JPS6215803A - Superconductive coil - Google Patents
Superconductive coilInfo
- Publication number
- JPS6215803A JPS6215803A JP60154030A JP15403085A JPS6215803A JP S6215803 A JPS6215803 A JP S6215803A JP 60154030 A JP60154030 A JP 60154030A JP 15403085 A JP15403085 A JP 15403085A JP S6215803 A JPS6215803 A JP S6215803A
- Authority
- JP
- Japan
- Prior art keywords
- thickness
- thin
- insulator
- conductor
- 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.)
- Pending
Links
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
- Superconductive Dynamoelectric Machines (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は超電導コイルの改良に係り、特に、冷却特性に
好適な信頼性の高い超電導コイルの絶縁−に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to improvements in superconducting coils, and particularly to highly reliable insulation of superconducting coils suitable for cooling characteristics.
従来の超電導コイルのコイル導体間の絶縁は、特公昭4
7−8265号公報に記載のように、導体の曲げにすみ
に十分耐え得るよう適切な間隔で導体間にスペーサを介
挿し、クーリングチャンネルも兼ねていた。しかし、極
薄の超電導4体は剛性が小さく、間隔をもってスペーサ
を介挿すると、導体が短絡する。一方、この短絡を防止
するため超電導4体の表面に各種のワニスを塗布し、導
体間を密着させる方法も採用されている。しかし、極薄
の平角形状の特殊な超電導4体ともなると、ワニスを塗
布してこのワニスを硬化のために、熱処理をすると超電
導4体の特性が出なくなる恐れがある。また、極薄のも
のは導体のエツジ間にワニスが塗布されないという欠点
がある。The insulation between the coil conductors of conventional superconducting coils was
As described in Japanese Patent No. 7-8265, spacers were inserted between the conductors at appropriate intervals to sufficiently withstand bending of the conductors, and also served as cooling channels. However, the four ultra-thin superconducting bodies have low rigidity, and if spacers are inserted at intervals, the conductors will short-circuit. On the other hand, in order to prevent this short circuit, a method has also been adopted in which various types of varnish are applied to the surfaces of the four superconducting bodies to bring the conductors into close contact. However, when it comes to special ultra-thin rectangular superconducting bodies, if a varnish is applied and then heat treated to harden the varnish, there is a risk that the characteristics of the superconducting bodies will no longer be exhibited. Also, extremely thin ones have the disadvantage that varnish cannot be applied between the edges of the conductor.
本発明の目的は、超電導コイルの等価剛性が高く、冷却
性能のよいコイル導体の絶縁システムを提供することに
ある。An object of the present invention is to provide a superconducting coil conductor insulation system with high equivalent rigidity and good cooling performance.
超電導コイルにとって重要な技術的問題には以下の点が
あげられている。The following points are listed as important technical issues for superconducting coils.
(1) ′M電導々体への冷却構造を好適とし、超電導
導体を臨界温度以下に保つこと。(1) The cooling structure for the 'M conductor should be suitable and the superconducting conductor should be kept below the critical temperature.
(2)コイル巻線の等価剛性を向上し、超電導4体に流
れる電流によって生じる電磁力に対する動きを押えるこ
と。(2) Improving the equivalent rigidity of the coil windings and suppressing their movement in response to the electromagnetic force generated by the current flowing through the four superconducting bodies.
この二点を改良するために、極薄絶縁を超電導導体に密
着させ、導体間の短絡のない好適な超電導コイルを形成
させる。In order to improve these two points, ultra-thin insulation is brought into close contact with the superconducting conductor to form a suitable superconducting coil without short circuits between the conductors.
第1図は、パンケーキ形コイルの構成を示したもので、
コイル巻線1は導体2および口出し線3により形成され
、この巻線1の外周をバンド4でボルト5により締付け
ている。Figure 1 shows the configuration of a pancake-shaped coil.
A coil winding 1 is formed of a conductor 2 and a lead wire 3, and the outer periphery of the winding 1 is tightened with a band 4 and a bolt 5.
一方、第2図は巻線の導体間の絶縁構成を示す。On the other hand, FIG. 2 shows the insulation structure between the conductors of the winding.
厚み約100μm、幅10mの極薄の超電導4体2の周
囲に厚み5〜10μm程度の極薄絶縁6が設けられてい
る。絶II#6には厚み5μmの基材に2〜3μmのレ
ジンを特殊な方法で塗布して、これをBステージに半硬
化させたものである。この絶縁を特殊な装置により導体
の周囲に包み込み、加熱して硬化させたものである。An ultra-thin insulator 6 with a thickness of about 5 to 10 μm is provided around the 4 ultra-thin superconducting bodies 2 with a thickness of about 100 μm and a width of 10 m. For Absolute II #6, a 2 to 3 μm thick resin was coated on a 5 μm thick base material using a special method, and this was semi-cured to B stage. This insulation is wrapped around the conductor using a special device and heated to harden it.
この種の絶縁を第2図のよう導体の厚み方向の両面に貼
付けないで、片面のみとすることも考えられるが、極薄
であり、導体間の短絡が生じるおそれが大である。この
場合、片面に厚物、例えば、導体厚みと同程度の絶縁層
を設けてもよいが、通電磁における電磁力による絶縁層
の変位量は大きくなり、コイルが動き、超電導特性が損
われる恐れがある。It is conceivable to apply this type of insulation to only one side of the conductor instead of pasting it on both sides in the thickness direction as shown in Fig. 2, but it is extremely thin and there is a high risk of short circuits occurring between the conductors. In this case, it is possible to provide a thick insulating layer on one side, for example, an insulating layer with the same thickness as the conductor, but the amount of displacement of the insulating layer due to electromagnetic force during electromagnetic conduction will be large, causing the coil to move and potentially damaging the superconducting properties. There is.
一般に、導体の弾性率を100%とすると、絶縁層の弾
性率は10〜20%程度となり、同じ電極力を受けると
絶縁層の変形率は大きい。Generally, when the elastic modulus of a conductor is 100%, the elastic modulus of an insulating layer is about 10 to 20%, and the deformation rate of an insulating layer is large when subjected to the same electrode force.
また1本発明の実施例では、極薄絶縁を導体の周囲全体
に包み込んであるが、第2図に示すように導体のエツジ
面7を包み込んで、絶縁層の切目8をクーリングチャン
ネルとしてもよい。隣の導体は第2図に示すように、絶
縁層の切目8のない面と組合わせるように構成する。こ
のように構成しても前述と同様の効果が得られる。Furthermore, in the embodiment of the present invention, the ultra-thin insulation is wrapped around the entire circumference of the conductor, but as shown in FIG. . The adjacent conductor is configured to mate with the uncut surface 8 of the insulating layer, as shown in FIG. Even with this configuration, the same effects as described above can be obtained.
このように、導体間の短絡防止を考慮した構成にしなく
てはならない。In this way, the structure must take into consideration prevention of short circuits between conductors.
以下に、極薄絶縁が必要な理由を説明する。The reason why ultra-thin insulation is necessary will be explained below.
本コイルの等価剛性、つまり、みかけ上の弾性係数は、
導体厚みtlmm、両面の合計絶縁厚みt2mそれぞれ
の材料の弾性係数E x * E x kg / il
l ” とすると等価の弾性係数は次式で表現される。The equivalent stiffness of this coil, that is, the apparent elastic modulus, is
Conductor thickness tlmm, total insulation thickness on both sides t2m, elastic modulus of each material E x * E x kg / il
l'', the equivalent elastic modulus is expressed by the following equation.
E、= (tよ+ti)/ (tt/Et+ta/E2
)この式かられかるように、絶縁物の厚みが薄く、また
、絶縁物の弾性係数の大きいものが、等価弾性係数は大
きくなり、通電時の電磁力による変位量も少なくなるこ
とがわかる。E, = (tyo+ti)/ (tt/Et+ta/E2
) As can be seen from this equation, it can be seen that the thinner the insulator is and the greater the elastic modulus of the insulator, the larger the equivalent elastic modulus and the smaller the amount of displacement due to electromagnetic force when energized.
本発明によれば、極薄の絶縁を導体周囲に包み込んであ
るので、導体間の短絡はなく、絶縁厚みも薄いので、何
らかの原因で導体が常電導に転移したときの発熱を冷媒
に伝えることができる。また、等価剛性も大きいので動
き(変位)も少なく、好適な超電導特性のコイル巻線が
得られる。According to the present invention, since the ultra-thin insulation is wrapped around the conductor, there is no short circuit between the conductors, and the thickness of the insulation is thin, so that the heat generated when the conductor changes to normal conductivity for some reason cannot be transmitted to the refrigerant. I can do it. Furthermore, since the equivalent rigidity is large, there is little movement (displacement), and a coil winding with suitable superconducting characteristics can be obtained.
第1図は本発明の一実施例の超電導4体の絶縁を示す導
体断面図、第2図は本発明の他の実施例を示す導体断面
組合せ図、第3図は、パンケーキ形超電導コイルを示す
平面図である。
1・・・超電導コイル巻線、2・・・平角超電導4体、
6・・・極薄絶縁。Fig. 1 is a cross-sectional view of a conductor showing insulation of four superconducting bodies according to an embodiment of the present invention, Fig. 2 is a combined cross-sectional view of a conductor showing another embodiment of the present invention, and Fig. 3 is a pancake-shaped superconducting coil. FIG. 1... Superconducting coil winding, 2... 4 rectangular superconducting bodies,
6...Ultra-thin insulation.
Claims (2)
ーキ形コイルにおいて、 前記超電導導体周囲に極薄の絶縁物を包み込んだことを
特徴とする超電導コイル。1. A pancake-shaped coil in which a superconducting conductor is wound flatwise in multiple layers, characterized in that an extremely thin insulator is wrapped around the superconducting conductor.
硬化状にしたものを導体周囲に設けたことを特徴とする
超電導コイル。2. A superconducting coil according to claim 1, characterized in that an extremely thin insulator comprising a base material and a thermosetting resin and semi-cured is provided around the conductor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60154030A JPS6215803A (en) | 1985-07-15 | 1985-07-15 | Superconductive coil |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60154030A JPS6215803A (en) | 1985-07-15 | 1985-07-15 | Superconductive coil |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6215803A true JPS6215803A (en) | 1987-01-24 |
Family
ID=15575371
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP60154030A Pending JPS6215803A (en) | 1985-07-15 | 1985-07-15 | Superconductive coil |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6215803A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008130785A (en) * | 2006-11-21 | 2008-06-05 | Sumitomo Electric Ind Ltd | Superconducting coil and superconducting apparatus equipped with the same |
JP2010045176A (en) * | 2008-08-12 | 2010-02-25 | Toshiba Corp | Superconducting magnet |
JP2011023724A (en) * | 2009-07-16 | 2011-02-03 | Siemens Plc | Method of manufacturing solenoidal magnet coil, and solenoidal magnet coil |
-
1985
- 1985-07-15 JP JP60154030A patent/JPS6215803A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008130785A (en) * | 2006-11-21 | 2008-06-05 | Sumitomo Electric Ind Ltd | Superconducting coil and superconducting apparatus equipped with the same |
JP2010045176A (en) * | 2008-08-12 | 2010-02-25 | Toshiba Corp | Superconducting magnet |
JP2011023724A (en) * | 2009-07-16 | 2011-02-03 | Siemens Plc | Method of manufacturing solenoidal magnet coil, and solenoidal magnet coil |
US8943676B2 (en) | 2009-07-16 | 2015-02-03 | Siemens Plc. | Method of manufacturing a solenoidal magnet structure |
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