JPH0325808A - Superconductor - Google Patents

Superconductor

Info

Publication number
JPH0325808A
JPH0325808A JP1158352A JP15835289A JPH0325808A JP H0325808 A JPH0325808 A JP H0325808A JP 1158352 A JP1158352 A JP 1158352A JP 15835289 A JP15835289 A JP 15835289A JP H0325808 A JPH0325808 A JP H0325808A
Authority
JP
Japan
Prior art keywords
conduit
inside layer
layer
base material
high resistance
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.)
Pending
Application number
JP1158352A
Other languages
Japanese (ja)
Inventor
Mamoru Shimada
守 嶋田
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP1158352A priority Critical patent/JPH0325808A/en
Publication of JPH0325808A publication Critical patent/JPH0325808A/en
Pending 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

Abstract

PURPOSE:To provide a superconductor of which pressure rise at the time of quench is small and of which loss by the eddy current at the time of a large change of the magnetic field is small by using copper or aluminium as the base material of a conduit of the most inside layer, and inserting high resistance members into the base material locally. CONSTITUTION:A conduit consists of an outside layer 2B and an inside layer 2C, and a superconductive wires 1 are housed in the conduit. The inside layer 2C of the conduit is formed with high resistance layers 3 to prevent the eddy current flowing in the inside layer 2C of the conduit at the time of a change of the magnetic field with the high resistance layers 3, and the loss by the eddy current can be reduced remarkably. At the time of quench, since the base material of the inside layer 2C of the conduit is copper of which electric resistance is low, the electric current flowing in the superconductive wires are shunted to the inside layer 2C of the conduit, and the calorific value is reduced to restrict the pressure rise.

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は大型の超電導コイル等に用いられるケーブル・
イン・コンジットタイプの超電導導体に関する. (従来の技術) 導体内部に冷媒を流して冷却するケーブル・イン・コン
ジットタイプの超電導導体においては、クエンチした場
合に内部の圧力が非常に大きくなる可能性がある.その
ため第3図に示すようにコンジットを多層化し、1つの
層を銅,アルミニウムなどの抵抗の低い材料で作ること
が考えられている. (発明が解決しようとする課題) しかし、従来の超電導導体を磁界変化の大きい場合に使
用すると、抵抗の低い材料の層において大きな渦電流が
流れ、それによって大きな損失が生ずるという問題点が
ある. 本発明は、上記のような問題点を解決するためになされ
たもので,クエンチした際の圧力上昇が小さく,かつ、
磁界変化が大きい場合にも、渦電流による損失が小さい
超電導導体を提供することを目的とする. 〔発明の構成〕 (課題を解決するための手段) 本発明においては、上記目的を達成するためにコンジッ
トを多層構造とし,少なくとも最内層のコンジットを銅
あるいはアルミニウムを母材とし、その母材に高抵抗部
材を入れた構造とする。
[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention relates to cables used in large superconducting coils, etc.
Concerning in-conduit type superconducting conductors. (Prior technology) In cable-in-conduit type superconducting conductors that are cooled by flowing a refrigerant inside the conductor, the internal pressure may become extremely large when quenched. Therefore, it is being considered to make the conduit multi-layered, as shown in Figure 3, with each layer made of a low-resistance material such as copper or aluminum. (Problem to be solved by the invention) However, when conventional superconducting conductors are used in cases where magnetic field changes are large, there is a problem in that large eddy currents flow in the layer of material with low resistance, resulting in large losses. The present invention was made to solve the above-mentioned problems, and the pressure increase during quenching is small, and
The objective is to provide a superconducting conductor with low loss due to eddy current even when magnetic field changes are large. [Structure of the Invention] (Means for Solving the Problems) In the present invention, in order to achieve the above object, the conduit has a multilayer structure, and at least the innermost layer of the conduit has a base material of copper or aluminum. The structure includes high-resistance members.

(作用) 本発明による超電導導体においては、磁界変化が生じた
場合に、電気抵抗の小さい層のコンジットにおいて発生
する渦電流を、その層に入れた電気抵抗の大きい材料か
らなる部材によって低減させる. (実施例) 以下、本発明の実施例を図面を用いて説明する. 第1図は本発明による超電導導体の断面を示す図である
. この実施例においてはコンジットが外層2Bおよび内層
2Cからなり、その内に超電導4I1が入っている. 外層2Bは電磁力,圧力等に耐えるために強度の高いS
US材により作られ、内層2Cは電気抵抗の低い銅を母
材とし、導体長手方向にわたって太きい電気抵抗を持つ
CuNiからなる高抵抗層3とからなる. コンジット内層2Cに高抵抗層3をつけることにより,
磁界変化が生じた勲にコンジット内M2Gに流れる渦電
流が高抵抗層3によって防げられ、渦電流による損失を
大幅に減少させることができる。
(Function) In the superconducting conductor according to the present invention, when a magnetic field change occurs, the eddy current generated in the conduit of the layer with low electrical resistance is reduced by the member made of the material with high electrical resistance placed in that layer. (Example) Examples of the present invention will be described below with reference to the drawings. FIG. 1 is a diagram showing a cross section of a superconducting conductor according to the present invention. In this embodiment, the conduit consists of an outer layer 2B and an inner layer 2C, in which the superconductor 4I1 is contained. The outer layer 2B is made of high-strength S to withstand electromagnetic force, pressure, etc.
The inner layer 2C is made of US material, and the inner layer 2C is made of copper, which has a low electrical resistance, as a base material, and the high resistance layer 3 is made of CuNi, which has a large electrical resistance in the longitudinal direction of the conductor. By attaching the high resistance layer 3 to the conduit inner layer 2C,
The high resistance layer 3 prevents eddy currents from flowing in the conduit M2G when a magnetic field change occurs, and losses due to eddy currents can be significantly reduced.

また、クエンチした際には、コンジット内層2Cが電気
抵抗の低い銅を母材とするため、超電導線に流れていた
通電電流がコンジット内層2Cに分流し、発熱量が低下
し,圧力上昇を押えることは、第3図に示した従来の超
電導導体と同様である.なお、コンジット内層2CをS
US、コンジット外眉2Bを高抵抗層3を持つ銅によっ
て構成しても本発明の超電導導体が得られる.また、高
抵抗層3を導体長手方向にらせん状にすれば渦電流を防
止する効果を高めることができる. (他の実施例) 第2図は本発明の他の実施例による超電導導体の断面を
示す図である.この実施例においては、コンジット内層
2Dが電圧抵抗の低い銅からなり、導体長手方向に沿う
高抵抗層4を、コンジット内層2Dの表面に加工した溝
にCuNiをうめ込むことにより形成した場合である. この実施例によれば、コンジット内層2Dの気密性が向
上するとともに、加工性も向上する.〔発明の効果〕 以上に詳述したように,本発明によれば磁界変化が生じ
た際の渦電流による損失を低減し、かつ,クエンチした
際の圧力上昇も低く押えることができるケーブル・イン
・コンジットタイプの超電導導体を提供することができ
る.
In addition, when quenching occurs, since the conduit inner layer 2C has a base material of copper with low electrical resistance, the current flowing through the superconducting wire is diverted to the conduit inner layer 2C, reducing the amount of heat generated and suppressing the pressure rise. This is similar to the conventional superconducting conductor shown in Figure 3. In addition, the conduit inner layer 2C is
US, the superconducting conductor of the present invention can be obtained even if the outer conduit 2B is made of copper having a high resistance layer 3. Further, by forming the high resistance layer 3 in a spiral shape in the longitudinal direction of the conductor, the effect of preventing eddy currents can be enhanced. (Other Embodiments) FIG. 2 is a diagram showing a cross section of a superconducting conductor according to another embodiment of the present invention. In this example, the conduit inner layer 2D is made of copper with low voltage resistance, and the high resistance layer 4 along the longitudinal direction of the conductor is formed by filling CuNi into a groove machined on the surface of the conduit inner layer 2D. .. According to this embodiment, the airtightness of the conduit inner layer 2D is improved, and workability is also improved. [Effects of the Invention] As detailed above, the present invention provides a cable insulator that can reduce loss due to eddy current when magnetic field changes occur and also suppress pressure rise when quenching. - Can provide conduit type superconducting conductors.

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

第1図は本発明の一実施例の超電導導体の断面図、第2
図は他の実施例の超電導導体の断面図、第3図は従来の
超電導導体の断面図である.1・・・超電導線
Fig. 1 is a sectional view of a superconducting conductor according to an embodiment of the present invention, Fig.
The figure is a cross-sectional view of a superconducting conductor according to another embodiment, and FIG. 3 is a cross-sectional view of a conventional superconducting conductor. 1...Superconducting wire

Claims (2)

【特許請求の範囲】[Claims] (1)コンジット内部に超電導線を入れたケーブル・イ
ン・コンジットタイプの超電導導体において、コンジッ
トは少なくとも2つ以上の層を持つ多層構造であり、少
なくとも最内層のコンジットが銅あるいはアルミニウム
を母材とし、その母材に高抵抗部材を入れたことを特徴
とする超電導導体。
(1) In a cable-in-conduit type superconducting conductor in which a superconducting wire is placed inside the conduit, the conduit has a multilayer structure with at least two layers, and at least the innermost layer of the conduit is made of copper or aluminum as a base material. , a superconducting conductor characterized by having a high-resistance material inserted into its base material.
(2)高抵抗部材はCuNiであることを特徴とする請
求項(1)記載の超電導導体。
(2) The superconducting conductor according to claim (1), wherein the high resistance member is CuNi.
JP1158352A 1989-06-22 1989-06-22 Superconductor Pending JPH0325808A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1158352A JPH0325808A (en) 1989-06-22 1989-06-22 Superconductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1158352A JPH0325808A (en) 1989-06-22 1989-06-22 Superconductor

Publications (1)

Publication Number Publication Date
JPH0325808A true JPH0325808A (en) 1991-02-04

Family

ID=15669779

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1158352A Pending JPH0325808A (en) 1989-06-22 1989-06-22 Superconductor

Country Status (1)

Country Link
JP (1) JPH0325808A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5343180A (en) * 1991-03-25 1994-08-30 Hitachi, Ltd. Coil structure and coil container
US5424702A (en) * 1991-09-19 1995-06-13 Hitachi, Ltd. Superconducting magnet

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5343180A (en) * 1991-03-25 1994-08-30 Hitachi, Ltd. Coil structure and coil container
US5424702A (en) * 1991-09-19 1995-06-13 Hitachi, Ltd. Superconducting magnet

Similar Documents

Publication Publication Date Title
US7598458B2 (en) Super-conductive cable
KR100706494B1 (en) Superconducting cable
US7633014B2 (en) Superconductor cable
KR101050677B1 (en) Superconducting cable and superconducting cable line using this superconducting cable
US4055887A (en) Method for producing a stabilized electrical superconductor
US4454380A (en) Stabilized multifilament superconductor made of brittle, prereacted Nb3 Sn filaments in a bronze matrix
US4176238A (en) Cooled multiphase ac cable
Ghosh et al. The effect of magnetic impurities and barriers on the magnetization and critical current of fine filament NbTi composites
MX2007011073A (en) Superconductive cable and dc power transmission using the superconductive cable.
JPH0325808A (en) Superconductor
CN1291337A (en) Construction method containing N phase multiple phase super conductive cable
KR100742499B1 (en) Core of magentic shield type superconducting cable and superconducting cable having the same
JPS599809A (en) Superconductive conductor
Verhaege et al. A new class of AC superconducting conductors
JPH0377607B2 (en)
JP2019149344A (en) High temperature superconducting wire, and high temperature superconducting coil
JP2000067663A (en) Superconductive conductor
JPH046713A (en) Aluminium stabilization superconductive wire
JPH07201231A (en) High-temperature superconductor element wire
JPH05282929A (en) Superconductive conductor and stabilizer used therefor
JPH06104026A (en) Connection structure of superconductor
JP3363164B2 (en) Superconducting conductor
JPH05109323A (en) Superconductive assembled conductor
JPH0714441A (en) Superconducting cable
JPH0254809A (en) Superconducting conductor