JPS615506A - Generator for magnetic field - Google Patents

Generator for magnetic field

Info

Publication number
JPS615506A
JPS615506A JP59126118A JP12611884A JPS615506A JP S615506 A JPS615506 A JP S615506A JP 59126118 A JP59126118 A JP 59126118A JP 12611884 A JP12611884 A JP 12611884A JP S615506 A JPS615506 A JP S615506A
Authority
JP
Japan
Prior art keywords
magnetic field
coil
magnetic
solenoid
central axis
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
JP59126118A
Other languages
Japanese (ja)
Other versions
JPH0518245B2 (en
Inventor
Haruo Urai
浦井 治雄
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric Co 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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP59126118A priority Critical patent/JPS615506A/en
Publication of JPS615506A publication Critical patent/JPS615506A/en
Publication of JPH0518245B2 publication Critical patent/JPH0518245B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00Magnets
    • H01F7/06Electromagnets; Actuators including electromagnets
    • H01F7/20Electromagnets; Actuators including electromagnets without armatures

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)

Abstract

PURPOSE:To increase intensity per unit currents of a magnetic field, to lower an applied current value required for the same generating magnetic field and to inhibit the heat dissipation of a coil by mounting a soft ferromagnetic material plate having a normal parallel with the central axis of the solenoid type coil to an end surface vertical to the central axis of the solenoid type coil. CONSTITUTION:A Helmholtz type coil in which coils such as solenoid type ones 1a, 1b are positioned oppositely through a clearance section 20 is used as a coil for generating a magnetic field. A sample piece 5 to which the magnetic field must be applied is positioned normally in the clearance section 20 in the coil in such a Helmholtz type magnetic-field generating coil. The magnetic field 21 generated is of a component in the direction along the central axis of the coil. Disks 2a, 2b consisting of a high permeability soft magnetic material are fitted brought into contact with end surfaces 10 vertical to the central axis of the solenoid type coil so as to each share holes together wit hollow sections 12 in the solenoid in such a case. Accordingly, magnetic field intensity generated per unit currents is increased, thus realizing a magnetic field generator having small power consumption in the coil section in the same magnetic field intensity.

Description

【発明の詳細な説明】 (産業上の利用分野)゛ 本□発明はソレノンド型コイルを用いて磁界を発生する
装置に関するものである。′更に詳しく述べれば1発生
磁界を強化することを可能とした構造を有する磁界発生
装置量に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Field of Application) The present invention relates to a device that generates a magnetic field using a solenoid coil. More specifically, the present invention relates to a magnetic field generating device having a structure that makes it possible to strengthen the generated magnetic field.

(従来技術とその問題点) 表−に垂直なiい一軸性磁気異方性を有する磁性材料薄
片中に存在する磁気バブルを利用した磁抵バブILt″
−子に於いては1通常磁気バブル番□安定に保持する目
的のために、磁性材料薄片に垂直な□バブル保i磁界(
以下□バイアス磁界と呼称する)゛カ必要である。バイ
アス磁界を発生するには、永久磁石を用いる方法やソレ
ノイド型中空コイルを用いる方法がよく知られている。
(Prior art and its problems) A magnetoresistive bubble ILt'' that utilizes magnetic bubbles existing in a thin piece of magnetic material having i-uniaxial magnetic anisotropy perpendicular to the surface.
- For the purpose of stably holding the magnetic bubble number □ in the child, the □ bubble holding field perpendicular to the thin piece of magnetic material (
(hereinafter referred to as □bias magnetic field) is required. To generate a bias magnetic field, methods using permanent magnets and methods using solenoid-type hollow coils are well known.

特に、磁気バブル素子の緒特性を測定−評価する際には
、前記レイイアス磁界を変化させることが重要である。
In particular, when measuring and evaluating the magnetic properties of a magnetic bubble element, it is important to change the magnetic field.

従りてとの目的のためには、バイアス磁界の発生は。Therefore, for the purpose of generating a bias magnetic field.

。工□□1゜1.。ヮヵ85え、わ、ッ271イド型コ
イルを用いるのが一般的である。
. Engineering□□1゜1. . It is common to use a waka85, wa, 271 id type coil.

一方、磁気バブル素子、特に磁気バブルを情報の担体と
して利用する磁気バブルメモリ素子では。
On the other hand, in magnetic bubble devices, especially magnetic bubble memory devices that utilize magnetic bubbles as information carriers.

情報の高密度化のために、用いる磁気バブルの径を微小
化することが行なわれてきた。磁気バブルを微小化する
に伴って、一般にはその磁性材料の飽和磁化Msを大き
くする必要がある。飽和磁化が大きくなると、これに従
って磁気バブルを安定に保持するバイアス磁界も大きく
なる。例えば、磁性材料として磁性ガーネット膜を用い
た場合、磁気バブル直径が3μm程度のときはバイアス
磁界としては、  1500e  程度であったのが、
2μm直径の磁気バブルを保持するバイアス磁界は約2
500e、14m直径tc対しては3500e 程度必
要とする。更に0.5μm直径の磁気バブルを安定に保
持するには6000e 程度のバイアス磁界が必要とな
る。
In order to increase the density of information, efforts have been made to miniaturize the diameter of the magnetic bubbles used. As magnetic bubbles become smaller, it is generally necessary to increase the saturation magnetization Ms of the magnetic material. As the saturation magnetization increases, the bias magnetic field that stably holds the magnetic bubble also increases accordingly. For example, when a magnetic garnet film is used as the magnetic material, when the magnetic bubble diameter is about 3 μm, the bias magnetic field is about 1500e;
The bias magnetic field that holds a 2 μm diameter magnetic bubble is approximately 2
For a diameter tc of 500e and 14m, approximately 3500e is required. Furthermore, a bias magnetic field of about 6000e is required to stably hold a magnetic bubble with a diameter of 0.5 μm.

この・様に、微小磁気バブルを利用した磁気バブル素子
を評価するには、高いバイアス磁界が必要とされる。高
いバイアス磁界を発生するには、磁界発生コイルに大き
な電流を印加すれば良いが。
As described above, a high bias magnetic field is required to evaluate a magnetic bubble device using minute magnetic bubbles. To generate a high bias magnetic field, it is sufficient to apply a large current to the magnetic field generating coil.

単純なコイルではコイルに発生するジーール熱は電流値
の自乗に比例するため、バイアス磁界の上昇に伴ない急
激にコイルの温度が上昇し、安定に磁気バブル素子の評
価・測定が行なえなくなる欠点を有している。
In a simple coil, the Ziehl heat generated in the coil is proportional to the square of the current value, so as the bias magnetic field increases, the temperature of the coil rises rapidly, making it impossible to stably evaluate and measure magnetic bubble elements. have.

(発明の目的) 本発明の目的は、上記の欠点を取り除くため。(Purpose of the invention) The aim of the invention is to eliminate the above-mentioned drawbacks.

ソレノイド型磁界発生コイルで発生する磁界の単位電流
当りの強度を大きくすることにより、同一発生磁界に要
する印加電流値を下げ、コイルの発熱を抑制する磁界発
生装置を提供することにある。
It is an object of the present invention to provide a magnetic field generating device which reduces the applied current value required for the same generated magnetic field and suppresses heat generation in the coil by increasing the strength per unit current of the magnetic field generated by a solenoid type magnetic field generating coil.

(発明の構成) 本発明による磁界発生装置の構成は、少なくとも1つの
ソレノイド型磁界発生コイルを有し、該ソレノイド型コ
イルの中心軸に垂直な端面に、該中心軸に平行な法線を
有する軟強磁性体平板を設けたことを特徴とするもので
ある。
(Configuration of the Invention) The configuration of the magnetic field generating device according to the present invention includes at least one solenoid type magnetic field generation coil, and has a normal line parallel to the central axis on an end face perpendicular to the central axis of the solenoid type coil. It is characterized by the provision of a soft ferromagnetic flat plate.

(構成の詳細な説F!A) 本発明は、磁界発生装置を上述の構成にするこ    
    1(とにより従来技術の欠点を解決するもので
ある。
(Detailed explanation of the configuration F!A) The present invention provides a magnetic field generating device having the above-described configuration.
1 (which solves the drawbacks of the prior art.

本発明の原理は、ソレノイド型磁界発生コイルの外端面
に高透磁率軟磁性体の平板を設け、もしそれが無ければ
、ソレノイド型磁界発生コイルの外部分に広く分散する
筈の磁束を、高透磁率磁性平板に吸収せしめ、いわゆる
鏡像効果により、ソレノイド内部の磁界を強調すること
にある。
The principle of the present invention is to provide a flat plate of high magnetic permeability soft magnetic material on the outer end surface of the solenoidal magnetic field generating coil, and to increase the magnetic flux that would otherwise be widely dispersed in the outer part of the solenoidal magnetic field generating coil. The purpose is to emphasize the magnetic field inside the solenoid by absorbing the magnetic permeability into a magnetic flat plate and using the so-called mirror image effect.

(実施例) 以下に本発明の実施例を図面を用いて睨明する。(Example) Embodiments of the present invention will be explained below with reference to the drawings.

実施例1 第1図を用いて本発明の第1の実施例を説明する。本実
施例では、al界発生用コイルとして、ソレノイド型コ
イルla、lbが間隙部20を介して対置シタヘルムホ
ルツ型コイルを用いている。通常この様なヘルムホルツ
型磁界発生コイルでは、磁界を印加すべき試料片5は、
コイルの間隙部20に置く。発生する磁界21は、コイ
ル中心軸に沿った方向の成分である。
Example 1 A first example of the present invention will be described with reference to FIG. In this embodiment, as the AL field generating coil, a Shita Helmholtz type coil is used in which the solenoid type coils la and lb are placed opposite each other with a gap 20 interposed therebetween. Normally, in such a Helmholtz type magnetic field generating coil, the sample piece 5 to which the magnetic field is applied is
Place it in the gap 20 of the coil. The generated magnetic field 21 is a component in the direction along the central axis of the coil.

高透磁率軟磁性体の円板2a、2bが夫々穴をソレノイ
ドの中空部12と共有する様に、ソレノイド型コイルの
中心軸に垂直な端面lOに接して設けられている。ソレ
ノイドコイルの寸法が、内径32酩、外径95騙、厚さ
が1511sで間隙の大きさが16簡の場合、肉厚3朋
のNiZn磁性フェライトの穴あき円゛板を設けると、
これがない場合に比べて、単位電流当り約20%強い磁
界が発生することが判明した。
Discs 2a and 2b made of a soft magnetic material with high magnetic permeability are provided in contact with an end surface 10 perpendicular to the central axis of the solenoid-type coil so as to share their respective holes with the hollow portion 12 of the solenoid. If the solenoid coil has an inner diameter of 32 mm, an outer diameter of 95 mm, a thickness of 1511 mm, and a gap size of 16 mm, if a perforated circular plate of NiZn magnetic ferrite with a wall thickness of 3 mm is provided,
It has been found that a magnetic field that is approximately 20% stronger per unit current is generated than in the case without this.

換言すれば、同じ発生磁界強度を得るには、約15チ少
ない電流値で済む、即ち、この磁界発生装置での消費電
力は約30%減少し、ジュール熱の発生はそれだけ抑え
られる。
In other words, to obtain the same generated magnetic field strength, a current value that is approximately 15 inches smaller is required, that is, the power consumption of this magnetic field generator is reduced by approximately 30%, and the generation of Joule heat is suppressed accordingly.

1m 第2図を用いて、第2の実施例を説明する0本実施例で
は、磁界発生用のコイルとしては前述の第1の実施例と
同様ソレノイド型コイルla、lbよりなるヘルムホル
ツ型コイルを用いる。高透磁率軟磁性体の平板2a、2
bは、前例と異なり、コイル中央の中空部に対応する穴
のない単なる円板である。この場合、中央部の穴がない
ことにより。
1m The second embodiment will be explained using FIG. use Flat plates 2a, 2 made of high magnetic permeability soft magnetic material
Unlike the previous example, b is simply a disk without a hole corresponding to the hollow part at the center of the coil. In this case, due to the lack of a hole in the central part.

前例では、穴を通じて外部へ分散していた磁束の漏れが
回避出来、より完全なコイルの鏡像が形成される。従っ
て、単位電流当りの発生磁界は、更に増大をみる0本例
の場合、約25Lsの増大をみた−即ち、同じ磁界を発
生するためには20%少ない電流で済み、コイルの、消
費電力的にみれば約35tsの減少となる。
In the previous example, leakage of the magnetic flux that was dispersed to the outside through the holes is avoided, and a more perfect mirror image of the coil is formed. Therefore, the generated magnetic field per unit current will further increase. In this example, we saw an increase of about 25 Ls - that is, to generate the same magnetic field, 20% less current is required, which reduces the power consumption of the coil. This is a decrease of about 35ts.

実施例3 第3図を用いて1本発明の第3の実施例を説明する、本
実施例では、第1の実施例で示した磁界発生装置を、磁
気バブル素子評価用コイルに応用している。ソレノイド
型コイルを対した間隙部20に1面内回転磁界発生用の
コイル6を設けである。
Example 3 A third example of the present invention will be described with reference to FIG. 3. In this example, the magnetic field generator shown in the first example is applied to a coil for evaluating magnetic bubble elements. There is. A coil 6 for generating a rotating magnetic field in one plane is provided in a gap 20 between the solenoid coils.

回転磁界コイルとしては、磁性フェライトリングに励起
用コイルを巻き付けた形状や、ヘルムホルツ型中空コイ
ル等がこの目的に適している。試料5はコイル間々隙部
加の中央部に設置される、ソレノイド型コイルの中空部
校及びこれに対応する穴あきの高透磁率円板2aを通し
て、光源7及び観察部8よりなる顕微鏡の如き光学観察
・手段により、試料の状態を1面内磁界及びこれに垂直
なコイル中心軸に沿った磁界を印加しつつ観察すること
が出来る。この様な磁界発生装置を用いれば、前述の如
き、直径0.5μm以下の磁気バブルを用いた素子も、
その特性を、コイル発熱を影響を受けずに評価すること
が出来る。
As the rotating magnetic field coil, a shape in which an excitation coil is wound around a magnetic ferrite ring, a Helmholtz type hollow coil, etc. are suitable for this purpose. The sample 5 is passed through a hollow part of a solenoid-type coil installed in the center of the coil gap and a corresponding perforated high-permeability disk 2a, and an optical system such as a microscope consisting of a light source 7 and an observation part 8 is By using the observation method, the state of the sample can be observed while applying an in-plane magnetic field and a magnetic field along the coil center axis perpendicular to this. If such a magnetic field generator is used, elements using magnetic bubbles with a diameter of 0.5 μm or less as described above can also be produced.
Its characteristics can be evaluated without being affected by coil heat generation.

(発明の効果) 以上に述べた様に1本発明を用いれば、単位゛電流あた
りの発生磁界強度が大きく、従って同じ磁界強度では、
コイル部分での消費電力の少ない磁界発生装置が実現さ
れる0本発明の枠材としては、前述の高透磁率を有する
磁性フェライトのみならず、パーマロイの如き、高透磁
率金属材料を用いでも本発明の効果は容易に得られるこ
とは、その原理からみて当然である。又、磁界発生コイ
ルとして、ソレノイド型コイルを対置組合せしたヘルム
ホルツ型のみならず、単なる1個のソレノイド型コイル
のみに対しても本発明を実施出来ることは明白である。
(Effects of the Invention) As described above, if the present invention is used, the generated magnetic field strength per unit current is large, so at the same magnetic field strength,
A magnetic field generating device with low power consumption in the coil portion is realized.The frame material of the present invention can be made of not only magnetic ferrite having high magnetic permeability as described above, but also high magnetic permeability metal materials such as permalloy. It is natural from the principle that the effects of the invention can be easily obtained. Furthermore, it is clear that the present invention can be practiced not only with a Helmholtz type magnetic field generating coil in which solenoid type coils are arranged in opposition, but also with a single solenoid type coil.

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

第1図〜第3図は本発明の実施例を示す概略図である。 図に於いて、la、lbはソレノイド製磁界発生コイル
、 2a、2bは高透磁率磁性材料平板、5は試料、6
は面内磁界発生コイル、7は光源部、8は観察部、10
はソレノイド製磁界発生コイルの中心軸に垂直な端面、
12はコイルの中空部、20はコイル間隙、21はコイ
ル中心軸に平行な磁界を示す。
1 to 3 are schematic diagrams showing embodiments of the present invention. In the figure, la and lb are solenoid magnetic field generating coils, 2a and 2b are high permeability magnetic material flat plates, 5 is a sample, and 6
is an in-plane magnetic field generating coil, 7 is a light source section, 8 is an observation section, 10
is the end face perpendicular to the central axis of the solenoid magnetic field generating coil,
12 is a hollow part of the coil, 20 is a coil gap, and 21 is a magnetic field parallel to the coil center axis.

Claims (4)

【特許請求の範囲】[Claims] (1)少なくとも1つのソレノイド型磁界発生コイルを
有し、該ソレノイド型コイルの中心軸に垂直な端面に、
該中心軸に平行な法線を有する軟強磁性体平板を設けた
ことを特徴とする磁界発生装置。
(1) It has at least one solenoid-type magnetic field generating coil, and on an end face perpendicular to the central axis of the solenoid-type coil,
A magnetic field generating device comprising a soft ferromagnetic flat plate having a normal line parallel to the central axis.
(2)軟磁性体平板がその中心部にソレノイド型磁界発
生コイルの内径にはぼ等しい開孔を有することを特徴と
する特許請求の範囲第1項記載の磁界発生装置。
(2) The magnetic field generating device according to claim 1, wherein the soft magnetic flat plate has an opening in its center that is approximately equal to the inner diameter of the solenoid type magnetic field generating coil.
(3)二つのソレノイド型磁界発生コイルを対置したヘ
ルムホルツ型コイルの両端面に軟強磁性体平板を設けた
特許請求の範囲第1項又は第2項記載の磁界発生装置。
(3) The magnetic field generating device according to claim 1 or 2, wherein soft ferromagnetic flat plates are provided on both end faces of a Helmholtz coil in which two solenoid type magnetic field generating coils are placed opposite each other.
(4)軟強磁性体としてフェライトを用いたことを特徴
とする特許請求の範囲第1項、第2項又は第3項記載の
磁界発生装置。
(4) The magnetic field generating device according to claim 1, 2, or 3, characterized in that ferrite is used as the soft ferromagnetic material.
JP59126118A 1984-06-19 1984-06-19 Generator for magnetic field Granted JPS615506A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59126118A JPS615506A (en) 1984-06-19 1984-06-19 Generator for magnetic field

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59126118A JPS615506A (en) 1984-06-19 1984-06-19 Generator for magnetic field

Publications (2)

Publication Number Publication Date
JPS615506A true JPS615506A (en) 1986-01-11
JPH0518245B2 JPH0518245B2 (en) 1993-03-11

Family

ID=14927082

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59126118A Granted JPS615506A (en) 1984-06-19 1984-06-19 Generator for magnetic field

Country Status (1)

Country Link
JP (1) JPS615506A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0325313A1 (en) * 1988-01-19 1989-07-26 Smit Transformatoren B.V. Apparatus for generating a magnetic field in a processing space

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0325313A1 (en) * 1988-01-19 1989-07-26 Smit Transformatoren B.V. Apparatus for generating a magnetic field in a processing space

Also Published As

Publication number Publication date
JPH0518245B2 (en) 1993-03-11

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