JPS6010498B2 - superconducting rotor - Google Patents
superconducting rotorInfo
- Publication number
- JPS6010498B2 JPS6010498B2 JP52054658A JP5465877A JPS6010498B2 JP S6010498 B2 JPS6010498 B2 JP S6010498B2 JP 52054658 A JP52054658 A JP 52054658A JP 5465877 A JP5465877 A JP 5465877A JP S6010498 B2 JPS6010498 B2 JP S6010498B2
- Authority
- JP
- Japan
- Prior art keywords
- liquid
- torque tube
- free surface
- superconducting rotor
- superconducting
- 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
Links
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- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Motor Or Generator Cooling System (AREA)
- Superconductive Dynamoelectric Machines (AREA)
Description
【発明の詳細な説明】
本発明は、液体ヘリウム等の冷却液体で超電導界磁巻線
を冷却する超電導回転子に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a superconducting rotor that cools superconducting field windings with a cooling liquid such as liquid helium.
第1図は従来のこの種超電導回転子の概略構造を示す縦
断側面図である。液体ヘリウム等のような冷却液体1は
、超電導回転子2の外部から実線矢印で示す如く、トル
クチューブ3内に注入され、トルクチューブ3に設けら
れた多数の半径方向貫通孔4を通して、トルクチューブ
3と内側ダンパ5との間に収納された超電導界磁巻線6
等を冷却する。FIG. 1 is a vertical sectional side view showing the schematic structure of a conventional superconducting rotor of this type. A cooling liquid 1 such as liquid helium is injected from the outside of the superconducting rotor 2 into the torque tube 3 as shown by solid arrows, and is passed through a large number of radial through holes 4 provided in the torque tube 3 into the torque tube. 3 and the inner damper 5.
etc. to cool down.
この冷却液体1は、トルクチュープ3内の空間、すなわ
ち内部室7を完全に充満していないので、超電導回転子
2の回転による遠心力によって、トルクチューブ3の内
壁8に、トルクチューブ3と同0状に片寄り、液体自由
表面9が形成される。なお、冷却液体1の一部は、超電
導界磁巻線6等の熱によりペーパーとなり、点線矢印で
示す如く超電導回転子2の外部に放出させる。第2図は
、超電導回転子2の回転中におけるトルクチューブ内壁
8の半径(液体外径)aと液体自由表面9の半径(液体
内径)bとの比a/bと、液体1が入っていない場合の
危険速度の。Since this cooling liquid 1 does not completely fill the space inside the torque tube 3, that is, the internal chamber 7, the centrifugal force caused by the rotation of the superconducting rotor 2 causes the cooling liquid 1 to be applied to the inner wall 8 of the torque tube 3 in the same manner as the torque tube 3. 0, and a liquid free surface 9 is formed. Note that a part of the cooling liquid 1 becomes paper due to the heat of the superconducting field winding 6 and the like, and is discharged to the outside of the superconducting rotor 2 as shown by dotted arrows. Figure 2 shows the ratio a/b between the radius (liquid outer diameter) a of the torque tube inner wall 8 and the radius (liquid inner diameter) b of the liquid free surface 9 during rotation of the superconducting rotor 2, and the ratio a/b of the radius (liquid inner diameter) of the torque tube inner wall 8 when the superconducting rotor 2 is rotating. Dangerous speed if not.
で超電導回転子2の回転速度○を割った値○/の。との
関係を示す特性図である。この第2図において、一点鎖
線のは液体1が入っている場合の危険速度で、一般にの
/の。The value obtained by dividing the rotational speed of the superconducting rotor 2 by ○/. FIG. In this Figure 2, the dot-dashed line indicates the critical speed when liquid 1 is contained, which is generally .
である。また、2本の実線間には斜線で示された回転速
度Q/のoの領域U‘ま、液体1の挙動に趣函する不安
定振動を起こす回転速度の範囲を示す。超電導回転子2
がこの不安定領域Uで回転すると、液体自由表面9は回
転触りこ対して同D状ではなくなり、トルクチューブ内
壁8に液体1による不均合い力が作用する。しかも、こ
の不均合い力は時間と共に増大するため、超電導回転子
2はその振動振幅が増大し、非常に危険な状態となって
、ついには破損するという重大な事態に立ち至る。本発
明の目的は、上記した従来技術の問題点を解消し、不安
定振動の発生を防止して、静粛に安定した状態で回転さ
せ得る超電導回転子を提供するにある。It is. Further, between the two solid lines, a diagonally shaded region U' of rotational speed Q/o indicates a rotational speed range in which unstable vibration similar to the behavior of the liquid 1 occurs. Superconducting rotor 2
When rotates in this unstable region U, the liquid free surface 9 no longer has the same D-shape as it rotates, and an unbalanced force due to the liquid 1 acts on the torque tube inner wall 8. Moreover, as this unbalanced force increases with time, the vibration amplitude of the superconducting rotor 2 increases, resulting in a very dangerous situation, and eventually leading to a serious situation of damage. SUMMARY OF THE INVENTION An object of the present invention is to solve the problems of the prior art described above, to prevent the occurrence of unstable vibrations, and to provide a superconducting rotor that can be rotated quietly and stably.
この目的を達成するため、本発明は、トルクチューブ内
に、中空リング状の浸債部材を、その外周側部分が自由
表面を形成している冷却液体内に浸潰され、その内周側
部分が自由表面から露出する状態で設け、浸溝部材の浸
贋部分で冷却液体の自由表面を前記トルクチューブの回
転軸心側に近付け、前記浸漬部材の露出部分で前記冷却
液体の自由表面を複数に区分したことを特徴とする。To achieve this object, the present invention provides a torque tube with a hollow ring-shaped immersion member immersed in a cooling liquid with its outer circumferential side forming a free surface and its inner circumferential side is exposed from the free surface, and the immersed portion of the immersion groove member brings the free surface of the cooling liquid closer to the rotation axis side of the torque tube, and the exposed portion of the immersion member extends the free surface of the cooling liquid in plurality. It is characterized by being divided into
以下、本発明の一実施例を第3図ないし第5図について
説明する。駆動軸10および給排軸11にそれぞれ端板
12,13を介して両端が支持された外側ダンパ14の
内部に、多数の貫通孔4を有するトルクチュープ3が外
側ダンパ14と同D状に取付けられている。Hereinafter, one embodiment of the present invention will be described with reference to FIGS. 3 to 5. A torque tube 3 having a large number of through holes 4 is attached in the same D shape as the outer damper 14 inside the outer damper 14 whose both ends are supported by the drive shaft 10 and supply/discharge shaft 11 via end plates 12 and 13, respectively. It is being
このトルクチューブ3の外側には、内側ダンパ5がトル
クチューブ3と同D状に取付けられており、これらトル
クチュープ3および内側ダンパ5によって形成された界
滋巻線室15内には、超電導界磁巻線6が収納され、ト
ルクチューブ3に取付支持される。トルクチユープ3の
両端部近くには、それぞれ仕切板16,17が固定され
、この仕切板16,17、トルクチューブ3および端板
12,13によって端部室18,19が構成されている
。また、内部室7内においては、内側円筒20および外
側円筒21がトルクチューブ3と同D状になるように仕
切板16,17に取付けられており、これらの円筒20
,21には透孔22,23がそれぞれ設けられ、これら
の透孔22,23はパイプ24で接続されている。An inner damper 5 is attached to the outside of the torque tube 3 in the same D shape as the torque tube 3, and a superconducting field is formed in the field winding chamber 15 formed by the torque tube 3 and the inner damper 5. A magnetic winding 6 is housed, and is attached and supported by the torque tube 3. Partition plates 16 and 17 are fixed near both ends of the torque tube 3, respectively, and end chambers 18 and 19 are constituted by the partition plates 16 and 17, the torque tube 3, and the end plates 12 and 13. Further, in the internal chamber 7, an inner cylinder 20 and an outer cylinder 21 are attached to partition plates 16 and 17 so as to have the same D shape as the torque tube 3, and these cylinders 20
, 21 are provided with through holes 22 and 23, respectively, and these through holes 22 and 23 are connected by a pipe 24.
このパイプ24は回転軸心に対して第4図に示す如く対
称形に配置される。中空状の給擬軸11には、これと同
0状に液体ヘリウム等の冷却液体1を注入する注入パイ
プ25が取付けられ、この注入パイプ25は仕切板17
を貫通して内側円筒室26まで延び、かつその先端部に
は放射状に液体1を放出させる吐出装置27が設けられ
ている。The pipe 24 is arranged symmetrically with respect to the rotation axis as shown in FIG. An injection pipe 25 for injecting cooling liquid 1 such as liquid helium is attached to the hollow supply shaft 11 in the same shape as this, and this injection pipe 25 is connected to the partition plate 17.
A discharge device 27 is provided at the distal end of the discharge device 27 to extend through the inner cylindrical chamber 26 and discharge the liquid 1 radially.
なお、この吐出装置27は、内側円筒20および外側円
筒21を貫通し、その吐出口28はトルクチューブ3と
外側円筒21との間に形成された中間室29に閉口して
いる。駆動鞠側の仕切板16には、内側円筒室26と端
部室18を蓮適する貫通孔30が設けられ、給費E軸1
1側の仕切板17には、第5図に示す如く、内側円筒室
26と端部室19を運通する貫通孔31が注入パイプ2
5に対して対称に複数個設けられている。Note that this discharge device 27 passes through the inner cylinder 20 and the outer cylinder 21, and its discharge port 28 closes into an intermediate chamber 29 formed between the torque tube 3 and the outer cylinder 21. The partition plate 16 on the drive ball side is provided with a through hole 30 through which the inner cylindrical chamber 26 and the end chamber 18 are connected.
As shown in FIG. 5, the partition plate 17 on the first side has a through hole 31 through which the inner cylindrical chamber 26 and the end chamber 19 communicate.
A plurality of them are provided symmetrically with respect to 5.
また、トルクチューブ3には、端部室18,19と外部
室32を蓮適する貫通孔33が設けられ、かつ給費E軸
11側の端部室19は給榎E軸11内の気体ヘリウム等
のガスを導出する通路34と貫通孔35により蓮適して
いる。そのため、駆動軸10側の端部室18は外部室3
2および給排軸11側の端部室19を通してガス導出通
路34に蓮適している。なお、36,37は駆動軸10
および給費E軸11を支承する軸受である。以上のよう
に構成された超電導回転子2において、外部から液体1
のペーパーを実線矢印で示すように、注入パイプ25お
よび吐出装置27を介して中間室29内に注入する。Further, the torque tube 3 is provided with a through hole 33 that connects the end chambers 18 and 19 and the external chamber 32, and the end chamber 19 on the side of the feeding shaft E-shaft 11 is provided with a gas such as helium in the feeding shaft E-shaft 11. The passage 34 and through hole 35 for leading out the lotus are suitable for the lotus. Therefore, the end chamber 18 on the drive shaft 10 side is the external chamber 3.
2 and the end chamber 19 on the supply/discharge shaft 11 side are connected to the gas outlet passage 34. In addition, 36 and 37 are the drive shaft 10
and a bearing that supports the allowance E shaft 11. In the superconducting rotor 2 configured as described above, the liquid 1 is supplied from the outside.
The paper is injected into the intermediate chamber 29 via the injection pipe 25 and the discharge device 27 as shown by the solid arrow.
そして、超電導回転子2を回転し、その速度が上昇して
rの/g(r:外側円筒21の外径、の:超電導回転子
の回転角速度、−g:重力の加速度)の関係になったと
き、先に注入したペーパーの代りに液体1を同様に注入
する。液体1は遠心力によりトルクチューブ内壁8側に
片寄り、貫通孔4より界磁巻線室15へ流入する。Then, the superconducting rotor 2 is rotated, and its speed increases to a relationship of r/g (r: outer diameter of the outer cylinder 21, n: rotational angular velocity of the superconducting rotor, -g: acceleration of gravity). At this time, liquid 1 is similarly injected in place of the previously injected paper. The liquid 1 is biased toward the inner wall 8 of the torque tube due to centrifugal force, and flows into the field winding chamber 15 through the through hole 4 .
界磁巻線室15および中間室29が液体1で満たされて
も、さらに液体1に圧力を加えて注入し、液体1の表面
9がパイプ24にくるか、あるいは内側円筒26内に少
量の液体1が入る状態にする。この際、液体1の一部は
トルクチュープ3に設けられた貫通孔4を通して界磁巻
線室15内に出入して、超電導界磁巻線6を冷却する。
超電導界磁巻線6等を冷却した液体1は、その温度が上
昇して一部はペーパーあるいはガス化し、液体表面に浮
上したり、あるいは液体表面より蒸発する。このペーパ
ーあるいはガスは、内側円筒室26に集まり、点線矢印
で示す方向に、仕切板貫通孔30、端部室18、トルク
チュープ貫通孔33、外部室32、トルクチューブ貫通
孔33および端部室19を流通して、超電導回転子2内
を冷却しつつ、給排軸内ガス導出通路34より外部に排
出される。Even if the field winding chamber 15 and the intermediate chamber 29 are filled with the liquid 1, the liquid 1 may be further injected under pressure until the surface 9 of the liquid 1 reaches the pipe 24 or a small amount of liquid 1 is inside the inner cylinder 26. Let liquid 1 enter. At this time, a portion of the liquid 1 enters and leaves the field winding chamber 15 through the through hole 4 provided in the torque tube 3 to cool the superconducting field winding 6.
The temperature of the liquid 1 that has cooled the superconducting field windings 6 and the like rises, and a portion thereof becomes paper or gas, floats to the surface of the liquid, or evaporates from the surface of the liquid. This paper or gas collects in the inner cylindrical chamber 26 and passes through the partition plate through hole 30, the end chamber 18, the torque tube through hole 33, the outer chamber 32, the torque tube through hole 33, and the end chamber 19 in the direction shown by the dotted arrow. The gas flows through the superconducting rotor 2 and is discharged to the outside from the supply/exhaust shaft gas outlet passage 34 while cooling the inside of the superconducting rotor 2 .
なお、注入パイプ25からは排出されたガス量に相当す
る液体1を外部より注入し、常時トルクチューブ3内の
液体1の量を一定に保つようにする。また、超電導回転
子2の回転を停止するに当っては、実線矢印とは逆の方
向へ液体1が流れるように負圧をかけ、内側円筒室26
、パイプ24内の液体1、および中間室29の液体1の
一部を超電導回転子2の外部に排出する。Note that the liquid 1 corresponding to the amount of the discharged gas is injected from the outside through the injection pipe 25, so that the amount of the liquid 1 inside the torque tube 3 is always kept constant. In addition, when stopping the rotation of the superconducting rotor 2, negative pressure is applied so that the liquid 1 flows in the direction opposite to the solid arrow.
, the liquid 1 in the pipe 24 and a part of the liquid 1 in the intermediate chamber 29 are discharged to the outside of the superconducting rotor 2.
ついで、超電導回転子2の回転数がrの2>gを満足す
る回転数において、超電導回転子2内部の残留液体が気
化するまで運転し、その後、回転を停止させる。あるい
はまた、上記回転数で運転中、注入パイプ25から液体
1の温度より高い温度の気体を中間室29内に送り、液
体1の気化を促進させることも行なわれている。このよ
うな液体1の注入、排出方法により、液体1の片寄りに
起因する超電導回転子2の熱変形による不釣り合い振動
は防止される。Next, the superconducting rotor 2 is operated at a rotation speed that satisfies 2>g of r until the residual liquid inside the superconducting rotor 2 is vaporized, and then the rotation is stopped. Alternatively, gas having a temperature higher than the temperature of the liquid 1 is sent from the injection pipe 25 into the intermediate chamber 29 during operation at the above-mentioned rotation speed to promote vaporization of the liquid 1. By such a method of injecting and discharging the liquid 1, unbalanced vibrations due to thermal deformation of the superconducting rotor 2 due to the deviation of the liquid 1 can be prevented.
本実施例によれば、超電導回転体2内部における液体1
の自由表面9は、パイプ24内にくるため、著しく少な
くなり、液体1の自由表面の挙動に起因する超電導回転
子2の不安定振動の発生を防ぎ、不安定振動の発生範囲
を減少させることができる。According to this embodiment, the liquid 1 inside the superconducting rotating body 2
Since the free surface 9 of the liquid 1 is located inside the pipe 24, it is significantly reduced, preventing the occurrence of unstable vibrations of the superconducting rotor 2 due to the behavior of the free surface of the liquid 1, and reducing the range in which unstable vibrations occur. I can do it.
その結果、超電導回転子2を安定にかつ静粛に回転させ
ることが可能となる。第6図は本発明の他の実施例を示
す。As a result, it becomes possible to rotate the superconducting rotor 2 stably and quietly. FIG. 6 shows another embodiment of the invention.
この例では、注入パイプ25の一端が超電導回転子2の
中央部附近まで延び、さらに注入パイプ25の池端には
、固定側冷煤通路と回転側冷煤通路をつなぐカップリン
グ38を介して冷嬢の供給、排出を行なう給排装置39
が設置されている。In this example, one end of the injection pipe 25 extends to near the center of the superconducting rotor 2, and the pond end of the injection pipe 25 is cooled via a coupling 38 that connects the stationary side cold soot passage and the rotating side cold soot passage. A supply/discharge device 39 for supplying and discharging women
is installed.
したがって、吐出装置27の吐出口28から注入される
液体’の冷却作用に関する熱対流が超電導回転子2に対
して対称となり、液体1を端部から注入する第3図の場
合に比べて、熱変形に起因する不釣り合い振動を少なく
することができる。また、第7図は本発明のさらに他の
実施例を示す。Therefore, the thermal convection related to the cooling effect of the liquid 'injected from the discharge port 28 of the discharge device 27 is symmetrical with respect to the superconducting rotor 2, and the heat convection is symmetrical with respect to the superconducting rotor 2, compared to the case of FIG. 3 in which the liquid 1 is injected from the end. Unbalanced vibrations caused by deformation can be reduced. Further, FIG. 7 shows still another embodiment of the present invention.
この実施例では、互に軸方向に間隔をあげて並談された
複数個の中空状リング40が、液体1中に内周側部分が
自由表面9に露出した状態で浸潰され、取付具41を介
してトルクチュ−ブ3に固定されている。In this embodiment, a plurality of hollow rings 40 arranged side by side with increasing intervals in the axial direction are immersed in the liquid 1 with the inner circumference side exposed to the free surface 9, and the mounting It is fixed to the torque tube 3 via 41.
したがって、中空状リング40の液体1中への浸積によ
り、液体1の自由表面9を回転軸線側に近付けて、これ
を少なくすることができるとともに、超電導回転子2内
部における液体1の容量を削減して、不釣り合い量を少
なくすることができ、その結果、液体1の自由表面の挙
動に起因する不安定振動、および不釣り合い振動を防止
することができる。Therefore, by immersing the hollow ring 40 into the liquid 1, the free surface 9 of the liquid 1 can be brought closer to the rotation axis side and reduced, and the capacity of the liquid 1 inside the superconducting rotor 2 can be reduced. As a result, unstable vibrations and unbalance vibrations caused by the behavior of the free surface of the liquid 1 can be prevented.
また、中空状リング40の内周側部分が液体10の自由
表面9上に露出し、これによって液体1の自由表面9は
軸方向に互に区分されているため、自由表面に起因する
不安定振動はさらに効果的に防止される。以上説明した
ように、本発明によれば、トルクチューブ内に注入され
て自由表面を形成している冷却液体内に、中空リング状
の浸贋部村の外周側部分を浸潰したので、冷却液体の自
由表面トルクチューブの回転軸心側に近付けて、この自
由表面を少なくすることができるとともに、冷却液体の
容量を削減して不釣り合い量を少なくすることができ、
冷却液体の自由表面に起因する不安定振動、および不釣
り合振動を防止することができる。In addition, since the inner peripheral side portion of the hollow ring 40 is exposed on the free surface 9 of the liquid 10, and the free surface 9 of the liquid 1 is thereby divided from each other in the axial direction, instability caused by the free surface can be avoided. Vibration is further effectively prevented. As explained above, according to the present invention, since the outer peripheral side of the hollow ring-shaped immersion part village is immersed in the cooling liquid injected into the torque tube and forming the free surface, cooling The free surface of the liquid can be brought closer to the axis of rotation of the torque tube to reduce this free surface, and the volume of cooling liquid can be reduced to reduce the amount of unbalance.
Unstable vibrations and unbalanced vibrations caused by the free surface of the cooling liquid can be prevented.
また、浸債部材の内周側部分を冷却液体の自由表面から
露出させ、この露出部分で冷却液体の自由表面を複数の
区分したので、自由表面に起因する不安定振動をさらに
効果的に防止することができる。その結果、超電導回転
子を静粛にかつ安定した状態で回転させることができる
。In addition, the inner circumferential portion of the bonding member is exposed from the free surface of the cooling liquid, and this exposed portion divides the free surface of the cooling liquid into multiple sections, which further effectively prevents unstable vibrations caused by the free surface. can do. As a result, the superconducting rotor can be rotated quietly and stably.
第1図は従来における超電導回転子の概略構造を示す縦
断側面図、第2図は内部液体の状態と回転数に関する不
安定振動の発生領域を示す特性図、第3図は本発明の一
実施例に係る超電導回転子の概略構造を示す縦断側面図
、第4図は第3図の×−X線断面図、第5図は第3図の
Y−Y線断面図、第6図および第7図は本発明の他の各
実施例に係る超電導回転子の概略構造を示す縦断側面図
である。
1・・・・・・冷却液体、2・・・・・・超電導回転子
「 3・・・…トルクチュ−ブ、5・・・・・・内側ダ
ンパ、6・・…・超電導界磁巻線、14・・・・・・外
側ダンパ、20・・・・・・内側円筒、21・・・・・
・外側円筒、24…・・・パイプ、40・・…・中空状
リング。
すーの
すZ風
丁3瀬
すム鼠
オS菌
汁 6 反幻
ブ7図Fig. 1 is a longitudinal cross-sectional side view showing the schematic structure of a conventional superconducting rotor, Fig. 2 is a characteristic diagram showing the state of the internal liquid and the region where unstable vibrations occur with respect to the rotation speed, and Fig. 3 is an embodiment of the present invention. A vertical side view showing a schematic structure of a superconducting rotor according to an example, FIG. 4 is a sectional view taken along the line X-X in FIG. 3, FIG. FIG. 7 is a longitudinal sectional side view showing a schematic structure of a superconducting rotor according to other embodiments of the present invention. 1...Cooling liquid, 2...Superconducting rotor 3...Torque tube, 5...Inner damper, 6...Superconducting field winding , 14...Outer damper, 20...Inner cylinder, 21...
-Outer cylinder, 24...pipe, 40...hollow ring. Sunosu Z Style 3 Sesumu Mouse S Bacterial Juice 6 Anti-Phantom 7 Diagram
Claims (1)
外周側に取付けられた超電導界磁巻線と、前記トルクチ
ユーブの内部に注入された前記超電導界磁巻線を冷却す
る冷却液体とを備え、前記冷却液体は、回転時に遠心力
により前記トルクチユーブの内壁側にトルクチユーブと
ほぼ同心状に片寄ってその内周側に自由表面を形成する
超電導回転子において、前記トルクチユーブ内に、中空
リング状の浸漬部材を、その外周側部分が自由表面を形
成している前記冷却液体内に浸漬され、その内周側部分
が自由表面から露出する状態で設け、前記浸漬部材の浸
漬部分で前記冷却液体の自由表面を前記トルクチユーブ
の回転軸心側に近付け、前記浸漬部材の露出部分で前記
冷却液体の自由表面を複数に区分したことを特徴とする
超電導回転子。 2 特許請求の範囲第1項において、前記浸漬部材は、
内側円筒、外側円筒およびこれらをつなぐ通路から構成
されていることを特徴とする超電導回転子。[Claims] 1. A cylindrical torque tube, a superconducting field winding attached to the outer circumference of the torque tube, and cooling for cooling the superconducting field winding injected into the torque tube. In the superconducting rotor, the cooling liquid is biased toward the inner wall of the torque tube due to centrifugal force during rotation to form a free surface on the inner circumferential side of the superconducting rotor. A hollow ring-shaped immersion member is provided in such a manner that its outer circumference side part is immersed in the cooling liquid forming a free surface, and its inner circumference side part is exposed from the free surface, and the immersion member is immersed. A superconducting rotor, characterized in that the free surface of the cooling liquid is brought closer to the rotation axis side of the torque tube at a portion thereof, and the free surface of the cooling liquid is divided into a plurality of portions at an exposed portion of the immersion member. 2. In claim 1, the immersion member:
A superconducting rotor comprising an inner cylinder, an outer cylinder, and a passage connecting these.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52054658A JPS6010498B2 (en) | 1977-05-12 | 1977-05-12 | superconducting rotor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52054658A JPS6010498B2 (en) | 1977-05-12 | 1977-05-12 | superconducting rotor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS53139108A JPS53139108A (en) | 1978-12-05 |
| JPS6010498B2 true JPS6010498B2 (en) | 1985-03-18 |
Family
ID=12976877
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP52054658A Expired JPS6010498B2 (en) | 1977-05-12 | 1977-05-12 | superconducting rotor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6010498B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4280071A (en) * | 1979-07-30 | 1981-07-21 | Westinghouse Electric Corp. | Vapor trap and regulator for superconductive turbogenerators |
-
1977
- 1977-05-12 JP JP52054658A patent/JPS6010498B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS53139108A (en) | 1978-12-05 |
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