JPH07201558A - Dry-molded ferrite magnet, its manufacture, and dry-molding device - Google Patents

Dry-molded ferrite magnet, its manufacture, and dry-molding device

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Publication number
JPH07201558A
JPH07201558A JP35368193A JP35368193A JPH07201558A JP H07201558 A JPH07201558 A JP H07201558A JP 35368193 A JP35368193 A JP 35368193A JP 35368193 A JP35368193 A JP 35368193A JP H07201558 A JPH07201558 A JP H07201558A
Authority
JP
Japan
Prior art keywords
dry
magnetic
peripheral surface
molding
distribution curve
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
JP35368193A
Other languages
Japanese (ja)
Other versions
JP2777693B2 (en
Inventor
Taketoshi Miyauchi
武寿 宮内
Kazuhiro Suzuki
一弘 鈴木
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.)
TDK Corp
Original Assignee
TDK Corp
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Abstract

PURPOSE:To prevent a ferrite magnet from being disturbed in orientation at its both ends by a method wherein an angle which a straight line connected between two optional points located on a Bd distribution curve makes with an X axis is specified, and a relation between the maximum and the minimum of Bd in an evaluation region and an area surrounded by a Bd distribution curve and an X axis are specified. CONSTITUTION:The length of a measurement region is indicated on an X-axis, Bd is indicated on a Y-axis, and a pattern of Bd distribution is plotted so as to draw a Bd distribution curve graph. The maximum value Bdm of Bd on a Y-axis on its inner peripheral surface is set to 60% of a length AB of a measurement region on an X axis. Provided that a center part of the measurement region that amounts to 60% of it is defined as an evaluation region, an angle of theta which a straight line connected between two optional points located on a Bd distribution curve makes with an X axis is set smaller than 45 deg.. A relation between the maximum and minimum value, alpha and beta, of Bd in the evaluation region of a Bd distribution curve graph, an area Bdi surrounded by the inner peripheral face of a Bd distribution curve and an X axis and an area Bdo surrounded with the outer peripheral face of a Bd distribution curve and an X axis are so as to satisfy formulas, I and II.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、乾式成形法を用いて製
造され、径方向に異方性を有する円弧状フェライト磁石
およびその製造方法と、前記乾式成形法に用いる成形装
置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an arc-shaped ferrite magnet manufactured by a dry molding method and having radial anisotropy, a manufacturing method thereof, and a molding apparatus used in the dry molding method.

【0002】[0002]

【従来の技術】家電製品や自動車の電装用などに用いら
れるモータには、高性能、かつ小型、軽量であることが
求められている。このようなモータは直流モータであ
り、磁石には、乾式成形による異方性円弧状フェライト
磁石や、乾式成形による異方性リング磁石が用いられて
いる。これらのモータ用磁石は径方向が磁化容易軸とな
るように異方性化されている。これらの磁石には、内周
面側の表面磁束密度が強く、しかも、内周面側の表面磁
束密度が周方向において均一であることが要求される。
内周面の周方向において表面磁束密度の変動が大きいと
コギングが生じ、良好なモータ特性が得られない。
2. Description of the Related Art Motors used for home appliances and electric components of automobiles are required to have high performance, small size and light weight. Such a motor is a DC motor, and an anisotropic arc-shaped ferrite magnet formed by dry molding or an anisotropic ring magnet formed by dry molding is used as the magnet. These motor magnets are anisotropy so that the easy axis is in the radial direction. These magnets are required to have a strong surface magnetic flux density on the inner peripheral surface side and have a uniform surface magnetic flux density on the inner peripheral surface side in the circumferential direction.
If the fluctuation of the surface magnetic flux density is large in the circumferential direction of the inner peripheral surface, cogging will occur and good motor characteristics cannot be obtained.

【0003】異方性円弧状フェライト磁石は、乾式成形
または湿式成形を用いて製造される。湿式成形は、配向
性は良好であるが、製造コストが高くなる。一方、乾式
成形では、円弧状磁石の両端部において配向が乱れやす
く、良好なモータ特性が得られにくい。
Anisotropic arc-shaped ferrite magnets are manufactured using dry molding or wet molding. Wet molding has good orientation, but increases manufacturing costs. On the other hand, in dry molding, the orientation tends to be disturbed at both ends of the arcuate magnet, and it is difficult to obtain good motor characteristics.

【0004】特公平2−12726号公報には、凹状湾
曲面を有する上パンチと凸状湾曲面を有する下パンチに
より圧縮成形する装置において、上パンチの成形空間側
表面に断面弓形状の非磁性体を嵌着して設けるととも
に、この非磁性体部分の厚みを非磁性体の外周面円弧中
心点と内周面円弧中心点を偏心させ、中央部を厚くした
ものが記載されている。同公報では、この成形装置を用
いることにより磁石内周面の磁気特性を大幅に向上させ
ることができるとしている。この成形装置は湿式成形用
である。また、特公平2−13452号公報にも、断面
弓形状の非磁性体を設けた成形装置が記載されている
が、この成形装置も湿式成形用である。
Japanese Examined Patent Publication No. 12726/1990 discloses an apparatus for compression molding with an upper punch having a concave curved surface and a lower punch having a convex curved surface, and a non-magnetic material having an arcuate cross section on the molding space side surface of the upper punch. It is described that the body is fitted and provided, and the thickness of the non-magnetic body portion is made eccentric between the center point of the outer circumferential surface arc and the center point of the inner circumferential surface arc of the non-magnetic material to thicken the central portion. According to the publication, the magnetic characteristics of the inner peripheral surface of the magnet can be significantly improved by using this molding device. This molding apparatus is for wet molding. Further, Japanese Patent Publication No. 2-13452 describes a molding device provided with a non-magnetic material having a bow-shaped cross section, but this molding device is also for wet molding.

【0005】[0005]

【発明が解決しようとする課題】本発明はこのような事
情からなされたものであり、径方向の異方性を有する円
弧状フェライト磁石を乾式成形を用いて製造する際に、
磁石両端部での配向の乱れを防ぐことを目的とする。
SUMMARY OF THE INVENTION The present invention has been made under the circumstances as described above, and when an arc-shaped ferrite magnet having radial anisotropy is manufactured by dry molding,
The purpose is to prevent orientation disorder at both ends of the magnet.

【0006】[0006]

【課題を解決するための手段】このような目的は、下記
(1)〜(6)の本発明により達成される。 (1)断面が円弧状であり、その径方向に異方性を有す
る弓形の乾式成形フェライト磁石であって、横軸を測定
領域長(周面の周方向長さ)、縦軸をBd(表面磁束密
度)としたBd分布グラフにおいて、縦軸のBdの最大
値が横軸の測定領域長(内周面の周方向長さ)の60%
となるように内周面のBd分布曲線をプロットし、測定
領域中央部60%を評価領域としたとき、前記評価領域
内において、Bd分布曲線上の任意の2点を通る直線と
横軸とのなす角度θが45°以下であり、前記評価領域
内において、Bdの最大値αとBdの最小値βとの関係
が (α−β)/α≦0.2 であり、前記Bd分布グラフにおいて、内周面のBd分
布曲線と横軸とが囲む面積をBdiとし、外周面のBd
分布曲線と横軸とが囲む面積をBdoとしたとき、 Bdi/Bdo=1.4〜1.9 であることを特徴とする乾式成形フェライト磁石。 (2)角度θが42°以下であり、 (α−β)/α≦0.18 であり、 Bdi/Bdo=1.5〜1.9 である上記(1)の乾式成形フェライト磁石。 (3)断面が円弧状の成形空間内にフェライト磁石の原
料粉末を充填して、磁場中で乾式成形することにより弓
形成形体を形成するための成形装置であって、それぞれ
少なくとも一部が強磁性体から構成される上型および下
型、非磁性体から構成される型枠、ならびに2個の配向
用強磁性体を有し、前記成形空間の凸状面が下側となる
ように、上型、下型および型枠により前記成形空間が形
成されており、成形空間の径方向に磁界を印加するため
の磁界印加手段を有し、2個の配向用強磁性体が、前記
成形空間の周方向の両側にそれぞれ型枠を介して設けら
れており、加圧開始時の下型の上端と、各配向用強磁性
体の上端とがほぼ一致することを特徴とする乾式成形装
置。 (4)前記下型が、成形空間に面する下部非磁性体を、
強磁性体から構成される下パンチの上側に設けたもので
ある上記(3)の乾式成形装置。 (5)前記上型が、成形空間に面する上部非磁性体を、
強磁性体から構成される上パンチの下側に設けたもので
ある上記(4)の乾式成形装置。 (6)上記(3)〜(5)のいずれかの乾式成形装置を
用いて上記(1)または(2)の乾式成形フェライト磁
石を製造することを特徴とする乾式成形フェライト磁石
の製造方法。
The above objects are achieved by the present invention described in (1) to (6) below. (1) A bow-shaped dry-molded ferrite magnet having an arc-shaped cross section and having anisotropy in its radial direction, in which the horizontal axis represents the measurement region length (circumferential length of the peripheral surface) and the vertical axis represents Bd ( In the Bd distribution graph of (surface magnetic flux density), the maximum value of Bd on the vertical axis is 60% of the measurement area length (circumferential length of the inner peripheral surface) on the horizontal axis.
When the Bd distribution curve of the inner peripheral surface is plotted so that 60% of the central portion of the measurement area is used as the evaluation area, a straight line passing through any two points on the Bd distribution curve and the horizontal axis in the evaluation area. Is less than or equal to 45 °, and the relationship between the maximum value α of Bd and the minimum value β of Bd is (α−β) /α≦0.2 in the evaluation region, and the Bd distribution graph In B, the area enclosed by the Bd distribution curve on the inner peripheral surface and the horizontal axis is defined as Bdi, and Bd on the outer peripheral surface is
When the area surrounded by the distribution curve and the horizontal axis is Bdo, Bdi / Bdo = 1.4 to 1.9. (2) The dry-molded ferrite magnet according to (1) above, wherein the angle θ is 42 ° or less, (α−β) /α≦0.18, and Bdi / Bdo = 1.5 to 1.9. (3) A molding device for forming a bow-shaped body by filling raw material powder of a ferrite magnet into a molding space having an arcuate cross section and performing dry molding in a magnetic field. An upper mold and a lower mold made of a magnetic material, a mold made of a non-magnetic material, and two orientation ferromagnetic materials, so that the convex surface of the molding space is on the lower side, The molding space is formed by an upper mold, a lower mold, and a mold, and has magnetic field applying means for applying a magnetic field in the radial direction of the molding space, and two orientation ferromagnetic bodies are provided in the molding space. A dry molding apparatus, which is provided on both sides in the circumferential direction of the mold through a mold, and the upper end of the lower mold at the start of pressurization and the upper end of each of the orientation ferromagnetic bodies are substantially aligned with each other. (4) The lower mold has a lower non-magnetic body facing the molding space,
The dry molding apparatus according to the above (3), which is provided on the upper side of the lower punch made of a ferromagnetic material. (5) The upper mold has an upper non-magnetic body facing the molding space,
The dry molding apparatus according to (4) above, which is provided below the upper punch made of a ferromagnetic material. (6) A method for manufacturing a dry-molded ferrite magnet, comprising manufacturing the dry-molded ferrite magnet according to (1) or (2) using the dry-molding apparatus according to any one of (3) to (5).

【0007】[0007]

【作用および効果】本発明では、上記のような配向用強
磁性体を設けた乾式成形装置を用いることにより、異方
性方向が径方向に揃った成形体が得られる。このため、
表面磁束密度分布曲線からわかるように、内周面側の表
面磁束密度が大きくかつその分布が均一な円弧状フェラ
イト磁石が得られる。したがって、本発明の磁石を用い
たモータは、強力であり、しかもコギングトルクが小さ
い。また、従来、磁石両端部での配向の乱れを原因とし
て、焼結時に内周面の両端部付近にクラックが多発して
いたが、本発明では磁石両端部での配向の乱れが著しく
少なくなるため、このようなクラックが激減する。
FUNCTION AND EFFECT According to the present invention, by using the dry molding apparatus provided with the above-mentioned ferromagnetic material for orientation, a molded article in which the anisotropic directions are aligned in the radial direction can be obtained. For this reason,
As can be seen from the surface magnetic flux density distribution curve, an arc-shaped ferrite magnet having a large surface magnetic flux density on the inner peripheral surface side and a uniform distribution can be obtained. Therefore, the motor using the magnet of the present invention is powerful and has a small cogging torque. Further, conventionally, cracks frequently occurred near both ends of the inner peripheral surface during sintering due to the disorder of the orientation at both ends of the magnet, but in the present invention, the disorder of the orientation at both ends of the magnet is significantly reduced. Therefore, such cracks are drastically reduced.

【0008】ところで、特公平3−32892号公報に
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
性フェライト磁石が記載されている。同公報の第1図
(A)には、周方向に測定した内周面および外周面の表
面磁束分布図が記載されている。しかし、この表面磁束
分布図について本発明と同様な測定を行なうと、角度θ
は約58°、(α−β)/αが約0.16、Bdi/B
doが約1.73であり、角度θが本発明範囲を外れて
いる。しかも、同公報には湿式成形についての記述しか
みられず、乾式成形に関する記述はない。
By the way, in Japanese Patent Publication No. 3-32892, there is a difference in that the arcuate cross-section has anisotropy in the radial direction of the arc surface, and the arc inner peripheral surface is a ferromagnetic surface and the outer peripheral surface is a weak magnetic surface. An isotropic ferrite magnet is described. FIG. 1 (A) of the publication discloses a surface magnetic flux distribution diagram of the inner peripheral surface and the outer peripheral surface measured in the circumferential direction. However, when the same measurement as the present invention is performed on this surface magnetic flux distribution diagram, the angle θ
Is about 58 °, (α-β) / α is about 0.16, Bdi / B
The do is about 1.73, and the angle θ is out of the range of the present invention. Moreover, only the description of wet molding is found in the publication, and there is no description of dry molding.

【0009】また、実開昭57−10729号公報に
は、断面が弧状の異方性フェライト磁石の成形用磁気回
路が開示されている。この成形用磁気回路は、ダイス
(型枠)の一部に強磁性体を設けたものであるが、強磁
性体と下パンチとの位置関係が本発明の乾式成形装置と
は異なる。実際、同公報第1図(b)に示される表面磁
束分布図について本発明と同様な測定を行なうと、角度
θが約47°、(α−β)/αが約0.22、Bdi/
Bdoが約1.48であり、角度θおよび(α−β)/
αが本発明範囲を外れている。
Further, Japanese Utility Model Laid-Open No. 57-10729 discloses a magnetic circuit for forming an anisotropic ferrite magnet having an arc-shaped cross section. In this magnetic circuit for molding, a ferromagnetic material is provided in a part of a die (form), but the positional relationship between the ferromagnetic material and the lower punch is different from that of the dry molding apparatus of the present invention. Actually, when the same measurement as in the present invention is performed on the surface magnetic flux distribution diagram shown in FIG. 1 (b) of the publication, the angle θ is about 47 °, (α−β) / α is about 0.22, and Bdi /
Bdo is about 1.48 and the angle θ and (α-β) /
α is outside the range of the present invention.

【0010】すなわち、角度θ、(α−β)/αおよび
Bdi/Bdoのすべてを満足する乾式成形フェライト
磁石は、従来、知られていない。
That is, a dry-molded ferrite magnet satisfying all of the angles θ, (α-β) / α and Bdi / Bdo has not been heretofore known.

【0011】[0011]

【具体的構成】以下、本発明の具体的構成を説明する。[Specific Configuration] The specific configuration of the present invention will be described below.

【0012】本発明の磁石は、断面が円弧状であり、そ
の径方向に異方性を有する弓形の乾式成形フェライト磁
石であり、いわゆる異方性セグメント磁石と称されるも
のである。本発明の磁石は、乾式成形法を用いて製造さ
れる。
The magnet of the present invention is an arc-shaped dry-molded ferrite magnet having an arc-shaped cross section and having anisotropy in its radial direction, and is a so-called anisotropic segment magnet. The magnet of the present invention is manufactured using a dry molding method.

【0013】本発明の磁石は、内周面の周方向にわたっ
て測定したBd(表面磁束密度)分布に特徴を有し、ま
た、内周面の前記Bd分布と、外周面の周方向にわたっ
て測定したBd分布との関係にも特徴を有する。外周面
および内周面の周方向のBd分布は、図2および図3に
示す手順で測定する。まず、非磁性のケースに組み込ん
だ磁石を、図2に示す内面着磁ヨークを使用して内面フ
ル着磁する。Bd測定に際しては、着磁した磁石の周面
付近にホール素子を配置する。このときのホール素子
は、周面の高さ方向(図3の上下方向)中央部に位置さ
せて、周面に接触させるか、できるだけ接近させて配置
する。そして、磁石を周方向に回転させることにより、
周面の周方向の一端Aから他端BにかけてのBd分布を
測定することができる。なお、磁石の回転は、ホール素
子と周面との距離が変動しないように行なう。
The magnet of the present invention is characterized by the Bd (surface magnetic flux density) distribution measured in the circumferential direction of the inner peripheral surface, and the Bd distribution of the inner peripheral surface and the circumferential direction of the outer peripheral surface. It also has a characteristic in relation to the Bd distribution. The circumferential Bd distributions of the outer peripheral surface and the inner peripheral surface are measured by the procedure shown in FIGS. 2 and 3. First, the magnet incorporated in the non-magnetic case is fully magnetized on the inner surface using the inner surface magnetizing yoke shown in FIG. When measuring Bd, a Hall element is arranged near the peripheral surface of the magnetized magnet. At this time, the Hall element is positioned at the center of the circumferential surface in the height direction (vertical direction in FIG. 3) and is brought into contact with the circumferential surface or as close as possible. Then, by rotating the magnet in the circumferential direction,
The Bd distribution can be measured from one end A to the other end B in the circumferential direction of the circumferential surface. The magnet is rotated so that the distance between the Hall element and the peripheral surface does not change.

【0014】このようにして測定されたBd分布を、横
軸を測定領域長(周面の周方向長さ)、縦軸をBdとし
たBd分布グラフにプロットし、図1に示すようなBd
分布曲線グラフとする。図1において、縦軸の内周面の
Bdの最大値Bdmは、横軸の測定領域長AB(図3に
おいて、内周面に沿って測ったAB間距離)の60%で
ある。そして、測定領域中央部60%を評価領域とした
とき、この評価領域内において、Bd分布曲線上の任意
の2点を通る直線と横軸とのなす角度θ(その最大値
は、領域内でのBd分布曲線の接線の傾きの最大値とな
る。)は、45°以下、好ましくは42°以下、より好
ましくは35°以下である。θが大きすぎると、磁石を
モータに適用したときにコギングトルクが大きくなって
しまう。
The Bd distribution thus measured is plotted on a Bd distribution graph in which the horizontal axis is the measurement region length (circumferential length of the peripheral surface) and the vertical axis is Bd.
Use a distribution curve graph. In FIG. 1, the maximum value Bdm of Bd on the inner circumferential surface on the vertical axis is 60% of the measurement area length AB on the horizontal axis (the AB distance measured along the inner circumferential surface in FIG. 3). When the central portion of the measurement area is 60%, the angle θ formed by the straight line passing through any two points on the Bd distribution curve and the horizontal axis in the evaluation area (the maximum value is within the area) The maximum value of the tangent slope of the Bd distribution curve is 45 ° or less, preferably 42 ° or less, and more preferably 35 ° or less. If θ is too large, the cogging torque will increase when the magnet is applied to the motor.

【0015】本発明では、図1のBd分布グラフの評価
領域内において、Bdの最大値αとBdの最小値βとの
関係が、 (α−β)/α≦0.2、 好ましくは (α−β)/α≦0.18、 より好ましくは (α−β)/α≦0.15 である。(α−β)/αが大きすぎると、磁石をモータ
に適用したときにトルク変動が大きくなってしまう。
In the present invention, the relation between the maximum value α of Bd and the minimum value β of Bd in the evaluation area of the Bd distribution graph of FIG. 1 is (α−β) /α≦0.2, preferably ( α-β) /α≦0.18, more preferably (α-β) /α≦0.15. If (α-β) / α is too large, the torque fluctuation will be large when the magnet is applied to the motor.

【0016】本発明では、Bd分布グラフにおいて、内
周面のBd分布曲線と横軸とが囲む面積をBdiとし、
外周面のBd分布曲線と横軸とが囲む面積をBdoとし
たとき、 Bdi/Bdo=1.4〜1.9、 好ましくは Bdi/Bdo=1.5〜1.9、 より好ましくは Bdi/Bdo=1.7〜1.9 である。Bdi/Bdoが小さすぎる磁石は内周面側の
磁気特性が不足する。一方、1.9を超えるBdi/B
doを得ようとすると、成形体の内周面と外周面とで密
度差を著しく大きくしなければならない。このため、焼
成時にクラックが多発し、成形が不可能となることもあ
る。
In the present invention, in the Bd distribution graph, the area surrounded by the Bd distribution curve on the inner peripheral surface and the horizontal axis is defined as Bdi,
When the area enclosed by the Bd distribution curve on the outer peripheral surface and the horizontal axis is Bdo, Bdi / Bdo = 1.4 to 1.9, preferably Bdi / Bdo = 1.5 to 1.9, and more preferably Bdi / Bdo = 1.7 to 1.9. A magnet having too small Bdi / Bdo has insufficient magnetic properties on the inner peripheral surface side. On the other hand, Bdi / B exceeding 1.9
In order to obtain do, the difference in density between the inner peripheral surface and the outer peripheral surface of the molded body must be significantly increased. For this reason, cracks frequently occur during firing, which may make molding impossible.

【0017】上述したBd分布に特徴を有する有する磁
石を、乾式成形法を用いて製造するためには、以下に説
明する本発明の乾式成形装置を用いることが好ましい。
In order to manufacture the above-mentioned magnet having a characteristic of Bd distribution by the dry molding method, it is preferable to use the dry molding apparatus of the present invention described below.

【0018】本発明の成形装置は、断面が円弧状の成形
空間内にフェライト磁石の原料粉末を充填して、磁場中
で乾式成形することにより弓形成形体を形成するための
ものである。本発明の成形装置は、それぞれ少なくとも
一部が強磁性体から構成される上型および下型、非磁性
体から構成される型枠、ならびに2個の配向用強磁性体
を有する。そして、上型、下型および型枠により成形空
間が形成されており、成形空間の凸状面は下側に存在す
る。
The forming apparatus of the present invention is for forming an arc-formed body by filling a raw material powder of a ferrite magnet into a forming space having an arcuate section and performing dry forming in a magnetic field. The molding apparatus of the present invention has an upper mold and a lower mold each of which at least a part is made of a ferromagnetic material, a mold made of a nonmagnetic material, and two orienting ferromagnetic materials. A molding space is formed by the upper mold, the lower mold, and the mold, and the convex surface of the molding space exists on the lower side.

【0019】図4に本発明の乾式成形装置の好ましい構
成例を示す。図4(a)に示す乾式成形装置は、上部パ
ンチ1、下部パンチ2、型枠3、上部非磁性体4、下部
非磁性体5および2個の配向用強磁性体61、62を有
し、さらに、成形空間7の径方向に磁界を印加するため
のコイル8を有する。この成形装置では、上部パンチ1
と上部非磁性体4とが上型を構成し、下部パンチ2と下
部非磁性体5とが下型を構成する。成形空間7は、その
凸状面が下側となるように、上部非磁性体4、下部非磁
性体5および型枠3により包囲されている。配向用強磁
性体61、62は、成形空間7の周方向の両側にそれぞ
れ型枠3を介して設けられている。なお、図4(a)
は、成形空間7の円弧状断面が現われる断面図であり、
図4(b)は、上部パンチ1を取り去ったときの成形装
置の上面図である。
FIG. 4 shows a preferred configuration example of the dry molding apparatus of the present invention. The dry molding apparatus shown in FIG. 4A has an upper punch 1, a lower punch 2, a mold 3, an upper non-magnetic body 4, a lower non-magnetic body 5 and two orienting ferromagnetic bodies 61, 62. Further, it has a coil 8 for applying a magnetic field in the radial direction of the molding space 7. In this molding machine, the upper punch 1
And the upper non-magnetic body 4 compose the upper die, and the lower punch 2 and the lower non-magnetic body 5 compose the lower die. The molding space 7 is surrounded by the upper non-magnetic body 4, the lower non-magnetic body 5 and the mold 3 such that the convex surface thereof faces downward. The orientation ferromagnetic bodies 61 and 62 are provided on both sides of the molding space 7 in the circumferential direction, with the mold 3 interposed therebetween. Note that FIG.
Is a sectional view showing an arcuate section of the molding space 7,
FIG. 4B is a top view of the molding apparatus when the upper punch 1 is removed.

【0020】このような成形装置では、以下のようにし
て成形が行なわれる。まず、上部パンチ型枠から上げた
状態で、型枠内に原料粉末を充填する。原料粉末は、通
常、型枠上面まで充填する。原料粉末充填後、上部パン
チを下降させることにより、成形空間を形成して原料粉
末を加圧成形する。すなわち、加圧時に下部パンチは移
動しない。加圧成形終了後、上部パンチを上昇させ、さ
らに下部パンチを上昇させて、型枠から成形体を取り出
す。その後、下部パンチを下降させて、原料粉末の充填
に備える。このような成形装置において、原料粉末の充
填深さとは、型枠上面から測定した成形空間最低位置の
深さである。
In such a molding apparatus, molding is performed as follows. First, the raw material powder is filled in the mold while being lifted from the upper punch mold. The raw material powder is usually filled up to the upper surface of the mold. After filling the raw material powder, the upper punch is lowered to form a molding space and press-mold the raw material powder. That is, the lower punch does not move during pressurization. After the pressure molding is completed, the upper punch is raised and the lower punch is further raised to take out the compact from the mold. Then, the lower punch is lowered to prepare for filling the raw material powder. In such a molding apparatus, the filling depth of the raw material powder is the depth at the lowest position of the molding space measured from the upper surface of the mold.

【0021】配向用強磁性体61、62は、その上端が
加圧開始時(原料粉末充填時)の下型の上端(図4では
下部非磁性体4の上端)とほぼ一致するように、好まし
くは、配向用強磁性体の上端と下型の上端とのずれ量
が、成形空間最大高さの30%以下となるように配置さ
れる。配向用強磁性体が成形空間7に対して前記範囲よ
り上側に位置していると、原料粉末の充填が困難とな
る。これは、原料粉末充填時にも配向磁界が印加されて
おり、この磁界によって原料粉末が型枠内に吸引される
ようにして充填が行なわれるため、配向用強磁性体が前
記範囲より上側であると、このような吸引作用が困難と
なるからである。一方、この範囲より下側に位置してい
ると、配向用強磁性体を設けたことによる効果が十分に
実現しなくなる。
The orientation ferromagnetic materials 61, 62 have their upper ends substantially aligned with the upper end of the lower die (the upper end of the lower non-magnetic member 4 in FIG. 4) at the start of pressing (when the raw material powder is filled). Preferably, it is arranged such that the amount of deviation between the upper end of the orientation ferromagnetic material and the upper end of the lower mold is 30% or less of the maximum height of the molding space. If the orientation ferromagnetic material is located above the range with respect to the molding space 7, it becomes difficult to fill the raw material powder. This is because the orientation magnetic field is applied even when the raw material powder is filled, and the raw material powder is attracted into the mold by the magnetic field to perform the filling, so that the orientation ferromagnetic material is above the range. Then, such a suction action becomes difficult. On the other hand, if it is located below this range, the effect of providing the orientation ferromagnetic material cannot be sufficiently realized.

【0022】配向用強磁性体61、62は、通常、図4
に示すように直方体状とされる。配向用強磁性体の寸法
は、以下の範囲であることが好ましい。まず、図4に示
す断面において、直方体状の配向用強磁性体61、62
の高さをh、幅をwとし、奥行をdとする。
The orienting ferromagnetic materials 61 and 62 are usually formed in the structure shown in FIG.
It has a rectangular parallelepiped shape as shown in. The dimension of the orientation ferromagnetic material is preferably in the following range. First, in the cross section shown in FIG. 4, rectangular parallelepiped orientation ferromagnetic bodies 61, 62 are formed.
Let h be the height, w be the width, and d be the depth.

【0023】hは充填深さと同等であることが好まし
く、具体的には、充填深さをHとしたとき、 0.5≦h/H であることが好ましい。h/Hが小さすぎると、配向用
強磁性体を設けたことによる効果が十分に実現しなくな
る。なお、h/Hを大きくしても、配向用強磁性体の位
置が適切であれば悪影響は殆どないが、h/Hが1.5
を超える大きさとしても効果は大きくならない。
It is preferable that h is equal to the filling depth. Specifically, when the filling depth is H, 0.5 ≦ h / H is preferable. If h / H is too small, the effect of providing the orientation ferromagnetic material cannot be sufficiently realized. Note that even if h / H is increased, there is almost no adverse effect if the position of the orientation ferromagnetic material is appropriate, but h / H is 1.5.
Even if the size exceeds, the effect does not increase.

【0024】また、図4に示す断面における成形空間7
の幅をWとしたとき w/W≧0.3 であることが好ましい。w/Wが小さすぎると、配向用
強磁性体を設けたことによる効果が十分に実現しなくな
る。なお、w/Wの上限は特になく、配向用強磁性体が
型枠内に収まる寸法とすればよいが、通常、w/Wは
1.5以下である。
Further, the molding space 7 in the cross section shown in FIG.
It is preferable that w / W ≧ 0.3 when the width of W is W. If w / W is too small, the effect of providing the orientation ferromagnetic material cannot be sufficiently realized. There is no particular upper limit on w / W, and the dimension may be such that the orientation ferromagnetic material fits in the mold, but usually w / W is 1.5 or less.

【0025】また、図4に示す成形空間7の奥行をDと
したとき、dは、Dと同等かやや大きいことが好まし
く、具体的には、 0.7≦d/D≦1.3 であることが好ましい。d/Dが小さすぎると、配向用
強磁性体を設けたことによる効果が十分に実現しなくな
る。一方、d/Dが大きすぎると、成形空間の四隅付近
で配向が乱れやすくなる。
Further, when the depth of the molding space 7 shown in FIG. 4 is D, d is preferably equal to or slightly larger than D. Specifically, 0.7 ≦ d / D ≦ 1.3 Preferably there is. If d / D is too small, the effect of providing the orientation ferromagnetic material cannot be sufficiently realized. On the other hand, if d / D is too large, the orientation tends to be disturbed near the four corners of the molding space.

【0026】配向用強磁性体と成形空間との距離、すな
わち、両者間に介在する型枠の厚さは、成形の際の破損
を避け、かつ配向用強磁性の効果への影響を抑えるため
に、通常、2〜10mm程度の厚さとされる。
The distance between the orientation ferromagnetic material and the molding space, that is, the thickness of the mold interposed therebetween, is to prevent damage during molding and to suppress the influence on the effect of the orientation ferromagnetic material. The thickness is usually about 2 to 10 mm.

【0027】下部非磁性体5は、図示の断面において中
央部が両端部よりも厚いことが好ましい。下部非磁性体
5の断面形状をこのようにすることにより、成形体端部
付近の配向がより中央を向いて径方向の配向度が良好と
なり、磁気特性が向上する。また、磁性体から構成され
る下部パンチ2と原料粉末との間に透磁率の低い非磁性
体が存在することになるので、急激な磁束変化が避けら
れ、焼成時の割れ発生が防止されて歩留りが向上する。
It is preferable that the lower non-magnetic member 5 has a central portion thicker than both end portions in the illustrated cross section. By setting the cross-sectional shape of the lower non-magnetic body 5 in this way, the orientation near the end of the molded body is more toward the center, the degree of radial orientation is improved, and the magnetic characteristics are improved. In addition, since a non-magnetic material having a low magnetic permeability exists between the lower punch 2 made of a magnetic material and the raw material powder, abrupt magnetic flux changes are avoided and cracking during firing is prevented. Yield is improved.

【0028】上部非磁性体4は、図示の断面において中
央部が両端部よりも薄いことが好ましい。上部非磁性体
4の断面形状をこのようにすることにより、成形体端部
付近の配向がより中央を向いて径方向の配向度が良好と
なり、磁気特性が向上する。また、磁性体から構成され
る上部パンチ1と原料粉末との間に透磁率の低い非磁性
体が存在することになるので、急激な磁束変化が避けら
れ、焼成時の割れ発生が防止されて歩留りが向上する。
It is preferable that the central portion of the upper non-magnetic member 4 is thinner than both end portions in the illustrated cross section. By setting the cross-sectional shape of the upper non-magnetic body 4 in this way, the orientation near the end of the molded body is more toward the center, the degree of radial orientation is improved, and the magnetic characteristics are improved. Further, since a non-magnetic material having a low magnetic permeability exists between the upper punch 1 made of a magnetic material and the raw material powder, abrupt magnetic flux change is avoided and cracking during firing is prevented. Yield is improved.

【0029】下部非磁性体5を、中央部が両端部よりも
厚くする場合、図示例のように中央部付近に平坦部を設
け、中央部が厚くなりすぎるのを防ぐ構成とすることが
好ましいが、下部非磁性体5の断面形状を、上縁と下縁
がそれぞれ円弧状であってこれらが偏心しているもの、
あるいは上縁と下縁とで曲率半径が異なるように構成し
てもよい。上部非磁性体4についても、同様である。
When the central portion of the lower non-magnetic member 5 is thicker than both end portions thereof, it is preferable that a flat portion is provided in the vicinity of the central portion to prevent the central portion from becoming too thick as shown in the figure. However, the cross-sectional shape of the lower non-magnetic member 5 is such that the upper edge and the lower edge are arcuate and are eccentric.
Alternatively, the upper edge and the lower edge may have different radii of curvature. The same applies to the upper non-magnetic body 4.

【0030】なお、上部非磁性体4および下部非磁性体
5は必須ではないが、より良好な配向性を得るためには
少なくとも下部非磁性体5を設けることが好ましく、さ
らに上部非磁性体4を設ければ、配向性はいっそう向上
する。また、これらの非磁性体を設けることにより、上
部パンチおよび下部パンチの寿命も長くなる。
Although the upper non-magnetic material 4 and the lower non-magnetic material 5 are not essential, it is preferable to provide at least the lower non-magnetic material 5 in order to obtain better orientation, and the upper non-magnetic material 4 is further provided. By providing, the orientation is further improved. Further, the life of the upper punch and the lower punch is extended by providing these non-magnetic materials.

【0031】下部非磁性体や上部非磁性体の構成材料は
特に限定されず、通常、非磁性ステンレス鋼や非磁性ス
テライトなどから適宜選択される。また、上部パンチ、
下部パンチ、配向用強磁性体は、S45C等の磁性材料
から構成すればよい。型枠は非磁性超硬材等から構成す
ればよい。
The constituent material of the lower non-magnetic material and the upper non-magnetic material is not particularly limited, and is usually appropriately selected from non-magnetic stainless steel and non-magnetic stellite. Also, the upper punch,
The lower punch and the ferromagnetic material for orientation may be made of a magnetic material such as S45C. The mold may be made of non-magnetic cemented carbide or the like.

【0032】成形条件は特に限定されず、成形時の圧力
や磁場強度などの各種条件は、通常の乾式成形法と同様
であってよい。
The molding conditions are not particularly limited, and various conditions such as pressure and magnetic field strength at the time of molding may be the same as those in the normal dry molding method.

【0033】本発明の乾式成形装置は、通常、厚さ(内
周面と外周面との距離)が3〜15mm程度の円弧状磁石
の製造に用いられる。
The dry molding apparatus of the present invention is usually used for manufacturing an arc-shaped magnet having a thickness (a distance between the inner peripheral surface and the outer peripheral surface) of about 3 to 15 mm.

【0034】[0034]

【実施例】以下、本発明の具体的実施例を示し、本発明
をさらに詳細に説明する。
EXAMPLES The present invention will be described in more detail below by showing specific examples of the present invention.

【0035】<実施例1>図4に示される構成の乾式成
形装置を用いて、フェライト磁石サンプルを作製した。
この成形装置は、 h/H=0.93、 w/W=0.41、 d/D=1.05 であり、いずれも本発明における好ましい範囲内であっ
た。また、各配向用強磁性体と成形空間との距離は、2
mmとした。なお、両配向用強磁性体は、その上端が原料
粉末充填時の下部非磁性体5の上端と一致する高さとな
るように配置した。
Example 1 A ferrite magnet sample was produced using the dry molding apparatus having the structure shown in FIG.
With this molding apparatus, h / H = 0.93, w / W = 0.41, and d / D = 1.05, all of which were within the preferred range of the present invention. Further, the distance between each orientation ferromagnetic material and the molding space is 2
mm. The orientation-oriented ferromagnetic bodies were arranged so that the upper ends thereof were at the same height as the upper ends of the lower non-magnetic bodies 5 at the time of filling the raw material powder.

【0036】この乾式成形装置の成形空間内に、フェラ
イト磁石の原料粉末を充填し、磁場中で加圧成形して、
径方向に異方性を有する円弧状の成形体を得た。次い
で、成形体を焼結し、円弧状の異方性フェライト磁石と
した。磁石の寸法は、外周面の曲率半径が11.8mm、
内周面の曲率半径が8.5mm、径方向を含む断面におけ
る幅が20.4mm、長さ(奥行)が18mmであった。こ
の磁石を本発明サンプルNo. 1−1とする。
The raw material powder of the ferrite magnet is filled in the molding space of this dry molding apparatus and pressure-molded in a magnetic field,
An arcuate shaped body having anisotropy in the radial direction was obtained. Then, the molded body was sintered to obtain an arc-shaped anisotropic ferrite magnet. As for the size of the magnet, the radius of curvature of the outer peripheral surface is 11.8 mm,
The radius of curvature of the inner peripheral surface was 8.5 mm, the width in the cross section including the radial direction was 20.4 mm, and the length (depth) was 18 mm. This magnet is referred to as Sample No. 1-1 of the present invention.

【0037】比較のために、配向用強磁性体を設けない
以外は図4と同様な構成の乾式成形装置を用い、上記本
発明サンプルNo. 1−1と同様にして円弧状フェライト
磁石サンプルを作製した。このサンプルを、比較サンプ
ルNo. 1−2とする。
For comparison, an arc-shaped ferrite magnet sample was prepared in the same manner as Sample No. 1-1 of the present invention, using a dry molding apparatus having the same structure as that shown in FIG. 4 except that the orientation ferromagnetic material was not provided. It was made. This sample is referred to as Comparative Sample No. 1-2.

【0038】これらのサンプルに対して前述した方法に
より内面フル着磁を行なった後、前述した方法により、
Bdを測定した。測定個数は、各サンプルにつき5個と
した。図5に、本発明サンプルNo. 1−1の内周面およ
び外周面のBd分布曲線を示す。ただし、図5のグラフ
は、内周面のBdの最大値が内周面の周方向長さの60
%とはなっていない。Bd測定結果から、前述した方法
により角度θ、(α−β)/αおよびBdi/Bdoを
求めた。この結果、本発明サンプルNo. 1−1では θ=32°、 (α−β)/α=0.14、 Bdi/Bdo=1.8 であり、いずれも本発明範囲内であったが、比較サンプ
ルNo. 1−2では θ=40°、 (α−β)/α=2.3、 Bdi/Bdo=1.2 であり、(α−β)/αとBdi/Bdoとが本発明範
囲を外れていた。すなわち、配向用強磁性体を設けなか
った場合、内周面の絶対的な磁気特性が低下すると共
に、内周面の磁気特性の均一性も低下することがわか
る。
After the inner surfaces of the samples were fully magnetized by the above-mentioned method, the above-mentioned method was performed.
Bd was measured. The number of measurements was 5 for each sample. FIG. 5 shows Bd distribution curves of the inner peripheral surface and the outer peripheral surface of Sample No. 1-1 of the present invention. However, in the graph of FIG. 5, the maximum value of Bd on the inner peripheral surface is 60 which is the circumferential length of the inner peripheral surface.
It is not%. From the Bd measurement results, the angles θ, (α-β) / α and Bdi / Bdo were obtained by the method described above. As a result, in the sample No. 1-1 of the present invention, θ = 32 °, (α-β) /α=0.14, and Bdi / Bdo = 1.8, which were all within the range of the present invention. In Comparative Sample No. 1-2, θ = 40 °, (α−β) /α=2.3, Bdi / Bdo = 1.2, and (α−β) / α and Bdi / Bdo are the present invention. It was out of range. That is, it can be seen that when the ferromagnetic material for orientation is not provided, the absolute magnetic characteristics of the inner peripheral surface deteriorate and the uniformity of the magnetic characteristics of the inner peripheral surface also deteriorates.

【0039】また、配向用強磁性体を設けずに上部非磁
性体の形状および寸法を最適化した乾式成形装置を用い
て磁石を作製したところ、Bdi/Bdoが1.4以上
となって内周面の絶対的な磁気特性は向上したが、角度
θが50°を超えてしまった。
Further, when a magnet was produced using a dry molding apparatus in which the shape and dimensions of the upper non-magnetic material were optimized without providing the orientation ferromagnetic material, Bdi / Bdo was 1.4 or more. Although the absolute magnetic characteristics of the peripheral surface were improved, the angle θ exceeded 50 °.

【0040】次に、サンプルNo. 1−1および1−2に
ついて、トータルフラックスΦを測定した。この結果、
本発明サンプルNo. 1−1ではΦ=7280MXであり、
比較サンプルNo. 1−2に対して+3.7%もの大幅な
向上が認められた。なお、トータルフラックスの3.7
%の増加は、湿式成形法に匹敵するものである。
Next, the total flux Φ was measured for Sample Nos. 1-1 and 1-2. As a result,
In the sample No. 1-1 of the present invention, Φ = 7280MX,
A significant improvement of + 3.7% was observed with respect to Comparative Sample No. 1-2. The total flux of 3.7
The increase in% is comparable to the wet molding method.

【0041】次に、本発明サンプルNo. 1−1を研削し
て厚さを3%減じ、比較サンプルNo. 1−2とトータル
フラックスを同等にした。研削後の磁石を本発明サンプ
ルNo. 1−3とする。この本発明サンプルNo. 1−3と
比較サンプルNo. 1−2とをそれぞれモータに組み込
み、磁石とロータとの吸引バランスによって生じるトル
クをトルクメータにより測定して、それぞれのコギング
トルクを測定した。この結果、本発明サンプルNo. 1−
3ではコギングトルクが22.14g・cm、比較サンプル
No. 1−2では27.64g・cmであり、本発明によりコ
ギングトルクが20%も減少することがわかった。
Next, the sample No. 1-1 of the present invention was ground to reduce the thickness by 3% to make the total flux equal to that of the comparative sample No. 1-2. The magnet after grinding is referred to as Sample No. 1-3 of the present invention. The sample No. 1-3 of the present invention and the comparative sample No. 1-2 were each incorporated in a motor, and the torque generated by the attraction balance between the magnet and the rotor was measured with a torque meter to measure the respective cogging torques. As a result, sample No. 1 of the present invention
3 has a cogging torque of 22.14 gcm, comparative sample
In No. 1-2, it was 27.64 g · cm, and it was found that the present invention reduced cogging torque by 20%.

【0042】なお、トータルフラックスを同等にしてコ
ギングトルクを比較したのは、トータルフラックスが大
きくなるとコギングトルクが著しく増加するためであ
る。ただし、本発明ではBd分布曲線が極めて滑らかに
なるので、トータルフラックスが3.7%も増加してい
るにもかかわらず、本発明サンプルNo. 1−1を用いた
場合のコギングトルクは29.63g・cmであり、比較サ
ンプルNo. 1−2より約7%増加しただけであった。こ
の結果から、本発明により、実用的な高トルクモータが
実現することが明らかである。
The reason why the cogging torque is compared with the total flux being the same is that the cogging torque is remarkably increased as the total flux is increased. However, in the present invention, since the Bd distribution curve becomes extremely smooth, the cogging torque when the sample No. 1-1 of the present invention is used is 29.10 despite the total flux increasing by 3.7%. It was 63 g · cm, which was only about 7% higher than that of Comparative Sample No. 1-2. From this result, it is clear that the present invention realizes a practical high torque motor.

【0043】<実施例2>図4に示される構成の乾式成
形装置を用いて、フェライト磁石サンプルを作製した。
この成形装置は、 h/H=1.00、 w/W=0.48、 d/D=1.02 であり、いずれも本発明における好ましい範囲内のもの
であった。また、各配向用強磁性体と成形空間との距離
は、2mmとした。なお、両配向用強磁性体は、その上端
が原料粉末充填時の下部非磁性体5の上端と一致する高
さとなるように配置した。
Example 2 A ferrite magnet sample was prepared using the dry molding apparatus having the structure shown in FIG.
This molding apparatus had h / H = 1.00, w / W = 0.48, and d / D = 1.02, all of which were within the preferred range of the present invention. The distance between each orientation ferromagnetic material and the molding space was 2 mm. The orientation-oriented ferromagnetic bodies were arranged so that the upper ends thereof were at the same height as the upper ends of the lower non-magnetic bodies 5 at the time of filling the raw material powder.

【0044】この乾式成形装置を用いて、実施例1と同
様にして円弧状の異方性フェライト磁石を作製した。磁
石の寸法は、外周面の曲率半径が11.5mm、内周面の
曲率半径が7.9mm、径方向を含む断面における幅が1
7.0mm、長さ(奥行)が16.6mmであった。この磁
石を本発明サンプルNo. 2−1とする。
Using this dry molding apparatus, an arc-shaped anisotropic ferrite magnet was produced in the same manner as in Example 1. The magnet has a radius of curvature of 11.5 mm on the outer peripheral surface, a radius of curvature of 7.9 mm on the inner peripheral surface, and a width of 1 in the cross section including the radial direction.
The length was 7.0 mm and the length (depth) was 16.6 mm. This magnet is referred to as Sample No. 2-1 of the present invention.

【0045】比較のために、配向用強磁性体を設けない
以外は図4と同様な構成の乾式成形装置を用い、上記本
発明サンプルNo. 2−1と同様にして円弧状フェライト
磁石サンプルを作製した。このサンプルを、比較サンプ
ルNo. 2−2とする。
For comparison, an arc-shaped ferrite magnet sample was prepared in the same manner as in the sample No. 2-1 of the present invention using a dry molding apparatus having the same structure as that shown in FIG. 4 except that the orientation ferromagnetic material was not provided. It was made. This sample is referred to as Comparative Sample No. 2-2.

【0046】これらのサンプルに対して、実施例1と同
様にしてBdを測定した。測定個数は、各サンプルにつ
き5個とした。図6に、本発明サンプルNo. 2−1の内
周面および外周面のBd分布曲線を示す。ただし、図6
のグラフは、内周面のBdの最大値が内周面の周方向長
さの60%とはなっていない。Bd測定結果から、前述
した方法により角度θ、(α−β)/αおよびBdi/
Bdoを求めた。この結果、本発明サンプルNo. 2−1
では θ=40°、 (α−β)/α=0.18、 Bdi/Bdo=1.53 であり、いずれも本発明範囲内であったが、比較サンプ
ルNo. 2−2では θ=47°、 (α−β)/α=0.21、 Bdi/Bdo=0.85 であり、すべてが本発明範囲を外れていた。
Bd of these samples was measured in the same manner as in Example 1. The number of measurements was 5 for each sample. FIG. 6 shows Bd distribution curves of the inner peripheral surface and the outer peripheral surface of Sample No. 2-1 of the present invention. However, FIG.
In the graph, the maximum value of Bd on the inner peripheral surface is not 60% of the circumferential length of the inner peripheral surface. From the Bd measurement result, the angles θ, (α-β) / α and Bdi /
Bdo was calculated. As a result, the present invention sample No. 2-1
Θ = 40 °, (α−β) /α=0.18, and Bdi / Bdo = 1.53, all of which were within the scope of the present invention, but in Comparative Sample No. 2-2, θ = 47. °, (α-β) /α=0.21, Bdi / Bdo = 0.85, all outside the range of the present invention.

【0047】次に、これらのサンプルをそれぞれモータ
に組み込み、外部駆動によりロータを回転させたときの
起電力Ecを測定した。起電力Ecは、モータ特性の指
標となる値である。この結果、本発明サンプルNo. 2−
1ではEc=3.816 Vであり、比較サンプルNo. 2
−2に対して+3.1%もの大幅な向上が認められた。
なお、起電力Ecの3.1%の増加は、湿式成形法に匹
敵するものである。
Next, each of these samples was incorporated into a motor, and the electromotive force Ec when the rotor was rotated by external driving was measured. The electromotive force Ec is a value that is an index of motor characteristics. As a result, the present invention sample No. 2-
In the case of No. 1, Ec = 3.816 V, and comparative sample No. 2
A significant improvement of + 3.1% was observed with respect to -2.
The increase of the electromotive force Ec by 3.1% is comparable to the wet molding method.

【0048】なお、上記各実施例で作製した各サンプル
を大量に製造したときに、本発明サンプルでは、クラッ
クの発生した磁石個数が比較サンプルより40%以上も
少なかった。このクラックとは、図7に示すように、磁
石内周面の両端部付近に生じるものであり、成形体の端
部付近の配向の乱れを主因とするものである。
When a large amount of each sample produced in each of the above-mentioned examples was manufactured, the number of magnets with cracks was 40% or less in the sample of the present invention as compared with the comparative sample. As shown in FIG. 7, the cracks are generated near both ends of the inner peripheral surface of the magnet, and are mainly caused by disordered orientation near the ends of the molded body.

【0049】以上の結果から、本発明の効果が明らかで
ある。
From the above results, the effect of the present invention is clear.

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

【図1】角度θおよび(α−β)/αを説明するBd分
布グラフである。
FIG. 1 is a Bd distribution graph illustrating an angle θ and (α−β) / α.

【図2】着磁方法の説明図である。FIG. 2 is an explanatory diagram of a magnetizing method.

【図3】Bd測定方法の説明図である。FIG. 3 is an explanatory diagram of a Bd measuring method.

【図4】(a)は、本発明の乾式成形装置の構成例の断
面図であり、(b)は、上部パンチ1を取り去ったとき
の成形装置の上面図である。
4A is a cross-sectional view of a configuration example of a dry molding apparatus of the present invention, and FIG. 4B is a top view of the molding apparatus when the upper punch 1 is removed.

【図5】実施例における本発明の磁石のBd分布曲線を
示すグラフである。
FIG. 5 is a graph showing a Bd distribution curve of the magnet of the present invention in an example.

【図6】実施例における本発明の磁石のBd分布曲線を
示すグラフである。
FIG. 6 is a graph showing a Bd distribution curve of the magnet of the present invention in an example.

【図7】磁石のクラックを説明するための斜視図であ
る。
FIG. 7 is a perspective view for explaining cracks in a magnet.

【符号の説明】[Explanation of symbols]

1 上部パンチ 2 下部パンチ 3 型枠 4 上部非磁性体 5 下部非磁性体 61、62 配向用強磁性体 7 成形空間 1 Upper Punch 2 Lower Punch 3 Form Frame 4 Upper Non-Magnetic Material 5 Lower Non-Magnetic Material 61, 62 Orientation Ferromagnetic Material 7 Molding Space

Claims (6)

【特許請求の範囲】[Claims] 【請求項1】 断面が円弧状であり、その径方向に異方
性を有する弓形の乾式成形フェライト磁石であって、 横軸を測定領域長(周面の周方向長さ)、縦軸をBd
(表面磁束密度)としたBd分布グラフにおいて、 縦軸のBdの最大値が横軸の測定領域長(内周面の周方
向長さ)の60%となるように内周面のBd分布曲線を
プロットし、測定領域中央部60%を評価領域としたと
き、前記評価領域内において、Bd分布曲線上の任意の
2点を通る直線と横軸とのなす角度θが45°以下であ
り、 前記評価領域内において、Bdの最大値αとBdの最小
値βとの関係が (α−β)/α≦0.2 であり、 前記Bd分布グラフにおいて、内周面のBd分布曲線と
横軸とが囲む面積をBdiとし、外周面のBd分布曲線
と横軸とが囲む面積をBdoとしたとき、 Bdi/Bdo=1.4〜1.9 であることを特徴とする乾式成形フェライト磁石。
1. An arc-shaped dry-molded ferrite magnet having an arc-shaped cross section and having anisotropy in its radial direction, wherein the horizontal axis is the measurement region length (circumferential length of the circumferential surface), and the vertical axis is Bd
In the Bd distribution graph with (surface magnetic flux density), the Bd distribution curve of the inner peripheral surface is set so that the maximum value of Bd on the vertical axis is 60% of the measurement area length (circumferential length of the inner peripheral surface) on the horizontal axis. Is plotted and, when the central portion of the measurement area is 60%, the angle θ between the straight line passing through any two points on the Bd distribution curve and the horizontal axis is 45 ° or less in the evaluation area, In the evaluation area, the relationship between the maximum value α of Bd and the minimum value β of Bd is (α−β) /α≦0.2, and in the Bd distribution graph, the Bd distribution curve of the inner peripheral surface and the lateral When the area surrounded by the axis is Bdi and the area surrounded by the Bd distribution curve of the outer peripheral surface and the horizontal axis is Bdo, Bdi / Bdo = 1.4 to 1.9. .
【請求項2】 角度θが42°以下であり、 (α−β)/α≦0.18 であり、 Bdi/Bdo=1.5〜1.9 である請求項1の乾式成形フェライト磁石。2. The dry-molded ferrite magnet according to claim 1, wherein the angle θ is 42 ° or less, (α−β) /α≦0.18, and Bdi / Bdo = 1.5 to 1.9. 【請求項3】 断面が円弧状の成形空間内にフェライト
磁石の原料粉末を充填して、磁場中で乾式成形すること
により弓形成形体を形成するための成形装置であって、 それぞれ少なくとも一部が強磁性体から構成される上型
および下型、非磁性体から構成される型枠、ならびに2
個の配向用強磁性体を有し、前記成形空間の凸状面が下
側となるように、上型、下型および型枠により前記成形
空間が形成されており、成形空間の径方向に磁界を印加
するための磁界印加手段を有し、 2個の配向用強磁性体が、前記成形空間の周方向の両側
にそれぞれ型枠を介して設けられており、加圧開始時の
下型の上端と、各配向用強磁性体の上端とがほぼ一致す
ることを特徴とする乾式成形装置。
3. A molding apparatus for forming a bow-shaped body by filling raw material powder of a ferrite magnet into a molding space having an arcuate cross section and performing dry molding in a magnetic field, each of which is at least a part. An upper die and a lower die made of a ferromagnetic material, a mold made of a non-magnetic material, and 2
Having the orienting ferromagnetic material, the molding space is formed by an upper mold, a lower mold, and a mold so that the convex surface of the molding space is on the lower side. It has a magnetic field applying means for applying a magnetic field, and two orientation ferromagnetic bodies are provided on both sides in the circumferential direction of the molding space via molds, respectively. And the upper ends of the ferromagnetic materials for orientation are substantially coincident with each other.
【請求項4】 前記下型が、成形空間に面する下部非磁
性体を、強磁性体から構成される下パンチの上側に設け
たものである請求項3の乾式成形装置。
4. The dry molding apparatus according to claim 3, wherein the lower die is provided with a lower non-magnetic body facing the molding space, above the lower punch made of a ferromagnetic body.
【請求項5】 前記上型が、成形空間に面する上部非磁
性体を、強磁性体から構成される上パンチの下側に設け
たものである請求項4の乾式成形装置。
5. The dry molding apparatus according to claim 4, wherein the upper die is provided with an upper non-magnetic body facing a molding space, below an upper punch made of a ferromagnetic body.
【請求項6】 請求項3〜5のいずれかの乾式成形装置
を用いて請求項1または2の乾式成形フェライト磁石を
製造することを特徴とする乾式成形フェライト磁石の製
造方法。
6. A method for producing a dry-molded ferrite magnet, characterized in that the dry-molded ferrite magnet according to claim 1 or 2 is manufactured using the dry-molding apparatus according to any one of claims 3 to 5.
JP35368193A 1993-12-29 1993-12-29 Dry-formed ferrite magnet, method for producing the same, and dry-forming apparatus Expired - Fee Related JP2777693B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP35368193A JP2777693B2 (en) 1993-12-29 1993-12-29 Dry-formed ferrite magnet, method for producing the same, and dry-forming apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP35368193A JP2777693B2 (en) 1993-12-29 1993-12-29 Dry-formed ferrite magnet, method for producing the same, and dry-forming apparatus

Publications (2)

Publication Number Publication Date
JPH07201558A true JPH07201558A (en) 1995-08-04
JP2777693B2 JP2777693B2 (en) 1998-07-23

Family

ID=18432498

Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP2777693B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007281437A (en) * 2006-03-15 2007-10-25 Tdk Corp Anisotropic ferrite magnet and motor
CN100392778C (en) * 2004-03-25 2008-06-04 Tdk株式会社 Magnet manufacturing method, magnetic powder molding method, and dry molding apparatus
CN116810975A (en) * 2023-06-28 2023-09-29 湖南航天磁电有限责任公司 A mold that increases the surface magnetic distribution waveform area of magnetic tiles on the outer arc strong magnetic surface

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101055786B (en) * 2006-03-15 2010-08-04 Tdk株式会社 Anisotropy ferrite magnet and motor

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN100392778C (en) * 2004-03-25 2008-06-04 Tdk株式会社 Magnet manufacturing method, magnetic powder molding method, and dry molding apparatus
JP2007281437A (en) * 2006-03-15 2007-10-25 Tdk Corp Anisotropic ferrite magnet and motor
CN116810975A (en) * 2023-06-28 2023-09-29 湖南航天磁电有限责任公司 A mold that increases the surface magnetic distribution waveform area of magnetic tiles on the outer arc strong magnetic surface

Also Published As

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