JPS62298085A - Magnetic bubble memory driving coil - Google Patents

Magnetic bubble memory driving coil

Info

Publication number
JPS62298085A
JPS62298085A JP61139240A JP13924086A JPS62298085A JP S62298085 A JPS62298085 A JP S62298085A JP 61139240 A JP61139240 A JP 61139240A JP 13924086 A JP13924086 A JP 13924086A JP S62298085 A JPS62298085 A JP S62298085A
Authority
JP
Japan
Prior art keywords
coil
magnetic field
bubble memory
winding
magnetic bubble
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
JP61139240A
Other languages
Japanese (ja)
Inventor
Yoshiya Kaneko
金子 淑也
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP61139240A priority Critical patent/JPS62298085A/en
Publication of JPS62298085A publication Critical patent/JPS62298085A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain an equal magnetic field distribution with a wide area by changing the winding density of a plane coil to form a bending coil by a place. CONSTITUTION:For the A part and B part of bending coils 10 and 10', the winding density is changed. Namely, the coils are wound so that the winding density can be dense at the A part and coarse at the B part. Thus, the magnetic flux density of the A part is raised, the magnetic field distribution shown by a curved line A as a whole is obtained and the scope of the equal magnetic field is expanded compared with the conventional example shown by a curved line B. In this way, the equal magnetic field distribution with a wide area can be obtained.

Description

【発明の詳細な説明】 3、発明の詳細な説明 〔概 要〕 絶t工導線を平面状に多重巻きした磁気バブルメモリ駆
動コイルであって、その巻線密度を場所により変えるこ
とにより、広い均一磁界エリヤを得ることを可能とする
[Detailed Description of the Invention] 3. Detailed Description of the Invention [Summary] This is a magnetic bubble memory drive coil that is made by multiple windings of continuous conductor wire in a flat shape, and by changing the winding density depending on the location, it can be used over a wide area. This makes it possible to obtain a uniform magnetic field area.

〔産業上の利用分野〕[Industrial application field]

本発明は磁気バブルメモリ装置の磁気バブル駆動コイル
に関するものである。
The present invention relates to a magnetic bubble drive coil for a magnetic bubble memory device.

磁気バブルの制御法として最も一般的な手法は、回転磁
界とパーマロイパターンによる制御法である。これはバ
ブル結晶上に列状に形成されたハーフディスク形等のパ
ーマロイパターンに対し、外部より回転磁界を印加し、
それによってパーマロイパターンに磁極を生ぜしめ、そ
の磁極の移動によってバブルを順次隣りのパターンに転
送するようにしている。
The most common method for controlling magnetic bubbles is a control method using a rotating magnetic field and a permalloy pattern. This involves applying a rotating magnetic field from the outside to permalloy patterns such as half-disk shapes formed in rows on bubble crystals.
This creates a magnetic pole in the permalloy pattern, and the movement of the magnetic pole causes the bubbles to be sequentially transferred to the adjacent pattern.

この回転磁界の発生は、直交して配置されたXコイルと
Yコイルとに正弦波又は三角波等の電流を位相をずらし
て流すことにより行なわれている。
This rotating magnetic field is generated by passing currents, such as sine waves or triangular waves, through an X coil and a Y coil arranged orthogonally to each other, with the phases shifted.

そしてX、Yコイルには第5図に示すようなソレノイド
コイル1,2が用いられているがチップ3からの端子出
し面積Aが小さく、特に高密度化され端子数の多い場合
には端子出しが困難となる。
Solenoid coils 1 and 2 as shown in Figure 5 are used for the X and Y coils, but the terminal area A from the chip 3 is small, especially when the density is increased and the number of terminals is large. becomes difficult.

このため平板状のコイルを平面のまま、あるいは折り曲
げた状態で使用する方式が提案されている。
For this reason, methods have been proposed in which a flat coil is used in a flat state or in a bent state.

(特公昭55−20307号公報) 〔従来の技術〕 第6図は平板状コイルを折り曲げた状態で使用する例で
あり、Xコイルは平板状コイルを180 ”折り曲げた
コイル4,4′を図の如く組合わせ、チップ3の外周に
巻いたソレノイドコイル(Yコイル)5と組合わせてい
る。
(Japanese Patent Publication No. 55-20307) [Prior Art] Fig. 6 shows an example in which a flat coil is used in a bent state. It is combined with a solenoid coil (Y coil) 5 wound around the outer periphery of the chip 3.

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

この従来方式の折り曲げコイルでは、第7図に示すよう
な磁界分布となり均一性の良い磁界をチップ全面に得よ
うとすると巻幅が広(なり形状やインダクタンスが大き
くなるという欠点がある。
This conventional bending coil has the disadvantage that the magnetic field distribution is as shown in FIG. 7, and when trying to obtain a highly uniform magnetic field over the entire surface of the chip, the winding width (curved shape) and inductance become large.

本発明はこのような点に鑑みて創作されたもので、簡易
な構成でチップに均一な磁界を与え、且つ小型化が可能
な折り曲げ形コイルを用いた磁気バブルメモリ駆動コイ
ルを提供することを目的としている。
The present invention was created in view of these points, and aims to provide a magnetic bubble memory drive coil using a folded coil that can apply a uniform magnetic field to a chip with a simple configuration and can be miniaturized. The purpose is

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

このため本発明においては、絶8i導線を平面状に多重
巻きして構成するコイルを折り曲げた状態で使用する磁
気バブルメモリ駆動コイルにおいて、上記コイルは場所
により巻線密度を変えたことを特徴としている。
Therefore, in the present invention, in a magnetic bubble memory drive coil that is used in a bent state, the coil is constructed by multiple windings of an 8i conducting wire in a plane shape, and the coil is characterized in that the winding density is changed depending on the location. There is.

〔作 用〕[For production]

折り曲げコイルを形成する平面状コイルの巻線密度を場
所により変えることにより、広い面積で均一な磁界分布
を得ることが可能となる。
By changing the winding density of the planar coil forming the bent coil depending on the location, it is possible to obtain a uniform magnetic field distribution over a wide area.

〔実施例〕〔Example〕

第1図は本発明の詳細な説明するための図であり、aは
コイル断面、bは磁界分布を示す図である。
FIG. 1 is a diagram for explaining the present invention in detail, in which a is a diagram showing a coil cross section and b is a diagram showing a magnetic field distribution.

本実施例は折り曲げコイル10 、10 ’を、そのA
部とB部とでは巻線密度を変えている。即ちA部では巻
線密度を密に、B部では粗になるように巻回している。
In this embodiment, the bent coils 10 and 10' are
The winding density is different between the part and the B part. That is, the winding density is densely wound in the A part and coarsely in the B part.

本実施例において巻線密度を変える手段としては、絶縁
巻線11の外径をA部では細く、B部では太くし、第2
図aに示す巻枠12で第2図すに示すように平板状に巻
回する。なお絶縁導線の太さを変えるには、芯線の太さ
を変えても、あるいは芯線の太さは同一で絶縁被覆の厚
さを変えても良い。
In this embodiment, the means for changing the winding density is to make the outer diameter of the insulated winding 11 thinner in the A section, thicker in the B section, and
The material is wound into a flat plate shape as shown in FIG. 2 using the winding frame 12 shown in FIG. In order to change the thickness of the insulated conductive wire, the thickness of the core wire may be changed, or the thickness of the core wire may be the same but the thickness of the insulation coating may be changed.

このように構成された本実施例は、A部の磁束密度が上
り、全体として第1図すに曲線Aで示すような磁界分布
となり、曲線Bで示す従来例に比し均一磁界の範囲が拡
大される。
In this embodiment configured in this way, the magnetic flux density in the A section increases, and the overall magnetic field distribution becomes as shown by curve A in Figure 1, and the range of the uniform magnetic field is wider than that of the conventional example shown by curve B. Expanded.

第3図は本発明の他の実施例を説明するための図である
FIG. 3 is a diagram for explaining another embodiment of the present invention.

本実施例は前実施例と同様に場所により巻線密度を変え
たもので、巻線を千鳥形とし、コイルの外側に行くほど
、その重なりを多くして巻線密度を太き(している。そ
して、このコイルを形成するには第4図の如き巻枠13
を用いて行なうことができる。即ち巻枠13は巻線用の
溝が内周に行く程幅が広くなっており、巻線の重なりが
多くなるようになっている。
In this example, as in the previous example, the winding density is changed depending on the location.The windings are staggered, and the closer they go to the outside of the coil, the more they overlap, making the winding density thicker. To form this coil, a winding frame 13 as shown in Fig. 4 is used.
This can be done using That is, in the winding frame 13, the width of the winding groove increases toward the inner circumference, so that the windings overlap each other more.

このように形成された本実施例は第3図に示すように、
その外側に行(はど巻線密度が大となるため、その磁界
分布は前実施例と同様になり、従来に比して均一磁界範
囲が拡大される。
This embodiment formed in this way is as shown in FIG.
Since the winding density is increased on the outside, the magnetic field distribution is similar to that of the previous embodiment, and the uniform magnetic field range is expanded compared to the conventional example.

〔発明の効果〕〔Effect of the invention〕

以上述べてきたように本発明によれば、極めて簡易な構
成で均一磁界範囲を大きくすることができ、実用的には
極めて有用である。
As described above, according to the present invention, the uniform magnetic field range can be increased with an extremely simple configuration, and is extremely useful in practice.

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

第1図は本発明の詳細な説明するための図、第2図は本
発明の実施例のコイルを巻(ための巻枠及び平面コイル
を示す図、 第3図は本発明の他の実施例を説明するための図、 第4図は本発明の他の実施例のコイルを巻(ための巻枠
を示す図、 第5図は従来のソレノイドコイルを用いた磁気バブルメ
モリ駆動コイルを示す図、 第6図は従来の折り曲げコイルを用いた磁気バブルメモ
リ駆動コイルを示す図、 第7図は第6図の■−■線断面における磁界分布を示す
図である。 第1図において、 10 、10 ’は折り曲げコイル、 11は絶縁導線である。
FIG. 1 is a diagram for explaining the present invention in detail, FIG. 2 is a diagram showing a winding frame and a plane coil for winding a coil according to an embodiment of the present invention, and FIG. 3 is a diagram showing another embodiment of the present invention. Figure 4 is a diagram for explaining an example. Figure 4 is a diagram showing a winding frame for winding a coil according to another embodiment of the present invention. Figure 5 is a diagram showing a magnetic bubble memory drive coil using a conventional solenoid coil. Fig. 6 is a diagram showing a magnetic bubble memory drive coil using a conventional bent coil, and Fig. 7 is a diagram showing a magnetic field distribution in a cross section taken along the line ■-■ in Fig. 6. In Fig. 1, 10 , 10' is a bent coil, and 11 is an insulated conductor.

Claims (1)

【特許請求の範囲】 1、絶縁導線を平面状に多重巻きして構成したコイルを
折り曲げた状態で使用する磁気バブルメモリ駆動コイル
において、 上記コイルは場所により巻線密度を変えたことを特徴と
する磁気バブルメモリ駆動コイル。
[Claims] 1. A magnetic bubble memory drive coil in which a coil formed by multiple windings of insulated conductive wire in a plane is used in a bent state, characterized in that the coil has a winding density that varies depending on the location. Magnetic bubble memory drive coil.
JP61139240A 1986-06-17 1986-06-17 Magnetic bubble memory driving coil Pending JPS62298085A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61139240A JPS62298085A (en) 1986-06-17 1986-06-17 Magnetic bubble memory driving coil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61139240A JPS62298085A (en) 1986-06-17 1986-06-17 Magnetic bubble memory driving coil

Publications (1)

Publication Number Publication Date
JPS62298085A true JPS62298085A (en) 1987-12-25

Family

ID=15240727

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61139240A Pending JPS62298085A (en) 1986-06-17 1986-06-17 Magnetic bubble memory driving coil

Country Status (1)

Country Link
JP (1) JPS62298085A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20120188039A1 (en) * 2005-07-22 2012-07-26 Winstead Assets Limited Field winding

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20120188039A1 (en) * 2005-07-22 2012-07-26 Winstead Assets Limited Field winding
US9361567B2 (en) 2005-07-22 2016-06-07 Winstead Assets Limited Inductor

Similar Documents

Publication Publication Date Title
US5448822A (en) Method of making a thin film magnetic head having multi-layer coils
JP2004305736A (en) Production method of shim wire coil
US3505569A (en) Inductive circuit component
JPS62298085A (en) Magnetic bubble memory driving coil
US3903437A (en) Linear motor winding and method of fabricating the same
JPS6229115A (en) Planar coil body
JP2602386Y2 (en) High frequency coil
JPH1032117A (en) Coil
US6984789B2 (en) Electrical cable and method of making
JPH01173611A (en) Manufacture of laminated inductor
US6075430A (en) Inductive component with wound core
JP2003017333A (en) Metal wire
JPS5998506A (en) Inductance element
JP3370924B2 (en) Winding method of split type superconducting coil
JP2002124427A (en) Method for manufacturing chip inductor
JPH03245746A (en) Stator coil
JPS62282424A (en) Manufacture of coil
JP2570491Y2 (en) choke coil
JPS5877221A (en) Manufacture of thick film transformer
SU397999A1 (en) METHOD OF MANUFACTURING A MULTI-REVOLUTION PACKAGE
JPH051046Y2 (en)
JPS5828335Y2 (en) superconducting magnet
JPS63302748A (en) Manufacture of rectangular-conductor coil
JPS62124616A (en) Coil structure of magnetic head
JPH09320863A (en) Transformer and its manufacture