JPH0561869B2 - - Google Patents
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- Publication number
- JPH0561869B2 JPH0561869B2 JP61056313A JP5631386A JPH0561869B2 JP H0561869 B2 JPH0561869 B2 JP H0561869B2 JP 61056313 A JP61056313 A JP 61056313A JP 5631386 A JP5631386 A JP 5631386A JP H0561869 B2 JPH0561869 B2 JP H0561869B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- field coil
- rotor
- insulation
- helium
- 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 - Fee Related
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Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment
Landscapes
- Superconductive Dynamoelectric Machines (AREA)
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は超電導回転電機の回転子の構造に関
するものである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] This invention relates to the structure of a rotor of a superconducting rotating electric machine.
従来この種の回転子として例えば特開昭57−
22372号公報に開示されたものがあり、その構成
を第4図に示す。第4図において、1はトルクチ
ユーブ、2はトルクチユーブ1の中央部を形成す
るコイル取付軸、3はコイル取付軸2に固定され
ている超電導界磁コイル、4はトルクチユーブ1
とコイル取付軸2を囲繞する常温ダンパ、5はこ
の常温ダンパ4とコイル取付軸2の間に配設され
ている低温ダンパ、6及び7はコイル取付軸2の
夫々外周部及び側面部に取り付けられたヘリウム
外筒、ヘリウム端板、8及び9は夫々駆動側、反
駆動側端部軸、10はこれらの端部軸8,9を軸
支する軸受、11は界磁電流供給用のスリツプリ
ング、12はトルクチユーブ1に形成或いは配置
されている熱交換器、13は側部輻射シールド、
14は真空部である。
Conventionally, this kind of rotor is known as, for example, Japanese Patent Application Laid-open No. 57-
There is one disclosed in Japanese Patent No. 22372, and its configuration is shown in FIG. In FIG. 4, 1 is a torque tube, 2 is a coil mounting shaft forming the center of the torque tube 1, 3 is a superconducting field coil fixed to the coil mounting shaft 2, and 4 is a torque tube 1.
and a room-temperature damper surrounding the coil mounting shaft 2; 5 is a low-temperature damper disposed between the room-temperature damper 4 and the coil mounting shaft 2; 6 and 7 are mounted on the outer periphery and side surface of the coil mounting shaft 2, respectively; 8 and 9 are drive side and non-drive side end shafts, 10 is a bearing that pivotally supports these end shafts 8 and 9, and 11 is a slip for supplying field current. ring, 12 is a heat exchanger formed or placed in the torque tube 1, 13 is a side radiation shield,
14 is a vacuum section.
上記構成からなる超電導回転機の回転子におい
ては、コイル取付軸2に配置されている超電導界
磁コイルを極低温に冷却することにより、電気抵
抗を零の状態とし、励磁損失をなくすことによ
り、この超電導界磁コイル3に強力な磁界を発生
させ、固定子(図示せず)に交流電力を発生させ
る。この超電導界磁コイル3を極低温に冷却、保
持するために液体ヘリウムを反駆動側端部軸9の
中央部から導入管(図示せず)を通じ、ヘリウム
外筒6、ヘリウム端板7により形成される液体ヘ
リウム容器部に供給する一方、回転子内部を真空
部14により高真空に保つと共に、極低温の超電
導界磁コイル3及びコイル取付軸2に回転トルク
を伝えるトルクチユーブ1を薄肉円筒とし、且つ
熱交換器12を設け、このトルクチユーブ1を通
じ極低温部に侵入する熱を極力減らす構造が最も
一般的である。さらに、側面からの輻射により侵
入する熱を低減するため、側部輻射シールド13
が設けられている。 In the rotor of the superconducting rotating machine having the above configuration, the superconducting field coil disposed on the coil mounting shaft 2 is cooled to an extremely low temperature to bring the electric resistance to zero and eliminate excitation loss. This superconducting field coil 3 generates a strong magnetic field, and a stator (not shown) generates alternating current power. In order to cool and maintain this superconducting field coil 3 at an extremely low temperature, liquid helium is introduced from the center of the non-drive side end shaft 9 through a pipe (not shown) formed by a helium outer cylinder 6 and a helium end plate 7. The torque tube 1 is made of a thin-walled cylinder and supplies the liquid helium to the liquid helium container section in which the helium is stored, while maintaining the inside of the rotor at a high vacuum in the vacuum section 14, and transmitting rotational torque to the ultra-low temperature superconducting field coil 3 and the coil mounting shaft 2. The most common structure is to provide a heat exchanger 12 and to reduce as much as possible the heat that enters the cryogenic part through the torque tube 1. Furthermore, in order to reduce the heat that enters due to radiation from the sides, the side radiation shield 13
is provided.
一方、常温ダンパ4及び低温ダンパ5は、固定
子からの高調波磁界をシールドし、超電導界磁コ
イル3を保護すると共に、電力系統のじよう乱に
よる回転子振動を減衰させる機能を有する一方、
常温ダンパ4は真空外筒としての機能、低温ダン
パはヘリウム容器部への輻射シールドとしての機
能を兼ねる方式が一般的である。なお第4図にお
いては、回転子内部のヘリウム導入、排出系を構
成する配管類及び回転子に接続されているヘリウ
ム導入、排出装置は省略した。 On the other hand, the normal temperature damper 4 and the low temperature damper 5 have the function of shielding harmonic magnetic fields from the stator, protecting the superconducting field coil 3, and attenuating rotor vibrations caused by disturbances in the power system.
Generally, the normal temperature damper 4 functions as a vacuum outer cylinder, and the low temperature damper functions as a radiation shield for the helium container. In FIG. 4, piping constituting a helium introduction and discharge system inside the rotor and a helium introduction and discharge device connected to the rotor are omitted.
第5図は第4図V−V線における断面図であ
り、図において、2はコイル取付軸、3は超電導
界磁コイル、6はヘリウム外筒、15は液体ヘリ
ウムの液溜め部、16はヘリウム蒸気空間、17
はコイル取付軸2に形成された超電導界磁コイル
3を収納するスロツト、18はスロツト17内に
配設され、超電導界磁コイル3とコイル取付軸2
との間の対地絶縁、19は超電導界磁コイル3を
固定するウエツジ、20はコイル取付軸2とヘリ
ウム外筒6との間に設けられたヘリウム流路、2
1は液溜め部15とスロツト17とに連通して設
けられたヘリウム流通孔、22a,22bは対地
絶縁18に形成された例えば円形状の貫通孔であ
る。このような回転子に使用される超電導界磁コ
イルとしては例えば特開昭57−186960号公報に開
示されたものがあり、その構成を第6図に示す。
図において、3は超電導界磁コイル、3aは複数
の超電導素線を撚り線等により成形された超電導
線であり、複数列、複数層巻回されている。23
はこれら超電導線3aの列間に挿入された列間絶
縁、24は超電導線3aの層間に挿入された層間
絶縁である。尚、超電導界磁コイル3は、超電導
線3aを1本持ちで、かつ超電導線3aの列間に
は列間絶縁23を、超電導線3aの層間には層間
絶縁24をそれぞれ挿入しながら巻回し、巻回後
はエポキシ樹脂で処理してモールド状に形成さ
れ、超電導線3aの短絡防止がなされている。 FIG. 5 is a cross-sectional view taken along the line V-V in FIG. helium vapor space, 17
18 is a slot for accommodating the superconducting field coil 3 formed on the coil mounting shaft 2;
19 is a wedge for fixing the superconducting field coil 3; 20 is a helium flow path provided between the coil mounting shaft 2 and the helium outer cylinder 6;
1 is a helium flow hole provided in communication with the liquid reservoir 15 and the slot 17, and 22a and 22b are through holes formed in the ground insulation 18, each having a circular shape, for example. A superconducting field coil used in such a rotor is disclosed in, for example, Japanese Patent Laid-Open No. 186960/1983, and its configuration is shown in FIG.
In the figure, 3 is a superconducting field coil, and 3a is a superconducting wire formed by twisting a plurality of superconducting strands, etc., and is wound in multiple rows and in multiple layers. 23
24 is inter-row insulation inserted between the rows of these superconducting wires 3a, and 24 is inter-layer insulation inserted between the layers of superconducting wires 3a. The superconducting field coil 3 has one superconducting wire 3a and is wound while inserting inter-column insulation 23 between the rows of the superconducting wire 3a and interlayer insulation 24 between the layers of the superconducting wire 3a. After winding, the superconducting wire 3a is treated with an epoxy resin and formed into a mold shape to prevent short circuits of the superconducting wire 3a.
一般的に超電導回転圧機においては、超電導界
磁コイルの極低温冷却をいかにして行なうかとい
う点に重要な技術問題がある。超電導界磁コイル
を超電導状態にするためには、超電導遷移温度以
下に冷却することが必要であり、現在ではヘリウ
ムを冷却媒体として絶対温度1Kないし20Kに保
持することが行なわれている。一方、このような
極低温状態においては超電導界磁コイルの比熱が
極めて小さくなつているため、超電導界磁コイル
内の微少な発熱あるいは超電導界磁コイルへの僅
かな侵入熱量によつて超電導界磁コイルの温度が
上昇し超電導遷移温度を越える恐れが常に存在す
る。従つて、超電導界磁コイル内の微少な発熱あ
るいは超電導界磁コイルへの僅かな侵入熱量をい
かに速かに除去して超電導界磁コイルの温度上昇
をおさえるかが超電導回転電機の設計上の重要な
ポイントとなる。 In general, in superconducting rotary pressure machines, there is an important technical problem in how to cool the superconducting field coil to a cryogenic temperature. In order to bring a superconducting field coil into a superconducting state, it is necessary to cool it below the superconducting transition temperature, and currently, helium is used as a cooling medium to maintain the absolute temperature at 1K to 20K. On the other hand, in such extremely low temperature conditions, the specific heat of the superconducting field coil is extremely small, so the superconducting field coil is heated by a small amount of heat generated within the superconducting field coil or by a small amount of heat entering the superconducting field coil. There is always a risk that the temperature of the coil will rise and exceed the superconducting transition temperature. Therefore, in the design of superconducting rotating electric machines, it is important to suppress the temperature rise of the superconducting field coil by quickly removing the minute amount of heat generated within the superconducting field coil or the slight amount of heat entering the superconducting field coil. This is a great point.
次に冷却動作について説明する。超電導界磁コ
イル3内の微少発熱、あるいは超電導界磁コイル
3への僅かな熱侵入によつて生じた熱は、超電導
界磁コイル3の外周側の対地絶縁18との僅かな
間隙に存在しているヘリウムに吸収される。吸熱
により膨張し密度が小さくなつたヘリウムは、遠
心力場の自然対流によつて対地絶縁18の貫通孔
22aを通り抜け、コイル取付軸2のヘリウム流
通孔21を経て液溜め部15に出る。一方、超電
導界磁コイル3回りで生ずるヘリウム不足は、ヘ
リウム流路20からウエツジ19の隙間及び対地
絶縁18の貫通孔22bを通つて超電導界磁コイ
ル3回りに流入するヘリウムによつて補われる。
吸熱膨張したヘリウムは、液溜め部15におい
て、その一部が蒸発することによつて冷却され
る。冷却されたヘリウムは、別のヘリウム流通孔
21から対地絶縁18の貫通孔22aを経て超電
導界磁コイル3の周囲に入り込み、さらに対地絶
縁18の貫通孔22b及びウエツジ19の隙間を
通りヘリウム流路20に出る。 Next, the cooling operation will be explained. Heat generated by slight heat generation within the superconducting field coil 3 or slight heat intrusion into the superconducting field coil 3 exists in a slight gap between the outer circumferential side of the superconducting field coil 3 and the ground insulation 18. It is absorbed by helium. Helium, which expands due to heat absorption and has a reduced density, passes through the through hole 22a of the ground insulation 18 due to the natural convection of the centrifugal force field, and exits to the liquid reservoir 15 through the helium flow hole 21 of the coil mounting shaft 2. On the other hand, the helium shortage occurring around the superconducting field coil 3 is compensated for by helium flowing from the helium channel 20 around the superconducting field coil 3 through the gap between the wedge 19 and the through hole 22b of the ground insulation 18.
The endothermically expanded helium is cooled in the liquid reservoir 15 by partially evaporating it. The cooled helium enters around the superconducting field coil 3 from another helium flow hole 21 through the through hole 22a of the ground insulation 18, and further passes through the through hole 22b of the earth insulation 18 and the gap between the wedge 19 and enters the helium flow path. Appears on the 20th.
以上のように円滑な自然循環を行なうことによ
り、超電導界磁コイル3の冷却が行なわれ、超電
導界磁コイル3を超電導遷移温度以下に保つてい
る。 By performing the smooth natural circulation as described above, the superconducting field coil 3 is cooled, and the superconducting field coil 3 is kept below the superconducting transition temperature.
しかしながら上述した従来装置では、超電導界
磁コイル3の冷却がその外周面からしか冷却され
ない構造となつており、超電導界磁コイル3内部
の超電導線3aで発熱した場合、超電導線3aの
熱は列間絶縁23、層間絶縁24、また他の超電
導線3aを介した熱伝導を経て超電導界磁コイル
3外周のヘリウムで冷却されて除去されることに
なり、冷却効果が悪く、超電導線3aの温度が上
昇し、超電導破壊(クエンチ)を生ずる問題点が
あつた。
However, in the conventional device described above, the superconducting field coil 3 is cooled only from its outer peripheral surface, and when heat is generated in the superconducting wire 3a inside the superconducting field coil 3, the heat of the superconducting wire 3a is Through heat conduction through the interlayer insulation 23, interlayer insulation 24, and other superconducting wires 3a, the helium on the outer periphery of the superconducting field coil 3 cools and removes the heat, resulting in a poor cooling effect and a drop in the temperature of the superconducting wire 3a. There was a problem in that the superconductivity increased, causing superconducting breakdown (quenching).
この発明は上記のような問題点を解消するため
になされたものであり、冷却効果を高め超電導破
壊を生ずることのない超電導回転電機の回転子を
提供することを目的とする。 The present invention has been made to solve the above-mentioned problems, and an object thereof is to provide a rotor for a superconducting rotating electrical machine that enhances the cooling effect and does not cause superconductor breakdown.
この発明に係る超電導回転電機の回転子は、超
電導界磁コイルの超電導線間の列間絶縁を穴付絶
縁材で構成し、層間絶縁を溝付絶縁材で構成した
ものである。
In the rotor of the superconducting rotating electric machine according to the present invention, the inter-row insulation between the superconducting wires of the superconducting field coil is made of a holed insulating material, and the interlayer insulation is made of a grooved insulating material.
この発明における超電導回転電機の回転子は、
超電導界磁コイルを超電導状態にするための冷媒
である液体ヘリウムが、穴付絶縁材で構成された
列間絶縁の穴部、溝付絶縁材で構成された層間絶
縁の溝部を通つて超電導界磁コイルの超電導線を
直接冷却する。
The rotor of the superconducting rotating electric machine in this invention is
Liquid helium, which is a refrigerant to bring the superconducting field coil into a superconducting state, generates a superconducting field through the holes in the interrow insulation made of holed insulating material and the grooves in the interlayer insulation made of grooved insulating material. Directly cools the superconducting wire of the magnetic coil.
以下、この発明の一実施例を図について説明す
る。第1図〜第3図において、3は超電導界磁コ
イル、3aは複数の超電導素線が撚り線等により
成形された超電導線であり、複数列、複数層巻回
されている。25は超電導線3aの列間に挿入さ
れ、複数の穴25aを有する例えばエポキシ系マ
イカルタ板等からなる穴付絶縁材で構成された列
間絶縁であり、第3図にす通り、複数の穴付絶縁
材により構成されている。26は超電導線3aの
層間に挿入され、第1図上において横方向の溝2
6aを有する例えばエポキシ系マイカル板等から
なる溝付絶縁材で構成された層間絶縁であり、超
電導界磁コイル3の長手方向に対し複数配設され
て構成されている。尚、超電導界磁コイル3は、
超電導線3aを1本持ちで、かつ超電導線3aの
列間には穴25aを有する列間絶縁25を、超電
導線3aの層間には溝26aを有する層間絶縁2
6をそれぞれ挿入しながら巻回されて形成され、
超電導線3aは列間絶縁25と層間絶縁26とに
囲まれた状態となり、超電導線3aの短絡防止が
なされている。また、超電導界磁コイル3のエポ
キシ樹脂処理は施していない。また、超電導線3
aは撚り線等により成形しているので、超電導線
3aと列間絶縁25、層間絶縁26との間には僅
かな隙間が存在している。
An embodiment of the present invention will be described below with reference to the drawings. In FIGS. 1 to 3, 3 is a superconducting field coil, and 3a is a superconducting wire formed by stranding a plurality of superconducting wires, which are wound in multiple rows and in multiple layers. Reference numeral 25 denotes an inter-row insulation which is inserted between the rows of the superconducting wires 3a and is made of a holed insulating material made of, for example, an epoxy micarta board and has a plurality of holes 25a. It is made of insulating material. 26 is inserted between the layers of the superconducting wire 3a, and in FIG.
6a, which is an interlayer insulation made of a grooved insulating material made of, for example, an epoxy-based mical plate, and is arranged in plural numbers in the longitudinal direction of the superconducting field coil 3. In addition, the superconducting field coil 3 is
An inter-column insulation 25 having one superconducting wire 3a and having a hole 25a between the rows of the superconducting wire 3a, and an inter-layer insulation 2 having a groove 26a between the layers of the superconducting wire 3a.
6 is wound while inserting each,
The superconducting wire 3a is surrounded by the intercolumn insulation 25 and the interlayer insulation 26, and short circuits of the superconducting wire 3a are prevented. Further, the superconducting field coil 3 was not treated with epoxy resin. Also, superconducting wire 3
Since a is made of twisted wire or the like, there is a slight gap between the superconducting wire 3a and the intercolumn insulation 25 and the interlayer insulation 26.
次に冷却動作について説明する。超電導界磁コ
イル3を超電導状態にするための冷媒である液体
ヘリウムは、超電導界磁コイル3の外表面を流れ
ると共に、超電導線3aと列間絶縁25、層間絶
縁26との間の僅かな隙間、列間絶縁25の穴2
5a、層間絶縁26の溝26aを通つて超電導線
3aの表面に流れ、超電導界磁コイル3の全ての
超電導線3aを液体ヘリウムによつて直接冷却す
るようになつている。従つて、超電導線3aで発
熱が生じても、超電導線3aの周囲の液体ヘリウ
ムですばやく熱が取り除かれ、超電導線3aの温
度上昇は極めて小さく、超電導破壊を生ずること
はない。 Next, the cooling operation will be explained. Liquid helium, which is a coolant for bringing the superconducting field coil 3 into a superconducting state, flows on the outer surface of the superconducting field coil 3 and also in the slight gaps between the superconducting wire 3a and the inter-column insulation 25 and the inter-layer insulation 26. , hole 2 of inter-row insulation 25
5a, it flows to the surface of the superconducting wire 3a through the groove 26a of the interlayer insulation 26, and all the superconducting wires 3a of the superconducting field coil 3 are directly cooled by liquid helium. Therefore, even if heat is generated in the superconducting wire 3a, the heat is quickly removed by the liquid helium around the superconducting wire 3a, and the temperature rise in the superconducting wire 3a is extremely small, and superconductor breakdown does not occur.
尚、上記実施例では層間絶縁26の溝26aは
両面にそれぞれ設けた場合について述べたが、片
面に設けるようにしてもよい。 In the above embodiment, the grooves 26a of the interlayer insulation 26 are provided on both sides, but they may be provided on one side.
この発明は以上説明した通り、超電導界磁コイ
ルの超電導線間の列間絶縁を穴付絶縁材で構成
し、層間絶縁を溝付絶縁材で構成したので、超電
導界磁コイルを超電導状態にするための冷媒であ
る液体ヘリウムが、穴付絶縁材で構成された列間
絶縁の穴、溝付絶縁材で構成された層間絶縁の溝
を通つて超電導界磁コイルの超電導線を直接冷却
するので冷却効果が向上し、超電導破壊を生ずる
ことのない信頼性の高い超電導回転電機の回転子
を得ることができる。
As explained above, in this invention, the inter-row insulation between the superconducting wires of the superconducting field coil is made of a holed insulating material, and the interlayer insulation is made of a grooved insulating material, so that the superconducting field coil is brought into a superconducting state. Liquid helium, the refrigerant for the superconducting field coils, directly cools the superconducting wires of the superconducting field coils through the holes in the interrow insulation made of holed insulating material and the grooves in the interlayer insulation made of grooved insulating material. It is possible to obtain a highly reliable rotor for a superconducting rotating electric machine with improved cooling effect and without superconductor breakdown.
第1図はこの発明の一実施例による超電導回転
電機の回転子における超電導界磁コイルを示す断
面図、第2図は第1図の要部拡大図、第3図は第
2図の−線における断面図、第4図は従来の
一般的な超電導回転電機の回転子を示す縦断面
図、第5図は第4図のV−V線における断面図、
第6図は従来の超電導界磁コイルを示す断面図で
ある。
図において、2はコイル取付軸、3は超電導界
磁コイル、3aは超電導線、25は列間絶縁、2
6は層間絶縁である。尚、図中同一符号は同一ま
たは相当部分を示す。
Fig. 1 is a sectional view showing a superconducting field coil in a rotor of a superconducting rotating electric machine according to an embodiment of the present invention, Fig. 2 is an enlarged view of the main part of Fig. 1, and Fig. 3 is a - line in Fig. 2. 4 is a vertical sectional view showing a rotor of a conventional general superconducting rotating electric machine, and FIG. 5 is a sectional view taken along line V-V in FIG. 4.
FIG. 6 is a sectional view showing a conventional superconducting field coil. In the figure, 2 is a coil mounting shaft, 3 is a superconducting field coil, 3a is a superconducting wire, 25 is an inter-row insulation, 2
6 is interlayer insulation. Note that the same reference numerals in the figures indicate the same or corresponding parts.
Claims (1)
れた超電導界磁コイルと、この超電導界磁コイル
を保持するコイル取付軸とを有する超電導回転電
機の回転子において、上記超電導界磁コイルの超
電導線間の列間絶縁を穴付絶縁材で、層間絶縁を
溝付絶縁材でそれぞれ構成したことを特徴とする
超電導回転電機の回転子。 2 穴付絶縁材はエポキシ系マイカルタ板で構成
されたことを特徴とする特許請求の範囲第1項記
載の超電導回転電機の回転子。 3 溝付絶縁材はエポキシ系マイカルタ板で構成
されたことを特徴とする特許請求の範囲第1項ま
たは第2項記載の超電導回転電機の回転子。[Scope of Claims] 1. A rotor for a superconducting rotating electric machine having a superconducting field coil formed by winding multiple rows and layers of superconducting wire, and a coil mounting shaft that holds the superconducting field coil, A rotor for a superconducting rotating electric machine, wherein the inter-row insulation between the superconducting wires of the superconducting field coil is made of a holed insulating material, and the interlayer insulation is made of a grooved insulating material. 2. A rotor for a superconducting rotating electric machine according to claim 1, wherein the insulating material with holes is made of an epoxy micarta plate. 3. A rotor for a superconducting rotating electrical machine according to claim 1 or 2, wherein the grooved insulating material is made of an epoxy micarta plate.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61056313A JPS62213548A (en) | 1986-03-12 | 1986-03-12 | Rotor of superconducting rotary electric machine |
| US07/009,920 US4739202A (en) | 1986-03-12 | 1987-02-02 | Superconducting electric rotary machine having grooved insulation for carrying coolant |
| FR8702094A FR2598045B1 (en) | 1986-03-12 | 1987-02-18 | SUPERCONDUCTING ELECTRIC ROTATING MACHINE |
| DE19873706437 DE3706437A1 (en) | 1986-03-12 | 1987-02-27 | SUPRALINE, ROTATING ELECTRICAL MACHINE |
| FR8713725A FR2603430B1 (en) | 1986-03-12 | 1987-10-05 | SUPERCONDUCTING ELECTRIC ROTATING MACHINE |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61056313A JPS62213548A (en) | 1986-03-12 | 1986-03-12 | Rotor of superconducting rotary electric machine |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62213548A JPS62213548A (en) | 1987-09-19 |
| JPH0561869B2 true JPH0561869B2 (en) | 1993-09-07 |
Family
ID=13023663
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61056313A Granted JPS62213548A (en) | 1986-03-12 | 1986-03-12 | Rotor of superconducting rotary electric machine |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62213548A (en) |
-
1986
- 1986-03-12 JP JP61056313A patent/JPS62213548A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62213548A (en) | 1987-09-19 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |