JPS6387161A - Rotary electric machine - Google Patents

Rotary electric machine

Info

Publication number
JPS6387161A
JPS6387161A JP22667586A JP22667586A JPS6387161A JP S6387161 A JPS6387161 A JP S6387161A JP 22667586 A JP22667586 A JP 22667586A JP 22667586 A JP22667586 A JP 22667586A JP S6387161 A JPS6387161 A JP S6387161A
Authority
JP
Japan
Prior art keywords
armature
field
cogging torque
magnetic
field system
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
Application number
JP22667586A
Other languages
Japanese (ja)
Inventor
Yoshimitsu Okawa
義光 大川
Hidetoshi Teruyama
照山 英俊
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 Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP22667586A priority Critical patent/JPS6387161A/en
Publication of JPS6387161A publication Critical patent/JPS6387161A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To reduce cogging torque, by using the armature of a salient pole type, and by providing a field system section with auxiliary grooves. CONSTITUTION:A rotary electric machine is composed of a back yoke 1, the field system section 2 of a permanent magnet, the armature core 4 of a salient pole type, and a threephase armature winding 5 wound up on the core. In this case, a section confronted with the armature core 4 in the field system section 2 is provided with auxiliary grooves 7a-7b in the direction of the axis of a rotational center 6. Then, magnetic flux generated from the field system section 2, bypassing field boundary sections 3a-3b and the auxiliary grooves 7a-7b, most of which are high magnetic reluctance, is absorbed by the armature core 4, and the state of the magnetic nonuniformity of the field system section is changed. Accordingly, harmonic component in relation to cogging torque is reduced, and the cogging torque can be reduced.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 こQ)発明は、給電するこdζより回転出力を得ろこ亡
ができる電動機、あZいは外部から回転力を与えここと
Cζより電気出力を得ろことができろ発電機亡いっrこ
回転電機に係り、特に界磁部亡章椰子亡の構成の改良に
関丁Zものである。
[Detailed description of the invention] [Field of industrial application] Q) The invention is an electric motor that can obtain a rotational output from a power supply and a rotational output from a Regarding rotary electric machines that can obtain output, I am particularly interested in improving the structure of the field section.

〔従来の技術〕[Conventional technology]

従来この種の回転市機として特公昭58−42707号
公報に示すもQlかあっ1こ。
A conventional rotary city machine of this type is shown in Japanese Patent Publication No. 58-42707, but it is called Ql or A1.

第4図は従来Q)回転電機0)−例を示ta略断面図で
ある。図Cζおいて、(1)はバー・クヨーク、(2)
+、t2極を形成する永久磁石Q)界磁部、(3&)(
8b)は上記界磁部(2)の境界部であり、(4)は突
極形の電機子鉄心、(5)は上記1に@子鉄心(4)に
巻装されγこ8相のiir機子機縁巻線り、界磁部(2
)ご電機子鉄心(4)は微少空隙を隔てて対向しており
、いずれか−万が他方に対して回転中心(6)を中心と
して回転自在ごなっでいる。
FIG. 4 is a schematic sectional view showing an example of a conventional Q) rotating electrical machine. In figure Cζ, (1) is Bar Quyoke, (2)
+, t2 permanent magnet forming pole Q) field part, (3 &) (
8b) is the boundary of the field part (2), (4) is the salient pole type armature core, and (5) is the 8-phase iir machine edge winding, field part (2
) The armature cores (4) are opposed to each other with a minute gap in between, and one of the armature cores (4) is rotatable relative to the other about the rotation center (6).

第4図の回転電機を電動機と考えるき、電機子巻線(5
)に順次通電才ろことEこより界磁部(2)とQ)電磁
相互作用により連続回転トルクを得ろことができる。ま
Tこ、発電機と考えろと、回転子である界磁部(2)を
外部から回転させろことにより電機子巻線(5)げ交流
出力を得ろこさができろ。
When considering the rotating electric machine in Figure 4 as an electric motor, the armature winding (5
) can be sequentially energized to obtain continuous rotating torque through electromagnetic interaction between the field part (2) and Q). Think of it as a generator, and by rotating the field part (2), which is the rotor, from the outside, you can get an AC output from the armature winding (5).

一般に突極形の電機子鉄心と界磁用永久磁石を用いTコ
場合は、磁気的に不均一部分が生じ21コめ、両者の相
互作用によりコギングトルクを発生才ろ欠点がある。
In general, when a salient pole type armature core and a field permanent magnet are used, magnetically non-uniform areas occur, and cogging torque is generated due to interaction between the two, which has the disadvantage of being ineffective.

コギングトルクは界a部とwI機子鉄心の磁気的不均一
性に関連し両方に周期性がある場合番とは、その両者に
共通して存在する調波成分+IM合成分成分1周波数と
なる。
Cogging torque is related to the magnetic inhomogeneity of the field a part and the wI machine core, and when both have periodicity, the frequency is the harmonic component + IM composite component 1 frequency that exists in common to both. .

第5図(1)は、第4図の回転電機の界磁部(2)の磁
界の周期性を1回転分表わしTコものであり、基本的な
調波成分は磁極数2を次数とする第2次調波底分となり
、第4次、第6次・・・・・・等の高調波成分を含む(
1回転に1回のくり返し成分を第1次調波底分とし、以
下同様扱いと才ろ。)。
Figure 5 (1) shows the periodicity of the magnetic field in the field part (2) of the rotating electric machine in Figure 4 for one rotation, and the fundamental harmonic component has the number of magnetic poles of 2 as the order. This is the second harmonic base and includes the fourth, sixth, etc. harmonic components (
The component that repeats once per revolution is considered the first harmonic base, and the rest can be treated in the same way. ).

111機子鉄心(4)l磁気的不均一性は突極部のパー
ミアンス変動に起因し、基本的な調波成分は第3次調波
底分となり、第6次、第9次・・・・・・等の高調ff
i分(含む。従って、コギングトルクはt記界a部(2
)とW機縁鉄心(4)OI調波成分が一致(整合)する
時1ζ発生し、本例)ζおいては、第6次、第12次・
・・・・・@の調波成分が主;ζ発生し、第5図(2)
にコギングトルク1回転分を示す。
111 Machine core (4) l Magnetic non-uniformity is caused by permeance fluctuations in the salient pole part, and the fundamental harmonic component is the 3rd harmonic bottom, 6th, 9th... ...etc. high pitch ff
i minutes (including. Therefore, the cogging torque is t boundary a part (2
) and W edge core (4) 1ζ occurs when the OI harmonic components match (match), and in this example) ζ, the 6th, 12th,
...The harmonic component of @ is mainly generated; ζ, as shown in Fig. 5 (2)
shows the cogging torque for one rotation.

〔発明が解決しようとtろ問題点〕[Problems that the invention does not solve]

前述の通り、突極形0 )B′電機子鉄心用い、界磁用
に永久磁石を用いる亡、山気的不均一を生じコギングト
ルクを発生する問題声があつ1こ。
As mentioned above, when using a salient pole type 0)B' armature core and using a permanent magnet for the field, there are complaints that unevenness occurs and cogging torque is generated.

こQ1発明は、突極形電機子を有しf(がらもコギング
トルクを著しく軽減させ1こ回転7機を得ろことを目的
としている。
The purpose of the Q1 invention is to significantly reduce the cogging torque by having a salient pole type armature and to obtain a single rotation 7 machine.

〔問題点を解決する1コめの手段〕 この発明に係る(口)転市機は、P個(但しPは2以上
J+!!1数)Q+磁極を形成才乙界磁部亡複数相Q1
電機子巻線か巻装された巻線用の溝および突極を有する
wI機子を具備し、上記界磁部を電機子のうちいずれか
一方を他方1ζ対して回転させろようにし、上記界磁部
の上記電機予き対向する位置に補助溝を設け、上記補助
溝を有する界磁部の磁気的不均一性の基本的な調波成分
の次数をnp(但しnは2以上の整数)とし、上記電機
子の巻線用の溝による磁気的不均一性の基本的な調波成
分をm次(但しmは整数)とtろとき、npがmの公倍
数またはmがnpO+公倍数さr(らないように構成し
γこものである。
[First means for solving the problem] The market switching machine according to the present invention has the ability to form P magnetic poles (where P is 2 or more and J+!!1), and has a field magnetic section that is capable of forming Q+ magnetic poles. Q1
The armature winding is provided with a wI armature having a groove for the wound winding and a salient pole, the field part is configured to rotate one of the armatures with respect to the other 1ζ, and the field An auxiliary groove is provided in the magnetic part at a position facing the electric machine, and the order of the fundamental harmonic component of the magnetic non-uniformity of the field part having the auxiliary groove is np (where n is an integer of 2 or more). If the fundamental harmonic component of the magnetic non-uniformity due to the grooves for the winding of the armature is the mth order (where m is an integer), then np is a common multiple of m or m is npO + common multiple r (It is constructed so that it does not occur.)

〔作用〕[Effect]

この発明Cζおいでは、界磁部に補助溝を設け1ここと
により、調e成分を高次1こt6゜〔発明の実施例〕 息下、この発発明の実施を図について説明する。
In this invention Cζ, an auxiliary groove is provided in the field part so that the harmonic e component can be adjusted to a higher order.

第1図は概略断面を示し、図中(1)から(6)は第4
図Q)従来例亡同様であり、+7aハ(7b)は界磁部
(2)でw!襲子鉄心(4ヒ対回才ろ部分をこ設けられ
Tコ補助溝であり、回転中心(6)の軸方向に設けられ
でいろ。
Figure 1 shows a schematic cross section, and (1) to (6) in the figure are the fourth
Figure Q) Same as the conventional example, +7a C (7b) is w! in the field part (2). The auxiliary groove is provided in the thruster iron core (the 4-piece rotation part is provided with a T-shaped auxiliary groove, and is provided in the axial direction of the rotation center (6).

界磁部(2)かち出る磁束は、大部分が磁気低抗の高い
界磁境界部(3aハ(3h)及び補助溝trh)。
Most of the magnetic flux emitted from the field part (2) comes from the field boundary part (3a c (3h) and the auxiliary groove trh) where the magnetic resistance is high.

(7h)を避けτ′N、s子鉄心(4)Gで吸収されろ
。こQ)結果界磁部(2)t7’!気的な不均一性の状
態は変化する。第1図に示し1ここの発明の実施例1ζ
おいては、界磁境界部(aaハ(3h)の間隔を2等分
する位置に補助ff1(7a)、(7J を設けてta
aJ、<7a)。
Avoid (7h) and absorb it by τ'N, s-core (4)G. Q) Result field part (2) t7'! The state of atmospheric heterogeneity changes. Embodiment 1 of the invention shown in FIG.
In this case, auxiliary ff1 (7a) and (7J) are provided at the position that equally divides the interval between the field boundaries (aac (3h)).
aJ, <7a).

tahハ(7b)0’全体が回転中心(6)に対してほ
ぼ等間隔きなるようiζ配置されている。
The entire tah (7b)0' is arranged at approximately equal intervals with respect to the center of rotation (6).

従−て界磁部(2)の磁気的不均一性の8期の基本成分
は第4次調び成分ごなり、第8次、第12次・・・・・
・等の高調波成分が含まtする、一方、電機子鉄心(4
)の有する調波成分は、第4図の従来例と同様であり、
その結果コキングトシレク亡しては主1ζ第12次、第
24次・・・・・・等の調波成分が発生し、基本的な調
波成分の次数は第4図OI従来例では第6次であルのに
対し、この実施例では第12次ご2倍の高次成分となっ
ており、第6次、第18次・・・・・・等の調波成分が
消滅、減少している。そして第2図はこ0)発明の界磁
部(2)の磁界の周期性とコギングトルク1回転分を示
す。
Therefore, the basic component of the 8th period of magnetic inhomogeneity in the field part (2) is the 4th harmonic component, the 8th order, the 12th order, etc.
On the other hand, the armature core (4
) has the same harmonic components as the conventional example shown in FIG.
As a result, harmonic components such as the 12th harmonic, the 24th harmonic, etc. of the main 1ζ are generated when the coking torque is lost, and the order of the fundamental harmonic component is the 6th harmonic in the OI conventional example shown in Figure 4. In contrast, in this example, the 12th order is twice as high-order, and the 6th, 18th, etc. harmonic components disappear or decrease. There is. FIG. 2 shows the periodicity of the magnetic field of the field section (2) of the invention and the cogging torque for one rotation.

一般にコギングトルクの各成分の大きさは、界磁部(2
)6市機子鉄心(4)t7i有τろ該当成分の大きさの
mlζ比例し、更!?:6欠取分になる程その大きさは
減少するUめ第6火成分に対し第12欠取分はかなり小
さくなる。
Generally, the magnitude of each component of cogging torque is
) 6 city machine iron core (4) t7i with τ is proportional to mlζ of the size of the corresponding component, further! ? :The size of the 6th fraction decreases as it becomes 6 fractions, whereas the 12th fraction becomes considerably smaller.

従ってこの発明により補助溝を設けることfζよりコギ
ングトルクに関与する調波成分を減少し、更に基本的な
調波成分を高次とすZこ亡によりコギングトルクを著し
く軽減するこ亡ができろ。
Therefore, by providing the auxiliary groove according to the present invention, it is possible to reduce the harmonic components related to cogging torque from fζ, and furthermore, it is possible to significantly reduce the cogging torque by increasing the basic harmonic components to a higher order. .

こQ)時突極形7椰子+71磁気的不均−性の基本的な
mv成分をm?:に亡すると、第m次、第2m次。
Q) What is the basic mv component of the time salient pole type 7 palm + 71 magnetic inhomogeneity? : When you die, the mth and 2mth.

第8m次・・・・・・等の&’4波成分を含んでおり、
補助溝のない界磁部0)磁気的不均一性の基本的な調波
成分は、その極数をPとすると第9次となり、補助溝を
設けること蚕こより界磁部の基本的な調波成分がnp次
(1旦しnは2以上の整数)きなるも0)とすこご、コ
ギングトルクの基本的な調波成分17>次数は、mとn
pの最小公倍数ごなろ。
Contains &'4 wave components such as 8th m order...
Field part without auxiliary grooves 0) The basic harmonic component of magnetic inhomogeneity is the 9th order, where the number of poles is P. Providing auxiliary grooves will improve the fundamental harmonic component of the field part. The fundamental harmonic components of cogging torque are m and n.
The least common multiple of p.

なお、補助溝ご界磁境界部の総数(npに相当)を電機
子突極数(mに相当λの公倍数ごならないようえ、ある
いはmがnpの公倍数亡なちないように配設する必要が
ある。
In addition, it is necessary to arrange the total number of auxiliary grooves and field boundaries (corresponding to np) so that the number of armature salient poles (corresponding to m) does not become a common multiple of λ, or so that m does not become a common multiple of np. There is.

ま1こ、界磁境界部さ補助溝の全体を回転中心に対して
等角度間隔あるいはほぼ等角r!i間隔ごなるように配
置することによりコギングトルク低減効果を更に高める
ことができる。
Well, the entire auxiliary groove at the field boundary part is equiangularly spaced or almost equiangularly r from the center of rotation! By arranging them at i intervals, the cogging torque reduction effect can be further enhanced.

第1図に示しrここの発発明1実施例においては、vI
機子を回転子tし、界磁部を@疋子とする場合Q1み蒼
こ限ち才その関係が逆であっても、効果は同一である。
In the first embodiment of the invention shown in FIG.
When the rotor is the rotor t and the field part is @ hiko, the effect is the same even if the relationship is reversed.

ま7:第3図に示すクロく補助溝(7aj(7N(70
J(7d)(7e)(7f)亡数を増D口することによ
りコギングトルクQ)基本調波成分+71次数を更に高
くすることができそQr大きさケ著しく低減することが
できる。
M7: Black auxiliary groove (7aj (7N (70
By increasing the numbers J(7d)(7e)(7f), the cogging torque Q) fundamental harmonic component +71st order can be further increased and the magnitude of Qr can be significantly reduced.

〔発明の効果〕〔Effect of the invention〕

以上のようにこの発明によれば従来の突極形の電機子を
使用し、界磁部に補助溝を設けるように構成しtこQr
でコギングトルクの低減を安価に効果的Gこ行なうこと
ができる。
As described above, according to the present invention, a conventional salient pole type armature is used, and an auxiliary groove is provided in the field part.
Cogging torque can be effectively reduced at low cost.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図はこの発明の一実施例による概略断面図、第2図
はこの発明による磁界分布ごコギングトルクを示す波形
図、第3図はこの発明の他の実施例による概略断面図、
第4図は従来の概略断面図、第5図は従来の磁界分布t
コギングトルクを示す波形図である。 図において(1)はバルクヨーク、(2)は界磁部、(
3a九Cab)は界磁磁極境界部、(4)は電機子、(
5)は電機子巻線、(6)ハ回転中心、<78)<7b
)t7C)<7d)(7e)(7f)は補助溝である。 なお、図中、同一符号は同一、ま1こは相当部分を示す
FIG. 1 is a schematic cross-sectional view according to an embodiment of the present invention, FIG. 2 is a waveform diagram showing magnetic field distribution and cogging torque according to the present invention, and FIG. 3 is a schematic cross-sectional view according to another embodiment of the present invention.
Fig. 4 is a conventional schematic cross-sectional view, and Fig. 5 is a conventional magnetic field distribution t.
FIG. 3 is a waveform diagram showing cogging torque. In the figure, (1) is the bulk yoke, (2) is the field part, (
3a9Cab) is the field magnetic pole boundary, (4) is the armature, (
5) is the armature winding, (6) C is the center of rotation, <78) <7b
)t7C)<7d) (7e) (7f) are auxiliary grooves. In addition, in the figures, the same reference numerals indicate the same parts, and squares indicate corresponding parts.

Claims (2)

【特許請求の範囲】[Claims] (1)P個(但しPは2以上の整数)の磁極を形成する
界磁部と複数相の電機子巻線が巻装された巻線用の溝及
び突極を有する電機子を具備し、上記界磁部と電機子の
うちいずれか一方を他方に対して回転させるようにし、
上記界磁部の上記電機子と対向する位置に補助溝を設け
、上記補助溝を有する界磁部の磁気的不均一性の基本的
な調波成分の次数をnp(但しnは2以上の整数)とし
、上記電機子の巻線用の溝による磁気的不均一性の基本
的な調波成分をm次(但しmは整数)とするとき、np
がmの公倍数またはmがnpの公倍数とならないように
構成したことを特徴とする回転電機。
(1) Equipped with a field part forming P magnetic poles (where P is an integer of 2 or more), and an armature having winding grooves and salient poles in which multi-phase armature windings are wound. , one of the field part and the armature is rotated relative to the other;
An auxiliary groove is provided in the field part at a position facing the armature, and the order of the fundamental harmonic component of the magnetic non-uniformity of the field part having the auxiliary groove is np (where n is 2 or more). np
1. A rotating electric machine characterized in that it is configured such that np is not a common multiple of m or m is not a common multiple of np.
(2)界磁磁極各境界部と各補助溝とを互いに回転中心
に対して等角度間隔もしくはほぼ等角度間隔となるよう
に配置したことを特徴とする特許請求の範囲第1項記載
の回転電機。
(2) The rotation according to claim 1, wherein each boundary part of the field magnetic pole and each auxiliary groove are arranged at equal angular intervals or approximately equal angular intervals with respect to the center of rotation. Electric machine.
JP22667586A 1986-09-25 1986-09-25 Rotary electric machine Pending JPS6387161A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22667586A JPS6387161A (en) 1986-09-25 1986-09-25 Rotary electric machine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22667586A JPS6387161A (en) 1986-09-25 1986-09-25 Rotary electric machine

Publications (1)

Publication Number Publication Date
JPS6387161A true JPS6387161A (en) 1988-04-18

Family

ID=16848893

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22667586A Pending JPS6387161A (en) 1986-09-25 1986-09-25 Rotary electric machine

Country Status (1)

Country Link
JP (1) JPS6387161A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005043715A3 (en) * 2003-10-31 2005-08-11 Magna Steyr Fahrzeugtechnik Ag Actuator with an electric control motor and controllable friction clutch provided with said actuator
JP2012227978A (en) * 2011-04-14 2012-11-15 Asmo Co Ltd Magnet yoke and dc motor
KR20140056985A (en) * 2012-11-02 2014-05-12 (주) 보쉬전장 Permanent magnet motor for cogging torque reduction
JP2018129985A (en) * 2017-02-10 2018-08-16 キヤノンプレシジョン株式会社 Motor and magnet

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2005043715A3 (en) * 2003-10-31 2005-08-11 Magna Steyr Fahrzeugtechnik Ag Actuator with an electric control motor and controllable friction clutch provided with said actuator
JP2007510400A (en) * 2003-10-31 2007-04-19 マグナ・シユタイル・フアールツオイクテヒニク・アクチエンゲゼルシヤフト・ウント・コンパニー・コマンデイトゲゼルシヤフト Actuator with electric servo motor and controllable friction clutch with electric servo motor
JP2012227978A (en) * 2011-04-14 2012-11-15 Asmo Co Ltd Magnet yoke and dc motor
KR20140056985A (en) * 2012-11-02 2014-05-12 (주) 보쉬전장 Permanent magnet motor for cogging torque reduction
JP2018129985A (en) * 2017-02-10 2018-08-16 キヤノンプレシジョン株式会社 Motor and magnet

Similar Documents

Publication Publication Date Title
JP4207386B2 (en) Inductor-type electric machine with magnet-equipped armature
KR101231024B1 (en) Consequent pole permanent magnet motor
EP0295718B1 (en) Method for winding a motor with armature teeths and field magnet
JP5542849B2 (en) Switched reluctance motor
JP2008514167A (en) Synchronous machine
JPH1014185A (en) Synchronous motor
JP2008514166A (en) Synchronous machine
JP2006149192A (en) Electrical rotating field apparatus and primary side
JP4657820B2 (en) Annular winding motor
Yokoi et al. Stator design of alternate slot winding for reducing torque pulsation with magnet designs in surface-mounted permanent magnet motors
JPS6223536B2 (en)
JPH0638475A (en) Permanent magnet rotary electric machine, controlling method therefor, controller and electric motor vehicle using the same
JPS6387161A (en) Rotary electric machine
JP2010057208A (en) Rotary electric machine
Harke Fractional slot windings with a coil span of two slots and less content of low order harmonics
JPH1169679A (en) Permanent magnet type motor
JPH05161325A (en) Synchronous motor with a reduced cogging torque
US20220085674A1 (en) Rotary electric machine
WO2008037264A1 (en) Winding scheme for a polyphase electric machine having a permanent magnet rotor
JPH04322152A (en) Three-phase brushless motor
JP2023049139A (en) Rotary electric machine
JPH0670524A (en) Brushless motor
JPS62114454A (en) Brushless motor
JP3713116B2 (en) 3-phase hybrid stepping motor
JP3612401B2 (en) 3-phase hybrid stepping motor