JPH0258710A - Magnetic head - Google Patents
Magnetic headInfo
- Publication number
- JPH0258710A JPH0258710A JP20938388A JP20938388A JPH0258710A JP H0258710 A JPH0258710 A JP H0258710A JP 20938388 A JP20938388 A JP 20938388A JP 20938388 A JP20938388 A JP 20938388A JP H0258710 A JPH0258710 A JP H0258710A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- core
- cores
- central
- sides
- 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
- 238000004804 winding Methods 0.000 claims abstract description 37
- 239000004020 conductor Substances 0.000 claims abstract description 12
- 238000005304 joining Methods 0.000 claims description 4
- 230000005236 sound signal Effects 0.000 abstract description 8
- 229910045601 alloy Inorganic materials 0.000 description 9
- 239000000956 alloy Substances 0.000 description 9
- 238000000034 method Methods 0.000 description 8
- 239000000853 adhesive Substances 0.000 description 7
- 239000010408 film Substances 0.000 description 7
- 239000000463 material Substances 0.000 description 7
- 230000001070 adhesive effect Effects 0.000 description 6
- 239000010409 thin film Substances 0.000 description 6
- 239000011521 glass Substances 0.000 description 5
- 238000004519 manufacturing process Methods 0.000 description 5
- 230000008569 process Effects 0.000 description 5
- 239000000696 magnetic material Substances 0.000 description 4
- 229910000702 sendust Inorganic materials 0.000 description 4
- 239000000758 substrate Substances 0.000 description 4
- 238000002844 melting Methods 0.000 description 3
- 229910000859 α-Fe Inorganic materials 0.000 description 3
- 238000005520 cutting process Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000008018 melting Effects 0.000 description 2
- 230000001681 protective effect Effects 0.000 description 2
- 230000035882 stress Effects 0.000 description 2
- 230000008901 benefit Effects 0.000 description 1
- 229910052790 beryllium Inorganic materials 0.000 description 1
- ATBAMAFKBVZNFJ-UHFFFAOYSA-N beryllium atom Chemical compound [Be] ATBAMAFKBVZNFJ-UHFFFAOYSA-N 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 238000000206 photolithography Methods 0.000 description 1
- 230000008646 thermal stress Effects 0.000 description 1
- 238000000427 thin-film deposition Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/17—Construction or disposition of windings
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/127—Structure or manufacture of heads, e.g. inductive
- G11B5/29—Structure or manufacture of unitary devices formed of plural heads for more than one track
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B5/00—Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
- G11B5/48—Disposition or mounting of heads or head supports relative to record carriers ; arrangements of heads, e.g. for scanning the record carrier to increase the relative speed
- G11B5/488—Disposition of heads
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Magnetic Heads (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は磁気ヘッド、特にコア半体どうしを突合せ接合
して得た磁気コアの巻線窓にコイル巻線を施してなる磁
気ヘッドに関するものである。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a magnetic head, and particularly to a magnetic head in which a coil winding is applied to a winding window of a magnetic core obtained by butt-joining core halves. It is.
[従来の技術]
従来より、静止画データを記録するスチルビデオ用磁気
ヘッドとして薄膜磁気ヘッド、あるいはバルクヘッドが
用いられている。薄膜磁気ヘッドは、薄膜堆積工程、お
よびフォトリソエッヂング工程などを用いて磁性体のみ
ならずコイル部分まで薄膜によって構成した磁気ヘッド
で、例えは第6図に示すような構成を有する。[Prior Art] Conventionally, a thin film magnetic head or a bulk head has been used as a still video magnetic head for recording still image data. A thin film magnetic head is a magnetic head in which not only the magnetic material but also the coil portion is made of a thin film using a thin film deposition process, a photolithography etching process, etc., and has a configuration as shown in FIG. 6, for example.
第6図において符号61はガラスなどから成る基板で、
この基板上には薄膜形成工程によって下部磁性体および
上部磁性体から成る磁気コア、ギャップ部分および導電
膜からなるコイル部分などを構成し、その上を絶縁層6
3で覆い、さらに保護板64を接合したものである。磁
気ギャップ部62は基板61および保護板64の間から
露出する。In FIG. 6, reference numeral 61 is a substrate made of glass or the like.
A magnetic core made of a lower magnetic material and an upper magnetic material, a gap part and a coil part made of a conductive film are formed on this substrate by a thin film forming process, and an insulating layer 6 is formed on the substrate.
3, and a protective plate 64 is further bonded to the protective plate 64. The magnetic gap portion 62 is exposed between the substrate 61 and the protection plate 64.
方、バルクヘッドは第7図に示すような構造を有する。On the other hand, the bulkhead has a structure as shown in FIG.
第7図において符号91.91は単結晶フェライトなど
から構成されたコア半体で、互いの接合部分にそれぞれ
高飽和磁束密度を有するセンダスト合金から成る合金磁
性材92が設けられている。In FIG. 7, reference numerals 91 and 91 indicate core halves made of single-crystal ferrite or the like, and an alloy magnetic material 92 made of Sendust alloy having a high saturation magnetic flux density is provided at the joint portions of the core halves.
コア半体91.91の一方には後にコイルを巻くための
巻線窓91aが設けられている。コア半体91.91は
ブロックのままギャップ材料を介してガラスなどから成
る接着材93によって接合され、その後スライスするこ
とによって第7図のような磁気コアが形成される。磁気
ギャップ94のトラック幅方向の長さは接着材93を埋
設する研削部の形状によって決定される。One of the core halves 91.91 is provided with a winding window 91a for later winding a coil. The core halves 91.91 are joined as blocks with an adhesive 93 made of glass or the like through a gap material, and then sliced to form a magnetic core as shown in FIG. The length of the magnetic gap 94 in the track width direction is determined by the shape of the grinding portion in which the adhesive 93 is embedded.
[発明が解決しようとする課題]
スチルビデオ技術では、映像信号が記録されるトラック
間のガートバンド部を利用して音声信号を記録再生する
ことが考えられる。この場合、第6図、第7図に示した
ような従来型のヘッドでは当然映像信号の記録再生のみ
しか行なえず、映像信号の記録再生と同時に音声信号を
記録再生するためには音声信号のためのヘッドが必要と
なるが、音声信号用のヘッドと映像信号用のヘッドを別
体とし、これらを磁気ディスクの記録領域に配置するに
はスペース的に無理があり、同一のへラドチップ内に音
声の記録再生用トラックを設ける必要があった。[Problems to be Solved by the Invention] In still video technology, it is conceivable to record and reproduce audio signals using guard band sections between tracks on which video signals are recorded. In this case, the conventional head shown in Figures 6 and 7 can only record and reproduce video signals, and in order to record and reproduce audio signals at the same time as video signals, it is necessary to record and reproduce audio signals simultaneously. However, since it would be unreasonable in terms of space to separate the head for audio signals and the head for video signals and place them in the recording area of the magnetic disk, it was necessary to have a head for audio signals and a head for video signals in the same Herad chip. It was necessary to provide a track for audio recording and playback.
ところが、第6図のような薄膜ヘッドではコイルを構成
する導体膜がトラック幅方向に大ぎなスペースを占有す
るため、2トラツクの薄膜ヘッドのトラック間スペース
に音声用ヘッドを形成するのは非常に困難であり、また
これを実現するには大幅なコスト増が予想される。また
、バルクヘッドの場合、必然的にコイル巻線が必要であ
り、このスペースのため同様に同一チップ内に音声用コ
アを設けるのは困難で、またクロストーク発生の問題が
あった。However, in a thin-film head like the one shown in Figure 6, the conductor film that makes up the coil occupies a large space in the track width direction, so it is very difficult to form an audio head in the space between the tracks of a two-track thin-film head. This would be difficult and would require a significant increase in costs. Further, in the case of a bulkhead, coil winding is inevitably required, and because of this space, it is difficult to similarly provide an audio core within the same chip, and there is also the problem of crosstalk.
本発明の課題は以上の問題を解決し、クロストークなど
の問題を生じることなく、占有スペースが小さい同一の
へラドチップ内に磁気ギャップを設は複数の信号の記録
再生を行なえるようにすることである。The object of the present invention is to solve the above-mentioned problems and to make it possible to record and reproduce multiple signals by providing a magnetic gap within the same Herad chip, which occupies a small space, without causing problems such as crosstalk. It is.
[課題を解決するための手段]
以上の課題を解決するために、本発明においては、コア
半体どうしを突合せ接合して得た磁気コアの巻線窓にコ
イル巻線を施してなる磁気ヘッドにおいて、3つの磁気
コアを非磁性導電体を介して積層し、中央の磁気コアを
挟持する両側の磁気コアの一方のコア半体のそれぞれほ
ぼ同じ位置に巻線窓を設け、中央の磁気コアを両側の磁
気コアの巻線窓に設けられるコイルの磁路と無関係にな
るように切り欠き、一方、中央の磁気コアの巻線窓を両
側の磁気コアの巻線窓が設けられているのと反対側のコ
ア半体に設け、両側の磁気コアを中央の磁気コアの巻線
窓に設けられるコイルの磁路と無関係になるように切り
欠いた構成を採用した。[Means for Solving the Problems] In order to solve the above problems, the present invention provides a magnetic head in which a coil winding is applied to a winding window of a magnetic core obtained by butt-joining core halves. In this method, three magnetic cores are laminated with a non-magnetic conductor in between, and winding windows are provided at approximately the same position on each core half of one of the magnetic cores on both sides sandwiching the central magnetic core. The winding windows of the central magnetic core are cut out so that they are independent of the magnetic path of the coil provided in the winding windows of the magnetic cores on both sides, and the winding windows of the central magnetic core are cut out so that the winding windows of the magnetic cores on both sides are It is provided on the core half on the opposite side, and the magnetic cores on both sides are cut out so that they are independent of the magnetic path of the coil provided in the winding window of the central magnetic core.
[作 用]
以上の構成によれば、3つの磁気コアの磁路を非磁性導
体および各磁気コアの切り欠きで磁気的および電気的に
遮断した状態で、中央の磁気コアと両側の磁気コアとで
それぞれ別の信号の記録再生をクロストークなく行なう
ことができる。[Function] According to the above configuration, the magnetic paths of the three magnetic cores are magnetically and electrically interrupted by the non-magnetic conductor and the notch of each magnetic core, and the central magnetic core and the magnetic cores on both sides are connected to each other. It is possible to record and reproduce separate signals without crosstalk.
[実施例]
以下、図面に示す実施例に基づき、本発明の詳細な説明
する。[Example] Hereinafter, the present invention will be described in detail based on the example shown in the drawings.
第1図および第2図はそれぞれ本発明を採用した磁気ヘ
ッドの斜視図および媒体摺動面側の正面図を示している
。FIGS. 1 and 2 show a perspective view and a front view of a magnetic head on the medium sliding surface side, respectively, employing the present invention.
図において符号11a〜13aおよびflb〜13bは
バルクヘッドを構成するコア半体である。本実施例では
、これらの左右のコア半体11a〜13aおよび11b
〜13bから成る3つの磁気コアを非磁性導電体9を介
して接合し、3つのギャップを形成する。それぞれのコ
ア11〜13のキャップ4.6.8のうち、磁気キャッ
プ4.8は静止画の1フレームを構成するそれぞれ1フ
イールドの映像信号の記録再生に、また中央の磁気ギャ
ップ6は音声信号の記録再生に用いられる。In the figure, reference numerals 11a to 13a and flb to 13b are core halves that constitute the bulkhead. In this embodiment, these left and right core halves 11a to 13a and 11b
Three magnetic cores consisting of ~13b are joined via a non-magnetic conductor 9 to form three gaps. Among the caps 4.6.8 of each core 11 to 13, the magnetic cap 4.8 is used for recording and reproducing video signals of one field each constituting one frame of a still image, and the magnetic gap 6 in the center is used for recording and reproducing audio signals. Used for recording and playback.
次にM3図(A)〜(C)に3つの磁気コア11〜13
の構造を示す。コア半体11a112a、13aはセン
ダストなどの合金膜3.5.7およびギャップ材4a、
6a、8aを介して他方のコア半体11b、12b、1
3bと接着オオ
剤2を介して接合されている。この基本構造そのものは
第7図に示した従来のバルクヘッドの場合と同様である
。コア半体11b、12aおよび13bには、後にコイ
ル巻線を施すための巻線窓11d、12d、13dが形
成されている。Next, M3 diagrams (A) to (C) show the three magnetic cores 11 to 13.
The structure of The core halves 11a, 112a and 13a are made of an alloy film 3.5.7 such as sendust and a gap material 4a,
6a, 8a to the other core half 11b, 12b, 1
3b via adhesive agent 2. This basic structure itself is the same as that of the conventional bulkhead shown in FIG. Winding windows 11d, 12d, and 13d are formed in the core halves 11b, 12a, and 13b for later coil winding.
ところか、コア半体11a、12b、13aには図示の
ように摺動面側より後方を大きく削り取った切欠部11
c、12cおよび13cが設けられている。これらの切
り欠き110〜13cは第1図のように各磁気コア11
〜13を接合した際、コイルによって中央の磁気コア1
2と両側の磁気コア11および13の間で各コアが磁気
的に結合しないようにするためのものである。However, as shown in the figure, the core halves 11a, 12b, and 13a have notches 11 that are largely cut away from the sliding surface side.
c, 12c and 13c are provided. These cutouts 110 to 13c are arranged in each magnetic core 11 as shown in FIG.
When connecting ~13, the central magnetic core 1 is connected by the coil.
This is to prevent magnetic coupling between the cores 2 and the magnetic cores 11 and 13 on both sides.
各切欠lie〜13cの形状は、図示のように媒体摺動
面を円筒状に研削されたコア半体の外周にほぼ相似した
形状となっている。切欠のギャップ面に平行な辺と摺動
面に平行な面が成す角度θはへラドコアの摺動力向の幅
を15摺動面の半径をRとするとθ<jan’(R+7
〒]/L)とするのが望ましく、θは本実施例では80
°とする。これによりギヤツブデプス10μ以上の時は
摺動面積が減少せず、またθをこの程度まで大きくする
ことにより巻線のスペースを確保できる。また、ギャッ
プ面と平行な辺とギャップ面の距11ttlは150μ
m程度とする。The shape of each notch 13c is approximately similar to the outer periphery of a core half whose medium sliding surface is ground into a cylindrical shape as shown in the figure. The angle θ formed by the side parallel to the gap plane of the notch and the plane parallel to the sliding surface is θ<jan'(R+7
〒]/L), and θ is 80 in this example.
°. As a result, when the gear tooth depth is 10 μ or more, the sliding area does not decrease, and by increasing θ to this extent, space for the winding can be secured. Also, the distance 11ttl between the side parallel to the gap plane and the gap plane is 150μ
It should be about m.
このように構成した各磁気コア11〜13を第1図に示
すように磁気ギャップ4.6.8が一直線上に整列する
ように接合し、巻線窓12dおよびIldと13dにそ
れぞれ別々に巻線を施すことによって中央の磁気コア1
2によって音声信号の記録再生を、またその両側の磁気
コア11.13により1フイールドづつの映像信号の記
録再生を同時に行なうことができる。各コアの磁路は切
欠lie〜13cおよび非磁性導電体9により磁気的、
電気的に遮蔽されているので、クロストークの問題もな
い。The magnetic cores 11 to 13 configured in this way are joined so that the magnetic gaps 4.6.8 are aligned in a straight line as shown in FIG. Central magnetic core 1 by applying wire
2 can simultaneously record and reproduce audio signals, and the magnetic cores 11 and 13 on both sides can simultaneously record and reproduce video signals one field at a time. The magnetic path of each core is formed by the notches 13c and the non-magnetic conductor 9.
Since it is electrically shielded, there is no problem with crosstalk.
次に、上記のような磁気ヘッドの製造工程を示す。まず
磁気コア11.12および13をそれぞれ別に構成する
が、これらのコアの製造工程はほぼ同じなので、ここで
は磁気コア11の製造工程を例示する。Next, the manufacturing process of the above magnetic head will be described. First, the magnetic cores 11, 12 and 13 are constructed separately, but since the manufacturing process for these cores is almost the same, the manufacturing process for the magnetic core 11 will be illustrated here.
まず、コア半体11a、11bと成るコア半体ブロック
を用意し、コア半体11bとなるブロックに巻線窓li
dを形成する。次に各ブロックの接合面に20μm程度
のセンダスト合金から成る合金膜3.3をスパッタリン
グし、続いて摺動面部分にコアの厚みに応じた間隔て後
に接着材2のための溝加工を行なう。この溝加工によっ
て、トラック幅を60μm程度に設定する。続いて、コ
ア半体ブロックの接合面にギャップ材としてS i O
2を0.25μm程度成膜する。First, core half blocks that will become the core half bodies 11a and 11b are prepared, and a winding window li is placed in the block that will become the core half body 11b.
form d. Next, an alloy film 3.3 made of Sendust alloy with a thickness of about 20 μm is sputtered on the joint surface of each block, and then grooves for the adhesive 2 are formed on the sliding surface at intervals according to the thickness of the core. . By this groove processing, the track width is set to about 60 μm. Next, SiO was applied as a gap material to the joint surfaces of the core half blocks.
2 to a thickness of about 0.25 μm.
次に、これらのコア半体を600を程度の作業温度を有
する低融点ガラスから成る接着材2によって突き合わせ
て接合し、その後切り欠き11cの部分を研削した後所
定の厚みにスライスして磁気コア11を得る。切り欠き
11cの接合面からの厚みtl(コア半体12dの場合
t2)は150μm程度とする。厚みtl、t2を15
0μm程度とするのは、これらが、約100μm以下に
おいてはコアの磁気特性が劣化するため、また巻線のス
ペース確保のためである。たとえば、0.35mm幅の
巻線窓を設けると、0.15n+mのコア厚(tl)を
引いても幅0.2mmの巻線スペースが確保される。な
お、切欠lieの2辺の成す角は前記の式によって決定
する。また、コアのスライスの際にはコアとギャップが
成す角度を直角または所定のアジマス角を有するように
切断方向を設定するのは言うまでもない。Next, these core halves are butted and joined together using an adhesive 2 made of low-melting glass having a working temperature of about 600 ℃, and after that, the notch 11c is ground and sliced to a predetermined thickness to form the magnetic core. Get 11. The thickness tl of the notch 11c from the joint surface (t2 in the case of the core half 12d) is approximately 150 μm. Thickness tl, t2 is 15
The reason why the thickness is about 0 μm is because the magnetic properties of the core deteriorate when the thickness is less than about 100 μm, and also to ensure space for the winding. For example, if a winding window with a width of 0.35 mm is provided, a winding space with a width of 0.2 mm is secured even after subtracting the core thickness (tl) of 0.15 n+m. Note that the angle formed by the two sides of the notch lie is determined by the above formula. Further, when slicing the core, it goes without saying that the cutting direction is set so that the angle formed by the core and the gap is perpendicular or has a predetermined azimuth angle.
以上と同様の手順によって磁気コア12.13も製造す
るが、中央の磁気コア12の両面には第1図あるいは第
3図(B)に示すようにベリリウムカッパなどから成る
非磁性導電体を10μm程度形成する。The magnetic cores 12 and 13 are also manufactured by the same procedure as above, but a non-magnetic conductor made of beryllium kappa or the like is coated with a thickness of 10 μm on both sides of the central magnetic core 12, as shown in FIG. 1 or FIG. 3(B). form a degree.
その後、各磁気コア11〜13を先の接着材2の低融点
ガラスよりもさらに作業温度の低い低融点ガラスを用い
て接合する。その際、磁気ギャップ4.6.8がほぼ一
直線上に整列するように位置合わせを行なう。Thereafter, each of the magnetic cores 11 to 13 is bonded using a low melting point glass whose working temperature is lower than that of the low melting point glass of the adhesive material 2. At this time, alignment is performed so that the magnetic gaps 4.6.8 are aligned substantially on a straight line.
続いて、巻線窓12dとIld、13dに同巻によるコ
イル巻線を施した後媒体摺動面を所望の曲率に加工して
、第1図に示すようなヘッドコアが完成される。Subsequently, coils are wound in the same manner around the winding windows 12d, Ild, and 13d, and the medium sliding surface is processed to have a desired curvature, thereby completing a head core as shown in FIG. 1.
以上ではメタルインギャップ型のヘッドを例示したが、
第4図および第5図に示すようにギャップ部分に高透磁
率の合金磁性膜を設けないフェライトによるバルクヘッ
ドでも、同様の構成を実施できる。この場合には合金膜
の製造工程が除去され、各コア半体が直接ギャップ材料
を介して接合されている点が上記実施例と異なる。The above example uses a metal-in-gap type head, but
As shown in FIGS. 4 and 5, a similar configuration can be implemented with a bulk head made of ferrite without a high permeability alloy magnetic film provided in the gap portion. This case differs from the above embodiment in that the manufacturing process of the alloy film is eliminated and the core halves are directly joined via the gap material.
このような構造によれば、センダスト合金などによる合
金膜の形成工程がないため製造工程が簡略化されると同
時に、各コアの接着工程における熱応力や、切断加工時
の加工応力によるフェライト材のひび割れなどを生じる
ことなく、歩留りよく磁気ヘッドの製造が行なえるとい
う利点がある。This structure simplifies the manufacturing process because there is no process to form an alloy film using sendust alloy, etc., and at the same time reduces the stress on the ferrite material due to thermal stress in the adhesion process of each core and processing stress during cutting. This method has the advantage that magnetic heads can be manufactured at a high yield without causing cracks or the like.
[発明の効果]
以上から明らかなように、本発明によれば、コア半体ど
うしを突合せ接合して得た磁気コアの巻線窓にコイル巻
線を施してなる磁気ヘッドにおいて、3つの磁気コアを
非磁性導電体を介して積層し、中央の磁気コアを挟持す
る両側の磁気コアの一方のコア半体のそれぞれほぼ同じ
位置に巻線窓を設け、中央の磁気コアを両側の磁気コア
の巻線窓に設けられるコイルの磁路と無関係になるよう
に切り欠き、一方、中央の磁気コアの巻線窓を両側の磁
気コアの巻線窓が設けられているのと反対側のコア半体
に設け、両側の磁気コアを中央の磁気コアの巻線窓に設
けられるコイルの磁路と無関係になるように切り欠いた
構成を採用しているので、3つの磁気コアの磁路を非磁
性導電体および各磁気コアの切り欠きで磁気的、電気的
に遮断した状態で、中央の磁気コアと両側の磁気コアと
でそれぞれ別の信号の記録再生をクロストークなく行な
える、また、同じへラドチップ内に複数の磁気ギャップ
を配置でき、スチルビデオにおける音声および映像信号
の記録再生など磁気ヘッドのスペースが制限されている
用途に好適な磁気ヘッドを提供できるなどの優れた効果
がある。[Effects of the Invention] As is clear from the above, according to the present invention, in a magnetic head in which a coil winding is applied to a winding window of a magnetic core obtained by butt-joining core halves, three magnetic The cores are laminated with a non-magnetic conductor in between, and a winding window is provided at approximately the same position on each of the core halves of one of the magnetic cores on both sides that sandwich the central magnetic core, and the central magnetic core is connected to the magnetic cores on both sides. The winding windows of the central magnetic core are cut out so that they are unrelated to the magnetic path of the coil, and the winding windows of the central magnetic core are cut out so that the winding windows of the magnetic cores on both sides are provided with the winding windows of the opposite side. It is installed in half, and the magnetic cores on both sides are cut out so that they are independent of the magnetic path of the coil provided in the winding window of the central magnetic core, so the magnetic path of the three magnetic cores is With the non-magnetic conductor and the notch in each magnetic core magnetically and electrically isolated, separate signals can be recorded and reproduced between the central magnetic core and the magnetic cores on both sides without crosstalk. A plurality of magnetic gaps can be arranged in the same Herad chip, and there are excellent effects such as providing a magnetic head suitable for applications where the space for a magnetic head is limited, such as recording and reproducing audio and video signals in still video.
第1図は本発明を採用した磁気ヘッドの斜視図、第2図
は第1図のヘッドの媒体摺動面の正面図、第3図(A)
〜(C)は第1図、82図の各磁気コアの側面図、第4
図、第5図は異なる実施例を示し、第4図は磁気ヘッド
の斜視図、第5図は媒体摺動面の正面図、第6図、第7
図はそれぞれ異なる従来の磁気ヘッドの構造を示した斜
視図である。
2・・・接着材
4.6.8・・・磁気ギャップ
9・・・非磁性導電体
11.12.13・・・磁気コア
11a、llb、12a、12b、13a、13b ・
=コア半体lie、12c、13c・・・切り欠きli
d、12d、13d・・・巻線窓Figure 1 is a perspective view of a magnetic head adopting the present invention, Figure 2 is a front view of the medium sliding surface of the head in Figure 1, and Figure 3 (A).
~(C) is a side view of each magnetic core in Figures 1 and 82, and Figure 4.
5 and 5 show different embodiments, FIG. 4 is a perspective view of the magnetic head, FIG. 5 is a front view of the medium sliding surface, and FIGS. 6 and 7.
The figures are perspective views showing the structures of different conventional magnetic heads. 2...Adhesive material 4.6.8...Magnetic gap 9...Nonmagnetic conductor 11.12.13...Magnetic core 11a, llb, 12a, 12b, 13a, 13b・
= Core half lie, 12c, 13c...notch li
d, 12d, 13d...Window window
Claims (1)
線窓にコイル巻線を施してなる磁気ヘッドにおいて、3
つの磁気コアを非磁性導電体を介して積層し、中央の磁
気コアを挟持する両側の磁気コアの一方のコア半体のそ
れぞれほぼ同じ位置に巻線窓を設け、中央の磁気コアを
両側の磁気コアの巻線窓に設けられるコイルの磁路と無
関係になるように切り欠き、一方、中央の磁気コアの巻
線窓を両側の磁気コアの巻線窓が設けられているのと反
対側のコア半体に設け、両側の磁気コアを中央の磁気コ
アの巻線窓に設けられるコイルの磁路と無関係になるよ
うに切り欠いたことを特徴とする磁気ヘッド。 2)磁気記録媒体の所定トラックに対して前記中央の磁
気コアにより第1の信号の記録再生を行なうとともに、
この第1の信号のトラックの両側の2つのトラックに対
して前記両側の磁気コアにより第2の信号の記録再生を
行なうことを特徴とする特許請求の範囲第1項に記載の
磁気ヘッド。 3)前記3つの磁気コアのギャップがほぼ同一直線上に
整列して設けられることを特徴とする特許請求の範囲第
1項または第2項に記載の磁気ヘッド。[Claims] 1) A magnetic head in which a coil winding is applied to a winding window of a magnetic core obtained by butt-joining core halves, comprising: 3
Two magnetic cores are laminated with a non-magnetic conductor in between, and a winding window is provided at approximately the same position on each core half of one of the magnetic cores on both sides that sandwich the central magnetic core. The winding window of the magnetic core is cut out so that it has no relation to the magnetic path of the coil, and the winding window of the central magnetic core is cut out on the side opposite to the winding windows of the magnetic cores on both sides. 1. A magnetic head, characterized in that the magnetic cores on both sides are cut out so as to have no relation to the magnetic path of the coil provided in the winding window of the central magnetic core. 2) Recording and reproducing the first signal with respect to a predetermined track of the magnetic recording medium using the central magnetic core;
2. The magnetic head according to claim 1, wherein the magnetic cores on both sides record and reproduce the second signal on two tracks on both sides of the first signal track. 3) The magnetic head according to claim 1 or 2, wherein gaps between the three magnetic cores are arranged substantially on the same straight line.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20938388A JPH0258710A (en) | 1988-08-25 | 1988-08-25 | Magnetic head |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP20938388A JPH0258710A (en) | 1988-08-25 | 1988-08-25 | Magnetic head |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0258710A true JPH0258710A (en) | 1990-02-27 |
Family
ID=16572005
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP20938388A Pending JPH0258710A (en) | 1988-08-25 | 1988-08-25 | Magnetic head |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0258710A (en) |
-
1988
- 1988-08-25 JP JP20938388A patent/JPH0258710A/en active Pending
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