JPS6014442B2 - hollow superconductor - Google Patents
hollow superconductorInfo
- Publication number
- JPS6014442B2 JPS6014442B2 JP1006081A JP1006081A JPS6014442B2 JP S6014442 B2 JPS6014442 B2 JP S6014442B2 JP 1006081 A JP1006081 A JP 1006081A JP 1006081 A JP1006081 A JP 1006081A JP S6014442 B2 JPS6014442 B2 JP S6014442B2
- Authority
- JP
- Japan
- Prior art keywords
- cooling medium
- hollow
- superconducting element
- path
- temperature
- 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
Landscapes
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
【発明の詳細な説明】
本発明は冷却媒体通路となる中空部を有する中空超電導
体に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a hollow superconductor having a hollow portion serving as a cooling medium passage.
従来のこの樋の中空超電導体は、一般に単一の中空部を
有し、これに冷却媒体を一方向に通流させる構造となっ
ている。The conventional hollow superconductor of this gutter generally has a single hollow part through which a cooling medium flows in one direction.
しかしながら、この構造のものでは中空部を通流した後
の冷却媒体を冷却装置に戻す際に冷却媒体の温度が上昇
してしまうため冷却効率が悪く、冷却装置として大容量
のものを必要とする欠点があった。また、冷却媒体は、
超電導素子に沿って一方向だけに流れるので、この冷却
媒体の上流側温度と下流側温度とに必然的に差が生じ、
これが原因して超電導素子の中心部全体を均一な温度に
冷却できない問題もあつた。本発明は上記の点に鑑みて
なされたもので、外管内に超電導素子を互いに離隔され
た2つの中空部を形成するように挿設して、それらをそ
れぞれ冷却媒体の往路、復路として用いることにより超
電導素子の中心部全体の均一冷却化および冷却効率の向
上を図った中空超電導体を提供するものである。However, with this structure, the temperature of the cooling medium increases when it returns to the cooling device after flowing through the hollow part, resulting in poor cooling efficiency and the need for a large-capacity cooling device. There were drawbacks. In addition, the cooling medium is
Since it flows in only one direction along the superconducting element, there is inevitably a difference between the upstream and downstream temperatures of this cooling medium.
This caused the problem that the entire center of the superconducting element could not be cooled to a uniform temperature. The present invention has been made in view of the above points, and involves inserting a superconducting element into the outer tube so as to form two hollow portions spaced apart from each other, and using these as an outward path and a return path for the cooling medium, respectively. This provides a hollow superconductor that achieves uniform cooling of the entire center of a superconducting element and improved cooling efficiency.
以下、本発明の実施例を図面を参照して説明する。Embodiments of the present invention will be described below with reference to the drawings.
図において1は外管であり、低温強度が高くかつ熱伝導
性の悪い、例えば厚さ0.5肋、幅32肌のSUS28
の平板を矩形管状に形成し、端面をTIG溶後したもの
である。In the figure, 1 is the outer tube, which is made of SUS28 with high low-temperature strength and poor thermal conductivity, for example, with a thickness of 0.5 ribs and a width of 32 skin.
The flat plate was formed into a rectangular tube shape, and the end surfaces were melted with TIG.
この外管1内には超電導素子2が挿通され、4個のスベ
ーサ3によって外管1内の中央部に位置するように保持
されている。超亀導素子2はそれぞれ例えば10本程度
の0.30の素線(一例として重量比でNb50%、′
ri50%の合金線)を銅によって安定化したもので、
全体として幅5凧、厚さ2脚程度の断面矩形状に形成さ
れている。そして、この超電導素子2の両側の中空部4
,5をそれぞれ冷却媒体の往路および復路としている。
上記のように機成された中空超電導体に50キロ.ガウ
スの磁界を作用させ、かつ中空部4,5に冷却媒体とし
て10k9/仇の超臨界圧Heガスを流通させ、臨界温
度以下に冷却しながら超電導素子2に通電すると、80
0アンペア程度まで抵抗値を示さず安定な超電導状態を
得ることができる。A superconducting element 2 is inserted into the outer tube 1 and held at the center of the outer tube 1 by four spacers 3. Each of the supertorque conductive elements 2 is made of, for example, about 10 wires of 0.30 (as an example, Nb 50% by weight, '
An alloy wire with an ri of 50%) stabilized with copper,
As a whole, it is formed into a rectangular cross-section with a width of about 5 kites and a thickness of about 2 legs. Hollow portions 4 on both sides of this superconducting element 2
, 5 are the forward and return paths of the cooling medium, respectively.
50 kg in the hollow superconductor constructed as above. When a Gaussian magnetic field is applied and supercritical pressure He gas of 10 k9/min is passed through the hollow parts 4 and 5 as a cooling medium, and the superconducting element 2 is energized while being cooled to below the critical temperature, 80
A stable superconducting state can be obtained with no resistance value down to approximately 0 ampere.
このように、本発明によれば外管内に超電導素子をはさ
んで互いに離隔された2つの中空部を形成し、その一方
を冷却媒体の往路とし、他方を復路としたことにより、
超電導素子の冷却効率を大幅に向上させることができる
。すなわち、本発明では復路を造流する冷却媒体が、往
路を通流する冷却媒体と超電導素子を介して熱交換を行
なうことにより、その温度上昇が極力押えられる。この
ため冷却装置としては比較的小容量のものの使用を可能
化できる。また、往路を流れる冷却媒体は、この往路の
上流側から下流側に向かうにしたがって温度上昇する。
同様に復路を流れる冷却媒体は、この復路の上流側から
下流側に向かうにしたがってさらに温度上昇する。した
がって、往路の最上流端を流れる冷却媒体と復路の最下
流端を流れる冷却媒体との温度差が最も大きく、往路の
滋下流端を流れる冷却媒体と復路の最上流端を流れる冷
却媒体との温度差が穣も小さい関係が自動的に形成され
る。そして、往路と復路とは熱交換壁とちての機能も発
揮する超電導素子によって仕切られている。したがって
、仕切り壁としての機能を果たしている超電導素子の中
心部は長手方向、つまり往路および復路に沿った方向に
均一な温度に保たれることになり、結局、超電導素子の
中心部全体を均一な温度に冷却することができ、理想的
な冷却を実現することができる。なお、上記実施例にお
けるスベーサ3は必らずしも必要でなく、外管自体を変
形させて突起を形成し、この突起により超電導素子の位
置決めと保持を行なってもよい。As described above, according to the present invention, by forming two hollow parts separated from each other by sandwiching the superconducting element in the outer tube, one of which is used as an outgoing path for the cooling medium, and the other is used as an incoming path,
The cooling efficiency of superconducting elements can be significantly improved. That is, in the present invention, the cooling medium flowing in the return path exchanges heat with the cooling medium flowing in the outgoing path via the superconducting element, thereby suppressing the temperature rise as much as possible. Therefore, it is possible to use a cooling device with a relatively small capacity. Further, the temperature of the cooling medium flowing in the outgoing path increases from the upstream side to the downstream side of the outgoing path.
Similarly, the temperature of the cooling medium flowing through the return path further increases from the upstream side to the downstream side of the return path. Therefore, the temperature difference between the cooling medium flowing at the most upstream end of the outgoing path and the cooling medium flowing at the most downstream end of the returning path is the largest, and the temperature difference between the cooling medium flowing at the downstream end of the outgoing path and the cooling medium flowing at the most upstream end of the returning path is the largest. A relationship with a small temperature difference is automatically formed. The outbound and return routes are separated by a superconducting element that also functions as a heat exchange wall. Therefore, the center of the superconducting element, which functions as a partition wall, is kept at a uniform temperature in the longitudinal direction, that is, along the outward and return paths, and as a result, the entire center of the superconducting element is maintained at a uniform temperature. It can be cooled to a certain temperature, and ideal cooling can be achieved. Note that the spacer 3 in the above embodiment is not necessarily necessary, and the outer tube itself may be deformed to form a protrusion, and the superconducting element may be positioned and held by this protrusion.
図面の簡単な説明図はこの発明の一実施例に係る中空超
電導体の断面図である。A simple explanatory diagram of the drawing is a sectional view of a hollow superconductor according to an embodiment of the present invention.
1・・・・・・外管、2・・・・・・超電導素子、3・
・・・・・スベーサ、4,5・・・・・・中空部。1...Outer tube, 2...Superconducting element, 3.
...Subesa, 4,5...Hollow part.
Claims (1)
互いに離隔された2つの中空部を形成する仕切り壁を兼
ねるように安定化された超電導素子を挿設し、上記2つ
の中空部の一方を冷却媒体の往路とし、他方を上記冷却
媒体の復路としたことを特徴とする中空超電導体。1. A stabilized superconducting element is inserted into the outer tube so as to double as a partition wall forming two hollow parts spaced apart from each other in the longitudinal direction between the inner surface of the outer pipe and the two hollow parts. A hollow superconductor characterized in that one of the sections is an outgoing path for a cooling medium, and the other is an incoming path for the cooling medium.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1006081A JPS6014442B2 (en) | 1981-01-26 | 1981-01-26 | hollow superconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1006081A JPS6014442B2 (en) | 1981-01-26 | 1981-01-26 | hollow superconductor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56123617A JPS56123617A (en) | 1981-09-28 |
| JPS6014442B2 true JPS6014442B2 (en) | 1985-04-13 |
Family
ID=11739837
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1006081A Expired JPS6014442B2 (en) | 1981-01-26 | 1981-01-26 | hollow superconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6014442B2 (en) |
-
1981
- 1981-01-26 JP JP1006081A patent/JPS6014442B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56123617A (en) | 1981-09-28 |
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