JP2002369426A - Permanent magnet for small synchronous generator - Google Patents

Permanent magnet for small synchronous generator

Info

Publication number
JP2002369426A
JP2002369426A JP2001174950A JP2001174950A JP2002369426A JP 2002369426 A JP2002369426 A JP 2002369426A JP 2001174950 A JP2001174950 A JP 2001174950A JP 2001174950 A JP2001174950 A JP 2001174950A JP 2002369426 A JP2002369426 A JP 2002369426A
Authority
JP
Japan
Prior art keywords
permanent magnet
synchronous generator
magnet
small synchronous
excitation
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP2001174950A
Other languages
Japanese (ja)
Inventor
Kenzo Hirakui
健三 平久井
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.)
NISSHO ENGINEERING KK
Original Assignee
NISSHO ENGINEERING KK
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 NISSHO ENGINEERING KK filed Critical NISSHO ENGINEERING KK
Priority to JP2001174950A priority Critical patent/JP2002369426A/en
Publication of JP2002369426A publication Critical patent/JP2002369426A/en
Pending legal-status Critical Current

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  • Permanent Magnet Type Synchronous Machine (AREA)
  • Permanent Field Magnets Of Synchronous Machinery (AREA)

Abstract

PROBLEM TO BE SOLVED: To increase the 'maximum energy product' and 'residual magnetic flux density' of an excitation permanent magnet, as much as possible. SOLUTION: A plurality of excitation permanent magnets, formed into a flat tip shape, are used for utilization of magnetic substances with high performance. By storing them in a polygonal magnetic case after polarization, the excitation permanent magnets with high magnetism can be produced. A synchronous generator of high efficiency and high performance can then be provided.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明が属する技術分野】本発明は、小型同期発電機に
おいて「最大エネルギー積」「残留磁束密度」の強力な
励磁用永久磁石の使用に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the use of a strong excitation permanent magnet having "maximum energy product" and "residual magnetic flux density" in a small synchronous generator.

【0002】[0002]

【従来の技術】現在の小型同期発電機における励磁用永
久磁石のほとんどは、電機子形状に合わせ必要分の間隔
を設けた図2で示す環状の永久磁石(1)を使用しその永
久磁石は電機子と同心の磁器ケース(3)に収めてその磁
器ケース自体を高速回転かることにより発電するのが一
般的である。
2. Description of the Related Art Most of permanent magnets for excitation in a small synchronous generator at present use an annular permanent magnet (1) shown in FIG. 2 provided with a necessary interval according to an armature shape. Generally, power is generated by housing the porcelain case (3) concentric with the armature and rotating the porcelain case itself at a high speed.

【0003】しかし、この方法ではほとんどの場合永久
磁石は環状の一個物で、焼結、射出成型等の方法で成型
したものを磁器ケースに挿入し又は、挿入前に必要な極
数をN極S極と交互に内周着磁、所謂磁化を施し励磁用
の永久磁石が製造されておる。
However, in this method, in most cases, the permanent magnet is an annular single piece, and a permanent magnet molded by a method such as sintering or injection molding is inserted into a porcelain case, or the number of poles required before insertion is set to N poles. Permanent magnets for excitation are produced by magnetizing the inner circumference, so-called magnetization, alternately with the S pole.

【0004】この場合は、一個物の成型未着磁磁性体を
磁器ケースに挿入し、内周着磁必要極数を一度に施すだ
けなので製造費用において安価に製造できる利点が有る
ので優れた小型同期発電機の永久磁石と考えがちで有
る。しかし、この方法で製造された磁性体は容易に製造
できると言うことだけで、実際の高効率発電につながら
ないことに留意しなければならない。
In this case, since only one molded non-magnetized magnetic body is inserted into the porcelain case and the number of poles required for magnetizing the inner circumference is applied at once, there is an advantage that the manufacturing cost can be reduced and the manufacturing cost can be reduced. They are often thought of as permanent magnets for synchronous generators. However, it should be noted that the magnetic material manufactured by this method simply cannot be manufactured simply because it can be easily manufactured.

【0005】又、時には一個物の環状形状を図2で示す
幾つかに分割成型された形状の磁性体(2)も使用するこ
とがある、その場合の磁性体も着磁における共通点は、
N極S極とを交互に隣り合せに着磁しなければならない
ため、極間は当然にして磁束を減衰させる必要が生じて
しまう。このことは全体的な磁束そのものが制限される
ことになってしまう。
In some cases, a magnetic material (2) in which a single annular shape is divided into several parts as shown in FIG. 2 is also used. In this case, the magnetic materials also have a common point in magnetization.
Since the N pole and the S pole must be alternately magnetized next to each other, the magnetic flux must be attenuated between the poles. This limits the overall magnetic flux itself.

【0006】更に、同期発電機における永久磁石は励磁
を目的にしておるため、極間に空隙を必要とするので通
常残留磁束密度は各極中央で最大になる様に、つまりN
極S極の残留磁束密度を平面でグラフ表示をすると図1
に示した様に各極中央で最大に、極間で「0」になる正弦
波を描く磁束の着磁が一般的である。従って、どのよう
な磁性体を使用したとしても「最大エネルギー積」「残
留磁束密度」等に限界が生じてしまうことは避けられな
いのが現状である。
Further, since the permanent magnet in the synchronous generator is intended for excitation and requires a gap between the poles, the residual magnetic flux density is usually maximized at the center of each pole, ie, N
When the residual magnetic flux density of the pole S pole is displayed in a graph on a plane, FIG.
As shown in (1), it is common to magnetize a magnetic flux that draws a sine wave that becomes “0” between poles at the center of each pole. Therefore, no matter what kind of magnetic material is used, it is currently unavoidable that the “maximum energy product”, “residual magnetic flux density” and the like are limited.

【0007】この改善策として、磁性体に対し着磁時の
治具の改善、着磁電流の制御改善、など行っておるがそ
の磁性体には自ずからの特性に限界が有り、飛躍的な改
善が成されてないのが現状である。
[0007] As a remedy, the jig for magnetizing the magnetic body is improved, and the control of the magnetizing current is improved. However, the magnetic body has a limit in its natural characteristics, and it is dramatically improved. At present, it has not been achieved.

【0008】[0008]

【発明が解決しようとする課題】解決しようとする問題
点は、同期発電機における「発電電圧は回転速度と磁束
の積からなる」から、当然にして磁束の大きさが必須条
件となりうる。よって限られた容積内での高残留磁束密
度の永久磁石が求められる。
The problem to be solved is that the power generation voltage is the product of the rotational speed and the magnetic flux in the synchronous generator, so that the magnitude of the magnetic flux can of course be an essential condition. Therefore, a permanent magnet having a high residual magnetic flux density within a limited volume is required.

【0009】[0009]

【課題を解決するための手段】本発明は、現存する磁性
体の中で極めて「最大エネルギー積」「残留磁束密度」
等の特性に優れた、ネオジウム(Nd)、鉄(Fe)、
ほう素(B)を主成分にした正方晶構造のNd2Fe14
Bの磁性体を採用し図3で示す平板チップ形状磁石(5)
とし、必要枚数分を使用することで従来の同期発電機励
磁用永久磁石を飛躍的に強力にし又、容積比で著しく小
型にすることを特徴とする。
SUMMARY OF THE INVENTION The present invention relates to a magnetic recording medium which has extremely high "maximum energy product" and "residual magnetic flux density" among existing magnetic materials.
Neodymium (Nd), iron (Fe),
Nd2Fe14 having a tetragonal structure with boron (B) as the main component
A flat chip-shaped magnet (5) shown in FIG.
By using the required number of magnets, the conventional permanent magnet for exciting the synchronous generator is remarkably strengthened and the volume ratio is remarkably reduced.

【0010】[0010]

【発明の実施の形態】基本的に製造コストを抑えるに
は、従来の形態を維持する必要があり平板チップ形状磁
石(5)を磁器ケースに密着させるため多角形にすること
と、必要枚数分を容易に挿入するため磁石挿入フレーム
(6)が必要となる。但し極数は偶数でなければならな
い。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS In order to reduce the manufacturing cost, it is basically necessary to maintain the conventional configuration. A flat chip-shaped magnet (5) should be made polygonal so as to be in close contact with a porcelain case. Magnet insertion frame for easy insertion
(6) is required. However, the number of poles must be even.

【0011】又、この磁石は平板チップ形状磁石(5)で
あるため、単純な両面着磁で、しかもその磁性体が持つ
最良の条件のもと、均一に着磁できるため都度の着磁に
よる品質差が無い安定した磁力の磁石が得られる。
Further, since this magnet is a flat chip-shaped magnet (5), it can be simply magnetized on both sides and can be magnetized uniformly under the best conditions of the magnetic material. A magnet with a stable magnetic force with no quality difference can be obtained.

【0012】[0012]

【実施例】図2は本発明との比較を表する従来の部品構
成を表す組図であって(1)から(3)はそれぞれの部品名
称である。
FIG. 2 is a set diagram showing a conventional component configuration showing a comparison with the present invention, wherein (1) to (3) are the component names.

【0013】図3は本発明の部品構成を表す組図であり
(4)から(7)はそれぞれの部品名称である、平板チップ
形状磁石(5)は着磁された後、面を変えてN極S極を交
互に磁石挿入フレーム(6)に配置し、多角形磁器ケース
(7)に収納することにより構成される。
FIG. 3 is an assembly diagram showing the component configuration of the present invention.
(4) to (7) are the names of the respective components. After the plate-shaped magnet (5) is magnetized, the N-pole and S-pole are alternately arranged on the magnet insertion frame (6) by changing the surface, Polygon porcelain case
It is configured by storing it in (7).

【0014】図4は本発明の組立斜視図であり(8)で示
す部分は、円柱形状である電機子(4)と平板チップ形状
磁石(5)であるから当然にして生じる最小間隔部であ
り、(9)は最大間隔部である。この種の同期発電機は、
電機子(4)と磁器ケースは同心で励磁用の永久磁石が回
転することが一般的であるから、多角形磁器ケース(7)
に平板チップ形状磁石(5)を装着した、多角形磁器ケー
ス(7)が回転することで磁石はN極S極を交互に装着さ
れた状態であるなら、電機子(4)に対し磁石間の磁力は
一番近づいた最小間隔部のとき磁力は最大で逆に一番離
れた最大間隔部なら弱くなることを繰返す、従って図1
のグラフと同様な擬似正弦波を描く磁力分布が形成され
る。よって多角形磁器ケース(7)は本発明に不可欠要素
である。
FIG. 4 is an assembling perspective view of the present invention. The portion indicated by (8) is a minimum gap which is naturally formed because of the cylindrical armature (4) and the flat chip-shaped magnet (5). Yes, (9) is the maximum interval. This type of synchronous generator
Since the armature (4) and the porcelain case are generally concentric and a permanent magnet for excitation rotates, the polygonal porcelain case (7)
If the polygonal porcelain case (7) with the flat chip-shaped magnet (5) mounted on it is rotated so that the magnets are alternately mounted with N and S poles, the armature (4) and the magnet When the magnetic force is at the shortest interval, the magnetic force repeats to be maximum, and conversely, becomes weak at the maximum interval, which is farthest away.
A magnetic force distribution that draws a pseudo sine wave similar to the graph of FIG. Therefore, the polygonal porcelain case (7) is an essential element of the present invention.

【0015】[0015]

【発明の効果】以上説明したように本発明の同期発電機
励磁用永久磁石は、平板チップ形状の磁性体に対し単純
に両面着磁により磁化し、必要数を環状に組み込んで多
角形磁器ケースに収納するだけの簡単な方法であるが、
各磁石は平板チップ形状で最大均一に着磁し複数の枚数
を使用するため、従来品のフェライト焼結磁石と比較し
て「最大エネルギー積」で約10倍、「残留磁束密度」
で約3倍と共に優れておるので高効率で高性能な発電が
得られるようになり、現存の家庭用風力発電機、携帯電
話充電用発電機、等各方面で利用でき高エネルギー化実
現の一助になる。
As described above, the synchronous generator exciting permanent magnet of the present invention is obtained by simply magnetizing a flat chip-shaped magnetic material by double-sided magnetization, and incorporating the required number in a ring shape into a polygonal porcelain case. It is a simple method of storing in
Each magnet is magnetized in the shape of a flat chip at the maximum, and it uses a plurality of magnets. Therefore, compared to conventional ferrite sintered magnets, the "maximum energy product" is about 10 times, and the "residual magnetic flux density"
, Which is about three times as good as that, it is possible to obtain high-efficiency and high-performance power generation, which can be used in existing home wind power generators, mobile phone charging generators, etc. become.

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

【図1】同期発電機用励磁永久磁石の磁束密度を表すグ
ラフ
FIG. 1 is a graph showing the magnetic flux density of an exciting permanent magnet for a synchronous generator.

【図2】従来型の同期発電機用励磁永久磁石の部品構成
FIG. 2 is a configuration diagram of a conventional excitation permanent magnet for a synchronous generator.

【図3】本発明の同期発電機用励磁永久磁石の部品構成
FIG. 3 is a structural view of parts of an exciting permanent magnet for a synchronous generator according to the present invention.

【図4】本発明の同期発電機の組立斜視図FIG. 4 is an assembled perspective view of the synchronous generator of the present invention.

【符号の説明】[Explanation of symbols]

(1) 環状の永久磁石 (2) 分割成型された形状の磁性体 (3) 磁器ケース (4) 電機子 (5) 平板チップ形状磁石 (6) 磁石挿入フレーム (7) 多角形磁器ケース (8) 電機子と平板チップ形状磁石との最小間隔部 (9) 電機子と平板チップ形状磁石との最大間隔部 (1) Annular permanent magnet (2) Divided molded magnetic material (3) Porcelain case (4) Armature (5) Flat chip shaped magnet (6) Magnet insertion frame (7) Polygonal porcelain case (8 ) Minimum gap between armature and flat chip magnet (9) Maximum gap between armature and flat chip magnet

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 小型同期発電機の電機子コイルに対する
励磁用永久磁石に付いて、そのN極、S極の単極を交互
に配置し環状に形成された小型同期発電機励磁用永久磁
石で、その磁石は単純な平板チップ形状であることを特
徴とする小型同期発電機の励磁用永久磁石であって、磁
器ケースは平板チップ形状磁石の使用枚数分の多角形で
あることと、平板チップ形状磁石を容易にセットするた
めの磁石挿入フレームを有した小型同期発電機の励磁用
永久磁石。
1. A small synchronous generator exciting permanent magnet formed in an annular shape by alternately arranging N poles and S poles of a single pole with respect to an exciting permanent magnet for an armature coil of the small synchronous generator. The magnet is a simple flat chip shape permanent magnet for excitation of a small synchronous generator, the porcelain case is polygonal for the number of flat chip shape magnets used, and the flat chip is Excitation permanent magnets for small synchronous generators with a magnet insertion frame to easily set shaped magnets.
JP2001174950A 2001-06-11 2001-06-11 Permanent magnet for small synchronous generator Pending JP2002369426A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2001174950A JP2002369426A (en) 2001-06-11 2001-06-11 Permanent magnet for small synchronous generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2001174950A JP2002369426A (en) 2001-06-11 2001-06-11 Permanent magnet for small synchronous generator

Publications (1)

Publication Number Publication Date
JP2002369426A true JP2002369426A (en) 2002-12-20

Family

ID=19016162

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2001174950A Pending JP2002369426A (en) 2001-06-11 2001-06-11 Permanent magnet for small synchronous generator

Country Status (1)

Country Link
JP (1) JP2002369426A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN100365919C (en) * 2003-01-10 2008-01-30 株式会社萌力克 Rotary electrical device
JP2009213259A (en) * 2008-03-04 2009-09-17 Mitsuba Corp Magnet generator
KR101471367B1 (en) * 2010-11-30 2014-12-11 대동모벨시스템 주식회사 Rotor Structure of BLDC Motor

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5444707A (en) * 1977-09-14 1979-04-09 Sony Corp Dc brushless motor
JPH01150470U (en) * 1988-04-07 1989-10-18
JPH02168828A (en) * 1988-12-21 1990-06-28 Matsushita Electric Ind Co Ltd Magnet fixing method
JP2001136690A (en) * 1999-11-10 2001-05-18 Isuzu Motors Ltd Rotor of rotating machine
JP2001145310A (en) * 1999-11-17 2001-05-25 Moriyama Manufacturing Co Ltd Magnetization of rotor for permanent-magnet generator, and inspecting method and device thereof

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5444707A (en) * 1977-09-14 1979-04-09 Sony Corp Dc brushless motor
JPH01150470U (en) * 1988-04-07 1989-10-18
JPH02168828A (en) * 1988-12-21 1990-06-28 Matsushita Electric Ind Co Ltd Magnet fixing method
JP2001136690A (en) * 1999-11-10 2001-05-18 Isuzu Motors Ltd Rotor of rotating machine
JP2001145310A (en) * 1999-11-17 2001-05-25 Moriyama Manufacturing Co Ltd Magnetization of rotor for permanent-magnet generator, and inspecting method and device thereof

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN100365919C (en) * 2003-01-10 2008-01-30 株式会社萌力克 Rotary electrical device
JP2009213259A (en) * 2008-03-04 2009-09-17 Mitsuba Corp Magnet generator
KR101471367B1 (en) * 2010-11-30 2014-12-11 대동모벨시스템 주식회사 Rotor Structure of BLDC Motor

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