JPS6025841B2 - compound superconductor - Google Patents
compound superconductorInfo
- Publication number
- JPS6025841B2 JPS6025841B2 JP53081090A JP8109078A JPS6025841B2 JP S6025841 B2 JPS6025841 B2 JP S6025841B2 JP 53081090 A JP53081090 A JP 53081090A JP 8109078 A JP8109078 A JP 8109078A JP S6025841 B2 JPS6025841 B2 JP S6025841B2
- Authority
- JP
- Japan
- Prior art keywords
- compound
- reinforcing material
- sectional area
- cross
- superconductor
- 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
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Classifications
-
- Y—GENERAL 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
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment
Landscapes
- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
【発明の詳細な説明】
本発明は化合物超電導体、特に化合物超電導線と補強材
とが金属的に接着されて一体化機造をなす化合物超電導
体に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a compound superconductor, and particularly to a compound superconductor in which a compound superconducting wire and a reinforcing material are metallically bonded to form an integrated structure.
ニオブ3−錫(N広Sn)、バナジウム3ーガリゥム(
V3Ga)などの化合物超電導材料は、高磁界ですぐれ
た超電導性を有するので、核融合装置のマグネット材料
として注目されているが、ニッケル・チタンなどのよう
な合金系超電導材料に比べ脆弱であるため、現状では強
大な電磁応力の加わる大型高磁界マグネットは作られて
いない。Niobium 3-tin (N-HiroSn), vanadium 3-gallium (
Compound superconducting materials such as V3Ga) have excellent superconductivity in high magnetic fields and are attracting attention as magnet materials for nuclear fusion devices, but they are weaker than alloy-based superconducting materials such as nickel and titanium. Currently, large, high-field magnets that are subject to strong electromagnetic stress have not been manufactured.
化合物超電導材料を用いた化合物超電導体としては、例
えば第1図および第2図に示すような構造のものが提案
されている。こられの図において、1は補強材、2は超
電導形成用材料、3は化合物超電導層、4はマトリック
ス、5は低融点金属である。すなわち、第1図に示すも
のは化合物超電導層3の形成されている撚線の中心部に
タングステンやステンレス鋼などの補強材1を入れてあ
り、第2図に示すものは補強材1を化合物超電導層3の
内部に内蔵した構造になっている。しかし、本発明者ら
が各種構造の化合物超電導体について研究を行った結果
、第1図の如き、撚線構造では本質的に強度が弱く、液
体ヘリウム中における磁界−電流−荷重重量試験におい
ても小さな応力で臨界電流の劣化が生じはじめることが
明らかとなり、また、第2図の如く補強材を化合物超電
導層の内部に内属する構造では、複合体としての成型加
工性が極めて悪く、大電流容量化合物超電導体を製作で
きないことが明らかとなった。本発明は、このような問
題点を除去し、強大な電磁応力に対しても磁界電流の劣
化がなく、電流密度の高い化合物超電導体を提供するこ
とを目的とするもので、化合物超電導線とこの化合物超
電導線より高強度、高騰性率を有する材料よりなる補強
材とが金属的に接着された一体化構造をなす化合物超電
導体において、前記化合物超電導線が表面にニオブ3一
錫化合物超電導層の形成されたニオブ線を複数本組み合
せた化合物多心線が銅マトリックス中に複数本埋込され
た板状体よりなり、前記補強材が鋼被覆ステンレス鋼板
よりなり、かつ前記化合物超電導体の全横断面に対する
補強材の横断面積(以下、全横断面積および横断面積を
それぞれ全断面積および断面積と称する。As compound superconductors using compound superconducting materials, structures such as those shown in FIGS. 1 and 2, for example, have been proposed. In these figures, 1 is a reinforcing material, 2 is a superconducting material, 3 is a compound superconducting layer, 4 is a matrix, and 5 is a low melting point metal. That is, in the case shown in Fig. 1, a reinforcing material 1 such as tungsten or stainless steel is placed in the center of the stranded wire where the compound superconducting layer 3 is formed, and in the case shown in Fig. 2, the reinforcing material 1 is made of a compound. It has a structure built inside the superconducting layer 3. However, as a result of research conducted by the present inventors on compound superconductors with various structures, it was found that the strength of the twisted wire structure as shown in Figure 1 is inherently low, and even in magnetic field-current-load weight tests in liquid helium. It has become clear that the critical current begins to deteriorate with a small stress, and the structure in which the reinforcing material is included inside the compound superconducting layer as shown in Figure 2 has extremely poor moldability as a composite, resulting in a large current capacity. It became clear that compound superconductors could not be produced. The present invention aims to eliminate such problems and provide a compound superconductor with high current density and no deterioration of magnetic field current even under strong electromagnetic stress. In a compound superconductor having an integrated structure in which a reinforcing material made of a material having higher strength and higher soaring rate than the compound superconducting wire is metallically bonded, the compound superconducting wire has a niobium tritin compound superconducting layer on the surface. The compound superconductor is made of a plate-like body in which a plurality of compound multi-core wires are embedded in a copper matrix, and the reinforcing material is made of a steel-coated stainless steel plate, and the entire compound superconductor is The cross-sectional area of the reinforcement relative to the cross-sectional area (hereinafter, the total cross-sectional area and the cross-sectional area are referred to as the total cross-sectional area and the cross-sectional area, respectively.
)の比率が20〜50パーセントであることご特徴とす
るものである。すなわち、本発明は化合物超電導線とこ
の化合物超電導線より高強度、高弾性率を有する材料よ
りなる補強材とを金属的に後着た一体化構造を用いるこ
とが目的達成のためには最も適しており、この化合物超
電導体の全断面積に対する補強材の断面積の比率を大き
くすことが必要である点に想到してなされたものである
。) is characterized by a ratio of 20 to 50%. That is, in order to achieve the purpose of the present invention, it is most suitable to use an integrated structure in which a compound superconducting wire and a reinforcing material made of a material having higher strength and higher elastic modulus than the compound superconducting wire are attached metallically. This was done based on the idea that it is necessary to increase the ratio of the cross-sectional area of the reinforcing material to the total cross-sectional area of the compound superconductor.
ここで、補強材に用いられる化合物超電導線より高強度
、高弾性率を有する材料にはステンレス鋼、タングステ
ンなどがあり、これらの化合物超電導線と補強材とを金
属的に接着された‐一体化構造とするには、銀ろう、圧
暖、溶接等の方法が用いられる。Here, there are materials such as stainless steel and tungsten that have higher strength and higher elastic modulus than the compound superconducting wire used as the reinforcing material. Methods such as silver soldering, pressure heating, and welding are used to construct the structure.
このような構造にすることによって、化合物超電導線と
補強材は、大きな電磁応力に対して、それぞれ独立に変
形挙動を生ずることなく、強固な一体化構造の化合物超
電導体として挙動する。With such a structure, the compound superconducting wire and the reinforcing material behave as a compound superconductor with a strong integrated structure without independently deforming in response to large electromagnetic stress.
なお、化合物超電導線と補強材を強固に金属的に接着さ
せるためには、補強材として単体のものよりも、例えば
銅とステンレス鋼とのクラッド材の如き複合補強材を用
いることが望ましい。また、本発明者者らの補強材の比
率(補強材断面積/化合物超電導体の全面積)を種々変
えて磁界−電流−力持性を測定した結果は、強材の比率
が20%未満では20〜30k9/柵の応力で臨界電流
が劣化し、補強材挿入の効果が少なく、また、補強材の
比率を20%以上にしていくと顕著に補強効果が現われ
、耐ストレス性は向上するが、50%以上では明らかに
超電導体全体の電流密度が低下することを示していた。In order to firmly bond the compound superconducting wire and the reinforcing material metallically, it is preferable to use a composite reinforcing material, such as a cladding material of copper and stainless steel, rather than a single reinforcing material. In addition, the results of measuring the magnetic field-current-force holding property by varying the ratio of reinforcing material (cross-sectional area of reinforcing material/total area of compound superconductor) by the present inventors show that when the ratio of reinforcing material is less than 20%, 20~30k9/The critical current deteriorates due to the stress of the fence, and the effect of reinforcing material insertion is small.Also, when the ratio of reinforcing material is increased to 20% or more, the reinforcing effect becomes noticeable and the stress resistance improves, but , 50% or more, it was clearly shown that the current density of the entire superconductor decreases.
従って、補強材の材質によって多少異なるが、大型高磁
界マグネットで負荷される電磁力に対して臨界電流が劣
化せず、かつ流密度の高い化合物超蚤導体して20〜5
0%の強材が有効であることがわかった。Therefore, although it varies somewhat depending on the material of the reinforcing material, a compound superconductor with a critical current that does not deteriorate against the electromagnetic force applied by a large, high-field magnet and has a high current density is used.
It was found that 0% reinforcement is effective.
なお、補強材の比率を単に20〜50%と増加しても化
合物超電導体の耐ストレス性に対しては効果が少なく、
化合物超電導線と補強材とが金属的に十分後着され、化
合物超電導体して一体的に挙動し得る構成にするとによ
って、はじめて20〜50q○の補強材挿入効果が発揮
される。Note that simply increasing the ratio of reinforcing material to 20 to 50% has little effect on the stress resistance of the compound superconductor;
The effect of inserting 20 to 50 q○ of reinforcing material can only be exhibited when the compound superconducting wire and the reinforcing material are sufficiently metallically attached to form a structure that can behave as a compound superconductor as one.
以下、実施例について説明する。Examples will be described below.
第3図は一実施例の構成を示すもので、こで用いられて
いる化合物超電導線6は超電導形成材料としてNb、銅
−錫(Cu−Sn)合金を用い安定化金属としてCuを
用いたNb3Sn化合物超電導体よりなり、具体的には
外寸法が2.16物×IQ奴の平角状のCuよりなるマ
トリックス7の中に、Cu−Sn被覆された外径5仏m
のNb線331本を押込んだ化合物多心線8をさらに2
04本組合せ埋込み、成形後700qCで10独特間真
空中で熱処理し、Nb線の表面に厚さ1仏mのN広Su
化合物超電導層を形成させたものであり、補強材1はC
u被覆ステンレス鋼を用い、化合物超電導線6と補強材
1とを鉛−錫(Pb−Sn)はんだ9で俵合たものであ
る。FIG. 3 shows the configuration of an example. The compound superconducting wire 6 used here uses Nb and a copper-tin (Cu-Sn) alloy as superconducting materials, and Cu as a stabilizing metal. A matrix 7 made of Nb3Sn compound superconductor, specifically, rectangular Cu with external dimensions of 2.16 x IQ, is covered with Cu-Sn and has an outer diameter of 5 mm.
2 more compound multi-core wires 8 into which 331 Nb wires were pressed
After embedding the 04 wires in combination and molding, heat treatment was performed in a vacuum at 700 qC for 10 hours, and a Nb Su film with a thickness of 1 French was applied to the surface of the Nb wires.
A compound superconducting layer is formed, and the reinforcing material 1 is C
U-coated stainless steel is used, and a compound superconducting wire 6 and a reinforcing material 1 are bonded together with lead-tin (Pb-Sn) solder 9.
また、本実例では、線村全断面積に対する比率が0〜5
0%にあたるステンレス鋼補強材を各用意し、それぞれ
上述のNはSn化合物超電導線にPb−Snはんだで接
合して試料とし、4.2Kで力を加えない状態、および
力を加えた状態につき、60KOeの磁界中で臨界電流
を側定た。In addition, in this example, the ratio to the total cross-sectional area of the line village is 0 to 5.
0% stainless steel reinforcing material was prepared, and the above-mentioned N was bonded to Sn compound superconducting wire with Pb-Sn solder as a sample. , the critical current was determined in a magnetic field of 60 KOe.
第4図は応力を変化せて臨界電流がどのように変化する
かについて測定した結果で、機軸、縦軸には、それぞれ
応力(k9/地)、力下における臨界電流と応力かない
状態における臨界電流の比(%)がとってあり、Aは補
強材が無い場合、Bは補強材の比率が20%の場合、C
は補強材の比率が24%の場合と例示している。Figure 4 shows the results of measuring how the critical current changes with varying stress. The machine axis and the vertical axis respectively show the stress (k9/earth), the critical current under force, and the critical current under no stress. The current ratio (%) is taken, A is when there is no reinforcing material, B is when the ratio of reinforcing material is 20%, C
exemplifies the case where the ratio of reinforcing material is 24%.
この図から明らかなように、応力が増大して行くと、あ
る応力で臨界電流は急激に劣化する。この時の力を臨界
力として、各試料の補強材断面積/全断面積に対する関
係を示したのが第5図で、機軸、縦軸にはそれぞれ、補
強材断面積/全断面積(%)、臨界応力(X9/柵)が
とってある。この図は補強材断面積/全断面積が20%
以上になると臨界応力が急激に増大することを示してい
る。すなわち、補強効果を有効ならしめるには、補強材
断面積/全断面積を20%以上にする必要があることを
示している。第6図は150k9/柵の力を負荷したき
の臨界電流を示したもので、機軸、縦軸にはそれぞれ、
補強材断面積/全断面積(%)、臨界電流(A)がとっ
てある。As is clear from this figure, as the stress increases, the critical current rapidly deteriorates at a certain stress level. Figure 5 shows the relationship between the cross-sectional area of the reinforcement material and the total cross-sectional area of each sample with the force at this time as the critical force. ), the critical stress (X9/fence) is taken. In this figure, the reinforcement cross-sectional area/total cross-sectional area is 20%.
This indicates that the critical stress increases rapidly when the value exceeds this value. In other words, it is shown that in order to make the reinforcing effect effective, the cross-sectional area of the reinforcing material/total cross-sectional area needs to be 20% or more. Figure 6 shows the critical current when a force of 150k9/fence is applied, and the mechanical and vertical axes are shown, respectively.
Reinforcement material cross-sectional area/total cross-sectional area (%) and critical current (A) are taken.
補強材が24%以上では7000〜720Mとほぼ同様
の臨界電流を示しているが、補強材が20%のきは68
0M、補強材が無に場合には29山Aまで劣化している
。第7図は第6図の縦軸を臨界電流密度(A/協)で書
き直した図で、この図は補強材断面積/全断面積が30
%付近で臨界電流密度がピークを持っていることを示し
ている。超電導マグネットにおいては、臨界電流密度は
大きい程望ましい。従って、補強効果が大でかつ臨界電
流密度を大ならしめる補強材補強材断面積/全断面積は
20〜50%の範囲になる。また、第6図において、補
強材断面積/全断面積が20%以上、’24%未満では
、わずかながら臨界電流の劣化が認められることから、
臨界電流の劣化の無い状態、すなわち補強材材断面積/
全断面積が24〜36%であることがさらに望ましい。
すなわち、この範囲を選べば超電導体の応力による電流
劣化を最小限にし、さらに線材全体の電流密度の低下を
おさえることができる。また、本実施例では補強材をは
んだを用いて結合する例を示したが、圧薮、溶接等他の
方法でも金属的に接着されて一体化構造となるものであ
れば同様に使用できる。When the reinforcing material is 24% or more, the critical current is almost the same as 7000-720M, but when the reinforcing material is 20%, the critical current is 68
In the case of 0M and no reinforcing material, it deteriorated to 29 peaks A. Figure 7 is a diagram in which the vertical axis of Figure 6 is rewritten as critical current density (A/Kyo), and this figure shows that the cross-sectional area of the reinforcing material/total cross-sectional area is 30
It shows that the critical current density has a peak around %. In a superconducting magnet, a higher critical current density is more desirable. Therefore, the cross-sectional area/total cross-sectional area of the reinforcing material that has a large reinforcing effect and increases the critical current density is in the range of 20 to 50%. In addition, in Fig. 6, when the cross-sectional area of the reinforcing material/total cross-sectional area is 20% or more and less than 24%, a slight deterioration of the critical current is observed.
Condition without deterioration of critical current, i.e. cross-sectional area of reinforcing material /
More preferably, the total cross-sectional area is 24-36%.
That is, by selecting this range, current deterioration due to stress in the superconductor can be minimized, and furthermore, a decrease in the current density of the entire wire can be suppressed. Further, although this embodiment shows an example in which the reinforcing material is bonded using solder, other methods such as pressure bushing or welding can be similarly used as long as the reinforcing material is bonded metallically to form an integrated structure.
このように、実施例記載の化合物超電導体は、線材全体
の断面積に対し最適補強材断面積を与えるため、大電流
量線材とし耐ストレス性と高電流密度とをそなえた線材
を造でき、従って、この大電流容量の化合物超電導体を
巻回した超電導コイルは大型化、高磁界化が容易で高電
流密度のため、経済的利点も大い。以上の如く、本発明
の化合物超電導体は、強大な電磁力に対しても臨界電流
の劣化がなく、電流密度の高い化合物超電導体を提供す
るもので、工業的効果の大なるのである。In this way, the compound superconductor described in the examples provides an optimal cross-sectional area of the reinforcing material with respect to the cross-sectional area of the entire wire, so it is possible to produce a wire with high current capacity and stress resistance and high current density. Therefore, a superconducting coil wound with a compound superconductor having a large current capacity can easily be made large and have a high magnetic field, and has a high current density, so it has great economic advantages. As described above, the compound superconductor of the present invention has great industrial effects because it provides a compound superconductor with high current density without deterioration of critical current even under strong electromagnetic force.
第1図および第2図は従来のそれぞれ異なる化合物超弦
導体の横断面図、第3図は本発明化合物超電導体の一実
施例の横断面図、第4図は本発明化合物超電導体におけ
る力と臨界電流との関係を示す特性線図、5図は同じく
補強材補強材断面積/全断面積と臨界力との関係を示す
特性線図、第6図は同じく補強材断面積/全断面積と臨
界電流との関係を示す特性線図、第7図は同じく補強材
断面積/全断面積と臨界電流密度との関係を示す特性線
図である。
1・・・…補強材、6・・・化合物超電導線、7・・・
Cuマトリックス、8・・…・化合物多心線、9・・…
・Pb−Snはんだ。
髪ー図
第2図
第3図
第4図
努S図
第5図
菊7図Figures 1 and 2 are cross-sectional views of different conventional compound superstring conductors, Figure 3 is a cross-sectional view of an embodiment of the compound superconductor of the present invention, and Figure 4 is the force in the compound superconductor of the present invention. Figure 5 is a characteristic diagram showing the relationship between reinforcement cross-sectional area/total cross-sectional area and critical force, and Figure 6 is a characteristic diagram showing the relationship between reinforcement cross-sectional area/total cross-sectional area and critical force. FIG. 7 is a characteristic diagram showing the relationship between area and critical current, and FIG. 7 is a characteristic diagram showing the relationship between reinforcing material cross-sectional area/total cross-sectional area and critical current density. 1... Reinforcement material, 6... Compound superconducting wire, 7...
Cu matrix, 8... Compound multi-core wire, 9...
・Pb-Sn solder. Hair Figure 2 Figure 3 Figure 4 Tsutomu S Figure 5 Chrysanthemum Figure 7
Claims (1)
弾性率を有する材料よりなる補強材とが金属的に接着さ
れた一体化構造をなす化合物超電導体において、前記化
合物超電導線が表面にニオブ3−錫化合物超電導層の形
成されたニオブ線を複数本組み合せた化合物多心線が銅
マトリツクス中に複数本埋込まれた板状体よりなり、前
記補強材が銅被覆ステンレス銅板よりなり、かつ前記化
合物超電導体の全横断面積に対する前記補強材の横断面
積の比率が20〜50パーセントであることを特徴とす
る化合物超電導体。 2 前記化合物超電導体の全横断面積に対する前記補強
材の横断面積に対する前記補強材の横断面積の比率が2
4〜36パーセントである特許請求の範囲第1項記載の
化合物超電導体。[Scope of Claims] 1. In a compound superconductor having an integrated structure in which a compound superconducting wire and a reinforcing material made of a material having higher strength and higher elastic modulus than the compound superconducting wire are metallically bonded, The wire is made of a plate-shaped body in which a plurality of compound multi-core wires, which are a combination of a plurality of niobium wires each having a niobium tri-tin compound superconducting layer formed on the surface thereof, are embedded in a copper matrix, and the reinforcing material is copper-coated stainless steel. A compound superconductor made of a copper plate, characterized in that the ratio of the cross-sectional area of the reinforcing material to the total cross-sectional area of the compound superconductor is 20 to 50 percent. 2 The ratio of the cross-sectional area of the reinforcing material to the total cross-sectional area of the compound superconductor to the cross-sectional area of the reinforcing material is 2.
A compound superconductor according to claim 1, which has a content of 4 to 36 percent.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP53081090A JPS6025841B2 (en) | 1978-07-04 | 1978-07-04 | compound superconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP53081090A JPS6025841B2 (en) | 1978-07-04 | 1978-07-04 | compound superconductor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS559326A JPS559326A (en) | 1980-01-23 |
| JPS6025841B2 true JPS6025841B2 (en) | 1985-06-20 |
Family
ID=13736682
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP53081090A Expired JPS6025841B2 (en) | 1978-07-04 | 1978-07-04 | compound superconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6025841B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62115046U (en) * | 1986-01-10 | 1987-07-22 |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| FR2874451B1 (en) * | 2004-08-17 | 2006-10-20 | Nexans Sa | COMPOSITE CONDUCTOR WITH MULTIFILAMENTARY BRINS SUPERCONDUCTING |
| JP2008282584A (en) * | 2007-05-08 | 2008-11-20 | Sumitomo Electric Ind Ltd | Superconducting tape and manufacturing method thereof |
-
1978
- 1978-07-04 JP JP53081090A patent/JPS6025841B2/en not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62115046U (en) * | 1986-01-10 | 1987-07-22 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS559326A (en) | 1980-01-23 |
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