JPH0459764B2 - - Google Patents
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- Publication number
- JPH0459764B2 JPH0459764B2 JP60283914A JP28391485A JPH0459764B2 JP H0459764 B2 JPH0459764 B2 JP H0459764B2 JP 60283914 A JP60283914 A JP 60283914A JP 28391485 A JP28391485 A JP 28391485A JP H0459764 B2 JPH0459764 B2 JP H0459764B2
- Authority
- JP
- Japan
- Prior art keywords
- conductor
- current lead
- hollow tube
- superconducting electromagnet
- helium gas
- 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 - Lifetime
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- Containers, Films, And Cooling For Superconductive Devices (AREA)
Description
【発明の詳細な説明】
〔発明の属する技術分野〕
この発明は低温容器内の超電導電磁石へ外部電
源より電力を供給するための超電導電磁石用電流
リードの導体構成に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of the Invention] The present invention relates to a conductor configuration of a current lead for a superconducting electromagnet for supplying power from an external power source to a superconducting electromagnet in a low-temperature container.
一般に超電導電磁石は液体ヘリウム等の極低温
冷媒によつて冷却されるため液体窒素シールドや
真空等によつて断熱された容器の内部に収納され
ている。電流リードは極低温に保持された超電導
マグネツトに常温部から電力を供給するもので、
一般に導体に発生するジユール熱と外部の常温部
から内部の極低温部へ伝導により侵入する熱を低
減するために、液体ヘリウムが蒸発した低温のヘ
リウムガスを用いて冷却する方式がとられてい
る。したがつて侵入熱が大きすぎると高価な液体
ヘリウムの消費量が多大となるばかりでなく、超
電導電磁石の特性に悪影響を及ぼすおそれもあ
る。
Generally, superconducting electromagnets are cooled by a cryogenic coolant such as liquid helium, and therefore are housed inside a container that is insulated by a liquid nitrogen shield, a vacuum, or the like. The current lead supplies power from room temperature to the superconducting magnet kept at an extremely low temperature.
Generally, in order to reduce the Joule heat generated in the conductor and the heat that invades from the outside room temperature part to the internal cryogenic part by conduction, a cooling method is used that uses low-temperature helium gas that is evaporated from liquid helium. . Therefore, if the intrusion heat is too large, not only will the consumption of expensive liquid helium become large, but there is also a possibility that the characteristics of the superconducting electromagnet will be adversely affected.
第2図に超電導電磁石装置の一般的な構成を示
す。低温容器1の内部には液体ヘリウムHeが入
つており、その中に超電導電磁石2が浸漬されて
いる。電流リード3は容器1を上蓋4に設けられ
たフランジ5を貫通して取付けられ、容器1内部
にある下端部は接続リード6を介して超電導電磁
石2に接続されている。液体ヘリウムHeの貯槽
の外側には、外部からの侵入熱を遮断するために
液体窒素シールドNが配設されている。また、電
流リード3の容器外部の上端部には図示しない外
部電源に接続するためのブスバー7が設けられて
いる。第2図の構成においては、容器1内で蒸発
したヘリウムガスを電流リード3の内部〓間に導
き電流リード3の内部において熱交換させ、極低
温部への侵入熱を減少させている。 Figure 2 shows the general configuration of a superconducting electromagnet device. Liquid helium He is contained inside the low temperature container 1, and a superconducting electromagnet 2 is immersed therein. The current lead 3 is attached to the container 1 by passing through a flange 5 provided on the upper lid 4, and the lower end inside the container 1 is connected to the superconducting electromagnet 2 via a connection lead 6. A liquid nitrogen shield N is provided outside the liquid helium He storage tank to block heat from entering from the outside. Further, a bus bar 7 for connecting to an external power source (not shown) is provided at the upper end of the current lead 3 outside the container. In the configuration shown in FIG. 2, the helium gas evaporated in the container 1 is guided between the interiors of the current leads 3 and exchanged with heat within the current leads 3, thereby reducing the amount of heat entering the cryogenic part.
第3図は第2図における電流リード3の横断面
を示すもので、中空管8の中に複数本の導体9を
稠密に挿入して形成された〓間10をヘリウムガ
スHeの流路として利用している。また中空管8
の外周はリード本体の絶縁するために絶縁物11
で取巻かれている。本構成によれば電流を通ずる
導体を複数本に分割することにより導体の冷却表
面積を増大させ、冷却効率を向上させる特徴があ
る。しかしながら本構成による電流リードを大電
流用に使用する場合は、導体の本数は多数本必要
となるため中空管へ挿入する作業性から導体の径
を細くすることに自ら限度を生じて導体の冷却表
面積を十分大きくすることができなかつた。この
ため冷却効果が低下して常温部から極低温部への
侵入熱が増大し、液体ヘリウムの消費量が増加し
て不経済な運転となる欠点があつた。 FIG. 3 shows a cross section of the current lead 3 shown in FIG. It is used as. Also hollow tube 8
The outer periphery of the lead body is covered with an insulator 11 to insulate the lead body.
is surrounded by. According to this configuration, the cooling surface area of the conductor is increased by dividing the conductor through which current flows into a plurality of pieces, thereby improving the cooling efficiency. However, when using the current lead with this configuration for large currents, a large number of conductors are required, so there is a limit to reducing the diameter of the conductor due to the workability of inserting it into a hollow tube. It was not possible to make the cooling surface area sufficiently large. As a result, the cooling effect is reduced, and the amount of heat entering from the room temperature section to the cryogenic section increases, which increases the amount of liquid helium consumed, resulting in uneconomical operation.
第4図は導体構成が別なる電流リード3の一部
破砕斜視図で、第3図の電流リードと同じような
外周を絶縁物で取巻かれた中空管8内に導体19
が収容される構成である。導体19は銅、銅合金
などの良電導体からなる丸棒状であつて外周に、
周上で2ケ所の対称な位置にスリツト21を備え
たデイスク状のフイン2が伝熱的に結合されてい
る。この導体19はヘリウムガスの流路を形成す
る中空管8に挿入されて電流リード本体が構成さ
れる。上述したデイスク状のフイン20のスリツ
ト21はそれぞれ90°の角度をもつて導体19の
外周に軸方向に所定のピツチを保つており、ヘリ
ウムガスの流路となつている。導体19にフイン
20を配置した理由は、冷却表面積を増大させて
冷却効率を向上させることと、ヘリウムガスが何
らかの原因でストツプした場合に導体19の温度
上昇を、フイン設置に伴う熱容量増加によつて遅
くするためである。しかしながらこのような利点
をもちながら、これらの構成においては、大電流
用に使用する場合には次のような欠点がある。す
なわち、導体に、大形で多数枚のデイスク状のス
リツト付きフインが必要であるためフインの切削
加工ならびに取付作業に多大の時間を必要とし、
コスト高の不経済な電流リードとなる問題があ
る。 FIG. 4 is a partially exploded perspective view of a current lead 3 with a different conductor configuration, in which a conductor 19 is placed inside a hollow tube 8 whose outer periphery is surrounded by an insulating material, similar to the current lead shown in FIG.
This is a configuration that accommodates. The conductor 19 is a round bar made of a good conductor such as copper or copper alloy, and has a shape on the outer periphery.
Disc-shaped fins 2 having slits 21 at two symmetrical positions on the circumference are thermally connected. This conductor 19 is inserted into a hollow tube 8 forming a flow path for helium gas to constitute a current lead body. The slits 21 of the disk-shaped fins 20 are each angled at 90° and maintain a predetermined pitch in the axial direction around the outer periphery of the conductor 19, forming a flow path for helium gas. The reason for arranging the fins 20 on the conductor 19 is to increase the cooling surface area to improve cooling efficiency, and to prevent the temperature rise of the conductor 19 from increasing when the helium gas is stopped for some reason by increasing the heat capacity due to the installation of the fins. This is to slow down the process. However, while having these advantages, these configurations have the following drawbacks when used for large currents. In other words, since the conductor requires a large number of disk-shaped fins with slits, it takes a lot of time to cut and install the fins.
There is a problem of high cost and uneconomical current leads.
すなわち以上述べた導体構成は何れも、大電流
用として使用する場合には問題があつた。 That is, all of the conductor configurations described above have problems when used for large current applications.
この本発明は上述した事情に鑑み、とくに大電
流使用時においても電流リードの冷却効果を向上
させ超電導電磁石への侵入熱を少なくして経済的
な電流リードを提供できるよう導体構成を改良す
ることを目的とする。
In view of the above-mentioned circumstances, the present invention aims to improve the conductor structure so as to improve the cooling effect of the current lead and reduce the amount of heat entering the superconducting electromagnet, especially when using a large current, thereby providing an economical current lead. With the goal.
この発明では上記目的達成のため電流リードの
導体構成を次のようにした。すなわちヘリウムガ
スの流路を形成する中空管の内部に、銅・銅合金
などの良電導材で形成した丸線導体と、ステンレ
ス・マンガン鋼・ニクロム鋼などの熱伝導率が小
さく低温にても高強度を有する材料で形成した丸
線材とをそれぞれ複数本混合させて稠密に挿入し
た。
In this invention, in order to achieve the above object, the conductor structure of the current lead is as follows. In other words, inside the hollow tube that forms the helium gas flow path, there is a round wire conductor made of a highly conductive material such as copper or copper alloy, and a conductor made of a material with low thermal conductivity such as stainless steel, manganese steel, or nichrome steel that can be used at low temperatures. A plurality of round wire rods made of a material having high strength were mixed and inserted densely.
第1図は本発明の実施例を示す電流リードの横
断面図である。この電流リードにおける導体構成
は、外周を絶縁物11にて被覆された中空管8の
内部に銅・銅合金などの良電導材で形成した複数
本の丸線導体29aと、ステンレス・マンガン
鋼・ニクロム鋼などの熱伝導率が小さくかつ低温
にても高強度を有する材料で形成した複数本の丸
線材29bとをそれぞれ混合させて稠密に挿入し
た。そして中空管8の内壁、丸線導体29aおよ
び丸線材29bで囲まれた数多い小さな〓間10
をヘリウムガスの流路として利用するものである
本構成によれば、冷却効率を向上できるとともに
製作性にも勝れた経済的な電流リードとすること
ができる。
FIG. 1 is a cross-sectional view of a current lead showing an embodiment of the present invention. The conductor structure of this current lead includes a plurality of round wire conductors 29a made of a good conductive material such as copper or copper alloy inside a hollow tube 8 whose outer periphery is covered with an insulator 11, and a plurality of round wire conductors 29a made of a good conductive material such as copper or copper alloy, and stainless steel or manganese steel. - A plurality of round wire rods 29b made of a material having low thermal conductivity and high strength even at low temperatures, such as nichrome steel, were mixed and inserted densely. Then, there are many small gaps 10 surrounded by the inner wall of the hollow tube 8, the round wire conductor 29a, and the round wire rod 29b.
According to this configuration, in which the helium gas is used as a flow path for helium gas, it is possible to improve the cooling efficiency and provide an economical current lead with excellent manufacturability.
この発明によれば、ヘリウムガスの流路を形成
する中空管内に電気伝導度の良い丸線導体と、熱
伝導率の小さい丸線材とをそれぞれ複数本混合し
て稠密に挿入したので、従来構造に比べて電流リ
ード本体の冷却表面積を大きくすることができ、
ヘリウムガスがストツプした場合でも、熱伝導率
の小さい丸線材の熱容量によつて、電流リード本
体の熱容量を増加でき、その結果温度上昇を遅く
するという利点がある。またこの丸線材は低温に
ても高強度を有するのでリード本体の剛性を増大
することができ、リード本体に作用する電磁力に
も十分耐え得る構造が得らえる。
According to this invention, a plurality of round wire conductors with good electrical conductivity and a plurality of round wires with low thermal conductivity are mixed and inserted densely into the hollow tube that forms the helium gas flow path. The cooling surface area of the current lead body can be increased compared to
Even when the helium gas is stopped, the heat capacity of the current lead body can be increased due to the heat capacity of the round wire with low thermal conductivity, which has the advantage of slowing down the temperature rise. Furthermore, since this round wire material has high strength even at low temperatures, the rigidity of the lead body can be increased, and a structure that can sufficiently withstand electromagnetic force acting on the lead body can be obtained.
第1図はこの発明の一実施例である超電導電磁
石装置用電流リードの横断面図、第2図は超電導
電磁石装置の縦断面図、第3図は従来構成による
超電導電磁石装置用電流リードの横断面図、第4
図は従来構成による他例の超電導電磁石装置用電
流リードの一部破砕斜視図である。
1:低温容器、3:電流リード、8:中空管、
9:導体、10:〓間、29a:丸棒導体、29
b:丸線材。
FIG. 1 is a cross-sectional view of a current lead for a superconducting electromagnet device according to an embodiment of the present invention, FIG. 2 is a longitudinal cross-sectional view of the superconducting electromagnet device, and FIG. 3 is a cross-sectional view of a current lead for a superconducting electromagnet device having a conventional configuration. Front view, 4th
The figure is a partially exploded perspective view of another example of a current lead for a superconducting electromagnet device having a conventional configuration. 1: Low temperature container, 3: Current lead, 8: Hollow tube,
9: Conductor, 10: Between, 29a: Round bar conductor, 29
b: Round wire rod.
Claims (1)
電磁石に外部電源より電力を供給するため中空管
内に導体を挿入し、この中空管内の〓間にヘリウ
ムガスを流通させる通電用電流リードにおいて;
前記中空管の内部に、銅・銅合金などの良電導材
で形成した丸線導体と、ステンレス鋼・マンガン
鋼・ニクロム鋼などの熱伝導率が小さく低温にて
も高強度を有する材料で形成した丸線材とをそれ
ぞれ複数本混合させて稠密に挿入したことを特徴
とする超電導電磁石装置用電流リード。1 In order to supply power from an external power supply to a superconducting electromagnet kept at an extremely low temperature in a cryogenic container, a conductor is inserted into a hollow tube, and in a current lead for flowing helium gas between the holes in this hollow tube;
Inside the hollow tube, there is a round wire conductor made of a highly conductive material such as copper or copper alloy, and a material with low thermal conductivity and high strength even at low temperatures such as stainless steel, manganese steel, or nichrome steel. A current lead for a superconducting electromagnet device, characterized in that a plurality of formed round wires are mixed and inserted densely.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60283914A JPS62142379A (en) | 1985-12-17 | 1985-12-17 | Current lead for superconductive electromagnet device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60283914A JPS62142379A (en) | 1985-12-17 | 1985-12-17 | Current lead for superconductive electromagnet device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62142379A JPS62142379A (en) | 1987-06-25 |
| JPH0459764B2 true JPH0459764B2 (en) | 1992-09-24 |
Family
ID=17671824
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60283914A Granted JPS62142379A (en) | 1985-12-17 | 1985-12-17 | Current lead for superconductive electromagnet device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62142379A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04100281A (en) * | 1990-08-20 | 1992-04-02 | Fuji Electric Co Ltd | Current lead for superconducting equipment |
-
1985
- 1985-12-17 JP JP60283914A patent/JPS62142379A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62142379A (en) | 1987-06-25 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
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Free format text: JAPANESE INTERMEDIATE CODE: R250 |
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