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JP2001069701A - Magnet motor - Google Patents

Magnet motor

Info

Publication number
JP2001069701A
JP2001069701A JP24320099A JP24320099A JP2001069701A JP 2001069701 A JP2001069701 A JP 2001069701A JP 24320099 A JP24320099 A JP 24320099A JP 24320099 A JP24320099 A JP 24320099A JP 2001069701 A JP2001069701 A JP 2001069701A
Authority
JP
Japan
Prior art keywords
rotor
axis
iron core
radius
magnetic
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
JP24320099A
Other languages
Japanese (ja)
Inventor
Atsushi Akeda
淳 明田
Hiroshi Machida
博史 町田
Makoto Hattori
誠 服部
Akihiro Hoshino
昭広 星野
Shinichi Isobe
真一 磯部
Tetsuo Kanie
徹雄 蟹江
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Heavy Industries Ltd
Original Assignee
Mitsubishi Heavy Industries Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mitsubishi Heavy Industries Ltd filed Critical Mitsubishi Heavy Industries Ltd
Priority to JP24320099A priority Critical patent/JP2001069701A/en
Publication of JP2001069701A publication Critical patent/JP2001069701A/en
Withdrawn legal-status Critical Current

Links

Classifications

    • 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
    • H02K1/12Stationary parts of the magnetic circuit
    • H02K1/14Stator cores with salient poles
    • H02K1/146Stator cores with salient poles consisting of a generally annular yoke with salient poles
    • 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
    • H02K1/27Rotor cores with permanent magnets
    • H02K1/2706Inner rotors
    • H02K1/272Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis
    • H02K1/274Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis the rotor consisting of two or more circumferentially positioned magnets
    • H02K1/2753Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis the rotor consisting of two or more circumferentially positioned magnets the rotor consisting of magnets or groups of magnets arranged with alternating polarity
    • H02K1/276Magnets embedded in the magnetic core, e.g. interior permanent magnets [IPM]

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Permanent Field Magnets Of Synchronous Machinery (AREA)

Abstract

PROBLEM TO BE SOLVED: To suppress the induction of torque ripples in order to narrow the width of the torque ripple and to control the occurrence of vibration and noise, by forming the cross sectional shape of the outside circumference of a rotor in a sinusoidal waveform by making the radius of the rotor smallest at the positions of the ends of magnetic poles and largest at the positions of their central parts. SOLUTION: A plurality of flat-plane permanent magnets 107 are embedded near the surface of the outside circumference of a rotor 102. Also, air ranges 114 for preventing the short-circuit of magnetic paths are drilled in an iron core 106 between both ends of the magnetic poles of the permanent magnets 107, by cutting out a part of the iron core 106 which exists at the positions by the width corresponding to the thickness of the permanent magnet 117. Then, the shape of the outside circumference of the rotor 102 is set in a sinusoidal waveform, in the range from q-axis between each of the neighboring ends to the same q-axis in the opposite ends of the magnetic poles in the outside circumference of one magnetic pole of each permanent magnet 107, by making the radius of the rotor smallest at the positions of the q-axis and largest at that of d-axis that corresponds to the central position of the magnetic poles.

Description

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

【0001】[0001]

【発明の属する技術分野】本発明は密閉形圧縮機に使用
する磁石モータに関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnet motor used in a hermetic compressor.

【0002】[0002]

【従来の技術】従来の密閉形圧縮機の磁石モータの概要
について、図6、及び図7に基づいて説明する。図6は
従来の密閉形圧縮機の磁石モータを説明し、(a)は
(b)のA−A線に沿った縦断面、(b)は(a)のB
−B線に沿った縦断面を示し、図7は図6の磁石モータ
の中心に配置された従来のロータの横断面を示してい
る。
2. Description of the Related Art An outline of a conventional magnet motor of a hermetic compressor will be described with reference to FIGS. 6A and 6B illustrate a conventional hermetic compressor magnet motor, in which FIG. 6A is a longitudinal section taken along line AA in FIG. 6B, and FIG.
FIG. 7 shows a longitudinal section along line -B, and FIG. 7 shows a transverse section of a conventional rotor arranged at the center of the magnet motor of FIG.

【0003】すなわち、10は磁石モータで、2つの主
要部分であるステータ1とロータ2とから構成されてい
る。
That is, reference numeral 10 denotes a magnet motor, which comprises two main parts, a stator 1 and a rotor 2.

【0004】ここでステータ1は、薄肉の磁性鋼板を多
数積層してなる円筒状コア3に、その周方向に所定の間
隔を隔てて設けられた複数のスロット4を通して、多数
の電線5を巻き付けることによって構成されている。
In the stator 1, a large number of electric wires 5 are wound around a cylindrical core 3 formed by laminating a large number of thin magnetic steel sheets through a plurality of slots 4 provided at predetermined intervals in a circumferential direction thereof. It is constituted by that.

【0005】他方、ロータ2は、薄肉の磁性鋼板を多数
積層して円筒形状をなした鉄芯6と、該鉄芯6の周方向
に所定の間隔を隔てて配置され、その磁極が周方向に向
かい、かつ製造上許す限りロータ2の外表面に近く埋設
されている複数個( 本図に示すものでは4個 )の永久磁
石7を有し、該鉄心6の中心には回転軸8が貫通固定さ
れている。
[0005] On the other hand, the rotor 2 has a cylindrical iron core 6 formed by laminating a number of thin magnetic steel plates, and is disposed at a predetermined interval in the circumferential direction of the iron core 6. And a plurality of (four in the figure) permanent magnets 7 buried as close to the outer surface of the rotor 2 as manufacturing permits, and a rotating shaft 8 is provided at the center of the iron core 6. It is fixed through.

【0006】そして前記ロータ2の上端には上端板1
1、下端には下端板12が配設され、この上端板11及
び下端板12の間に配置された鉄芯6、永久磁石7と共
にリベット13により一体的に固着締結してロータ2が
構成されている。
An upper end plate 1 is provided at the upper end of the rotor 2.
1, a lower end plate 12 is disposed at the lower end, and the iron core 6 and the permanent magnet 7 disposed between the upper end plate 11 and the lower end plate 12 are integrally fixedly fastened together with rivets 13 to form the rotor 2. ing.

【0007】なお、前記した構造の永久磁石7の配置に
おいては、隣り合う永久磁石7の両端に形成される鉄心
6部分の存在によって、永久磁石7による磁束がロータ
2内で磁気回路を形成する磁路短絡構造となるのを防止
するため、永久磁石7の両磁極端部間には、この位置に
介在する鉄心6の一部を切欠き、該永久磁石7の厚さL
と略同じ幅で、かつロータ2の外周に沿った形状の空気
領域14が設けられている。
In the arrangement of the permanent magnets 7 having the above-described structure, the magnetic flux generated by the permanent magnets 7 forms a magnetic circuit in the rotor 2 due to the presence of the iron cores 6 formed at both ends of the adjacent permanent magnets 7. In order to prevent a magnetic path short-circuiting structure, a part of the iron core 6 interposed between the magnetic pole ends of the permanent magnet 7 is cut out, and the thickness L of the permanent magnet 7 is reduced.
An air region 14 having substantially the same width as that of the rotor 2 and a shape along the outer periphery of the rotor 2 is provided.

【0008】[0008]

【発明が解決しようとする課題】しかしながら、前記の
様に構成された従来のロータ2にあっては、ロータ2の
外周寄りで隣り合う永久磁石の磁極端部間に形成した空
気領域14を設けることによって、ロータ2の永久磁石
の磁極中心部を通るd軸及び隣り合う永久磁石の磁極端
部間を通るq軸における磁束の偏りは少なくなるが、図
4、及び図5中に黒丸点をプロットした「R(円形
状)」のデータを含めて示す様に、永久磁石7によるギ
ャップ磁束密度分布が矩形(図4参照)となって多くの
空間高調波の高次成分にトルク脈動を誘発し、また、平
均発生トルクに対して最大トルク脈動幅が大きくなり
(図5参照)、振動及び騒音が発生するという不具合が
あった。
However, in the conventional rotor 2 configured as described above, the air region 14 formed between the magnetic pole tips of the adjacent permanent magnets near the outer periphery of the rotor 2 is provided. By this, the bias of the magnetic flux on the d-axis passing through the center of the magnetic pole of the permanent magnet of the rotor 2 and the q-axis passing between the pole tips of the adjacent permanent magnets is reduced, but the black dots in FIG. 4 and FIG. As shown including the plotted "R (circular)" data, the gap magnetic flux density distribution by the permanent magnet 7 becomes rectangular (see FIG. 4) and induces torque pulsation in many high-order components of spatial harmonics. In addition, the maximum torque pulsation width becomes larger than the average generated torque (see FIG. 5), and there is a problem that vibration and noise are generated.

【0009】本発明は、このような従来の磁石モータの
ロータにおける不具合を解消し、トルク脈動の誘発を抑
制してトルク脈動幅を小さくし、振動及び騒音の発生の
抑制を図る様にした磁石モータを提供することを課題と
するものである。
The present invention solves such a problem in the rotor of the conventional magnet motor, suppresses the induction of torque pulsation, reduces the torque pulsation width, and suppresses the generation of vibration and noise. It is an object to provide a motor.

【0010】[0010]

【課題を解決するための手段】本発明は前記した課題を
解決すべくなされたもので、薄肉の磁性鋼板を多数積層
して鉄芯を形成し、この鉄芯の周方向に所定の間隔を隔
てて複数の永久磁石を、その磁極が周方向に向かうよう
に配置して埋設し、鉄芯の中心に固定軸を貫通固定して
なるロータを有する磁石モータにおいて、周方向で隣り
合う永久磁石の磁極端部間に介在する鉄芯の一部に磁路
短絡防止用の空気領域を穿設すると共に、ロータの断面
における外周形状を、ロータの半径が前記磁極端部の位
置で最小となり、磁極中心部の位置で最大となるように
正弦波変化させて形成した磁石モータを提供するもので
ある。
DISCLOSURE OF THE INVENTION The present invention has been made to solve the above-mentioned problems, and an iron core is formed by laminating a large number of thin magnetic steel sheets, and a predetermined interval is provided in the circumferential direction of the iron core. In a magnet motor having a rotor in which a plurality of permanent magnets are arranged and buried so that their magnetic poles face in the circumferential direction and a fixed shaft is fixed through the center of the iron core, permanent magnets adjacent in the circumferential direction are used. While drilling an air region for preventing magnetic path short circuit in a part of the iron core interposed between the magnetic pole tips, the outer peripheral shape in the cross section of the rotor, the radius of the rotor is minimized at the position of the magnetic pole tip, An object of the present invention is to provide a magnet motor formed by changing a sine wave so as to be maximum at a position of a magnetic pole center.

【0011】すなわち本発明によれば、ロータの半径を
磁極端部の位置と磁極中心部の位置で異ならせ、前者の
位置を最小、後者の位置を最大としてこの間で正弦波変
化させることにより、トルク脈動の誘発を抑制してトル
ク脈動幅を小さくし、振動及び騒音の発生を抑制する様
にしたものである。
That is, according to the present invention, the radius of the rotor is made different between the position of the magnetic pole end and the position of the center of the magnetic pole, and the sine wave is changed between the former position being the minimum and the latter being the maximum. The torque pulsation width is reduced by suppressing the induction of torque pulsation, thereby suppressing the generation of vibration and noise.

【0012】[0012]

【発明の実施の形態】本発明の実施の一形態について図
1乃至図5に基づいて説明する。図1は本実施の形態に
おける磁石モータの横断面図、図2、及び図3はロータ
の横断面図で、説明の便宜上ロータの形状に一定の差を
与えたものを示し、図2は磁極中心のロータ外周曲率小
の場合、図3は磁極中心のロータ外周曲率大の場合を示
し、図4はロータ電気角に対するギャップ磁束密度分
布、図5はロータ位置に対するモータ発生トルクを示す
説明図である。
DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described with reference to FIGS. FIG. 1 is a cross-sectional view of a magnet motor according to the present embodiment, and FIGS. 2 and 3 are cross-sectional views of a rotor in which a certain difference is given to the shape of the rotor for convenience of explanation. FIG. 3 shows a case where the radius of curvature of the rotor at the center is small, FIG. 3 shows a case where the radius of curvature of the rotor at the center of the magnetic pole is large, FIG. 4 is an explanatory view showing a gap magnetic flux density distribution with respect to the rotor electrical angle, and FIG. is there.

【0013】本実施の形態においては、ステータ101
とロータ102を主要部分として構成される磁石モータ
110において、ステータ101は前記した従来のもの
と同一であるので説明を省略し、ロータ102について
説明する。
In this embodiment, the stator 101
In the magnet motor 110 mainly including the rotor 102 and the rotor 102, the stator 101 is the same as the above-described conventional motor, and thus the description thereof is omitted, and the rotor 102 will be described.

【0014】すなわち、ロータ102は薄肉の磁性鋼板
が多数積層して鉄芯106を形成し、同鉄芯106の中
心には回転軸108が貫通固定され、他方、鉄芯106
の周囲には、周方向に所定の間隔を隔てて配置されてそ
の磁極が周方向に向かい、かつ許す限りロータ102の
外周表面近くに複数個(ここでは4個)の平板形状の永
久磁石107が埋設され、リベット113で一体的に固
着締結されている。
That is, the rotor 102 forms an iron core 106 by laminating a large number of thin magnetic steel plates, and a rotary shaft 108 is fixed through the center of the iron core 106.
, A plurality (four in this case) of plate-shaped permanent magnets 107 are arranged at predetermined intervals in the circumferential direction, and their magnetic poles face in the circumferential direction, and as close to the outer peripheral surface of the rotor 102 as possible. Are embedded and fixedly fastened together with rivets 113.

【0015】又、該永久磁石107の両磁極端部間の鉄
芯106には、永久磁石107の厚さに相当する幅でこ
こに介在する鉄芯106の一部を切り欠いて磁路短絡防
止用の空気領域114が穿設されている。
The iron core 106 between the two magnetic pole ends of the permanent magnet 107 has a width corresponding to the thickness of the permanent magnet 107, and a part of the iron core 106 interposed therebetween is cut off to short-circuit the magnetic path. An air region 114 for prevention is provided.

【0016】そしてロータ102の外周形状は、各永久
磁石107一極の磁極外周において、隣接する磁極端部
相互の間のq軸から逆の磁極端部における同様のq軸ま
での間において、ロータ102の半径がq軸の位置で最
小となり、他方、磁極中心の位置に当たるd軸の位置で
最大となるように正弦波変化する形状に設定されてい
る。
The outer peripheral shape of the rotor 102 is such that, at the outer circumference of one magnetic pole of each permanent magnet 107, the rotor 102 extends from the q-axis between adjacent pole tips to a similar q-axis at the opposite pole tip. The shape of the sine wave is set such that the radius of 102 becomes minimum at the position of the q-axis and maximum at the position of the d-axis corresponding to the center of the magnetic pole.

【0017】この様に構成された本実施の形態におい
て、前記正弦波変化する形状の程度に差をつけたものと
して、いま、ロータ102の半径がq軸での半径とd軸
での半径の差が永久磁石107の厚さLの1/2枚分の
断面形状となるものを図2に示してその場合のq軸から
d軸まで変化する半径をR1 とし、また、永久磁石10
7の厚さLの1枚分の断面形状となるものを図2に示し
てその場合のq軸からd軸まで変化する半径をR2 とす
れば、それぞれの場合におけるロータ102の半径は次
の式で設定される。
In the present embodiment having the above-described configuration, it is assumed that the shape of the sine wave-changing shape is different, and the radius of the rotor 102 is now the radius of the q axis and the radius of the d axis. the varying radius what difference is half sheets of the cross-sectional shape of the thickness L of the permanent magnet 107 shown in FIG. 2 from the q-axis in this case up to d-axis and R 1, also the permanent magnet 10
7 is a cross-sectional shape of one sheet having a thickness L of FIG. 7, and in this case, the radius changing from the q axis to the d axis is R 2, and the radius of the rotor 102 in each case is as follows. Is set by the following equation.

【0018】 R1 =(AL/2)+L/2 sinθ (図2の場合); R2 =(AL)+L sinθ (図3の場合); ここで R1 、R2 :ロータ102の変化する半
径; A:d軸でのロータ102の半径(R1 =R2 ); L:永久磁石107の厚さ; θ:電気角(0°≦θ≦180°); q軸からd軸まで変化する半径をR1 、R2 の何れの場
合でも、ロータ102の外周形状が、各永久磁石107
一極の磁極外周において、磁極端部(q軸)から逆の磁
極端部(q軸)までの間、ロータ102の半径がq軸で
最小となり、磁極中心(d軸)で最大となるように正弦
波変化する形状に設定されているので、ロータ102と
円筒内面を有するステータ101にて形成されるエアギ
ャップは正弦波状に変化する。
R 1 = (AL / 2) + L / 2 sin θ (case of FIG. 2); R 2 = (AL) + L sin θ (case of FIG. 3); where R 1 , R 2 : change of the rotor 102 Radius: A: radius of rotor 102 on d axis (R 1 = R 2 ); L: thickness of permanent magnet 107; θ: electrical angle (0 ° ≦ θ ≦ 180 °); changes from q axis to d axis Regardless of whether the radius of the rotation is R 1 or R 2 , the outer peripheral shape of the rotor 102
At the outer circumference of one pole, between the pole tip (q axis) and the opposite pole tip (q axis), the radius of the rotor 102 is minimum on the q axis and maximum at the center of the pole (d axis). The air gap formed by the rotor 102 and the stator 101 having a cylindrical inner surface changes in a sinusoidal manner.

【0019】そして図4、及び図5において黒三角でプ
ロットした「R1 (曲率小)」及び白抜き四角でプロッ
トした「R2 (曲率大)」で示す様に、ギャップ磁束密
度分布、及びトルク脈動は前記従来の技術として説明し
た「R(円形状)」で示すものに比べて抑制された小幅
のものとなる。
As shown by “R 1 (small curvature)” plotted with black triangles and “R 2 (large curvature)” plotted with open squares in FIGS. 4 and 5, gap magnetic flux density distribution and The torque pulsation has a smaller width than that shown by "R (circular shape)" described as the related art.

【0020】また、図2で示した変化する半径をR1
するものは、前記した様に永久磁石107厚さの1/2
枚分の変化で、これを1枚分変化させた図3における変
化する半径をR2 としたものに比べ、前者は後者より曲
率半径が大きいのでR1 を曲率小とし、R2 を曲率大と
しており、R1 とR2 の比較ではR2 の方がR1 より、
一層抑制された小幅のものとなる。
In the case where the changing radius shown in FIG. 2 is R 1 , as described above, one-half of the thickness of the permanent magnet 107 is used.
A change in sheets, which compared the varying radius in FIG. 3 was changed one sheet to those with R 2, the former because the radius of curvature is larger the R 1 and the small-curvature than the latter, the curvature size of R 2 In the comparison between R 1 and R 2 , R 2 is greater than R 1 .
The width is further reduced and reduced.

【0021】これはすなわち、d軸部ロータ102外周
の曲率の大小は、q軸とd軸のロータ102半径の差の
大小によって選択できることを示している。
This means that the magnitude of the curvature of the outer periphery of the d-axis rotor 102 can be selected according to the magnitude of the difference between the radius of the rotor 102 on the q-axis and the radius of the rotor 102.

【0022】かくして本実施の形態によれば、ロータ1
02外周の曲率が大きくなるにつれ、ギャップ磁束密度
分布は矩形波から正弦波に近ずき(図4参照)、発生ト
ルクに対する最大トルク脈動が小さくなる(図5参照)
ので、振動及び騒音を効果的に低減することが出来たも
のである。
Thus, according to the present embodiment, the rotor 1
02, as the curvature of the outer circumference increases, the gap magnetic flux density distribution approaches a sine wave from a rectangular wave (see FIG. 4), and the maximum torque pulsation with respect to the generated torque decreases (see FIG. 5).
Therefore, vibration and noise can be effectively reduced.

【0023】以上、本発明を図示の実施の形態について
説明したが、本発明はかかる実施の形態に限定されず、
本発明の範囲内でその具体的構造に種々の変更を加えて
よいことはいうまでもない。
Although the present invention has been described with reference to the illustrated embodiments, the present invention is not limited to such embodiments.
It goes without saying that various changes may be made to the specific structure within the scope of the present invention.

【0024】[0024]

【発明の効果】以上、本発明によれば、薄肉の磁性鋼板
を多数積層して鉄芯を形成し、この鉄芯の周方向に所定
の間隔を隔てて複数の永久磁石を、その磁極が周方向に
向かうように配置して埋設し、鉄芯の中心に固定軸を貫
通固定してなるロータを有する磁石モータにおいて、周
方向で隣り合う永久磁石の磁極端部間に介在する鉄芯の
一部に磁路短絡防止用の空気領域を穿設すると共に、ロ
ータの断面における外周形状を、ロータの半径が前記磁
極端部の位置で最小となり、磁極中心部の位置で最大と
なるように正弦波変化させて形成し磁石モータを構成し
ているので、ロータの半径を磁極端部の位置と磁極中心
部の位置で異ならせ、前者の位置を最小、後者の位置を
最大としてこの間で正弦波変化させることにより、トル
ク脈動の誘発を抑制してトルク脈動幅を小さくし、振動
及び騒音の発生を抑制させて、好適な磁石モータを得る
ことが出来たものである。
As described above, according to the present invention, an iron core is formed by laminating a large number of thin magnetic steel sheets, and a plurality of permanent magnets whose magnetic poles are formed at predetermined intervals in the circumferential direction of the iron core. In a magnet motor having a rotor arranged and buried so as to face in the circumferential direction and having a fixed shaft penetrated and fixed at the center of the iron core, the iron core interposed between the magnetic pole ends of the permanent magnets adjacent in the circumferential direction is A part of the air region for preventing a magnetic path short circuit is formed, and the outer peripheral shape in the cross section of the rotor is set so that the radius of the rotor is minimized at the position of the magnetic pole tip and maximized at the position of the magnetic pole center. Since the magnet motor is formed by changing the sine wave, the radius of the rotor is made different between the position of the magnetic pole end and the position of the center of the magnetic pole, and the former position is minimized, and the latter position is maximized. Wave change prevents torque pulsation induction And to reduce the torque pulsation width, by suppressing the generation of vibration and noise, in which it was possible to obtain a suitable magnet motor.

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

【図1】本発明の実施の一形態に係る磁石モータの横断
面図である。
FIG. 1 is a cross-sectional view of a magnet motor according to one embodiment of the present invention.

【図2】図1の磁石モータに組み入れるロータの一例を
示す横断面図である。
FIG. 2 is a cross-sectional view showing an example of a rotor incorporated in the magnet motor of FIG.

【図3】図1の磁石モータに組み入れるロータの他の例
を示す横断面図である。
FIG. 3 is a cross-sectional view showing another example of a rotor incorporated in the magnet motor of FIG.

【図4】ロータ電気角に対するギャップ磁束密度分布を
説明する説明図である。
FIG. 4 is an explanatory diagram illustrating a gap magnetic flux density distribution with respect to a rotor electrical angle.

【図5】ロータ位置に対するモータ発生トルクを示す説
明図である。
FIG. 5 is an explanatory diagram showing a motor generated torque with respect to a rotor position.

【図6】従来の磁石モータを示し、(a)は(b)のA
−A線に沿った縦断面図、(b)は(a)のB−B線に
沿った縦断面図である。
6A and 6B show a conventional magnet motor, wherein FIG. 6A shows A of FIG.
FIG. 4B is a longitudinal sectional view along the line A, and FIG. 4B is a longitudinal sectional view along the line BB in FIG.

【図7】図6の磁石モータに組み入れるロータを示す横
断面図である。
FIG. 7 is a cross-sectional view showing a rotor incorporated in the magnet motor of FIG.

【符号の説明】[Explanation of symbols]

1 ステータ 2 ロータ 3 円筒状コア 4 スロット 5 電線 6 鉄芯 7 永久磁石 8 回転軸 10 磁石モータ 11 上端板 12 下端板 13 リベット 14 空気領域 101 ステータ 102 ロータ 106 鉄芯 107 永久磁石 108 回転軸 110 磁石モータ 113 リベット 114 空気領域 DESCRIPTION OF SYMBOLS 1 Stator 2 Rotor 3 Cylindrical core 4 Slot 5 Electric wire 6 Iron core 7 Permanent magnet 8 Rotation axis 10 Magnet motor 11 Upper end plate 12 Lower end plate 13 Rivets 14 Air area 101 Stator 102 Rotor 106 Iron core 107 Permanent magnet 108 Rotation axis 110 Magnet Motor 113 Rivets 114 Air area

─────────────────────────────────────────────────────
────────────────────────────────────────────────── ───

【手続補正書】[Procedure amendment]

【提出日】平成12年2月10日(2000.2.1
0)
[Submission date] February 10, 2000 (2000.2.1
0)

【手続補正1】[Procedure amendment 1]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0017[Correction target item name] 0017

【補正方法】変更[Correction method] Change

【補正内容】[Correction contents]

【0017】この様に構成された本実施の形態におい
て、前記正弦波変化する形状の程度に差をつけたものと
して、いま、ロータ102の半径がq軸での半径とd軸
での半径の差が永久磁石107の厚さLの1/2枚分の
断面形状となるものを図2に示してその場合のq軸から
d軸まで変化する半径をR1 とし、また、永久磁石10
7の厚さLの1枚分の断面形状となるものを図3に示し
てその場合のq軸からd軸まで変化する半径をR2 とす
れば、それぞれの場合におけるロータ102の半径は次
の式で設定される。
In the present embodiment having the above-described configuration, it is assumed that the shape of the sine wave-changing shape is different, and the radius of the rotor 102 is now the radius of the q axis and the radius of the d axis. the varying radius what difference is half sheets of the cross-sectional shape of the thickness L of the permanent magnet 107 shown in FIG. 2 from the q-axis in this case up to d-axis and R 1, also the permanent magnet 10
7 is a cross-sectional shape corresponding to one sheet having a thickness L of FIG. 7, and the radius of change from the q-axis to the d-axis in that case is R 2, and the radius of the rotor 102 in each case is Is set by the following equation.

【手続補正2】[Procedure amendment 2]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】0018[Correction target item name] 0018

【補正方法】変更[Correction method] Change

【補正内容】[Correction contents]

【0018】 R1 =(A−L/2)+L/2 sinθ (図2の場合); R2 =(A−L)+L sinθ (図3の場合); ここで R1 、R2 :ロータ102の変化する半
径; A:d軸でのロータ102の半径(R1 =R2 ); L:永久磁石107の厚さ; θ:電気角(0°≦θ≦180°); q軸からd軸まで変化する半径をR1 、R2 の何れの場
合でも、ロータ102の外周形状が、各永久磁石107
一極の磁極外周において、磁極端部(q軸)から逆の磁
極端部(q軸)までの間、ロータ102の半径がq軸で
最小となり、磁極中心(d軸)で最大となるように正弦
波変化する形状に設定されているので、ロータ102と
円筒内面を有するステータ101にて形成されるエアギ
ャップは正弦波状に変化する。
[0018] (in the case of FIG. 2) R 1 = (A- L / 2) + L / 2 sinθ; R 2 = (A-L) + L sinθ ( case of FIG. 3); wherein R 1, R 2: rotor A: radius of the rotor 102 on the d axis (R 1 = R 2 ); L: thickness of the permanent magnet 107; θ: electrical angle (0 ° ≦ θ ≦ 180 °); from the q axis Regardless of whether the radius changing up to the d-axis is R 1 or R 2 , the outer peripheral shape of the rotor 102
At the outer circumference of one pole, between the pole tip (q axis) and the opposite pole tip (q axis), the radius of the rotor 102 is minimum on the q axis and maximum at the center of the pole (d axis). The air gap formed by the rotor 102 and the stator 101 having a cylindrical inner surface changes in a sinusoidal manner.

フロントページの続き (72)発明者 服部 誠 愛知県西春日井郡西枇杷島町旭町3丁目1 番地 三菱重工業株式会社エアコン製作所 内 (72)発明者 星野 昭広 名古屋市中村区岩塚町字高道1番地 三菱 重工業株式会社名古屋機器製作所内 (72)発明者 磯部 真一 名古屋市中村区岩塚町字高道1番地 三菱 重工業株式会社名古屋機器製作所内 (72)発明者 蟹江 徹雄 名古屋市中村区岩塚町字高道1番地 三菱 重工業株式会社名古屋研究所内 Fターム(参考) 5H622 AA03 CA02 CA07 CA13 CB05 CB06 PP10 PP11 PP14 PP16Continued on the front page (72) Inventor Makoto Hattori 3-1-1 Asahicho, Nishibiwajima-cho, Nishi-Kasugai-gun, Aichi Prefecture Inside Air Conditioning Works of Mitsubishi Heavy Industries, Ltd. (72) Inventor: Shinichi Isobe, Nagoya City, Nagoya City, Nagoya, Nagoya, Iwazuka, Nagoya, Machinery Works (72) Inventor: Mitsubishi Heavy Industries, Ltd. Address Mitsubishi Heavy Industries, Ltd. Nagoya Laboratory F-term (reference) 5H622 AA03 CA02 CA07 CA13 CB05 CB06 PP10 PP11 PP14 PP16

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 薄肉の磁性鋼板を多数積層して鉄芯を形
成し、この鉄芯の周方向に所定の間隔を隔てて複数の永
久磁石を、その磁極が周方向に向かうように配置して埋
設し、鉄芯の中心に固定軸を貫通固定してなるロータを
有する磁石モータにおいて、周方向で隣り合う永久磁石
の磁極端部間に介在する鉄芯の一部に磁路短絡防止用の
空気領域を穿設すると共に、ロータの断面における外周
形状を、ロータの半径が前記磁極端部の位置で最小とな
り、磁極中心部の位置で最大となるように正弦波変化さ
せて形成したことを特徴とする磁石モータ。
An iron core is formed by laminating a large number of thin magnetic steel plates, and a plurality of permanent magnets are arranged at predetermined intervals in a circumferential direction of the iron core so that their magnetic poles face in a circumferential direction. In a magnet motor having a rotor embedded and fixed with a fixed shaft passing through the center of the iron core, a part of the iron core interposed between the magnetic pole ends of the permanent magnets adjacent in the circumferential direction is used to prevent a magnetic path short circuit. And the outer peripheral shape in the cross section of the rotor is formed by changing the sine wave so that the radius of the rotor is minimum at the position of the magnetic pole tip and maximum at the position of the magnetic pole center. A magnet motor.
JP24320099A 1999-08-30 1999-08-30 Magnet motor Withdrawn JP2001069701A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24320099A JP2001069701A (en) 1999-08-30 1999-08-30 Magnet motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24320099A JP2001069701A (en) 1999-08-30 1999-08-30 Magnet motor

Publications (1)

Publication Number Publication Date
JP2001069701A true JP2001069701A (en) 2001-03-16

Family

ID=17100331

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24320099A Withdrawn JP2001069701A (en) 1999-08-30 1999-08-30 Magnet motor

Country Status (1)

Country Link
JP (1) JP2001069701A (en)

Cited By (17)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003081748A1 (en) * 2002-03-22 2003-10-02 Ebm-Papst St. Georgen Gmbh & Co. Kg Inner rotor motor
KR100486589B1 (en) * 2002-10-26 2005-05-03 엘지전자 주식회사 Structure of rotor for magnetic type motor
EP1713156A1 (en) * 2005-04-14 2006-10-18 Kabushiki Kaisha Toyota Jidoshokki Rotating electric machine with embedded permanent magnets
US7183685B2 (en) 2002-12-19 2007-02-27 Danfoss Compressors Gmbh Rotor for an electric motor
WO2007072622A1 (en) * 2005-12-21 2007-06-28 Honda Motor Co., Ltd. Electric motor
JP2007300692A (en) * 2005-04-14 2007-11-15 Toyota Industries Corp Rotary electric machine with embedded permanent magnet, motor for car air conditioner and enclosed motor-driven compressor
US20090115279A1 (en) * 2005-06-30 2009-05-07 Alessandro Spaggiari Rotor For An Electrical Machine
US7652405B2 (en) 2006-02-28 2010-01-26 Kabushiki Kaisha Toyota Jidoshokki Permanent magnet embedment rotating electric machine, motor for car air conditioner, and enclosed electric compressor
US7667363B2 (en) 2006-04-20 2010-02-23 Kabushiki Kaisha Toyota Jidoshokki Permanent magnet embedment rotating electric machine, motor for car air conditioner, and enclosed electric compressor
JP2012125016A (en) * 2010-12-07 2012-06-28 Yaskawa Electric Corp Motor
US20150130317A1 (en) * 2013-11-12 2015-05-14 Hon Hai Precision Industry Co., Ltd. Rotor and motor using the same
WO2016146910A1 (en) * 2015-03-16 2016-09-22 Valeo Equipements Electriques Moteur Rotor of a rotary electric machine with optimised placement of attachment means
EP3346583A1 (en) * 2017-01-04 2018-07-11 Chicony Power Technology Co., Ltd. Motor rotor and method for forming the same
CN112653273A (en) * 2020-12-23 2021-04-13 珠海格力节能环保制冷技术研究中心有限公司 Motor and compressor
WO2021140171A1 (en) * 2020-01-10 2021-07-15 Metabowerke Gmbh Arrangement comprising a stator laminate and a rotor laminate
CN113177277A (en) * 2021-05-06 2021-07-27 南京师范大学 Low-electromagnetic-torque-ripple and low-noise rotor and parametric modeling method thereof
US20230023710A1 (en) * 2019-12-17 2023-01-26 IFP Energies Nouvelles Synchronous reluctance machine having a variable air gap

Cited By (26)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6919663B2 (en) 2002-03-22 2005-07-19 Ebm-Papst St. Georgen Gmbh & Co. Kg Internal rotor motor
WO2003081748A1 (en) * 2002-03-22 2003-10-02 Ebm-Papst St. Georgen Gmbh & Co. Kg Inner rotor motor
KR100486589B1 (en) * 2002-10-26 2005-05-03 엘지전자 주식회사 Structure of rotor for magnetic type motor
US7183685B2 (en) 2002-12-19 2007-02-27 Danfoss Compressors Gmbh Rotor for an electric motor
JP2007300692A (en) * 2005-04-14 2007-11-15 Toyota Industries Corp Rotary electric machine with embedded permanent magnet, motor for car air conditioner and enclosed motor-driven compressor
US7521833B2 (en) 2005-04-14 2009-04-21 Kabushiki Kaisha Toyota Jidoshokki Permanent magnet embedment rotating electric machine, motor for car air conditioner, and enclosed electric compressor
EP1713156A1 (en) * 2005-04-14 2006-10-18 Kabushiki Kaisha Toyota Jidoshokki Rotating electric machine with embedded permanent magnets
US20090115279A1 (en) * 2005-06-30 2009-05-07 Alessandro Spaggiari Rotor For An Electrical Machine
US8405269B2 (en) * 2005-06-30 2013-03-26 Spal Automotive S.R.L. Rotor for an electrical machine
WO2007072622A1 (en) * 2005-12-21 2007-06-28 Honda Motor Co., Ltd. Electric motor
US8339010B2 (en) 2005-12-21 2012-12-25 Honda Motor Co., Ltd Dual rotor electric machine having a field-controlling rotor
JPWO2007072622A1 (en) * 2005-12-21 2009-05-28 本田技研工業株式会社 Electric motor
US7652405B2 (en) 2006-02-28 2010-01-26 Kabushiki Kaisha Toyota Jidoshokki Permanent magnet embedment rotating electric machine, motor for car air conditioner, and enclosed electric compressor
US7667363B2 (en) 2006-04-20 2010-02-23 Kabushiki Kaisha Toyota Jidoshokki Permanent magnet embedment rotating electric machine, motor for car air conditioner, and enclosed electric compressor
JP2012125016A (en) * 2010-12-07 2012-06-28 Yaskawa Electric Corp Motor
CN102570636A (en) * 2010-12-07 2012-07-11 株式会社安川电机 Electric motor
US20150130317A1 (en) * 2013-11-12 2015-05-14 Hon Hai Precision Industry Co., Ltd. Rotor and motor using the same
WO2016146910A1 (en) * 2015-03-16 2016-09-22 Valeo Equipements Electriques Moteur Rotor of a rotary electric machine with optimised placement of attachment means
FR3033960A1 (en) * 2015-03-16 2016-09-23 Valeo Equip Electr Moteur ROTOR OF ROTATING ELECTRIC MACHINE WITH IMPLANTATION OF OPTIMIZED MOUNTING MEANS
EP3346583A1 (en) * 2017-01-04 2018-07-11 Chicony Power Technology Co., Ltd. Motor rotor and method for forming the same
US20230023710A1 (en) * 2019-12-17 2023-01-26 IFP Energies Nouvelles Synchronous reluctance machine having a variable air gap
WO2021140171A1 (en) * 2020-01-10 2021-07-15 Metabowerke Gmbh Arrangement comprising a stator laminate and a rotor laminate
CN114731069A (en) * 2020-01-10 2022-07-08 麦太保有限公司 Device formed by stator lamination and rotor lamination
CN112653273A (en) * 2020-12-23 2021-04-13 珠海格力节能环保制冷技术研究中心有限公司 Motor and compressor
CN112653273B (en) * 2020-12-23 2022-04-08 珠海格力节能环保制冷技术研究中心有限公司 Motor and compressor
CN113177277A (en) * 2021-05-06 2021-07-27 南京师范大学 Low-electromagnetic-torque-ripple and low-noise rotor and parametric modeling method thereof

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