JPH041483B2 - - Google Patents
Info
- Publication number
- JPH041483B2 JPH041483B2 JP61126401A JP12640186A JPH041483B2 JP H041483 B2 JPH041483 B2 JP H041483B2 JP 61126401 A JP61126401 A JP 61126401A JP 12640186 A JP12640186 A JP 12640186A JP H041483 B2 JPH041483 B2 JP H041483B2
- Authority
- JP
- Japan
- Prior art keywords
- current supply
- inner tube
- cryogenic refrigerant
- gas
- cooled
- 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
Links
- 239000003507 refrigerant Substances 0.000 claims description 34
- 239000004020 conductor Substances 0.000 claims description 24
- 230000005284 excitation Effects 0.000 claims description 6
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 claims description 4
- 229910052802 copper Inorganic materials 0.000 claims description 4
- 239000010949 copper Substances 0.000 claims description 4
- 238000007599 discharging Methods 0.000 claims description 3
- 239000000463 material Substances 0.000 claims description 3
- 239000007789 gas Substances 0.000 description 33
- 238000001816 cooling Methods 0.000 description 15
- 239000001307 helium Substances 0.000 description 7
- 229910052734 helium Inorganic materials 0.000 description 7
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 7
- 239000007788 liquid Substances 0.000 description 7
- PPBRXRYQALVLMV-UHFFFAOYSA-N Styrene Chemical compound C=CC1=CC=CC=C1 PPBRXRYQALVLMV-UHFFFAOYSA-N 0.000 description 2
- 239000002826 coolant Substances 0.000 description 2
- 102100040287 GTP cyclohydrolase 1 feedback regulatory protein Human genes 0.000 description 1
- 101710185324 GTP cyclohydrolase 1 feedback regulatory protein Proteins 0.000 description 1
- 239000000112 cooling gas Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000006260 foam Substances 0.000 description 1
- 238000009434 installation Methods 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
- 238000003466 welding Methods 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Landscapes
- Containers, Films, And Cooling For Superconductive Devices (AREA)
Description
【発明の詳細な説明】
〔発明の目的〕
(産業上の利用分野)
本発明は極低温冷媒容器に収容した極低温冷媒
中に浸漬冷却された超電導マグネツトへ、常温環
境下におかれた励磁用電源から電流を供給するた
めの電流供給リードの改良に関すものである。[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention is directed to excitation of a superconducting magnet that is immersed and cooled in a cryogenic refrigerant housed in a cryogenic refrigerant container and placed in a room temperature environment. This invention relates to an improvement in a current supply lead for supplying current from a commercial power source.
(従来の技術)
従来、極低温冷媒容器に収容した液体ヘリウム
等の極低温冷媒中に浸漬冷却された超電導マグネ
ツトの超電導コイルに、常温環境下におかれた励
磁用電源から電流を供給するための手段として、
電流供給リードが使用されてきている。そして、
この種の電流供給リードに関する技術について
は、電流供給リード低温端での極低温冷媒への侵
入熱に伴う蒸発極低温冷媒によつてリード表面と
の熱交換を行ない、電流供給リードをその全長に
わたり冷却して侵入熱を減少させるように構成し
たガス冷却電流供給リードがある。(Prior art) Conventionally, a current is supplied from an excitation power supply placed in a normal temperature environment to a superconducting coil of a superconducting magnet that is immersed and cooled in a cryogenic coolant such as liquid helium stored in a cryogenic coolant container. As a means of
Current supply leads have been used. and,
Regarding the technology related to this type of current supply lead, heat exchange with the lead surface is performed by the evaporated cryogenic refrigerant due to the heat entering the cryogenic refrigerant at the low temperature end of the current supply lead, and the current supply lead is extended over its entire length. There are gas-cooled current supply leads configured to cool and reduce incoming heat.
しかしながら、2個以上の複数個の超電導コイ
ルを備え、これらの各超電導コイルをそれぞれ独
立して励磁することによつて磁場配位を調整する
ような、例えばジヤイロトロン用超電導マグネツ
ト等の超電導マグネツトでは、それに伴つて電流
供給リードの本数が多くなることから、各々の電
流供給リードに上述のガス冷却電流供給リードを
夫々独立に適用すると、次のような問題が生じる
ことになる。 However, in a superconducting magnet, such as a superconducting magnet for a gyrotron, which has two or more superconducting coils and adjusts the magnetic field configuration by independently exciting each of these superconducting coils, As a result, the number of current supply leads increases, and if the above-mentioned gas cooling current supply leads are independently applied to each current supply lead, the following problem will occur.
(a) ガス冷却電流供給リードの総断面積が非常に
大きくなり、結果的に極低温冷媒容器への熱侵
入量が大きくなる。(a) The total cross-sectional area of the gas cooling current supply lead becomes very large, resulting in a large amount of heat intrusion into the cryogenic refrigerant container.
(b) 上述の熱侵入量を少なくするためにリードの
長さを長くすると、ガス冷却電流供給リードの
構成が非常に複雑で大形となるばかりでなく、
各々のガス流路が狭くかつ長くなることから、
僅かな空気の侵入で水分によつてガス流路が閉
塞してしまう。(b) If the length of the lead is increased in order to reduce the amount of heat intrusion mentioned above, the structure of the gas-cooled current supply lead not only becomes very complicated and large, but also
As each gas flow path becomes narrower and longer,
Even the slightest intrusion of air can cause the gas flow path to become clogged with moisture.
(c) 各々の電流供給リードに対する冷却ガス流量
のアンバランスを生じ易いため、リード断面の
選定、ガス冷却管の設計等、各々の電流供給リ
ードに最適な限界設計を行なうことが出来な
い。(c) Since the cooling gas flow rate for each current supply lead tends to be unbalanced, it is not possible to perform optimal limit design for each current supply lead, such as selection of lead cross section and design of gas cooling pipe.
(発明が解決しようとする問題点)
以上のように、従来のガス冷却電流供給リード
においては、極低温冷媒容器への熱侵入量が大き
く、構成が複雑で大形であるばかりでなく、電流
供給リードに最適な限界設計を行なうことが出来
ないという問題があつた。(Problems to be Solved by the Invention) As described above, in the conventional gas cooling current supply lead, the amount of heat entering the cryogenic refrigerant container is large, the structure is complicated and large, and the current supply lead is There was a problem in that it was not possible to perform an optimal limit design for the supply lead.
そこで本発明では、リードの長さを長くするこ
となく極低温冷媒容器への熱侵入量を少なくし、
構成の簡単化ならびに小形化を図り、しかも最適
な限界設計を行なうことが可能な信頼性の高いガ
ス冷却電流供給リードを提供することを目的とす
るものである。 Therefore, in the present invention, the amount of heat entering the cryogenic refrigerant container is reduced without increasing the length of the lead,
The object of the present invention is to provide a highly reliable gas-cooled current supply lead that is simple in structure and compact, and allows optimal limit design.
(問題点を解決するための手段)
上記の目的を達成するるために本発明では、極
低温冷媒容器に収容した極低温冷媒中に浸漬冷却
された超電導マグネツトへ、常温環境下におかれ
た励磁用電源から電流を供給するための電流供給
リードにおいて、上記極低温冷媒容器に下端部が
取付けられた外管と、上端部側に極低温冷媒蒸発
ガス放出用の穴を有し、上記外管の内側に一定の
空隙を存して配設された内管と、この内管の外周
側に当該内管の長さよりも長くなるように巻回さ
れ、常温環境下のリード端子を介して上記超電導
マグネツトの超電導コイルに電流を供給する複数
本の電流供給用導体とを備えて成り、蒸発した極
低温冷媒を、上記外管と内管との間の空隙部を通
上記極低温冷媒蒸発ガス放出用穴より内管の内側
を通して大気中へ放出する構成としたことを特徴
とする。
(Means for Solving the Problems) In order to achieve the above object, the present invention provides a superconducting magnet that is immersed and cooled in a cryogenic refrigerant housed in a cryogenic refrigerant container and is placed in a normal temperature environment. The current supply lead for supplying current from the excitation power source has an outer tube whose lower end is attached to the cryogenic refrigerant container and a hole for releasing evaporative gas of the cryogenic refrigerant on the upper end side. An inner tube is arranged with a certain gap inside the tube, and the inner tube is wound around the outer circumference of the inner tube to be longer than the length of the inner tube. and a plurality of current supply conductors for supplying current to the superconducting coils of the superconducting magnet, the evaporated cryogenic refrigerant is passed through the gap between the outer tube and the inner tube to evaporate the cryogenic refrigerant. The gas is discharged into the atmosphere through the inner tube through the gas discharge hole.
(作 用)
上述のガス冷却電流供給リードにおいては、超
電導マグネツトの超電導コイルに電流を供給する
ための複数本の電流供給用導体を、外管と内管と
の間の空隙により形成される単一のガス流路に共
通に配置していることから、このガス流路を通過
する蒸発した極低温冷媒により、各々の電流供給
用導体が流量アンバランスを生じることなく冷却
されることになる。また、複数本の電流供給用導
体を単一のガス冷却管内に配置していることか
ら、極低温冷媒容器への熱侵入量が低減されるこ
とになる。さらに、上述の熱侵入量の軽減により
ガス冷却管の長さを長くしなくてもよいことか
ら、構成が簡単でしかもコンパクトなものとな
る。(Function) In the above-mentioned gas-cooled current supply lead, a plurality of current supply conductors for supplying current to the superconducting coil of the superconducting magnet are connected to a single conductor formed by the gap between the outer tube and the inner tube. Since they are commonly disposed in one gas flow path, each current supply conductor is cooled by the evaporated cryogenic refrigerant passing through this gas flow path without causing flow imbalance. Furthermore, since a plurality of current supply conductors are arranged within a single gas cooling pipe, the amount of heat entering the cryogenic refrigerant container is reduced. Furthermore, the above-mentioned reduction in the amount of heat intrusion eliminates the need to increase the length of the gas cooling pipe, resulting in a simple and compact configuration.
(実施例)
以下、本発明を図面に示す一実施例を参照して
説明する。(Example) The present invention will be described below with reference to an example shown in the drawings.
第1図は本発明によるガス冷却電流供給リード
の構成例を示す縦断面図、また第2図は第1図に
おける平面図を示すものである。 FIG. 1 is a longitudinal sectional view showing an example of the configuration of a gas-cooled current supply lead according to the present invention, and FIG. 2 is a plan view of FIG. 1.
図において、1は上端部に図示しない真空容器
に連結されるフランジ1aを有し、例えばステン
レスから外管であり、その下端部を極低温冷媒で
ある液体ヘリウムが収容された図示しない極低温
冷媒容器に溶接等により取付けている。一方、2
は上端部にフランジ2aを有し、例えば熱伝導の
小さいGFRPからなる内管であり、上記外管1の
内側に図示の如く一定の空隙を存して配設してい
る。また、この内管2は上端部側の図示位置に、
周方向に沿つて液体ヘリウム蒸発ガス放出用の複
数個の穴2bを有し、この液体ヘリウム蒸発ガス
放出用穴2bよりも下方の内管2外周側には、当
該内管2の長さよりも長くなるように複数本(本
例では2本)の電流供給用導体3を内管2に沿つ
てら線状に巻回している。さらに、この2本の電
流供給用導体3には常温環境下のリード端子4を
接続し、常温環境下におかれた励磁用電源からこ
のリード端子4を介して、図示しない超電導マグ
ネツトの超電導コイルに電流を供給するようにし
ている。以上のようにして、蒸発した液体ヘリウ
ムを、上記外管1と内管2との間の空隙部を通し
上記極低温冷媒蒸発ガス放出用穴2bより内管2
の内側を通して大気中へ放出する構成とすること
により、各々の電流供給用導体3を冷却するよう
にしている。なお、上述の電流供給用導体3の材
料としては、例えば熱伝導の小さい銅(りん脱酸
銅)を用いる。また、内管2の下端部から極低温
冷媒蒸発ガス放出用穴2bにかけては、その内部
に液体ヘリウムガスの管内への侵入を阻止するた
めに、例えば発泡スチロールを詰物5として詰め
込んでいる。 In the figure, reference numeral 1 has a flange 1a connected to a vacuum container (not shown) at its upper end, and is an outer tube made of stainless steel, for example. It is attached to the container by welding, etc. On the other hand, 2
The inner tube has a flange 2a at its upper end and is made of, for example, GFRP with low thermal conductivity, and is disposed inside the outer tube 1 with a certain gap as shown in the figure. Moreover, this inner tube 2 is located at the illustrated position on the upper end side.
It has a plurality of holes 2b for releasing liquid helium evaporated gas along the circumferential direction, and on the outer peripheral side of the inner tube 2 below the holes 2b for releasing liquid helium evaporated gas, there is a hole 2b that is longer than the length of the inner tube 2. A plurality of current supply conductors 3 (two in this example) are wound in a spiral shape along the inner tube 2 so as to be long. Furthermore, a lead terminal 4 under a normal temperature environment is connected to these two current supply conductors 3, and a superconducting coil of a superconducting magnet (not shown) is connected to the excitation power supply under a normal temperature environment via the lead terminal 4. It is designed to supply current to. As described above, the evaporated liquid helium is passed through the gap between the outer tube 1 and the inner tube 2 and from the cryogenic refrigerant evaporated gas release hole 2b to the inner tube 2.
Each current supply conductor 3 is cooled by discharging it into the atmosphere through the inside of the current supply conductor 3. Note that as the material of the above-mentioned current supply conductor 3, for example, copper (phosphorus-deoxidized copper) having low thermal conductivity is used. Furthermore, from the lower end of the inner tube 2 to the hole 2b for releasing cryogenic refrigerant evaporated gas, a stuffing 5 of, for example, styrene foam is packed inside to prevent liquid helium gas from entering the tube.
かかる構成のガス冷却電流供給リードにおいて
は、複数本の電流供給用導体3を、外管1および
内管2からなる単一のガス冷却管内に共通に配置
していることから、ガス冷却電流供給リードの総
断面積が著しく小さくなり、結果的に極低温冷媒
容器への熱侵入量を大幅に低減することが可能と
なる。また、複数本の電流供給用導体3を外管1
と内管2との間の空隙により形成される単一のガ
ス流路に共通に配置していることから、このガス
流路を通過する蒸発した液体ヘリウムにより、
各々の電流供給用導体3が流量アンバランスを生
じることなく均一に冷却されて冷却効率を高める
ことができる。これにより、リード断面の選定、
ガス冷却管の設計等、各々の電流供給用導体に最
適な限界設計を行なうことが可能となる。さら
に、極低温冷媒容器への熱侵入量を少なくするた
めに、電流供給用導体3の長さは長くしても、外
管1および内管2からなるガス冷却管の長さは短
かくて済むことから、ガス冷却電流供給リードの
構成が極めて簡単で小形となるばかりでなく、ガ
ス流路が広くかつ短かくなるため、従来のように
僅かな空気の侵入に伴う水分によつてガス流路が
閉塞するというような事も無くなる。さらにま
た、電流供給用導体3の本数が複数本であつても
ガス冷却管は1本でよいことから、極低温容器上
面のスペースが少なくて済み、液体ヘリウムの回
収または放出用の配管も1系統で済むため、ガス
冷却電流供給リードの設置が極めて容易となる。 In the gas cooling current supply lead having such a configuration, since the plurality of current supply conductors 3 are commonly arranged in a single gas cooling pipe consisting of the outer tube 1 and the inner tube 2, the gas cooling current supply lead is The total cross-sectional area of the leads becomes significantly smaller, and as a result, it becomes possible to significantly reduce the amount of heat entering the cryogenic refrigerant container. In addition, a plurality of current supply conductors 3 are connected to the outer tube 1.
Since they are commonly arranged in a single gas flow path formed by the gap between the inner tube 2 and the inner tube 2, evaporated liquid helium passing through this gas flow path causes
Each current supply conductor 3 is uniformly cooled without causing flow imbalance, and cooling efficiency can be improved. This allows selection of lead cross section,
It becomes possible to perform optimal limit design for each current supply conductor, such as the design of a gas cooling pipe. Furthermore, in order to reduce the amount of heat intrusion into the cryogenic refrigerant container, even if the length of the current supply conductor 3 is long, the length of the gas cooling tube consisting of the outer tube 1 and the inner tube 2 is short. This not only makes the configuration of the gas cooling current supply lead extremely simple and compact, but also makes the gas flow path wider and shorter, which prevents gas flow from being caused by moisture caused by a small amount of air intrusion. There will no longer be any road blockages. Furthermore, even if the number of current supply conductors 3 is multiple, only one gas cooling pipe is required, so the space on the top surface of the cryogenic container is small, and the number of pipes for recovering or discharging liquid helium is also one. Because it only requires a power grid, installation of gas cooling current supply leads is extremely easy.
尚、本発明は上述した実施例に限定されるもの
ではなく、次のようにしても同様に実施すること
ができるものである。 It should be noted that the present invention is not limited to the embodiments described above, but can be similarly implemented in the following manner.
(a) 上記実施例では、電流供給用導体3の材料と
しては熱伝導の小さい銅を用いたが、これに限
らずその他の熱伝導の小さい材料を用いて形成
するようにしてもよいものである。(a) In the above embodiment, the current supply conductor 3 is made of copper, which has low thermal conductivity; however, it is not limited to this, and may be formed using other materials with low thermal conductivity. be.
(b) 上記実施例では、本発明をジヤイロトロン用
超電導マグネツトに適用した場合を述べたが、
これに限らずその他の超電導マグネツトについ
ても本発明を同様に適用することができるもの
である。(b) In the above embodiment, the present invention was applied to a superconducting magnet for a gyrotron.
The present invention is not limited to this, and the present invention can be similarly applied to other superconducting magnets.
(c) 上記実施例では、電流供給用導体3を内管2
にら線状に巻回した場合を述べたが、これに限
らず内管2の長さよりも長くなるように、その
他の所定の形状に巻回するようにしてもよいも
のである。(c) In the above embodiment, the current supply conductor 3 is connected to the inner tube 2.
Although the case of winding in a linear shape has been described, the present invention is not limited to this, and it may be wound in other predetermined shapes so as to be longer than the length of the inner tube 2.
(d) 上記実施例では、8本の電流供給用導体3を
内管2に巻回した場合を述べたが、これに限ら
ず2本以上の複数本の電流供給用導体3を内管
2に巻回するようにしてもよいものである。(d) In the above embodiment, a case was described in which eight current supply conductors 3 were wound around the inner tube 2, but the present invention is not limited to this, and two or more current supply conductors 3 were wound around the inner tube 2. It is also possible to wind it around.
その他、本発明はその要旨を変更しない範囲
で、種々に変形して実施することができるもので
ある。 In addition, the present invention can be modified and implemented in various ways without changing the gist thereof.
以上説明したように本発明によれば、極低温冷
媒容器に収容した極低温冷媒中に浸漬冷却された
超電導マグネツトへ、常温環境下におかれた励磁
用電源から電流を供給するための電流供給リード
において、上記極低温冷媒容器に下端部が取付け
られた外管と、上端部側に極低温冷媒蒸発ガス放
出用の穴を有し、上記外管の内側に一定の空隙を
存して配設された内管と、この内管の外周側に当
該内管の長さよりも長くなるように巻回され、常
温環境下のリード端子を介して上記超電導マグネ
ツトの超電導コイルに電流を供給する複数本の電
流供給用導体とを備えて成り、蒸発した極低温冷
媒を、上記外管と内管との間の空隙部を通し上記
極低温冷媒蒸発ガス放出用穴より内管の内側を通
して大気中へ放出する構成としたので、リードの
長さを長くすることなく極低温冷媒容器への熱侵
入量を少なくし、構成の簡単化ならびに小形化を
図り、しかも最適な限界設計を行なうことが可能
な極めて信頼性の高いガス冷却電流供給リードが
提供できる。
As explained above, according to the present invention, a current is supplied from an excitation power source placed in a normal temperature environment to a superconducting magnet immersed and cooled in a cryogenic refrigerant contained in a cryogenic refrigerant container. The lead has an outer tube whose lower end is attached to the cryogenic refrigerant container and a hole on the upper end side for releasing evaporated gas of the cryogenic refrigerant, and is arranged with a certain gap inside the outer tube. A plurality of coils are wound around the outer circumferential side of the inner tube so as to be longer than the length of the inner tube, and supply current to the superconducting coil of the superconducting magnet through lead terminals in a normal temperature environment. The evaporated cryogenic refrigerant is passed through the gap between the outer tube and the inner tube, and is passed inside the inner tube through the hole for releasing evaporated gas of the cryogenic refrigerant into the atmosphere. Since the structure is designed to release heat to the cryogenic refrigerant container, the amount of heat entering the cryogenic refrigerant container is reduced without increasing the length of the lead, simplifying the structure and downsizing, and making it possible to perform optimal limit design. This provides an extremely reliable gas-cooled current supply lead.
第1図は本発明の一実施例を示す縦断面構成
図、第2図は同実施例における平面図を示すもの
である。
1…外管、1a…フランジ、2…内管、2a…
フランジ、2b…極低温冷媒蒸発ガス放出用穴、
3…電流供給用導体、4…リード端子、5…詰
物。
FIG. 1 is a vertical cross-sectional configuration diagram showing an embodiment of the present invention, and FIG. 2 is a plan view of the same embodiment. 1... Outer tube, 1a... Flange, 2... Inner tube, 2a...
Flange, 2b...hole for releasing cryogenic refrigerant evaporative gas,
3... Current supply conductor, 4... Lead terminal, 5... Filling.
Claims (1)
漬冷却された超電導マグネツトへ、常温環境下に
おかれた励磁用電源から電流を供給するための電
流供給リードにおいて、前記極低温冷媒容器に下
端部が取付けられた外管と、上端部側に極低温冷
媒蒸発ガス放出用の穴を有し、前記外管の内側に
一定の空隙を存して配設された内管と、この内管
の外周側に当該内管の長さよりも長くなるように
巻回され、常温環境下のリード端子を介して前記
超電導マグネツトの超電導コイルに電流を供給す
る複数本の電流供給用導体とを備えて成り、蒸発
した極低温冷媒を、前記外管と内管との間の空隙
部を通し前記極低温冷媒蒸発ガス放出用穴より内
管の内側を通して大気中へ放出する構成としたこ
とを特徴とするガス冷却電流供給リード。 2 電流供給用導体の材料としては、熱伝導の小
さい銅を用いるようにしたことを特徴とする特許
請求の範囲第1項記載のガス冷却電流供給リー
ド。 3 電流供給用導体は、内管に沿つてら線状に巻
回するようにしたことを特徴とする特許請求の範
囲第1項記載のガス冷却電流供給リード。[Scope of Claims] 1. In a current supply lead for supplying current from an excitation power source placed in a normal temperature environment to a superconducting magnet immersed and cooled in a cryogenic refrigerant contained in a cryogenic refrigerant container, the An outer tube having a lower end attached to a cryogenic refrigerant container, and an inner tube having a hole on the upper end side for releasing evaporated gas of the cryogenic refrigerant, and an inner tube arranged with a certain gap inside the outer tube. a tube, and a plurality of current supplies wound around the outer circumferential side of the inner tube so as to be longer than the length of the inner tube, and supplying current to the superconducting coil of the superconducting magnet through lead terminals in a normal temperature environment. and a conductor for discharging the evaporated cryogenic refrigerant into the atmosphere through the gap between the outer tube and the inner tube and through the cryogenic refrigerant evaporated gas release hole through the inside of the inner tube. A gas-cooled current supply lead characterized by: 2. The gas-cooled current supply lead according to claim 1, wherein copper, which has low thermal conductivity, is used as the material of the current supply conductor. 3. The gas-cooled current supply lead according to claim 1, wherein the current supply conductor is wound in a spiral shape along the inner tube.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61126401A JPS62283609A (en) | 1986-05-31 | 1986-05-31 | Gas cooled current supplying lead |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61126401A JPS62283609A (en) | 1986-05-31 | 1986-05-31 | Gas cooled current supplying lead |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62283609A JPS62283609A (en) | 1987-12-09 |
| JPH041483B2 true JPH041483B2 (en) | 1992-01-13 |
Family
ID=14934241
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61126401A Granted JPS62283609A (en) | 1986-05-31 | 1986-05-31 | Gas cooled current supplying lead |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS62283609A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03283678A (en) * | 1990-03-30 | 1991-12-13 | Fuji Electric Co Ltd | Current lead of superconducting magnet apparatus |
| JP2734171B2 (en) * | 1990-05-11 | 1998-03-30 | 富士電機株式会社 | Current lead of superconducting magnet device |
| JP5011181B2 (en) * | 2008-03-19 | 2012-08-29 | 昭和電線ケーブルシステム株式会社 | Oxide superconducting current lead |
-
1986
- 1986-05-31 JP JP61126401A patent/JPS62283609A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62283609A (en) | 1987-12-09 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US20200258670A1 (en) | Reactor, motor driver, power conditioner and machine | |
| US6838968B2 (en) | Transformer with forced liquid coolant | |
| US4363773A (en) | Superconductive electromagnet apparatus | |
| JPH041483B2 (en) | ||
| JPH04573B2 (en) | ||
| JPH06504401A (en) | Hollow electrical conductors that can be cooled at low temperatures and their applications | |
| JPH0510809B2 (en) | ||
| JPS61229306A (en) | Superconducting coil | |
| JPS61179508A (en) | Forced cooling superconducting coil device | |
| JP3178119B2 (en) | Gas-cooled current leads for superconducting coils | |
| JPH0246007Y2 (en) | ||
| JPH0656902B2 (en) | Superconducting device | |
| JPH05335144A (en) | Superconductor system and current lead conductor | |
| JP2739159B2 (en) | Toroidal magnet | |
| JP3322981B2 (en) | Permanent current switch | |
| JPS58184775A (en) | Heat insulating container for superconductive magnet | |
| JPH02308507A (en) | foil wound transformer | |
| JPS61187311A (en) | Foil-wound transformer | |
| JPS6155071B2 (en) | ||
| KR900005484Y1 (en) | Electro-magnetic apparatus | |
| JP3228967B2 (en) | Superconducting coil | |
| JPH02264408A (en) | Gas insulated transformer | |
| JPS58118105A (en) | Foil wound type transformer | |
| JPS63274121A (en) | Mechanism for cooling coil | |
| JPS59121810A (en) | Foil-wound transformer |