JPH01251306A - Magnetic flux generator - Google Patents

Magnetic flux generator

Info

Publication number
JPH01251306A
JPH01251306A JP63076809A JP7680988A JPH01251306A JP H01251306 A JPH01251306 A JP H01251306A JP 63076809 A JP63076809 A JP 63076809A JP 7680988 A JP7680988 A JP 7680988A JP H01251306 A JPH01251306 A JP H01251306A
Authority
JP
Japan
Prior art keywords
magnetic
magnetic flux
cover
hole
core
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
JP63076809A
Other languages
Japanese (ja)
Inventor
Masaaki Sato
雅昭 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.)
Panasonic System Solutions Japan Co Ltd
Original Assignee
Matsushita Graphic Communication Systems Inc
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 Matsushita Graphic Communication Systems Inc filed Critical Matsushita Graphic Communication Systems Inc
Priority to JP63076809A priority Critical patent/JPH01251306A/en
Publication of JPH01251306A publication Critical patent/JPH01251306A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/127Structure or manufacture of heads, e.g. inductive
    • G11B5/1278Structure or manufacture of heads, e.g. inductive specially adapted for magnetisations perpendicular to the surface of the record carrier
    • GPHYSICS
    • G11INFORMATION STORAGE
    • G11BINFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
    • G11B5/00Recording by magnetisation or demagnetisation of a record carrier; Reproducing by magnetic means; Record carriers therefor
    • G11B5/10Structure or manufacture of housings or shields for heads
    • G11B5/11Shielding of head against electric or magnetic fields

Landscapes

  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Magnetic Heads (AREA)

Abstract

PURPOSE:To concentrate magnetic flux in a small area by covering the magnetic pole part of a magnetic core with a cover made of superconducting material and generating the magnetic flux concentratedly through a small through hole formed through the cover. CONSTITUTION:A recording and reproducing coil 2 is wound on a core 1 and a cover made of the superconducting material is fitted in the magnetic pole part of its one end. The cover 3 has an almost rectangular parallelepiped shape and the magnetic pole part of the core 1 is fitted clossely in a rectangular hole part formed on the upper side of the cover 3. A through hole 4 is formed from the bottom part of the rectangular hole to the lower face of the cover 3. Consequently, slitting high-density magnetic flux whose sectional shape is thin can be operated on a medium 5, therefore, even when a main magnetic pole of a conventional opposed head is eliminated, high-performance recording can be performed. Thus, the forming the through hole sufficiently thin, much magnetic flux can be concentrated in the very small area.

Description

【発明の詳細な説明】 産業上の利用分野 この発明は、例えば磁気ヘッドや偏向ヨークなどに応用
される磁束発生装置に関し、特に、非常に小さな領域に
高密度の磁束を集中させる技術に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a magnetic flux generating device applied to, for example, a magnetic head or a deflection yoke, and particularly relates to a technique for concentrating high-density magnetic flux in a very small area.

従来の技術 例えば磁気記録再生装置において情報の記録密度を高め
るためには、非常に小さな領域に高密度の磁束を所定の
形態で発生する磁気ヘッドが必要になる。一般的な磁気
ディスク装置のリング型ヘッドでは、コアのギャップ部
分に高透磁率材料を配して、小さな磁極により多くの磁
束を集中させるようにしている(メタルインギャップ式
のヘッド)。また特開昭57−120221号公報に記
載されている垂直磁化記録再生用リング型ヘッドでは、
コアのギャップ部に超伝導材料を挾み込み、ギャップを
直接横断する磁束をなくし、ギャップの外側に膨出する
磁束を増大させるように工夫している。また垂直磁気記
録の分野では、主磁極と補助磁極とを対向させた対向型
ヘッドなど、いくつかの形式のヘッドが知られており、
それぞれに長所、短所を有している。
2. Description of the Related Art In order to increase the recording density of information in, for example, a magnetic recording/reproducing device, a magnetic head is required that generates high-density magnetic flux in a predetermined form in a very small area. In the ring-shaped head of a typical magnetic disk drive, a high magnetic permeability material is placed in the gap part of the core to concentrate more magnetic flux into a small magnetic pole (metal-in-gap head). Furthermore, in the ring type head for perpendicular magnetization recording/reproducing described in Japanese Patent Application Laid-Open No. 57-120221,
A superconducting material is inserted into the gap of the core to eliminate the magnetic flux that directly crosses the gap and to increase the magnetic flux that bulges outside the gap. In the field of perpendicular magnetic recording, several types of heads are known, such as a facing type head in which a main magnetic pole and an auxiliary magnetic pole face each other.
Each has advantages and disadvantages.

発明が解決しようとする課題 高密度で断面積の小さな磁束を発生するには、磁極片と
して透磁率および飽和磁束密度の大きな材料を用いると
ともに、磁束を拡散させないように磁極の形態を工夫し
なければならない。透磁率の大きな材料を用いても、磁
極の磁路断面積を小さくすると、その部分で磁気飽和が
起きて高密度の磁束を発生することができない。反対に
磁極の磁路断面積を大きくすれば、磁気飽和が起きにく
くなるが、そこから生じる磁束の断面積も大きくなり、
磁束を集中させることができない。
Problems to be Solved by the Invention In order to generate high-density magnetic flux with a small cross-sectional area, it is necessary to use a material with high magnetic permeability and saturation magnetic flux density for the magnetic pole pieces, and to devise the form of the magnetic poles so as not to diffuse the magnetic flux. Must be. Even if a material with high magnetic permeability is used, if the cross-sectional area of the magnetic path of the magnetic pole is made small, magnetic saturation will occur in that area, making it impossible to generate high-density magnetic flux. On the other hand, if you increase the cross-sectional area of the magnetic path of the magnetic pole, magnetic saturation becomes less likely to occur, but the cross-sectional area of the magnetic flux generated from it also increases.
Unable to concentrate magnetic flux.

この発明は上述した従来の問題点に鑑みなされたもので
、その目的は、飽和磁束密度の大きな磁極(磁路の断面
積が大きい)から発生する磁束を非常に小さな領域に集
中させることができるようにした磁束発生装置を提供す
ることにある。
This invention was made in view of the above-mentioned conventional problems, and its purpose is to make it possible to concentrate the magnetic flux generated from a magnetic pole with a large saturation magnetic flux density (the cross-sectional area of the magnetic path is large) into a very small area. An object of the present invention is to provide a magnetic flux generating device.

課題を解決するだめの手段 そこでこの発明では、磁気コアの磁極部分を超伝導材料
製のカバーで覆い、このカバーに形成した小さな貫通孔
を通って集中的に磁束が生じるように構成した。
Means to Solve the Problem In the present invention, the magnetic pole portion of the magnetic core is covered with a cover made of superconducting material, and magnetic flux is generated intensively through a small through hole formed in the cover.

作用 超伝導材料がもつマイスナー効果(超伝導体の内部には
磁束が入り込まないという性質)により、前記磁極から
空間に放出される磁束は前超伝導材料製のカバーによっ
て曲げられて、前記カバーの貫通孔の部分に集中する。
Due to the Meissner effect (the property that magnetic flux does not enter the inside of a superconductor) of the working superconducting material, the magnetic flux emitted from the magnetic pole into space is bent by the cover made of the superconducting material, and the magnetic flux is bent by the cover made of the superconducting material. Concentrate on the through hole.

実施例 第1図は本発明の一実施例による垂直磁化記録再生用ヘ
ッドの構成を示している。角柱状の磁気コア1に記録再
生用のコイル2が巻かれており、その一端の磁極部分に
超伝導材料製カバー3が装着されている。カバー3はほ
ぼ直方体状の外形をしており、その上面側に形成された
角孔部分にコア1の磁極部分がびったシと嵌合している
。この角孔の底部分からカバー3の下面にわたって貫通
孔4が形成されている。この貫通孔4のカバー3の下面
の開口形状は同図CB)のように細いスリット状になっ
ている。なお、5は磁気記録媒体である。
Embodiment FIG. 1 shows the structure of a perpendicular magnetization recording/reproducing head according to an embodiment of the present invention. A recording/reproducing coil 2 is wound around a prismatic magnetic core 1, and a cover 3 made of superconducting material is attached to a magnetic pole portion at one end of the coil 2. The cover 3 has an approximately rectangular parallelepiped outer shape, and the magnetic pole portion of the core 1 is fitted into a square hole formed on the upper surface thereof. A through hole 4 is formed extending from the bottom of this square hole to the lower surface of the cover 3. The opening shape of the through hole 4 on the lower surface of the cover 3 is in the shape of a thin slit as shown in FIG. CB). Note that 5 is a magnetic recording medium.

コイル2に電流を流してコアlを励磁すると、その上下
端が磁極となり、周囲の空間に両磁極を結んで拡がる磁
束が生じる。図中の点線は磁束を示している。カバー3
を装着しであるコア1の下端の磁極部分では、空間に生
じる磁束がカバー3に入シ込めないので(超伝導材料の
マイスナー効果)、磁束は図のようにカバー3の乱形状
に沿って曲がり、貫通孔4を通りて外部に出る。
When a current is passed through the coil 2 to excite the core l, its upper and lower ends become magnetic poles, and a magnetic flux is generated that connects the two magnetic poles and spreads in the surrounding space. The dotted line in the figure indicates magnetic flux. cover 3
At the magnetic pole part at the lower end of the core 1, where the magnetic flux is attached, the magnetic flux generated in the space cannot enter the cover 3 (Meissner effect of superconducting material), so the magnetic flux follows the irregular shape of the cover 3 as shown in the figure. It bends and exits through the through hole 4.

ここでコア1の磁極断面積をSIとし、磁極近傍での平
均の磁束密度をBl、貫通孔4の下面開口部の断面積を
S’、この開口部近傍の磁束密度をB2とすると、磁束
の保存法則により、 S + X B 1 ”” S 2X B 2が成り立
つ。したがって、貫通孔4の下面開口部近傍の磁束密度
B、は、 であり、貫通孔4の開口面積S2を小さくするほど磁束
密度B2が大きくなる。つまり、磁極で発生した磁束が
すべて小さな貫通孔4に集まυ、大きな磁束密度となる
Here, if the magnetic pole cross-sectional area of the core 1 is SI, the average magnetic flux density near the magnetic pole is Bl, the cross-sectional area of the lower opening of the through hole 4 is S', and the magnetic flux density near this opening is B2, then the magnetic flux According to the conservation law, S + X B 1 "" S 2X B 2 holds true. Therefore, the magnetic flux density B near the bottom opening of the through hole 4 is as follows, and the smaller the opening area S2 of the through hole 4 is, the larger the magnetic flux density B2 becomes. In other words, all the magnetic flux generated by the magnetic poles gathers in the small through hole 4, υ, resulting in a large magnetic flux density.

この実施例のヘッドによれば、断面形状が細いスリット
状の高密度の磁束を媒体5に作用させることができるの
で、従来の対向型ヘッドにおける主磁極をなくしても、
高性能な磁気記録を行なえる。
According to the head of this embodiment, a high-density magnetic flux in the form of a slit with a narrow cross-sectional shape can be applied to the medium 5, so even if the main magnetic pole in the conventional facing type head is eliminated,
Capable of high-performance magnetic recording.

第2図は本発明によって改良した垂直磁化記録再生用の
リング型ヘッドを示している。コア1はリング型という
よりコ字型に近い形をしており、その中央部分にコイル
2が巻かれている。コアlはほぼ全体的に超伝導材料製
のカバー3に包み込まれている。カバー3には、コア1
の両端の磁極面からカバー3の上面に達する2つの貫通
孔4aと4bが形成されている。カバー3の上面におけ
る貫通孔4aと4bの開口形状は第2図(ト)のように
2本の平行なスリットになっている。
FIG. 2 shows a ring-shaped head for perpendicular magnetization recording and reproducing improved according to the present invention. The core 1 is shaped more like a U-shape than a ring, and the coil 2 is wound around its center. The core l is almost entirely enclosed in a cover 3 made of superconducting material. Cover 3 has core 1
Two through holes 4a and 4b are formed that reach the top surface of the cover 3 from the magnetic pole faces at both ends. The opening shapes of the through holes 4a and 4b on the upper surface of the cover 3 are two parallel slits as shown in FIG. 2(G).

コア1の両磁極を結ぶように生じる磁束は、−方の貫通
孔4aを通ってカバー3の上面側へ出て、空間内でU字
状に曲って、他方の貫通孔4bを通って磁極に達する。
The magnetic flux generated to connect both magnetic poles of the core 1 passes through the - side through hole 4a, exits to the upper surface side of the cover 3, curves in a U-shape in the space, passes through the other through hole 4b, and connects to the magnetic pole. reach.

ここで記録媒体5に作用する磁束の断面形状を充分に細
くするには、カバー3の貫通孔4as4bの開口形状を
細いスリット状にすれば良く、コア1の磁極形状は磁気
飽和が起きないように充分に大きくすることができる。
Here, in order to make the cross-sectional shape of the magnetic flux acting on the recording medium 5 sufficiently thin, the opening shape of the through hole 4as4b of the cover 3 should be made into a thin slit shape, and the shape of the magnetic pole of the core 1 should be such that magnetic saturation does not occur. can be made large enough to

第3図は本発明の第3実施例による磁束発生装置の構成
を示している。コア1はC字型であシ、中央部分にコイ
ル2が巻かれている。コア1は全体的に超伝導材料製の
カバー3に包み込まれている。カバー3はコアlのギャ
ップ部分に入シ込んだ凹部6を有し、全体としてC字型
に近い外形になっている。カバー3における凹部6の相
対向した2つの面から内部のコアl磁極面に向けて小さ
な貫通孔4aと4bが形成されている。この2つの貫通
孔4a、4bは例えば丸孔で、同一直線状に並んで形成
されている。コア1の一方の磁極から生じた磁束は貫通
孔4aで細く絞られ、凹部6の空間を横断し、貫通孔4
bを通って他方の磁極に達する。貫通孔4a、4bの断
面積を小さくすることで、凹部6に極めて細くて強い磁
束を生成することができる。この実施例のようにして精
密で強力な偏向ヨークを構成することができる。
FIG. 3 shows the configuration of a magnetic flux generator according to a third embodiment of the present invention. The core 1 is C-shaped, and a coil 2 is wound around the center. The core 1 is entirely enclosed in a cover 3 made of superconducting material. The cover 3 has a recess 6 inserted into the gap portion of the core 1, and has an outer shape close to a C-shape as a whole. Small through holes 4a and 4b are formed from two opposing surfaces of the recess 6 in the cover 3 toward the magnetic pole surface of the internal core. These two through-holes 4a and 4b are, for example, round holes, and are formed aligned in the same straight line. The magnetic flux generated from one magnetic pole of the core 1 is narrowed by the through hole 4a, crosses the space of the recess 6, and flows through the through hole 4.
b and reaches the other magnetic pole. By reducing the cross-sectional area of the through holes 4a and 4b, an extremely thin and strong magnetic flux can be generated in the recess 6. In this embodiment, a precise and strong deflection yoke can be constructed.

発明の効果 以上詳細に説明したように、この発明に係る磁束発生装
置では、コアの磁極部分を磁束を通さない超伝導材料製
カバーで覆い、このカバーに形成した貫通孔を磁路とす
るように構成したので、貫通孔を充分に細く形成するこ
とで、非常に小さな領域に多くの磁束を集中させること
ができる。この磁束集中のためにコア磁極を小さくする
必要はなく、シたがって従来のように磁気飽和によって
磁束密度を充分に高められないという問題は解消される
。この発明により実施例で示したような高性能な磁気ヘ
ッドを実現することができ、情報の記録密度を大幅に高
められる等、さまざまな有用な効果につながる。
Effects of the Invention As explained in detail above, in the magnetic flux generating device according to the present invention, the magnetic pole portion of the core is covered with a cover made of a superconducting material that does not allow magnetic flux to pass through, and the through hole formed in this cover is used as a magnetic path. Therefore, by forming the through hole sufficiently thin, a large amount of magnetic flux can be concentrated in a very small area. There is no need to reduce the size of the core magnetic pole for this magnetic flux concentration, and therefore the problem of not being able to sufficiently increase the magnetic flux density due to magnetic saturation as in the prior art is solved. The present invention makes it possible to realize a high-performance magnetic head as shown in the embodiments, leading to various useful effects such as greatly increasing the recording density of information.

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

第1図は本発明の第1実施例による磁気ヘッドの概略構
成図、第2図は本発明の第2実施例による磁気ヘッドの
概略構成図、第3図は本発明の第3実施例による磁束発
生装置の概略構成図である。 1・・・磁気コア、2・・・コイル、3・・・超伝導材
料製カバー、4.4a、4b・・・貫通孔、5・・・磁
気記録媒体、6・・・凹部。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 第2図 (Aン 第 3 図
FIG. 1 is a schematic diagram of a magnetic head according to a first embodiment of the present invention, FIG. 2 is a schematic diagram of a magnetic head according to a second embodiment of the present invention, and FIG. 3 is a diagram of a magnetic head according to a third embodiment of the present invention. FIG. 1 is a schematic configuration diagram of a magnetic flux generator. DESCRIPTION OF SYMBOLS 1... Magnetic core, 2... Coil, 3... Superconducting material cover, 4.4a, 4b... Through hole, 5... Magnetic recording medium, 6... Recessed part. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 (Figure 3)

Claims (1)

【特許請求の範囲】[Claims] 磁気コアの磁極部分を超伝導材料製のカバーで覆い、こ
のカバーに形成した小さな貫通孔を通って集中的に磁束
が生じるようにした磁束発生装置。
A magnetic flux generator in which the magnetic pole part of the magnetic core is covered with a cover made of superconducting material, and magnetic flux is generated in a concentrated manner through small through holes formed in the cover.
JP63076809A 1988-03-30 1988-03-30 Magnetic flux generator Pending JPH01251306A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63076809A JPH01251306A (en) 1988-03-30 1988-03-30 Magnetic flux generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63076809A JPH01251306A (en) 1988-03-30 1988-03-30 Magnetic flux generator

Publications (1)

Publication Number Publication Date
JPH01251306A true JPH01251306A (en) 1989-10-06

Family

ID=13615993

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63076809A Pending JPH01251306A (en) 1988-03-30 1988-03-30 Magnetic flux generator

Country Status (1)

Country Link
JP (1) JPH01251306A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1996017257A1 (en) * 1994-11-17 1996-06-06 Gregory Aharonian Apparatus and method for concentrating natural magnetic fields using superconducting materials and application thereof

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1996017257A1 (en) * 1994-11-17 1996-06-06 Gregory Aharonian Apparatus and method for concentrating natural magnetic fields using superconducting materials and application thereof

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