JPH0332892B2 - - Google Patents
Info
- Publication number
- JPH0332892B2 JPH0332892B2 JP59186134A JP18613484A JPH0332892B2 JP H0332892 B2 JPH0332892 B2 JP H0332892B2 JP 59186134 A JP59186134 A JP 59186134A JP 18613484 A JP18613484 A JP 18613484A JP H0332892 B2 JPH0332892 B2 JP H0332892B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic flux
- circumferential surface
- magnet
- characteristic
- inner circumferential
- 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 - Lifetime
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F7/00—Magnets
- H01F7/02—Permanent magnets [PM]
- H01F7/0205—Magnetic circuits with PM in general
- H01F7/021—Construction of PM
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
Description
【発明の詳細な説明】
産業上の利用分野
この発明は、モーター、発電機等に多用される
断面弓形の異方性フエライト磁石の改良に係り、
表面磁束分布図における円弧内外周面の周方向の
表面磁束分布特性を特定形状となし、円弧内周面
の磁気特性を著しく向上させた断面弓形異方性フ
エライト磁石に関する。[Detailed Description of the Invention] Industrial Application Field This invention relates to the improvement of anisotropic ferrite magnets with an arcuate cross section, which are often used in motors, generators, etc.
The present invention relates to an anisotropic ferrite magnet having an arcuate cross section, in which the surface magnetic flux distribution characteristics in the circumferential direction of the inner and outer circumferential surfaces of an arc in a surface magnetic flux distribution diagram are shaped into a specific shape, and the magnetic properties of the inner circumferential surface of the arc are significantly improved.
従来の技術
近年、モーターや発電機等の回転電気機器にお
いては、小型・高性能化が不可欠となり、かかる
機器に使用される断面弓形異方性フエライト磁石
も、トータル磁束(φ)T、磁束密度(Bg)、表面
磁束分布のフラツト化などの磁気特性の向上が図
られていた。すなわち、特公昭46−17118号等に
示される種々の構成からなる成形装置を用いて磁
石全体に均等に高磁気特性が発揮されるよう考慮
されていた。Conventional technology In recent years, smaller size and higher performance have become essential for rotating electrical equipment such as motors and generators, and the anisotropic ferrite magnets with an arcuate cross section used in such equipment also have low total magnetic flux (φ) T and magnetic flux density. (Bg), the magnetic properties were improved by flattening the surface magnetic flux distribution. That is, consideration was given to uniformly exhibiting high magnetic properties throughout the magnet by using molding apparatuses having various configurations as shown in Japanese Patent Publication No. 17118/1983.
さらに今日、前記断面弓形異方性フエライト磁
石におけるコイル等との対向面である内周円弧面
の磁気特性向上が新たに切望されている。 Furthermore, today, there is a new desire to improve the magnetic properties of the inner circumferential arcuate surface, which is the surface facing the coil etc. in the anisotropic ferrite magnet having an arcuate cross section.
すなわち、従来の断面弓形異方性フイライト磁
石における内周面の磁気特性は、例えば、内周面
の周方向(第2図の断面弓形磁石におけるX方
向)における表面磁束分布状態は、第3図のA図
に示すように、最高値は両端にあり、その最高値
間は平坦で大きく落込んでいる。また、内周面の
軸方向(第2図のX方向に直交方向のY方向)の
磁束分布は、第3図のB図に示すように、最高値
は両端にあり、その最高値間は著しく落込んでい
る。 That is, the magnetic properties of the inner circumferential surface of a conventional anisotropic fluorite magnet with an arcuate cross section are, for example, the surface magnetic flux distribution state in the circumferential direction of the inner circumferential surface (the X direction in the arcuate cross section magnet of FIG. As shown in Figure A, the highest values are at both ends, and the area between the highest values is flat with a large drop. In addition, the magnetic flux distribution in the axial direction of the inner circumferential surface (the Y direction perpendicular to the X direction in Figure 2) has its highest value at both ends, as shown in Figure B in Figure 3, and the distance between the highest values is It has fallen significantly.
さらに、磁石の内周面と外周面との磁気特性差
は、通常僅かであり、磁石の圧縮成形時の水抜き
等の影響により、数%の差を生じることがある
が、内周面の磁気特性を積極的に向上させ得るも
のでない。 Furthermore, the difference in magnetic properties between the inner circumferential surface and the outer circumferential surface of a magnet is usually small, and a difference of a few percent may occur due to the effects of water removal during compression molding of the magnet. It cannot actively improve magnetic properties.
発明が解決しようとする課題
この発明は、回転電気機器等の小型・高性能化
に適した磁気特性を有する断面弓形異方性フイラ
イト磁石を目的とし、該磁石の内周面と外周面の
磁気特性差を積極的に設けて、内周面の磁気特性
を大幅に向上させた断面弓形異方性フエライト磁
石を目的としている。Problems to be Solved by the Invention The present invention aims to provide an anisotropic filtrite magnet with an arcuate cross section and magnetic properties suitable for downsizing and improving the performance of rotating electrical equipment, etc. The objective is to create an anisotropic ferrite magnet with an arcuate cross-section that significantly improves the magnetic properties of the inner circumferential surface by actively creating property differences.
課題を解決するための手段
この発明は、
断面弓形で円弧面の半径方向に異方性を有し、
円弧内周面が強磁性面でかつ外周面が弱磁性面か
らなる異方性フイライト磁石において、表面磁束
分布図における円弧内周面の周方向の表面磁束分
布特性の最高値部分が該分布の中央部で凸状を形
成する特性を有し、
円弧外周面の周方向の表面磁束分布特性が該分
布の中央部で凹状を形成する特性を有することを
特徴とする異方性フイライト磁石である。Means for Solving the Problems This invention has an arcuate cross section and anisotropy in the radial direction of the circular arc surface,
In an anisotropic filtrate magnet whose inner circumferential surface is a ferromagnetic surface and whose outer circumferential surface is a weakly magnetic surface, the highest value of the surface magnetic flux distribution characteristic in the circumferential direction of the inner circumferential surface of the arc in the surface magnetic flux distribution diagram is the maximum value of the distribution. An anisotropic filtrite magnet having a characteristic of forming a convex shape at the center, and a surface magnetic flux distribution characteristic of the circumferential direction of the arcuate outer peripheral surface having a characteristic of forming a concave shape at the center of the distribution. .
作 用
一般に、従来から知られる断面弓形異方性フイ
ライト磁石の内周面と外周面との磁気特性差は僅
かであり、磁石の圧縮成形時の水抜き等の影響に
より、数%の差を生じることがあつたが、内周面
の磁気特性を積極的に向上させるものでなかつ
た。Function Generally, the difference in magnetic properties between the inner and outer circumferential surfaces of conventionally known anisotropic fluorite magnets with an arcuate cross section is slight, and due to the effects of water removal during compression molding of the magnet, the difference is only a few percent. However, it did not actively improve the magnetic properties of the inner circumferential surface.
この発明は、上記の磁気特性差を積極的に活用
することを知見したもので、従来から知られてい
るスラリー状の磁石原料を用い、ダイス内で成形
体の上下面の磁場強さを変えて圧縮成型する際
に、上パンチと磁石原料間に、ステンレス等から
なる断面弓形状の非磁性体フイルター、例えば、
非磁性体厚みをその外周面円弧中心点と内周面円
弧中心点とを偏心させて中央部を厚肉とした非磁
性体フイルターを介在させて圧縮成型することに
より、内周面側の磁気特性が外周面に比べて大き
く向上した断面弓形異方性フイライト磁石が得ら
れる。 This invention was based on the discovery that the above-mentioned difference in magnetic properties can be actively utilized, and by using the conventionally known slurry magnet raw material, the magnetic field strength on the upper and lower surfaces of the compact is changed in the die. During compression molding, a non-magnetic filter made of stainless steel or the like with a bow-shaped cross section is placed between the upper punch and the magnet raw material.
By compressing and molding the non-magnetic material through a non-magnetic filter with a thick central part by making the center point of the arc on the outer circumferential surface eccentric and the center point of the circular arc on the inner circumferential surface eccentric, the magnetic field on the inner circumferential surface side is A cross-section arcuate anisotropic filtrite magnet whose properties are greatly improved compared to the outer circumferential surface is obtained.
第2図に示す断面弓形形状からなるこの発明に
より異方性フイライト磁石における内周面の磁気
特性は、例えば、内周面の周方向、すなわち、第
2図の断面弓形磁石におけるX方向における表面
磁束分布状態は、第1図Aの実線aに示すよう
に、最高値は中央部にあり、中央部が大きな凸状
を形成しており、また、外周面のX方向の表面磁
束分布は、第1図Aの破線bに示すように中央部
が凹状を形成する特性を示しており、内周面と外
周面の磁気特性差が大きく、かつ内周面の磁気特
性の向上が著しいことが分る。 The magnetic properties of the inner circumferential surface of the anisotropic fluorite magnet according to the present invention having the arcuate cross-section shown in FIG. 2 are as follows: As shown by the solid line a in Figure 1A, the magnetic flux distribution state has the highest value in the center, forming a large convex shape, and the surface magnetic flux distribution in the X direction of the outer peripheral surface is as follows. As shown by the broken line b in Figure 1A, the central part exhibits the characteristic of forming a concave shape, and the difference in magnetic properties between the inner circumferential surface and the outer circumferential surface is large, and the magnetic properties of the inner circumferential surface are significantly improved. I understand.
さらに、前記した両端の最高値間が平坦で大き
く落込んでいる従来磁石の同分布と比較し、最高
値が高く、平均値も高くなる特性が得られる。 Furthermore, compared to the same distribution of conventional magnets in which the range between the maximum values at both ends is flat with a large drop, characteristics are obtained in which the maximum value is high and the average value is also high.
また、内周面の軸方向、すなわち、第2図のX
方向に直交方向のY方向の磁束分布は、第1図B
の実線aに示すように、最高値を含めてほぼフラ
ツトな特性が得られ、また、外周面のY方向の表
面磁束分布は、同図Bの破線bに示す特性を示し
ており、内周面の磁気特性の向上が著しいことが
分る。さらに、前記した両端の最高値間が大きく
落込んでいる従来磁石の同分布と比較し、最高値
は同等以上で、その平均値が極めて高くなる特性
が得られる。 In addition, in the axial direction of the inner circumferential surface, that is,
The magnetic flux distribution in the Y direction perpendicular to the direction is shown in Figure 1B.
As shown by the solid line a in Figure B, almost flat characteristics were obtained including the maximum value, and the surface magnetic flux distribution in the Y direction on the outer circumferential surface showed the characteristics shown by the broken line b in Figure B. It can be seen that the magnetic properties of the surface are significantly improved. Furthermore, compared to the same distribution of conventional magnets in which the maximum value at both ends is greatly depressed, the maximum value is equal to or higher than that, and the average value is extremely high.
実施例
スラリー状の磁石原料を、ダイス内で成形体の
上下面の磁場強さを変えて圧縮成型する際に、上
パンチと磁石原料間にステンレスからなる断面弓
形状で、非磁性体厚みをその外周面円弧中心点と
内周面円弧中心点とを偏心させて中央部を厚肉と
した非磁性体フイルターを介在させて圧縮成型す
る湿式成型方法により、円弧面半径方向に着磁
し、外径65mm×内径30mm×高さ36mmの断面弓形異
方性フイライト磁石を作製し、内周面及び外周面
の表面磁束分布を測定したところ、第1図の磁束
分布図を得た。Example When compression molding a slurry magnet raw material in a die by changing the magnetic field strength on the upper and lower surfaces of the molded object, an arc-shaped cross section made of stainless steel is used between the upper punch and the magnet raw material to reduce the thickness of the non-magnetic material. The arc surface is magnetized in the radial direction by a wet molding method in which the center point of the arc on the outer circumferential surface and the center point of the arc on the inner circumferential surface are made eccentric, and a non-magnetic filter with a thick central portion is interposed and compression molded. A cross-section arcuate anisotropic fluorite magnet with an outer diameter of 65 mm, an inner diameter of 30 mm, and a height of 36 mm was prepared, and the surface magnetic flux distribution on the inner and outer circumferential surfaces was measured, and the magnetic flux distribution diagram shown in FIG. 1 was obtained.
また、同寸法の従来の磁石を製造して内周面及
び外周面の表面磁束分布を測定し、本発明のもの
と比較したところ、内周面中央部における磁束は
15%高く、内周面のΦTも6%高い値を示した。
また、内周面中央部と外周面中央部との磁束差
は、従来磁石が100G程度であるのに、本発明の
磁石は300G以上の差が得られた。 In addition, when we manufactured a conventional magnet with the same dimensions and measured the surface magnetic flux distribution on the inner and outer circumferential surfaces and compared it with that of the present invention, we found that the magnetic flux at the center of the inner circumferential surface was
15% higher, and Φ T of the inner peripheral surface also showed a 6% higher value.
Further, while the difference in magnetic flux between the central part of the inner circumferential surface and the central part of the outer circumferential surface is about 100 G in conventional magnets, the difference in magnetic flux between the central part of the inner circumferential surface and the central part of the outer circumferential surface is 300 G or more in the magnet of the present invention.
発明の効果
この発明は、円弧面の半径方向に異方性を有す
る断面弓形の異方性フイライト磁石において、円
弧内周面の周方向の表面磁束分布を中央部で凸状
を形成する特性となし、また円弧外周面の周方向
の表面磁束分布を中央部で凹状を形成する特性と
することにより、実施例に明らかな如く内周面と
外周面の磁気特性差が大きくなり、内周面の磁気
特性が著しく向上する。Effects of the Invention The present invention provides an anisotropic fluorite magnet having an arcuate cross-section and anisotropy in the radial direction of the arcuate surface. None, and by making the surface magnetic flux distribution in the circumferential direction of the arcuate outer circumferential surface have a characteristic of forming a concave shape at the center, the difference in magnetic properties between the inner circumferential surface and the outer circumferential surface becomes large, as is clear from the examples, and the inner circumferential surface The magnetic properties of the material are significantly improved.
第1図はこの発明による断面弓形異方性フイラ
イト磁石の表面磁束分布図であり、同図AはX方
向、同図BはY方向の場合を示す。第2図は断面
弓形磁石の斜視図である。第3図は従来の断面弓
形異方性フイライト磁石の内周面の表面磁束分布
図であり、同図AはX方向、同図BはY方向の場
合を示す。
FIG. 1 is a surface magnetic flux distribution diagram of a fluorite magnet having an anisotropic arcuate cross section according to the present invention, in which A shows the case in the X direction and B shows the case in the Y direction. FIG. 2 is a perspective view of a cross-section arcuate magnet. FIG. 3 is a surface magnetic flux distribution diagram of the inner circumferential surface of a conventional anisotropic fluorite magnet having an arcuate cross section, where A shows the case in the X direction and FIG. 3 B shows the case in the Y direction.
Claims (1)
し、円弧内周面が強磁性面でかつ外周面が弱磁性
面からなる異方性フエライト磁石において、 表面磁束分布図における円弧内周面の周方向の
表面磁束分布特性の最高値部分が該分布の中央部
で凸状を形成する特性を有し、 円弧外周面の周方向の表面磁束分布特性が該分
布の中央部で凹状を形成する特性を有することを
特徴とする異方性フエライト磁石。[Scope of Claims] 1. In an anisotropic ferrite magnet having an arcuate cross section and anisotropy in the radial direction of the arcuate surface, the inner peripheral surface of the arc is a ferromagnetic surface and the outer peripheral surface is a weakly magnetic surface, the surface magnetic flux In the distribution diagram, the highest value part of the surface magnetic flux distribution characteristic in the circumferential direction of the inner circumferential surface of the arc has the characteristic of forming a convex shape at the center of the distribution, and the surface magnetic flux distribution characteristic in the circumferential direction of the outer circumferential surface of the arc has the characteristic of forming a convex shape at the center of the distribution. An anisotropic ferrite magnet characterized by having a characteristic of forming a concave shape in the central part.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18613484A JPS6163005A (en) | 1984-09-04 | 1984-09-04 | Anisotropy ferrite magnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18613484A JPS6163005A (en) | 1984-09-04 | 1984-09-04 | Anisotropy ferrite magnet |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6163005A JPS6163005A (en) | 1986-04-01 |
| JPH0332892B2 true JPH0332892B2 (en) | 1991-05-15 |
Family
ID=16182963
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18613484A Granted JPS6163005A (en) | 1984-09-04 | 1984-09-04 | Anisotropy ferrite magnet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6163005A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2009078337A (en) * | 2007-09-27 | 2009-04-16 | Kurimoto Ltd | Tubular body boring device and tubular body boring method |
-
1984
- 1984-09-04 JP JP18613484A patent/JPS6163005A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6163005A (en) | 1986-04-01 |
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