JPH0524746B2 - - Google Patents

Info

Publication number
JPH0524746B2
JPH0524746B2 JP61056321A JP5632186A JPH0524746B2 JP H0524746 B2 JPH0524746 B2 JP H0524746B2 JP 61056321 A JP61056321 A JP 61056321A JP 5632186 A JP5632186 A JP 5632186A JP H0524746 B2 JPH0524746 B2 JP H0524746B2
Authority
JP
Japan
Prior art keywords
field coil
superconducting
superconducting field
channel
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
Application number
JP61056321A
Other languages
Japanese (ja)
Other versions
JPS62213556A (en
Inventor
Koichi Ooshita
Akinori Ueda
Hidenao Hatanaka
Susumu Maeda
Toshiki Hirao
Mitsuhiro Uchida
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 JP61056321A priority Critical patent/JPS62213556A/en
Priority to US07/009,920 priority patent/US4739202A/en
Priority to FR8702094A priority patent/FR2598045B1/en
Priority to DE19873706437 priority patent/DE3706437A1/en
Publication of JPS62213556A publication Critical patent/JPS62213556A/en
Priority to FR8713725A priority patent/FR2603430B1/en
Publication of JPH0524746B2 publication Critical patent/JPH0524746B2/ja
Granted legal-status Critical Current

Links

Classifications

    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

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  • 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.

〔従来の技術〕[Conventional technology]

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3図に示す。第3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、17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. 3, 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, 17 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に配設されている超電導界
磁コイル3を極低温に冷却することにより、電機
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 3 disposed on the coil mounting shaft 2 is cooled to an extremely low temperature to bring the electrical resistance to zero and eliminate excitation loss. As a result, a strong magnetic field is generated in the superconducting field coil 3, and AC power is generated in the stator (not shown). 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3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. 3, 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4図は第3図−線における断面図、即
ち、特開昭57−202852号公報に示されたものであ
り、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内の両サイドに配
設されたサイドつめもの、19は超電導界磁コイ
ル3を固定するウエツジ、20,21は超電導界
磁コイル3の外周面、内周面にそれぞれ接する上
部つめもの、下部つめものであり、それぞれ例え
ば円形状の貫通孔20a,21aを有している。
22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、23は液溜め部15と
スロツト17の底部とに連通して設けられたコイ
ル取付軸ヘリウム流通孔である。
FIG. 4 is a sectional view taken along the line shown in FIG.
6 is a helium outer cylinder, 15 is a liquid helium reservoir, 16 is a helium vapor space, 17 is a slot for housing the superconducting field coil 3 formed on the coil mounting shaft 2, and 18 is a slot on both sides of the slot 17. The disposed side claws include a wedge 19 for fixing the superconducting field coil 3, and 20 and 21 an upper claw and a lower claw that are in contact with the outer circumferential surface and inner circumferential surface of the superconducting field coil 3, respectively. For example, it has circular through holes 20a and 21a.
22 is a helium flow path provided between the coil mounting shaft 2 and the helium outer cylinder 6, and 23 is a coil mounting shaft helium flow hole provided in communication with the liquid reservoir 15 and the bottom of the slot 17.

一般的に超電導回転電機においては、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
内の微少の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。
Generally speaking, in superconducting rotating electric 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.

次に冷却動作を第5図に基づいて説明する。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の周囲の僅かな間〓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
自然対流によつて下部つめもの21の貫通孔21
aを通り抜け、コイル取付軸2のヘリウム流通孔
23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22からウエツジ19の〓間及び上部つめ
もの20の貫通孔20a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、別のコイル取付軸ヘ
リウム流通孔23から下部つめもの21の貫通孔
21aを経て超電導界磁コイル3の周囲に入り込
み、さらに上部つめもの20の貫通孔20a及び
ウエツジ19の〓間を通りヘリウム流路22に出
る。
Next, the cooling operation will be explained based on FIG. 5. The heat generated by slight heat generation within the superconducting field coil 3 or by slight heat intrusion into the superconducting field coil 3 is absorbed by the helium that exists in a small space around the superconducting field coil 3. be done. The helium, which expands due to heat absorption and becomes less dense, flows through the through hole 21 of the lower cuff 21 due to the natural convection of the centrifugal force field.
a, and exits to the liquid reservoir 15 through the helium flow hole 23 of the coil mounting shaft 2. On the other hand, the helium shortage that occurs around the superconducting field coil 3 is compensated for by helium flowing from the helium channel 22 into the area around the superconducting field coil 3 through the gap between the wedges 19 and the through hole 20a of the upper pawl 20. be exposed.
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 through the helium flow hole 23 of another coil mounting shaft, through the through hole 21a of the lower pawl 21, and further into the through hole 20a of the upper pawl 20 and the bottom of the wedge 19. It exits to the helium flow path 22 through the gap.

以上のように円滑な自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 self-circulation as described above, the superconducting field coil 3 is cooled, and the superconducting field coil 3 is kept below the superconducting transition temperature.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来の超電導回転電機の回転子では、上部つめ
もの20、下部つめもの21の貫通孔20a,2
0aが半径方向のみで、それらの軸方向の間隔も
広いため、超電導界磁コイル3上のこれら貫通孔
20a,20a近傍と、これら貫通孔20a,2
0aから遠く離れた場所とでは、第5図に示すよ
うにヘリウム流路の長さに大きな差が生じる。従
つて、もし貫通孔20a,20aから遠く離れた
場所において、微少発熱又は僅かな熱侵入が生じ
た場合は、熱を吸収したヘリウムはコイル取付軸
ヘリウム流通孔23へ逃げにくくなり、この場所
の超電導界磁コイル3の温度が上昇し、容易に超
電導臨界温度を越えて、クエンチに至るという問
題点があつた。
In the rotor of a conventional superconducting rotating electric machine, the through holes 20a, 2 of the upper pawl 20 and the lower pawl 21 are
0a is only in the radial direction and the distance between them in the axial direction is wide.
As shown in FIG. 5, there is a large difference in the length of the helium flow path at a location far away from 0a. Therefore, if slight heat generation or slight heat intrusion occurs in a place far away from the through holes 20a, 20a, the helium that has absorbed the heat will be difficult to escape to the coil mounting shaft helium flow hole 23, and the helium at this location will be There was a problem in that the temperature of the superconducting field coil 3 rose and easily exceeded the superconducting critical temperature, leading to 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、超電導界磁コイルの熱除去を
円滑に行ない、超電導界磁コイルの性能を向上で
きる超電導回転電機の回転子を得ることを目的と
する。
This invention was made to solve the above-mentioned problems, and aims to provide a rotor for a superconducting rotating electrical machine that can smoothly remove heat from a superconducting field coil and improve the performance of the superconducting field coil. purpose.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る超電導回転電機の回転子は、上
部つめものの超電導界磁コイルに接しない面に形
成された軸方向に延びる流路と幅方向に延びる流
路とを有する第1の流路溝と、この第1の流路溝
の軸方向に延びる流路と幅方向に延びる流路とに
複数形成された第1の小孔と、下部つめものの超
電導界磁コイルに接する面に形成された軸方向に
延びる流路と幅方向に延びる流路とを有する第2
の流路溝と、この第2の流路溝の軸方向に延びる
流路と幅方向に延びる流路とに複数形成された第
2の小孔とを備えたものである。
The rotor of a superconducting rotating electric machine according to the present invention has a first channel groove having a channel extending in the axial direction and a channel extending in the width direction, which is formed on a surface of the upper part of the nail not in contact with the superconducting field coil. , a plurality of first small holes formed in a channel extending in the axial direction and a channel extending in the width direction of the first channel groove, and an axis formed in a surface of the lower parting that is in contact with the superconducting field coil. a second channel having a channel extending in the direction and a channel extending in the width direction;
, and a plurality of second small holes formed in a channel extending in the axial direction and a channel extending in the width direction of the second channel groove.

〔作用〕[Effect]

この発明における超電導回転電機の回転子は、
上部つめものに形成した第1の流路溝、第1の小
孔及び下部つめものに形成した第2の流路溝、第
2の小孔により、ヘリウムの流通が軸方向、幅方
向において良くなり超電導界磁コイルの熱除去を
円滑に行え、超電導界磁コイルの性能が向上す
る。
The rotor of the superconducting rotating electrical machine in this invention is
The first flow groove and first small hole formed in the upper pawl and the second flow groove and second small hole formed in the lower pawl allow helium to flow well in the axial and width directions. Therefore, heat can be smoothly removed from the superconducting field coil, and the performance of the superconducting field coil is improved.

〔実施例〕〔Example〕

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2図において、2,3,6,1
5,16,19,22,23は上述した従来の回
転子の構成と同様である。24は超電導界磁コイ
ル3の外周面に接する上部つめもの、25は上部
つめもの24の超電導界磁コイル3と接する面に
形成された軸方向に延びる流路および超電導界磁
コイル3の幅方向に延びる流路から構成された第
1の流路溝、26は第1の流路溝25に複数形成
された第1の小孔であり、ウエツジ19間の〓間
に相対向する部分にも形成されている。27は超
電導界磁コイル3の内周面に接する下部つめも
の。28は下部つめもの27の超電導界磁コイル
3と接する面に形成された軸方向に延びる流路お
よび超電導界磁コイル3の幅方向に延びる流路か
ら構成された第2の流路溝、29は第2の流路溝
28に複数形成された第2の小孔であり、コイル
取付軸ヘリウム流通孔23と相対向する部分にも
形成されている。
An embodiment of the present invention will be described below with reference to the drawings. In Figures 1 and 2, 2, 3, 6, 1
5, 16, 19, 22, and 23 have the same structure as the conventional rotor described above. 24 is an upper pawl in contact with the outer peripheral surface of the superconducting field coil 3; 25 is a channel extending in the axial direction formed on the surface of the upper pawl 24 in contact with the superconducting field coil 3, and in the width direction of the superconducting field coil 3; The first flow groove 26 is a plurality of first small holes formed in the first flow groove 25, and the first flow groove 26 is a plurality of first small holes formed in the first flow groove 25. It is formed. 27 is a lower pawl that is in contact with the inner peripheral surface of the superconducting field coil 3. Reference numeral 28 denotes a second channel groove 29 formed of a channel extending in the axial direction and a channel extending in the width direction of the superconducting field coil 3 formed on the surface of the lower pawl 27 in contact with the superconducting field coil 3; A plurality of second small holes are formed in the second flow path groove 28, and are also formed in a portion facing the coil mounting shaft helium flow hole 23.

次い動作について説明する。超電導界磁コイル
3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の周囲の僅かな間〓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
下部つめもの27の第2の小孔29に入り、下部
つめもの27の第2の流路溝28を通つてコイル
取付軸ヘリウム流通孔23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、ヘルウム流路22からウエツジ1
9の〓間及び上部つめもの24の第1の流路溝2
5を通り、上部つめもの24の第1の小孔26を
経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
コイル取付軸ヘリウム流通孔23から下部つめも
の27の第2の流路溝28を通り、下部つめもの
27の第2の小孔29を経て超電導界磁コイル3
の周囲に入り込み、さらに上部つめもの24の第
1の小孔26、第1の流路溝25及びウエツジ1
9の〓間を通りヘリウム流路22に出る。このよ
うに円滑な自然循環を行うことにより、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。
Next, the operation will be explained. The heat generated by the slight heat generated by the superconducting field coil 3 or by a slight amount of heat entering the superconducting field coil 3 is absorbed by the helium that exists in a small space around the superconducting field coil 3. Ru. The helium, which expands due to heat absorption and has a lower density, enters the second small hole 29 of the lower cuff 27 by natural convection of the centrifugal force field, and passes through the second flow channel groove 28 of the lower cuff 27. The coil mounting shaft exits to the liquid reservoir 15 through the helium flow hole 23. On the other hand, the helium shortage occurring around the superconducting field coil 3 causes the helium flow path 22 to
9 and the first channel groove 2 of the upper pawl 24
5 and flowing around the superconducting field coil 3 through the first small hole 26 of the upper pawl 24. The endothermically expanded helium is cooled in the liquid reservoir 15 by partially evaporating it. The cooled helium passes from the helium flow hole 23 on another coil mounting shaft through the second flow groove 28 of the lower pawl 27, passes through the second small hole 29 of the lower pawl 27, and enters the superconducting field coil 3.
The first small hole 26 of the upper pawl 24, the first channel groove 25 and the wedge 1
9 and exits to the helium flow path 22. By performing smooth natural circulation in this manner, the superconducting field coil 3 is cooled, and the superconducting field coil 3 is kept below the superconducting transition temperature.

〔発明の効果〕〔Effect of the invention〕

この発明は以上説明した通り、上部つめものの
超電導界磁コイルに接する面に形成された軸方向
に延びる流路と幅方向に延びる流路とを有する第
1の流路溝と、この第1の流路溝の軸方向に延び
る流路と幅方向に延びる流路とに複数形成された
第1の小孔と、下部つめものの超電導界磁コイル
に接する面に形成された軸方向に延びる流路と幅
方向に延びる流路とを有する第2の流路溝と、こ
の第2の流路溝の軸方向に延びる流路と幅方向に
延びる流路とに複数形成された第2の小孔とを備
えているので、ヘリウムの流通が軸方向、幅方向
において良くなり超電導界磁コイルの熱除去を円
滑に行え、超電導界磁コイルの性能向上が図れる
超電導回転電機の回転子を得ることができる。
As explained above, the present invention includes a first channel groove having a channel extending in the axial direction and a channel extending in the width direction, which is formed on the surface of the upper nail that is in contact with the superconducting field coil; A plurality of first small holes are formed in the axially extending channel and the widthwise channel of the channel groove, and the axially extending channel is formed in the surface of the lower parting that is in contact with the superconducting field coil. a second channel groove having a channel extending in the width direction; and a plurality of second small holes formed in the channel extending in the axial direction and the channel extending in the width direction of the second channel groove. Therefore, it is possible to obtain a rotor for a superconducting rotating electrical machine that improves helium flow in the axial and width directions, allows smooth heat removal from the superconducting field coil, and improves the performance of the superconducting field coil. can.

【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超電導回転
電機の回転子におけるヘリウムの流れを示す断面
図、第2図はこの発明に係わる上部つめもの、下
部つめものを示す平面図、第3図は一般的な超電
導回転電機の回転子の全体概念を示す断面図、第
4図は第3図−線における断面図、第5図は
従来の超電導回転電機の回転子におけるヘリウム
の流れ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、17はスロツト、24は上部つめも
の、25は第1の流路溝、26は第1の小孔、2
7は下部つめもの、28は第2の流路溝、29は
第2の小孔である。尚、図中同一符号は同一又は
相当部分を示す。
FIG. 1 is a sectional view showing the flow of helium in the rotor of a superconducting rotating electrical machine according to an embodiment of the present invention, FIG. 2 is a plan view showing the upper and lower parts of the invention, and FIG. A cross-sectional view showing the overall concept of the rotor of a general superconducting rotating electric machine, Fig. 4 is a cross-sectional view along the line shown in Fig. 3, and Fig. 5 is a cross-sectional view showing the flow of helium in the rotor of a conventional superconducting rotating electric machine. It is. In the figure, 2 is a coil mounting shaft, 3 is a superconducting field coil, 17 is a slot, 24 is an upper pawl, 25 is a first channel groove, 26 is a first small hole, 2
7 is a lower pawl, 28 is a second channel groove, and 29 is a second small hole. Note that the same reference numerals in the figures indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 1 コイル取付軸に設けられたスロツト内に収納
される超電導界磁コイル、この超電導界磁コイル
の外周面、内周面にそれぞれ接する上部つめも
の、下部つめものを備えたものにおいて、上記上
部つめものの上記超電導界磁コイルに接する面に
形成された軸方向に延びる流路と幅方向に延びる
流路とを有する第1の流路溝、この第1の流路溝
の軸方向に延びる流路と幅方向に延びる流路とに
複数形成された第1の小孔、上記下部つめものの
上記超電導界磁コイルに接する面に形成された軸
方向に延びる流路と幅方向に延びる流路とを有す
る第2の流路溝、この第2の流路溝の軸方向に延
びる流路と幅方向に延びる流路とに複数形成され
た第2の小孔を備えたことを特徴とする超電導回
転電機の回転子。
1. In a superconducting field coil housed in a slot provided in a coil mounting shaft, and an upper claw and a lower claw that are in contact with the outer circumferential surface and inner circumferential surface of the superconducting field coil, respectively, the above-mentioned upper claw a first channel groove having an axially extending channel and a widthwise channel formed on a surface in contact with the superconducting field coil; a channel extending in the axial direction of the first channel groove; and a plurality of first small holes formed in a channel extending in the width direction, a channel extending in the axial direction formed in a surface of the lower pawl that is in contact with the superconducting field coil, and a channel extending in the width direction. A superconducting rotation characterized by comprising: a second passage groove having a second passage groove, and a plurality of second small holes formed in a passage extending in the axial direction and a passage extending in the width direction of the second passage groove. Electric machine rotor.
JP61056321A 1986-03-12 1986-03-12 Rotor of superconducting rotating electric machine Granted JPS62213556A (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP61056321A JPS62213556A (en) 1986-03-12 1986-03-12 Rotor of superconducting rotating 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
JP61056321A JPS62213556A (en) 1986-03-12 1986-03-12 Rotor of superconducting rotating electric machine

Publications (2)

Publication Number Publication Date
JPS62213556A JPS62213556A (en) 1987-09-19
JPH0524746B2 true JPH0524746B2 (en) 1993-04-08

Family

ID=13023904

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61056321A Granted JPS62213556A (en) 1986-03-12 1986-03-12 Rotor of superconducting rotating electric machine

Country Status (1)

Country Link
JP (1) JPS62213556A (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4282450A (en) * 1979-09-25 1981-08-04 Westinghouse Electric Corp. Dynamoelectric machine with cryostable field winding
JPS57162945A (en) * 1981-03-31 1982-10-06 Mitsubishi Electric Corp Rotor for superconductive rotary electric machine
JPS57202851A (en) * 1981-06-05 1982-12-11 Mitsubishi Electric Corp Rotor for superconductive rotary electric machine

Also Published As

Publication number Publication date
JPS62213556A (en) 1987-09-19

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