JPS59180118A - Magnetic thrust bearing - Google Patents

Magnetic thrust bearing

Info

Publication number
JPS59180118A
JPS59180118A JP5571683A JP5571683A JPS59180118A JP S59180118 A JPS59180118 A JP S59180118A JP 5571683 A JP5571683 A JP 5571683A JP 5571683 A JP5571683 A JP 5571683A JP S59180118 A JPS59180118 A JP S59180118A
Authority
JP
Japan
Prior art keywords
iron core
thrust bearing
rotating part
magnetic thrust
electric machine
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
JP5571683A
Other languages
Japanese (ja)
Inventor
Toshio Inoue
俊夫 井上
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric Co Ltd
Fuji Electric Manufacturing Co 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 Fuji Electric Co Ltd, Fuji Electric Manufacturing Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP5571683A priority Critical patent/JPS59180118A/en
Publication of JPS59180118A publication Critical patent/JPS59180118A/en
Pending legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16CSHAFTS; FLEXIBLE SHAFTS; ELEMENTS OR CRANKSHAFT MECHANISMS; ROTARY BODIES OTHER THAN GEARING ELEMENTS; BEARINGS
    • F16C32/00Bearings not otherwise provided for
    • F16C32/04Bearings not otherwise provided for using magnetic or electric supporting means
    • F16C32/0406Magnetic bearings
    • F16C32/044Active magnetic bearings

Abstract

PURPOSE:To prevent damage to a rotary part by putting in the lower side a fixation part iron core of a thrust bearing joined to the stator side and putting in the upper side, in opposition to said iron core, a rotary part iron core of a magnetic thrust bearing joined to the rotor side and further providing an exciting coil on the plane of opposition of both cores. CONSTITUTION:A rotary part iron core 7 of a magnetic thrust bearing 1 joined to a rotor 3 side and a fixation part iron core 4 of a magnetic thrust bearing 1 joined to a stator 2 side are arranged in opposition to each other through a gap 8 with the rotary part iron core 7 in the upper side. Said iron core 7 and 4 are respectively provided with an exciting coil 5 and 6 same in the number of coiling. The coils are connected so as to make series with each other and also excited so as to generate magnetomotive force by means of the same current and in the direction reverse to each other. When the rotor 3 moves up and down due to change of load operating on it, change of the lifting force 10 of the magnetic thrust bearing due to change of the gap 8, corresponding to said change of load, operates to absorb a change of load.

Description

【発明の詳細な説明】 〔発1!、fの属引る技術分野〕 本発明はその回転部が電気機械の回転子側にその固定部
が電気機械の固定子側ζこ結合され前記回転部と固定部
とが適宜のギャップを介して相互ζこ対向する如く配置
されるとともζこ、相互の間ζこ働らく磁気力により回
転子をつり上げる如く作j4E −4−る室軸形電気機
械の磁気スラスト:tl+受に関する。
[Detailed description of the invention] [Voice 1! , f technical field] The present invention provides a method in which the rotating part is connected to the rotor side of an electric machine, and the fixed part is connected to the stator side of the electric machine, and the rotating part and the fixed part are connected through an appropriate gap. The present invention relates to a magnetic thrust (tl+) bearing for a chamber-shaft type electric machine in which the rotor is lifted up by the magnetic force acting between the shafts and the rotor when the shafts are arranged so as to face each other.

この1重の磁気スラスト軸受は回転子に作用するスラス
ト荷重が回転子の重量と同方向に増大した場合これに追
随して前記磁気力が増大し、したん5つて前記回転子を
つリートげる力も増大するよう番こなることか望まれる
In this single magnetic thrust bearing, when the thrust load acting on the rotor increases in the same direction as the weight of the rotor, the magnetic force increases accordingly, and the rotor is immediately removed. It is hoped that this will be done in such a way that the power of

〔従来技術とその問題点〕[Prior art and its problems]

一般にこの種の磁気スラスト軸受は′fイ気機械の始動
時の静止摩擦トルク並びに定常運転時の・i#l+受損
失全損失し円滑な始動と運転効率の向上船こ寄−辱りL するとともに、lt 線機械のスラスト軸受の小形イヒ
と信頼性の向上をもたらすことは良く知られてl/)る
In general, this type of magnetic thrust bearing reduces the static friction torque at the time of machine startup and the total loss during steady operation, resulting in smooth startup and improved operating efficiency. In addition, it is well known that the thrust bearings of LT line machines can be made smaller and their reliability can be improved.

従来の磁気スラスト軸受は第1図に示す」く、磁気スラ
スト軸受1の回転部鉄心7が適宜のギャップ8を介して
固定部鉄心4の下側に位置し力)つ相互の間に働らく磁
気力を生ずる励磁コイル5が固定部鉄心4のギャップ8
側にのみ設けられ−CI、)る0今励磁コイル5に図示
の4j性の方向に励磁電流6をIiえると前記軸受】の
固定部鉄心4.ギャップ8.1Qび(こ回転部鉄心7を
周囲する[ス示の矢印の方向に磁束9が生じ、固定部鉄
心4と回転部鉄心7吉の間に生ずる磁気吸引力により回
転部鉄心7したがって電気機械の回転子3を含む回転部
が(l]定部鉄心4に向って上方につり上げられる。こ
の場合回r減部(こ1動らくつり−[げ力10はギャッ
プ8の陽さζこ対して第2図に示す如き特性を有してい
る。即(ら励磁電流6をパラメータとしてスラスト荷屯
11が下方に向って増大するとギャップ8が広がって磁
気吸引力したがってつり上げ力10が減少し、逆にスラ
スト荷電が上に向って働らくとギャップ8が短、縮して
吸引力したがってつり上げ力10が増大する。通常の室
軸1a、気機械例えば水屯発1d機の場合(こは水車を
含む発2に機の回転部の総重量の相当部分を磁気スラス
) 4M+受1が荷担し、残余の取囲をンζラスト軸受
(図示せず)が荷担する如くに磁気スラスト荷電1の励
磁電流6を調整して運転を行ない、発電機回転部に著し
い逆スラスト力が勧らかない限り安定した運転を期待す
ることができる。しかしイ1」らかの理由で’A t 
48回転部ζこ大きな逆スラストが作用すると該回転部
が上方に持ち上げられるが、磁気スラスト・IQII受
1の固定部鉄心4と回転部鉄心7との間に働らくつり上
げ力10は第2図に示4− Do < 、ギ−へ・ツブ
8が短縮すればする程増大する特性を有しているから、
終には発電機回転部が浮き上り、発電機ζこ設i−tら
れる逆スラスト軸受(図示せず)に過大の負荷が作用し
てこれを損傷する虞れを生ずる。しかし従来の磁気スラ
スト軸受の構成ではこれを防1F−rることかできない
In a conventional magnetic thrust bearing, as shown in FIG. 1, the rotating part iron core 7 of the magnetic thrust bearing 1 is located below the fixed part iron core 4 through a suitable gap 8, so that no force acts between them. The excitation coil 5 that generates magnetic force is connected to the gap 8 of the fixed part iron core 4.
When an excitation current 6 is applied to the excitation coil 5 provided only on the side -CI,), the excitation current 6 is applied to the excitation coil 5 in the direction of the 4j direction shown in the drawing, and the fixed part iron core 4. Magnetic flux 9 is generated in the direction of the arrow shown in the gap 8.1Q (around the rotating part iron core 7), and the magnetic attraction force generated between the fixed part iron core 4 and the rotating part iron core 7 causes the rotating part iron core 7 to The rotating part including the rotor 3 of the electric machine is lifted upwards toward the fixed part iron core 4. In this case, the rotating part (the lifting force 10 is equal to On the other hand, it has the characteristics as shown in Fig. 2.When the thrust load 11 increases downward using the excitation current 6 as a parameter, the gap 8 widens and the magnetic attraction force and therefore the lifting force 10 decreases. On the other hand, when the thrust charge acts upward, the gap 8 is shortened and the suction force and thus the lifting force 10 increases. A considerable portion of the total weight of the rotating parts of the machine is charged to the generator 2, including the water wheel, by magnetic thrust) 4M + bearing 1 carries the load, and the remaining surroundings are carried by the Nζ last bearing (not shown). By adjusting the excitation current 6 of 1, stable operation can be expected as long as a significant reverse thrust force is not induced in the rotating part of the generator.However, for some reason, 'A t
48 Rotating part ζ When a large reverse thrust acts on the rotating part, the rotating part is lifted upward, but the lifting force 10 acting between the fixed part iron core 4 and the rotating part iron core 7 of the magnetic thrust/IQII receiver 1 is as shown in Fig. 2. As shown in 4-Do < , since it has the characteristic that it increases as the gear tube 8 becomes shorter,
Eventually, the rotating part of the generator will float up, and an excessive load will be applied to the reverse thrust bearing (not shown) installed in the generator, creating the risk of damaging it. However, the configuration of conventional magnetic thrust bearings can only prevent this from occurring.

〔発明の目的〕[Purpose of the invention]

本発明は従来の磁気スラスト軸受の有する前記の如き欠
点に鑑み、電気機械の回転部に著しい逆スラスト力が作
用した場合ζこ、磁気スラスト・(((1受の固定部鉄
心と回転部鉄心光の間に生ずるつり上げ力が前記逆スラ
スト力を吸収して安定した電気機械・])運転を維持す
ることができ、しかも構成の?+1′I単な磁気スラス
ト軸受を提供することを目的と4−る。
In view of the above-mentioned drawbacks of conventional magnetic thrust bearings, the present invention has been developed to prevent magnetic thrust bearings from occurring when a significant reverse thrust force is applied to the rotating part of an electric machine. The purpose of the present invention is to provide a simple magnetic thrust bearing that can maintain stable electric machine operation by absorbing the reverse thrust force caused by the lifting force generated between the light beams. 4-ru.

〔発明の交点〕[Intersection of inventions]

前記の目的を達成するために本発明では首記の磁気スラ
スト・ill受において、前記電気機械の固定子側に結
合される前記スラスト軸受の固定部鉄心を下側に、前記
′電気機械の回転子側に結合される・iil記磁気スラ
スト軸受の回転部鉄心を上側に適当なギャップを介して
相互に対向させかつ両者の対向する面にそれぞれ同一巻
回数の励磁コイルを設けるとともk、それぞれの励磁コ
イルが生ずる起磁力が相?ilこ逆方向ζこなる如く直
列に励磁することζこより、磁気スラスト軸受の固定部
鉄心と回転部鉄心とのギャップを介して相互に対面する
部分が磁気的(・こ同一極性となって相互反撥力を生じ
、該反撥力ζこより[旬記電気機械の回転部をつり上げ
るよう1こするものである。
In order to achieve the above object, the present invention provides the above-mentioned magnetic thrust illumination bearing, in which the fixed part iron core of the thrust bearing coupled to the stator side of the electric machine is placed on the lower side. By arranging the rotating part iron cores of the magnetic thrust bearings coupled to the child side to face each other with a suitable gap above, and providing excitation coils with the same number of turns on the opposing surfaces of both, k, respectively. Is the magnetomotive force generated by the excitation coil phase? By excitation in series in opposite directions ζ, the parts of the magnetic thrust bearing that face each other across the gap between the fixed part iron core and the rotating part iron core are magnetically A repulsive force is generated, and the repulsive force ζ is used to lift the rotating part of the electric machine.

〔発明の実施)>1 ) 、氾3図において電気機械の回転子3の側に結合された
磁気スラストΦfIt受lの回転部鉄心7吉電気機械の
固定−′r−2側に結澄された(庭気スラス) ’il
l受1の固定部鉄心4とはギーヤップ8を介して回転部
鉄心7を上側にして対向して配置される。回転部鉄心7
と固定部鉄心4とζこはそれぞれ同一巻回数の励磁コイ
ル12及び13が設けられ、前記電気機械の固定子2側
に設けられるブラシと回転r−3側に設けられるスリッ
プリング(共にス示せず)を介して相互に直列になる如
く凄続さイル1同−電流でしかも相互に逆方向の起磁力
を発生ずる如くに励磁される。その結果磁気スラスト軸
受1の回転部鉄心7と固定部鉄心4とのギャップ8を介
して相互に対面する部分が磁気的ζこ同一の極性となり
、固定部鉄心4と回転部鉄心7との間lこ相互反撥力が
働らく。その結果回転部鉄心7を介して前記電気機械の
回転子31こ対するつり上げ力1oが生じ電気機械の回
・紙部がつり上げられる。この場合(こ生ずる′つり上
げ力10のギャップ8の長さζこ対する特性は従来のi
気スラス) 軸受の場合と同様に第2図ζこ示す如くで
あるが、本発明の磁気スラスト噛受1こおいては回転部
鉄心7が固定部鉄心4の上側に位・べしているから、下
向きの荷重1】が大ζこなつ′C回転子3が下降してギ
ャップ8の長さが短縮されると回転部鉄心7とII、1
定子鉄心4との間の反撥力、したがつ′CつりFげ力1
0が増大し、逆?こ回転子3にL向きの逆スラスト力が
作用しく一1昇するとギヤツブ8が広がり回転部鉄心7
と固定部鉄心4との間の反撥力、したがってつり1−げ
力が減退する。換gすればこの場合には回転止31こ作
用する荷重の変動(こより回転子3が一ヒ下すると、ぞ
イ1.ζこ対応するギャップ8の変化ζこよる磁気スラ
スト軸受のつり上げ力10の変化が前記荷置の変動を吸
収する叩くに働らく。したり5つて今何らかの理由ζこ
より・油記准気機械の回転部に逆スラスト旬が作用して
回転部が浮き一ヒろうとしてt、)、fin気スラスラ
スト軸受1ャップ8が増大することζこより回転部に対
するつり上げ力10が減少し電気機械の回転部総重量と
つり上げ力の和が前記1更スラストカと再度均衡する点
て安定するから、従来の磁気スラスト軸受の場合の如く
回転部が著しく浮き上り逆スラスト軸受(図示せず)に
過大な負荷が作用し、これが損1易を受ける虞れはなく
なるっ 〔発明の効果〕 本発明は以上ζこ説明した1口<その回転部がr1″C
気機械の回転モ側にその固定部が電気機械の固定子〇(
1]に結合され、前記回転部と固定部とが適宜のギャッ
プを介して相互(こ対向する如くに配流されるとともに
、相互の間ζこ働らく磁気力により回転子を一つり上げ
る如く作用する立輛形電気機械の磁気スラスト軸受にお
いて、前記電気機械の固定:f−供、11ζこ結合され
る前記スラスト軸受の固定部鉄心を下側に、前記電気機
械の回転子側に結合される前記磁気スラスト軸受の回1
伝部鉄心を上側に適宜のギャップを介して相互ζこ対向
させかつ両者の対向する面にそれぞれ同一巻回数の励磁
コイルを設けるとともに、それぞれの励磁コイルが生「
る起磁力が相互に逆方向ζこなる叩く直列Oこ励磁する
よう(こすることζこより、磁気スラスト・1411受
の固定部鉄心と回転部鉄心とのギャップを介して対向す
る部分が磁・気的に・iη−極性になって生ずる反撥力
により+ijl記電気機械の回転部をつりLげる−70
くに作用しかつ・ifJ記161転部に1動らくスラス
ト力の変動に応じて前記つり−にげ力がその変動を吸収
する叩くに変叱伯ろから、前記回転部ζこ著しい逆スラ
スト力が作用し7ても前記回転部総重量と前記つり上げ
力との4131)> 、ij記逆スラスト力と均衡して
安定し、前記回転部が不当に浮き上って逆スラスト軸受
に過大な負荷がか\り損傷を生ずることを防市できる効
果がある。
[Practice of the Invention]>1) In Figure 3, the rotating part iron core 7 of the magnetic thrust ΦIt receiver connected to the rotor 3 side of the electric machine is connected to the fixed -'r-2 side of the electric machine. ta (niwaki surasu) 'il
The fixed part iron core 4 of the l receiver 1 is arranged to face the fixed part iron core 4 with the rotating part iron core 7 on the upper side with a gear up 8 interposed therebetween. Rotating part iron core 7
The fixed part iron cores 4 and ζ are provided with excitation coils 12 and 13 having the same number of turns, respectively, and a brush provided on the stator 2 side of the electric machine and a slip ring provided on the rotating r-3 side (both shown in FIG. The coils 1 are connected in series with each other through the coils 1 and 2, and are excited with the same current so as to generate magnetomotive forces in mutually opposite directions. As a result, the parts of the rotating part iron core 7 and the fixed part iron core 4 of the magnetic thrust bearing 1 that face each other through the gap 8 have the same magnetic polarity, and the polarity between the fixed part iron core 4 and the rotating part iron core 7 becomes the same. A mutual repulsive force acts. As a result, a lifting force 1o is generated against the rotor 31 of the electric machine via the rotating part iron core 7, and the rotating and paper parts of the electric machine are lifted up. In this case, the characteristics of the lifting force 10 and the length ζ of the gap 8 are as compared to the conventional i
As in the case of bearings, as shown in FIG. , the downward load 1] is large. When the rotor 3 descends and the length of the gap 8 is shortened, the rotating part iron cores 7 and II, 1
The repulsive force between the stator core 4 and the resulting force 1
0 increases and vice versa? A reverse thrust force in the L direction acts on the rotor 3, and when the rotor 3 rises, the gear lug 8 expands and the rotating part iron core 7
The repulsive force between the fixed part iron core 4 and the lifting force is reduced. In other words, in this case, the change in the load acting on the rotation stop 31 (when the rotor 3 is lowered by one step, the change in the gap 8) is 1. This change acts to absorb the fluctuations in the cargo position.For some reason, the reverse thrust force acts on the rotating part of the machine and the rotating part is about to float. t,), the fin thrust thrust bearing 1 cap 8 increases, and the lifting force 10 on the rotating parts decreases, and the sum of the total weight of the rotating parts of the electric machine and the lifting force becomes balanced again with the above-mentioned thrust force. Since it is stable, there is no risk that the rotating part will rise significantly and an excessive load will be applied to the reverse thrust bearing (not shown), which could easily cause damage, as in the case of conventional magnetic thrust bearings. 〕 The present invention is based on the above-described one opening < whose rotating part is r1''C.
The fixed part on the rotating side of the electric machine is the stator of the electric machine (
1], the rotating part and the fixed part are distributed so as to face each other through an appropriate gap, and the magnetic force acting between them acts to lift the rotor up by one. In a magnetic thrust bearing for a vertical electric machine, the fixing part of the electric machine is connected to the fixed part iron core of the thrust bearing on the lower side, and the fixed part iron core of the thrust bearing is connected to the lower side of the fixed part of the thrust bearing, and Magnetic thrust bearing times 1
The transmission iron cores are placed on the upper side facing each other with an appropriate gap in between, and excitation coils with the same number of turns are provided on the opposing surfaces of both, and each excitation coil is
In such a way that the magnetomotive forces in mutually opposite directions ζ are excited by the series O (by rubbing ζ), the parts of the magnetic thrust 1411 receiver that face each other across the gap between the fixed part iron core and the rotating part iron core are magnetized. The repulsive force generated by the polarity of the air lifts the rotating part of the electrical machine -70
If the rotating part ζ acts on the rotating part and changes in response to the fluctuation of the thrust force, the lifting force absorbs the fluctuation, so the rotating part ζ has a significant reverse thrust force. Even if 7 is applied, the total weight of the rotating part and the lifting force are stable in balance with the reverse thrust force described in ij, and the rotating part is unduly lifted and an excessive load is placed on the reverse thrust bearing. It has the effect of preventing damage caused by building.

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

、’I”、 1図は従来の磁気スラスト軸受の構成を示
す概略図、第2図は一般に磁気スラスト軸受(こおける
つリートげ力とギャップとの関係を示す特性図、第31
媚は本発明の磁気スラスト軸受の構成を示す概略図をそ
れぞれ表わす。 ] 磁気スラスト!軸受、2.−@気機械の固定子(i
iil、3 准気機械′D回転子側、4・固定部鉄心、
7 回転部鉄心、8 ギャップ、10・・つり上げJJ
、12 回転部鉄心励磁コイル、13・固定部鉄心励磁
コイル。
,'I'', Figure 1 is a schematic diagram showing the configuration of a conventional magnetic thrust bearing, Figure 2 is a characteristic diagram showing the relationship between the tension force and the gap in a magnetic thrust bearing (Fig. 31).
The figures each represent a schematic diagram showing the configuration of the magnetic thrust bearing of the present invention. ] Magnetic thrust! Bearing, 2. −@Ki Machine Stator (i
iii, 3 Quasi-air machine 'D rotor side, 4. Fixed part iron core,
7 Rotating part iron core, 8 Gap, 10... Lifting JJ
, 12 Rotating part iron core excitation coil, 13 Fixed part iron core excitation coil.

Claims (1)

【特許請求の範囲】[Claims] 】)その回転部が電気機4賊の回転子側にその固定部が
電気機械の固定子側に結合され、前記回転部と固定部と
が適宜のギャップを介して相互に対向する如くlこ配置
されるとともに、相互の間(こ働らく磁気力により回転
子をつり上げる如く作用する室軸形電気機械の磁気スラ
スト軸受において、前記電気機械の固定子側に結合され
る前記スラスト軸受の固定部鉄心を下側に、前記電気機
械の回転F側に結合される前記磁気スラスト軸受の回転
部鉄心をに側に適宜のギャップを介して相互に対向させ
かつ両者の対向する面にそれぞれ同一巻回数の励磁コイ
ルを設けるとともに、それぞれの励磁コイルの生ずる起
磁力が相互に逆方向になる如く直列に1励磁するように
してなる磁気スラスト軸受。
]) The rotating part is connected to the rotor side of the electric machine, and the fixed part is connected to the stator side of the electric machine, such that the rotating part and the fixed part face each other with an appropriate gap between them. In a magnetic thrust bearing of a chamber-shaft electric machine, which acts to lift up a rotor by magnetic force, the fixed part of the thrust bearing is connected to the stator side of the electric machine. The rotating part iron core of the magnetic thrust bearing, which is connected to the rotating F side of the electric machine, is placed opposite to each other with an appropriate gap between the iron core on the lower side and the rotating part iron core of the magnetic thrust bearing connected to the rotation F side of the electric machine. A magnetic thrust bearing is provided with excitation coils and is configured to be excited in series so that the magnetomotive forces generated by the respective excitation coils are in opposite directions.
JP5571683A 1983-03-31 1983-03-31 Magnetic thrust bearing Pending JPS59180118A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5571683A JPS59180118A (en) 1983-03-31 1983-03-31 Magnetic thrust bearing

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5571683A JPS59180118A (en) 1983-03-31 1983-03-31 Magnetic thrust bearing

Publications (1)

Publication Number Publication Date
JPS59180118A true JPS59180118A (en) 1984-10-13

Family

ID=13006596

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5571683A Pending JPS59180118A (en) 1983-03-31 1983-03-31 Magnetic thrust bearing

Country Status (1)

Country Link
JP (1) JPS59180118A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6019319A (en) * 1996-02-08 2000-02-01 Falbel; Gerald Momentum wheel energy storage system using magnetic bearings

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6019319A (en) * 1996-02-08 2000-02-01 Falbel; Gerald Momentum wheel energy storage system using magnetic bearings

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