JPS60177603A - Superconductive coil - Google Patents

Superconductive coil

Info

Publication number
JPS60177603A
JPS60177603A JP59032533A JP3253384A JPS60177603A JP S60177603 A JPS60177603 A JP S60177603A JP 59032533 A JP59032533 A JP 59032533A JP 3253384 A JP3253384 A JP 3253384A JP S60177603 A JPS60177603 A JP S60177603A
Authority
JP
Japan
Prior art keywords
conductor
superconductor
coil
superconducting
insulating materials
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
JP59032533A
Other languages
Japanese (ja)
Other versions
JPH0226362B2 (en
Inventor
Sunao Ichihara
直 市原
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP59032533A priority Critical patent/JPS60177603A/en
Publication of JPS60177603A publication Critical patent/JPS60177603A/en
Publication of JPH0226362B2 publication Critical patent/JPH0226362B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01BCABLES; CONDUCTORS; INSULATORS; SELECTION OF MATERIALS FOR THEIR CONDUCTIVE, INSULATING OR DIELECTRIC PROPERTIES
    • H01B12/00Superconductive or hyperconductive conductors, cables, or transmission lines
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F6/00Superconducting magnets; Superconducting coils
    • H01F6/06Coils, e.g. winding, insulating, terminating or casing arrangements therefor
    • 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

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)

Abstract

PURPOSE:To enhance hardness, and to obtain a superconductive coil not to generate deterioration even when the coil is used for a long period by a method wherein when tube type electrically insulating materials are to be fitted on a slender superconductor interposing an interval between them to enhance cooling performance thereof, the insulating materials thereof are formed of a glass epoxy laminate having high Young's modulus. CONSTITUTION:Tube type electrically insulating materials 3a are fitted on a slender superconductor 2 interposing the prescribed interval between them to form a wire for superconducting coil. At this construction, a laminate of large Young's modulus such as glass epoxy, etc. is used for the insulating materials 3a, and made to surround the superconductor 2 fastening the conductor to some extent. At this time, when the superconductor 2 is not a round shape but is a square shape, the section of the insulating material 3a is formed also in a square shape conforming thereto. Accordingly, hardness of the winding is enlarged, and the coil is stabilized.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は、超電導コイルに関するものであり、もう少
し詳しくいうと、細長い導体に、この導体の一部を露出
させて導体絶縁を施した超電導線を巻回してなる超電導
コイルに関するものである。
[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to a superconducting coil. More specifically, the present invention relates to a superconducting coil, and more specifically, a superconducting wire comprising a long and thin conductor with conductor insulation provided by exposing a part of the conductor. This relates to a superconducting coil formed by winding.

〔従来技術〕[Prior art]

従来、この種の装置とし【第1図、第一図に示すものが
あった。第1図に示す超電導線を巻回した巻線部分lに
使用する超電導線は、第2図に示すように、細長い超電
導導体コに絶縁テープ3かつる巻状に巻付け、導体露出
部参を確保するとともK、超電導導体間の電気絶縁を行
5ものであった。
Conventionally, there have been devices of this type shown in FIG. The superconducting wire used for the winding part l shown in Fig. 1 is wrapped around a long and slender superconducting conductor with an insulating tape 3 in a helical shape, as shown in Fig. 2, and the exposed part of the conductor is It was also necessary to ensure electrical insulation between the superconducting conductors.

この種の超電導コイルは、冷媒である液体ヘリウムに浸
漬して冷却し、冷却性能向上のためになるべく超電導導
体コな冷媒に直接さらし、常温から極低温まで速やかに
冷却し、かつ、冷却後通電中のじよう乱による発熱、交
流損失による発熱を、速やかに除去し、もって安定な通
電状態を確保する必要がある。第一図に示した導体絶縁
3は以上の性能を得るためのものである。導体絶縁3と
しては、超電導導体λへの巻付のしやすさのため柔軟性
のある高分子化合物テープを使用していた。
This type of superconducting coil is cooled by immersing it in liquid helium, which is a refrigerant, and in order to improve cooling performance, the superconducting conductor is exposed directly to the refrigerant as much as possible, quickly cooled from room temperature to extremely low temperature, and then energized after cooling. It is necessary to promptly remove heat generated by internal turbulence and heat generated by alternating current loss, thereby ensuring a stable energized state. The conductor insulation 3 shown in FIG. 1 is for obtaining the above performance. As the conductor insulation 3, a flexible polymer compound tape was used because it could be easily wrapped around the superconducting conductor λ.

しかし、従来の超電導コイルは以上のように構成されて
いたので、導体絶縁Jが柔軟であることから、巻線全体
として剛性が弱く、長期間の使用により導体絶縁3がゆ
る木、安定な通電を行い難いという欠点があった。
However, since conventional superconducting coils were constructed as described above, since the conductor insulation J is flexible, the rigidity of the winding as a whole is weak, and after long-term use, the conductor insulation 3 loosens, resulting in stable current flow. The disadvantage was that it was difficult to carry out.

〔発明の概要〕[Summary of the invention]

この発明は、上記のような従来のものの欠点を除去する
ことを目的とするもので、導体絶縁を剛性の大きいチュ
ーブ状のものにすることにより、冷却特性がよく、機械
的にも安定な超電導コイルを提供するものである。
The purpose of this invention is to eliminate the above-mentioned drawbacks of the conventional ones. By making the conductor insulation into a tube-like material with high rigidity, it is possible to create a superconducting conductor with good cooling characteristics and mechanical stability. It provides coils.

〔発明の実施例〕[Embodiments of the invention]

以下、この発明の一実施例を第3図について説明する。 An embodiment of the present invention will be described below with reference to FIG.

図において、超電導導体−に間隔をおいて被着される導
体絶縁3aは、ヤング率が大きい物質でなるチューブ状
のもので、さらに熱収縮量が小さく、経年による寸法変
化が少なく、機械的強度ぶ大きい等の特性も併有する電
気絶縁材が望ましい。例えばガラスエポキシ積層品の丸
管が好適である。超電導導体コは、ある程度しまり加減
で導体絶縁3aに挿入する。超電導導体は丸でなく第す
図、第3図に示す角形断面の超電導導体2aであっても
よく、この場合、導体絶縁3bは、もちろん角形管とす
る。
In the figure, the conductor insulation 3a, which is adhered to the superconducting conductor at intervals, is a tube-shaped material made of a material with a large Young's modulus, has a small amount of thermal shrinkage, has little dimensional change over time, and has mechanical strength. It is desirable to use an electrical insulating material that also has characteristics such as large size. For example, a round tube made of glass epoxy laminate is suitable. The superconducting conductor is inserted into the conductor insulation 3a with a certain degree of tightness. The superconducting conductor may not be round but may be a superconducting conductor 2a having a rectangular cross section as shown in FIGS.

第6図、第7図は他の実施例を示し、超電導導体コaに
間隔をおいて被着された導体絶縁3Cは、長さ方向に切
欠き13を形成した断面C字状のもので、ヤング率の大
きい物質でなる。
FIGS. 6 and 7 show another embodiment, in which the conductor insulation 3C applied at intervals to the superconducting conductor core a has a C-shaped cross section with notches 13 formed in the length direction. , made of a material with a large Young's modulus.

以上の構成により、まえの実施例と同様の幼芽な奏する
に加えて、超電導導体2aの横方向から超電導導体、2
4を挾みこむようにして、導体絶縁3Cを超電導導体X
aに被着できるという利点がある。
With the above configuration, in addition to producing seedlings similar to the previous embodiment, the superconducting conductor 2a can be seen from the lateral direction of the superconducting conductor 2a.
4 and insert the conductor insulation 3C into the superconducting conductor
It has the advantage that it can be applied to a.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明は、導体絶縁の材料として機械
的特性が良好で剛い材料を用いたので、巻線剛性が高く
、長期間の使用に対しても劣化の少ない安定な超電導コ
イルが得られる。
As described above, this invention uses a rigid material with good mechanical properties as the conductor insulation material, so it is possible to create a superconducting coil that has high winding rigidity and is stable with little deterioration even after long-term use. can get.

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

第1図は従来の超電導コイルの断面図、第2図は従来の
超電導線の側面図、第3図はこの発明の一実施例の要部
斜視図、第V図は第3因の変形例の斜視図、第3図は第
V図のものの横断面図、第6図はこの発明の他の実施例
の斜視図、第7図は第6図のものの横断面図である。 l・・超電導巻線、コ、λa−Φ超電導導体1.7a、
3b、3C・・導体絶縁、13・・切欠き。 なお、各図中、同一符号は同−又は相当部分を示す。 兇1図 兜2図 χ3図 篤4図 %5図 憾7図 スハ
Fig. 1 is a sectional view of a conventional superconducting coil, Fig. 2 is a side view of a conventional superconducting wire, Fig. 3 is a perspective view of a main part of an embodiment of the present invention, and Fig. V is a modification of the third factor. 3 is a cross-sectional view of the one shown in FIG. V, FIG. 6 is a perspective view of another embodiment of the invention, and FIG. 7 is a cross-sectional view of the one shown in FIG. 6. l... superconducting winding, λa-Φ superconducting conductor 1.7a,
3b, 3C...Conductor insulation, 13...Notch. In each figure, the same reference numerals indicate the same or corresponding parts. Figure 1 Helmet 2 Figure χ3 Figure Atsushi 4 Figure %5 Figure 7 Figure Suha

Claims (1)

【特許請求の範囲】 (1) 間隔をおいてチューブ状の導体絶縁な被着した
超電導導体を巻回してなる超電導コイル。 (コ)長さ方向に切欠きのある導体絶縁を備えた特許請
求の範囲第1項記載の超電導コイル。 (3) 導体絶縁がガラスエポキシ積層品でなる特許請
求の範囲第1項記載の超電導コイル。
[Claims] (1) A superconducting coil formed by winding tube-shaped conductor-insulated superconducting conductors at intervals. (g) The superconducting coil according to claim 1, which is provided with conductor insulation having a notch in the length direction. (3) The superconducting coil according to claim 1, wherein the conductor insulation is a glass epoxy laminate.
JP59032533A 1984-02-24 1984-02-24 Superconductive coil Granted JPS60177603A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59032533A JPS60177603A (en) 1984-02-24 1984-02-24 Superconductive coil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59032533A JPS60177603A (en) 1984-02-24 1984-02-24 Superconductive coil

Publications (2)

Publication Number Publication Date
JPS60177603A true JPS60177603A (en) 1985-09-11
JPH0226362B2 JPH0226362B2 (en) 1990-06-08

Family

ID=12361578

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59032533A Granted JPS60177603A (en) 1984-02-24 1984-02-24 Superconductive coil

Country Status (1)

Country Link
JP (1) JPS60177603A (en)

Also Published As

Publication number Publication date
JPH0226362B2 (en) 1990-06-08

Similar Documents

Publication Publication Date Title
JPH03245504A (en) Magnet for critical magnetic field measuring device
US5114908A (en) Superconductive conductor
US5571606A (en) Ceramic superconducting lead resistant to breakage
JP3796850B2 (en) Terminal structure of superconducting cable conductor and connection method thereof
GB1172026A (en) Superconducting Windings
JPS60177603A (en) Superconductive coil
US5759960A (en) Superconductive device having a ceramic superconducting lead resistant to breakage
JPS5764906A (en) Impregnated superconductive coil
JPS5961010A (en) Superconductive magnet
JPS62214680A (en) Superconductor for thermal persistent current switch
JP2600413B2 (en) Hybrid superconducting coil
JPS5543427A (en) Resistance thermometer
JPS607368B2 (en) superconducting coil
JPH048885B2 (en)
JPS61265881A (en) Thermal type superconductive switch
Sharma et al. Multifilamentary V3Ga wires and tapes with composite cores
JPH04277605A (en) Superconductive conductor and coil
JPS603545Y2 (en) superconducting winding
JPS5873104A (en) Superconductive magnet
JPH0448609A (en) Transformer
JPS6289304A (en) superconducting magnet
JPH02186510A (en) Superconductor
JP3352735B2 (en) Superconducting flexible cable
JPH03284155A (en) Superconductive coil
JP2846323B2 (en) AC superconducting wire