JPS61251438A - Rotor of rotary electric machine - Google Patents
Rotor of rotary electric machineInfo
- Publication number
- JPS61251438A JPS61251438A JP9147585A JP9147585A JPS61251438A JP S61251438 A JPS61251438 A JP S61251438A JP 9147585 A JP9147585 A JP 9147585A JP 9147585 A JP9147585 A JP 9147585A JP S61251438 A JPS61251438 A JP S61251438A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic pole
- rotor
- pole surface
- stator
- rear side
- 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.)
- Pending
Links
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K1/00—Details of the magnetic circuit
- H02K1/06—Details of the magnetic circuit characterised by the shape, form or construction
- H02K1/22—Rotating parts of the magnetic circuit
- H02K1/24—Rotor cores with salient poles ; Variable reluctance rotors
Abstract
Description
【発明の詳細な説明】 〔発明の利用分野〕 本発明は回転電機の回転子に関するものである。[Detailed description of the invention] [Field of application of the invention] The present invention relates to a rotor for a rotating electric machine.
第3図には突極形の回転電機の回転子の従来例が示され
ている。同図に示されているように回転子はシャフトl
、このシャフトlの上に設けられたヨーク2、このヨー
ク2の外周上に設けられ、かつその表面3aが固定子4
と空隙を介して対向配置された磁極3、この磁極3の胴
部に装着された界磁巻線5等を備えている。FIG. 3 shows a conventional example of a salient pole type rotor of a rotating electric machine. As shown in the figure, the rotor is connected to the shaft l
, a yoke 2 provided on this shaft l, provided on the outer periphery of this yoke 2, and whose surface 3a is connected to the stator 4.
The magnetic pole 3 is arranged to face the magnetic pole 3 with an air gap therebetween, and a field winding 5 attached to the body of the magnetic pole 3 is provided.
このように構成された回転子で磁極30表面3aすなわ
ち磁極表面3aは同図に示されているように、固定子4
の内周面に対して同心円上の周の一部をなすようになっ
ているので、磁極表面3aの円弧に沿りた空隙は極く端
部を除いてはほぼ一様であシ、従って磁極3の回転方向
wllc対して前側である磁極表面3aの前方側6と後
側である後方側7とKおける空隙は等しい。なお同図に
おいてdは界磁巻線起磁力の磁軸s’Raoは合成起磁
力の磁軸、Aは電機子反作用起磁力の磁軸である。In the rotor configured in this manner, the surface 3a of the magnetic pole 30, that is, the surface 3a of the magnetic pole 30 is connected to the stator 4 as shown in the figure.
The air gap along the arc of the magnetic pole surface 3a is almost uniform except for the very edges, and therefore The air gap between the front side 6 of the magnetic pole surface 3a, which is the front side, and the rear side 7, which is the rear side, of the magnetic pole surface 3a with respect to the rotation direction wllc of the magnetic pole 3 is equal. In the figure, d is the magnetic axis of the field winding magnetomotive force, s'Rao is the magnetic axis of the composite magnetomotive force, and A is the magnetic axis of the armature reaction magnetomotive force.
このような回転子を有する突極機の負荷運転中における
磁極表面3aの空隙部の起磁力分布が第4図に示されて
いる。同図においてdoは界磁巻線起磁力分布曲線、R
ooは合成起磁力分布曲線、A(1tri電機子反作用
起磁力分布曲線であシ、縦軸のRp 6は起磁力である
。同図および第3図から明らかなように合成起磁力の磁
軸Roは突極機の運転の場合に回転方向と反対の方向へ
界磁巻線起磁力の磁軸dよシずれるので、磁軸RoK相
当する磁極表面3a、すなわち磁極表面3aの後方饅7
が過熱する傾向があった。すなわち負荷時の磁極表面3
aの磁束分布も第4図忙示されているように5界磁巻線
起磁力の磁軸dから回軸方向に対して後側の合成起磁力
の磁軸R0の位置にピークがずれることになる。この状
態で回転すると、固定子4側のスロットの影響でこの磁
束のピーク値は高周波で変動するので、磁極表面3aの
後方側7が渦電流によシ加熱される。なおこの磁極表面
3aの後方側7の過熱を予防するものとして特開昭54
−10903号公報がある。FIG. 4 shows the magnetomotive force distribution in the gap of the magnetic pole surface 3a during load operation of a salient pole machine having such a rotor. In the figure, do is the field winding magnetomotive force distribution curve, R
oo is the composite magnetomotive force distribution curve, A (1tri armature reaction magnetomotive force distribution curve), and Rp on the vertical axis is the magnetomotive force.As is clear from the same figure and Fig. 3, the magnetic axis of the composite magnetomotive force When the salient pole machine is operated, Ro is shifted from the magnetic axis d of the field winding magnetomotive force in the direction opposite to the rotation direction, so the magnetic pole surface 3a corresponding to the magnetic axis RoK, that is, the rear portion 7 of the magnetic pole surface 3a
had a tendency to overheat. In other words, the magnetic pole surface 3 under load
As shown in Figure 4, the magnetic flux distribution of a also has a peak that deviates from the magnetic axis d of the 5-field winding magnetomotive force to the position of the magnetic axis R0 of the composite magnetomotive force on the rear side with respect to the rotational axis direction. become. When rotating in this state, the peak value of this magnetic flux fluctuates at high frequency due to the influence of the slots on the stator 4 side, so that the rear side 7 of the magnetic pole surface 3a is heated by eddy current. In addition, as a method for preventing overheating of the rear side 7 of the magnetic pole surface 3a, Japanese Patent Application Laid-Open No. 1983
There is a publication No.-10903.
本発明は以上の点に鑑みなされたものであシ、磁極表面
の温度を均一化することを可能とした回転電機の回転子
を提供することを目的とするものである。The present invention has been made in view of the above points, and an object of the present invention is to provide a rotor for a rotating electrical machine that makes it possible to equalize the temperature of the magnetic pole surface.
〔発明の概要〕
すなわち本発明はシャフトと、このシャフト上に設けら
れたヨークと、このヨークの外周上に設けられ、かつそ
の表面が固定子と空隙を介して対向配置された磁極と、
この磁極の胴部に装着された界磁巻線とを備えた回転電
機の回転子において、前記磁極を、その磁極表面と前記
固定子との空隙を前記磁極表面の回転方向に対する後方
側を前方側よシ大きく形成したことを特徴とするもので
あシ、これによって磁極は、その磁極表面と固定子との
空隙が磁極表面の回転方向に対する後方側が前方側よシ
大きく形成されるようKなる。[Summary of the Invention] That is, the present invention includes a shaft, a yoke provided on the shaft, a magnetic pole provided on the outer periphery of the yoke, and whose surface is arranged opposite to a stator with a gap therebetween.
In a rotor of a rotating electric machine equipped with a field winding attached to the body of the magnetic pole, the magnetic pole is arranged so that the gap between the magnetic pole surface and the stator is positioned so that the rear side with respect to the rotational direction of the magnetic pole surface is forward. The magnetic pole is characterized by being formed larger from the side, so that the gap between the magnetic pole surface and the stator is larger on the rear side with respect to the rotation direction of the magnetic pole surface than on the front side. .
以下、図示した実施例に基づいて本発明を説明する。第
1図には本発明の一実施例が示されている。なお従来と
同じ部品には同じ符号が付されているので説明を省略す
る。本実施例では磁極3bを、その磁極表面3aと固定
子4との空隙を磁極表面3aの回転方向Wに対する後方
側7を前方側6より大きく形成した。このようにすると
とにより磁極3bは、その磁極表面3aと固定子4との
空隙が磁極表面3aの回転方向Wに対する後方側7が前
方側6よシ大きく形成されるようになって、磁極表面3
aの温度を均一化することを可能とした回転電機の回転
子を得ることができる。The present invention will be explained below based on the illustrated embodiments. FIG. 1 shows an embodiment of the invention. It should be noted that the same parts as in the conventional one are given the same reference numerals, so the explanation will be omitted. In this embodiment, the gap between the magnetic pole surface 3a and the stator 4 of the magnetic pole 3b is formed so that the rear side 7 with respect to the rotation direction W of the magnetic pole surface 3a is larger than the front side 6. By doing this, in the magnetic pole 3b, the air gap between the magnetic pole surface 3a and the stator 4 is formed larger on the rear side 7 with respect to the rotation direction W of the magnetic pole surface 3a than on the front side 6, so that the magnetic pole surface 3
It is possible to obtain a rotor for a rotating electrical machine that makes it possible to equalize the temperature of a.
すなわち磁極表面3aと固定子4との空隙を磁極表面3
aの回転方向wK対する前方側6と後方側7とで非対称
とし、従来の固定子4の内周と同心円状としていた磁極
表面3aの形状(図中2点鎖線表示)に対し、図中実線
表示のように後方側7部での空隙が大きくなるように1
また前方側6では反対に小さくなるようにした。このよ
うにすることによシ突極機の負荷運転中における磁極表
面3aの空隙部の起磁力分布は第2図に示されているよ
うに1従来例(2点鎖線表示)に比較して本実施例(実
線表示)の合成起磁力分布曲線Roeのピーク値RP1
が従来例のピーク値RF。より小さくなる。このように
合成起磁力の磁軸R1における起磁力のピーク値が小さ
くなるのは、磁軸R1に相当する磁極表面3aの後方側
7と固定子4との空隙を前方側6の空隙より大きくした
ためで、磁極表面3aの後方側7と固定子4との磁気抵
抗が磁極表面3aの前方側6と固定子4との磁気抵抗よ
シ大きくなって、磁極表面3aの後方側7の磁束が磁極
表面3aの前方側6の磁束より小さくなるからである。In other words, the air gap between the magnetic pole surface 3a and the stator 4 is
Contrary to the shape of the magnetic pole surface 3a (indicated by a two-dot chain line in the figure), which is asymmetrical between the front side 6 and the rear side 7 with respect to the rotation direction wK of a and is concentric with the inner periphery of the stator 4 in the conventional art, the solid line in the figure 1 so that the gap on the rear side 7 becomes larger as shown.
On the other hand, the front side 6 is made smaller. By doing this, the magnetomotive force distribution in the gap of the magnetic pole surface 3a during load operation of the salient pole machine is as shown in FIG. Peak value RP1 of the composite magnetomotive force distribution curve Roe in this example (solid line display)
is the peak value RF of the conventional example. become smaller. The reason why the peak value of the magnetomotive force on the magnetic axis R1 of the composite magnetomotive force becomes smaller is that the air gap between the rear side 7 of the magnetic pole surface 3a corresponding to the magnetic axis R1 and the stator 4 is made larger than the air gap on the front side 6. As a result, the magnetic resistance between the rear side 7 of the magnetic pole surface 3a and the stator 4 becomes larger than the magnetic resistance between the front side 6 of the magnetic pole surface 3a and the stator 4, and the magnetic flux on the rear side 7 of the magnetic pole surface 3a increases. This is because it is smaller than the magnetic flux on the front side 6 of the magnetic pole surface 3a.
従って磁極表面3aの後方側7における渦電流による発
熱量が低下するようになって、後方側7の過熱が防止さ
れるようになシ、磁極表面3aの温度を均一にすること
ができる。Therefore, the amount of heat generated by the eddy current on the rear side 7 of the magnetic pole surface 3a is reduced, overheating of the rear side 7 is prevented, and the temperature of the magnetic pole surface 3a can be made uniform.
またこのように磁極表面5aの後方側7と固定子4との
空隙を前方側6のそれよシ大きくすることによシ、回転
中の磁極表面3aの風の流れは乱流となって、従来よシ
も磁極表面3aの後方側7の冷却効果を向上させること
ができる。Furthermore, by making the air gap between the rear side 7 of the magnetic pole surface 5a and the stator 4 larger than that between the front side 6, the flow of air on the rotating magnetic pole surface 3a becomes turbulent. The cooling effect on the rear side 7 of the magnetic pole surface 3a can be improved compared to the conventional case.
第5図には本発明の他の実施例が示されている。Another embodiment of the invention is shown in FIG.
本実施例は磁極表面3aの前方側6は変えないで磁極表
面3aの後方側7のみの空隙が大きくなるようKした。In this embodiment, the air gap is made larger only on the rear side 7 of the magnetic pole surface 3a without changing the front side 6 of the magnetic pole surface 3a.
このようにすることにより磁極表面3aの後方側7と固
定子4との空隙が、磁極表面3aの前方側6と固定子4
との空隙よシ大きくなって、前述の場合と同様な作用効
果を奏することができるが、これは界磁巻線5の界磁電
流容量に余裕がある場合に有効である。By doing this, the gap between the rear side 7 of the magnetic pole surface 3a and the stator 4 is increased, and the gap between the front side 6 of the magnetic pole surface 3a and the stator 4 is
The air gap between the magnet and the magnet becomes larger, and the same effect as in the case described above can be achieved, but this is effective when the field current capacity of the field winding 5 has a margin.
上述のように本発明は磁極表面の温度が均一化するよう
になって、磁極表面の温度を均一化することを可能とし
た回転電機の回転子を得ることができる。As described above, the present invention makes it possible to obtain a rotor for a rotating electric machine in which the temperature of the magnetic pole surface becomes uniform, thereby making it possible to equalize the temperature of the magnetic pole surface.
第1図は本発明の回転1!機の回転子の一実施例の断面
図、第2図は同じく一実施例の磁極表面の空隙部の起磁
力分布図、第3図は従来の回転電機の回転子の断面図、
第4図は同じ〈従来の磁極表面の空隙部の起磁力分布図
、第5図は本発明の回転電機の回転子の他の実施例の断
面図である。Figure 1 shows rotation 1 of the present invention! FIG. 2 is a magnetomotive force distribution diagram of the gap in the magnetic pole surface of the same example; FIG. 3 is a cross-sectional view of the rotor of a conventional rotating electrical machine;
FIG. 4 is the same conventional magnetomotive force distribution diagram in the gap portion of the magnetic pole surface, and FIG. 5 is a sectional view of another embodiment of the rotor of the rotating electrical machine of the present invention.
Claims (1)
、このヨークの外周上に設けられ、かつその表面が固定
子と空隙を介して対向配置された磁極と、この磁極の胴
部に装着された界磁巻線とを備えた回転電機の回転子に
おいて、前記磁極を、その磁極表面と前記固定子との空
隙を前記磁極表面の回転方向に対する後方側を前方側よ
り大きく形成したことを特徴とする回転電機の回転子。1. A shaft, a yoke provided on the shaft, a magnetic pole provided on the outer periphery of the yoke and whose surface faces the stator with an air gap in between, and a magnetic pole attached to the body of the magnetic pole. In the rotor of a rotating electric machine, the rotor is characterized in that the magnetic pole is formed so that the gap between the magnetic pole surface and the stator is larger on the rear side with respect to the rotational direction of the magnetic pole surface than on the front side. The rotor of a rotating electrical machine.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9147585A JPS61251438A (en) | 1985-04-26 | 1985-04-26 | Rotor of rotary electric machine |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9147585A JPS61251438A (en) | 1985-04-26 | 1985-04-26 | Rotor of rotary electric machine |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61251438A true JPS61251438A (en) | 1986-11-08 |
Family
ID=14027420
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9147585A Pending JPS61251438A (en) | 1985-04-26 | 1985-04-26 | Rotor of rotary electric machine |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61251438A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2011151138A3 (en) * | 2010-05-31 | 2012-09-13 | Robert Bosch Gmbh | Electrical machine with reduced noise development |
-
1985
- 1985-04-26 JP JP9147585A patent/JPS61251438A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2011151138A3 (en) * | 2010-05-31 | 2012-09-13 | Robert Bosch Gmbh | Electrical machine with reduced noise development |
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