JPS6028376B2 - Manufacturing method for rolled magnets - Google Patents

Manufacturing method for rolled magnets

Info

Publication number
JPS6028376B2
JPS6028376B2 JP15977678A JP15977678A JPS6028376B2 JP S6028376 B2 JPS6028376 B2 JP S6028376B2 JP 15977678 A JP15977678 A JP 15977678A JP 15977678 A JP15977678 A JP 15977678A JP S6028376 B2 JPS6028376 B2 JP S6028376B2
Authority
JP
Japan
Prior art keywords
magnet
shaped
magnetic
roll
manufacturing
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.)
Expired
Application number
JP15977678A
Other languages
Japanese (ja)
Other versions
JPS5586104A (en
Inventor
耕二 肥谷
敬之 三好
寛治 町田
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 Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP15977678A priority Critical patent/JPS6028376B2/en
Publication of JPS5586104A publication Critical patent/JPS5586104A/en
Publication of JPS6028376B2 publication Critical patent/JPS6028376B2/en
Expired legal-status Critical Current

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  • Manufacturing Cores, Coils, And Magnets (AREA)

Description

【発明の詳細な説明】 本発明は押出し成形した異万性複合フェライト磁石によ
って外周多極のロール状マグネットを得るロール状マグ
ネットの製造法に係り、磁極位置および極間部を全て有
効な磁気配向に成形し表面の磁束密度を向上させたもの
を提供しようとするものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for producing a rolled magnet with a multi-pole outer circumference using an extruded heterotropic composite ferrite magnet, in which the magnetic pole positions and the space between the poles are all aligned in an effective magnetic orientation. The objective is to provide a material that is molded to improve the surface magnetic flux density.

従来におけるロール状マグネットとしては第1図に示す
ようにシャフト1の外周面にパイプ状に成形し焼結した
等方向性フェライト磁石2を固着したものが使用されて
いた。
As shown in FIG. 1, a conventional roll-shaped magnet has been used in which an isotropic ferrite magnet 2 formed into a pipe shape and sintered is fixed to the outer peripheral surface of a shaft 1.

この構成によるものは、暁縞収縮による寸法歪みが大き
く細く長くなる程歪みが大きいため製造寸法に限界があ
り、パイプ状の中心孔の歪みによりシャフト1との綾合
が困難で接着性が悪く、磁石としての比重が5.0と大
きく、競縞工程が必要なため、磁石内部にすができやす
く表面磁束密度がばらつく要因になっていた。
With this configuration, there is a limit to the manufacturing dimensions because the dimensional distortion due to dawn shrinkage is large and the distortion becomes larger as the thinner and longer the pipe becomes longer.Due to the distortion of the pipe-shaped center hole, it is difficult to mate with the shaft 1 and the adhesion is poor. Since the specific gravity as a magnet is as high as 5.0 and a striation process is required, soot tends to form inside the magnet, causing variations in surface magnetic flux density.

また、他の従来例としては、第2図に示すようにシャフ
ト1の表面に外周から中心方向に強磁性を有する磁気異
方性の扇状暁絹磁石3を磁極数だけ所定位置に貼付けて
構成したものもある。
In addition, as another conventional example, as shown in FIG. 2, magnetically anisotropic fan-shaped Akira silk magnets 3 having ferromagnetism are pasted at predetermined positions on the surface of the shaft 1 from the outer periphery toward the center, as many as the number of magnetic poles. Some did.

しかしながら、この構成においても異方性嬢結磁石3を
使用するため素材が高く工程も複雑となってコスト面が
不利となり、ロール表面の鞄方向に均一な磁力を得るた
めロール状マグネット表面の真直性が必要となり、磁石
の研摩、貼合せなど高度な工法が必要で、さらに長いロ
ール状マグネットが必要なときは加工の限界により軸万
向に分割した磁石を継ぎ合せるため継目の磁力が低下す
る欠点があった。本発明は以上のような従来の欠点を除
去するものである。
However, even in this configuration, since the anisotropic magnet 3 is used, the material is expensive and the process is complicated, resulting in a cost disadvantage. This requires advanced construction methods such as magnet polishing and bonding, and when longer rolled magnets are required, due to processing limitations, magnets that have been split in all directions are spliced together, reducing the magnetic force at the joint. There were drawbacks. The present invention eliminates the drawbacks of the prior art as described above.

以下、本発明の実施例を図面第3図〜第8図により説明
する。
Embodiments of the present invention will be described below with reference to FIGS. 3 to 8.

まず、第3図に示すように磁気異方性処理をしたフェラ
イト粒子4と、このフェライト粒子4を接合するゴムお
よびまたは合成樹脂の媒質5との混合物を押出し成形し
て磁石6を得る。
First, as shown in FIG. 3, a magnet 6 is obtained by extruding a mixture of ferrite particles 4 subjected to magnetic anisotropy treatment and a medium 5 of rubber and/or synthetic resin for bonding the ferrite particles 4.

この磁石6の磁気配向はフェライト粒子4の流れに沿っ
て配向されるため、第4図のB一日曲線で示すように押
出し方向b方向に対して磁石6の厚さ方向a方向に強磁
性を示す磁気異方性磁石となるbまた、この押出し配向
の異方性磁石6の磁気特性としては、フェライト粒子4
の配合量が重量比で80〜90%にて最大の磁気エネル
ギー(BHmax)をもち、成形材厚は5.0肋以下で
あれば配向率が低下しないとされている。
Since the magnetic orientation of the magnet 6 is oriented along the flow of the ferrite particles 4, ferromagnetism occurs in the thickness direction a of the magnet 6 with respect to the extrusion direction b, as shown by the B-day curve in FIG. The magnetic properties of the extrusion-oriented anisotropic magnet 6 are such that the ferrite particles 4
It is said that the orientation ratio will not decrease if the blending amount is 80 to 90% by weight and the maximum magnetic energy (BHmax) is obtained, and the thickness of the molded material is 5.0 or less.

本発明はこの押出し配向の複合フェライト磁石を使って
ロール状マグネットを成形するに当り、磁気異方性磁石
の強磁性方向を有効に活用し、ロール状マグネット表面
の必要磁極に強磁性が集中するように配向させたロール
状マグネットを得るようにするものである。
In forming a roll-shaped magnet using this extrusion-oriented composite ferrite magnet, the present invention makes effective use of the ferromagnetic direction of the magnetically anisotropic magnet, so that ferromagnetism is concentrated at the necessary magnetic poles on the surface of the roll-shaped magnet. The purpose is to obtain a roll-shaped magnet that is oriented in this manner.

例えば、ロール状マグネットの表面磁極が8極対称にな
る場合を想定して説明すると、第5図に示すようにシャ
フト7の周囲に8等分した扇状の磁石体8を8個組合せ
、しかもその扇状の磁石体8は第3図に示す方法で押出
し成形されて3個の磁石ピース9,10,11によって
構成されている。
For example, assuming that the surface magnetic poles of a rolled magnet are 8 poles symmetrical, as shown in FIG. The fan-shaped magnet body 8 is formed by extrusion molding using the method shown in FIG. 3, and is composed of three magnet pieces 9, 10, and 11.

磁石ピース9は扇状をしており、外周面にはU字状の凹
溝12を形成した形状をしており、磁石ピース10は上
記凹溝12にはまり合うU字状で外周面に凹溝13を形
成した形状をしており、磁石ピース11は凹溝13には
まり合う内周がU字状で外周が円弧面状をしている。こ
の磁石体8の分割数は磁気配向が滑らかに変化し、極間
mにて90度になればマグネット内部の磁路として最も
都合が良くなるので細かく分割する程有効であるが直径
5仇舷以下の形状のロール状マグネットにおいては最低
3段階に分けて個々に押出し成形すれば効果が発揮され
ることになる。
The magnet piece 9 is fan-shaped and has a U-shaped groove 12 on its outer circumferential surface, and the magnet piece 10 has a U-shaped groove on its outer circumferential surface that fits into the groove 12. The magnet piece 11 has a U-shaped inner circumference that fits into the groove 13 and an arcuate outer circumference. The number of divisions of this magnet body 8 is such that the magnetic orientation changes smoothly, and a distance of 90 degrees between poles is most convenient for the magnetic path inside the magnet, so the finer the division, the more effective it is. For roll-shaped magnets having the following shapes, the effect will be exhibited if extrusion molding is carried out individually in at least three stages.

このようにして組込んで構成したロール状マグネットは
第3図に示すようになる。この構成のマグネットの磁気
異方性は磁極部nにおいては放射方向01こ強磁性とな
り、極間部mに向って順次角度が変化し、極間部mにて
順次角度が変化し、極間部mにて円周方向Pに強磁性を
もっているためマグネット全体を有効に活用することに
なる。また他の実施例として第7図に示すようにシャフ
ト7の周囲に8個のU字状凹溝12を等間隔に形成した
磁石素体14を押出し成形により得たものを取付け、こ
の各凹溝12に押出し成形による磁石ピ−ス10,11
を組込んで第8図に示すようなロール状マグネットとす
ることができる。この構成によるものにおいても、上述
と同様の効果が得られることになり、さらに各磁極の位
置規制が確実で組立て作業も容易になるという別の効果
が得られる。このようなロール状マグネットの表面磁束
密度は上記のBHmax=uMQ史の素材をフル着磁し
たとき、110〜1300ガラスまで向上し、単にリン
グ状に押出し配向させた場合の600〜800ガウスを
ズ和風こ向上し、第1図に示す等万性フェライト暁綾磁
石の1100〜1200ガウスに匹敵するか、むしろそ
れ以上の強磁力磁石として利用することが可能となる。
The rolled magnet constructed in this manner is shown in FIG. The magnetic anisotropy of the magnet with this configuration is ferromagnetic in the radial direction 01 at the magnetic pole part n, the angle changes sequentially toward the interpolar part m, and the angle changes sequentially toward the interpolar part m. Since the portion m has ferromagnetism in the circumferential direction P, the entire magnet can be effectively utilized. As another example, as shown in FIG. 7, a magnet body 14 obtained by extrusion molding in which eight U-shaped grooves 12 are formed at equal intervals is attached around the shaft 7, and each of the grooves is Magnet pieces 10 and 11 are extruded into the groove 12.
can be incorporated into a rolled magnet as shown in FIG. With this configuration as well, the same effects as described above can be obtained, and another effect is obtained in that the position of each magnetic pole is reliably regulated and the assembly work is facilitated. The surface magnetic flux density of such a roll-shaped magnet increases to 110-1300 glass when the material with the BHmax=uMQ history described above is fully magnetized, and it surpasses the 600-800 Gauss when it is simply extruded and oriented in a ring shape. It has improved the Japanese style and can be used as a strong magnetic magnet with a magnetic force comparable to, or even higher than, the 1,100 to 1,200 Gauss of the isomeriferous ferrite Akaya magnet shown in FIG.

以上のように本発明のロール状マグネットの製造法によ
れば押出し成形により磁気異方性が可能なため暁緒など
の工法が不要となり、形状が安定するため磁気特性が安
定し、工数も大幅に低減でき、複合フェライト材料のた
め比重が3.5と小さく軽量化が計れ、マグネット全体
を有効に活用するため磁極部の磁束密度が高くなり強磁
力となるため小型化が計れ、後加工が容易となり割れや
欠けなどの発生もなく信頼性に富んだものが提供できる
などの利点をもち、工業的価値の大なるものである。
As described above, according to the manufacturing method of the rolled magnet of the present invention, magnetic anisotropy can be achieved by extrusion molding, eliminating the need for construction methods such as shading, stabilizing the shape, stabilizing the magnetic properties, and significantly reducing the number of man-hours. Composite ferrite material has a specific gravity of 3.5, making it lightweight. Since the entire magnet is effectively utilized, the magnetic flux density at the magnetic poles increases, resulting in strong magnetic force, making it possible to downsize and facilitate post-processing. It has the advantage of being highly reliable without cracking or chipping, and is of great industrial value.

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

第1図、第2図は従来のロール状マグネットの斜視図、
第3図は本発明のロール状マグネットの製造法に採用す
る磁気異万性磁石の製造法を示す説明図、第4図は同磁
気異方性磁石のB−日特性図、第5図は同方法による組
立工程の説明図、第6図は同方法により得たロール状マ
グネットの側面図、第7図は他の実施例の組立工程の説
明図、第8図は同方法により得たロール状マグネットの
側面図である。 4・・・・・・フェライト粒子、5・・・・・・媒質、
6・・…・磁石、7・・・・・・シャフト、8・・・・
・・磁石体、9〜11・・・・・・磁石チップ、12・
・・・・・凹溝、13・・・・・・凹溝、14・・・・
・・磁石秦体。 第1図 第2図 第3図 第4図 第5図 第6図 第7図 第8図
Figures 1 and 2 are perspective views of conventional rolled magnets;
FIG. 3 is an explanatory diagram showing the method of manufacturing an anisotropic magnet adopted in the method of manufacturing a rolled magnet of the present invention, FIG. 4 is a B-day characteristic diagram of the anisotropic magnet, and FIG. An explanatory diagram of the assembly process by the same method, FIG. 6 is a side view of a rolled magnet obtained by the same method, FIG. 7 is an explanatory diagram of the assembly process of another example, and FIG. 8 is a roll obtained by the same method. FIG. 3 is a side view of a shaped magnet. 4... Ferrite particles, 5... Medium,
6...Magnet, 7...Shaft, 8...
... Magnet body, 9-11 ... Magnet chip, 12.
...concave groove, 13...concave groove, 14...
...Magnet Qin body. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8

Claims (1)

【特許請求の範囲】[Claims] 1 フエライト粒子と媒質の混合物を押出し成形するこ
とによりフエライト粒子の流出方向に直角に強磁性を示
す磁気異方性の複合フエライト磁石によつて外周多極の
ロール状マグネツトを製造する方法において、上記押出
し成形により成形された複数の磁石ピースを組み合わせ
て扇状の磁石体を構成し、この磁石体の磁化容易軸がほ
ぼ放射状になるように配列させることを特徴とするロー
ル状マグネツトの製造法。
1. In the method of manufacturing a roll-shaped magnet with a multi-pole outer circumference using a magnetically anisotropic composite ferrite magnet that exhibits ferromagnetism perpendicular to the outflow direction of the ferrite particles by extrusion molding a mixture of ferrite particles and a medium, the above A method for producing a roll-shaped magnet, which comprises combining a plurality of extrusion-molded magnet pieces to form a fan-shaped magnet body, and arranging the magnet bodies so that their easy magnetization axes are substantially radial.
JP15977678A 1978-12-22 1978-12-22 Manufacturing method for rolled magnets Expired JPS6028376B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15977678A JPS6028376B2 (en) 1978-12-22 1978-12-22 Manufacturing method for rolled magnets

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15977678A JPS6028376B2 (en) 1978-12-22 1978-12-22 Manufacturing method for rolled magnets

Publications (2)

Publication Number Publication Date
JPS5586104A JPS5586104A (en) 1980-06-28
JPS6028376B2 true JPS6028376B2 (en) 1985-07-04

Family

ID=15701006

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15977678A Expired JPS6028376B2 (en) 1978-12-22 1978-12-22 Manufacturing method for rolled magnets

Country Status (1)

Country Link
JP (1) JPS6028376B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63259366A (en) * 1987-04-14 1988-10-26 株式会社 前川製作所 Method of promoting heat transfer such as refrigeration, heating, drying or the like by jet air current

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4820433A (en) * 1986-09-05 1989-04-11 Nippon Zeon Co., Ltd. Magnetic powder for magnetic recording
JP2590432Y2 (en) * 1991-10-15 1999-02-17 シャープ株式会社 Induction heating cooker
JP4857959B2 (en) * 2006-06-30 2012-01-18 Tdk株式会社 Magnet for magnet roll

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63259366A (en) * 1987-04-14 1988-10-26 株式会社 前川製作所 Method of promoting heat transfer such as refrigeration, heating, drying or the like by jet air current

Also Published As

Publication number Publication date
JPS5586104A (en) 1980-06-28

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