JPS59138007A - Superconductive conductor - Google Patents

Superconductive conductor

Info

Publication number
JPS59138007A
JPS59138007A JP58012399A JP1239983A JPS59138007A JP S59138007 A JPS59138007 A JP S59138007A JP 58012399 A JP58012399 A JP 58012399A JP 1239983 A JP1239983 A JP 1239983A JP S59138007 A JPS59138007 A JP S59138007A
Authority
JP
Japan
Prior art keywords
core material
superconducting
conductor
slit
superconducting conductor
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
JP58012399A
Other languages
Japanese (ja)
Inventor
茂樹 礒嶋
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.)
Sumitomo Electric Industries Ltd
Original Assignee
Sumitomo Electric Industries 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 Sumitomo Electric Industries Ltd filed Critical Sumitomo Electric Industries Ltd
Priority to JP58012399A priority Critical patent/JPS59138007A/en
Publication of JPS59138007A publication Critical patent/JPS59138007A/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

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 発明の分野 この発明は、芯材とその周囲に配置される超電導ストラ
ンドとからなる超電導導体に関するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a superconducting conductor comprising a core material and superconducting strands disposed around the core material.

先行技術の説明 一般的に、超電導7グネツトに用いられる大電流容量の
超電導導体は、第1図に示されるような撚り線型導体で
ある。第2図は、第1図に示される超電ss体の断面図
である。図示されるように、超電導導体1は、複数本の
超電導ストランド2を有している。また、導体製作時の
撚り芯として、およびコイル製作時の巻テンション印加
または励磁時の1111張力の発生に対する補強材とし
で芯材3が用いられる。この芯材3は、S IJ Sな
どの高抗張力材から作られる。
Description of the Prior Art Generally, the high current capacity superconducting conductor used in a superconducting 7-net is a stranded conductor as shown in FIG. FIG. 2 is a sectional view of the superelectric SS body shown in FIG. 1. As illustrated, the superconducting conductor 1 has a plurality of superconducting strands 2. Further, the core material 3 is used as a twisted core when manufacturing a conductor, and as a reinforcing material against the generation of 1111 tension during application of winding tension or excitation during manufacturing of a coil. This core material 3 is made from a high tensile strength material such as S IJ S.

このような構成の超電導導体1は、以下に述べるような
欠点があった。第3図および第4図を用いて説明する。
The superconducting conductor 1 having such a configuration has the following drawbacks. This will be explained using FIGS. 3 and 4.

第3図は、超電導導体1が巻かれた超電導7グネツ1〜
を示す断面図であり、磁力線を矢印で示す。第4図は第
3図に示されるマグネットの端部に位@する超電導導体
1と磁力線との関係を拡大して示す図でのる。図示され
るように、マグネットの端部では磁力線の半径方向の成
分、つまり第3図または第4図に6いてL右方向;:向
υ)−う成分が人き(なる。また、各導体は第3図(二
示されるようにフラットワイズに巻線されている。
Figure 3 shows superconducting 7 wires 1 to 1 wrapped around superconducting conductor 1.
is a cross-sectional view showing lines of magnetic force with arrows. FIG. 4 is an enlarged view showing the relationship between the superconducting conductor 1 located at the end of the magnet shown in FIG. 3 and the lines of magnetic force. As shown in the figure, at the end of the magnet, the radial component of the magnetic field lines, that is, the component in the L right direction in FIG. is wound flatwise as shown in Figure 3 (2).

したがって、マグネットの端部に位置する導体では、第
4図に示されるように、磁力線が導体1の芯材3のフラ
ン1〜面とほぼ直交するようになる。
Therefore, in the conductor located at the end of the magnet, the lines of magnetic force are approximately perpendicular to the flange 1 plane of the core material 3 of the conductor 1, as shown in FIG.

そのため、パルスマグネットにおいて磁場が急変すると
、芯材3に大きな渦電流損が発生する。
Therefore, when the magnetic field suddenly changes in the pulsed magnet, a large eddy current loss occurs in the core material 3.

発明の目的 それゆえに、この発明は、超電導マグネットの端部に配
置されても、発生する渦電流を非常に小° さくし得る
超電導導体を提供することを目的とする。
OBJECTS OF THE INVENTION Therefore, an object of the present invention is to provide a superconducting conductor that can significantly reduce the generated eddy current even if it is placed at the end of a superconducting magnet.

この発明は、芯材に孔を設けたことを*徴どする超電導
導体であり、この孔の存在によって発生渦電流を非常に
小さくすることができる。
This invention is a superconducting conductor that is characterized by having holes in its core material, and the presence of these holes makes it possible to significantly reduce the generated eddy current.

実施例の説明 第5図は、この発明に従った超電導導体に用いられる芯
材を示す斜視図である。図示されていないが、超電導ス
トランドが第1図に示されるものと同様にこの芯材3の
周囲に撚り線として配置され超電導導体を構成する。図
示されるように、芯材3には芯材3を貫通するスリット
4がSΩけられている。スリット4の幅は、好ましくは
芯材3がその強度を維持できるように可能な限り狭くさ
れる。また、スリット4の長さ、位置、頻度(敞)など
も同様に、芯材3が抗張力部材としての機能をできるだ
け損わない範囲で適当に定められる。
DESCRIPTION OF EMBODIMENTS FIG. 5 is a perspective view showing a core material used in a superconducting conductor according to the present invention. Although not shown, superconducting strands are arranged as twisted wires around this core material 3 to constitute a superconducting conductor, similar to that shown in FIG. As shown in the figure, the core material 3 is provided with a slit 4 that penetrates the core material 3 by SΩ. The width of the slit 4 is preferably made as narrow as possible so that the core material 3 can maintain its strength. Further, the length, position, frequency, etc. of the slits 4 are similarly appropriately determined within a range that does not impair the function of the core material 3 as a tensile strength member as much as possible.

このスリット4の存在によって、芯材3のフラット面に
渦電流が発生しても大きな渦電流ループは切られること
になる。
Due to the presence of this slit 4, even if an eddy current occurs on the flat surface of the core material 3, a large eddy current loop is cut off.

第5図においてスリット4は芯材3の長さ方向、つまり
周囲の超電導ストランドが延びる方向とほぼ平行に延び
て形成されている。しかし、渦電流ループを切るために
スリットを設けるしのであるから、異なった方向、たと
えば芯材3の長さ方向と交差する方向に延びて形成され
たスリットであってもよい、また同様の意味から、芯材
3に設けられるのは樹長いスリットに限られず、スリッ
トの概念に含まれない貫通孔であってもよい。ただ、孔
をどのような形状に1ノようとも、またはどのような方
向に延ばそうとも、前述したように芯材3が抗張力部材
と1ノでの機能をできるだけ損わない範囲で定めなけれ
ばならない。
In FIG. 5, the slit 4 is formed to extend substantially parallel to the length direction of the core material 3, that is, the direction in which the surrounding superconducting strands extend. However, since the slit is provided to cut the eddy current loop, the slit may be formed extending in a different direction, for example, in a direction intersecting the length direction of the core material 3, or the slit may have the same meaning. Therefore, what is provided in the core material 3 is not limited to a long slit, but may be a through hole that is not included in the concept of a slit. However, no matter what shape the hole is made or in what direction it extends, as mentioned above, it must be determined within a range that does not impair the function of the core material 3 as a tensile strength member as much as possible. .

発明の効果 上述されたように、この発明に従った超電導導体はその
芯材に孔が設けられている。したがって、この孔の存在
によって、大きな渦電流ループが切られるので、発生す
る渦電流は非常に小さいものとなる。したがって、超電
導マグネットの端部における渦電流損失を大幅に抑制す
ることができる。
Effects of the Invention As mentioned above, the superconducting conductor according to the present invention has holes in its core material. Therefore, due to the presence of this hole, a large eddy current loop is cut, so that the eddy currents generated are very small. Therefore, eddy current loss at the ends of the superconducting magnet can be significantly suppressed.

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

第1図は従来の超電S導体を示す斜視図であり、第2図
はその断面図である。第3図は、超電導導体を巻いた超
電導マグネットを示す断面図であり、磁力線を矢印で示
している。第4図は、第3図に示される超電導マグネッ
トの端部に位置する超電導導体と磁力線との関係を拡大
して示す図である。 第5図は、この発明に従った超電導導体の芯材を示す斜
視図である。 図において、1は超電導導体、2は超電導ストランド、
3は芯材、4はスリットを示す。
FIG. 1 is a perspective view showing a conventional superconducting S conductor, and FIG. 2 is a sectional view thereof. FIG. 3 is a cross-sectional view showing a superconducting magnet wound with a superconducting conductor, and lines of magnetic force are indicated by arrows. FIG. 4 is an enlarged view showing the relationship between the superconducting conductor located at the end of the superconducting magnet shown in FIG. 3 and lines of magnetic force. FIG. 5 is a perspective view showing a core material of a superconducting conductor according to the present invention. In the figure, 1 is a superconducting conductor, 2 is a superconducting strand,
3 indicates a core material, and 4 indicates a slit.

Claims (2)

【特許請求の範囲】[Claims] (1) 芯材とその周囲に配置される超電導ストランド
とからなる超電導導体において、前記芯材に孔を設けた
ことを特徴とする超電導導体。
(1) A superconducting conductor consisting of a core material and superconducting strands arranged around the core material, characterized in that the core material is provided with a hole.
(2) 前記孔は細長いスリットである、特許請求の範
囲第1項記載の超電導番導体。
(2) The superconducting conductor according to claim 1, wherein the hole is an elongated slit.
JP58012399A 1983-01-27 1983-01-27 Superconductive conductor Pending JPS59138007A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58012399A JPS59138007A (en) 1983-01-27 1983-01-27 Superconductive conductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58012399A JPS59138007A (en) 1983-01-27 1983-01-27 Superconductive conductor

Publications (1)

Publication Number Publication Date
JPS59138007A true JPS59138007A (en) 1984-08-08

Family

ID=11804180

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58012399A Pending JPS59138007A (en) 1983-01-27 1983-01-27 Superconductive conductor

Country Status (1)

Country Link
JP (1) JPS59138007A (en)

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