JPH0789741B2 - Superconducting rotating electric machine rotor - Google Patents
Superconducting rotating electric machine rotorInfo
- Publication number
- JPH0789741B2 JPH0789741B2 JP61056325A JP5632586A JPH0789741B2 JP H0789741 B2 JPH0789741 B2 JP H0789741B2 JP 61056325 A JP61056325 A JP 61056325A JP 5632586 A JP5632586 A JP 5632586A JP H0789741 B2 JPH0789741 B2 JP H0789741B2
- Authority
- JP
- Japan
- Prior art keywords
- rotor
- helium
- upper insulator
- outer peripheral
- peripheral side
- 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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- Windings For Motors And Generators (AREA)
- 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。The present invention relates to the structure of a rotor of a superconducting rotating electric machine.
第7図,第8図は、例えば特開昭57−202852号公報に示
された従来の回転子を示す断面図である。図において、
(1)はコイル取付軸、(2)はコイル取付軸(1)に
設けられたヘリウム蒸気空間、(3)は液体ヘリウム溜
り、(4)はコイル取付軸(1)に設けられたスロツ
ト、(5)はスロツト(4)内に収納された超電導界磁
コイル、(6a)は超電導界磁コイル(5)の反ヘリウム
蒸気空間側に配設された上部絶縁物、(6b)は上部絶縁
物(6a)以外のスロツト内絶縁物、(7)はウエツジ、
(8)はヘリウム外筒、(9)はコイル取付軸(1)と
ヘリウム外筒(8)の間に設けられたヘリウム流路、
(10)は液体ヘリウム溜り(3)とスロツト(4)とに
連通して設けられた取付軸ヘリウム流路孔、(11a)は
上部絶縁物(6a)に形成された例えば円形状の貫通孔、
(11b)は上部絶縁物(6a)以外の絶縁物(6b)に形成
された例えば円形状の貫通孔である。7 and 8 are sectional views showing a conventional rotor disclosed in, for example, Japanese Patent Laid-Open No. 57-202852. In the figure,
(1) is a coil mounting shaft, (2) is a helium vapor space provided on the coil mounting shaft (1), (3) is a liquid helium reservoir, (4) is a slot provided on the coil mounting shaft (1), (5) is a superconducting field coil housed in the slot (4), (6a) is an upper insulator arranged on the antihelium vapor space side of the superconducting field coil (5), and (6b) is an upper insulating layer. Insulator in slot other than item (6a), (7) wedge,
(8) is a helium outer cylinder, (9) is a helium flow path provided between the coil mounting shaft (1) and the helium outer cylinder (8),
(10) is a mounting shaft helium passage hole provided in communication with the liquid helium reservoir (3) and the slot (4), and (11a) is, for example, a circular through hole formed in the upper insulator (6a). ,
(11b) is, for example, a circular through hole formed in the insulator (6b) other than the upper insulator (6a).
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
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。Generally, in a superconducting rotating electric machine, there is an important technical problem in how to perform cryogenic cooling of a superconducting field coil. In order to bring the superconducting field coil into the superconducting state, it is necessary to cool it to a temperature below the superconducting transition temperature, and at present, helium is kept at an absolute temperature of 1K to 20K as a cooling medium. On the other hand, in such an extremely low temperature state, the specific heat of the superconducting field coil is extremely small.Therefore, a slight heat generation in the superconducting field coil or a small amount of heat entering the superconducting field coil causes There is always the risk that the temperature of the coil will rise and exceed the superconducting transition temperature. Therefore, it is important for the design of a superconducting rotating electric machine how to quickly remove the minute heat generation in the superconducting field coil or the small amount of heat entering the superconducting field coil to suppress the temperature rise of the superconducting field coil. It will be a point.
次に冷却動作について説明する。超電導界磁コイル
(5)内の微少発熱,あるいは超電導界磁コイル(5)
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(5)の外周側の絶縁物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、遠心力揚の自然対流によつて絶縁
物(6b)の貫通孔(11b)を通り抜け、コイル取軸
(1)のヘリウム流路孔(10)を経て液体ヘリウム溜り
(3)に出る。一方、超電導界磁コイル(5)回りで生
ずるヘリウム不足は、ヘリウム流路(9)からウエツジ
(7)の隙間及び上部絶縁物(6a)の貫通孔(6a)を通
つて超電導界磁コイル(5)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、液体ヘリウ
ム溜り(3)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
路孔(10)から絶縁物(6b)の貫通孔(11b)を経て超
電導界磁コイル(5)の周囲に入り込み、さらに上部絶
縁物(6a)の貫通孔(11a)及びウエツジ(7)の隙間
を通りヘリウム流路(9)に出る。Next, the cooling operation will be described. Minute heat generation in the superconducting field coil (5) or superconducting field coil (5)
The heat generated by the slight heat penetration into the superconducting field coil (5) is absorbed by the helium present in the slight gap with the insulator on the outer peripheral side of the superconducting field coil (5). Helium that has expanded in density and decreased in density due to heat absorption passes through the through hole (11b) in the insulator (6b) by natural convection due to centrifugal force, and then passes through the helium flow path hole (10) in the coil take-up shaft (1). Pass through the liquid helium pool (3). On the other hand, the helium shortage that occurs around the superconducting field coil (5) passes through the gap between the helium flow path (9) and the wedge (7) and the through hole (6a) of the upper insulator (6a), and 5) Supplemented by helium flowing in around. The heat-expanded helium is cooled by evaporating a part of it in the liquid helium pool (3). The cooled helium enters the periphery of the superconducting field coil (5) from another helium channel hole (10) through the through hole (11b) of the insulator (6b), and further penetrates the upper insulator (6a). It passes through the gap between the hole (11a) and the wedge (7) and exits into the helium channel (9).
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(5)の冷却が行なわれ、超電導界磁コイ
ル(5)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 (5) is cooled, and the superconducting field coil (5) is maintained at the superconducting transition temperature or lower.
超電導状態では超電導界磁コイル(5)に電圧はほとん
ど発生しないが、超電導状態が破壊されると数百ないし
1000V程度の電圧が発生するので、この電圧で絶縁破壊
されないように十分な絶縁を施しておく必要がある。In the superconducting state, almost no voltage is generated in the superconducting field coil (5), but if the superconducting state is destroyed, several hundreds or
Since a voltage of about 1000V is generated, it is necessary to provide sufficient insulation so that this voltage will not cause dielectric breakdown.
従来の回転子では第7図,第8図に示すように、超電導
界磁コイル(5)をコイル取付軸(1)のスロツト
(4)内に収納し、超電導界磁コイル(5)の周囲に絶
縁物を配置している。また、超電導界磁コイル(5)を
冷却するヘリウムを流通させる為、上部絶縁物(6a)に
孔(11a)をあけてその流路としなければならない、し
かし、孔(11a)をあけた部分では絶縁性能が低下する
ことになる。このことに対する解決策としては、上部絶
縁物(6a)の厚みを厚くし、充分な絶縁距離をとる方法
が考えられるが、絶縁物がスロツト(4)内に占める容
積はかなりのものとなる。従つて、その容積分だけスロ
ツト(4)内の他の部品を小さくしなければならず、特
に超電導界磁コイル(5)の容積を小さくするというこ
とは超電導界磁コイル(5)容量の低下につなかり、性
能上大きな問題となる。あるいは絶縁物外のスロツト
(4)内部品を同一容積にすれば、上部絶縁物(6a)の
厚みを増した分だけスロツト(4)の深さを深く製作し
なければならず効率的でない。In the conventional rotor, as shown in FIGS. 7 and 8, the superconducting field coil (5) is housed in the slot (4) of the coil mounting shaft (1) to surround the superconducting field coil (5). Insulators are placed on. In order to circulate helium that cools the superconducting field coil (5), a hole (11a) must be formed in the upper insulator (6a) to form the flow path, but the part where the hole (11a) is formed. Then, the insulation performance will decrease. As a solution to this, a method of increasing the thickness of the upper insulator (6a) and providing a sufficient insulation distance can be considered, but the volume occupied by the insulator in the slot (4) becomes considerable. Therefore, the other parts in the slot (4) must be made smaller by the volume thereof, and particularly making the volume of the superconducting field coil (5) smaller means that the capacity of the superconducting field coil (5) decreases. It becomes a big problem in terms of performance. Alternatively, if the parts inside the slot (4) outside the insulator are made to have the same volume, the depth of the slot (4) must be made deeper by an amount corresponding to the increased thickness of the upper insulator (6a), which is not efficient.
この発明は上記のような問題点を解消する為になされた
ものであり、超電導界磁コイル容量を低下させず且つス
ロツトの深さを必要以上に深く製作せずに、絶縁距離の
増大を可能にすることを目的とする。The present invention has been made to solve the above problems, and it is possible to increase the insulation distance without decreasing the superconducting field coil capacity and without making the slot depth deeper than necessary. The purpose is to
この発明に係る回転子は、超電導界磁コイルの外周側に
接する上部絶縁物を2分割し、2分割した上部絶縁物の
内周側上部絶縁物の外周側に軸方向ヘリウム流路溝およ
び円周方向ヘリウム流路溝を設け、外周側と内周側の上
部絶縁物に設けた半径方向ヘリウム流路孔を軸方向にづ
らせた位置に設けたものである。A rotor according to the present invention has an upper insulator that is in contact with an outer peripheral side of a superconducting field coil, is divided into two, and an inner peripheral side of the upper divided insulator is divided into two parts. Circumferential helium flow passage grooves are provided, and radial helium flow passage holes provided in the outer insulator and the inner peripheral side upper insulator are provided at positions axially aligned with each other.
この発明においては、上部絶縁物を2分割し、内周側上
部絶縁物の外周側に、軸方向ヘリウム流路溝および円周
方向ヘリウム流路溝を設けるとともに、円周方向ヘリウ
ム流路溝に連通する半径方向ヘリウム流路孔を設けてい
るので、外周側上部絶縁物の半径方向ヘリウム流路孔を
通って流入するヘリウムは軸方向ヘリウム流路溝および
円周方向ヘリウム流路溝により全域に亙って効率よく拡
散され、内周側上部絶縁物の半径方向ヘリウム流路孔を
通って超電導界磁コイルの全面に均一に供給できる。さ
らに、上部絶縁物の半径方向ヘリウム流路孔を軸方向に
づらせた位置に設けることによつて、絶縁距離を増大さ
せることができるので、スロツト内の絶縁物の厚みの増
加を抑制することができる。In the present invention, the upper insulator is divided into two, and the axial helium channel groove and the circumferential helium channel groove are provided on the outer peripheral side of the inner peripheral side upper insulator, and the circumferential helium channel groove is formed. Since the radial helium flow passages that communicate with each other are provided, the helium that flows in through the radial helium flow passage holes on the outer peripheral side upper insulating material is entirely covered by the axial helium flow passage groove and the circumferential helium flow passage groove. It is efficiently diffused and can be uniformly supplied to the entire surface of the superconducting field coil through the helium flow passage holes in the radial direction of the upper insulator on the inner circumference side. Further, by providing the radial helium flow passage holes in the upper insulator at positions axially offset from each other, the insulation distance can be increased, so that the increase in the thickness of the insulator in the slot can be suppressed. You can
〔実施例〕 以下に、この発明の一実施例における超電導回転電機の
回転子の構成を、第1図ないし第6図に基づいて説明す
る。第1図,第2図の(1)〜(5),(6b),(7)
〜(10),(11b)は、上記従来の回転子の構成と同様
のものである。第1図において(6c)は超電導界磁コイ
ル(5)の外周側に取付けられた、2分割されたうちの
内周側の上部絶縁物、(6d)は2分割されたうちの外周
側の上部絶縁物である。第2図において、(6c)は内周
側上部絶縁物、(6d)は外周側上部絶縁物、(11c)は
前記内周側上部絶縁物(6c)に設けられ、前記超電導界
磁コイル(5)を冷却した液体ヘリウムが流れるように
設けられた半径方向ヘリウム流路孔、即ち、第1の冷媒
流路孔である。(11d)は前記内周側上部絶縁物(6c)
に設けられ前記内周側上部絶縁物(6c)の半径方向ヘリ
ウム流路孔(11c)とつながる軸方向ヘリウム流路溝、
即ち第2の冷媒流路溝である。(11e)は前記内周側上
部絶縁物(6c)に設けられ、前記軸方向ヘリウム流路溝
(11d)と交差し、前記内周側上部絶縁物(6c)のヘリ
ウム流路孔(11c)とつながる位置の円周方向に設けら
れた円周方向ヘリウム流路溝、即ち第1の冷媒流路溝で
ある。(11f)は前記外周側上部絶縁物(6d)の前記内
周側上部絶縁物(6c)の円周方向ヘリウム流路溝(11
e)と軸方向にづれた位置に設けられた半径方向流路
孔、即ち第2の冷媒流路孔である。(11g)はウエツジ
(7)の前記外周側上部絶縁物(6d)に設けられた半径
方向ヘリウム流路孔(11f)と連通する位置に設けられ
たヘリウム流路孔、即ち第3の冷媒流路孔である。第3
図ないし第6図は第1図,第2図の理解を助けるための
図である。[Embodiment] The configuration of the rotor of the superconducting rotary electric machine according to an embodiment of the present invention will be described below with reference to FIGS. 1 to 6. 1 and 2 (1) to (5), (6b), (7)
(10) and (11b) have the same structure as the conventional rotor. In FIG. 1, (6c) is an upper insulator attached to the outer peripheral side of the superconducting field coil (5) on the inner peripheral side of the two parts, and (6d) is an outer peripheral side of the two divided parts. It is an upper insulator. In FIG. 2, (6c) is provided on the inner peripheral side upper insulator, (6d) is provided on the outer peripheral side upper insulator, (11c) is provided on the inner peripheral side upper insulator (6c), and the superconducting field coil ( 5) is a radial helium flow channel hole provided so that liquid helium that has cooled 5), that is, a first coolant flow channel hole. (11d) is the inner peripheral upper insulator (6c)
An axial helium channel groove connected to the radial helium channel hole (11c) of the inner peripheral upper insulator (6c),
That is, the second coolant channel groove. (11e) is provided in the inner peripheral side upper insulator (6c), intersects with the axial helium flow channel groove (11d), and is a helium flow channel hole (11c) in the inner peripheral side upper insulator (6c). It is a circumferential helium channel groove provided in the circumferential direction at a position connected to, that is, a first refrigerant channel groove. (11f) is a circumferential helium channel groove (11) of the inner peripheral upper insulation (6c) of the outer peripheral upper insulation (6d).
e) A radial flow passage hole, that is, a second coolant flow passage hole provided at a position axially separated from e). (11g) is a helium flow passage hole provided at a position communicating with the radial helium flow passage hole (11f) provided in the outer peripheral upper insulator (6d) of the wedge (7), that is, the third refrigerant flow. It is a road hole. Third
FIGS. 1 to 6 are views for helping understanding of FIGS. 1 and 2.
上記のように構成された回転子は、ウェッジ(7)から
ヘリウム流路孔(11g)を通って流入するヘリウムは、
外周側上部絶縁物(6d)の半径方向ヘリウム流路孔(11
f)を通って内周側上部絶縁物(6c)の外周側に流入す
る。そこで、軸方向ヘリウム流路溝(11d)内を通って
各円周方向ヘリウム流路溝(11e)に流入する。さら
に、半径方向ヘリウム流路孔(11c)を通って超電導界
磁コイル5に供給される。したがって、ヘリウムは、軸
方向ヘリウム流路溝(11d)および円周方向ヘリウム流
路溝(11e)により内周側上部絶縁物(6c)の外周側全
域に効率よく拡散され、半径方向ヘリウム流路孔(11
c)から超電導界磁コイル(5)の全面に亙って均一に
供給される。その結果、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を向上できる。ま
た、内周側上部絶縁物(6c)の円周方向ヘリウム流路溝
(11e)と外周側上部絶縁物(6d)の半径方向ヘリウム
流路孔(11f)を軸方向にづらせていることが絶縁距離
すなわち、超電導界磁コイル(5)から内周側上部絶縁
物(6c)に設けられた半径方向ヘリウム流路孔(11
c)、円周方向ヘリウム流路溝(11e)の壁面を経て、上
記内周側上部絶縁物(6c)の外周面の上記円周方向ヘリ
ウム流路溝(11e)と上記半径方向ヘリウム流路孔(11
f)の軸方向のづれた距離を経て、上記外周側上部絶縁
物(6d)の半径方向ヘリウム流路孔(11f)の壁面を通
りエツジ(7)至る距離を増大させるので、その分上部
絶縁物は薄いものでよくなる。従つて、上部絶縁物とそ
れ以外の絶縁物(6d)のスロツト内に占める容積の割合
は減少し、逆に超電導界磁コイル(5)の容積を増すこ
とができるので超電導界磁コイル容量の増加が可能とな
る。In the rotor configured as described above, the helium flowing from the wedge (7) through the helium passage hole (11g) is
Radial helium flow passage hole (11
It flows through f) to the outer peripheral side of the inner peripheral upper insulator (6c). Then, it passes through the axial helium channel groove (11d) and flows into each circumferential helium channel groove (11e). Further, it is supplied to the superconducting field coil 5 through the radial helium flow passage hole (11c). Therefore, the helium is efficiently diffused by the axial helium flow channel groove (11d) and the circumferential helium flow channel groove (11e) to the entire outer peripheral side of the inner peripheral upper insulator (6c), and the radial helium flow channel is formed. Hole (11
It is uniformly supplied from c) over the entire surface of the superconducting field coil (5). As a result, the heat of the superconducting field coil can be smoothly removed, and the performance of the superconducting field coil can be improved. In addition, the circumferential helium channel groove (11e) of the inner peripheral upper insulator (6c) and the radial helium channel hole (11f) of the outer peripheral upper insulator (6d) are axially aligned. Is the insulation distance, that is, the radial helium flow passage hole (11) provided in the upper insulation (6c) on the inner circumference side from the superconducting field coil (5).
c), through the wall surface of the circumferential helium flow channel (11e), the circumferential helium flow channel (11e) and the radial helium flow channel on the outer peripheral surface of the inner peripheral side upper insulator (6c) Hole (11
The distance to the edge (7) through the wall surface of the radial direction helium flow passage hole (11f) of the outer peripheral side upper insulator (6d) is increased through the axial distance of (f). Things are better with thin things. Therefore, the ratio of the volume occupied by the upper insulator and the other insulator (6d) in the slot decreases, and conversely the volume of the superconducting field coil (5) can be increased. It is possible to increase.
この発明は以上説明した通り上部絶縁物を2分割し、内
周側上部絶縁物の外周側に、軸方向ヘリウム流路溝およ
び円周方向ヘリウム流路溝を設けるとともに、円周方向
ヘリウム流路溝に連通する半径方向ヘリウム流路孔を設
けているので、外周側上部絶縁物の半径方向ヘリウム流
路孔を通って流入するヘリウムは軸方向ヘリウム流路溝
および円周方向ヘリウム流路溝により全域に亙って効率
よく拡散され、内周側上部絶縁物の半径方向ヘリウム流
路孔を通って超電導界磁コイルの全面に均一に供給で
き、超電導コイルの熱除去を円滑に行うことができる。
さらに、上部絶縁物の半径方向ヘリウム流路孔を軸方向
にづらせた位置に設けることにより、絶縁距離を増大さ
せ超電導界磁コイル容量の増大を可能とし、また絶縁物
の耐電圧の増加を可能にした超電導回転電機の回転子を
提供することができる。According to the present invention, as described above, the upper insulator is divided into two, and the axial helium channel groove and the circumferential helium channel groove are provided on the outer peripheral side of the inner peripheral side upper insulator, and the circumferential helium channel is provided. Since the radial helium flow passage that communicates with the groove is provided, the helium that flows in through the radial upper helium flow passage of the outer peripheral side insulating material is generated by the axial helium flow passage groove and the circumferential helium flow passage groove. Efficiently diffuses over the entire area, can be uniformly supplied to the entire surface of the superconducting field coil through the radial helium flow passage hole of the inner peripheral upper insulator, and the heat of the superconducting coil can be smoothly removed. .
Furthermore, by providing radial helium flow passage holes in the upper insulator at axially spaced positions, it is possible to increase the insulation distance, increase the superconducting field coil capacity, and increase the withstand voltage of the insulator. It is possible to provide the rotor of the superconducting rotating electric machine that is enabled.
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
転子を示す断面図、第2図は第1図のスロツト頂部付近
の断面側面図、第3図,第4図はそれぞれこの発明に係
る内周側上部絶縁物の正面図と断面側面図、第5図,第
6図はそれぞれこの発明に係る外周側上部絶縁物の正面
図と断面側面図、第7図は従来の超電導回転電機の回転
子の断面図、第8図は第7図のスロツト頂部付近の詳細
図である。 図において、(1)はコイル取付軸、(4)はスロツ
ト、(5)は超電導界磁コイル、(6c)は内周側上部絶
縁物、(6d)は外周側上部絶縁物、(7)はウエツジ、
(11c)は半径方向ヘリウム流路孔、(11d)は軸方向ヘ
リウム流路溝、(11e)は円周方向ヘリウム流路溝、(1
1f)は半径方向ヘリウム流路孔、(11g)はヘリウム流
路孔である。 なお、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 a rotor of a superconducting rotating electric machine according to an embodiment of the present invention, FIG. 2 is a sectional side view of the vicinity of the slot top portion of FIG. 1, and FIGS. A front view and a cross-sectional side view of the inner peripheral side upper insulating material, FIGS. 5 and 6 are a front view and a cross-sectional side view of the outer peripheral side upper insulating material according to the present invention, and FIG. 7 is a conventional superconducting rotating electric machine. FIG. 8 is a sectional view of the rotor of FIG. 8, and FIG. 8 is a detailed view near the slot top portion of FIG. In the figure, (1) is a coil mounting shaft, (4) is a slot, (5) is a superconducting field coil, (6c) is an inner peripheral upper insulation, (6d) is an outer peripheral upper insulation, and (7). Is a wedge,
(11c) is a radial helium flow channel hole, (11d) is an axial helium flow channel groove, (11e) is a circumferential helium flow channel groove, (1
1f) is a radial helium channel hole, and (11g) is a helium channel hole. The same reference numerals in the drawings indicate the same or corresponding parts.
───────────────────────────────────────────────────── フロントページの続き (72)発明者 前田 進 兵庫県神戸市兵庫区和田崎町1丁目1番2 号 三菱電機株式会社神戸製作所内 (72)発明者 大下 幸一 兵庫県神戸市兵庫区和田崎町1丁目1番2 号 三菱電機株式会社神戸製作所内 (72)発明者 平尾 俊樹 兵庫県神戸市兵庫区和田崎町1丁目1番2 号 三菱電機株式会社神戸製作所内 (72)発明者 内田 満広 兵庫県神戸市兵庫区和田崎町1丁目1番2 号 三菱電機株式会社神戸製作所内 (56)参考文献 特開 昭56−56168(JP,A) 特開 昭57−162945(JP,A) 特開 昭57−202851(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Susumu Maeda 1-2-2 Wadazakicho, Hyogo-ku, Kobe-shi, Hyogo Mitsubishi Electric Corporation Kobe Works (72) Inventor Koichi Oshita Hyogo-ku, Kobe-shi, Hyogo 1-2-2 Wadazakicho Mitsubishi Electric Co., Ltd. Kobe Works (72) Inventor Toshiki Hirao 1-2-2 Wadazakicho, Hyogo-ku, Kobe Hyogo Prefecture Mitsubishi Electric Co., Ltd. (72) Inventor Mitsuhiro Uchida 1-2-1, Wadasaki-cho, Hyogo-ku, Kobe-shi, Hyogo Mitsubishi Electric Corporation Kobe Works (56) Reference JP-A-56-56168 (JP, A) JP-A-57-162945 (JP, A) ) JP-A-57-202851 (JP, A)
Claims (1)
けたスロット中に収納された超電導コイル、 該超電導コイルの回転子外周側に接して設けられた内周
側上部絶縁物、 この内周側上部絶縁物の外側に接して設けられた外周側
上部絶縁物、 該外周側上部絶縁物の外周側に接するウェッジ、 前記内周側上部絶縁物の外周面に回転子円周方向に設け
た複数の第1の冷媒流路溝、 該第1の冷媒流路溝と交差し前記内周側上部絶縁物の外
周面中央部に回転子軸方向に設けた第2の冷媒流路溝、 を有する超電導回転電機の回転子において、 前記内周側上部絶縁物を回転子半径方向に貫通し前記複
数の第1の冷媒流路溝の各々の位置に設けた複数の第1
の冷媒流路孔、 前記外周側上部絶縁物の回転子円周方向中央部を回転子
半径方向に貫通し前記第1の冷媒流路孔の位置から回転
子軸方向にずれた位置に設けた複数の第2の冷媒流路
孔、 前記ウェッジを回転子半径方向に貫通し前記第2の冷媒
流路孔と連通する位置に設けた複数の第3の冷媒流路孔 を備えたことを特徴とする超電導回転電機の回転子。1. A superconducting coil housed in a slot provided on the outer periphery of a coil mounting shaft of a rotor of a rotary electric machine, an inner peripheral upper insulator provided in contact with the outer peripheral side of the rotor of the superconducting coil, An outer peripheral upper insulator provided in contact with the outer side of the peripheral upper insulator, a wedge in contact with the outer peripheral side of the outer upper insulator, provided in the rotor circumferential direction on the outer peripheral surface of the inner upper insulator A plurality of first coolant channel grooves, a second coolant channel groove that intersects with the first coolant channel grooves and is provided in the rotor axial direction at the center of the outer peripheral surface of the inner peripheral side upper insulator, In a rotor of a superconducting rotating electric machine having a plurality of first refrigerant passage grooves which penetrate the inner peripheral side upper insulator in a rotor radial direction and are provided at respective positions of the plurality of first refrigerant passage grooves.
Of the coolant passage hole of the outer peripheral side, which penetrates through the rotor circumferential center in the rotor circumferential direction in the rotor radial direction, and is provided at a position displaced from the position of the first coolant passage hole in the rotor axial direction. A plurality of second refrigerant flow passage holes, and a plurality of third refrigerant flow passage holes provided at positions that penetrate the wedge in the rotor radial direction and communicate with the second refrigerant flow passage holes. The superconducting rotating electric machine rotor.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61056325A JPH0789741B2 (en) | 1986-03-12 | 1986-03-12 | Superconducting rotating electric machine rotor |
| 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 |
|---|---|---|---|
| JP61056325A JPH0789741B2 (en) | 1986-03-12 | 1986-03-12 | Superconducting rotating electric machine rotor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62213560A JPS62213560A (en) | 1987-09-19 |
| JPH0789741B2 true JPH0789741B2 (en) | 1995-09-27 |
Family
ID=13024027
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61056325A Expired - Fee Related JPH0789741B2 (en) | 1986-03-12 | 1986-03-12 | Superconducting rotating electric machine rotor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0789741B2 (en) |
Family Cites Families (3)
| 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 |
-
1986
- 1986-03-12 JP JP61056325A patent/JPH0789741B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62213560A (en) | 1987-09-19 |
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