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JP6965677B2 - Rotating machine and rotating machine system - Google Patents
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JP6965677B2 - Rotating machine and rotating machine system - Google Patents

Rotating machine and rotating machine system Download PDF

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JP6965677B2
JP6965677B2 JP2017197266A JP2017197266A JP6965677B2 JP 6965677 B2 JP6965677 B2 JP 6965677B2 JP 2017197266 A JP2017197266 A JP 2017197266A JP 2017197266 A JP2017197266 A JP 2017197266A JP 6965677 B2 JP6965677 B2 JP 6965677B2
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armature
yoke
rotor
magnetic flux
permanent magnets
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JP2019071735A (en
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新 草瀬
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Denso Corp
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P25/00Arrangements or methods for the control of AC motors characterised by the kind of AC motor or by structural details
    • H02P25/02Arrangements or methods for the control of AC motors characterised by the kind of AC motor or by structural details characterised by the kind of motor
    • H02P25/022Synchronous motors
    • H02P25/024Synchronous motors controlled by supply frequency
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K1/00Details of the magnetic circuit
    • H02K1/06Details of the magnetic circuit characterised by the shape, form or construction
    • H02K1/22Rotating parts of the magnetic circuit
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K21/00Synchronous motors having permanent magnets; Synchronous generators having permanent magnets
    • H02K21/12Synchronous motors having permanent magnets; Synchronous generators having permanent magnets with stationary armatures and rotating magnets
    • H02K21/14Synchronous motors having permanent magnets; Synchronous generators having permanent magnets with stationary armatures and rotating magnets with magnets rotating within the armatures

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  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Control Of Ac Motors In General (AREA)
  • Iron Core Of Rotating Electric Machines (AREA)
  • Permanent Magnet Type Synchronous Machine (AREA)
  • Permanent Field Magnets Of Synchronous Machinery (AREA)

Description

本発明は、表面磁石型の回転電機及び回転電機システムに関するものである。 The present invention relates to a surface magnet type rotary electric machine and a rotary electric machine system.

永久磁石を用いた回転電機として表面磁石型モータ(SPMモータ)が知られており、その表面磁石型モータは、永久磁石による磁極全体に分布する磁化トルクを利用できることから高性能モータとして普及している。 A surface magnet type motor (SPM motor) is known as a rotary electric machine using a permanent magnet, and the surface magnet type motor has become widespread as a high-performance motor because it can utilize the magnetization torque distributed over the entire magnetic pole by the permanent magnet. There is.

また一方で、磁極の方向を最適化するための技術としてハルバッハ配列(Halbach Array)を用いた磁気回路が知られている。例えば特許文献1には、ホイール駆動回転電機の回転子として、周方向所定ピッチで極性交互に配置されて略径方向に磁化された磁極磁石と、各磁極磁石の間にそれぞれ設けられ、略周方向へ磁化されたヨーク磁石とを有する界磁子を用いた構成が開示されている。 On the other hand, a magnetic circuit using a Halbach Array is known as a technique for optimizing the direction of magnetic poles. For example, in Patent Document 1, as a rotor of a wheel-driven rotary electric machine, magnetic pole magnets that are alternately arranged at predetermined pitches in the circumferential direction and magnetized in the substantially radial direction are provided between the magnetic pole magnets, respectively, and have a substantially circumferential circumference. A configuration using a field magnet having a yoke magnet magnetized in the direction is disclosed.

特開2006−187116号公報Japanese Unexamined Patent Publication No. 2006-187116

ところで、表面磁石型モータは、永久磁石が回転子表面に貼り付けられた界磁子を有し、電機子側から見た磁気抵抗が空気と同程度の大きなものとなっている。そのため、一般に、界磁子を電機子側から定格レベルの電流でコントロールすることは困難であり、これまでには実用技術視点で研究された例も見当たらない。ゆえに、既存の表面磁石型モータでは、誘起電圧が高くなる高速にて出力低下が生じたり、電機子の鉄損が増加したりするなどの問題を抱えるものとなっている。なお、上述したハルバッハ配列を採用した回転電機も、界磁磁界を可変とすることを実現できるものでないと考えられる。 By the way, the surface magnet type motor has a field magnet in which a permanent magnet is attached to the surface of the rotor, and the magnetic resistance seen from the armature side is as large as that of air. Therefore, in general, it is difficult to control the field magnet from the armature side with a rated level current, and no examples have been studied from the viewpoint of practical technology. Therefore, the existing surface magnet type motor has problems such as a decrease in output at a high speed at which the induced voltage becomes high and an increase in iron loss of the armature. It is considered that the rotary electric machine adopting the Halbach array described above cannot realize the variable field magnetic field.

本発明は、上記課題に鑑みてなされたものであり、その主たる目的は、表面磁石型の回転電機において、回転子により生じる界磁磁束を好適に変化させて可変界磁磁束を実現することにある。 The present invention has been made in view of the above problems, and a main object thereof is to realize a variable field magnetic flux by suitably changing the field magnetic flux generated by a rotor in a surface magnet type rotary electric machine. be.

以下、上記課題を解決するための手段、及びその作用効果について説明する。なお以下においては、理解の容易のため、発明の実施の形態において対応する構成の符号を括弧書き等で適宜示すが、この括弧書き等で示した具体的構成に限定されるものではない。 Hereinafter, means for solving the above problems and their actions and effects will be described. In the following, for the sake of easy understanding, the reference numerals of the corresponding configurations in the embodiment of the invention are appropriately shown in parentheses or the like, but the present invention is not limited to the specific configurations shown in the parentheses or the like.

第1の手段は、
回転自在に支持された回転子(12)と、
前記回転子と同軸配置され、多相交流電流が通電される電機子巻線(23)が巻装された電機子(13)と、
を備えた永久磁石側の回転電機(10)であって、
前記回転子は、
磁化方向を径方向とし、かつ前記電機子に対向する極が交互にN極、S極となるようにして周方向に互いに離間された位置に設けられた複数の永久磁石(32)と、
鉄心材よりなり、周方向に隣り合う前記永久磁石の間においてそれら永久磁石の周方向側面どうしを繋ぎ、かつ前記複数の永久磁石を環状に連結するヨーク部材(34)と、
を有しており、
前記電機子巻線における通電の位相制御により、前記永久磁石から前記電機子へ向かう界磁磁束の強さを変更することが可能になっている。
The first means is
Rotor (12) rotatably supported and
An armature (13) that is coaxially arranged with the rotor and is wound with an armature winding (23) that is energized with a multi-phase alternating current.
It is a rotating electric machine (10) on the permanent magnet side equipped with
The rotor
A plurality of permanent magnets (32) provided at positions separated from each other in the circumferential direction so that the magnetization direction is the radial direction and the poles facing the armature are alternately N poles and S poles.
A yoke member (34) made of an iron core material, connecting the peripheral side surfaces of the permanent magnets between the permanent magnets adjacent to each other in the circumferential direction, and connecting the plurality of permanent magnets in an annular shape.
Have and
By controlling the phase of energization in the armature winding, it is possible to change the strength of the field magnetic flux from the permanent magnet to the armature.

上記構成の回転電機において、回転子は、磁化方向(磁極の向き)を径方向とし、かつ電機子に対向する極が交互にN極、S極となるようにして周方向に互いに離間された位置に設けられた複数の永久磁石を有している。そして、その複数の永久磁石は、鉄心であるヨーク部材により、永久磁石の周方向側面どうしが繋がれ(橋絡され)、かつ環状に連結されている。ここで、永久磁石では、電機子側の径方向端面とヨーク部材側の周方向側面とを通じて界磁磁束が流れる構成となっており、電機子巻線の通電により起磁力が生じる場合に、その起磁力の向きと永久磁石ごとの磁極とに応じて、永久磁石にて生じる界磁磁束の分布が異なるものとなる。この場合、隣り合う永久磁石の周方向側面を通じて流れる界磁磁束を好適に変化させることができる。これにより、表面磁石型の回転電機において、回転子により生じる界磁磁束を好適に変化させて可変界磁磁束を実現することができる。 In the rotating electric machine having the above configuration, the rotors are separated from each other in the circumferential direction so that the magnetization direction (direction of the magnetic pole) is the radial direction and the poles facing the armature are alternately N poles and S poles. It has a plurality of permanent magnets provided at the positions. The plurality of permanent magnets are connected (bridged) to each other in the circumferential direction of the permanent magnets by a yoke member which is an iron core, and are connected in an annular shape. Here, the permanent magnet has a configuration in which a field magnetic flux flows through the radial end surface on the armature side and the circumferential side surface on the armature member side, and when the magnetomotive force is generated by the energization of the armature winding, the magnetic flux is generated. The distribution of the field magnetic flux generated by the permanent magnets differs depending on the direction of the magnetomotive force and the magnetic poles of each permanent magnet. In this case, the field magnetic flux flowing through the circumferential side surfaces of the adjacent permanent magnets can be suitably changed. As a result, in the surface magnet type rotary electric machine, the field magnetic flux generated by the rotor can be suitably changed to realize the variable field magnetic flux.

上述した第1の手段について、図12を用いて補足説明をする。図12では、回転子において永久磁石101とヨーク部材102(鉄心)とを直線状に展開して示しており、上側が電機子側、下側が電機子の反対側である。電機子巻線に電流を流すと、破線で示すようにループ状に起磁力が生じる。なお、回転子の周方向における起磁力発生の位置、すなわち各永久磁石101に対する起磁力の向きは、電機子巻線の通電位相に依存したものとなっている。ここで、永久磁石101では、図12(a)に示すように、磁石磁束の向き(磁石のN→Sの向き)と電機子巻線の起磁力の向きとが同じになる場合と、(b)に示すように、磁石磁束の向きと電機子巻線の起磁力の向きとが逆になる場合とがあり、そのうち(b)の場合には界磁磁束が弱められる。また、ヨーク部材102では、その両隣となる2つの永久磁石101の磁束の向きに応じて、径方向において電機子に近い側と遠い側とで内部磁束の向きが相違している。かかる場合、図12の(a)、(b)に示すように、電機子巻線の起磁力、すなわち電機子巻線の通電位相に応じて、界磁磁束の強さが相違することになる。これにより、可変界磁回転電機を実現することができる。 The first means described above will be supplementarily described with reference to FIG. In FIG. 12, the permanent magnet 101 and the yoke member 102 (iron core) are linearly developed and shown in the rotor, the upper side is the armature side, and the lower side is the opposite side of the armature. When an electric current is passed through the armature winding, a magnetomotive force is generated in a loop shape as shown by the broken line. The position where the magnetomotive force is generated in the circumferential direction of the rotor, that is, the direction of the magnetomotive force with respect to each permanent magnet 101 depends on the energization phase of the armature winding. Here, in the permanent magnet 101, as shown in FIG. 12A, the direction of the magnetic flux of the magnet (the direction of N → S of the magnet) and the direction of the motive force of the armature winding are the same, and ( As shown in b), the direction of the magnet magnetic flux and the direction of the electromotive force of the armature winding may be opposite, and in the case of (b), the field magnetic flux is weakened. Further, in the yoke member 102, the directions of the internal magnetic fluxes are different between the side closer to the armature and the side farther from the armature in the radial direction according to the directions of the magnetic fluxes of the two permanent magnets 101 adjacent to the yoke member 102. In such a case, as shown in FIGS. 12A and 12B, the strength of the field magnetic flux differs depending on the magnetomotive force of the armature winding, that is, the energization phase of the armature winding. .. As a result, a variable field rotating electric machine can be realized.

ここで、ハルバッハ配列により磁石配置した技術との違いについて述べておく。なお、ハルバッハ配列は、1980年代に米国ローレンス・バークレー研の物理学者のKlaus Halbachが粒子加速器のビームを収束する目的で考案した、磁束集中効果のための永久磁石の特殊配列である。近年では、永久磁石式MRIや電動機、リニアモータ、磁気浮上式鉄道、自由電子レーザ発生用のアンジュレータなどの分野において利用が増えつつある技術である。 Here, the difference from the technique of arranging magnets by the Halbach array will be described. The Halbach array is a special array of permanent magnets for the magnetic flux concentration effect, which was devised by Klaus Halbach, a physicist at the Lawrence Berkeley Laboratory in the United States, for the purpose of converging the beam of the particle accelerator in the 1980s. In recent years, it is a technology that is increasingly used in fields such as permanent magnet type MRI, electric motors, linear motors, magnetic levitation type railways, and undulators for generating free electron lasers.

ハルバッハ配列の有名な特徴の一つに図13に示す磁束の片面集中現象がある。図13では、極磁石111とヨーク磁石112とが互いの磁化方向が直交する関係に交互配列されており、かかる構成においては、ヨーク磁石112とその当接する極磁石111の向きとの相互の方向の関係で磁束が配列の上下のいずれかの側に集中する。このとき、図13(a)、(b)に示すようにヨーク磁石112の磁化の向きを逆転すると、磁束の集中する側が反転する。このように永久磁石の配列のさせ方のみで磁束を集中させることができ、鉄片やコイルを用いることない磁界の集中方法として知られている。 One of the famous features of the Halbach array is the one-sided concentration phenomenon of magnetic flux shown in FIG. In FIG. 13, the polar magnets 111 and the yoke magnets 112 are alternately arranged in a relationship in which the magnetization directions are orthogonal to each other. The magnetic flux is concentrated on either the upper or lower side of the array. At this time, if the direction of magnetization of the yoke magnet 112 is reversed as shown in FIGS. 13 (a) and 13 (b), the side where the magnetic flux is concentrated is reversed. In this way, the magnetic flux can be concentrated only by the method of arranging the permanent magnets, and it is known as a method of concentrating the magnetic field without using an iron piece or a coil.

図12の構成(第1の手段での回転電機)は、図13における極間の磁石(ヨーク磁石112)を、鉄心であるヨーク部材102に変更したものである。ハルバッハ配列ではヨークが磁石であり、自身が起磁力(磁化)を保有しているが、鉄心の場合はそれがない。したがって、このままだと極磁石を側面短絡する手段にしかなっていない。この点、図12の構成では、隣り合う2つの永久磁石101がヨーク部材102(鉄心)により側面短絡されており、かかる構成では、上記のとおり電機子巻線における通電の位相制御により界磁磁束の強さを変更することが可能になっている。 In the configuration of FIG. 12 (rotary electric machine in the first means), the magnet between the poles (yoke magnet 112) in FIG. 13 is changed to a yoke member 102 which is an iron core. In the Halbach array, the yoke is a magnet, and it has its own magnetomotive force (magnetization), but in the case of an iron core, it does not. Therefore, as it is, it is only a means for short-circuiting the polar magnet on the side surface. In this regard, in the configuration of FIG. 12, two adjacent permanent magnets 101 are short-circuited on the side surface by the yoke member 102 (iron core), and in such a configuration, the field magnetic flux is controlled by the phase control of the energization in the armature winding as described above. It is possible to change the strength of.

第2の手段では、前記ヨーク部材は、周方向に隣り合う前記永久磁石の間において径方向に複数設けられている。 In the second means, a plurality of the yoke members are provided in the radial direction between the permanent magnets adjacent to each other in the circumferential direction.

ヨーク部材を、周方向に隣り合う永久磁石の間において径方向に複数設ける構成とした。ここで、永久磁石の周方向側面にヨーク部材を連結する構成では、その磁石側面の付近において磁束が周回して磁束の常時漏れが生じる。ただし、ヨーク部材を径方向に複数に分けて設けることにより、磁石側面での磁束漏れを抑制することができる。 A plurality of yoke members are provided in the radial direction between the permanent magnets adjacent to each other in the circumferential direction. Here, in the configuration in which the yoke member is connected to the circumferential side surface of the permanent magnet, the magnetic flux circulates in the vicinity of the side surface of the magnet, and the magnetic flux constantly leaks. However, by providing the yoke member in a plurality of parts in the radial direction, it is possible to suppress magnetic flux leakage on the side surface of the magnet.

なお、複数設けられたヨーク部材は、少なくとも周方向側面又はその付近にて複数に分離されていればよく、例えばヨーク部材において隣り合う永久磁石間の中間部分に橋渡し部が設けられていてもよい。 It should be noted that the plurality of yoke members may be separated into a plurality of members at least on or near the side surface in the circumferential direction, and for example, a bridging portion may be provided in an intermediate portion between adjacent permanent magnets in the yoke member. ..

第3の手段では、前記ヨーク部材は、前記電機子側の周面において、前記永久磁石の側面に接続されるヨーク端部に対して周方向中間部分が径方向に凹んだ形状となっている。 In the third means, the yoke member has a shape in which an intermediate portion in the circumferential direction is concave in the radial direction with respect to the end portion of the yoke connected to the side surface of the permanent magnet on the peripheral surface on the armature side. ..

ヨーク部材を、電機子側の周面において周方向中間部分が径方向に凹んだ形状とした。そのため、周方向に並ぶ永久磁石とヨーク部材との間で磁束の流れを促進するとともに、ヨーク部材から電機子への漏れ磁束を減らすことができる。これにより、エネルギ効率の改善を図ることができる。 The yoke member has a shape in which the middle portion in the circumferential direction is recessed in the radial direction on the peripheral surface on the armature side. Therefore, the flow of magnetic flux between the permanent magnets arranged in the circumferential direction and the yoke member can be promoted, and the leakage flux from the yoke member to the armature can be reduced. This makes it possible to improve energy efficiency.

第4の手段では、前記ヨーク部材には、周方向に隣り合う前記永久磁石の間に前記電機子とは反対側に延びるヨーク支持部(35)が接続されており、前記ヨーク部材ごとの前記ヨーク支持部が連結部(33)により一体的に連結されている。 In the fourth means, a yoke support portion (35) extending to the opposite side of the armature is connected between the permanent magnets adjacent to each other in the circumferential direction to the yoke member, and the yoke member is connected to the yoke member. The yoke support portion is integrally connected by the connecting portion (33).

ヨーク部材に、周方向に隣り合う永久磁石の間に電機子とは反対側に延びるヨーク支持部を接続し、ヨーク部材ごとのヨーク支持部を連結部により一体的に連結する構成とした。これにより、周方向に隣り合う永久磁石の間にそれぞれヨーク部材を設ける構成において、複数の永久磁石と複数のヨーク部材とを環状に配置しつつ好適に結合させることができる。この場合、ヨーク支持部は、隣り合う永久磁石の間において電機子の反対側に接続されているため、ヨーク支持部を介しての磁束漏れが抑制されるものとなっている。 A yoke support portion extending in the direction opposite to the armature is connected to the yoke member between permanent magnets adjacent to each other in the circumferential direction, and the yoke support portion for each yoke member is integrally connected by the connecting portion. Thereby, in the configuration in which the yoke members are provided between the permanent magnets adjacent to each other in the circumferential direction, the plurality of permanent magnets and the plurality of yoke members can be suitably coupled while being arranged in an annular shape. In this case, since the yoke support portion is connected to the opposite side of the armature between adjacent permanent magnets, magnetic flux leakage through the yoke support portion is suppressed.

第5の手段では、回転電機と、前記電機子巻線における通電の位相制御を実施する制御部(42)と、を備える回転電機システムであって、前記制御部は、電機子電流の位相を前記回転子のq軸に対して回転方向に進めることにより界磁磁束を弱め、電機子電流の位相を前記回転子のq軸に対して回転方向に遅らせることにより界磁磁束を強める制御を実施する。 The fifth means is a rotary electric machine system including a rotary electric machine and a control unit (42) for performing phase control of energization in the armature winding, and the control unit controls the phase of the armature current. Control is performed to weaken the field magnetic flux by advancing in the rotational direction with respect to the q-axis of the rotor, and to strengthen the field magnetic flux by delaying the phase of the armature current in the rotational direction with respect to the q-axis of the rotor. do.

制御部により、電機子電流の位相を回転子のq軸に対して回転方向に進める又は遅らせることにより、界磁磁束を弱めたり強めたりするようにした。これにより、所望のとおりにトルク等を制御することができる。 The control unit advances or delays the phase of the armature current in the rotational direction with respect to the q-axis of the rotor to weaken or strengthen the field magnetic flux. Thereby, the torque and the like can be controlled as desired.

回転電機の縦断面図。Vertical sectional view of a rotary electric machine. 回転子と電機子とを示す横断面図。Cross-sectional view showing a rotor and an armature. 回転子の要部を拡大して示す図。The figure which shows the main part of a rotor in an enlarged manner. 電機子による励磁の向きと磁界分布との関係を示す図。The figure which shows the relationship between the direction of the excitation by an armature and the magnetic field distribution. 実施形態の回転電機について等価回路を用いた考察の説明図。Explanatory drawing of consideration using an equivalent circuit about the rotary electric machine of an embodiment. 一般的な表面磁石型モータについて等価回路を用いた考察の説明図。Explanatory drawing of consideration using an equivalent circuit about a general surface magnet type motor. 二層ヨークが単層ヨークに対して優位性を有することの説明図。Explanatory drawing that a double-layer yoke has an advantage over a single-layer yoke. トルク出力をしている状態の磁束分布のシミュレーション結果を示す図。The figure which shows the simulation result of the magnetic flux distribution in the state of torque output. 有限要素法磁場解析のシミュレーション結果を示す図。The figure which shows the simulation result of the finite element method magnetic field analysis. 有限要素法磁場解析シミュレーションによるトルク最大時と磁束最小時との磁束密度分布を示す図。The figure which shows the magnetic flux density distribution at the time of the maximum torque and the time of the minimum magnetic flux by the finite element method magnetic field analysis simulation. 別例における回転子と電機子とを示す横断面図。The cross-sectional view which shows the rotor and the armature in another example. 電機子による励磁の向きと磁界分布との関係を示す図。The figure which shows the relationship between the direction of the excitation by an armature and the magnetic field distribution. ハルバッハ配列における磁界の集中現象を示す図。The figure which shows the magnetic field concentration phenomenon in the Halbach array.

以下、実施形態を図面に基づいて説明する。本実施形態における回転電機は、例えば車両動力源として用いられるものとなっている。ただし、回転電機は、産業用、車両用、家電用、OA機器用、遊技機用などとして広く用いられることが可能となっている。なお、以下の各実施形態相互において、互いに同一又は均等である部分には、図中、同一符号を付しており、同一符号の部分についてはその説明を援用する。 Hereinafter, embodiments will be described with reference to the drawings. The rotary electric machine in this embodiment is used, for example, as a vehicle power source. However, the rotary electric machine can be widely used for industrial use, vehicle use, home appliance use, OA equipment use, game machine use, and the like. In each of the following embodiments, parts that are the same or equal to each other are designated by the same reference numerals in the drawings, and the description thereof will be incorporated for the parts having the same reference numerals.

本実施形態に係る回転電機10は、表面磁石型の同期式多相交流モータであり、インナロータ構造(内転構造)のものとなっている。回転電機10の概要を図1及び図2に示す。図1は、回転電機10の回転軸11に沿う方向での縦断面図であり、図2は、回転軸11に直交する方向での回転子12及び電機子13の横断面図である。以下の記載では、回転軸11が延びる方向を軸方向とし、回転軸11を中心として放射状に延びる方向を径方向とし、回転軸11を中心として円周状に延びる方向を周方向としている。 The rotary electric machine 10 according to the present embodiment is a surface magnet type synchronous multi-phase AC motor having an inner rotor structure (adduction structure). The outline of the rotary electric machine 10 is shown in FIGS. 1 and 2. FIG. 1 is a vertical cross-sectional view of the rotary electric machine 10 in a direction along the rotation axis 11, and FIG. 2 is a cross-sectional view of the rotor 12 and the armature 13 in a direction orthogonal to the rotation axis 11. In the following description, the direction in which the rotating shaft 11 extends is the axial direction, the direction in which the rotating shaft 11 extends radially is the radial direction, and the direction in which the rotating shaft 11 extends in a circumferential shape is the circumferential direction.

回転電機10は、回転軸11に固定された回転子12と、回転子12を包囲する位置に設けられる電機子13と、これら回転子12及び電機子13を収容するハウジング14とを備えている。回転子12及び電機子13は同軸に配置されている。ハウジング14は、有底筒状の一対のハウジング部材14a,14bを有し、ハウジング部材14a,14bが開口部同士で接合された状態でボルト15の締結により一体化されている。ハウジング14には軸受け16,17が設けられ、この軸受け16,17により回転軸11及び回転子12が回転自在に支持されている。 The rotary electric machine 10 includes a rotor 12 fixed to a rotary shaft 11, an armature 13 provided at a position surrounding the rotor 12, and a housing 14 for accommodating the rotor 12 and the armature 13. .. The rotor 12 and the armature 13 are arranged coaxially. The housing 14 has a pair of bottomed cylindrical housing members 14a and 14b, and the housing members 14a and 14b are integrated by fastening bolts 15 in a state where the housing members 14a and 14b are joined to each other at the openings. Bearings 16 and 17 are provided in the housing 14, and the rotating shaft 11 and the rotor 12 are rotatably supported by the bearings 16 and 17.

図2に示すように、電機子13は、周方向に複数のスロット21を有する円環状の電機子コア22と、電機子コア22の各スロット21に巻装された3相(U相、V相、W相)の電機子巻線23とを備えている。電機子コア22は、円環状の複数の電磁鋼板を軸方向に積層し、カシメ等により固定することで構成されている。電機子コア22は、円環状のヨーク24と、ヨーク24から径方向内側へ突出し周方向に所定距離を隔てて配列された複数のティース25とを有し、隣り合うティース25の間にスロット21が形成されている。各ティース25は、周方向に等間隔でそれぞれ設けられている。 As shown in FIG. 2, the armature 13 includes an annular armature core 22 having a plurality of slots 21 in the circumferential direction, and three phases (U phase, V) wound around each slot 21 of the armature core 22. It is provided with an armature winding 23 (phase, W phase). The armature core 22 is configured by laminating a plurality of annular electromagnetic steel sheets in the axial direction and fixing them by caulking or the like. The armature core 22 has an annular yoke 24 and a plurality of teeth 25 protruding inward in the radial direction from the yoke 24 and arranged at a predetermined distance in the circumferential direction, and a slot 21 is provided between the adjacent teeth 25. Is formed. Each tooth 25 is provided at equal intervals in the circumferential direction.

各スロット21は、電機子巻線23の1相あたり2個ずつ隣り合わせにして設けられている。つまり、電機子コア22には、周方向に繰り返し2個ずつ配置されたU相スロット、V相スロット及びW相スロットが形成されている。各スロット21には、ティース25に巻回されるようにして電機子巻線23が巻装されている。電機子巻線23は、例えば複数の導体セグメントが互いに接合されることで構成されている。 Two slots 21 are provided side by side for each phase of the armature winding 23. That is, the armature core 22 is formed with two U-phase slots, two V-phase slots, and two W-phase slots repeatedly arranged in the circumferential direction. An armature winding 23 is wound around each slot 21 so as to be wound around the teeth 25. The armature winding 23 is configured, for example, by joining a plurality of conductor segments to each other.

回転子12は、回転軸11に固定される回転子コア31と、その回転子コア31に保持された複数の永久磁石32とを有している。回転子コア31は、回転軸11に対して固定される筒状の中央固定部33と、周方向に隣り合う永久磁石32の間においてそれら永久磁石32の周方向側面どうしを繋ぎ(橋絡し)、かつ複数の永久磁石32を環状に連結するロータヨーク34と、回転軸11を中心にして径方向に延び、中央固定部33及びロータヨーク34を繋ぐ複数のヨーク支持部35とを有している。ロータヨーク34は鉄心材よりなり、これが「ヨーク部材」に相当する。本実施形態では、中央固定部33とロータヨーク34とヨーク支持部35とを電磁鋼板にて一体に形成しており、複数の電磁鋼板を軸方向に積層し、カシメ等により固定することで、回転子コア31が構成されている。 The rotor 12 has a rotor core 31 fixed to the rotating shaft 11 and a plurality of permanent magnets 32 held by the rotor core 31. The rotor core 31 connects (bridges) the peripheral side surfaces of the permanent magnets 32 between the cylindrical central fixing portion 33 fixed to the rotating shaft 11 and the permanent magnets 32 adjacent to each other in the circumferential direction. ), And a rotor yoke 34 that connects a plurality of permanent magnets 32 in an annular shape, and a plurality of yoke support portions 35 that extend radially around the rotation shaft 11 and connect the central fixing portion 33 and the rotor yoke 34. .. The rotor yoke 34 is made of an iron core material, which corresponds to a "yoke member". In the present embodiment, the central fixing portion 33, the rotor yoke 34, and the yoke supporting portion 35 are integrally formed of an electromagnetic steel plate, and a plurality of electromagnetic steel plates are laminated in the axial direction and fixed by caulking or the like to rotate. The child core 31 is configured.

ロータヨーク34には、複数の永久磁石32が所定間隔で組み付けられている。詳しくは、複数の永久磁石32は、ロータヨーク34により、電機子13において同相の電機子巻線23が巻装されるピッチと同じ間隔で、周方向にそれぞれ配置されている。また、各永久磁石32は、磁化方向(磁極の向き)を径方向とし、かつ電機子13に対向する極が交互にN極、S極となるように周方向に互いに離間された位置に設けられている。 A plurality of permanent magnets 32 are assembled to the rotor yoke 34 at predetermined intervals. Specifically, the plurality of permanent magnets 32 are arranged by the rotor yoke 34 in the circumferential direction at the same intervals as the pitch at which the armature windings 23 having the same phase are wound on the armature 13. Further, each permanent magnet 32 is provided at a position separated from each other in the circumferential direction so that the magnetization direction (direction of the magnetic pole) is the radial direction and the poles facing the armature 13 are alternately N poles and S poles. Has been done.

また、図3に示すように、ロータヨーク34は、径方向において内外2つに分けて設けられており、外周側が外周側ヨーク34a、内周側が内周側ヨーク34bとなっている。外周側ヨーク34a及び内周側ヨーク34bは、いずれも永久磁石32の周方向側面から周方向に延びるように設けられており、それらの間には空間部が設けられている。なお、外周側ヨーク34aと内周側ヨーク34bとの間の空間部には、両ヨーク34a,34bを繋ぐ橋渡し部が設けられていてもよい。外周側ヨーク34aは、径方向において電機子13に近い側に設けられ、内周側ヨーク34bは、径方向において電機子13から遠い側に設けられている。外周側ヨーク34a及び内周側ヨーク34bにより、径方向に分かれた2つの磁気回路が形成されるようになっている。外周側ヨーク34aの径方向の幅L1と内周側ヨーク34bの径方向の幅L2とは、L1>L2である。ただし、L1=L2、又はL1<L2であってもよい。 Further, as shown in FIG. 3, the rotor yoke 34 is provided separately in the inner and outer directions in the radial direction, and the outer peripheral side is the outer peripheral side yoke 34a and the inner peripheral side is the inner peripheral side yoke 34b. Both the outer peripheral side yoke 34a and the inner peripheral side yoke 34b are provided so as to extend in the circumferential direction from the circumferential side surface of the permanent magnet 32, and a space portion is provided between them. A bridging portion connecting both yokes 34a and 34b may be provided in the space between the outer peripheral side yoke 34a and the inner peripheral side yoke 34b. The outer peripheral side yoke 34a is provided on the side closer to the armature 13 in the radial direction, and the inner peripheral side yoke 34b is provided on the side farther from the armature 13 in the radial direction. The outer peripheral side yoke 34a and the inner peripheral side yoke 34b form two magnetic circuits separated in the radial direction. The radial width L1 of the outer peripheral side yoke 34a and the radial width L2 of the inner peripheral side yoke 34b are L1> L2. However, L1 = L2 or L1 <L2 may be satisfied.

外周側ヨーク34aは、電機子13側(図の上側)の外周面において、永久磁石32の側面に接続されるヨーク端部に対して周方向中間部分が径方向に凹んでおり、凹部36となっている。この場合、外周側ヨーク34aは、周方向に隣り合う永久磁石32の間において、周方向中間部分が径方向に縮小され、かつ両端部分が拡大された形状(ブーツ形状)となっている。 The outer peripheral side yoke 34a has a circumferential middle portion recessed in the radial direction with respect to the yoke end portion connected to the side surface of the permanent magnet 32 on the outer peripheral surface on the armature 13 side (upper side in the drawing), and the concave portion 36 and the outer peripheral side yoke 34a. It has become. In this case, the outer peripheral side yoke 34a has a shape (boot shape) in which the peripheral intermediate portion is reduced in the radial direction and both end portions are enlarged between the permanent magnets 32 adjacent to each other in the circumferential direction.

また、内周側ヨーク34bは、電機子13の反対側(図の下側)の内周面において、永久磁石32の側面に接続されるヨーク端部に対して周方向中間部分が径方向に凹んでおり、凹部37となっている。この場合、内周側ヨーク34bは、周方向に隣り合う永久磁石32の間において、周方向中間部分が径方向に縮小され、かつ両端部分が拡大された形状(ブーツ形状)となっている。 Further, the inner peripheral side yoke 34b has a circumferential intermediate portion in the radial direction with respect to the yoke end portion connected to the side surface of the permanent magnet 32 on the inner peripheral surface on the opposite side (lower side in the drawing) of the armature 13. It is recessed and has a recess 37. In this case, the inner peripheral side yoke 34b has a shape (boot shape) in which the peripheral intermediate portion is reduced in the radial direction and both end portions are enlarged between the permanent magnets 32 adjacent to each other in the circumferential direction.

各内周側ヨーク34bには、周方向に隣り合う永久磁石32の間に電機子13とは反対側に延びるヨーク支持部35が接続されており、内周側ヨーク34bごとのヨーク支持部35が、連結部としての中央固定部33により一体的に連結されている。各内周側ヨーク34bには、隣り合う永久磁石間にヨーク支持部35が接続されていることから、永久磁石32の内側(反電機子側)の径方向端面には電磁鋼板等の軟磁性体が存在しない、仮に存在しても永久磁石32の表面を覆う程度のものとなっている。 A yoke support portion 35 extending in the direction opposite to the armature 13 is connected between the permanent magnets 32 adjacent to each other in the circumferential direction to each inner peripheral side yoke 34b, and a yoke support portion 35 for each inner peripheral side yoke 34b is connected. Is integrally connected by a central fixing portion 33 as a connecting portion. Since the yoke support portion 35 is connected between the adjacent permanent magnets on each inner peripheral side yoke 34b, the inner (anti-armature side) radial end surface of the permanent magnets 32 is soft magnetic such as an electromagnetic steel plate. The body does not exist, and even if it exists, it covers the surface of the permanent magnet 32.

図1に示すように、回転電機システムは、インバータ41と制御部42とを備えている。インバータ41は、回転電機10において各相の電機子巻線23に接続され、相ごとに通電電流を調整する。インバータ41は、周知のとおり相巻線の相数と同数の上下アームを有するブリッジ回路であり、各アームにはスイッチ(半導体スイッチング素子)がそれぞれ設けられている。制御部42は、CPUや各種メモリを有するマイクロコンピュータよりなり、例えば力行トルク指令値や発電電圧指令値に基づいて、所定のスイッチング周波数(キャリア周波数)でインバータ41の各スイッチをオンオフし、これにより回転電機10の各相電流についてフィードバック制御を実施する。また、制御部42は、電機子巻線23の各相の電流(相電流)について位相を制御することが可能になっている。 As shown in FIG. 1, the rotary electric machine system includes an inverter 41 and a control unit 42. The inverter 41 is connected to the armature winding 23 of each phase in the rotary electric machine 10, and adjusts the energizing current for each phase. As is well known, the inverter 41 is a bridge circuit having the same number of upper and lower arms as the number of phases of the phase winding, and each arm is provided with a switch (semiconductor switching element). The control unit 42 comprises a CPU and a microcomputer having various memories, and turns on and off each switch of the inverter 41 at a predetermined switching frequency (carrier frequency) based on, for example, a power running torque command value and a generated voltage command value. Feedback control is performed for each phase current of the rotary electric machine 10. Further, the control unit 42 can control the phase of the current (phase current) of each phase of the armature winding 23.

上記構成の回転電機10での特徴的な作用は、図12において説明したとおりであるが、図4を用いて、回転電機10での特徴的な作用を再度説明しておく。 The characteristic action of the rotary electric machine 10 having the above configuration is as described with reference to FIG. 12, but the characteristic action of the rotary electric machine 10 will be described again with reference to FIG.

電機子巻線23に電流を流すと、電機子巻線23の通電位相に応じて、破線で示すようにループ状に起磁力が生じる。ここで、永久磁石32では、図4(a)に示すように、磁石磁束の向き(磁石のN→Sの向き)と電機子巻線23の起磁力の向きとが同じになる場合と、(b)に示すように、磁石磁束の向きと電機子巻線23の起磁力の向きとが逆になる場合とがある。(a)の場合には、図の時計回り方向の向きで起磁力が生じており、電機子13に対して遠い側の内周側ヨーク34bを介して磁束が流れる。また、(b)の場合には、図の反時計回り方向の向きで起磁力が生じており、電機子13に対して近い側の外周側ヨーク34aを介して磁束が流れる。(a)の場合には界磁磁束が強められることになり、(b)の場合には界磁磁束が弱められることになる。かかる場合、電機子巻線の起磁力、すなわち電機子巻線の通電位相に応じて、界磁磁束の変更が可能になっている。 When a current is passed through the armature winding 23, a magnetomotive force is generated in a loop shape as shown by a broken line according to the energization phase of the armature winding 23. Here, in the permanent magnet 32, as shown in FIG. 4A, the direction of the magnetic flux of the magnet (the direction of N → S of the magnet) and the direction of the magnetomotive force of the armature winding 23 are the same. As shown in (b), the direction of the magnetic flux of the magnet and the direction of the magnetomotive force of the armature winding 23 may be opposite to each other. In the case of (a) has occurred magnetomotive force in the clockwise direction in the orientation of FIG, magnetic flux flows through the far side of the inner peripheral side yoke 34b relative to the armature 13. In the case of (b) is generated magnetomotive force in the counterclockwise direction in the orientation of FIG, magnetic flux flows through the outer peripheral side yoke 34a near side with respect to the armature 13. In the case of (a), the field magnetic flux is strengthened, and in the case of (b), the field magnetic flux is weakened. In such a case, the field magnetic flux can be changed according to the magnetomotive force of the armature winding, that is, the energization phase of the armature winding.

上記構成では、永久磁石32の側面にロータヨーク34が連結されており、換言すれば、永久磁石32の磁化方向に対して略垂直にロータヨーク34が密着する構成となっている。また、磁石側面の略全面にロータヨーク34が連結されている。そのため、磁束の流れを変えやすいものとなっている。 In the above configuration, the rotor yoke 34 is connected to the side surface of the permanent magnet 32, in other words, the rotor yoke 34 is in close contact with the permanent magnet 32 substantially perpendicular to the magnetization direction. Further, the rotor yoke 34 is connected to substantially the entire surface of the side surface of the magnet. Therefore, it is easy to change the flow of magnetic flux.

また、図5及び図6は、等価回路を用いた考察の説明図である。図5には、本実施形態の回転電機10を想定した等価回路を示し、図6には、本実施形態と磁石配置と量とを揃えた一般的な表面磁石型モータを想定した等価回路を示す。Rgは電機子13と回転子12との間のエアギャップに相当し、Ryは外周側ヨーク34a及び内周側ヨーク34bにそれぞれ相当し、Rcは一般的な表面磁石型モータのロータコアCに相当する。図5及び図6では(b)に電機子通電時を示し、(c)に無通電時を示す。なお、図5(b)の状態は図4(a)の状態に相当する。 Further, FIGS. 5 and 6 are explanatory views of consideration using an equivalent circuit. FIG. 5 shows an equivalent circuit assuming the rotary electric machine 10 of the present embodiment, and FIG. 6 shows an equivalent circuit assuming a general surface magnet type motor having the same magnet arrangement and amount as the present embodiment. show. Rg corresponds to the air gap between the armature 13 and the rotor 12, Ry corresponds to the outer peripheral side yoke 34a and the inner peripheral side yoke 34b, respectively, and Rc corresponds to the rotor core C of a general surface magnet type motor. do. In FIGS. 5 and 6, FIG. 5B shows the time when the armature is energized, and FIG. 6C shows the time when the armature is not energized. The state of FIG. 5 (b) corresponds to the state of FIG. 4 (a).

図5において、(b)の電機子通電時には、磁石磁束は極間で殆ど漏れることなく電機子13へ到達すると考えられる。より詳しくは、極間での漏れが生じても、それを上回る逆方向の磁束が電機子13から供給され、差し引きの差分は低くなり、結局は外周側ヨーク34a(電機子側ヨーク)の通過磁束量(漏れ磁束量)が減ることとなる。 In FIG. 5, it is considered that the magnet magnetic flux reaches the armature 13 with almost no leakage between the poles when the armature of (b) is energized. More specifically, even if a leakage occurs between the poles, a magnetic flux in the opposite direction exceeding that is supplied from the armature 13, the difference in subtraction becomes low, and eventually the outer peripheral side yoke 34a (armature side yoke) passes through. The amount of magnetic flux (amount of leakage flux) will be reduced.

また、(c)の無通電時には、ロータヨーク34(34a,34b)が永久磁石32の側面に当接していることから、磁束がショートカットする。つまり換言すれば、永久磁石32の起磁力がフルに使われない自己循環漏洩となると考えられる。 Further, when the power is not supplied in (c), the rotor yokes 34 (34a, 34b) are in contact with the side surface of the permanent magnet 32, so that the magnetic flux is short-cut. In other words, it is considered that the magnetomotive force of the permanent magnet 32 is not fully used, resulting in self-circulation leakage.

この場合、電機子通電時には永久磁石32の磁束がフルに使われるのに対し、無通電時には磁束がショートカットする。したがって、上記構成の回転電機10では、電機子通電時に永久磁石32の作用範囲が磁化方向に比較的長くなり、無通電時に永久磁石32の作用範囲が磁化方向に比較的短くなる構成を有することになる。この点において、回転電機10は、可変磁束磁気回路とでもいえる要素を持つものとなっている。 In this case, the magnetic flux of the permanent magnet 32 is fully used when the armature is energized, whereas the magnetic flux is short-cut when the armature is not energized. Therefore, the rotary electric machine 10 having the above configuration has a configuration in which the working range of the permanent magnet 32 is relatively long in the magnetization direction when the armature is energized, and the working range of the permanent magnet 32 is relatively short in the magnetization direction when the armature is not energized. become. In this respect, the rotary electric machine 10 has an element that can be said to be a variable magnetic flux magnetic circuit.

なお、図6に示すように、一般的な表面磁石型モータでは、電機子とは逆側(図の下側)で永久磁石32が軟磁性体のロータコアCに結合されており、電機子通電時及び無通電時のいずれにおいても、磁束経路は同じになる。そのため、界磁磁束を変えることが困難なものとなっている。 As shown in FIG. 6, in a general surface magnet type motor, a permanent magnet 32 is coupled to a soft magnetic rotor core C on the side opposite to the armature (lower side in the figure), and the armature is energized. The magnetic flux path is the same at both the time and the non-energized state. Therefore, it is difficult to change the field magnetic flux.

ここで、ロータヨーク34を内周側及び外周側で2つに分けて設けていることの優位点を図7を用いて補足する。図7(a)は、ロータヨーク34を径方向の内外に分けずに単層で設けた構成を示し、(b)は、ロータヨーク34を径方向の内外に分けて二層に設けた構成を示す。 Here, the advantage of providing the rotor yoke 34 separately on the inner peripheral side and the outer peripheral side will be supplemented with reference to FIG. 7. FIG. 7A shows a configuration in which the rotor yoke 34 is provided as a single layer without dividing the rotor yoke 34 into the inside and outside in the radial direction, and FIG. 7B shows a configuration in which the rotor yoke 34 is divided into the inside and outside in the radial direction and provided in two layers. ..

本実施形態では、永久磁石32の側面にロータヨーク34を連結する構成であるため、その磁石側面の付近において磁束が周回して磁束の常時漏れが生じる。ここで、図7(a)の場合には、磁石側面での磁束の常時漏れが大きいため、効率の低下が懸念される。これに対して、(b)の場合には、ロータヨーク34を径方向に分割することで、磁束の周回範囲が狭められるため、磁石側面での磁束漏れが軽減される。 In the present embodiment, since the rotor yoke 34 is connected to the side surface of the permanent magnet 32, the magnetic flux circulates in the vicinity of the side surface of the magnet, and the magnetic flux constantly leaks. Here, in the case of FIG. 7A, since the magnetic flux constantly leaks from the side surface of the magnet, there is a concern that the efficiency may decrease. On the other hand, in the case of (b), by dividing the rotor yoke 34 in the radial direction, the magnetic flux circulation range is narrowed, so that magnetic flux leakage on the side surface of the magnet is reduced.

図8には、回転電機10における磁束の流れをFEA(有限要素法)シミュレーションにて解析した結果を示す。これはトルク出力時の解析結果を示すものである。図8によれば、永久磁石32の磁束は、外周側ヨーク34aを通って戻ってくるような漏れ方でなく、電機子13に有効にわたっていることが分かる。なお、弱め界磁磁束を生じさせる場合には、磁石磁束が外周側ヨーク34aを介して多く漏洩することとなる。 FIG. 8 shows the result of analyzing the flow of magnetic flux in the rotary electric machine 10 by FEA (finite element method) simulation. This shows the analysis result at the time of torque output. According to FIG. 8, it can be seen that the magnetic flux of the permanent magnet 32 effectively extends to the armature 13 rather than leaking back through the outer peripheral side yoke 34a. When a weakened field magnetic flux is generated, a large amount of magnetic flux leaks through the outer peripheral side yoke 34a.

また、図9は、本実施形態の回転電機10と一般的な表面磁石型モータとについて電機子電流に対する磁束の弱まり度合いを比較したものである。本実施形態の回転電機10では、一般的な表面磁石型モータに対して約半分の電流で同等の磁束に抑制できることが分かる。すなわち、省電流で磁束を大きく変更できるものであることが分かる。 Further, FIG. 9 compares the degree of weakening of the magnetic flux with respect to the armature current between the rotary electric machine 10 of the present embodiment and the general surface magnet type motor. It can be seen that the rotary electric machine 10 of the present embodiment can suppress the magnetic flux to the same level with a current about half that of a general surface magnet type motor. That is, it can be seen that the magnetic flux can be significantly changed by saving current.

また、図10には、有限要素法磁場解析シミュレーションによるトルク最大時と磁束最小時との磁束密度分布を示す。(a)は、本実施形態の回転電機10についてトルク最大時のシミュレーション結果を示し、(b)は、本実施形態の回転電機10について磁束最小時のシミュレーション結果を示し、(c)は、一般的な表面磁石型モータについてトルク最大時のシミュレーション結果を示し、(d)は、一般的な表面磁石型モータについて磁束最小時のシミュレーション結果を示す。 Further, FIG. 10 shows the magnetic flux density distribution at the maximum torque and the minimum magnetic flux by the finite element method magnetic field analysis simulation. (A) shows the simulation result of the rotary electric machine 10 of the present embodiment at the maximum torque, (b) shows the simulation result of the rotary electric machine 10 of the present embodiment at the minimum magnetic flux, and (c) is the general. The simulation result at the maximum torque is shown for a typical surface magnet type motor, and (d) shows the simulation result at the minimum magnetic flux for a general surface magnet type motor.

本実施形態の回転電機10では、図10(a)の場合に磁石磁束が電機子13にフルで到達し、(b)の場合に磁石磁束がロータヨーク34によりショートカットされている(自己循環漏洩が生じている)ことが分かる。また、一般的な表面磁石型モータでは、(d)の場合に、(b)に示す回転電機10に比べて電機子側への漏れ磁束が多くなっていることが分かる。 In the rotary electric machine 10 of the present embodiment, the magnet magnetic flux reaches the armature 13 at full in the case of FIG. 10A, and the magnet magnetic flux is short-cut by the rotor yoke 34 in the case of (b) (self-circulation leakage occurs). It turns out that it is happening). Further, it can be seen that in the general surface magnet type motor, in the case of (d), the leakage flux to the armature side is larger than that of the rotary electric machine 10 shown in (b).

以上詳述した本実施形態によれば、以下の優れた効果が得られる。 According to the present embodiment described in detail above, the following excellent effects can be obtained.

回転電機10の回転子12において、複数の永久磁石32を、磁化方向を径方向とし、かつ電機子13に対向する極が交互にN極、S極となるようにして周方向に互いに離間された位置に設けるとともに、その複数の永久磁石32を、鉄心であるロータヨーク34により、磁石側面どうしを繋ぎ、かつ環状に連結する構成とした。ここで、永久磁石32では、電機子13側の径方向端面とロータヨーク34側の周方向側面とを通じて界磁磁束が流れる構成となっており、電機子巻線23の通電により起磁力が生じる場合に、その起磁力の向きと永久磁石32ごとの磁極とに応じて、永久磁石32にて生じる界磁磁束の分布が異なるものとなる。この場合、隣り合う永久磁石32の周方向側面を通じて流れる界磁磁束を好適に変化させることができる。これにより、表面磁石型の回転電機10において、回転子12により生じる界磁磁束を好適に変化させて可変界磁磁束を実現することができる。 In the rotor 12 of the rotating electric machine 10, the plurality of permanent magnets 32 are separated from each other in the circumferential direction so that the magnetization direction is the radial direction and the poles facing the armature 13 are alternately N poles and S poles. The plurality of permanent magnets 32 are connected to each other by a rotor yoke 34, which is an iron core, and are connected in an annular shape. Here, the permanent magnet 32 has a configuration in which a field magnetic flux flows through the radial end surface on the armature 13 side and the circumferential side surface on the rotor yoke 34 side, and a magnetomotive force is generated by energization of the armature winding 23. In addition, the distribution of the field magnetic flux generated by the permanent magnet 32 differs depending on the direction of the magnetomotive force and the magnetic pole of each permanent magnet 32. In this case, the field magnetic flux flowing through the circumferential side surfaces of the adjacent permanent magnets 32 can be preferably changed. As a result, in the surface magnet type rotary electric machine 10, the field magnetic flux generated by the rotor 12 can be suitably changed to realize the variable field magnetic flux.

ロータヨーク34を、周方向に隣り合う永久磁石32の間において径方向に複数に分けて設ける構成とした。ここで、永久磁石32の側面にロータヨーク34を連結する構成では、その磁石側面の付近において磁束が周回して磁束の常時漏れが生じる。ただし、ロータヨーク34を径方向に複数に分けて設けることにより、磁石側面での磁束漏れを抑制することができる。 The rotor yoke 34 is provided in a plurality of radial directions between the permanent magnets 32 adjacent to each other in the circumferential direction. Here, in the configuration in which the rotor yoke 34 is connected to the side surface of the permanent magnet 32, the magnetic flux circulates in the vicinity of the side surface of the magnet, and the magnetic flux constantly leaks. However, by providing the rotor yoke 34 in a plurality of parts in the radial direction, magnetic flux leakage on the side surface of the magnet can be suppressed.

ロータヨーク34を、電機子13側の周面において周方向中間部分が径方向に凹んだ形状とした。そのため、周方向に並ぶ永久磁石32とロータヨーク34との間で磁束の流れを促進するとともに、ロータヨーク34から電機子13への漏れ磁束を減らすことができる。これにより、エネルギ効率の改善を図ることができる。 The rotor yoke 34 has a shape in which the middle portion in the circumferential direction is concave in the radial direction on the peripheral surface on the armature 13 side. Therefore, the flow of magnetic flux between the permanent magnets 32 arranged in the circumferential direction and the rotor yoke 34 can be promoted, and the leakage flux from the rotor yoke 34 to the armature 13 can be reduced. This makes it possible to improve energy efficiency.

ロータヨーク34に、周方向に隣り合う永久磁石32の間に電機子13とは反対側に延びるヨーク支持部35を接続し、複数のヨーク支持部35を中央固定部33(連結部)により一体的に連結する構成とした。これにより、周方向に隣り合う永久磁石32の間にそれぞれロータヨーク34を設ける構成において、複数の永久磁石32と複数のロータヨーク34とを環状に配置しつつ好適に結合させることができる。この場合、ヨーク支持部35は、隣り合う永久磁石32の間において電機子13の反対側に接続されているため、ヨーク支持部35を介しての磁束漏れを抑制できるものとなっている。 A yoke support portion 35 extending in the direction opposite to the armature 13 is connected to the rotor yoke 34 between permanent magnets 32 adjacent to each other in the circumferential direction, and a plurality of yoke support portions 35 are integrated by a central fixing portion 33 (connecting portion). It was configured to be connected to. Thereby, in the configuration in which the rotor yokes 34 are provided between the permanent magnets 32 adjacent to each other in the circumferential direction, the plurality of permanent magnets 32 and the plurality of rotor yokes 34 can be suitably coupled while being arranged in an annular shape. In this case, since the yoke support portion 35 is connected to the opposite side of the armature 13 between the adjacent permanent magnets 32, magnetic flux leakage through the yoke support portion 35 can be suppressed.

制御部42により、電機子電流の位相を回転子12のq軸に対して回転方向に進める又は遅らせることにより、界磁磁束を弱めたり強めたりするようにした。これにより、所望のとおりにトルク等を制御することができる。 The control unit 42 advances or delays the phase of the armature current in the rotational direction with respect to the q-axis of the rotor 12, thereby weakening or increasing the field magnetic flux. Thereby, the torque and the like can be controlled as desired.

(他の実施形態)
上記実施形態を例えば次のように変更してもよい。
(Other embodiments)
The above embodiment may be changed as follows, for example.

・上記実施形態では、ロータヨーク34を径方向の内外に2つに分けて、それぞれを外周側ヨーク34a、内周側ヨーク34bとしたが、この構成を変更してもよい。ロータヨーク34を径方向の内外に3つ以上に分ける構成としてもよい。又は、ロータヨーク34を径方向に分けずに設ける構成であってもよい。 -In the above embodiment, the rotor yoke 34 is divided into two inside and outside in the radial direction, and each of them is the outer peripheral side yoke 34a and the inner peripheral side yoke 34b, but this configuration may be changed. The rotor yoke 34 may be divided into three or more in and out in the radial direction. Alternatively, the rotor yoke 34 may be provided without being divided in the radial direction.

・回転子12を図11のように構成することも可能である。図11では、回転軸11に固定された略円板状の絶縁プレート51を有し、その絶縁プレート51の外周側に、所定間隔で永久磁石32が取り付けられるとともに、各永久磁石32の間にそれぞれロータヨーク34が取り付けられている。絶縁プレート51は、合成樹脂等の絶縁材料よりなる。本構成では、絶縁プレート51が永久磁石32及びロータヨーク34を保持する保持部材となっている。 -It is also possible to configure the rotor 12 as shown in FIG. In FIG. 11, a substantially disk-shaped insulating plate 51 fixed to the rotating shaft 11 is provided, and permanent magnets 32 are attached to the outer peripheral side of the insulating plate 51 at predetermined intervals, and between the permanent magnets 32. A rotor yoke 34 is attached to each. The insulating plate 51 is made of an insulating material such as synthetic resin. In this configuration, the insulating plate 51 is a holding member that holds the permanent magnet 32 and the rotor yoke 34.

・上記実施形態では、インナロータ式の回転電機での適用例を説明したが、これ以外にアウタロータ式の回転電機に適用することも可能である。 -In the above embodiment, an example of application to an inner rotor type rotary electric machine has been described, but other than this, it can also be applied to an outer rotor type rotary electric machine.

10…回転電機、12…回転子、13…電機子、23…電機子巻線、32…永久磁石、34…ロータヨーク(ヨーク部材)。 10 ... Rotor, 12 ... Rotor, 13 ... Armature, 23 ... Armature winding, 32 ... Permanent magnet, 34 ... Rotor yoke (yoke member).

Claims (5)

回転自在に支持された回転子(12)と、
前記回転子と同軸配置され、多相交流電流が通電される電機子巻線(23)が巻装された電機子(13)と、
を備えた表面磁石型の回転電機(10)であって、
前記回転子は、
磁化方向を径方向とし、かつ前記電機子に対向する極が交互にN極、S極となるようにして周方向に互いに離間された位置に設けられた複数の永久磁石(32)と、
鉄心材よりなり、周方向に隣り合う前記永久磁石の間においてそれら永久磁石の周方向側面どうしを繋ぎ、かつ前記複数の永久磁石を環状に連結するヨーク部材(34)と、
を有しており、
前記ヨーク部材において、周方向に隣り合う前記永久磁石の各周方向側面の間に一方の永久磁石側から他方の永久磁石側へ向かう向きで界磁磁束を生じさせることが可能となっており、
前記電機子巻線の通電位相に応じて、前記ヨーク部材において周方向に互いに逆向きで界磁磁束を生じさせることにより、前記永久磁石から前記電機子へ向かう界磁磁束の強さを変更することが可能になっている回転電機。
Rotor (12) rotatably supported and
An armature (13) that is coaxially arranged with the rotor and is wound with an armature winding (23) that is energized with a multi-phase alternating current.
A surface magnet type rotary electric machine (10) equipped with
The rotor
A plurality of permanent magnets (32) provided at positions separated from each other in the circumferential direction so that the magnetization direction is the radial direction and the poles facing the armature are alternately N poles and S poles.
A yoke member (34) made of an iron core material, connecting the peripheral side surfaces of the permanent magnets between the permanent magnets adjacent to each other in the circumferential direction, and connecting the plurality of permanent magnets in an annular shape.
Have and
In the yoke member, it is possible to generate a field magnetic flux in the direction from one permanent magnet side to the other permanent magnet side between the peripheral side surfaces of the permanent magnets adjacent to each other in the circumferential direction.
The strength of the field magnetic flux from the permanent magnet to the armature is changed by generating field magnetic fluxes in the yoke members in opposite directions in the circumferential direction according to the energization phase of the armature winding. A rotating electric machine that makes it possible.
前記ヨーク部材は、周方向に隣り合う前記永久磁石の各周方向側面の間に、当該周方向側面から周方向に延び、かつ径方向に並ぶ複数のヨーク部材(34a,34b)として設けられている請求項1に記載の回転電機。 The yoke members are provided between the peripheral side surfaces of the permanent magnets adjacent to each other in the circumferential direction as a plurality of yoke members (34a, 34b) extending in the circumferential direction from the circumferential side surfaces and arranging in the radial direction. The rotary electric machine according to claim 1. 前記ヨーク部材は、前記電機子側の周面において、前記永久磁石の側面に接続されるヨーク端部に対して周方向中間部分が径方向に凹んだ形状となっている請求項1又は2に記載の回転電機。 2. The rotating electric machine described. 前記ヨーク部材には、周方向に隣り合う前記永久磁石の間に前記電機子とは反対側に延びるヨーク支持部(35)が接続されており、前記ヨーク部材ごとの前記ヨーク支持部が連結部(33)により一体的に連結されている請求項1乃至3のいずれか1項に記載の回転電機。 A yoke support portion (35) extending in the direction opposite to the armature is connected to the yoke member between the permanent magnets adjacent to each other in the circumferential direction, and the yoke support portion for each yoke member is connected to the connecting portion. The rotary electric machine according to any one of claims 1 to 3, which is integrally connected by (33). 請求項1乃至4のいずれか1項に記載の回転電機と、
前記電機子巻線における通電の位相制御を実施する制御部(42)と、
を備える回転電機システムであって、
前記制御部は、電機子電流の位相を前記回転子のq軸に対して回転方向に進めることにより界磁磁束を弱め、電機子電流の位相を前記回転子のq軸に対して回転方向に遅らせることにより界磁磁束を強める制御を実施する回転電機システム。
The rotary electric machine according to any one of claims 1 to 4,
A control unit (42) that controls the phase of energization in the armature winding, and
It is a rotary electric system equipped with
The control unit weakens the field magnetic flux by advancing the phase of the armature current in the rotational direction with respect to the q-axis of the rotor, and causes the phase of the armature current to be in the rotational direction with respect to the q-axis of the rotor. A rotary armature system that controls to strengthen the field magnetic current by delaying it.
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