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JP3690261B2 - Rotating electric machine - Google Patents

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Publication number
JP3690261B2
JP3690261B2 JP2000327290A JP2000327290A JP3690261B2 JP 3690261 B2 JP3690261 B2 JP 3690261B2 JP 2000327290 A JP2000327290 A JP 2000327290A JP 2000327290 A JP2000327290 A JP 2000327290A JP 3690261 B2 JP3690261 B2 JP 3690261B2
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Japan
Prior art keywords
magnetic
magnetic pole
sub
pole
electrical machine
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Expired - Fee Related
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JP2000327290A
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Japanese (ja)
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JP2002136087A (en
Inventor
雅浩 加藤
正昇 大見
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Denso Corp
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Denso Corp
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Priority to JP2000327290A priority Critical patent/JP3690261B2/en
Priority to US09/977,679 priority patent/US6465925B2/en
Priority to DE10152538A priority patent/DE10152538A1/en
Priority to IT2001RM000629A priority patent/ITRM20010629A1/en
Publication of JP2002136087A publication Critical patent/JP2002136087A/en
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Description

【0001】
【発明の属する技術分野】
本発明は、永久磁石界磁型の回転電機に関し、特に副磁極付きの永久磁石界磁型の回転電機に関するものである。
【0002】
【従来の技術】
この種の回転電機として、特公昭57−12380号公報に開示された技術が知られている。この公報に開示された回転電機は、各主磁極の極間に、隣接する主磁極の電機子側の磁極面の極性と同極性の一対の磁極面を周方向両端面に有する永久磁石からなる副磁極を配置して、主磁極間における漏れ磁束を抑え、主磁極からギャップを介して電機子に到る有効磁束を増すものである。この技術によって、回転電機の外形寸法を変えることなく、出力を増大することができる。また、この技術を用いることによって、回転電機の出力を変えることなく、外形寸法を小型化することができる。
【0003】
【発明が解決しようとする課題】
回転電機の運転中においては、電機子に電流が流れ、電機子反作用による磁束分布が発生する。図6には、回転電機の界磁および電機子の展開図および、それに対応する電機子反作用による磁束分布を示す。この磁束分布は、図6に示すように、三角波状を成しており、隣り合う主磁極間、すなわち副磁極位置において最大となる。図6より明らかなように、副磁極に作用する磁束は、主磁極に作用する磁束よりΔHだけ大きい。つまり電機子反作用の影響は副磁極が最も強く受ける。副磁極には、それ自身の磁化方向とは異なる電機子反作用による大きい磁束が作用して、副磁極が減磁される。電機子反作用が大きい場合には、副磁極に不可逆減磁が発生してしまう。副磁極に不可逆減磁が発生した場合には、電機子反作用が取り除かれても副磁極の磁束密度は低下したままで元に戻らない。従って、副磁極が果たすべき主磁極間における漏れ磁束の抑制機能が低下し、回転電機の出力が低下する恐れがある。
【0004】
本発明は、上記のような点に鑑みなされたものであり、副磁極の磁気特性を適切に選定するという容易な手段により、最大電機子反作用発生時における副磁極の不可逆減磁を防止し、副磁極が果たしている主磁極間の漏れ磁束抑制機能を維持して、出力低下の起きない信頼性の高い回転電機を提供することを目的とする。
【0005】
【課題を解決するための手段】
本発明は上記目的を達成する為、以下の技術的手段を採用する。
【0007】
本発明の請求項1に記載の回転電機は、副磁極石の磁束密度を、回転電機運転時の最大電機子反作用による副磁極の不可逆減磁発生後の磁束密度が所定の値以上となるような値に設定した。これにより、回転電機運転中の最大電機子反作用による副磁極の不可逆減磁発生後においても、副磁極は、主磁極間の漏れ磁束抑制機能上必要あるいはそれ以上の磁束密度に保持されるので、回転電機の出力を安定して維持することができる。特に、本発明の請求項2のように、副磁極の磁束密度を、主磁極の磁束密度より大きい値に設定することにより、主磁極に副磁極よりも安価な材質を用いることができるので、回転電機のコスト上昇を抑えつつ、副磁極が果たしている主磁極間の漏れ磁束抑制機能を安定して維持することができる。
【0008】
本発明の請求項3に記載の回転電機は、請求項1または請求項2に記載の回転電機における最大電機子反作用は、回転電機始動時における拘束電流によるものである。一般に、回転電機の最大電機子電流は回転電機始動時における拘束電流である。これにより、回転電機運転中の最大電機子反作用による副磁極の機能低下を確実に防止することができる。
【0009】
【発明の実施の形態】
(第1の実施形態)
以下、本発明の第1の実施形態による回転電機1を、エンジンの始動用電動機に適用した場合を例に図面に基づいて説明する。
【0010】
図4は、本発明の第1の実施形態による回転電機1の構成を示す。
【0011】
回転電機1は、筒状のヨーク2内に設けられており、ヨーク2内で回転自在に設けられた電機子6と、ヨーク2の内側に固定された界磁磁極3を備える。
【0012】
電機子6は、ヨーク2内で回転自在に支持されたシャフト7、このシャフト7に固定されたコア8、電機子コイル(図示せず)、正極ブラシ(図示せず)および負極ブラシ(図示せず)が摺接する整流子(図示せず)から構成される。
【0013】
界磁磁極3は、電機子コイルが発生する磁束に作用する磁束を生じさせる複数(第1の実施形態では6個)の主磁極4a〜4f、この主磁極4a〜4fの極間に配置されて主磁極4a〜4fの有効磁束を増大させる複数(第1の実施形態では6個)の副磁極5a〜5fから構成される。
【0014】
主磁極4a〜4fは、ヨーク2から電機子6に向かう方向に磁極方向を持つ永久磁石で、図4に示すように、電機子6側の極性が、空間的に60°ずつずれるように、N極とS極が交互に位置するように等間隔で配置されている。つまり、主磁極4aの電機子6側の極性がS極であると、主磁極4c、4eの電機子6側の極性がS極で、主磁極4b、4d、4fの極性がN極である。
【0015】
副磁極5a〜5fは、隣接する2個の主磁極(4aと4b、4bと4c、4cと4d、4dと4e、4eと4f、4fと4a)の極間に配置され、両側の主磁極に向かう方向に磁極方向を持ち、隣接する主磁極の側面の極性に対して同一極性が対向する永久磁石である。つまり、主磁極3aと主磁極3bの間に、主磁極4a側にS極が向き、主磁極4b側にN極が向く副磁極5aを配置した場合、主磁極4bと主磁極4c間に、主磁極4bにNが向き、主磁極4cにSが向く副磁極5bが、主磁極4cと主磁極4dの間に、主磁極4c側にS極が向き、主磁極4d側にN極が向く副磁極5cが、主磁極4dと主磁極4e間に、主磁極4dにNが向き、主磁極4eにSが向く副磁極5dが、主磁極4eと主磁極4fの間に、主磁極4e側にS極が向き、主磁極4f側にN極が向く副磁極5eが、主磁極4f主磁極と4a間に、主磁極4fにNが向き、主磁極4aにSが向く副磁極5fが配置されている。
【0016】
次に、本発明の第1の実施形態による回転電機1の運転中における副磁極5a〜5fの磁気特性の変動および材質の選定について説明する。
【0017】
図2には、回転電機1の副磁極5a〜5fのB−H特性を示す。縦軸は磁束密度B、横軸は磁界の強さHである。H=0の時の磁束密度Brは、副磁極5a〜5f単体の残留磁束密度である。副磁極5a〜5fの動作点Aは、B−H特性とパーミアンス線Pとの交点である。B−H特性は、動作点Aから図2の左方へ直線的に変化し、屈曲点Cにおいてその傾きが変化し、屈曲点Cから左方は傾きがより急になる。さらに、図2に示すB−H特性は、副磁極5a〜5fの機能、つまり、主磁極4a〜4fの漏れ磁束抑制機能を維持する上で必要且つ十分なものである。
【0018】
先ず、本発明の第1の実施形態による回転電機1の運転中における副磁極5a〜5fの磁気特性の変動について説明する。
【0019】
電機子反作用が無い場合、副磁極5a〜5fの動作点Aにおける磁束密度はB0である。次に、回転電機1が運転され、電機子反作用により逆磁界−H1が作用すると、パーミアンス線Pは図の左方へ平行移動するので、副磁極5a〜5fの動作点は点Dとなる。さらに、電機子反作用による逆磁界−H1がなくなると、副磁極5a〜5fの動作点は点DからB−H特性上を再び点Aへ戻る。すなわち、不可逆減磁は発生しない。
【0020】
最大電機子反作用による逆磁界−H2が作用すると、パーミアンス線Pは図の左方へ平行移動し、副磁極5a〜5fの動作点は屈曲点Cを通り過ぎて点Eとなる。この場合、逆磁界−H2がなくなっても、副磁極5a〜5fの動作点は点Aへは戻らずに、線分CAと平行な線分EA’上を図の右方へ点A’まで戻る。点A’は、パーミアンス線Pと線分EA’との交点である。この時の磁束密度はB1であり、B0より小さくなる。すなわち、副磁極5a〜5fにおいて不可逆減磁が生じており、B0−B1が、電機子反作用による逆磁界−H2による不逆減磁量となる。不可逆減磁発生後の副磁極5a〜5fのB−H特性は曲線A’ETとなるので、副磁極5a〜5fの機能、つまり、主磁極4a〜4fの漏れ磁束抑制機能を維持することができない。
【0021】
次に、副磁極5a〜5fの材質の選定について説明する。
【0022】
図1には、2種類の異なる永久磁石材料X、およびYを用いた場合における、回転電機1の副磁極5a〜5fのB−H特性を示す。永久磁石材料YのB−H特性は、図2に示したB−H特性と同一である。
【0023】
図1に示すとおり、永久磁石材料XのB−H特性における屈曲点Fは、永久磁石材料YのB−H特性における屈曲点Cより図の左方にあり、永久磁石材料Xの保磁力は、永久磁石材料Yの保磁力より大きい。
【0024】
回転電機1の最大電機子反作用により逆磁界−H2が作用すると、永久磁石材料Xによる副磁極5a〜5fの動作点は図1中の点Gとなる。この点Gは、屈曲点Fより右側、つまりB−H特性が直線状の部分にあるので、逆磁界−H2がなくなると、副磁極5a〜5fの動作点は点Aへ戻る。すなわち、不可逆減磁は発生しない。従って、副磁極5a〜5f材料に、より保磁力の大きい永久磁石材料Xを採用することにより、最大電機子反作用による逆磁界−H2が作用した場合において、副磁極5a〜5fの不可逆減磁を防止することができる。
【0025】
ここで、最大電機子反作用について簡単に説明する。一般に、回転電機1における電機子反作用の大きさは、電機子コイル(図示せず)に流れる電流の大きさに比例する。エンジン始動用電動機の場合には、電機子コイル(図示せず)に流れる最大電流は、キースイッチがONされて、回転電機1に通電され、且つ電機子が回転していない時の電流(いわゆる拘束電流)となる。ところで拘束電流は、バッテリ(図示せず)の容量が大きいほど、また温度が低いほど大きくなる。従って、回転電機1における最大電機子反作用は、最低使用温度条件下において、使用する可能性があるバッテリの中で最大容量のものと組合わせた時の拘束電流により最大となる。この値を基にして、副磁極5a〜5fの磁気特性を算定すればよい。
【0026】
以上説明した、本発明の第1の実施形態による回転電機1においては、副磁極5a〜5f材料に、最大電機子反作用による逆磁界を受けても不可逆減磁を起こさないような、保磁力の大きい永久磁石材料Xを採用することにより、副磁極5a〜5fの不可逆減磁を防止し、副磁極5a〜5fの主磁極4a〜4fの漏れ磁束抑制機能を維持して、回転電機1の出力低下を防止することができた。
【0027】
一方、主磁極4a〜4fに作用する最大電機子反作用による逆磁界の大きさは、図6に示すように、副磁極5a〜5fに作用する最大電機子反作用による逆磁界の大きさより小さい。従って、主磁極4a〜4fに、副磁極5a〜5fに用いた永久磁石材料Xより保磁力の小さい安価な材料を用いても、主磁極4a〜4fが最大電機子反作用による逆磁界を受けて不可逆減磁を起こすことを防止ができる。この場合は、コスト上昇を抑えつつ、副磁極5a〜5fの不可逆減磁を防止し、副磁極5a〜5fの主磁極4a〜4fの漏れ磁束抑制機能を維持して、回転電機1の出力低下を防止することができる。
【0028】
(第2の実施形態)
本発明の第2の実施形態の回転電機1においては、副磁極5a〜5fの材質の選定方法が第1の実施形態と異なっている。すなわち、第1の実施形態においては、永久磁石材料の保磁力に着目して選定したが、第2の実施形態では磁束密度に着目して選定している。
【0029】
以下に、副磁極5a〜5fの材質の選定について説明する。
【0030】
図3には、2種類の異なる永久磁石材料W、およびYを用いた場合における、回転電機1の副磁極5a〜5fのB−H特性を示す。永久磁石材料YのB−H特性は、図2に示したB−H特性と同一である。
【0031】
図3に示すように、保磁力は、永久磁石材料Wと永久磁石材料Yは同じである。しかし、磁束密度関しては、永久磁石材料Wは永久磁石材料Yより大きい。電機子反作用が無い場合、副磁極5a〜5fの動作点は点Jであり、その時の磁束密度はB2である。また、永久磁石材料WのB−H特性における屈曲点Kは、永久磁石材料YのB−H特性における屈曲点Cより図の右方にある。
【0032】
ここで、回転電機1の最大電機子反作用により逆磁界−H2が作用すると、永久磁石材料Wによる副磁極5a〜5fの動作点は、図3に示すように、屈曲点Kを通り過ぎて点Lとなる。従って、逆磁界−H2がなくなっても、副磁極5a〜5fの動作点は点Jへは戻らずに、線分KJと平行な線分LM上を図の右方へ点Mまで戻る。点Mは、パーミアンス線Pと線分LMとの交点である。この時の磁束密度はB3であり、B2より小さくなる。すなわち、副磁極5a〜5fにおいて不可逆減磁が発生し、B2−B3が、最大電機子反作用による逆磁界−H2による不可逆減磁量となる。しかし、不可逆減磁発生後においても、副磁極5a〜5fのB−H特性は曲線MLTとなり、副磁極5a〜5fの主磁極4a〜4fの漏れ磁束抑制機能を維持するための必要十分条件である曲線ACTを上回るので、副磁極5a〜5fは主磁極4a〜4fの漏れ磁束抑制機能を維持できる。以後は、最大電機子反作用による逆磁界−H2を何回受けても、副磁極5a〜5fのB−H特性は曲線MLTで安定する。
【0033】
以上説明した、本発明の第2の実施形態による回転電機1においては、副磁極5a〜5f材料に、最大電機子反作用による不可逆減磁発生後においても磁束密度が所定の値以上となるような、磁束密度の大きい永久磁石材料Wを採用することにより、副磁極5a〜5fの主磁極4a〜4fの漏れ磁束抑制機能を維持して、回転電機1の出力低下を防止することができる。
【0034】
一方、主磁極4a〜4fに作用する最大電機子反作用による逆磁界の大きさは、図6に示すように、副磁極5a〜5fに作用する最大電機子反作用による逆磁界の大きさより小さい。従って、主磁極4a〜4fに、副磁極5a〜5fに用いた永久磁石材料Wより磁束密度の小さい安価な材料を用いても、最大電機子反作用による不可逆減磁発生後における主磁極4a〜4fの磁束密度を所定の値以上とすることができる。この場合は、コスト上昇を抑えつつ、副磁極5a〜5fの主磁極4a〜4fの漏れ磁束抑制機能を維持して、回転電機1の出力低下を防止することができる。
【0035】
また、本発明の第1の実施形態、または第2の実施形態の回転電機1において、図5に示すように、主磁極4a〜4fと副磁極5a〜5fの間に軟磁性体9a〜9f(たとえば軟鉄)を挿入した構成としたものであってもよい。
【図面の簡単な説明】
【図1】本発明の第1の実施形態による回転電機1の副磁極5a〜5fにおいて、2種類の異なる永久磁石材料X、およびYを用いた場合における、それぞれのB−H特性を示す。
【図2】本発明の第1の実施形態による回転電機1の副磁極5a〜5fのB−H特性を示す線図である。
【図3】本発明の第2の実施形態による回転電機1の副磁極5a〜5fにおいて、2種類の異なる永久磁石材料W、およびYを用いた場合における、それぞれのB−H特性を示す。
【図4】本発明の第1の実施形態による回転電機1の模式径方向断面図である。
【図5】第1の実施形態、または第2の実施形態の変形例による回転電機1の変形例の模式径方向断面図である。
【図6】一般的な永久磁石界磁型の回転電機における、界磁および電機子の展開図および、それに対応する電機子反作用による磁束分布を示す説明図である。
【符号の説明】
1 回転電機
2 ヨーク
3 界磁磁極
4a〜4f 主磁極
5a〜5f 副磁極
6 電機子
7 シャフト
8 コア
9a〜9f 軟磁性体
A 動作点
A’ 動作点
B 磁束密度
0〜B3 磁束密度
Br 残留磁束密度
C 屈曲点
D 動作点
E 動作点
F 屈曲点
G 動作点
H 磁界の強さ、磁束
J 動作点
K 屈曲点
L 動作点
M 動作点
P パーミアンス線
W 永久磁石
X 永久磁石
Y 永久磁石
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a permanent magnet field type rotating electrical machine, and more particularly to a permanent magnet field type rotating electrical machine with a sub-pole.
[0002]
[Prior art]
As this type of rotating electric machine, a technique disclosed in Japanese Patent Publication No. 57-12380 is known. The rotating electrical machine disclosed in this publication is composed of a permanent magnet having a pair of magnetic pole faces at the opposite end faces in the circumferential direction between the poles of each main magnetic pole and having the same polarity as the magnetic pole face on the armature side of the adjacent main magnetic pole. The sub magnetic pole is arranged to suppress the leakage magnetic flux between the main magnetic poles and increase the effective magnetic flux reaching the armature from the main magnetic pole through the gap. With this technique, the output can be increased without changing the external dimensions of the rotating electrical machine. In addition, by using this technique, the outer dimensions can be reduced without changing the output of the rotating electrical machine.
[0003]
[Problems to be solved by the invention]
During operation of the rotating electrical machine, a current flows through the armature, and a magnetic flux distribution is generated due to the armature reaction. FIG. 6 shows a developed view of the field and armature of the rotating electric machine and the magnetic flux distribution due to the corresponding armature reaction. As shown in FIG. 6, this magnetic flux distribution has a triangular wave shape, and is maximized between adjacent main magnetic poles, that is, at the position of the sub magnetic pole. As is clear from FIG. 6, the magnetic flux acting on the sub magnetic pole is larger by ΔH than the magnetic flux acting on the main magnetic pole. That is, the sub-magnetic pole is most strongly affected by the armature reaction. A large magnetic flux due to an armature reaction different from the magnetization direction of the sub magnetic pole acts on the sub magnetic pole to demagnetize the sub magnetic pole. When the armature reaction is large, irreversible demagnetization occurs in the auxiliary magnetic pole. When irreversible demagnetization occurs in the secondary magnetic pole, even if the armature reaction is removed, the magnetic flux density of the secondary magnetic pole remains lowered and does not return. Therefore, the function of suppressing the leakage magnetic flux between the main magnetic poles to be fulfilled by the sub magnetic pole is lowered, and the output of the rotating electrical machine may be lowered.
[0004]
The present invention has been made in view of the above points, and by an easy means of appropriately selecting the magnetic characteristics of the sub-pole, preventing irreversible demagnetization of the sub-pole when the maximum armature reaction occurs, An object of the present invention is to provide a highly reliable rotating electrical machine that maintains the leakage magnetic flux suppressing function between main magnetic poles fulfilled by the sub-magnetic pole and does not cause a decrease in output.
[0005]
[Means for Solving the Problems]
In order to achieve the above object, the present invention employs the following technical means.
[0007]
In the rotating electrical machine according to claim 1 of the present invention, the magnetic flux density of the auxiliary pole stone is set so that the magnetic flux density after irreversible demagnetization of the auxiliary magnetic pole due to the maximum armature reaction during the rotating electrical machine operation becomes a predetermined value or more. Was set to an appropriate value. Thereby, even after the irreversible demagnetization of the secondary magnetic pole due to the maximum armature reaction during operation of the rotating electrical machine, the secondary magnetic pole is maintained at a magnetic flux density that is necessary or higher for the leakage magnetic flux suppression function between the main magnetic poles. The output of the rotating electrical machine can be stably maintained. In particular, as in claim 2 of the present invention, by setting the magnetic flux density of the sub magnetic pole to a value larger than the magnetic flux density of the main magnetic pole, a material cheaper than the sub magnetic pole can be used for the main magnetic pole. While suppressing an increase in cost of the rotating electrical machine, the leakage magnetic flux suppressing function between the main magnetic poles fulfilled by the sub-magnetic pole can be stably maintained.
[0008]
In the rotating electrical machine according to claim 3 of the present invention, the maximum armature reaction in the rotating electrical machine according to claim 1 or 2 is due to the restraint current at the time of starting the rotating electrical machine. In general, the maximum armature current of a rotating electrical machine is a binding current when starting the rotating electrical machine. As a result, it is possible to reliably prevent the function deterioration of the sub magnetic pole due to the maximum armature reaction during the operation of the rotating electric machine.
[0009]
DETAILED DESCRIPTION OF THE INVENTION
(First embodiment)
Hereinafter, an example in which the rotating electrical machine 1 according to the first embodiment of the present invention is applied to an engine starting motor will be described with reference to the drawings.
[0010]
FIG. 4 shows the configuration of the rotating electrical machine 1 according to the first embodiment of the present invention.
[0011]
The rotating electrical machine 1 is provided in a cylindrical yoke 2, and includes an armature 6 that is rotatably provided in the yoke 2, and a field magnetic pole 3 that is fixed inside the yoke 2.
[0012]
The armature 6 includes a shaft 7 rotatably supported in the yoke 2, a core 8 fixed to the shaft 7, an armature coil (not shown), a positive brush (not shown), and a negative brush (not shown). Z) is composed of a commutator (not shown) in sliding contact.
[0013]
The field magnetic pole 3 is arranged between a plurality of (six in the first embodiment) main magnetic poles 4a to 4f that generate magnetic flux acting on the magnetic flux generated by the armature coil, and between the main magnetic poles 4a to 4f. The plurality of (6 in the first embodiment) sub magnetic poles 5a to 5f that increase the effective magnetic flux of the main magnetic poles 4a to 4f.
[0014]
The main magnetic poles 4a to 4f are permanent magnets having a magnetic pole direction in a direction from the yoke 2 toward the armature 6, and as shown in FIG. 4, the armature 6 side polarity is spatially shifted by 60 °. N poles and S poles are arranged at equal intervals so as to be alternately positioned. That is, when the polarity of the main pole 4a on the armature 6 side is S, the polarity of the main poles 4c, 4e on the armature 6 side is S, and the polarity of the main poles 4b, 4d, 4f is N. .
[0015]
The sub magnetic poles 5a to 5f are arranged between two adjacent main magnetic poles (4a and 4b, 4b and 4c, 4c and 4d, 4d and 4e, 4e and 4f, 4f and 4a). A permanent magnet having a magnetic pole direction in the direction toward the surface and having the same polarity opposite to the polarity of the side surface of the adjacent main magnetic pole. That is, between the main magnetic pole 3a and the main magnetic pole 3b, when the sub magnetic pole 5a with the S pole facing the main magnetic pole 4a and the N pole facing the main magnetic pole 4b is disposed between the main magnetic pole 4a and the main magnetic pole 4b, The sub-magnetic pole 5b with N facing the main magnetic pole 4b and S facing the main magnetic pole 4c has the S pole facing the main magnetic pole 4c and the N pole facing the main magnetic pole 4d between the main magnetic pole 4c and the main magnetic pole 4d. The sub magnetic pole 5c is between the main magnetic pole 4d and the main magnetic pole 4e, the main magnetic pole 4d is facing N, the main magnetic pole 4e is facing S, and the sub magnetic pole 5d is between the main magnetic pole 4e and the main magnetic pole 4f. A sub-magnetic pole 5e with an S-pole facing toward the main pole 4f and an N-pole facing toward the main magnetic pole 4f is disposed between the main magnetic pole 4f and the main magnetic pole 4a. Has been.
[0016]
Next, changes in the magnetic characteristics of the sub magnetic poles 5a to 5f and selection of materials during operation of the rotating electrical machine 1 according to the first embodiment of the present invention will be described.
[0017]
FIG. 2 shows the BH characteristics of the sub magnetic poles 5 a to 5 f of the rotating electrical machine 1. The vertical axis represents the magnetic flux density B, and the horizontal axis represents the magnetic field strength H. The magnetic flux density Br when H = 0 is the residual magnetic flux density of the sub magnetic poles 5a to 5f alone. The operating point A of the sub magnetic poles 5a to 5f is an intersection of the BH characteristic and the permeance line P. The BH characteristic changes linearly from the operating point A to the left in FIG. 2, and its inclination changes at the bending point C, and the inclination from the bending point C to the left becomes steeper. Further, the BH characteristic shown in FIG. 2 is necessary and sufficient for maintaining the function of the sub magnetic poles 5a to 5f, that is, the function of suppressing the leakage magnetic flux of the main magnetic poles 4a to 4f.
[0018]
First, changes in the magnetic characteristics of the sub magnetic poles 5a to 5f during the operation of the rotating electrical machine 1 according to the first embodiment of the present invention will be described.
[0019]
If the armature reaction is not, the magnetic flux density at the operating point A of the auxiliary pole 5a~5f is B 0. Next, when the rotating electrical machine 1 is operated and the reverse magnetic field −H 1 is applied due to the armature reaction, the permeance line P moves in parallel to the left in the figure, so that the operating points of the sub magnetic poles 5a to 5f are point D. . Further, when the reverse magnetic field −H 1 due to the armature reaction disappears, the operating point of the sub magnetic poles 5 a to 5 f returns from the point D to the point A again on the BH characteristic. That is, no irreversible demagnetization occurs.
[0020]
When the reverse magnetic field −H 2 due to the maximum armature reaction acts, the permeance line P moves in parallel to the left in the figure, and the operating points of the sub magnetic poles 5a to 5f pass through the bending point C to become point E. In this case, even if the reverse magnetic field −H 2 disappears, the operating point of the sub magnetic poles 5a to 5f does not return to the point A, but on the line EA ′ parallel to the line segment CA to the right in the figure, the point A ′. Return to. Point A ′ is the intersection of permeance line P and line segment EA ′. The magnetic flux density at this time is B 1 and is smaller than B 0 . That is, irreversible demagnetization occurs in the sub magnetic poles 5a to 5f, and B 0 -B 1 becomes an irreversible demagnetization amount due to the reverse magnetic field -H 2 due to the armature reaction. Since the BH characteristics of the sub magnetic poles 5a to 5f after the occurrence of irreversible demagnetization are curves A'ET, the function of the sub magnetic poles 5a to 5f, that is, the leakage magnetic flux suppressing function of the main magnetic poles 4a to 4f can be maintained. Can not.
[0021]
Next, selection of materials for the sub magnetic poles 5a to 5f will be described.
[0022]
FIG. 1 shows the BH characteristics of the sub magnetic poles 5a to 5f of the rotating electrical machine 1 when two different types of permanent magnet materials X and Y are used. The BH characteristic of the permanent magnet material Y is the same as the BH characteristic shown in FIG.
[0023]
As shown in FIG. 1, the bending point F in the BH characteristic of the permanent magnet material X is on the left side of the bending point C in the BH characteristic of the permanent magnet material Y, and the coercive force of the permanent magnet material X is It is larger than the coercive force of the permanent magnet material Y.
[0024]
When the reverse magnetic field −H 2 acts due to the maximum armature reaction of the rotating electrical machine 1, the operating point of the sub magnetic poles 5 a to 5 f by the permanent magnet material X is a point G in FIG. This point G is the right side of the bending point F, i.e. since B-H characteristic is in the linear portion, the opposing magnetic field -H 2 is eliminated, the operating point of the sub pole 5a~5f returns to point A. That is, no irreversible demagnetization occurs. Therefore, by adopting the permanent magnet material X having a larger coercive force as the material of the sub magnetic poles 5a to 5f, the irreversible demagnetization of the sub magnetic poles 5a to 5f is performed when the reverse magnetic field −H 2 due to the maximum armature reaction acts. Can be prevented.
[0025]
Here, the maximum armature reaction will be briefly described. In general, the magnitude of the armature reaction in the rotating electrical machine 1 is proportional to the magnitude of the current flowing through the armature coil (not shown). In the case of an engine starter motor, the maximum current that flows through an armature coil (not shown) is the current when the key switch is turned on to energize the rotating electrical machine 1 and the armature is not rotating (so-called Bound current). By the way, the binding current increases as the capacity of the battery (not shown) increases and as the temperature decreases. Therefore, the maximum armature reaction in the rotating electrical machine 1 is maximized by the binding current when combined with the battery having the maximum capacity among the batteries that may be used under the minimum use temperature condition. The magnetic characteristics of the sub magnetic poles 5a to 5f may be calculated based on this value.
[0026]
In the rotary electric machine 1 according to the first embodiment of the present invention described above, the coercive force of the auxiliary magnetic poles 5a to 5f has a coercive force that does not cause irreversible demagnetization even when subjected to a reverse magnetic field due to the maximum armature reaction. By adopting a large permanent magnet material X, the irreversible demagnetization of the sub magnetic poles 5a to 5f is prevented, the leakage magnetic flux suppressing function of the main magnetic poles 4a to 4f of the sub magnetic poles 5a to 5f is maintained, and the output of the rotating electrical machine 1 The decrease could be prevented.
[0027]
On the other hand, the magnitude of the reverse magnetic field due to the maximum armature reaction acting on the main magnetic poles 4a to 4f is smaller than the magnitude of the reverse magnetic field due to the maximum armature reaction acting on the sub magnetic poles 5a to 5f, as shown in FIG. Therefore, even if an inexpensive material having a smaller coercive force than the permanent magnet material X used for the sub magnetic poles 5a to 5f is used for the main magnetic poles 4a to 4f, the main magnetic poles 4a to 4f receive a reverse magnetic field due to the maximum armature reaction. It is possible to prevent irreversible demagnetization. In this case, while suppressing an increase in cost, the irreversible demagnetization of the sub magnetic poles 5a to 5f is prevented, the leakage magnetic flux suppressing function of the main magnetic poles 4a to 4f of the sub magnetic poles 5a to 5f is maintained, and the output of the rotating electrical machine 1 is reduced. Can be prevented.
[0028]
(Second Embodiment)
In the rotating electrical machine 1 according to the second embodiment of the present invention, the material selection method for the sub magnetic poles 5a to 5f is different from that of the first embodiment. That is, in the first embodiment, the selection is made focusing on the coercive force of the permanent magnet material, but in the second embodiment, the selection is made focusing on the magnetic flux density.
[0029]
Below, selection of the material of sub magnetic pole 5a-5f is demonstrated.
[0030]
FIG. 3 shows the BH characteristics of the sub magnetic poles 5a to 5f of the rotating electrical machine 1 when two different types of permanent magnet materials W and Y are used. The BH characteristic of the permanent magnet material Y is the same as the BH characteristic shown in FIG.
[0031]
As shown in FIG. 3, the coercive force is the same for the permanent magnet material W and the permanent magnet material Y. However, regarding the magnetic flux density, the permanent magnet material W is larger than the permanent magnet material Y. If the armature reaction is not, the operating point of the sub pole 5a~5f is a point J, the magnetic flux density at this time is B 2. Further, the bending point K in the BH characteristic of the permanent magnet material W is on the right side of the drawing from the bending point C in the BH characteristic of the permanent magnet material Y.
[0032]
Here, when the reverse magnetic field −H 2 acts due to the maximum armature reaction of the rotating electrical machine 1, the operating points of the sub magnetic poles 5 a to 5 f by the permanent magnet material W pass through the bending point K as shown in FIG. L. Therefore, even if the reverse magnetic field −H 2 disappears, the operating point of the sub magnetic poles 5a to 5f does not return to the point J, but returns to the point M to the right in the drawing on the line LM parallel to the line KJ. Point M is an intersection of permeance line P and line segment LM. The magnetic flux density at this time is B 3 and is smaller than B 2 . That is, irreversible demagnetization occurs in the sub magnetic poles 5a to 5f, and B 2 -B 3 becomes an irreversible demagnetization amount due to the reverse magnetic field −H 2 due to the maximum armature reaction. However, even after irreversible demagnetization occurs, the BH characteristics of the sub magnetic poles 5a to 5f become the curve MLT, which is a necessary and sufficient condition for maintaining the leakage magnetic flux suppressing function of the main magnetic poles 4a to 4f of the sub magnetic poles 5a to 5f. Since it exceeds a certain curve ACT, the sub magnetic poles 5a to 5f can maintain the leakage magnetic flux suppressing function of the main magnetic poles 4a to 4f. Thereafter, no matter how many times the reverse magnetic field -H2 due to the maximum armature reaction is received, the BH characteristics of the sub magnetic poles 5a to 5f are stabilized at the curve MLT.
[0033]
In the rotating electrical machine 1 according to the second embodiment of the present invention described above, the magnetic flux density is not less than a predetermined value even after irreversible demagnetization occurs due to the maximum armature reaction in the sub magnetic poles 5a to 5f. By adopting the permanent magnet material W having a high magnetic flux density, it is possible to maintain the leakage magnetic flux suppressing function of the main magnetic poles 4a to 4f of the sub magnetic poles 5a to 5f and prevent the output of the rotating electrical machine 1 from being lowered.
[0034]
On the other hand, the magnitude of the reverse magnetic field due to the maximum armature reaction acting on the main magnetic poles 4a to 4f is smaller than the magnitude of the reverse magnetic field due to the maximum armature reaction acting on the sub magnetic poles 5a to 5f, as shown in FIG. Therefore, even if an inexpensive material having a smaller magnetic flux density than the permanent magnet material W used for the sub magnetic poles 5a to 5f is used for the main magnetic poles 4a to 4f, the main magnetic poles 4a to 4f after occurrence of irreversible demagnetization due to the maximum armature reaction. The magnetic flux density can be a predetermined value or more. In this case, while suppressing an increase in cost, the leakage magnetic flux suppressing function of the main magnetic poles 4a to 4f of the sub magnetic poles 5a to 5f can be maintained, and a decrease in the output of the rotating electrical machine 1 can be prevented.
[0035]
Further, in the rotating electrical machine 1 according to the first embodiment or the second embodiment of the present invention, as shown in FIG. 5, the soft magnetic bodies 9a to 9f are interposed between the main magnetic poles 4a to 4f and the sub magnetic poles 5a to 5f. (For example, soft iron) may be inserted.
[Brief description of the drawings]
FIG. 1 shows respective BH characteristics when two different kinds of permanent magnet materials X and Y are used in the sub magnetic poles 5a to 5f of the rotating electrical machine 1 according to the first embodiment of the present invention.
FIG. 2 is a diagram showing BH characteristics of sub magnetic poles 5a to 5f of the rotating electrical machine 1 according to the first embodiment of the present invention.
FIG. 3 shows respective BH characteristics when two different types of permanent magnet materials W and Y are used in the sub magnetic poles 5a to 5f of the rotating electrical machine 1 according to the second embodiment of the present invention.
FIG. 4 is a schematic radial sectional view of the rotating electrical machine 1 according to the first embodiment of the present invention.
FIG. 5 is a schematic radial cross-sectional view of a modified example of the rotating electrical machine 1 according to the first embodiment or a modified example of the second embodiment.
FIG. 6 is a development view of a field and an armature in a general permanent magnet field type rotating electric machine, and an explanatory diagram showing a magnetic flux distribution due to an armature reaction corresponding thereto.
[Explanation of symbols]
1 rotary electric machine 2 yoke 3 field magnetic pole 4a~4f main magnetic 5a~5f auxiliary magnetic pole 6 armature 7 shaft 8 cores 9a~9f soft magnetic A operating point A 'operating point B the magnetic flux density B 0 .about.B 3 flux density Br Residual magnetic flux density C Bending point D Operating point E Operating point F Bending point G Operating point H Magnetic field strength, magnetic flux J Operating point K Bending point L Operating point M Operating point P Permeance wire W Permanent magnet X Permanent magnet Y Permanent magnet

Claims (3)

ヨーク内周面に周方向一定間隔を隔てて極性交互に配設される永久磁石からなると共に各磁極面が電機子に対面して形成される複数の主磁極と、
前記主磁極間に配設され隣接する前記主磁極の電機子側の前記磁極面の極性と同極性の一対の磁極面を周方向両端面に有する永久磁石からなる副磁極と、を備える回転電機において、
前記副磁極の残留磁束密度を、前記回転電機運転時の最大電機子反作用による前記副磁極の不可逆減磁発生後の残留磁束密度が所定の値以上となるような値に設定したことを特徴とする回転電機。
A plurality of main magnetic poles formed of permanent magnets alternately arranged with a certain interval in the circumferential direction on the inner circumferential surface of the yoke and each magnetic pole surface facing the armature;
A rotating electric machine comprising: a sub-magnetic pole made of a permanent magnet having a pair of magnetic pole faces having the same polarity as the polarity of the magnetic pole face on the armature side of the adjacent main pole arranged between the main magnetic poles; In
The residual magnetic flux density of the auxiliary magnetic pole is set to a value such that the residual magnetic flux density after occurrence of irreversible demagnetization of the auxiliary magnetic pole due to the maximum armature reaction during operation of the rotating electric machine becomes a predetermined value or more. Rotating electric machine.
前記副磁極の残留磁束密度を、前記主磁極の磁束密度より大きい値に設定したことを特徴とする請求項1に記載の回転電機。The rotating electrical machine according to claim 1 , wherein the residual magnetic flux density of the sub magnetic pole is set to a value larger than the magnetic flux density of the main magnetic pole. 前記最大電機子反作用は回転電機始動時における拘束電流によるものであることを特徴とする請求項1または請求項2に記載の回転電機。 3. The rotating electrical machine according to claim 1, wherein the maximum armature reaction is caused by a restraining current when starting the rotating electrical machine.
JP2000327290A 2000-10-26 2000-10-26 Rotating electric machine Expired - Fee Related JP3690261B2 (en)

Priority Applications (4)

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JP2000327290A JP3690261B2 (en) 2000-10-26 2000-10-26 Rotating electric machine
US09/977,679 US6465925B2 (en) 2000-10-26 2001-10-16 Rotary electric machine having auxiliary poles
DE10152538A DE10152538A1 (en) 2000-10-26 2001-10-24 Rotating electrical machine with auxiliary poles
IT2001RM000629A ITRM20010629A1 (en) 2000-10-26 2001-10-24 ELECTRIC ROTARY MACHINE WITH AUXILIARY POLES.

Applications Claiming Priority (1)

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