JPH05109324A - Superconductive conductor - Google Patents

Superconductive conductor

Info

Publication number
JPH05109324A
JPH05109324A JP3264551A JP26455191A JPH05109324A JP H05109324 A JPH05109324 A JP H05109324A JP 3264551 A JP3264551 A JP 3264551A JP 26455191 A JP26455191 A JP 26455191A JP H05109324 A JPH05109324 A JP H05109324A
Authority
JP
Japan
Prior art keywords
wire
conductor
type
rods
superconducting
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.)
Granted
Application number
JP3264551A
Other languages
Japanese (ja)
Other versions
JP3363164B2 (en
Inventor
Takaaki Sasaoka
高明 笹岡
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.)
Hitachi Cable Ltd
Original Assignee
Hitachi Cable 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 Hitachi Cable Ltd filed Critical Hitachi Cable Ltd
Priority to JP26455191A priority Critical patent/JP3363164B2/en
Publication of JPH05109324A publication Critical patent/JPH05109324A/en
Application granted granted Critical
Publication of JP3363164B2 publication Critical patent/JP3363164B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related 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)

Abstract

PURPOSE:To improve the required current density of a large-current capacity conductor comprising oxide superconducting wire-rods used therein. CONSTITUTION:For superconducting wire-rods 1 composing an assembled conductor are used wire rods of two kinds consisting of a type A and a type B, for example, tape-shaped wire-rods 1a and 1b each comprising an Ag coat 3 applied to a core 2 made of a Tl group oxide superconductor. Then 50 sheets of the type A wire-rods 1a are used on each of two surface-sides of the assembled conductor and 50 sheets of the type B wire-rods 1b on the inner side thereof to be laminated upon one another, and then a small-diameter lead-wire 4 is wound round the periphery of the resulting laminate to assemble these wire-rods into the conductor.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、酸化物系超電導線材を
用いた集合導体に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an aggregate conductor using an oxide-based superconducting wire.

【0002】[0002]

【従来の技術】超電導導体の電流大容量化を目的として
超電導線材を集合化して導体とすることがある。
2. Description of the Related Art Superconducting wires are sometimes assembled into a conductor for the purpose of increasing the current capacity of the superconducting conductor.

【0003】超電導線材は磁場(B)によって流し得る
電流密度(Jc)が変化する。このJc−B特性は、超
電導線材の材料又は温度によっても異なり、同系の材料
であっても熱処理条件や添加剤の差によって大きく異な
ることがある。また、酸化物系超電導線材は現在開発の
途上にあるが、添加剤、配合比、熱処理条件、減面加工
条件等の差でJc−B特性のみならず、Jc以上の電流
密度下における抵抗値も異なる。
The current density (Jc) that can flow in the superconducting wire changes depending on the magnetic field (B). The Jc-B characteristics differ depending on the material or temperature of the superconducting wire, and even the materials of the same system may differ greatly depending on the heat treatment conditions and the difference in additives. Also, although oxide-based superconducting wire is currently under development, not only the Jc-B characteristics but also the resistance value under the current density of Jc or more due to the difference in additives, compounding ratio, heat treatment conditions, surface-reduction processing conditions, Is also different.

【0004】[0004]

【発明が解決しようとする課題】酸化物系超電導線材の
臨界電流(Ic)は数mTの弱い磁場中ですら低下する
ことが知られている。従って、酸化物系超電導線材を集
合化して電流大容量化を図る場合においても、導体通電
による自己磁界値によって集合導体としてのIcが制約
されてしまう。
It is known that the critical current (Ic) of an oxide-based superconducting wire decreases even in a weak magnetic field of several mT. Therefore, even when the oxide-based superconducting wires are assembled to increase the current capacity, the self magnetic field value due to conduction of the conductor restricts the Ic as the assembled conductor.

【0005】このような超電導導体を設計する場合、各
素線の磁界ー臨界電流密度(Jc−B特性)としては同
質のものを使う場合が多い。しかし、導体断面の自己磁
界分布は均一にはならず、Jc−B特性の同じ線材を束
ねることは、集合導体としてのIcを高める最良の手法
とはいえない。
When designing such a superconducting conductor, in many cases, the same magnetic field-critical current density (Jc-B characteristic) is used for each wire. However, the self-magnetic field distribution in the conductor cross section is not uniform, and bundling wires having the same Jc-B characteristics is not the best method for increasing Ic as a collective conductor.

【0006】本発明の目的は、酸化物系超電導線材を用
いた電流大容量導体の所要電流密度を向上させることの
できる超電導導体を提供することにある。
An object of the present invention is to provide a superconducting conductor capable of improving the required current density of a large-current conductor using an oxide-based superconducting wire.

【0007】[0007]

【課題を解決するための手段】本発明の要旨は、酸化物
系超電導線材集合導体の構成法として、運転時に加わる
自己磁界分布に応じてJc−B特性の異なる複数種の酸
化物系超電導線材を用いて断面を構成したことにある。
即ち、自己磁界の大きくなる断面の位置に高磁場低電流
型の線材を用い、自己磁界の小さくなる断面の位置に低
磁場高電流型の線材を配置したことにある。
The gist of the present invention is, as a method of constructing an oxide-based superconducting wire aggregate conductor, a plurality of types of oxide-based superconducting wires having different Jc-B characteristics depending on the self-magnetic field distribution applied during operation. The cross section was constructed using.
That is, the high magnetic field low current type wire rod is used at the position of the cross section where the self magnetic field becomes large, and the low magnetic field high current type wire rod is arranged at the position of the cross section where the self magnetic field becomes small.

【0008】この場合、超電導線材としては、例えばY
−Ba−Cu−O、Bi−Sr−Cu−O、Bi−Sr
−Ca−Cu−O、Tl−Ba−Cu−O、Tl−Ba
−Ca−Cu−O、Tl−Sr−Ca−Cu−O、La
−Na−Cu−O、La−Ba−Cu−O、La−Sr
−Cu−O等の酸化物系超電導体にAg、Cu、Al、
それらを主体とした合金等の常電導体からなる被覆を施
したものが用いられるが、Jc−B特性の異なる複数種
のものを導体断面の磁場分布に応じて、例えば磁場の大
きいところには高磁場でJcの大きな線材を用い、磁場
の小さいところには低磁場でJcの大きな線材を用いる
等して配置される。
In this case, as the superconducting wire, for example, Y
-Ba-Cu-O, Bi-Sr-Cu-O, Bi-Sr
-Ca-Cu-O, Tl-Ba-Cu-O, Tl-Ba
-Ca-Cu-O, Tl-Sr-Ca-Cu-O, La
-Na-Cu-O, La-Ba-Cu-O, La-Sr
-Cu-O and other oxide-based superconductors with Ag, Cu, Al,
Those coated with a normal conductor such as an alloy mainly containing them are used, but a plurality of types having different Jc-B characteristics are used depending on the magnetic field distribution of the conductor cross section, for example, in a place where the magnetic field is large. A wire having a large Jc in a high magnetic field is used, and a wire having a large Jc in a low magnetic field is arranged in a place where the magnetic field is small.

【0009】[0009]

【作用】導体断面の磁場分布に応じてJc−B特性の異
なる線材を配置したので、素線構成の最適化がはかれ、
超電導線材集合導体としての超電導臨界電流密度を向上
させることができる。
[Function] Since wires having different Jc-B characteristics are arranged according to the magnetic field distribution of the conductor cross section, the wire configuration is optimized,
The superconducting critical current density as a superconducting wire aggregate conductor can be improved.

【0010】[0010]

【実施例】図1は、本発明に当って試作した超電導集合
導体の構造を示したものである。ここでは超電導線材と
して2種類のタイプA及びタイプBのテープ状線材1a
及び1b、例えばTl系の酸化物超電導体からなるコア
2にAg製造の被覆3を施したものを用いた。個々のテ
ープ状態線材1a及び1bの寸法は全て同一で、厚さ
0.15mm、幅2.7mm、超電導占積率約30%となっ
ており、集合導体は上下の各表面側にタイプAのテープ
状線材1aを夫々25枚、内側にタイプBの線材1bを
50枚配置して積層した後、径の細い導線4を巻き付け
て集合化したものである。
EXAMPLE FIG. 1 shows the structure of a superconducting collective conductor prototyped according to the present invention. Here, there are two types of tape-shaped wire 1a of type A and type B as superconducting wire.
And 1b, for example, a core 2 made of a Tl-based oxide superconductor coated with Ag-made coating 3 was used. The individual tape-state wire rods 1a and 1b all have the same dimensions, with a thickness of 0.15 mm, a width of 2.7 mm, and a superconducting space factor of about 30%. 25 pieces of tape-shaped wire rods 1a are arranged and 50 pieces of type-B wire rods 1b are arranged inside and laminated, and then a conductor wire 4 having a small diameter is wound and assembled.

【0011】この場合、タイプAの線材1aとタイプB
の線材1bの製造条件は、夫々900℃×50時間の熱
処理を4回繰返すまでは同じで、この後タイプAの線材
1aについてのみ800℃×20時間の熱処理を1回付
加した。
In this case, type A wire 1a and type B
The manufacturing conditions of the wire rod 1b were the same until the heat treatment at 900 ° C. for 50 hours was repeated four times, and thereafter, only for the type A wire rod 1a, the heat treatment at 800 ° C. for 20 hours was added once.

【0012】図4は、上記のようにして製作したタイプ
AとタイプBの線材1a及び1bのJc−B特性を示し
たものである。タイプAとタイプBは夫々異なる特性を
持ち、Jcは高磁場でタイプAの線材が大きく、低磁場
でタイプBの線材の方が大きくなっている。
FIG. 4 shows the Jc-B characteristics of the type A and type B wire rods 1a and 1b manufactured as described above. Type A and type B have different characteristics, and Jc has a large type A wire rod in a high magnetic field and a large type B wire rod in a low magnetic field.

【0013】前記した集合導体の臨界磁界は表面の最大
値で約20mTとなる。しかし、導体の内側には数mT
の磁界しか加わらず、内側にタイプAの線材を用いるよ
りタイプBの線材を用いた方が大きな電流を流すことが
できる。
The maximum magnetic field of the above-mentioned assembly conductor is about 20 mT on the surface. However, a few mT inside the conductor
However, a larger current can be applied by using the type B wire rod than by using the type A wire rod on the inside.

【0014】この超電導線材集合導体の臨界電流(I
c)を実測したところ320Aとなり、タイプAの線材
1aのみ100枚積層した集合導体(280A)より大
きなIcを示すことが確認された。
The critical current (I
When c) was actually measured, it was 320 A, and it was confirmed that Ic was larger than that of the assembly conductor (280 A) in which only 100 sheets of the type A wire 1a were laminated.

【0015】図2は、超電導集合導体の別の例を示し、
銅安定化材からなる中空パイブ6の周囲に複数の酸化物
系超電導線材をタイプAの線材5aとタイプBの線材5
bを交互に配置し、低温半田7等で集合化したもので、
中空パイプ6内に液体窒素や液体ヘリウム等の寒剤を流
すことで冷却効果を高めることができる。
FIG. 2 shows another example of the superconducting collective conductor,
A plurality of oxide-based superconducting wire rods are provided around the hollow pipe 6 made of a copper stabilizing material, the wire rod 5a of type A and the wire rod 5 of type B.
b arranged alternately, and assembled with low temperature solder 7 etc.,
By flowing a cryogen such as liquid nitrogen or liquid helium in the hollow pipe 6, the cooling effect can be enhanced.

【0016】図3は、さらに集合導体の別の例を示すも
ので、例えば銅板をU字状に成形した安定化材8内に複
数のテープ状の酸化物系超電導線材1を内側にタイプB
の線材1b、外側にタイプBの線材1bを夫々積層状態
に収容し、低温半田7等で一体化したものをテープ状の
電気絶縁層9を介して接合し、電流往復型の導体とした
ものである。
FIG. 3 shows another example of the collective conductor. For example, a plurality of tape-shaped oxide-based superconducting wires 1 are typed inside a stabilizing material 8 in which a copper plate is formed in a U shape.
Wire rod 1b, and type B wire rod 1b on the outside, respectively, are housed in a laminated state, and integrated by low-temperature solder 7 or the like to be joined via a tape-shaped electric insulating layer 9 to form a current reciprocating conductor. Is.

【0017】[0017]

【発明の効果】以上の説明から明らかなように、本発明
によれば、素線構成の最適化により超電導線材集合導体
としての超電導臨界電流密度を向上させることができ、
超電導電力ケーブル、電流リード用の導体等として有用
である。
As is apparent from the above description, according to the present invention, it is possible to improve the superconducting critical current density as a superconducting wire aggregate conductor by optimizing the strand configuration.
It is useful as a conductor for superconducting power cables and current leads.

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

【図1】本発明に係る超電導導体の一実施例の概要を示
す説明図。
FIG. 1 is an explanatory view showing an outline of one embodiment of a superconducting conductor according to the present invention.

【図2】超電導導体の別の例を示す説明図。FIG. 2 is an explanatory view showing another example of a superconducting conductor.

【図3】超電導導体の別の例を示す説明図。FIG. 3 is an explanatory view showing another example of a superconducting conductor.

【図4】Jc−B特性図。FIG. 4 is a Jc-B characteristic diagram.

【符号の説明】[Explanation of symbols]

1a及び5a タイブAの酸化物超電導線材 1b及び5b タイプBの酸化物超電導線材 2 酸化物超電導体のコア 3 Agの被覆 4 導線 6 中空パイプ 7 低温半田 8 安定化材 9 電気絶縁層 1a and 5a Type A oxide superconducting wire 1b and 5b Type B oxide superconducting wire 2 Oxide superconductor core 3 Ag coating 4 Conductive wire 6 Hollow pipe 7 Low temperature solder 8 Stabilizer 9 Electrical insulating layer

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】常超電導金属からなる被覆材を含む酸化物
系超電導線材を複数本集合した超電導導体であって、該
導体断面の自己磁界の大きくなる位置に高磁場低電流型
の素線を配置し、自己磁界の小さくなる位置に低磁場高
電流型の素線を配置してなることを特徴とする超電導導
体。
1. A superconducting conductor comprising a plurality of oxide-based superconducting wire rods including a coating material made of a normal superconducting metal, wherein a high magnetic field, low current type element wire is provided at a position where the self magnetic field of the conductor cross section becomes large. A superconducting conductor characterized by arranging and arranging a low magnetic field and high current type element wire at a position where the self magnetic field becomes small.
JP26455191A 1991-10-14 1991-10-14 Superconducting conductor Expired - Fee Related JP3363164B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26455191A JP3363164B2 (en) 1991-10-14 1991-10-14 Superconducting conductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26455191A JP3363164B2 (en) 1991-10-14 1991-10-14 Superconducting conductor

Publications (2)

Publication Number Publication Date
JPH05109324A true JPH05109324A (en) 1993-04-30
JP3363164B2 JP3363164B2 (en) 2003-01-08

Family

ID=17404845

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26455191A Expired - Fee Related JP3363164B2 (en) 1991-10-14 1991-10-14 Superconducting conductor

Country Status (1)

Country Link
JP (1) JP3363164B2 (en)

Also Published As

Publication number Publication date
JP3363164B2 (en) 2003-01-08

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