JPH02266859A - Stator for dc machine - Google Patents
Stator for dc machineInfo
- Publication number
- JPH02266859A JPH02266859A JP8682189A JP8682189A JPH02266859A JP H02266859 A JPH02266859 A JP H02266859A JP 8682189 A JP8682189 A JP 8682189A JP 8682189 A JP8682189 A JP 8682189A JP H02266859 A JPH02266859 A JP H02266859A
- Authority
- JP
- Japan
- Prior art keywords
- field
- permanent magnet
- magnetic flux
- armature
- winding
- 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
Landscapes
- Dc Machiner (AREA)
- Permanent Field Magnets Of Synchronous Machinery (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は直流機における固定子の界磁構造及びその製造
方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a field structure of a stator in a DC machine and a method of manufacturing the same.
従来の装置は、特開昭48−39906号公報に記載の
ように、補極は電機子反作用を利用して励磁するように
し、更に制御巻線を設けて補極に生ずる磁束を制御でき
るように構成されていた。In the conventional device, as described in Japanese Patent Application Laid-open No. 48-39906, the commutating poles are excited using armature reaction, and a control winding is further provided to control the magnetic flux generated in the commutating poles. It was composed of
上記従来技術は、電機子反作用の減磁界側に配置した永
久磁石の永久減磁についての配慮がされておらず、実用
時に永久減磁による直流機の性能が低下する問題があっ
た。The above-mentioned conventional technology does not take into consideration the permanent demagnetization of the permanent magnet placed on the demagnetizing field side of the armature reaction, and there is a problem that the performance of the DC machine deteriorates due to permanent demagnetization in practical use.
更には補極は制御巻線によって補極の磁束量を制御する
ものであるから、磁束を増す方向に制御すると無負荷回
転数が減少し、磁束を減少する方向に制御するとトルク
が低下する問題があった。Furthermore, since the amount of magnetic flux of the commutating pole is controlled by the control winding, if the magnetic flux is controlled to increase, the no-load rotation speed will decrease, and if the magnetic flux is controlled to decrease, the torque will decrease. was there.
本発明の目的は、永久磁石の永久減磁防止と補極の制御
巻線による磁束の増加を図ることにある。An object of the present invention is to prevent permanent demagnetization of a permanent magnet and to increase magnetic flux by a control winding of a commutating pole.
上記目的を達成するために、電機子反作用の増磁界側に
永久磁石を、減磁界側に巻線界磁を並置した界磁構造に
したものである。In order to achieve the above object, a field structure is used in which a permanent magnet is juxtaposed on the magnetizing field side of the armature reaction, and a winding field is juxtaposed on the demagnetizing field side.
直流機の界磁極において、電機子反作用の増磁界側に永
久磁石を配置することによって、永久磁石に電機子反作
用の減磁界が作用しないため、永久磁石の永久減磁が発
生しない。このため、永久磁石からは安定した磁束量が
得られる。By arranging the permanent magnet on the side of the magnetizing field of the armature reaction in the field pole of the DC machine, the demagnetizing field of the armature reaction does not act on the permanent magnet, so permanent demagnetization of the permanent magnet does not occur. Therefore, a stable amount of magnetic flux can be obtained from the permanent magnet.
また、同減磁界側に巻線界磁を並置することにより直巻
特性が得られる。即ち、高負荷時には大電流によって磁
束量が増し高トルクが得られ、軽負荷時には低電流によ
って高回転が得られる。Further, by arranging a winding field on the same demagnetizing field side, a series winding characteristic can be obtained. That is, when the load is high, a large current increases the amount of magnetic flux and high torque is obtained, and when the load is light, a low current allows high rotation.
したがって、永久磁石と巻線界磁を組合せることによっ
て、従来に比し高性能な直流機を得ることができる。Therefore, by combining permanent magnets and wire-wound fields, it is possible to obtain a DC machine with higher performance than conventional machines.
以下、本発明の一実施例を第1図により説明する。 An embodiment of the present invention will be described below with reference to FIG.
1は直流機の固定子で、2は円筒状の継鉄、3は継鉄内
周に固定された永久磁石、4は界磁巻線5を巻装した磁
極で、永久磁石3と磁極4によって界磁極6を構成して
いる。7は電機子であり、電機子巻線8を巻装して成る
。1 is a stator of a DC machine, 2 is a cylindrical yoke, 3 is a permanent magnet fixed to the inner periphery of the yoke, 4 is a magnetic pole around which a field winding 5 is wound; The field pole 6 is constituted by the above. Reference numeral 7 denotes an armature, which is formed by winding an armature winding 8.
第2図は、界磁極の構成を固定子1の中央部から見た図
で、磁極4の軸長Lpは電機子鉄芯の積厚とほぼ等しく
定めるが、永久磁石3の軸長り。FIG. 2 is a view of the configuration of the field poles as seen from the center of the stator 1. The axial length Lp of the magnetic poles 4 is determined to be approximately equal to the stacking thickness of the armature core, but the axial length of the permanent magnets 3.
は上記積厚より大きく定め、永久磁石からの有効磁束の
増加を図ったものである。is set to be larger than the above stacking thickness in order to increase the effective magnetic flux from the permanent magnet.
更に第3図は、永久磁石3の形状をコの字形として界磁
巻線5の側面部にも配置した構造である。Furthermore, FIG. 3 shows a structure in which the permanent magnet 3 is U-shaped and is also placed on the side surface of the field winding 5.
以上のような構成において、動作を第4図により説明す
る。まず、10のスイッチを投入すると9のバッテリー
の十から流れた電流は界磁巻線5を通り、磁極4を励磁
して電機子7を通り、再びバッテリーの−に戻る。The operation of the above configuration will be explained with reference to FIG. First, when the switch 10 is turned on, the current flowing from the battery 9 passes through the field winding 5, excites the magnetic pole 4, passes through the armature 7, and returns to the - battery again.
このような動作において、界磁極の磁束量は第5図に示
すように電機子電流Iaが小さい領域では永久磁石3か
らの磁束量が電機子鉄心を通るため、巻線界磁単独機に
比較し大きな磁束量が得られるため大きなトルクが得ら
れる。In such an operation, the amount of magnetic flux of the field pole is smaller than that of a machine with only a wound field because the amount of magnetic flux from the permanent magnet 3 passes through the armature core in the region where the armature current Ia is small, as shown in Figure 5. Since a large amount of magnetic flux can be obtained, large torque can be obtained.
次に電機子電流Iaが大きな領域では、界磁巻線からの
大きな磁束量に加え、永久磁石からの磁束量も加わるた
め、更に大きな磁束量が得られることにより大きなトル
クを発生することができる。Next, in a region where the armature current Ia is large, in addition to the large amount of magnetic flux from the field winding, the amount of magnetic flux from the permanent magnet is also added, so a larger amount of magnetic flux is obtained, which makes it possible to generate a larger torque. .
電機子電流の中間の領域では、従来永久磁石式と巻線界
磁式の中間のトルク特性が得られる。In an intermediate range of armature current, torque characteristics between those of the conventional permanent magnet type and the wound field type can be obtained.
また、第1図において、電機子巻線に通電すると電機子
反作用によって磁極4の側に減磁界が、永久磁石3の側
には増磁界が作用する。このため、永久磁石は永久減磁
の発生が起こらないため、いかなる使用条件においても
性能が低下する欠陥は発生しない。更には、永久磁石性
能の保磁力が小さくて良いため残留磁束密度の大きな磁
石を選択できるので、界磁極の磁束量を増加する効果が
得られる。Further, in FIG. 1, when the armature winding is energized, a demagnetizing field acts on the magnetic pole 4 side and an increasing field acts on the permanent magnet 3 side due to armature reaction. For this reason, permanent magnets do not suffer from permanent demagnetization, so defects that degrade performance do not occur under any usage conditions. Furthermore, since the coercive force of the permanent magnet performance may be small, a magnet with a large residual magnetic flux density can be selected, so that the effect of increasing the amount of magnetic flux of the field pole can be obtained.
第2図は界磁極の磁極長さを示したが、磁極4の軸長L
pは電機子7の鉄芯積層より厚くしても磁束量を増加す
る効果は無いが、永久磁石3の軸長はトルク増加に効果
あるためL p < L−とじトルク性能向上を図る。Figure 2 shows the magnetic pole length of the field pole, but the axial length L of magnetic pole 4 is
Even if p is made thicker than the iron core lamination of the armature 7, it will not have the effect of increasing the amount of magnetic flux, but since the axial length of the permanent magnet 3 will have an effect on increasing the torque, L p < L - Stapling torque performance is improved.
第3図は更に永久磁石の端部の磁束を有効に活用し、高
性能化を図った構造である。FIG. 3 shows a structure that further improves performance by effectively utilizing the magnetic flux at the end of the permanent magnet.
尚、永久磁石3の内径寸法と磁極4の内径寸法は同一と
することがなく、どちらかに差を設けても良い。Note that the inner diameter dimension of the permanent magnet 3 and the inner diameter dimension of the magnetic pole 4 do not have to be the same, and a difference may be provided in either one.
また、磁極4は別体成形品を固定しても良く、継鉄と同
時に打抜いた積層鉄心によっても良い。Further, the magnetic pole 4 may be fixed as a separate molded product, or may be a laminated core punched out at the same time as the yoke.
本発明によれば、電機子電流の小さい領域においては巻
線式より高トルク、磁石式より高回転の性能が得られ、
電機子電流が大きい領域においては磁石式より高トルク
の性能が得られる磁気回路構成としたことで従来の直流
機では一長一短があり、用途において制限があったが、
本発明によって広い用途に使用できる効果がある。According to the present invention, in a region where the armature current is small, higher torque than the wire-wound type and higher rotation performance than the magnet type can be obtained.
In areas where the armature current is large, the magnetic circuit configuration provides higher torque performance than the magnetic type, so conventional DC machines have advantages and disadvantages and are limited in their applications.
The present invention has the advantage that it can be used in a wide range of applications.
更には永久磁石の永久減磁の発生がないため、使用条件
に制限がなく、用途が拡大できる。Furthermore, since there is no permanent demagnetization of the permanent magnet, there are no restrictions on the usage conditions and the range of applications can be expanded.
第1図は本発明の一実施例を示す直流機の要部正面図、
第2図、第3図は界磁極を中心部から見た平面図、第4
図は一実施例の回路図、第S図は一実施例の電機子電流
に対する界磁極磁束量を示す図である。
1・・・固定子、2・・・継鉄、3・・・永久磁石、4
・・・m極、5・・・界磁巻線、6・・・界磁極、7・
・・電機子、8・・・電第
図
第
図FIG. 1 is a front view of the main parts of a DC machine showing one embodiment of the present invention;
Figures 2 and 3 are plan views of the field poles viewed from the center;
The figure is a circuit diagram of one embodiment, and FIG. S is a diagram showing the amount of field pole magnetic flux with respect to armature current of one embodiment. 1...Stator, 2...Yoke, 3...Permanent magnet, 4
...m pole, 5...field winding, 6...field pole, 7.
...Armature, 8...Electronic chart diagram
Claims (1)
において、電機子反作用の増磁界側に永久磁石を、同減
磁界側に巻線磁界を並置して磁極構成を特徴とする直流
機の固定子。1. In the stator of a DC machine consisting of a yoke, a permanent magnet, and a winding field, the magnetic pole structure is characterized by juxtaposing the permanent magnet on the side of the increasing field of armature reaction and the winding magnetic field on the side of the demagnetizing field. Stator of DC machine.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8682189A JPH02266859A (en) | 1989-04-07 | 1989-04-07 | Stator for dc machine |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8682189A JPH02266859A (en) | 1989-04-07 | 1989-04-07 | Stator for dc machine |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02266859A true JPH02266859A (en) | 1990-10-31 |
Family
ID=13897473
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8682189A Pending JPH02266859A (en) | 1989-04-07 | 1989-04-07 | Stator for dc machine |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02266859A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6563248B2 (en) | 2000-12-28 | 2003-05-13 | Asmo Co., Ltd. | Hybrid-magnet DC motor |
| US6707213B2 (en) | 2002-04-04 | 2004-03-16 | Asmo Co., Ltd. | Hybrid magnet type DC motor |
| JP2010063255A (en) * | 2008-09-03 | 2010-03-18 | Mitsubishi Electric Corp | Dc series motor and starter |
-
1989
- 1989-04-07 JP JP8682189A patent/JPH02266859A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6563248B2 (en) | 2000-12-28 | 2003-05-13 | Asmo Co., Ltd. | Hybrid-magnet DC motor |
| US6707213B2 (en) | 2002-04-04 | 2004-03-16 | Asmo Co., Ltd. | Hybrid magnet type DC motor |
| JP2010063255A (en) * | 2008-09-03 | 2010-03-18 | Mitsubishi Electric Corp | Dc series motor and starter |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP3152405B2 (en) | Electric motor | |
| US4517483A (en) | Permanent magnet rotor with saturable flux bridges | |
| US4454438A (en) | Synchronized induction motor | |
| EP0889574A1 (en) | Reluctance type rotating machine with permanent magnets | |
| JPH08340651A (en) | Permanent magnet and permanent magnet type rotating electrical machine | |
| US4794291A (en) | Permanent magnet field DC machine | |
| JPH08316049A (en) | DC reactor | |
| JPH0116102B2 (en) | ||
| IE43265B1 (en) | Rare earth permanent magnet rotor for dynamo electric machines and method of manufacturing same | |
| US4727273A (en) | Permanent magnet type electric motor | |
| EP0215441A2 (en) | Miniature electric rotating machine | |
| JP2010154676A (en) | Permanent magnet motor and hermetic compressor | |
| JPS6158459A (en) | Permanent magnet field type DC machine | |
| JPH02266859A (en) | Stator for dc machine | |
| JPS6149901B2 (en) | ||
| JP3784629B2 (en) | Current limiter | |
| JPH0767274A (en) | Permanent magnet rotor | |
| JPS6212741B2 (en) | ||
| JPH0810981B2 (en) | Permanent magnet type DC rotating electric machine | |
| JPH02266858A (en) | Stator for dc machine | |
| JPH04344159A (en) | Dc motor | |
| JPH0833304A (en) | Voice coil type linear motor | |
| JPS60219951A (en) | magnetic electric motor | |
| JP3690261B2 (en) | Rotating electric machine | |
| JPH0140308Y2 (en) |