JPH0510904B2 - - Google Patents

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Publication number
JPH0510904B2
JPH0510904B2 JP63128446A JP12844688A JPH0510904B2 JP H0510904 B2 JPH0510904 B2 JP H0510904B2 JP 63128446 A JP63128446 A JP 63128446A JP 12844688 A JP12844688 A JP 12844688A JP H0510904 B2 JPH0510904 B2 JP H0510904B2
Authority
JP
Japan
Prior art keywords
magnetic flux
core
pole
commutating
short
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.)
Expired - Lifetime
Application number
JP63128446A
Other languages
Japanese (ja)
Other versions
JPH01298937A (en
Inventor
Haruo Oharagi
Kazuo Tawara
Mitsuhiro Nitobe
Nobutaka Suzuki
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.)
Hitachi Setsubi Engineering Co Ltd
Hitachi Ltd
Original Assignee
Hitachi Setsubi Engineering Co Ltd
Hitachi 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 Hitachi Setsubi Engineering Co Ltd, Hitachi Ltd filed Critical Hitachi Setsubi Engineering Co Ltd
Priority to JP12844688A priority Critical patent/JPH01298937A/en
Priority to US07/353,473 priority patent/US5015905A/en
Priority to EP89109533A priority patent/EP0343681B1/en
Priority to DE68917786T priority patent/DE68917786T2/en
Publication of JPH01298937A publication Critical patent/JPH01298937A/en
Publication of JPH0510904B2 publication Critical patent/JPH0510904B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は直流機に係り、特に圧延機などに使用
される大形直流電動機の整流特性を改善するため
の固定子構造に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a DC machine, and more particularly to a stator structure for improving the rectification characteristics of a large DC motor used in a rolling mill or the like.

〔従来の技術〕[Conventional technology]

直流機には古くから回転数の増加に対して無火
花帯位置が減励磁側へ移動する無火花帯の移動現
象があり、この対策として、回転数に対して補極
分路電流を調整する方式や、別電源を用いて補極
磁束を調整する方式等が用いられている。しか
し、これらの方式は直流機本体以外に整流補償装
置を付加する必要があるため高価となる。そこ
で、直流機本体の内部構造をわずかに改造するだ
けで対策し得るものとして特開昭62−71463号公
報に示すものが本発明者らによつて提案されてい
る。
DC machines have long had the phenomenon of non-sparking band movement, where the position of the non-sparking band moves to the de-excited side as the rotational speed increases.As a countermeasure to this, it is necessary to adjust the interpolation shunt current according to the rotational speed. method, and a method of adjusting the interpole magnetic flux using a separate power source. However, these systems are expensive because they require a rectification compensation device to be added in addition to the DC machine main body. Therefore, the inventors of the present invention have proposed a solution shown in Japanese Patent Application Laid-Open No. 62-71463, which can be solved by simply modifying the internal structure of the DC machine body.

この方式を第4図〜第7図について説明する。 This method will be explained with reference to FIGS. 4 to 7.

第4図は直流機の要部展開図である。継鉄1の
内周には主極2と補極3とが設けられている。主
極2は主極鉄心4と磁極片4Aおよび界磁巻線5
とで形成され、固定子12の内部で回転する電機
子6の電機子巻線7に主磁束を与える役目をし、
補極3は補極鉄心8と補極巻線9とから形成さ
れ、電機子巻線7を流れる電流が反転する整流現
象時に整流起電力を発生させるための補極磁束を
与える役目をしている。また、主極2と補極3と
の間には補極鉄心8の電機子6側近傍の側面と磁
極片4Aの側面とを短絡する短絡鉄心10,10
A,10Bが設けられている。
Figure 4 is an exploded view of the main parts of the DC machine. A main pole 2 and a complementary pole 3 are provided on the inner periphery of the yoke 1. The main pole 2 includes a main pole iron core 4, a magnetic pole piece 4A, and a field winding 5.
It serves to provide main magnetic flux to the armature winding 7 of the armature 6 rotating inside the stator 12,
The commutator 3 is formed from a commutator iron core 8 and a commutator winding 9, and serves to provide a commutator magnetic flux to generate a rectified electromotive force during a rectification phenomenon in which the current flowing through the armature winding 7 is reversed. There is. Further, between the main pole 2 and the commutator pole 3, there are short-circuit cores 10, 10 that short-circuit the side surface of the commutator core 8 near the armature 6 side and the side surface of the magnetic pole piece 4A.
A and 10B are provided.

このような構成の直流機における低速運転時お
よび高速運転時の動作を第5図イ,ロに示す。こ
れらの図において、φMP,φMP1,φMP2は主磁束、
φIP,φIP1〜φIP3は補極磁束、φIA,φIA1,φIA2

流補償用補極磁束である。同図イの低速運転時で
は強め界磁であるため主磁束φMP1が大となり、主
極鉄心4と継鉄1との磁束密度が高く、磁気的に
飽和した状態となるので、短絡鉄心10Bを通し
て洩れる漏洩補極磁束はφIP1のみとなり、残りの
φIP2,φIP3は電機子6側へ入射して整流起電力を
発生するための整流補償用補極磁束φIA1となる。
The operation of a DC machine with such a configuration during low-speed operation and high-speed operation is shown in FIGS. 5A and 5B. In these figures, φ MP , φ MP1 , φ MP2 are the main magnetic flux,
φ IP , φ IP1 to φ IP3 are interpolation magnetic fluxes, and φ IA , φ IA1 , φ IA2 are commutating magnetic fluxes for rectification compensation. During low-speed operation in Figure A, the main magnetic flux φ MP1 increases due to the strong field, and the magnetic flux density between the main pole iron core 4 and the yoke 1 is high, resulting in a magnetically saturated state. The leakage commutating magnetic flux leaking through is only φ IP1 , and the remaining φ IP2 and φ IP3 become commutating compensating magnetic flux φ IA1 for entering the armature 6 side and generating a rectifying electromotive force.

また、同図ロの高速運転時では弱め界磁である
から、主磁束φMP2が小となり、主極鉄心4と継鉄
1との磁束密度が低く、磁気的に飽和していない
状態となるので、短絡鉄心10Bを介して補極磁
束φIPが主極鉄心4へ漏れ易くなり、補極磁束
φIP1,φIP2が主極鉄心4への漏洩補極磁束となり、
補極磁束φIP3が電機子6へ入射して整流補償用補
極磁束φIA2となる。このように電機子6へ入射す
る整流補償用補極磁束量が高速運転時には低速運
転時より小さくなるので、無火花帯の移動現像を
防止することができる。
In addition, during high-speed operation in Figure B, the field is weakened, so the main magnetic flux φ MP2 is small, and the magnetic flux density between the main pole iron core 4 and the yoke 1 is low, resulting in a state where it is not magnetically saturated. Therefore, the commutating magnetic flux φ IP tends to leak to the main pole iron core 4 via the short-circuited iron core 10B, and the commutating magnetic fluxes φ IP1 and φ IP2 become the leaking commutating magnetic flux to the main pole iron core 4,
The commutating magnetic flux φ IP3 enters the armature 6 and becomes the commutating magnetic flux φ IA2 for commutation compensation. In this manner, the amount of commutating magnetic flux for rectification compensation incident on the armature 6 is smaller during high-speed operation than during low-speed operation, so that movement and development of the non-spark zone can be prevented.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかし、上記従来技術では上記短絡鉄心として
具体的にどのような磁性材料を使用するかについ
てまでは配慮されておらず、例えばこの種直流機
の鉄心材料として通常良く使用される積層鉄板を
上記短絡鉄心として使用した場合には、過渡運転
時における負荷電流の急変時にブラシから火花を
発生するという問題があることが判明した。この
ようなことは正逆回転、力行、回生制動運転を行
なう、いわゆる4象限運転される直流機に適用し
た場合、負荷電流の急変が頻繁に起こるので特に
問題となる。
However, in the above-mentioned conventional technology, no consideration is given to what kind of magnetic material to use as the short-circuiting iron core. When used as an iron core, it was found that there was a problem in that sparks were generated from the brushes when the load current suddenly changed during transient operation. This is particularly problematic when applied to a so-called four-quadrant DC machine that performs forward/reverse rotation, power running, and regenerative braking operation, since sudden changes in load current occur frequently.

本発明の目的は、上記従来技術の課題を解決
し、直流機本体の内部構造を改造するだけで無火
花帯移動現象を防止し、いかなる運転状態におい
てもブラシからの火花発生を防止することができ
る直流機を提供するにある。
The purpose of the present invention is to solve the above-mentioned problems of the prior art, to prevent the no-spark band movement phenomenon by simply modifying the internal structure of the DC machine body, and to prevent the generation of sparks from the brush in any operating condition. We are able to provide DC machines that can.

〔課題を解決するための手段〕[Means to solve the problem]

上記の目的を達成するため、本発明は、短絡鉄
心を経由する漏洩補極磁束の流通路の少なくとも
一部に漏洩補極磁束の急激な変化によつてうず電
流を発生する磁束変化抑制部材を設けたことを特
徴とする。
In order to achieve the above object, the present invention includes a magnetic flux change suppressing member that generates an eddy current due to a sudden change in the leakage magnetic flux of the magnetic flux in at least a part of the flow path of the leakage magnetic flux of the magnetic flux that passes through the short-circuited core. It is characterized by having been established.

〔作用〕[Effect]

短絡鉄心を経由する漏洩補極磁束の流通路に設
けられた磁束変化抑制部材は、負荷電流の急激な
変化に対して漏洩補極磁束の変化を抑制するよう
にうず電流を発生し、それによつて、負荷電流の
急変時に良好な整流状態を得るための補極磁束を
確保することができるので、ブラシからの火花発
生を防止することができる。
The magnetic flux change suppressing member provided in the flow path of the leakage magnetic flux of the magnetic pole via the short-circuited core generates an eddy current so as to suppress the change of the leakage magnetic flux of the magnetic pole in response to a sudden change in the load current. Therefore, it is possible to secure the interpolation magnetic flux for obtaining a good rectification state when the load current suddenly changes, and therefore it is possible to prevent the generation of sparks from the brush.

〔実施例〕〔Example〕

本発明の実施例を説明するのに先立つて、従来
装置において負荷電流の急変時にブラシから火花
が発生する理由についての本発明者等の究明結果
を、第6図イ〜ハおよび第7図を用いて簡単に説
明する。
Prior to explaining the embodiments of the present invention, the results of the investigation by the present inventors regarding the reason why sparks are generated from the brush in the conventional device when the load current suddenly changes are shown in Figs. 6A to 7C. This will be briefly explained using

第6図イは時間を横軸にとり、縦軸に負荷電流
の変化を示す特性図である。4象限運転される直
流機などにおいては、負荷電流が急増し、定常時
を経て急減する(負方向の電流変化は図示せず)。
同図ロは負荷電流の急増時における低速運転時の
動作を示す直流機の要部展開図である。同図に示
す低速運転時においては、強め界磁であるため主
磁束φMP1が大となり、補極磁束φIPのうち従来と
同様にφIP1が短絡鉄心10Bを通して主極鉄心4
へ洩れ、漏洩補極磁束となる。同図ハは電機子反
作用起磁力を示した特性図で、補極中心で最大と
なる。このため、同図ロにおいて、負荷電流の急
増時における補極磁束φIP3は、補極空隙長が主極
空隙長より大きいこと、電機子反作用起磁力が補
極に対して強く作用することから、補極鉄心8よ
り直接電機子6へ入射して整流補償用補極磁束と
なりにくく、短絡鉄心10Aを通して主極鉄心4
へ漏れ、漏洩補極磁束となる。この結果、電機子
6側へ入射して整流起電力を発生させるための補
極磁束はφIP2のみとなり、整流補償用補極磁束
φIA1が小さくなる。
FIG. 6A is a characteristic diagram in which time is plotted on the horizontal axis and changes in load current are plotted on the vertical axis. In a DC machine operated in four quadrants, the load current rapidly increases, reaches a steady state, and then rapidly decreases (current changes in the negative direction are not shown).
Figure B is an exploded view of the main parts of the DC machine, showing the operation during low-speed operation when the load current increases rapidly. During low-speed operation shown in the figure, the main magnetic flux φ MP1 is large due to the strong field, and φ IP1 of the interpole magnetic flux φ IP passes through the short-circuited iron core 10B to the main pole iron 4 as in the conventional case.
leakage to the magnetic flux, resulting in leakage commutating magnetic flux. Figure C is a characteristic diagram showing the armature reaction magnetomotive force, which is maximum at the center of the commutating pole. Therefore, in Figure B, the commutating magnetic flux φ IP3 at the time of a sudden increase in the load current is due to the fact that the commutating pole air gap length is larger than the main pole air gap length and that the armature reaction magnetomotive force acts strongly on the commutating pole. , it is difficult to directly enter the armature 6 from the commutator core 8 and become a commutator magnetic flux for rectification compensation, and the main pole core 4 passes through the short-circuit core 10A.
leaks to the magnetic flux, resulting in leakage commutating magnetic flux. As a result, the commutating magnetic flux that enters the armature 6 side to generate a rectified electromotive force becomes only φ IP2 , and the commutating compensating magnetic flux φ IA1 becomes small.

第7図は横軸に負荷電流をとり、縦軸に整流補
償用補極磁束φIAを示した特性図で、定常運転時
に対して過渡運転時(負荷電流の急変時)の整流
補償用補極磁束が減少する。このことは負荷電流
の急減時および高速運転時にも同様のことが言え
る。これより、過渡運転時においては負荷電流の
変化に対して漏洩補極磁束が増加し、整流補償用
補極磁束が減少し、ブラシから火花を発生する問
題が生ずることが判明した。
Figure 7 is a characteristic diagram showing the load current on the horizontal axis and the commutating pole magnetic flux φ IA for rectification compensation on the vertical axis. Polar magnetic flux decreases. The same holds true when the load current suddenly decreases and during high-speed operation. From this, it has been found that during transient operation, leakage commutating magnetic flux increases in response to changes in load current, commutating compensating commutating flux decreases, and a problem occurs in which sparks are generated from the brush.

ここで、本発明を第1図イ,ロ〜第3図に示す
実施例に基づいて説明する。第1図イ,ロは本発
明の一実施例に係る直流機の要部展開図および短
絡鉄心部分の一部斜視図である。各図で、従来の
ものと同一又は等価の部分には同じ符号を付して
説明を省略する。補極鉄心8の電機子6側近傍の
側面に積層鉄板13からなる短絡鉄心10,10
A,10Bが設けられ、この短絡鉄心10の主極
鉄心4側の側面に塊状鉄心14からなる磁束変化
抑制部材11,11A,11Bが設けられてい
る。同図ロに示すように、磁束変化抑制部材11
Bは矢印の方向に漏洩補極磁束φIP1が変化しよう
とすると、それを抑制する方向にうず電流icを発
生する。
The present invention will now be described based on the embodiments shown in FIGS. 1A and 3B. FIGS. 1A and 1B are an exploded view of main parts and a partial perspective view of a short-circuit core portion of a DC machine according to an embodiment of the present invention. In each figure, parts that are the same or equivalent to those of the conventional one are given the same reference numerals, and explanations thereof will be omitted. Short-circuit cores 10, 10 made of laminated iron plates 13 are installed on the side surface of the commutating pole core 8 near the armature 6 side.
A, 10B are provided, and magnetic flux change suppressing members 11, 11A, 11B made of a block iron core 14 are provided on the side surface of the short-circuited iron core 10 on the main pole iron core 4 side. As shown in FIG.
B generates an eddy current IC in the direction of suppressing the change in the leakage interpolation magnetic flux φ IP1 in the direction of the arrow.

このような構成で、第2図イに示すように負荷
電流が急増すると、主極磁束φMP、補極磁束φIP
低速運転時には同図ロのように、また高速運転時
には同図ハのようにそれぞれ作用する。すなわ
ち、低速運転時には強め界磁であるため主磁束
φMP1が大となり、主極鉄心4と継鉄1との磁束密
度が高く、磁気的に飽和した状態となつているの
で、短絡鉄心10Bを通して洩れる漏洩補極磁束
は従来と同様にφPI1のみとなる。一方、負荷電流
の急増に伴つて急増し短絡鉄心10Aを通して主
極鉄心4へ洩れようとする漏洩補極磁束は磁束変
化抑制部材11Aに発生するうず電流によつて抑
制されるので、漏洩補極磁束φIP1以外の補極磁束
φIP2,φIP3は電機子6側へ入射して整流起電力を
発生させるための整流補償用補極磁束φIA1とな
る。
With this configuration, when the load current increases rapidly as shown in Figure 2 A, the main pole magnetic flux φ MP and the interpolation magnetic flux φ IP change as shown in Figure 2 B during low-speed operation, and as shown in Figure 2 C during high-speed operation. Each works as follows. That is, during low-speed operation, the main magnetic flux φ MP1 becomes large due to the strong field, and the magnetic flux density between the main pole iron core 4 and the yoke 1 is high and magnetically saturated, so that the magnetic flux is The leakage commutator magnetic flux is only φ PI1 as in the conventional case. On the other hand, the leakage commutator magnetic flux that increases rapidly with the sudden increase in load current and tries to leak to the main pole core 4 through the short-circuit core 10A is suppressed by the eddy current generated in the magnetic flux change suppressing member 11A, so the leakage commutator flux The commutating magnetic fluxes φ IP2 and φ IP3 other than the magnetic flux φ IP1 become the commutating magnetic flux φ IA1 for commutation compensation which is incident on the armature 6 side and generates a rectifying electromotive force.

また、高速運転時には弱め界磁であるから主磁
束φMP2が小となり、主極鉄心4と継鉄1との磁束
密度が低く、磁気的に飽和していない状態となつ
ているので、短絡鉄心10Bを通して洩れる漏洩
補極磁束は従来と同様にφIP1,φIP2となる。一方、
負荷電流の急増に伴つて急増し短絡鉄心10Aを
通して主極鉄心4へ洩れようとする漏洩補極磁束
は磁束変化抑制部材11Aに発生するうず電流に
よつて抑制されるので、漏洩補極磁束φIP1,φIP2
を除く残りの補極磁束φIP3が電機子6側へ入射し
て整流補償用補極磁束φIA2となる。
In addition, during high-speed operation, the field is weakened, so the main magnetic flux φ MP2 becomes small, and the magnetic flux density between the main pole iron core 4 and the yoke 1 is low and is not magnetically saturated, so the short-circuited iron core The leakage interpolation magnetic fluxes leaking through 10B are φ IP1 and φ IP2 as in the conventional case. on the other hand,
The leakage commutator magnetic flux that increases rapidly as the load current increases and tries to leak to the main pole core 4 through the short-circuit core 10A is suppressed by the eddy current generated in the magnetic flux change suppressing member 11A, so that the leakage commutator flux φ IP1IP2
The remaining commutating magnetic flux φ IP3 excluding the commutating magnetic flux φ IP3 enters the armature 6 side and becomes commutating magnetic flux φ IA2 for commutation compensation.

このようにして電機子6側へ入射する磁束量が
高速運転時には低速運転時より小さくなるので、
直流機本体のみで無火花帯の移動現象が防止でき
る。また、塊状鉄心11は負荷電流の急激な変化
に対してうず電流を発生し、漏洩補極磁束の変化
を抑制するので、負荷電流の急変時においても充
分な整流補償用補極磁束を確保できる。
In this way, the amount of magnetic flux incident on the armature 6 side becomes smaller during high-speed operation than during low-speed operation, so
The movement of the no-spark zone can be prevented only by using the DC machine itself. In addition, the block iron core 11 generates eddy current in response to sudden changes in load current and suppresses changes in leakage commutating magnetic flux, so that sufficient commutating flux for commutation compensation can be ensured even when load current suddenly changes. .

第3図は負荷電流を横軸にとり、縦軸に定常運
転時と過渡運転時の整流補償用補極磁束φIAを示
す特性図である。同図から明らかなように、負荷
電流が急変する過渡運転時における整流補償用補
極磁束を定常運転時とほぼ同様に得られることか
ら、過渡運転時におけるブラシの火花発生を防止
できる効果がある。
FIG. 3 is a characteristic diagram showing the load current on the horizontal axis and the commutating pole magnetic flux φ IA for commutation compensation during steady operation and transient operation on the vertical axis. As is clear from the figure, commutating magnetic flux for rectification compensation during transient operation when the load current changes suddenly can be obtained almost in the same way as during steady operation, which is effective in preventing brush sparks during transient operation. .

なお、上記実施例では、短絡鉄心10として積
層鉄心13を用い、その主極鉄心4側の側面に塊
状鉄心14からなる磁束変化抑制部材11を設け
た例について説明したが、磁束変化抑制部材11
を短絡鉄心10の補極鉄心8側の側面に設けた
り、短絡鉄心10として塊状鉄心を用い、これを
磁束変化抑制部材11の塊状鉄心として兼用した
り、あるいは磁束変化抑制部材11として、塊状
鉄心14を設ける代りに、積層鉄板13からなる
短絡鉄心10の一部にその鉄板間を短絡する短絡
層を設けても同様の効果が得られる。
In the above embodiment, an example was described in which the laminated core 13 is used as the short-circuit core 10 and the magnetic flux change suppressing member 11 made of the lumpy core 14 is provided on the side surface of the laminated core 13 on the side of the main pole core 4. However, the magnetic flux change suppressing member 11
is provided on the side surface of the short-circuit core 10 on the side of the commutating pole core 8, or a block core is used as the short-circuit core 10, and this is also used as the block core of the magnetic flux change suppressing member 11, or a block core is used as the magnetic flux change suppressing member 11. 14, a similar effect can be obtained by providing a short-circuiting layer that short-circuits between the iron plates in a part of the short-circuiting iron core 10 made of the laminated iron plates 13.

〔発明の効果〕〔Effect of the invention〕

以上述べたように、本発明によれば、短絡鉄心
を経由する漏洩補極磁束の流通路の少なくとも一
部に漏洩補極磁束の急変によつてうず電流を発生
する磁束変化抑制部材を設けたので、この部材に
発生するうず電流により負荷電流の急変に対して
漏洩補極磁束の変化を抑制し必要とする整流補償
用補極磁束を確保することができ、過渡運転時に
おけるブラシからの火花発生を防止することがで
きる。
As described above, according to the present invention, a magnetic flux change suppressing member that generates an eddy current due to a sudden change in the leakage magnetic flux of the magnetic flux is provided in at least a part of the flow path of the leakage magnetic flux of the magnetic flux that passes through the short-circuited core. Therefore, the eddy current generated in this member can suppress changes in the leakage commutator magnetic flux in response to sudden changes in load current, secure the necessary commutator compensator flux, and prevent sparks from the brush during transient operation. Occurrence can be prevented.

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

第1図イ,ロは本発明の一実施例に係る直流機
の要部展開図および短絡鉄心部分の斜視図、第2
図イは負荷電流の特性図、第2図ロ,ハは第1図
イに示した直流機の低速運転時および高速運転時
の動作説明図、第3図は第1図イに示した直流機
の負荷電流と補極磁束の関係を示す特性図、第4
図は従来の直流機の要部展開図、第5図イ,ロは
第4図に示した直流機の低速運転時および高速運
転時の動作説明図、第6図イは運転時の負荷電流
の特性図、第6図ロは第4図に示した直流機の負
荷電流急変時における動作説明図、第6図ハは電
機子反作用起磁力の特性図、第7図は従来の直流
機における負荷電流と補極磁束の関係を示す特性
図である。 1……継鉄、2……主極、3……補極、4……
主極鉄心、5……界磁巻線、6……電機子、7…
…電機子巻線、8……補極鉄心、9……補極巻
線、10……短絡鉄心、11……塊状鉄心。
Figures 1A and 1B are an exploded view of main parts and a perspective view of a short-circuit core part of a DC machine according to an embodiment of the present invention,
Figure A is a characteristic diagram of the load current, Figure 2 B and C are explanatory diagrams of the operation of the DC machine shown in Figure 1 A during low-speed operation and high-speed operation, and Figure 3 is the DC current shown in Figure 1 A. Characteristic diagram showing the relationship between machine load current and interpolation magnetic flux, No. 4
The figure is an exploded view of the main parts of a conventional DC machine, Figure 5 A and B are explanatory diagrams of the operation of the DC machine shown in Figure 4 during low-speed operation and high-speed operation, and Figure 6 A is the load current during operation. Figure 6 (b) is an explanatory diagram of the operation of the DC machine shown in Figure 4 when the load current suddenly changes, Figure 6 (c) is a characteristic diagram of the armature reaction magnetomotive force, and Figure 7 is a diagram of the operation of the DC machine shown in Figure 4. FIG. 3 is a characteristic diagram showing the relationship between load current and interpolation magnetic flux. 1... Yoke, 2... Main pole, 3... Complementary pole, 4...
Main pole iron core, 5... Field winding, 6... Armature, 7...
...Armature winding, 8...Commuting pole core, 9...Commuting pole winding, 10...Short circuit core, 11...Lump core.

Claims (1)

【特許請求の範囲】 1 電機子6と、固定子12とを備えた直流機で
あつて、 電機子6は、電機子巻線7を備えて、固定子1
2内で回転するものであり、 固定子12は、継鉄1と、複数の主極2と、複
数の補極3と、短絡鉄心10と、磁束変化抑制部
材11とを備えたものであり、 主極2は、主極鉄心4と、界磁巻線5とを備え
て、継鉄1の内周側に取付けられたものであり、 補極3は、補極鉄心8と、補極巻線9とを備え
て、主極2間の継鉄1の内周側に取付けられたも
のであり、 短絡鉄心10は、主極鉄心4と補極鉄心8との
間で界磁巻線5および補極巻線9より電機子6側
に片寄つた位置においてほぼ周方向に延在して設
けられて、漏洩補極磁束を流通させるものであ
り、 磁束変化抑制部材11は、短絡鉄心10を経由
する漏洩補極磁束の流通路の少なくとも一部に設
けられて、漏洩補極磁束の急激な変化によりうず
電流を発生してこの漏洩補極磁束の急激な変化を
抑制するものである 直流機。 2 短絡鉄心10は、積層鉄板13で構成された
ものであり、 磁束変化抑制部材11は、塊状鉄心14で構成
されたものである 特許請求の範囲第1項に記載の直流機。 3 短絡鉄心10は、塊状鉄心で構成されて、磁
束変化抑制部材11を兼用しているものである 特許請求の範囲第1項に記載の直流機。
[Claims] 1. A DC machine including an armature 6 and a stator 12, wherein the armature 6 is provided with an armature winding 7, and the stator 1 is provided with an armature winding 7.
The stator 12 includes a yoke 1, a plurality of main poles 2, a plurality of commutating poles 3, a short-circuit core 10, and a magnetic flux change suppressing member 11. The main pole 2 includes a main pole iron core 4 and a field winding 5, and is attached to the inner peripheral side of the yoke 1, and the commutating pole 3 includes a commutating pole iron core 8 and a commutating pole. The short-circuit core 10 is provided with a field winding between the main pole core 4 and the commutating pole core 8. 5 and the commutator winding 9 toward the armature 6 side, extending substantially in the circumferential direction to allow leakage commutator magnetic flux to flow. A direct current is provided in at least a part of the flow path of the leakage magnetic flux of the leakage magnetic pole, and generates an eddy current due to a sudden change in the magnetic flux of the leakage magnetic pole, thereby suppressing a sudden change in the magnetic flux of the leakage magnetic pole. Machine. 2. The DC machine according to claim 1, wherein the short-circuit core 10 is composed of a laminated iron plate 13, and the magnetic flux change suppressing member 11 is composed of a block core 14. 3. The DC machine according to claim 1, wherein the short-circuit core 10 is made of a block core and also serves as the magnetic flux change suppressing member 11.
JP12844688A 1988-05-27 1988-05-27 Stator for dc electric machine Granted JPH01298937A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP12844688A JPH01298937A (en) 1988-05-27 1988-05-27 Stator for dc electric machine
US07/353,473 US5015905A (en) 1988-05-27 1989-05-17 DC dynamoelectric machine with interpoles having magnetic flux bypassing members
EP89109533A EP0343681B1 (en) 1988-05-27 1989-05-26 Dynamoelectric DC machine
DE68917786T DE68917786T2 (en) 1988-05-27 1989-05-26 Dynamoelectric DC machine.

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12844688A JPH01298937A (en) 1988-05-27 1988-05-27 Stator for dc electric machine

Publications (2)

Publication Number Publication Date
JPH01298937A JPH01298937A (en) 1989-12-01
JPH0510904B2 true JPH0510904B2 (en) 1993-02-12

Family

ID=14984920

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12844688A Granted JPH01298937A (en) 1988-05-27 1988-05-27 Stator for dc electric machine

Country Status (1)

Country Link
JP (1) JPH01298937A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102237734B (en) * 2010-04-23 2015-08-12 德昌电机(深圳)有限公司 A kind of motor

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5138604U (en) * 1974-09-18 1976-03-23
JPS61202171U (en) * 1985-06-05 1986-12-18
JPS6271463A (en) * 1985-09-25 1987-04-02 Hitachi Ltd dc machine

Also Published As

Publication number Publication date
JPH01298937A (en) 1989-12-01

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