JPS5928868A - Permanent magnet type dc electric machine - Google Patents
Permanent magnet type dc electric machineInfo
- Publication number
- JPS5928868A JPS5928868A JP13625982A JP13625982A JPS5928868A JP S5928868 A JPS5928868 A JP S5928868A JP 13625982 A JP13625982 A JP 13625982A JP 13625982 A JP13625982 A JP 13625982A JP S5928868 A JPS5928868 A JP S5928868A
- Authority
- JP
- Japan
- Prior art keywords
- permanent magnet
- magnet
- magnetic
- center
- poles
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K23/00—DC commutator motors or generators having mechanical commutator; Universal AC/DC commutator motors
- H02K23/02—DC commutator motors or generators having mechanical commutator; Universal AC/DC commutator motors characterised by arrangement for exciting
- H02K23/04—DC commutator motors or generators having mechanical commutator; Universal AC/DC commutator motors characterised by arrangement for exciting having permanent magnet excitation
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Permanent Field Magnets Of Synchronous Machinery (AREA)
- Dc Machiner (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は永久磁石式1u流磯に係り、特に異方性覗
永久磁石全主極に用い、その主極に補助磁極を並設して
形成した界磁を有する永久磁石式iM流磯に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a permanent magnet type 1u floating rock, in particular, a permanent magnet used for all main poles of an anisotropic peeking permanent magnet and having a field formed by arranging auxiliary magnetic poles in parallel to the main pole. Regarding magnetic iM Nagaiso.
従来一般に知られているスクータ等の永久磁石式直流機
は、例えばt時公昭48−35721号公報にある如<
?Ifl幾子反幾月反作用減磁対策として減磁作用側に
補極を設けることが行われている。Conventionally known permanent magnet type DC machines such as scooters are described, for example, in Publication No. 48-35721.
? Ifl Ikuko As a countermeasure against demagnetization caused by the anti-Ikumo reaction, a commutating pole is provided on the demagnetization side.
即ち、回転子中心から放射状に伸びる中心線と平行に両
端をψノ断した異カ性永級磁石(主磁極)と、この磁石
と空隙をもって隣接する補助磁極(鉄心)とで+1q成
したものか、あるいは主磁極と補助磁極の対向面を全面
にわたり密着して4’l’l’成したものとがあるが1
周知の通り異方性永久磁石eユ半径方向に磁束が通るた
め回転方向に補助磁極を密着して並設した場合は両者の
間に漏洩イ1゛釦、!3φ。In other words, a magnet with +1q is formed by a heterogeneous permanent magnet (main magnetic pole) with both ends cut in ψ parallel to the center line extending radially from the rotor center, and an auxiliary magnetic pole (iron core) adjacent to this magnet with an air gap. Alternatively, there is one in which the opposing surfaces of the main magnetic pole and auxiliary magnetic pole are closely contacted over the entire surface to form a 4'l'l'.
As is well known, the magnetic flux passes through the anisotropic permanent magnet e in the radial direction, so if the auxiliary magnetic poles are closely placed side by side in the direction of rotation, there will be no leakage between them! 3φ.
が形成される。従って後者の場合は有効磁束の減少とな
って回転トルクの減少となる。−男前者の場合は+J+
il洩磁束は減少するが両値」―間に全長にわ/こり望
隙があるため第5図(イ)点線で示すようにアーマチャ
1++llからみた磁束分イ1テ波形にお・いて高)′
+、 67j時には1両者間に急峻な落ち込みが生じ、
滑らかな運転が望めず、出力数ドと共に磁気■の発生、
fAi !+71Jが生じる。因みに上記出力低下は0
.8k wスタータで約5当の出力低下となる。is formed. Therefore, in the latter case, the effective magnetic flux decreases, resulting in a decrease in rotational torque. -If you are a man, +J+
Although the leakage magnetic flux decreases, both values are high in the waveform due to the magnetic flux seen from armature 1++ll as shown by the dotted line in Figure 5 (a) because there is a gap over the entire length between them. ′
+, At 67j, there is a steep drop between the two,
Smooth operation cannot be expected, and the output power decreases and magnetic ■ occurs.
fAi! +71J is generated. By the way, the above output decrease is 0
.. With an 8kW starter, the output will be reduced by about 5 equivalents.
本発明の目的は磁束分布波形がt’+tらかで、回転l
・ルクの向」−する水久磁石式iu流機を提供するに必
る。The object of the present invention is that the magnetic flux distribution waveform is smooth at t'+t, and the rotation l
・It is necessary to provide a water-cooled magnet-type IU flow machine.
本発明は継鉄の内周1141に配置aされ異方性永久磁
石からなる主磁極と、該永久磁イjの減磁作用側に並設
された4iM助磁極とを備えた固ボ子からなる永久磁石
式直1)It、機において、前記隣り合う二つの磁極ケ
夫々(i)l甑の半径方向内側で接し、少なくとも両磁
極のいずれか一方に漏洩磁路a断空隙部を形成したもの
で、漏洩磁束を少なくして回転トルクの向上を図ること
ができる。The present invention is based on a solid bonnet having a main pole made of an anisotropic permanent magnet arranged on the inner circumference 1141 of the yoke, and a 4iM auxiliary pole arranged in parallel on the demagnetizing side of the permanent magnet I. In the permanent magnet type straight machine, the two adjacent magnetic poles (i) are in contact with each other on the radial inner side of the pole, and a leakage magnetic path a-cutting gap is formed in at least one of the two magnetic poles. This makes it possible to reduce leakage magnetic flux and improve rotational torque.
以下本発明の実施例を図面に基づき、1;ト明する。Embodiments of the present invention will be explained below based on the drawings.
第1図は永久磁石式直流を表をスタータに用いた場合で
、電動機部を主体に説明する。図において継鉄1の内周
面1aにtよフエライ系で円弧状の異方性永久磁石2が
等1[11廂に4個配置され、接着剤により固定されて
いる。この永久(1践石C1第2図に示す通り軸心0か
ら扇状に広かつ7迎放射線」二で911j面かり+hJ
7され、磁気反作用による減磁界発生側には鉄心からな
るfili助イ砿極3が配置aされ、前記永久磁石2の
τil 1IIlに−バ1;を密着して両足されている
。4は漏洩磁b16遮1vi梁隙部で、異方性磁石f)
&有の磁石の半径方向中心を更にして補助磁極に漏洩す
る磁束を阻止するために形成されたものでろる。この窒
隙郡は両:M而を放射線上で切断した永久磁石2に、回
転軸の中心Oと永久磁石の回転方向中心を結んだ中心線
と平行に引かれ、磁石の1 / 2 H幅の地点r通る
線分の外l1(11をカントして形成したものである。FIG. 1 shows a case where a permanent magnet type direct current is used as a starter, and the motor section will be mainly explained. In the figure, four circular arc-shaped anisotropic permanent magnets 2 are arranged on the inner circumferential surface 1a of the yoke 1, and are fixed with adhesive. This eternity (1 stone C1 as shown in Figure 2, spread out in a fan-like manner from the axis 0 and 7 rays) 2 = 911j surface + hJ
7, and a fili auxiliary pole 3 made of an iron core is placed on the side where a demagnetizing field is generated due to magnetic reaction. 4 is the leakage magnetic b16 shield 1vi beam gap, anisotropic magnet f)
The radial center of the magnet with & is formed to further prevent magnetic flux from leaking to the auxiliary magnetic pole. This nitrogen gap group is drawn parallel to the center line connecting the center O of the rotating shaft and the center in the rotational direction of the permanent magnet on the permanent magnet 2 which has been cut on the radiation line, and has a width of 1/2 H of the magnet. It is formed by canting the outer l1 (11) of the line segment passing through point r.
すなわち永久磁石2のN、S極の中性点eよ1/211
のJル点にある)こめ、最少限中性点までとれは磁束の
漏洩i/、11MI止され回転トルクも3〜5%アンプ
することができる。In other words, the neutral point e of the N and S poles of the permanent magnet 2 is 1/211
If the magnetic flux is reached to the minimum neutral point (at the J point), the leakage of magnetic flux can be stopped by 11 MI, and the rotational torque can also be increased by 3 to 5%.
一方ポールエンクロージャの関係を第3図を参照して説
明する。上記実施例は所謂4ボ一ル方式で、!する/〔
め、永久Ill布石と補助極3を結合した角度奮θとす
)Lけ
/1
θ1lli1sはおよそ70°(=J近で一般の回転機
と同様である。On the other hand, the relationship between the pole enclosures will be explained with reference to FIG. The above embodiment is a so-called 4-volume system. do/〔
Therefore, the angle θ that combines the permanent Ill and the auxiliary pole 3) is approximately 70° (= near J, which is similar to a general rotating machine).
−に11己ポ゛−ルエンクローンャは大きくなると着磁
(& (D i’Jlli k IMj (!l Rb
t rJ、 増−1−カ、11 iit VCオイテ電
ttQ 子反作用の坂磁界の影2141)を受けやすく
減磁率が高くな〃、性能の向上を図ることができ一11
/″1o このため異方性フェライト磁石でもポールエ
ンクロージャを大さくとることは効果がなく、磁石の使
用献金減少きせ経済的に有利な方向とし、0.7〜0.
8程度である。従ってこの範囲内で有効磁束を増−Pす
には一■二記したように漏洩磁路を遮断することが一番
効果的である。-11 self-pole encloners become magnetized (& (D i'Jlli k IMj (!l Rb
t rJ, increase -1-power, 11 iit VC Oite electric ttQ is susceptible to the shadow of the slope magnetic field of the child reaction (2141), and the demagnetization rate is not high, so performance can be improved.
/''1o For this reason, even with anisotropic ferrite magnets, increasing the size of the pole enclosure is ineffective, and reducing the amount of money spent on magnets is economically advantageous.
It is about 8. Therefore, in order to increase the effective magnetic flux within this range, it is most effective to block the leakage magnetic path as described in Section 1.2.
以上述べたように異方性永久磁石は内径側が841観で
あれば外径側がN極となり、永久磁石の厚さの中心部が
極性の生じない中性点となっている。As described above, if the inner diameter side of the anisotropic permanent magnet is 841 mm, the outer diameter side is the N pole, and the center of the thickness of the permanent magnet is the neutral point where no polarity occurs.
従って第1図および第2図に示す如く主磁束が通る磁気
回路は永久磁石2→市俵子A・→空隙部21→補助磁極
3→継鉄1→永久磁石2と形成され、永久磁石2と前曲
磁極:うが接する側面はできる限り永久磁石2の中性点
以下の部分とし、その先端は電機子との空隙?、より大
きな梁間が生じるように永久イ)8石の外周角部に磁束
の中心を通る放射線と平r1に切断される平行面もしく
けそれ以上に太き′If、空間が生じるような而を設け
て永久イ激石の1IIl1而部からの間伐イ改来全減少
させている。Therefore, as shown in Figs. 1 and 2, the magnetic circuit through which the main magnetic flux passes is formed as follows: permanent magnet 2 -> Ichibarako A -> air gap 21 -> auxiliary magnetic pole 3 -> yoke 1 -> permanent magnet 2. And the forward-curved magnetic pole: The side surface in contact with the back should be as far as possible below the neutral point of permanent magnet 2, and its tip should be in the air gap with the armature. , in order to create a larger gap between the beams, there is a permanent a) parallel plane that is cut by the radiation passing through the center of the magnetic flux and the plane r1 at the outer peripheral corner of the 8 stones, so that a wider space is created. By setting up a permanent stone, thinning from the first part of the stone has been completely reduced.
上1尼空間の切IQ1而が磁束の中心ケ通るhk、射線
と平行であることケよフェライト粉末を型により成形す
る際抜き方向が一定となり生産1(Lに大きく貢献する
。Above 1, the cutting IQ of the space must be parallel to the ray, which passes through the center of the magnetic flux.When molding ferrite powder with a mold, the punching direction is constant and greatly contributes to production 1 (L).
次に本発明品ど従来品を第4図、第5図にて比較して説
明する。Next, the product of the present invention and the conventional product will be compared and explained with reference to FIGS. 4 and 5.
第4図(ロ)は永久(a石2と補助磁極3の内周対向面
を笛着させて外径部に漏洩磁路窒隙部4を形成したもの
で高負荷時の電機子側からみた磁束分布は補助磁極31
11から主磁極2にかけて緩く滑らかにILf1科し限
られた磁極幅内で有効磁束を増やl〜、磁気蒔の発生、
振動にも効果的となっている。Fig. 4 (b) shows a permanent (a-stone 2 and auxiliary magnetic pole 3) whose opposing surfaces on the inner periphery are bonded together to form a leakage magnetic path gap 4 on the outer diameter. The observed magnetic flux distribution is the auxiliary magnetic pole 31
11 to the main magnetic pole 2, the effective magnetic flux is increased within the limited magnetic pole width, and magnetic flux is generated.
It is also effective against vibrations.
一方、45図(11)に示す如く、上d]シ実施例とI
J、逆テーパにして、外周部で突合せることも考えら7
Lるがこの場合C,第51図(インの磁束分布波形(実
線)が示しでいる如くイ巖東が0に近くなる部分が生じ
回転トルク、磁気+4、振動は改善されない。これは空
1!141 Kよって磁極が1托俄子尋体部分に対向し
ない部分が生じるだめである。この磁束のIんち込みe
;j、点線で示しであるように磁1祇間に元金に借間を
形成したものまりtま小さいが好ましいものでi、 f
xい。On the other hand, as shown in Figure 45 (11), the above d] Example and I
J, I am considering making it a reverse taper and butting it at the outer periphery 7
In this case, as shown in Fig. 51 (in magnetic flux distribution waveform (solid line)), there is a part where I becomes close to 0, and rotational torque, magnetic +4, and vibration are not improved. !141 K, there will be a part where the magnetic pole does not oppose the body part.
; j, As shown by the dotted line, the one with a borrowed time on the principal amount is small, but it is preferable, i, f
Yes.
本発明の実施例によれ(ば効果的に漏洩磁路を遮l、I
′r′cきるためJM定されたボ・−ル−Lン′クロー
ンヤのiijΣ四内で永久磁石、 tili助イ角イ3
を最少形状tic L、て有効的に配置道でき1回転ト
ルクも現状の構造体格を維持して5X程度回上させるこ
とができる。又磁束分布が滑らかとなるため磁気「、撮
動が抑えられ騒iの少ないiI!Iカ俵が得られる。According to an embodiment of the present invention (if the leakage magnetic path is effectively blocked, I
In order to cut 'r'c, there is a permanent magnet within the iijΣ4 of the JM defined ball-rule-Ln' clone, tili auxiliary angle A3
With the minimum shape tic L, it can be effectively arranged and the one-turn torque can be increased by about 5X while maintaining the current structure. In addition, since the magnetic flux distribution is smooth, magnetic imaging is suppressed and a bale with less noise can be obtained.
第6図d、本発明の匝の実施例を示すもので、永久磁石
21の接合面G11lは′f+ti助磁悌31と磁石の
先に向けてテーパを除去することによつ−C亀洩磁路遮
バノj空1!/!j43を形成しておル、この罎合も漏
洩イ1荘束を有効に過[Ulできる。FIG. 6d shows an embodiment of the box of the present invention, in which the joint surface G11l of the permanent magnet 21 is formed by removing the taper toward the tip of the magnet with the 'f+ti auxiliary magnet 31. Magnetic path blocker sky 1! /! 43, this combination can also effectively eliminate leakage.
第7図tユ史に他の実施例で、空隙部42を前紡磁極3
2側に設けたもので、この場合磁イ]22の911j端
而は放射i+J5!上にそってリノに1形成さj’L
−C、それと対向する補助磁極側は円状に除去されるが
、軟鉄等の鉄製である/こめj似めて容易に成形するこ
とが出来、接佇面のj陥を自由にコントロールでさる利
点がある。In another embodiment of FIG. 7, the gap 42 is
In this case, the 911j of 22 is radiation i + J5! 1 formed on the lino along the top j'L
-C, the auxiliary magnetic pole side facing it is removed in a circular shape, but it is made of iron such as soft iron./It can be easily shaped to resemble the tangential surface, and the depression of the tangential surface can be freely controlled. There are advantages.
このように副洩磁路避断窒()1丹」、主磁鷺、前曲(
−極のいずれか一力を1.A除することによって形成さ
れるがいず)Lの場合でも同等の効果がノυノ待できる
。In this way, the secondary magnetic leakage path is cut off ()1tan'', the main magnetic heron, and the previous song (
-Put either one of the poles into 1. Although it is formed by dividing A, the same effect can be obtained in the case of L.
第4it目の’−An*例Vま永久磁石23.補助磁極
33のいす!しにも切欠け?i:設けて内径111tl
で突ばせることによって空隙43を形成したもので、こ
の場合も永久磁石側のテーバに金歯て?)1j助磁極を
自由に成形できる利点がある。4th '-An*Example Vma permanent magnet 23. A chair with 33 auxiliary magnetic poles! Even a notch? i: Provided with an inner diameter of 111 tl
The air gap 43 is formed by poking it in with a gold tooth in this case as well. )1j There is an advantage that the auxiliary pole can be formed freely.
以上本発明によれば高負荷時におOる磁束分布波形t(
r’i7らかで1回転トルクの犬さい永久イミ石式直b
1こ(琺が提出でき0゜
図面の囲1iなIIシa明
第1し;I ld: A:冗明の永久イ丑石式直bit
俵を採〕14L/こスタータのIJ!? ’itへel
: Itj[曲図、第2図は第1図にふ゛ける一部11
11而図、第3図は岨イー夏式直bM、 (戊の上ンク
ロージーー・寸θζ図、第4図(イ)(r+)tp本つ
111すJ i′C:I、>ける高負荷時のトシ、餞子
側からみ/こ直東分布図および磁極のIIjl造図、第
5図(イ)(n) fri LE来に」、・りる高負荷
時の市慎子1111からみ7Ll丑東分布1kaおよび
イ市山の<tQ造図、第6図〜第8図は他の実施例にお
りる永久磁石と前曲磁1但の関保を示ず部分1ン;1で
ある。As described above, according to the present invention, the magnetic flux distribution waveform t(
r'i7 Easy and one-turn torque dog-sai permanent imite stone straight b
1 (I can submit 0゜ drawing box 1i II Shea Akira 1st;
Gather bales] 14L/This starter's IJ! ? 'it to el
: Itj [Song chart, Figure 2 is part 11 of Figure 1]
11 diagram, Figure 3 is a summer type direct bM, Toshi of time, viewed from the dumpling side / Direct east distribution map and IIjl construction map of magnetic poles, Figure 5 (a) (n) fri LE coming'', 7Ll Ushito viewed from Ichi Shinko 1111 at high load The distribution 1ka and Iichiyama's <tQ diagrams, FIGS. 6 to 8, do not show the separation between the permanent magnet and the precurved magnet 1 in other embodiments, but the part 1 is 1.
1・・・庸;鉄、2・・・永久磁石(主磁凱)、3・・
・前助磁弔 2 図
寛6 図
17図
麗8図1...Yon; Iron, 2...Permanent magnet (main magnet Gai), 3...
・Maesuke magnetic condolence 2 Zukan 6 Figure 17 Rei 8
Claims (1)
なる主イ1ム極と、該永久慈占の減磁作用側に5A接し
で並設される補助磁極とを備えた固定子からなる永久磁
石式1a流機tこおいて、前記隣り合う二つの磁極は夫
々磁極の半径方向内側で接し、平径方向外側に漏洩磁路
運断窒隙部全形成したことを!Pヶ徴とする永久磁石式
直流機。 2、特許ll1v求の+l+α囲第1項第1項記載て、
前記二つの磁極は回転+111心からの放射線−りで接
していることケ特徴とする永久磁石式直流イ残。 3、l)ゲ♂ト請求の範囲第1項記載において、前記漏
洩磁路a断空隙部は半径方向における両磁極の中心位置
より外イ11すに形成したことを特徴と一ノーる永久磁
石式直流機。 4、 lpy yF請求の範囲第3項記載において、
空隙部Vよ主磁極の外周角部に形成され、その角部の切
断面は主磁極の中心を通る放射線と平行であること全特
徴とする永久磁石式IM流機。[Claims] 1. A main pole made of a four-sided permanent magnet (disposed on the inner circumferential surface of the yoke) and a main pole made of a four-sided permanent magnet are arranged in parallel with 5A contact on the demagnetizing side of the permanent magnet. In this permanent magnet type 1a flow machine consisting of a stator equipped with auxiliary magnetic poles, the two adjacent magnetic poles are in contact with each other on the inside in the radial direction of the magnetic poles, and there is a leakage magnetic path distribution gap on the outside in the radial direction. The whole division has been formed! Permanent magnet type DC machine with P symbol. 2. Paragraph 1 of the +l+α enclosure of the patent ll1v request,
A permanent magnet direct current magnet characterized in that the two magnetic poles are in contact with each other at a radius of 111 degrees of rotation from the center. 3.l) Gate The permanent magnet according to claim 1, characterized in that the leakage magnetic path a-cutting gap is formed at an outer side 11 from the center position of both magnetic poles in the radial direction. Type DC machine. 4. lpy yF Claim 3,
A permanent magnet type IM flow machine characterized in that a gap V is formed at an outer peripheral corner of a main magnetic pole, and a cut surface of the corner is parallel to a radiation passing through the center of the main magnetic pole.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13625982A JPS5928868A (en) | 1982-08-06 | 1982-08-06 | Permanent magnet type dc electric machine |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13625982A JPS5928868A (en) | 1982-08-06 | 1982-08-06 | Permanent magnet type dc electric machine |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5928868A true JPS5928868A (en) | 1984-02-15 |
JPH0423505B2 JPH0423505B2 (en) | 1992-04-22 |
Family
ID=15170997
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13625982A Granted JPS5928868A (en) | 1982-08-06 | 1982-08-06 | Permanent magnet type dc electric machine |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5928868A (en) |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5768655A (en) * | 1980-10-13 | 1982-04-27 | Hitachi Ltd | Permanent magnet field system provided with auxiliary magnetic poles |
-
1982
- 1982-08-06 JP JP13625982A patent/JPS5928868A/en active Granted
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5768655A (en) * | 1980-10-13 | 1982-04-27 | Hitachi Ltd | Permanent magnet field system provided with auxiliary magnetic poles |
Also Published As
Publication number | Publication date |
---|---|
JPH0423505B2 (en) | 1992-04-22 |
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