JPH0121564B2 - - Google Patents

Info

Publication number
JPH0121564B2
JPH0121564B2 JP57097398A JP9739882A JPH0121564B2 JP H0121564 B2 JPH0121564 B2 JP H0121564B2 JP 57097398 A JP57097398 A JP 57097398A JP 9739882 A JP9739882 A JP 9739882A JP H0121564 B2 JPH0121564 B2 JP H0121564B2
Authority
JP
Japan
Prior art keywords
superconducting wire
superconductor
refrigerant
oxide
oxide powder
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
Application number
JP57097398A
Other languages
Japanese (ja)
Other versions
JPS58214212A (en
Inventor
Yasuzo Tanaka
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Furukawa Electric Co Ltd
Original Assignee
Furukawa Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Furukawa Electric Co Ltd filed Critical Furukawa Electric Co Ltd
Priority to JP57097398A priority Critical patent/JPS58214212A/en
Publication of JPS58214212A publication Critical patent/JPS58214212A/en
Publication of JPH0121564B2 publication Critical patent/JPH0121564B2/ja
Granted legal-status Critical Current

Links

Classifications

    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Landscapes

  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【発明の詳細な説明】 本発明は熱伝導性に優れた強制冷却型超電導線
を提供せんとするものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention aims to provide a forced cooling type superconducting wire with excellent thermal conductivity.

従来の強制冷却型超電導線は第1図に示す如く
安定化金属3に超電導体2を内蔵した複数本の素
線1をステンレス鋼管4内に集合せしめ、該素線
1とステンレス管4との間隙部5に超臨界ヘリウ
ムを強制的に循環せしめるか又は第2図に示す如
く安定化金属3に超電導体2を複数本内蔵し中央
部に導通管6を設け、該管内に液体ヘリウムを導
入せしめて冷却せしめているものである。
A conventional forced cooling type superconducting wire, as shown in FIG. Either supercritical helium is forcibly circulated in the gap 5, or as shown in FIG. 2, a plurality of superconductors 2 are built into the stabilizing metal 3, a conduction pipe 6 is provided in the center, and liquid helium is introduced into the pipe. At least it is cooled down.

而して導体に局部的に常電導部が発生した場
合、どのようにして冷却して超電導状態に復帰せ
しめるかということである。その方法としては莫
大な量の安定化金属を複合するとか導体の表面積
を増大せしめるとか或いは導体と冷媒との間に極
薄な熱障壁材を介在せしめているものである。
If a normal conductive part is locally generated in a conductor, the problem is how to cool it and return it to a superconducting state. Methods for this include compounding large amounts of stabilizing metals, increasing the surface area of the conductor, or interposing an extremely thin thermal barrier material between the conductor and the refrigerant.

然しこれらの方法において設計段階から予測し
がたい熱発生が導体内に発生した場合、急激に冷
媒が沸騰し超電導体からの大電流が常電導体に分
流しきれない場合超電導体や導体の全体が溶断す
るという大きな事故となる。
However, when using these methods, if heat generation occurs inside the conductor that cannot be predicted from the design stage, the refrigerant boils suddenly and the large current from the superconductor cannot be diverted to the normal conductor, causing damage to the entire superconductor or conductor. This could lead to a major accident in which the gas melts down.

本発明はかかる欠点を改善せんとして鋭意研究
を行つた結果、強制冷却型超電導体と冷媒との熱
伝導率を改善し、如何なる状態においても溶断し
ない超電導体からなる超電導線を見出したもので
ある。即ち本発明は強制冷却型超電導線におい
て、酸化物粉体内に超電導体を埋込み且つ少くと
も1個の冷媒連通管を設けたものである。
The present invention has been made as a result of extensive research aimed at improving these drawbacks, and has resulted in the discovery of a superconducting wire made of a superconductor that improves the thermal conductivity between a forced cooling superconductor and a refrigerant and does not melt under any conditions. . That is, the present invention provides a forced cooling type superconducting wire in which a superconductor is embedded in oxide powder and at least one refrigerant communication pipe is provided.

本発明超電導体を図面により説明する。第3図
に示す如く超電導体2が安定化金属3内に埋込ま
れた複数本の素線1をステンレス管などの圧力管
4内に収納し、更に圧力管内に冷媒8の通路とな
る微多孔質導通管9を設け且つ酸化物粉7を充填
したものである。
The superconductor of the present invention will be explained with reference to the drawings. As shown in FIG. 3, a superconductor 2 has a plurality of wires 1 embedded in a stabilizing metal 3, which are housed in a pressure tube 4 such as a stainless steel tube, and further inside the pressure tube there is a fine wire that serves as a passage for a refrigerant 8. A porous conduction pipe 9 is provided and oxide powder 7 is filled.

この超電導体はNbTi合金の如き合金超電導体
又はNb3Sn、V3Gaの如き化合物超電導体でもよ
い。
The superconductor may be an alloy superconductor such as a NbTi alloy or a compound superconductor such as Nb 3 Sn, V 3 Ga.

又、安定化金属としては高導電性であることが
望ましくCu、Al、Agなどがよく、必要に応じて
ブロンズ、キユプロニツケルなでの合金材料と複
合したものでもよい。
Further, the stabilizing metal preferably has high conductivity, preferably Cu, Al, Ag, etc., and may be composited with an alloy material such as bronze or Cypronickel if necessary.

なお、本発明においては必ずしも大量の安定化
金属を設ける必要はない。
Note that in the present invention, it is not necessarily necessary to provide a large amount of stabilizing metal.

又圧力管としてはマグネツト巻線における電磁
力に耐え且つ冷媒圧(10〜20Kg/cm2)に耐えると
共に水や大気に対し優れた耐蝕性を有することが
必要である。
Further, the pressure pipe must be able to withstand the electromagnetic force in the magnet winding, withstand the refrigerant pressure (10 to 20 kg/cm 2 ), and have excellent corrosion resistance against water and the atmosphere.

又、導通管としては非磁性以外に材質面での制
限はないがその周面に多数の微孔を設けてあり、
冷媒を滲出せしめるようにしてある。この導通管
は通常超電導線の長手方向に導通するものである
が、径方向に導通せしめてもよい。更にその位置
は導体の中央に設ける必要はなく、且つ1本以上
ならば本数に制限はない。
In addition, there are no restrictions on the material used for the conduction tube other than non-magnetic material, but there are many fine holes on the circumference.
It is designed to allow the refrigerant to seep out. This conduction tube normally conducts in the longitudinal direction of the superconducting wire, but it may conduct in the radial direction. Furthermore, the position does not need to be provided in the center of the conductor, and there is no limit to the number of conductors as long as there is one or more.

又酸化物としてはAl2O3、BeO、CuOなど何れ
でもよく、酸化物の熱伝導率は密度、温度領域、
不純物含有量、熱源との密着接続性などによつて
10〜100倍程度変化するものである。
The oxide may be any of Al 2 O 3 , BeO, CuO, etc., and the thermal conductivity of the oxide depends on the density, temperature range,
Depending on impurity content, close connection with heat source, etc.
It changes by about 10 to 100 times.

次に本発明の実施例について説明する。中央部
にNbバリセーを介して無酸素銅の外側に100000
本のNbコアを内蔵したブロンズマトリツスから
構成された1.69mmφの複合線をえた。この素線57
本と+100メツシユのAl2O3粉とBeO粉との1:
1混合粉とを肉厚0.8mm;外径10×25mmのSUS管
内に収納した。又該管の中央部には、予め周面に
150メツシユ相当の微孔を多数設けた内径3mmφ、
外径3.5mmφの軟銅連通管を挿着した。
Next, examples of the present invention will be described. 100,000 on the outside of oxygen-free copper through Nb Valise in the center
We obtained a 1.69mmφ composite wire made of bronze matrix with a built-in Nb core. This wire 57
Book and +100 mesh Al 2 O 3 powder and BeO powder 1:
1 mixed powder was housed in a SUS tube with a wall thickness of 0.8 mm and an outer diameter of 10 x 25 mm. In addition, in the center of the tube, there is a
Inner diameter 3mmφ with many micro holes equivalent to 150 mesh,
An annealed copper communication tube with an outer diameter of 3.5 mmφ was inserted.

然る後アルゴン雰囲気において700℃×100Hr
加熱しNbとブロンズとの界面にNb3Snを形成し
本発明超電導線をえた。
After that, 700℃×100Hr in argon atmosphere.
The superconducting wire of the present invention was obtained by heating to form Nb 3 Sn at the interface between Nb and bronze.

又本発明と比較するために酸化物粉を全く使用
することなく、その他はすべて同様にして比較例
超電導線をえた。
In addition, for comparison with the present invention, a comparative superconducting wire was obtained in the same manner except that no oxide powder was used.

これらの超電導線について800mmφのパンケー
キコイルとして1.8K超臨界ヘリウムを循環せし
め外部磁界12Tにおける臨界電流値を測定した。
For these superconducting wires, 1.8K supercritical helium was circulated as a pancake coil of 800 mmφ, and the critical current value was measured in an external magnetic field of 12 T.

本発明においては第1回目の通電で35000A、
第2回以降も35000±100Aの範囲にて安定した状
態で通電可能であつた。又磁界の変動に対しても
極めて安定な導体であつた。
In the present invention, the first energization is 35000A,
Even after the second test, it was possible to conduct electricity stably within the range of 35,000±100A. It was also an extremely stable conductor against fluctuations in the magnetic field.

一方比較例においては第1回目の通電で
21050Aまで通電しえたが、常電導状態に転移す
る過程でヘリウム圧力が異常を示し、第2回目の
通電においては5000A以上で温度の上昇が著しく
通電不可能となつた。第3回目以降も5000A以上
の通電は出来なかつた。
On the other hand, in the comparative example, at the first energization
Although it was possible to energize up to 21,050A, the helium pressure showed an abnormality during the transition to the normal conduction state, and on the second energization, the temperature rose significantly above 5,000A, making it impossible to energize. Even after the third attempt, it was not possible to pass current of more than 5000A.

以上詳述した如く本発明によれば次の如き効果
を有するものである。
As detailed above, the present invention has the following effects.

(1) 超電導状態から常電導状態への転移の際の発
熱を効率よく冷媒に伝達する。
(1) Efficiently transfer the heat generated during the transition from the superconducting state to the normal conducting state to the refrigerant.

(2) 超電導線の周辺の安定化金属量が減少できる
ため導体の電流密度を高くできる。
(2) Since the amount of stabilizing metal around the superconducting wire can be reduced, the current density of the conductor can be increased.

(3) 素線間の電気的絶縁性が向上する。(3) Electrical insulation between wires is improved.

(4) 高温加熱時の素線の接合や融着を防止するこ
とが出来ると共に可撓性のケーブルになる。
(4) It is possible to prevent the joining and fusing of wires during high-temperature heating, and the cable becomes flexible.

(5) 酸化物の粒子を細かくし超臨界ヘリウムの物
性から粒子の間隙にヘリウムを十分に浸透させ
ることができる。
(5) By making the oxide particles finer and using the physical properties of supercritical helium, it is possible to sufficiently infiltrate helium into the gaps between the particles.

【図面の簡単な説明】[Brief explanation of drawings]

第1図及び第2図は従来の超電導線の1例を示
す概略説明図、第3図は本発明超電導線の1例を
示す概略説明図である。 1……素線、2……超電導体、3……安定化金
属、4……圧力管、5……間隙部、6……導通
管、7……酸化物粉、8……冷媒、9……微多孔
質導通管。
1 and 2 are schematic explanatory diagrams showing an example of a conventional superconducting wire, and FIG. 3 is a schematic explanatory diagram showing an example of the superconducting wire of the present invention. DESCRIPTION OF SYMBOLS 1...Element wire, 2...Superconductor, 3...Stabilizing metal, 4...Pressure tube, 5...Gap, 6...Conducting tube, 7...Oxide powder, 8...Refrigerant, 9 ...Microporous conduction tube.

Claims (1)

【特許請求の範囲】 1 強制冷却型超電導線において、酸化物粉体内
に複数本の超電導体を埋込むと共に冷媒滲出孔を
有する少なくとも1本の冷媒連通管を設けたこと
を特徴とする超電導線。 2 超電導体が高導電性金属を介して酸化物粉体
内に埋込まれていることを特徴とする特許請求の
範囲第1項記載の超電導線。 3 酸化物粉体が酸化アルミニウム、酸化ベリリ
ウムからなることを特徴とする特許請求の範囲第
1項記載の超電導線。
[Scope of Claims] 1. A forced cooling type superconducting wire, characterized in that a plurality of superconductors are embedded in oxide powder and at least one refrigerant communication pipe having a refrigerant seepage hole is provided. . 2. The superconducting wire according to claim 1, wherein the superconductor is embedded in oxide powder via a highly conductive metal. 3. The superconducting wire according to claim 1, wherein the oxide powder is made of aluminum oxide or beryllium oxide.
JP57097398A 1982-06-07 1982-06-07 Superconductive conductor Granted JPS58214212A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57097398A JPS58214212A (en) 1982-06-07 1982-06-07 Superconductive conductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57097398A JPS58214212A (en) 1982-06-07 1982-06-07 Superconductive conductor

Publications (2)

Publication Number Publication Date
JPS58214212A JPS58214212A (en) 1983-12-13
JPH0121564B2 true JPH0121564B2 (en) 1989-04-21

Family

ID=14191407

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57097398A Granted JPS58214212A (en) 1982-06-07 1982-06-07 Superconductive conductor

Country Status (1)

Country Link
JP (1) JPS58214212A (en)

Also Published As

Publication number Publication date
JPS58214212A (en) 1983-12-13

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