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JP2006262603A - Rotary electric machine - Google Patents

Rotary electric machine Download PDF

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Publication number
JP2006262603A
JP2006262603A JP2005075655A JP2005075655A JP2006262603A JP 2006262603 A JP2006262603 A JP 2006262603A JP 2005075655 A JP2005075655 A JP 2005075655A JP 2005075655 A JP2005075655 A JP 2005075655A JP 2006262603 A JP2006262603 A JP 2006262603A
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Prior art keywords
magnet
stator
main
circumferential
auxiliary magnet
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Inventor
Takahiro Nakayama
孝博 中山
Makoto Morizaki
誠 森▲崎▼
義之 ▲高▼部
Yoshiyuki Takabe
Yoshito Nishikawa
義人 西川
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Asmo Co Ltd
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Asmo Co Ltd
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a rotary electric machine in which torque ripples can be reduced, using a simple arrangement. <P>SOLUTION: The rotary electric machine 1 comprises a stator 2 arranged with a winding 6, and a rotor 3 where a main magnet 9 magnetized in the radial direction and an auxiliary magnet 10, magnetized in a direction other than the radial direction, are provided alternately in the circumferential direction on a rotor core 8 supported rotatably for the stator 2. The circumferential width Wr of the stator 2 side side face of the main magnet 9 is set narrower than the circumferential width Ws of the side face of the stator 2 side of the auxiliary magnet 10, arranged in the circumferential direction between the main magnets 9. One auxiliary magnet 10 is provided between respective main magnets 9. <P>COPYRIGHT: (C)2006,JPO&NCIPI

Description

本発明は、回転電機に関するものである。   The present invention relates to a rotating electrical machine.

従来、特許文献1に開示されているように、回転子に設けられた永久磁石をハルバッハ配列とした回転電機が提案されている。永久磁石をハルバッハ配列とすることで、特定の方向の磁力を強めることができ、例えば同量の磁石で形成された通常配列の磁石と比較して、マグネットトルクを多く利用することができる。このため、回転電機を大きくすることなく高出力化を図ることができる。   Conventionally, as disclosed in Patent Document 1, a rotating electrical machine in which permanent magnets provided on a rotor are arranged in a Halbach array has been proposed. By making the permanent magnets in the Halbach arrangement, the magnetic force in a specific direction can be increased, and for example, a larger amount of magnet torque can be used compared to a normal arrangement magnet formed of the same amount of magnets. For this reason, high output can be achieved without increasing the size of the rotating electrical machine.

ここで、永久磁石がハルバッハ配列とされた回転電機の一例を図8に示す。図8に示す回転電機20は、巻線が配設された固定子21と、永久磁石22を有する回転子23とを備えており、永久磁石22は、ラジアル方向に着磁された主磁石24と、主磁石24の磁極方向と直角方向に着磁された補助磁石25とを備えている。この構成により、永久磁石22のエアギャップ側の磁力を強めることができるため、例えば永久磁石が補助磁石を含まない場合と比較して、同じ磁石量で高出力化を図ることができる。   Here, an example of a rotating electrical machine in which the permanent magnets are arranged in a Halbach array is shown in FIG. The rotating electrical machine 20 shown in FIG. 8 includes a stator 21 provided with windings and a rotor 23 having a permanent magnet 22, and the permanent magnet 22 is a main magnet 24 magnetized in the radial direction. And an auxiliary magnet 25 magnetized in a direction perpendicular to the magnetic pole direction of the main magnet 24. With this configuration, since the magnetic force on the air gap side of the permanent magnet 22 can be increased, for example, compared with a case where the permanent magnet does not include an auxiliary magnet, higher output can be achieved with the same magnet amount.

このような回転電機における特性の向上が望まれており、例えば特許文献2には、永久磁石を多分割化した回転電機が提案されている。この構成とすれば、回転電機におけるエアギャップ部での表面磁束密度分布が正弦波に近づくため、コギングトルクを低減し低リップル化を図ることができる。
特開平11−308793号公報 特開2002−354721号公報
For example, Patent Document 2 proposes a rotating electrical machine in which a permanent magnet is divided into multiple parts. With this configuration, the surface magnetic flux density distribution in the air gap portion of the rotating electrical machine approaches a sine wave, so that the cogging torque can be reduced and the ripple can be reduced.
JP 11-308793 A JP 2002-354721 A

しかしながら、特許文献2の構成であると、多くの永久磁石を組み付ける必要があるため、磁石をそれぞれ高精度で形成する必要があるとともに、組み付けのための工程数が増加する。このため、製造が煩雑であり、手間がかかるという問題があった。また、回転子の表面磁束密度分布が正弦波に近づくといっても、やはりトルクリップルは発生するという問題があった。   However, with the configuration of Patent Document 2, it is necessary to assemble a large number of permanent magnets, so that it is necessary to form the magnets with high accuracy, and the number of steps for assembly increases. For this reason, there existed a problem that manufacture was complicated and time-consuming. Even if the surface magnetic flux density distribution of the rotor approaches a sine wave, there is still a problem that torque ripple occurs.

本発明は、上記課題を解決するためになされたものであって、その目的は、簡易な構成でトルクリップルを低減することができる回転電機を提供することにある。   The present invention has been made to solve the above-described problems, and an object thereof is to provide a rotating electrical machine capable of reducing torque ripple with a simple configuration.

上記課題を解決するため、請求項1に記載の発明は、巻線が配設された固定子と、前記固定子に対して回転可能に支持されたロータコアに、ラジアル方向に着磁された主磁石とラジアル方向以外に着磁された補助磁石とが周方向に交互に設けられてなる回転子と、を備えた回転電機であって、前記主磁石は、前記固定子側の側面の周方向幅が、周方向に前記主磁石の間に配置された前記補助磁石の固定子側の側面の周方向幅よりも小さくなるように設定されている。   In order to solve the above-mentioned problem, the invention according to claim 1 is characterized in that a main body magnetized in a radial direction on a stator provided with windings and a rotor core supported rotatably with respect to the stator. A rotating electrical machine including a magnet and auxiliary magnets magnetized in a direction other than the radial direction, wherein the main magnet is a circumferential direction of a side surface on the stator side. The width is set to be smaller than the circumferential width of the side surface on the stator side of the auxiliary magnet arranged between the main magnets in the circumferential direction.

請求項2に記載の発明は、請求項1に記載の回転電機において、前記補助磁石は、前記各主磁石間にそれぞれ1つ設けられている。
請求項3に記載の発明は、請求項1又は2に記載の回転電機において、前記補助磁石は、該補助磁石の径方向に延びる中心線に対して直角方向に着磁されている。
According to a second aspect of the present invention, in the rotating electric machine according to the first aspect, one auxiliary magnet is provided between the main magnets.
According to a third aspect of the present invention, in the rotating electrical machine according to the first or second aspect, the auxiliary magnet is magnetized in a direction perpendicular to a center line extending in a radial direction of the auxiliary magnet.

請求項4に記載の発明は、請求項1乃至3のいずれか1項に記載の回転電機において、前記各主磁石は、前記固定子側の側面の周方向幅Wrが、磁極ピッチ幅Pに対して、0.2P<Wr<0.5Pとなる磁石形状を有する。   According to a fourth aspect of the present invention, in the rotating electrical machine according to any one of the first to third aspects, the main magnet has a circumferential width Wr on the side surface on the stator side that is a magnetic pole pitch width P. On the other hand, it has a magnet shape such that 0.2P <Wr <0.5P.

請求項5に記載の発明は、請求項1乃至4のいずれか1項に記載の回転電機において、前記主磁石は、径方向に延びる中心線から周方向両端部にかけて、徐々に磁束量が小さくなるように形成されている。   According to a fifth aspect of the present invention, in the rotating electrical machine according to any one of the first to fourth aspects, the amount of magnetic flux of the main magnet gradually decreases from a center line extending in the radial direction to both ends in the circumferential direction. It is formed to become.

請求項6に記載の発明は、請求項1乃至5のいずれか1項に記載の回転電機において、前記固定子は、スロットレスである。
請求項7に記載の発明は、巻線が配設された固定子と、前記固定子に対して回転可能に支持されたロータコアに、ラジアル方向に着磁された主磁石とラジアル方向以外に着磁された補助磁石とが周方向に交互に設けられてなる回転子と、を備えた回転電機であって、前記主磁石は、周方向両端面がなす角度が、周方向に前記主磁石の間に配置された前記補助磁石の周方向両端面がなす角度よりも小さくなるように設定されている。
According to a sixth aspect of the present invention, in the rotating electrical machine according to any one of the first to fifth aspects, the stator is slotless.
According to a seventh aspect of the present invention, a main magnet magnetized in a radial direction and a rotor magnet other than the radial direction are attached to a stator provided with windings and a rotor core supported rotatably with respect to the stator. A rotating electric machine including a rotor with magnetized auxiliary magnets provided alternately in the circumferential direction, wherein the main magnet has an angle formed between the circumferential end surfaces of the main magnet in the circumferential direction. It is set to be smaller than the angle formed by the circumferential end surfaces of the auxiliary magnets disposed therebetween.

(作用)
請求項1に記載の発明によれば、主磁石は、固定子側の側面の周方向幅が、周方向に主磁石の間に配置された補助磁石の固定子側の側面の周方向幅よりも小さくなるように設定されている。このため、主磁石と補助磁石との境目部分、即ち、主磁石からの磁束と補助磁石からの磁束とがぶつかりあい表面磁束がピークとなる部位が、主磁石の前記周方向幅と補助磁石の前記周方向幅とが等しい場合と比較して近づく。この結果、表面磁束密度分布が正弦波に近づくため、トルクリップルを低減することができる。また、主磁石の固定子側の側面の周方向幅を補助磁石の固定子側の側面の周方向幅よりも小さくするのみの構成であるため、磁極数に対して磁石数を増加させるなどの必要がない。従って、簡易な構成でトルクリップルを低減することができる。
(Function)
According to the first aspect of the present invention, the main magnet has a circumferential width on the side surface on the stator side that is greater than a circumferential width on the side surface on the stator side of the auxiliary magnet disposed between the main magnets in the circumferential direction. Is set to be smaller. For this reason, the boundary portion between the main magnet and the auxiliary magnet, that is, the portion where the magnetic flux from the main magnet and the magnetic flux from the auxiliary magnet collide and the surface magnetic flux peaks, the circumferential width of the main magnet and the auxiliary magnet It approaches as compared with the case where the circumferential width is equal. As a result, since the surface magnetic flux density distribution approaches a sine wave, torque ripple can be reduced. Moreover, since the circumferential width of the side surface on the stator side of the main magnet is only made smaller than the circumferential width of the side surface on the stator side of the auxiliary magnet, the number of magnets is increased with respect to the number of magnetic poles, etc. There is no need. Therefore, torque ripple can be reduced with a simple configuration.

請求項2に記載の発明によれば、補助磁石は、各主磁石間にそれぞれ1つ設けられているため、例えば各主磁石間に補助磁石が周方向に複数に形成された場合と比較して、部品点数を低減することができ、しかも補助磁石を形成するために高精度の加工が必要とされない。   According to the invention described in claim 2, since one auxiliary magnet is provided between each main magnet, for example, compared with a case where a plurality of auxiliary magnets are formed between the main magnets in the circumferential direction. Thus, the number of parts can be reduced, and high-precision machining is not required to form the auxiliary magnet.

請求項3に記載の発明によれば、補助磁石の着磁方向は補助磁石の径方向に延びる中心線に対して直角方向とされているため、回転子が正逆何れの方向に回転しても回転力が変わらない。このため、正逆方向ともに出力性能が同じ回転電機とすることができる。   According to the third aspect of the present invention, the magnetizing direction of the auxiliary magnet is perpendicular to the center line extending in the radial direction of the auxiliary magnet, so the rotor rotates in either the forward or reverse direction. The rotational force does not change. For this reason, it can be set as the rotary electric machine with the same output performance in the forward / reverse direction.

請求項4に記載の発明によれば、主磁石の固定子側の側面の周方向幅Wrが、磁極ピッチ幅Pに対して0.2P<Wr<0.5Pとされることで、主磁石の周方向幅を補助磁石の周方向幅よりも大きくする場合と比較して、出力トルクを保持しながら、トルクリップルを低減することができる。   According to the fourth aspect of the present invention, the circumferential width Wr of the side surface on the stator side of the main magnet is 0.2P <Wr <0.5P with respect to the magnetic pole pitch width P, whereby the main magnet As compared with the case where the circumferential width of the auxiliary magnet is made larger than the circumferential width of the auxiliary magnet, the torque ripple can be reduced while maintaining the output torque.

請求項5に記載の発明によれば、主磁石は補助磁石との境目部分に近づくに従って磁束量が小さくなるように形成されているため、この部分に発生する磁束量のピークが低減され、表面磁束密度分布がより正弦波に近づく。このため、よりトルクリップルを低減することができる。   According to the fifth aspect of the present invention, since the main magnet is formed so that the amount of magnetic flux decreases as it approaches the boundary portion with the auxiliary magnet, the peak of the amount of magnetic flux generated in this portion is reduced, and the surface The magnetic flux density distribution is closer to a sine wave. For this reason, torque ripple can be further reduced.

請求項6に記載の発明によれば、固定子がスロットレスとされることで、回転子がスムーズに回転し、よりトルクリップルを低減することができる。
請求項7に記載の発明によれば、主磁石は、周方向両端面がなす角度が、周方向に主磁石の間に配置された補助磁石の周方向両端面がなす角度よりも小さくなるように設定されている。このため、主磁石と補助磁石との境目部分、即ち、主磁石からの磁束と補助磁石からの磁束とがぶつかりあい表面磁束がピークとなる部位が、主磁石の前記角度と補助磁石の前記角度とが等しい場合と比較して近づく。この結果、表面磁束密度分布が正弦波に近づくため、トルクリップルを低減することができる。また、主磁石の周方向両端面がなす角度を補助磁石の周方向両端面がなす角度よりも小さくするのみの構成であるため、磁極数に対して磁石数を増加させるなどの必要がない。従って、簡易な構成でトルクリップルを低減することができる。
According to the sixth aspect of the present invention, since the stator is slotless, the rotor rotates smoothly and torque ripple can be further reduced.
According to the seventh aspect of the present invention, the angle formed by the circumferential end surfaces of the main magnet is smaller than the angle formed by the circumferential end surfaces of the auxiliary magnets disposed between the main magnets in the circumferential direction. Is set to For this reason, the boundary between the main magnet and the auxiliary magnet, that is, the portion where the magnetic flux from the main magnet and the magnetic flux from the auxiliary magnet collide with each other and the surface magnetic flux reaches its peak is the angle of the main magnet and the angle of the auxiliary magnet. Compared to the case where and are equal. As a result, since the surface magnetic flux density distribution approaches a sine wave, torque ripple can be reduced. Further, since the angle formed by the circumferential end surfaces of the main magnet is merely made smaller than the angle formed by the circumferential end surfaces of the auxiliary magnet, there is no need to increase the number of magnets with respect to the number of magnetic poles. Therefore, torque ripple can be reduced with a simple configuration.

本発明によれば、簡易な構成でトルクリップルを低減することができる。   According to the present invention, torque ripple can be reduced with a simple configuration.

以下、本発明を具体化した一実施の形態について、図面を参照して説明する。
図1に示すように、本実施の形態の回転電機1は、固定子2と、回転子3とを備えている。
Hereinafter, an embodiment of the present invention will be described with reference to the drawings.
As shown in FIG. 1, the rotating electrical machine 1 according to the present embodiment includes a stator 2 and a rotor 3.

固定子2は、略円筒形状に形成されたステータコア4と、ステータコア4の内側に放射状に形成された複数の(本実施形態では12個)のティース5と、これらティース5に巻装された巻線6とを備えている。この巻線6は図示しない電源装置に接続されており、電源供給されることで回転子3を回転させる回転磁界を発生させるように構成されている。   The stator 2 includes a stator core 4 formed in a substantially cylindrical shape, a plurality (12 in this embodiment) of teeth 5 formed radially inside the stator core 4, and a winding wound around the teeth 5. Line 6. The winding 6 is connected to a power supply device (not shown), and is configured to generate a rotating magnetic field that rotates the rotor 3 when supplied with power.

回転子3は、固定子2の内側に回転可能に支持されている。回転子3は、回転軸7を中心に固定子2に対して回転可能に設けられたロータコア8に、主磁石9と補助磁石10とが周方向に交互に設けられて形成されている。各主磁石9と補助磁石10との境目は、径方向となるように形成されている。主磁石9はラジアル方向に着磁されており、補助磁石10は、回転軸7と直交する平面上において、補助磁石10の径方向に延びる中心線Lsに対して直角方向に着磁されている。尚、主磁石9は周方向にわたって均一に着磁されており、補助磁石10は径方向に均一に着磁されているものである。本実施の形態では、回転子3は、8極表面磁石形の回転子とされており、補助磁石10は各主磁石9間にそれぞれ1つ設けられている。また、主磁石9の固定子2側(外周側)の側面の周方向幅Wrは、補助磁石10の固定子側(外周側)の側面の周方向幅Wsよりも小さくなるように設定されている。詳しくは、主磁石9の周方向両側に形成された補助磁石10の径方向に延びる中心線Ls間の周方向幅を磁極ピッチ幅Pとすると、主磁石9は、周方向幅Wrが、磁極ピッチ幅Pに対して、0.2P<Wr<0.5Pとなるように形成されている。尚、周方向に配置された複数の主磁石9及び補助磁石10は一体的に形成されており、略円筒形状の磁性体が着磁されることで形成されている。   The rotor 3 is rotatably supported inside the stator 2. The rotor 3 is formed by alternately providing main magnets 9 and auxiliary magnets 10 in the circumferential direction on a rotor core 8 provided to be rotatable with respect to the stator 2 around a rotation shaft 7. The boundary between each main magnet 9 and auxiliary magnet 10 is formed to be in the radial direction. The main magnet 9 is magnetized in the radial direction, and the auxiliary magnet 10 is magnetized in a direction perpendicular to the center line Ls extending in the radial direction of the auxiliary magnet 10 on a plane orthogonal to the rotating shaft 7. . The main magnet 9 is uniformly magnetized in the circumferential direction, and the auxiliary magnet 10 is uniformly magnetized in the radial direction. In the present embodiment, the rotor 3 is an 8-pole surface magnet type rotor, and one auxiliary magnet 10 is provided between each main magnet 9. Further, the circumferential width Wr of the side surface on the stator 2 side (outer peripheral side) of the main magnet 9 is set to be smaller than the circumferential width Ws of the side surface on the stator side (outer peripheral side) of the auxiliary magnet 10. Yes. Specifically, when the circumferential width between the center lines Ls extending in the radial direction of the auxiliary magnet 10 formed on both sides in the circumferential direction of the main magnet 9 is a magnetic pole pitch width P, the main magnet 9 has a circumferential width Wr. The pitch width P is formed so that 0.2P <Wr <0.5P. The plurality of main magnets 9 and auxiliary magnets 10 arranged in the circumferential direction are integrally formed, and are formed by magnetizing a substantially cylindrical magnetic body.

実施例として、上記の構成の回転電機1について実測を行った。
先ず、回転電機1の表面磁束密度分布を測定した。比較のために、8極表面磁石形の回転電機として、図8に示す従来例の回転電機20と、図9に示す比較例としての回転電機30とを用いて表面磁束密度分布を測定した。なお、回転電機20,30について、永久磁石22,32の体積を、実施例の主磁石9及び補助磁石10をあわせた体積と同じとし、磁極ピッチ幅を同一にして測定を行った。回転電機20は、主磁石24の固定子21側の側面の周方向幅が補助磁石25の固定子21側の側面の周方向幅と略同じである点で本実施例の回転電機1と構成が異なる。また、比較例の回転電機30は、回転子31の永久磁石32が主磁石33のみで構成されており、補助磁石を含まない点で本実施例の回転電機1と構成が異なる。つまり、回転電機30の永久磁石32はラジアル方向に着磁された磁石のみで形成されている。
As an example, the rotating electrical machine 1 having the above configuration was measured.
First, the surface magnetic flux density distribution of the rotating electrical machine 1 was measured. For comparison, the surface magnetic flux density distribution was measured using a conventional rotating electrical machine 20 shown in FIG. 8 and a rotating electrical machine 30 as a comparative example shown in FIG. 9 as an 8-pole surface magnet type rotating electrical machine. In addition, about the rotary electric machines 20 and 30, the volume of the permanent magnets 22 and 32 was made the same as the volume which combined the main magnet 9 and the auxiliary magnet 10 of the Example, and it measured by making magnetic pole pitch width the same. The rotating electrical machine 20 is configured in the same manner as the rotating electrical machine 1 of the present embodiment in that the circumferential width of the side surface of the main magnet 24 on the stator 21 side is substantially the same as the circumferential width of the side surface of the auxiliary magnet 25 on the stator 21 side. Is different. Further, the rotating electrical machine 30 of the comparative example is different from the rotating electrical machine 1 of the present embodiment in that the permanent magnet 32 of the rotor 31 is composed only of the main magnet 33 and does not include an auxiliary magnet. That is, the permanent magnet 32 of the rotating electrical machine 30 is formed only of magnets magnetized in the radial direction.

その結果を図2に示す。ここでは、1極対分に相当する90°分を電気角360゜分として表示している。図2に示すように、回転電機30では、磁束密度分布は矩形波状の分布となった。また、回転電機20では磁束密度分布は正弦波形状に近づき、回転電機1で磁束密度分布はより正弦波形状に近づいた。   The result is shown in FIG. Here, 90 ° corresponding to one pole pair is displayed as an electrical angle of 360 °. As shown in FIG. 2, in the rotating electrical machine 30, the magnetic flux density distribution is a rectangular wave distribution. Further, in the rotating electrical machine 20, the magnetic flux density distribution approaches a sine wave shape, and in the rotating electrical machine 1, the magnetic flux density distribution approaches a sine wave shape.

また、図2に示す磁束密度分布から波形解析を行った結果を図3に示す。図3は、表面磁束密度分布に含まれる高調波成分の強度を示しており、比較例の回転電機30における高調波成分を基準として、それに対する比率で実施例及び従来例の高調波成分を示している。   Moreover, the result of having performed waveform analysis from magnetic flux density distribution shown in FIG. 2 is shown in FIG. FIG. 3 shows the intensity of the harmonic component included in the surface magnetic flux density distribution, and shows the harmonic component of the example and the conventional example in a ratio with respect to the harmonic component in the rotating electrical machine 30 of the comparative example. ing.

図3に示すように、1次の基本成分は、比較例、従来例と比較して、実施例が最も大きくなった。この結果により、本実施例の回転電機1では、従来例の回転電機20と比較して、大きな回転トルクを発生できるものと考えられる。また、実施例では、従来例と比較して、高調波成分が高次側に移動している。この結果により、本実施例の回転電機1では、コギングトルクを低減できると考えられる。   As shown in FIG. 3, the example of the primary basic component was the largest in comparison with the comparative example and the conventional example. From this result, it is considered that the rotating electrical machine 1 of the present embodiment can generate a larger rotational torque than the rotating electrical machine 20 of the conventional example. In the embodiment, compared with the conventional example, the harmonic component is moved to the higher order side. From this result, it is considered that the cogging torque can be reduced in the rotating electrical machine 1 of the present embodiment.

また、補助磁石10の固定子2側の側面の周方向幅Wsに対するトルクリップル及び出力トルクの変化を図4に示す。図4に示すように、周方向幅Wsが0.5P(即ち、従来例の回転電機20における補助磁石25の固定子21側の側面の周方向幅)よりも大きくなるに従い、トルクリップルは徐々に低減された。そして、周方向幅Wsが0.8Pよりも大きくなると、トルクリップルが増加傾向となった。   FIG. 4 shows changes in torque ripple and output torque with respect to the circumferential width Ws of the side surface of the auxiliary magnet 10 on the stator 2 side. As shown in FIG. 4, the torque ripple gradually increases as the circumferential width Ws becomes larger than 0.5P (that is, the circumferential width of the side surface on the stator 21 side of the auxiliary magnet 25 in the conventional rotating electrical machine 20). Reduced to When the circumferential width Ws becomes larger than 0.8P, the torque ripple tends to increase.

この結果により、補助磁石10の周方向幅Wsが0.5P<Ws<0.8Pの範囲にあるとき、即ち、主磁石9の周方向幅Wrが0.2P<Wr<0.5Pの範囲にあるとき、従来例の回転電機20の場合と比較して、トルクリップルの発生を抑制できることが確認できた。なお、図4に示すように、補助磁石10の周方向幅Wsが0.5P<Ws<0.8Pの範囲にあるとき、出力トルクは低下傾向にあるが、ほぼ保持されていた。   As a result, when the circumferential width Ws of the auxiliary magnet 10 is in the range of 0.5P <Ws <0.8P, that is, the circumferential width Wr of the main magnet 9 is in the range of 0.2P <Wr <0.5P. It was confirmed that the occurrence of torque ripple can be suppressed as compared with the conventional rotating electrical machine 20. As shown in FIG. 4, when the circumferential width Ws of the auxiliary magnet 10 is in the range of 0.5P <Ws <0.8P, the output torque tends to decrease, but is almost maintained.

次に、上記実施の形態の特徴的な作用効果を以下に記載する。
(1)主磁石9は、固定子2側の側面の周方向幅Wrが、周方向に主磁石9の間に配置された補助磁石10の固定子2側の側面の周方向幅Wsよりも小さくなるように設定されている。このため、主磁石9と補助磁石10との境目部分、即ち、主磁石9からの磁束と補助磁石10からの磁束とがぶつかりあい表面磁束がピークとなる部位が、主磁石の前記周方向幅と補助磁石の前記周方向幅とが等しい場合と比較して近づく。この結果、表面磁束密度分布が正弦波に近づくため、トルクリップルを低減することができる。また、主磁石9の固定子2側の側面の周方向幅Wrを補助磁石10の固定子2側の側面の周方向幅Wsよりも小さくするのみの構成であるため、磁極数に対して磁石数を増加させるなどの必要がない。従って、簡易な構成でトルクリップルを低減することができる。
Next, characteristic effects of the above embodiment will be described below.
(1) In the main magnet 9, the circumferential width Wr of the side surface on the stator 2 side is larger than the circumferential width Ws of the side surface on the stator 2 side of the auxiliary magnet 10 disposed between the main magnets 9 in the circumferential direction. It is set to be smaller. For this reason, the boundary portion between the main magnet 9 and the auxiliary magnet 10, that is, the portion where the magnetic flux from the main magnet 9 and the magnetic flux from the auxiliary magnet 10 collide with each other and the surface magnetic flux reaches its peak is the circumferential width of the main magnet. Compared with the case where the circumferential width of the auxiliary magnet is equal. As a result, since the surface magnetic flux density distribution approaches a sine wave, torque ripple can be reduced. In addition, since the circumferential width Wr of the side surface of the main magnet 9 on the stator 2 side is only made smaller than the circumferential width Ws of the side surface of the auxiliary magnet 10 on the stator 2 side, the number of magnetic poles There is no need to increase the number. Therefore, torque ripple can be reduced with a simple configuration.

(2)補助磁石10は、各主磁石9間にそれぞれ1つ設けられているため、例えば各主磁石間に補助磁石が周方向に複数に形成された場合と比較して、部品点数を低減することができ、しかも補助磁石10を形成するために高精度の加工が必要とされない。   (2) Since one auxiliary magnet 10 is provided between each main magnet 9, for example, the number of parts is reduced compared to a case where a plurality of auxiliary magnets are formed between the main magnets in the circumferential direction. In addition, high-precision processing is not required to form the auxiliary magnet 10.

(3)補助磁石10の着磁方向は補助磁石10の径方向に延びる中心線Lsに対して直角方向とされているため、回転子3が正逆何れの方向に回転しても回転力が変わらない。このため、正逆方向ともに出力性能が同じ回転電機とすることができる。尚、この補助磁石10の着磁方向は、回転軸7と直交する平面上においての方向である。   (3) Since the magnetizing direction of the auxiliary magnet 10 is perpendicular to the center line Ls extending in the radial direction of the auxiliary magnet 10, the rotational force is generated even if the rotor 3 rotates in either forward or reverse direction. does not change. For this reason, it can be set as the rotary electric machine with the same output performance in the forward / reverse direction. The magnetization direction of the auxiliary magnet 10 is a direction on a plane orthogonal to the rotation axis 7.

(4)主磁石9の周方向幅Wrが、磁極ピッチ幅Pに対して0.2P<Wr<0.5Pとされることで、主磁石の周方向幅を補助磁石の周方向幅よりも大きくする場合と比較して、出力トルクを保持しながら、トルクリップルを低減することができる。   (4) Since the circumferential width Wr of the main magnet 9 is 0.2P <Wr <0.5P with respect to the magnetic pole pitch width P, the circumferential width of the main magnet is made larger than the circumferential width of the auxiliary magnet. Compared with the case of increasing the torque ripple, the torque ripple can be reduced while maintaining the output torque.

上記実施の形態は、以下のように変更してもよい。
・上記実施の形態では、主磁石9は周方向にわたって均一に着磁されているものとしたが、周方向に磁束量が変化するように着磁してもよい。例えば、図5(a)に示す上記実施形態の回転電機1を構成する各主磁石9を、図5(b)に示すように、径方向中心線Lrから両端部にかけて、徐々に磁束量が小さくなるように形成してもよい。このように構成すれば、主磁石9は補助磁石10との境目部分に近づくに従って磁束量が小さくなるように形成されているため、この部分に発生する磁束量のピークが低減され、図6に太線で示すように、表面磁束密度分布がより正弦波形状に近づく。このため、よりトルクリップルの低減を図ることができる。
The above embodiment may be modified as follows.
In the above embodiment, the main magnet 9 is uniformly magnetized in the circumferential direction, but may be magnetized so that the amount of magnetic flux changes in the circumferential direction. For example, as shown in FIG. 5B, the amount of magnetic flux gradually increases from the radial center line Lr to both ends of each main magnet 9 constituting the rotating electrical machine 1 of the above embodiment shown in FIG. You may form so that it may become small. With this configuration, the main magnet 9 is formed so that the amount of magnetic flux decreases as it approaches the boundary portion with the auxiliary magnet 10, so that the peak of the amount of magnetic flux generated in this portion is reduced, and FIG. As indicated by the bold line, the surface magnetic flux density distribution approaches a sine wave shape. For this reason, torque ripple can be further reduced.

・上記実施形態では、複数の主磁石9及び補助磁石10は、略円筒形状に一体的に形成されているものとしたが、各主磁石及び補助磁石が径方向に沿った面でそれぞれ分割されたものとしてもよい。   In the above embodiment, the plurality of main magnets 9 and auxiliary magnets 10 are integrally formed in a substantially cylindrical shape, but each main magnet and auxiliary magnet are divided on a surface along the radial direction. It is also good.

・上記実施形態では、複数の主磁石9及び補助磁石10は、略円筒形状に一体的に形成されているものとしたが、軸方向に垂直な面で複数部に分割し、それぞれを適当なスキュー角だけずらしてもよい。この構成とすれば、コギングトルクを低減することができる。   In the above embodiment, the plurality of main magnets 9 and auxiliary magnets 10 are integrally formed in a substantially cylindrical shape, but are divided into a plurality of parts on a plane perpendicular to the axial direction, and each of them is appropriately formed. The skew angle may be shifted. With this configuration, the cogging torque can be reduced.

・主磁石9及び補助磁石10の外周側に、ステンレス等で形成された金属製のカバーをかぶせてもよい。
・周方向に配置された複数の主磁石9と補助磁石10とロータコア8との間に、磁性材料で形成された鉄を挟んでもよい。
A metal cover formed of stainless steel or the like may be placed on the outer peripheral side of the main magnet 9 and the auxiliary magnet 10.
-Iron formed of a magnetic material may be sandwiched between a plurality of main magnets 9, auxiliary magnets 10, and rotor cores 8 arranged in the circumferential direction.

・上記実施の形態では、固定子2はティース5が形成されることでスロットが形成された構成としたが、図7に示すように、固定子2をスロットレスとした回転電機15としてもよい。このように構成すれば、回転子3がスムーズに回転し、よりトルクリップルの低減を図ることができる。   In the above embodiment, the stator 2 has a structure in which slots are formed by forming the teeth 5, but as shown in FIG. 7, the stator 2 may be a rotary electric machine 15 in which the stator 2 is slotless. . If comprised in this way, the rotor 3 will rotate smoothly and it can aim at reduction of a torque ripple more.

・上記実施の形態では、巻線6は集中巻式としたが、分布巻式としてもよい。
・上記実施の形態では、インナロータ型の回転電機について説明したが、本発明をアウトロータ型の回転電機に適用してもよい。その場合、主磁石の内周側面(固定子側の側面)の周方向幅が、補助磁石の内周側面の周方向幅よりも小さくなるように設定すればよい。
In the above embodiment, the winding 6 is a concentrated winding type, but may be a distributed winding type.
In the above embodiment, the inner rotor type rotating electric machine has been described. However, the present invention may be applied to an outrotor type rotating electric machine. In that case, what is necessary is just to set so that the circumferential width of the inner peripheral side surface (side surface on the stator side) of the main magnet is smaller than the circumferential width of the inner peripheral side surface of the auxiliary magnet.

・上記実施形態では、主磁石9の固定子2側の側面の周方向幅Wrが補助磁石10の固定子2側の側面の周方向幅Wsよりも小さくなるように設定したが、主磁石の周方向両端面がなす角度が、補助磁石の周方向両端面がなす角度よりも小さくなるように設定してもよい。   In the above embodiment, the circumferential width Wr of the side surface of the main magnet 9 on the stator 2 side is set to be smaller than the circumferential width Ws of the side surface of the auxiliary magnet 10 on the stator 2 side. You may set so that the angle which the circumferential direction both end surfaces make may become smaller than the angle which the circumferential direction both end surfaces of an auxiliary magnet make.

本実施の形態における回転電機の概略構成図。The schematic block diagram of the rotary electric machine in this Embodiment. 回転電機の電気角−表面磁束密度分布特性図。The electrical angle-surface magnetic flux density distribution characteristic figure of a rotary electric machine. 回転電機の表面磁束密度分布の高調波成分の分布を示す説明図。Explanatory drawing which shows distribution of the harmonic component of the surface magnetic flux density distribution of a rotary electric machine. 補助磁石の固定子側の側面の周方向幅−トルクリップル及び出力トルク特性図。The circumferential direction width-torque ripple and output torque characteristic view of the side surface on the stator side of the auxiliary magnet. (a),(b)は変形例の回転電機の説明図。(A), (b) is explanatory drawing of the rotary electric machine of a modification. 変形例の回転電機の電気角−表面磁束密度分布特性図。The electrical angle-surface magnetic flux density distribution characteristic figure of the rotary electric machine of a modification. 変形例の回転電機の概略構成図。The schematic block diagram of the rotary electric machine of a modification. 従来例の回転電機の概略構成図。The schematic block diagram of the rotary electric machine of a prior art example. 比較例の回転電機の概略構成図。The schematic block diagram of the rotary electric machine of a comparative example.

符号の説明Explanation of symbols

1,15…回転電機、2…固定子、3…回転子、6…巻線、8…ロータコア、9…主磁石、10…補助磁石、Wr…主磁石の固定子側の側面の周方向幅、Ws…補助磁石の固定子側の側面の周方向幅、Lr…主磁石の径方向に延びる中心線、Ls…補助磁石の径方向に延びる中心線、P…磁極ピッチ幅。   DESCRIPTION OF SYMBOLS 1,15 ... Rotary electric machine, 2 ... Stator, 3 ... Rotor, 6 ... Winding, 8 ... Rotor core, 9 ... Main magnet, 10 ... Auxiliary magnet, Wr ... Circumferential width of side surface of main magnet on the stator side , Ws: circumferential width of the side surface on the stator side of the auxiliary magnet, Lr: center line extending in the radial direction of the main magnet, Ls: center line extending in the radial direction of the auxiliary magnet, P: magnetic pole pitch width.

Claims (7)

巻線が配設された固定子と、
前記固定子に対して回転可能に支持されたロータコアに、ラジアル方向に着磁された主磁石とラジアル方向以外に着磁された補助磁石とが周方向に交互に設けられてなる回転子と、
を備えた回転電機であって、
前記主磁石は、前記固定子側の側面の周方向幅が、周方向に前記主磁石の間に配置された前記補助磁石の固定子側の側面の周方向幅よりも小さくなるように設定されていることを特徴とする回転電機。
A stator provided with windings;
A rotor in which a main magnet magnetized in a radial direction and an auxiliary magnet magnetized in a direction other than the radial direction are alternately provided in a circumferential direction on a rotor core supported rotatably with respect to the stator;
A rotating electric machine with
The main magnet is set so that the circumferential width of the side surface on the stator side is smaller than the circumferential width of the side surface on the stator side of the auxiliary magnet disposed between the main magnets in the circumferential direction. Rotating electric machine characterized by that.
請求項1に記載の回転電機において、
前記補助磁石は、前記各主磁石間にそれぞれ1つ設けられていることを特徴とする回転電機。
In the rotating electrical machine according to claim 1,
One auxiliary magnet is provided between the main magnets, respectively.
請求項1又は2に記載の回転電機において、
前記補助磁石は、該補助磁石の径方向に延びる中心線に対して直角方向に着磁されていることを特徴とする回転電機。
In the rotating electrical machine according to claim 1 or 2,
The rotary electric machine is characterized in that the auxiliary magnet is magnetized in a direction perpendicular to a center line extending in a radial direction of the auxiliary magnet.
請求項1乃至3のいずれか1項に記載の回転電機において、
前記各主磁石は、前記固定子側の側面の周方向幅Wrが、磁極ピッチ幅Pに対して、
0.2P<Wr<0.5P
となる磁石形状を有することを特徴とする回転電機。
The rotating electrical machine according to any one of claims 1 to 3,
Each of the main magnets has a circumferential width Wr of the side surface on the stator side with respect to the magnetic pole pitch width P.
0.2P <Wr <0.5P
A rotating electric machine characterized by having a magnet shape.
請求項1乃至4のいずれか1項に記載の回転電機において、
前記主磁石は、径方向に延びる中心線から周方向両端部にかけて、徐々に磁束量が小さくなるように形成されていることを特徴とする回転電機。
The rotating electrical machine according to any one of claims 1 to 4,
The rotating machine is characterized in that the main magnet is formed such that the amount of magnetic flux gradually decreases from a center line extending in the radial direction to both ends in the circumferential direction.
請求項1乃至5のいずれか1項に記載の回転電機において、
前記固定子は、スロットレスであることを特徴とする回転電機。
The rotating electrical machine according to any one of claims 1 to 5,
The rotating electric machine according to claim 1, wherein the stator is slotless.
巻線が配設された固定子と、
前記固定子に対して回転可能に支持されたロータコアに、ラジアル方向に着磁された主磁石とラジアル方向以外に着磁された補助磁石とが周方向に交互に設けられてなる回転子と、
を備えた回転電機であって、
前記主磁石は、周方向両端面がなす角度が、周方向に前記主磁石の間に配置された前記補助磁石の周方向両端面がなす角度よりも小さくなるように設定されていることを特徴とする回転電機。
A stator provided with windings;
A rotor in which a main magnet magnetized in a radial direction and an auxiliary magnet magnetized in a direction other than the radial direction are alternately provided in a circumferential direction on a rotor core supported rotatably with respect to the stator;
A rotating electric machine with
The main magnet is set such that an angle formed by both circumferential end surfaces is smaller than an angle formed by the circumferential end surfaces of the auxiliary magnet disposed between the main magnets in the circumferential direction. Rotating electric machine.
JP2005075655A 2005-03-16 2005-03-16 Rotary electric machine Abandoned JP2006262603A (en)

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US11682935B2 (en) 2020-09-29 2023-06-20 Honda Motor Co., Ltd. Rotary electric machine with rotor having permanent magnets with ratios of total surface area and a stator with tooth having wide ends
US11682934B2 (en) 2020-09-29 2023-06-20 Honda Motor Co., Ltd. Rotary electric machine with rotor having permanent magnets with ratios of total surface area and a stator with tooth having coils with offset from flange portions
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Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2010074112A1 (en) 2008-12-25 2010-07-01 株式会社 東芝 Linear motor
JP2013046460A (en) * 2011-08-23 2013-03-04 Yaskawa Electric Corp Mover of linear motor and linear motor
US9118237B2 (en) 2011-08-23 2015-08-25 Kabushiki Kaisha Yaskawa Denki Mover for a linear motor and linear motor
JP2013094030A (en) * 2011-10-27 2013-05-16 Hokuto Co Ltd Armature coil and synchronous rotary machine
JP2015153790A (en) * 2014-02-11 2015-08-24 日東電工株式会社 Permanent magnet and method of producing permanent magnet
US11682935B2 (en) 2020-09-29 2023-06-20 Honda Motor Co., Ltd. Rotary electric machine with rotor having permanent magnets with ratios of total surface area and a stator with tooth having wide ends
US11682934B2 (en) 2020-09-29 2023-06-20 Honda Motor Co., Ltd. Rotary electric machine with rotor having permanent magnets with ratios of total surface area and a stator with tooth having coils with offset from flange portions
US11695307B2 (en) 2020-09-29 2023-07-04 Honda Motor Co., Ltd. Rotary electric machine with rotor having permanent magnets and stator with teeth having flange portion, expanding portion and base portion

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