JP2009124852A - Rotor for rotary electric machine, and rotary electric machine - Google Patents

Rotor for rotary electric machine, and rotary electric machine Download PDF

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JP2009124852A
JP2009124852A JP2007295858A JP2007295858A JP2009124852A JP 2009124852 A JP2009124852 A JP 2009124852A JP 2007295858 A JP2007295858 A JP 2007295858A JP 2007295858 A JP2007295858 A JP 2007295858A JP 2009124852 A JP2009124852 A JP 2009124852A
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rotor
magnets
magnetic pole
electrical machine
magnet
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Nobuko Hamashima
暢子 濱島
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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 rotor for a rotary electric machine capable of achieving easy manufacture as well as high torque by tilting the orientation of magnets relative to a diametrical direction, and to provide the rotary electric machine with the rotor. <P>SOLUTION: The magnets having magnetic poles different from each other in a peripheral direction are polarized so that a radial magnetic flux passing through one point on a center line of the magnetic pole set on the outer-peripheral side of the respective magnetic poles is generated. At the same time, a ratio (R/r) of a distance R from an axial line of a rotating shaft to the one point on the center line of the magnetic pole to a distance r from the axial line of the rotating shaft to a surface (an outer-peripheral surface) of the magnet is set to ≥1.1. <P>COPYRIGHT: (C)2009,JPO&INPIT

Description

本発明は、回転電機のロータ及び回転電機に関するものである。   The present invention relates to a rotor of a rotating electrical machine and a rotating electrical machine.

従来、回転電機のインナロータでは、回転軸の軸線と直交する断面において磁場配向が径方向外側に向かって狭まるように放射状をなす磁石を備えたものがある(例えば特許文献1参照)。このようなロータでは、ステータと対向する磁石表面の磁束密度増加により強磁場が発生し、その結果、回転電機のトルク出力が向上するようになっている。
特開2005−253146号公報
2. Description of the Related Art Conventionally, an inner rotor of a rotating electrical machine includes a magnet having a radial shape such that a magnetic field orientation narrows radially outward in a cross section orthogonal to the axis of the rotation axis (see, for example, Patent Document 1). In such a rotor, a strong magnetic field is generated by increasing the magnetic flux density on the magnet surface facing the stator, and as a result, the torque output of the rotating electrical machine is improved.
JP 2005-253146 A

しかしながら、上記のようなロータにおいて、磁石における放射状の配向方向を結んだ一点(収束点)が磁石表面から近い、即ち、配向の径方向に対する傾斜が大きいと、大きなトルク向上効果が得られるが、磁石の配向傾斜を大きくしようとする程、その着磁が難しくなるという問題があり、この点においてなお改善の余地があった。   However, in the rotor as described above, when one point (convergence point) connecting the radial orientation directions in the magnet is close to the magnet surface, that is, when the inclination with respect to the radial direction of the orientation is large, a large torque improvement effect can be obtained. There is a problem that the magnetization becomes more difficult as the orientation gradient of the magnet is increased, and there is still room for improvement in this respect.

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、磁石の配向を径方向に対し傾斜させて高トルク化を図りつつも、容易に製造することができる回転電機のロータ及びこのロータを備えた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 its object is to provide a rotating electrical machine that can be easily manufactured while increasing the torque by inclining the orientation of the magnet with respect to the radial direction. And providing a rotating electric machine including the rotor.

上記課題を解決するために、請求項1に記載の発明は、周方向に交互に異なる磁極配置とされた磁石が回転軸に一体回転可能に設けられてなる回転電機のロータであって、前記磁石は、各磁極においてその外周側に設定された磁極中心線上の一点を通る放射状の磁束が生じるように着磁され、前記回転軸の軸線から前記磁極中心線上の一点までの距離Rと、前記回転軸の軸線から前記磁石の表面までの距離rとの比の値(R/r)が、1.1以上に設定されたことをその要旨とする。   In order to solve the above problem, the invention according to claim 1 is a rotor of a rotating electrical machine in which magnets having different magnetic pole arrangements alternately in a circumferential direction are provided on a rotary shaft so as to be integrally rotatable, The magnet is magnetized so that a radial magnetic flux passing through one point on the magnetic pole center line set on the outer circumferential side of each magnetic pole is generated, and the distance R from the axis of the rotating shaft to one point on the magnetic pole center line, The gist is that the ratio value (R / r) to the distance r from the axis of the rotation axis to the surface of the magnet is set to 1.1 or more.

この発明では、周方向に交互に異なる磁極配置とされた磁石は、各磁極においてその外周側に設定された磁極中心線上の一点を通る放射状の磁束が生じるように着磁され、回転軸の軸線から磁極中心線上の一点までの距離Rと、回転軸の軸線から磁石の表面までの距離rとの比の値(R/r)が1.1以上に設定される。ここで、距離R,rの比の値(ラジアル配向中心位置)とトルクとの関係を示す関係図から(図4参照)、そのR/rの値が1.1以上の範囲では、回転軸の軸線から磁極中心線上の一点と磁石の表面とが接近しない、即ち、磁石の配向傾斜が大きくならないようにしつつも、配向が径方向に沿う場合(図4中、トルク比が「1」)より大きなトルクを得られる。これにより、磁石の配向を径方向に対し傾斜させて回転電機のトルク出力を向上させつつも容易に製造することが可能となる。   In the present invention, magnets having different magnetic pole arrangements alternately in the circumferential direction are magnetized so that a radial magnetic flux passing through one point on the magnetic pole center line set on the outer circumferential side of each magnetic pole is generated, and the axis of the rotating shaft The ratio value (R / r) between the distance R from the center of the magnetic pole to one point on the magnetic pole center line and the distance r from the axis of the rotation axis to the surface of the magnet is set to 1.1 or more. Here, from the relational diagram showing the relationship between the value of the ratio of the distances R and r (radial orientation center position) and the torque (see FIG. 4), the rotation axis is within the range where the value of R / r is 1.1 or more. When a point on the magnetic pole center line does not approach from the axis of the magnet and the surface of the magnet, that is, the orientation is along the radial direction while preventing the orientation gradient of the magnet from increasing (the torque ratio is “1” in FIG. 4). Greater torque can be obtained. Thereby, it becomes possible to manufacture easily while making the orientation of the magnet inclined with respect to the radial direction and improving the torque output of the rotating electrical machine.

請求項2に記載の発明は、請求項1に記載の回転電機のロータにおいて、前記距離R,rの比の値(R/r)が、1.1以上、1.6以下に設定されたことをその要旨とする。
この発明では、距離R,rの比の値(R/r)が1.1以上、1.6以下に設定される。このため、容易に製造しつつも、R/rの値が1の場合、即ち、磁石の配向が最大で製造が最も困難となるとき以上の大きなトルク出力を得ることができる(図4参照)。
According to a second aspect of the present invention, in the rotor of the rotating electric machine according to the first aspect, a ratio value (R / r) of the distances R and r is set to 1.1 or more and 1.6 or less. This is the gist.
In the present invention, the ratio value (R / r) of the distances R and r is set to 1.1 or more and 1.6 or less. For this reason, while producing easily, when the value of R / r is 1, that is, when the orientation of the magnet is maximum and the production is most difficult, a larger torque output can be obtained (see FIG. 4). .

請求項3に記載の発明は、請求項2に記載の回転電機のロータにおいて、前記距離R,rの比の値(R/r)が、1.1以上、1.2以下に設定されたことをその要旨とする。
この発明では、距離R,rの比の値(R/r)を1.1以上、1.2以下に設定することで、1.1以上、1.6以下の範囲の中でもより一層の高トルク化に貢献できる。
According to a third aspect of the present invention, in the rotor of the rotating electric machine according to the second aspect, a ratio value (R / r) of the distances R and r is set to 1.1 or more and 1.2 or less. This is the gist.
In the present invention, the ratio value (R / r) of the distances R and r is set to 1.1 or more and 1.2 or less, so that it is even higher in the range of 1.1 or more and 1.6 or less. Can contribute to torque.

請求項4に記載の発明は、請求項1〜3のいずれか1項に記載のロータと、前記ロータの周囲に設けられ、該ロータの回転のための磁界を発生させる巻線が巻回されてなるステータとを備えた回転電機であることをその要旨とする。   According to a fourth aspect of the present invention, there is provided the rotor according to any one of the first to third aspects, and a winding that is provided around the rotor and that generates a magnetic field for rotating the rotor. The gist of the present invention is that the rotating electrical machine includes a stator.

この発明では、請求項1〜3のいずれか1項に記載のロータがステータの内側に設けられて回転電機が構成される。このため、磁石の配向を径方向に対し傾斜させて高トルク化を図りつつも、容易に製造することができる回転電機を提供することができる。   In this invention, the rotor according to any one of claims 1 to 3 is provided inside the stator to constitute a rotating electrical machine. Therefore, it is possible to provide a rotating electrical machine that can be easily manufactured while increasing the torque by inclining the orientation of the magnet with respect to the radial direction.

従って、上記記載の発明によれば、磁石の配向を径方向に対し傾斜させて高トルク化を図りつつも、容易に製造することができる回転電機のロータ及びこのロータを備えた回転電機を提供することができる。   Therefore, according to the above-described invention, there is provided a rotor of a rotating electrical machine that can be easily manufactured while increasing the torque by inclining the orientation of the magnet with respect to the radial direction, and a rotating electrical machine including the rotor. can do.

以下、本発明を具体化した一実施形態を図面に従って説明する。
図1に示すように、回転電機としてのブラシレスモータ(以下、モータという)1は、ステータ2とロータ3とを備える。ステータ2は、略円筒状に形成され、径方向内側に延びる12個のティース4と、それらティース4にそれぞれ巻回された巻線5とを備える。ステータ2は、その巻線5に図示しない電源装置からの電源が供給されるとロータ3を回転させるための回転磁界を発生するように構成される。
DESCRIPTION OF EXEMPLARY EMBODIMENTS Hereinafter, an embodiment of the invention will be described with reference to the drawings.
As shown in FIG. 1, a brushless motor (hereinafter referred to as a motor) 1 as a rotating electrical machine includes a stator 2 and a rotor 3. The stator 2 is formed in a substantially cylindrical shape, and includes twelve teeth 4 extending radially inward, and windings 5 wound around the teeth 4. The stator 2 is configured to generate a rotating magnetic field for rotating the rotor 3 when power from a power supply device (not shown) is supplied to the winding 5.

ステータ2の内側に回転可能に支持されたロータ3は、回転軸6と、回転軸6に固着された略円筒状のロータコア7と、ロータコア7の外周面に固定された10個の磁石8a,8bとを備えている。各磁石8a,8bは、円弧状をなし同一形状に形成されるとともに、磁束方向(磁石中の矢印)が外側を向いて外周面がN極となっている磁石8aと、磁束方向が内周側を向いて外周面がS極となっている磁石8bとが周方向に交互に配置されている(図2参照)。尚、各磁石8a,8bは周方向において互いに当接している。   The rotor 3 rotatably supported inside the stator 2 includes a rotating shaft 6, a substantially cylindrical rotor core 7 fixed to the rotating shaft 6, and ten magnets 8 a fixed to the outer peripheral surface of the rotor core 7. 8b. Each of the magnets 8a and 8b has an arc shape and is formed in the same shape, and the magnetic flux direction (arrow in the magnet) faces the outside and the outer peripheral surface is an N pole, and the magnetic flux direction is the inner circumference. The magnets 8b facing the side and having an S-pole outer peripheral surface are alternately arranged in the circumferential direction (see FIG. 2). The magnets 8a and 8b are in contact with each other in the circumferential direction.

図2に示すように、磁石8a,8bは、回転軸6の軸線Lと直交する断面において、径方向外側ほどその磁極中心線CL(ロータ径方向に沿うとともに各磁石8a,8bの周方向中心を通る線)に近づくように傾斜する磁束が生じる構成とされている。換言すると、磁石8a,8bは、その外側に配置された磁極中心線CL上の一点Pを通る放射状の磁束が生じる構成とされている。尚、磁石8a,8bの周方向中心部においては径方向(磁極中心線CL)に沿う磁束が生じている。   As shown in FIG. 2, the magnets 8 a and 8 b are arranged in the cross section orthogonal to the axis L of the rotating shaft 6, and the magnetic pole center line CL (the center in the circumferential direction of each magnet 8 a and 8 b is along the rotor radial direction). The magnetic flux which inclines so that it may approach the (line which passes through) is produced. In other words, the magnets 8a and 8b are configured to generate a radial magnetic flux that passes through one point P on the magnetic pole center line CL disposed on the outside thereof. Note that a magnetic flux along the radial direction (magnetic pole center line CL) is generated at the circumferential center of the magnets 8a and 8b.

このような磁石8a,8bの製造態様について図3に従って説明する。
図3に示すように、磁石8aは、その製造に際し所謂着磁器の一対の鉄芯11,12に挟まれる。この一対の鉄芯11,12にはそれぞれコイル(図示略)が巻回されており、一方の鉄芯11は磁石8aの内周面全面に当接し、他方の鉄芯12は磁石8aの外側でその周方向を2等分する直線(磁極中心線CLに一致)に沿って延出成形されている。そして、各鉄芯11,12に巻回されたコイルへの通電によりそれら鉄芯11,12に磁石8aの外側に配置された前記直線(CL)上の一点(点Pに一致)を通る放射状の磁束を生じさせ、磁石8aは、前述したような外側に配置された点Pを中心とする放射状の配向に着磁される。尚、磁石8bの着磁は、各鉄芯11,12に生じさせる磁束の極性を反転させることを除き、概ね同様に行われるためその説明を割愛する。このような点Pを外側に配置する着磁では、その点Pを磁石8a,8bの外周面から遠い位置に設定すればする程、磁石8a,8bの配向傾斜が緩やかとなり容易に着磁可能となっている。
A manufacturing mode of such magnets 8a and 8b will be described with reference to FIG.
As shown in FIG. 3, the magnet 8 a is sandwiched between a pair of iron cores 11 and 12 of a so-called magnetizer during its manufacture. Coils (not shown) are wound around the pair of iron cores 11 and 12, respectively. One iron core 11 is in contact with the entire inner peripheral surface of the magnet 8a, and the other iron core 12 is outside the magnet 8a. And extending along a straight line (corresponding to the magnetic pole center line CL) that bisects the circumferential direction. And, by energizing the coils wound around the iron cores 11 and 12, the iron cores 11 and 12 are radially passing through one point (matching the point P) on the straight line (CL) arranged outside the magnet 8a. The magnet 8a is magnetized in a radial orientation centered on the point P arranged outside as described above. Magnetization of the magnet 8b is performed in substantially the same manner except that the polarity of the magnetic flux generated in each of the iron cores 11 and 12 is reversed, and the description thereof is omitted. When magnetizing such a point P on the outside, as the point P is set at a position farther from the outer peripheral surface of the magnets 8a and 8b, the orientation inclination of the magnets 8a and 8b becomes gentler and can be easily magnetized. It has become.

上記のようなロータ3において、回転軸6の軸線Lから磁極中心線CL上の一点Pまでの距離を距離R、軸線Lから磁石8a,8bの外側の表面(外周面)までの距離を距離rとすると、磁石8a,8bのラジアル配向中心位置(点P)を表すこれら距離R,rの比の値(R/r)は、「1.125」に設定されている。   In the rotor 3 as described above, the distance from the axis L of the rotating shaft 6 to one point P on the magnetic pole center line CL is the distance R, and the distance from the axis L to the outer surface (outer peripheral surface) of the magnets 8a and 8b is the distance. Assuming r, the ratio value (R / r) of these distances R and r representing the radial orientation center position (point P) of the magnets 8a and 8b is set to “1.125”.

ここで、本発明者は、図4に示すように、距離R,rの比の値(R/r)に対するトルク特性を調べた。尚、同一形状(軸線Lから磁石8a,8bの外周面までの距離rが一定)という条件において、磁石8a,8bを径方向に配向した場合のトルクを「1」としている。   Here, as shown in FIG. 4, the inventor examined the torque characteristics with respect to the ratio value (R / r) of the distances R and r. Note that the torque when the magnets 8a and 8b are oriented in the radial direction under the condition of the same shape (the distance r from the axis L to the outer peripheral surfaces of the magnets 8a and 8b is constant) is “1”.

この図4から明らかなように、距離R,rの比の値(R/r)が1以上であれば、トルク比が約1.3以上で保持されており、高トルク化が見込めることが確認される。この範囲中において、R/rの値が小さくならない、即ち、磁石8a,8bの配向傾斜が大きくならない範囲を含まない「1.1」以上の範囲では磁石8a,8bの着磁容易化に非常に有利となる。また、このようなR/rの値が「1.1」以上の範囲の中で「1.6」以下の範囲では、配向傾斜が最大で着磁が最も困難となるR/rの値が「1」のとき以上のトルクを得ることができる。そして、本実施形態のR/rの値は、この1.1〜1.6の範囲の中でも、特に顕著なトルク向上効果が見込める1.1〜1.2の範囲でトルク比がほぼ最大となる「1.125」に設定されている。   As is clear from FIG. 4, if the ratio value (R / r) of the distances R and r is 1 or more, the torque ratio is maintained at about 1.3 or more, and a high torque can be expected. It is confirmed. In this range, the value of R / r does not decrease, that is, the range of “1.1” or more that does not include the range in which the orientation inclination of the magnets 8a and 8b does not increase is extremely easy to magnetize the magnets 8a and 8b. Is advantageous. In addition, when the value of R / r is in the range of “1.6” or less within the range of “1.1” or more, the value of R / r at which the orientation gradient is maximum and magnetization is most difficult is When “1”, a torque higher than that can be obtained. The value of R / r in this embodiment is almost the maximum in the range of 1.1 to 1.2 in which the remarkable torque improvement effect can be expected, among the range of 1.1 to 1.6. Is set to “1.125”.

また、図5には、距離R,rの比の値(R/r)を「1.125」とした場合のロータ3の表面磁束密度(図5中、実線で示す)と、磁石8a,8bを径方向に配向した場合のロータの表面磁束密度(図5中、2点鎖線で示す)とを比較して示す。この図5に示すように、距離R,rの比の値(R/r)を「1.125」とした場合のロータ3の表面磁束密度は、磁石8a,8bを径方向に配向した場合のロータの表面磁束密度と比較して高くなっている。即ち、本実施形態のモータ1の高トルク化が図られている。   5 shows the surface magnetic flux density of the rotor 3 (indicated by the solid line in FIG. 5) when the ratio value (R / r) of the distances R and r is “1.125”, and the magnets 8a, 8a, A comparison is made with the surface magnetic flux density (indicated by a two-dot chain line in FIG. 5) of the rotor when 8b is oriented in the radial direction. As shown in FIG. 5, the surface magnetic flux density of the rotor 3 when the ratio value (R / r) of the distances R and r is “1.125” is obtained when the magnets 8a and 8b are oriented in the radial direction. It is higher than the surface magnetic flux density of the rotor. That is, the torque of the motor 1 of this embodiment is increased.

こうして構成される本実施形態のモータ1では、点Pが外側に配置されるよう磁石8a,8bの配向を径方向に対し傾斜させることで高トルク化を図りつつも着磁の容易化が図られ、このような磁石8a,8bを用いることで、ロータ3、ひいてはモータ1全体を容易に製造することが可能となっている。   In the motor 1 of the present embodiment configured as described above, the magnets 8a and 8b are inclined with respect to the radial direction so that the point P is arranged on the outer side, thereby facilitating magnetization while achieving high torque. By using such magnets 8a and 8b, the rotor 3, and thus the motor 1 as a whole can be easily manufactured.

次に、本実施形態の特徴的な作用効果を記載する。
(1)本実施形態では、周方向に交互に異なる磁極配置とされた磁石8a,8bは、各磁極においてその外周側に設定された磁極中心線CL上の一点Pを通る放射状の磁束が生じるように着磁され、回転軸6の軸線Lから磁極中心線CL上の一点Pまでの距離Rと、回転軸6の軸線Lから磁石8a,8bの表面(外周面)までの距離rとの比の値(R/r)が1.1以上に設定される。図4に示す距離R,rの比の値(ラジアル配向中心位置)とトルクとの関係を示す関係図から、そのR/rの値が1.1以上の範囲では、回転軸6の軸線Lから磁極中心線CL上の一点Pと磁石8a,8bの表面とが接近しない、即ち、磁石8a,8bの配向傾斜が大きくならないようにしつつも、配向が径方向に沿う場合(図4中、トルク比が「1」)より大きなトルクを得られる。これにより、磁石8a,8bの配向を径方向に対し傾斜させてモータ1のトルク出力を向上させつつも容易に製造することが可能となる。
Next, characteristic effects of the present embodiment will be described.
(1) In the present embodiment, the magnets 8a and 8b having different magnetic pole arrangements alternately in the circumferential direction generate a radial magnetic flux passing through one point P on the magnetic pole center line CL set on the outer circumferential side of each magnetic pole. The distance R from the axis L of the rotating shaft 6 to a point P on the magnetic pole center line CL and the distance r from the axis L of the rotating shaft 6 to the surfaces (outer peripheral surfaces) of the magnets 8a and 8b. The ratio value (R / r) is set to 1.1 or more. From the relationship diagram showing the relationship between the value of the ratio of the distances R and r (radial orientation center position) and the torque shown in FIG. 4, the axis L of the rotary shaft 6 is within a range where the R / r value is 1.1 or more. In the case where the orientation is along the radial direction while the point P on the magnetic pole center line CL and the surfaces of the magnets 8a and 8b do not approach each other, that is, the orientation inclination of the magnets 8a and 8b does not increase (in FIG. Torque ratio is larger than “1”). Accordingly, the magnets 8a and 8b can be easily manufactured while the torque output of the motor 1 is improved by inclining the orientation of the magnets 8a and 8b with respect to the radial direction.

また、同図4に示すように、R/rの値が1.1以上、1.6以下の範囲では、その値が「1」の場合、即ち、磁石8a,8bの配向が最大で製造が最も困難となるとき以上の大きなトルク出力を得ることができる。そして、R/rの値が1.1以上、1.2以下の範囲では、1.1〜1.6の範囲の中でもより一層の高トルク化に貢献でき、更にその中でも「1.125」に設定する本実施形態では、ほぼ最大のトルク向上効果を得ることができる。   Further, as shown in FIG. 4, when the value of R / r is 1.1 or more and 1.6 or less, when the value is “1”, that is, the orientation of the magnets 8a and 8b is maximum. A torque output larger than that when it becomes the most difficult can be obtained. When the value of R / r is 1.1 or more and 1.2 or less, it can contribute to higher torque even within the range of 1.1 to 1.6, and among them, “1.125”. In the present embodiment, which is set to, a substantially maximum torque improvement effect can be obtained.

尚、本発明の実施形態は、以下のように変更してもよい。
・上記実施形態では、距離R,rの比の値(R/r)が「1.125」に設定されたが、その値以外に1.1以上の範囲内で変更してもよい。尚、R/rの値を大きくする程、磁石8a,8bの着磁が容易となる。
In addition, you may change embodiment of this invention as follows.
In the above embodiment, the ratio value (R / r) of the distances R and r is set to “1.125”, but may be changed within a range of 1.1 or more in addition to the value. As the value of R / r is increased, the magnets 8a and 8b are easily magnetized.

・上記実施形態では、磁極毎に分割された全部で10個の磁石8a,8bを用いたが、磁極が10極形成された1個の環状磁石を用いてもよい。
・上記実施形態では、ステータ2の極数を12(スロット)とし、ロータ3の極数を10としたが、それぞれ適宜変更してもよい。
In the above embodiment, a total of ten magnets 8a and 8b divided for each magnetic pole are used, but one annular magnet having ten magnetic poles may be used.
In the above embodiment, the number of poles of the stator 2 is 12 (slots) and the number of poles of the rotor 3 is 10. However, the number of poles may be changed as appropriate.

・上記実施形態では、ブラシレスモータ1に具体化したが、例えばブラシ付モータ等の他のモータに具体化してもよい。
次に、上記実施形態及び別例から把握できる技術的思想を以下に追記する。
In the above embodiment, the brushless motor 1 is embodied. However, for example, the motor may be embodied in another motor such as a brush motor.
Next, a technical idea that can be grasped from the above embodiment and another example will be added below.

(イ)距離R,rの比の値(R/r)が、1.1以上、2.0以下に設定される。
この構成によれば、製造の容易化を図りつつも、回転電機のトルク出力を効率的に向上させることが可能となる(図4参照)。
(A) The ratio value (R / r) of the distances R and r is set to 1.1 or more and 2.0 or less.
According to this configuration, it is possible to efficiently improve the torque output of the rotating electrical machine while facilitating manufacture (see FIG. 4).

本実施形態におけるブラシレスモータを示す模式図。The schematic diagram which shows the brushless motor in this embodiment. ロータの部分拡大図。The elements on larger scale of a rotor. 磁石の製造態様を示す模式図。The schematic diagram which shows the manufacture aspect of a magnet. ラジアル配向中心位置とトルクとの関係を示す関係図。FIG. 5 is a relationship diagram showing a relationship between radial alignment center position and torque. ロータの表面磁束密度分布図。The surface magnetic flux density distribution figure of a rotor.

符号の説明Explanation of symbols

L…軸線、CL…磁極中心線、P…磁極中心線CL上の一点、1…回転電機としてのブラシレスモータ、2…ステータ、3…ロータ、5…巻線、6…回転軸、8a,8b…磁石。   L: Axis line, CL: Magnetic pole center line, P: One point on the magnetic pole center line CL, 1 ... Brushless motor as a rotating electric machine, 2 ... Stator, 3 ... Rotor, 5 ... Winding, 6 ... Rotating shaft, 8a, 8b …magnet.

Claims (4)

周方向に交互に異なる磁極配置とされた磁石が回転軸に一体回転可能に設けられてなる回転電機のロータであって、
前記磁石は、各磁極においてその外周側に設定された磁極中心線上の一点を通る放射状の磁束が生じるように着磁され、
前記回転軸の軸線から前記磁極中心線上の一点までの距離Rと、前記回転軸の軸線から前記磁石の表面までの距離rとの比の値(R/r)が、1.1以上に設定されたことを特徴とする回転電機のロータ。
A rotor of a rotating electrical machine in which magnets having different magnetic pole arrangements alternately in the circumferential direction are provided on a rotating shaft so as to be integrally rotatable,
The magnet is magnetized so that a radial magnetic flux passing through one point on the magnetic pole center line set on the outer peripheral side of each magnetic pole is generated,
A ratio value (R / r) between a distance R from the axis of the rotating shaft to a point on the magnetic pole center line and a distance r from the axis of the rotating shaft to the surface of the magnet is set to 1.1 or more. A rotor of a rotating electrical machine characterized by being made.
請求項1に記載の回転電機のロータにおいて、
前記距離R,rの比の値(R/r)が、1.1以上、1.6以下に設定されたことを特徴とする回転電機のロータ。
The rotor of the rotating electrical machine according to claim 1,
A rotor of a rotating electrical machine, wherein a ratio value (R / r) of the distances R and r is set to 1.1 or more and 1.6 or less.
請求項2に記載の回転電機のロータにおいて、
前記距離R,rの比の値(R/r)が、1.1以上、1.2以下に設定されたことを特徴とする回転電機のロータ。
In the rotor of the rotating electrical machine according to claim 2,
A rotor of a rotating electrical machine, wherein a ratio value (R / r) of the distances R and r is set to 1.1 or more and 1.2 or less.
請求項1〜3のいずれか1項に記載のロータと、
前記ロータの周囲に設けられ、該ロータの回転のための磁界を発生させる巻線が巻回されてなるステータと
を備えたことを特徴とする回転電機。
The rotor according to any one of claims 1 to 3,
A rotating electrical machine comprising: a stator provided around the rotor and wound with a winding that generates a magnetic field for rotating the rotor.
JP2007295858A 2007-11-14 2007-11-14 Rotor for rotary electric machine, and rotary electric machine Abandoned JP2009124852A (en)

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Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015154533A (en) * 2014-02-12 2015-08-24 Wolongモーター制御技術株式会社 motor
JP2016165185A (en) * 2015-03-06 2016-09-08 アイシン精機株式会社 Electric motor
WO2019219986A3 (en) * 2019-03-11 2020-01-16 Siemens Gamesa Renewable Energy A/S Magnet assembly comprising magnet devices each having a focusing magnetic domain alignment pattern

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015154533A (en) * 2014-02-12 2015-08-24 Wolongモーター制御技術株式会社 motor
JP2016165185A (en) * 2015-03-06 2016-09-08 アイシン精機株式会社 Electric motor
WO2019219986A3 (en) * 2019-03-11 2020-01-16 Siemens Gamesa Renewable Energy A/S Magnet assembly comprising magnet devices each having a focusing magnetic domain alignment pattern

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