価値は極めて高いといえる。
Furthermore, the present invention can be easily realized using existing equipment without major changes to the conventional head manufacturing process, and its practical value can be said to be extremely high.

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

第1図(A)は本発明を適用した磁気ヘッドの一実施例
を示す断面図、第1図(B)は第1図(A)に示す磁気
ヘッドの磁気ギャップ近傍を拡大して示す模式図である
。 第2図(A)は本発明の他の実施例を示す断面図、第2
図(B)は第2図(A)に示す磁気ヘッドの磁気ギャッ
プ近傍を拡大して示す模式図である。 第3図(A)は本発明のさらに他の実施例を示す断面図
、第3図(B)は第3図(A)に示す磁気ヘッドの磁気
ギャップ近傍を拡大して示す模式図である。 第4図(A)は本発明のさらに他の実施例を示す断面図
、第4図(B)は第4図(A)に示す磁気ヘッドの磁気
ギャップ近傍を拡大して示す模式第5図(A)は従来の
磁気ヘッドを示す断面図、第5図(B)は第5図(A)
に示す磁気ヘッドの磁気ギャップ近傍を拡大して示す模
式図である。 1.2・・・・・磁気コア半体 3・・・・・・ギャップスペーサ 5・・・・・・巻線溝 5a ・・・・・第1の切削面
FIG. 1(A) is a cross-sectional view showing one embodiment of a magnetic head to which the present invention is applied, and FIG. 1(B) is an enlarged schematic diagram showing the vicinity of the magnetic gap of the magnetic head shown in FIG. 1(A). It is a diagram. FIG. 2(A) is a sectional view showing another embodiment of the present invention;
FIG. 2(B) is an enlarged schematic diagram showing the vicinity of the magnetic gap of the magnetic head shown in FIG. 2(A). FIG. 3(A) is a cross-sectional view showing still another embodiment of the present invention, and FIG. 3(B) is an enlarged schematic diagram showing the vicinity of the magnetic gap of the magnetic head shown in FIG. 3(A). . FIG. 4(A) is a sectional view showing still another embodiment of the present invention, and FIG. 4(B) is a schematic diagram showing an enlarged view of the vicinity of the magnetic gap of the magnetic head shown in FIG. 4(A). (A) is a cross-sectional view showing a conventional magnetic head, and Figure 5 (B) is Figure 5 (A).
FIG. 2 is an enlarged schematic diagram showing the vicinity of the magnetic gap of the magnetic head shown in FIG. 1.2... Magnetic core half 3... Gap spacer 5... Winding groove 5a... First cutting surface

Claims (1)

【特許請求の範囲】 一対の磁気コア半体を突き合わせて磁気ギャップを形成
するとともに、前記磁気コア半体の少なくとも一方の接
合面に設けられた巻線溝によって前記磁気ギャップのデ
プスを規制してなる磁気ヘッドにおいて、 前記巻線溝の磁気ギャップ側の切削面のうち、前記デプ
スを規制する磁気ギャップ近傍部分の傾斜角度を前記接
合面に対して80°〜90°とし、その磁気記録媒体走
行方向の長さを前記デプスの0.3〜1.5倍とすると
ともに、これよりも離れた位置での傾斜角度を前記接合
面に対して20°〜70°とし、前記磁気ギャップ側の
切削面を屈曲させたことを特徴とする磁気ヘッド。
[Scope of Claims] A magnetic gap is formed by abutting a pair of magnetic core halves, and the depth of the magnetic gap is regulated by a winding groove provided on the joint surface of at least one of the magnetic core halves. In the magnetic head, of the cut surface of the winding groove on the magnetic gap side, a portion near the magnetic gap that regulates the depth has an inclination angle of 80° to 90° with respect to the bonding surface, and the magnetic recording medium travels. The length in the direction is set to 0.3 to 1.5 times the depth, and the inclination angle at a position further away from this is set to 20° to 70° with respect to the joint surface, and cutting on the magnetic gap side is performed. A magnetic head characterized by a curved surface.
JP4642287A 1987-02-28 1987-02-28 Magnetic head Pending JPS63213106A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4642287A JPS63213106A (en) 1987-02-28 1987-02-28 Magnetic head

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4642287A JPS63213106A (en) 1987-02-28 1987-02-28 Magnetic head

Publications (1)

Publication Number Publication Date
JPS63213106A true JPS63213106A (en) 1988-09-06

Family

ID=12746713

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4642287A Pending JPS63213106A (en) 1987-02-28 1987-02-28 Magnetic head

Country Status (1)

Country Link
JP (1) JPS63213106A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5535078A (en) * 1993-02-12 1996-07-09 Data Card Corporation Magnetic multi-track read/write head with recessed core gap structure and shield arrangement
US5572390A (en) * 1992-11-11 1996-11-05 Japan Energy Corporation Magnetic head including an apex portion with two chamfered portions having optimized angles
US5583728A (en) * 1994-02-04 1996-12-10 Japan Energy Corporation Improved magnetic head having smoothed chamfered surface for reducing magnetic scattering

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5572390A (en) * 1992-11-11 1996-11-05 Japan Energy Corporation Magnetic head including an apex portion with two chamfered portions having optimized angles
US5535078A (en) * 1993-02-12 1996-07-09 Data Card Corporation Magnetic multi-track read/write head with recessed core gap structure and shield arrangement
US5583728A (en) * 1994-02-04 1996-12-10 Japan Energy Corporation Improved magnetic head having smoothed chamfered surface for reducing magnetic scattering

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