JPS63144761A - Superconducting winding - Google Patents
Superconducting windingInfo
- Publication number
- JPS63144761A JPS63144761A JP28883686A JP28883686A JPS63144761A JP S63144761 A JPS63144761 A JP S63144761A JP 28883686 A JP28883686 A JP 28883686A JP 28883686 A JP28883686 A JP 28883686A JP S63144761 A JPS63144761 A JP S63144761A
- Authority
- JP
- Japan
- Prior art keywords
- tape
- superconducting wire
- superconducting
- winding
- wire
- 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
- 238000004804 winding Methods 0.000 title claims abstract description 59
- 238000001816 cooling Methods 0.000 claims abstract description 33
- 239000000835 fiber Substances 0.000 claims abstract description 14
- 229920000728 polyester Polymers 0.000 claims abstract description 6
- 239000000919 ceramic Substances 0.000 claims description 6
- 239000004952 Polyamide Substances 0.000 claims description 2
- 239000004698 Polyethylene Substances 0.000 claims description 2
- 239000004642 Polyimide Substances 0.000 claims description 2
- 229920002647 polyamide Polymers 0.000 claims description 2
- -1 polyethylene Polymers 0.000 claims description 2
- 229920000573 polyethylene Polymers 0.000 claims description 2
- 229920001721 polyimide Polymers 0.000 claims description 2
- 210000003298 dental enamel Anatomy 0.000 claims 1
- 239000012209 synthetic fiber Substances 0.000 claims 1
- 229920002994 synthetic fiber Polymers 0.000 claims 1
- 239000004745 nonwoven fabric Substances 0.000 abstract description 16
- 239000004744 fabric Substances 0.000 abstract description 3
- 238000010438 heat treatment Methods 0.000 abstract description 3
- 239000004020 conductor Substances 0.000 description 17
- 229910052734 helium Inorganic materials 0.000 description 9
- 239000001307 helium Substances 0.000 description 9
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 9
- 239000007788 liquid Substances 0.000 description 9
- 238000010791 quenching Methods 0.000 description 7
- 230000000171 quenching effect Effects 0.000 description 7
- 230000000694 effects Effects 0.000 description 6
- 238000009413 insulation Methods 0.000 description 6
- 238000000034 method Methods 0.000 description 4
- 239000000853 adhesive Substances 0.000 description 3
- 230000001070 adhesive effect Effects 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 2
- 239000003990 capacitor Substances 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 239000003822 epoxy resin Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 229920000647 polyepoxide Polymers 0.000 description 1
- 238000003825 pressing Methods 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
Landscapes
- Superconductive Dynamoelectric Machines (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は超電導発電機に用いる超電導界磁巻線に係り、
特に、冷却性向上を図った界磁巻線に関する。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a superconducting field winding used in a superconducting generator,
In particular, it relates to field windings with improved cooling performance.
超電導線を密巻きした、例えば、超電導発電機−リング
チャンネルを形成することはむずかしい。It is difficult to form a superconducting generator-ring channel in which superconducting wires are closely wound, for example.
密巻き巻線にすると導体間にギャップがほとんどできな
いので、絶縁性も問題であるが、液体ヘリウムの通流す
るクーリングチャンネルがないために冷却性が悪く、外
部擾乱等による過渡時に超電導界磁巻線はクエンチを起
す問題があった。このようなことから、特開昭54−7
509号公報に示されているように、ガラスクロステー
プにエポキシ樹脂を含浸して半硬化させたセミキュアテ
ープを超電導線の表面にある幅の間隔をあけて螺旋状に
巻回して、巻線導体間にクーリングチャンネルの形状と
絶縁を行っていた。このようにすると螺旋状の長いクー
リングチャンネルが形成され、液体ヘリウムの流れが悪
く、セミキュアテープが巻線導体に接着している部分は
冷却されないので、超電導界磁巻線の冷却性は十分でな
く過渡時にクエンチを起すこともあった。また、絶縁性
の点では、セミキュアテープがある幅の間隔をあけて導
体に巻か・れているため、セミキュアテープの巻かれて
いない所同士が接触して短絡を起し、これが原因で超電
導界磁巻線はクエンチを起し焼損することもあった。Insulation is also a problem because there are almost no gaps between the conductors when the winding is tightly wound, but there is no cooling channel for liquid helium to flow, so the cooling performance is poor, and the superconducting field winding is difficult to maintain during transients caused by external disturbances. The line had the problem of quenching. For this reason, Japanese Unexamined Patent Application Publication No. 54-7
As shown in Publication No. 509, a semi-cured glass cloth tape impregnated with an epoxy resin and semi-cured is wound spirally on the surface of a superconducting wire at intervals of a certain width. Cooling channels were shaped and insulated between the conductors. In this way, a long spiral cooling channel is formed, the flow of liquid helium is poor, and the part where the semi-cure tape is bonded to the winding conductor is not cooled, so the cooling performance of the superconducting field winding is insufficient. In some cases, quenching occurred during transient periods. In addition, in terms of insulation, since the semi-cure tape is wrapped around the conductor at a certain width interval, the unwrapped parts of the semi-cure tape may come into contact with each other and cause a short circuit. In some cases, the superconducting field windings were quenched and burned out.
上記従来技術は超電導界磁巻線内部のクーリングチャン
ネルの方向性1巻線導体の冷却面積及び絶縁性について
十分に考慮されておらず、過渡時に超電導界磁巻線のク
エンチ及び短絡焼損の問題があった。The above-mentioned conventional technology does not sufficiently consider the cooling area and insulation of the directional single-turn conductor of the cooling channel inside the superconducting field winding, resulting in problems such as quenching of the superconducting field winding and short-circuit burnout during transients. there were.
本発明の目的は巻線の冷却性及び絶縁性を向上させ、ク
エンチ及び短絡焼損のない超電導界磁巻線を提供するこ
とにある。An object of the present invention is to provide a superconducting field winding that improves the cooling performance and insulation properties of the winding and is free from quenching and short-circuit burnout.
すなわち、本発明は、ポリエステル繊維等からなる不織
布に加熱した金網を当てて、縦方向、及び、横方向の溝
を設け、この不織布からテープを切り出してこのテープ
を超電導線の表面に半掛け1回の絶縁をしてドラムに巻
回したのち、通電により超電導線を加熱して不織布テー
プを自己融着させる。この絶縁さ九た超電導線をソレノ
イド状。That is, in the present invention, a heated wire mesh is applied to a nonwoven fabric made of polyester fiber or the like to form vertical and horizontal grooves, a tape is cut out from this nonwoven fabric, and the tape is hung halfway on the surface of a superconducting wire. After the superconducting wire is insulated and wound around a drum, the superconducting wire is heated by electricity to self-fuse the nonwoven tape. This insulated superconducting wire is shaped like a solenoid.
又は、鞍形状に巻線して数層口ごとにバインドを行って
巻線導体が電磁力等で動かないように強力に支持する。Alternatively, the wire is wound in a saddle shape and bound every few layers to strongly support the wire conductor so that it does not move due to electromagnetic force or the like.
こうすることによって、巻線内部には径方向2周方向及
び軸方向のクーリングチャンネルができて冷却性は良く
、巻線導体は全表面絶縁されているので電磁力等により
、巻線導体が引合って短絡も起すようなことがない。By doing this, cooling channels are created inside the winding in two circumferential directions in the radial direction and in the axial direction, resulting in good cooling performance.Since the entire surface of the winding conductor is insulated, the winding conductor is not pulled by electromagnetic force, etc. There is no chance of a short circuit occurring if the capacitors meet.
本発明ではポリエステル繊維等から成る溝付テ−プを超
電導線に巻回して用いるが、ただ、巻回しただけでは巻
線作業の際にゆるんだり、はぐれたりして具合が悪く、
さりとて、接着剤を導体又はテープに塗ったのではテー
プの目づまり、又は、接着剤が導体表面を覆うため液体
ヘリウムが導体に直接触れないので冷却性が悪い。本発
明のようにテープを超電導線に自己融着させればテープ
はほぐれることなく、液体ヘリウムは自己融着されてい
る所以外では導体と直接触れるので、冷却効果は大であ
る。テープとしては不織布又は組込布のどちらでもよい
が、目の粗いテープの方が冷却効果は大である。クーリ
ングチャンネルは巻線の径方向、周方向及び軸方向に形
成され、液体ヘリウムが流れ易くなって冷却性能が向上
する。In the present invention, a grooved tape made of polyester fiber or the like is used by winding it around a superconducting wire, but simply winding it causes the wire to loosen or come off during the winding process, making it uncomfortable.
However, if adhesive is applied to the conductor or tape, the tape will become clogged, or the adhesive will cover the surface of the conductor, so liquid helium will not come into direct contact with the conductor, resulting in poor cooling performance. If the tape is self-fused to the superconducting wire as in the present invention, the tape will not come undone, and the liquid helium will come into direct contact with the conductor in areas other than the areas where it is self-fused, so the cooling effect will be great. The tape may be made of either non-woven fabric or incorporated fabric, but coarse tape has a greater cooling effect. Cooling channels are formed in the radial, circumferential, and axial directions of the winding, making it easier for liquid helium to flow, improving cooling performance.
テープ溝の深さは0.1mm程度であるが、過渡時に発
生する巻線の損失を除去するのにはこの程度の溝で十分
である。また、超電導線はこのテープで全面が覆われて
いるので巻線導体間で短絡を起すようなことはなく、巻
線の絶縁の面からも効果が大きい。The depth of the tape groove is approximately 0.1 mm, but a groove of this depth is sufficient to eliminate winding loss that occurs during transition. Furthermore, since the entire surface of the superconducting wire is covered with this tape, short circuits do not occur between the winding conductors, and this is highly effective in terms of winding insulation.
以下、図示した実施例に基づいて本発明を説明する。第
1図ないし第6図には本発明の一実施例が示されている
。第2図は本発明に用いるポリエステル繊維の不織布1
から成る縦、横の溝2付きの絶縁テープ3を示す。不織
布に縦、横の溝2を付ける作業は、幅広の不織布に18
0℃程度に加熱した金網を押し当てて行う。絶縁テープ
3はこの方法で溝を付けた幅広の不織布から10〜15
mの幅に切り出して作る。溝2の深さは不織布の厚さに
よって異るが、0.2■厚さの不織布で0.10 ny
n程度が可能である。溝幅は4W11とした。The present invention will be explained below based on the illustrated embodiments. An embodiment of the present invention is shown in FIGS. 1-6. Figure 2 shows a polyester fiber nonwoven fabric 1 used in the present invention.
An insulating tape 3 with vertical and horizontal grooves 2 is shown. The work of creating vertical and horizontal grooves 2 on the non-woven fabric is done using a 18 mm
This is done by pressing a wire mesh heated to around 0°C. The insulating tape 3 is made of a wide non-woven fabric with grooves made using this method.
Cut it out to a width of m. The depth of groove 2 varies depending on the thickness of the nonwoven fabric, but it is 0.10 ny for a nonwoven fabric with a thickness of 0.2 mm.
About n is possible. The groove width was 4W11.
第3図は超電導線4に絶縁テープ3を無掛けで巻いてド
ラムに巻回し、このドラムに通電を行って超電導線を1
80℃程度に加熱して不織布1の繊維を超電導線表面に
自己融着させる絶縁超電導線5の一実施例を示す。繊維
の自己融着面6は強力に接着し、絶縁テープ3が超電導
線4から簡単には剥れない。なお、自己融着には種々な
加熱方法が考えられるが、上記の方法が有効である。Figure 3 shows the superconducting wire 4 wrapped with insulating tape 3 without being wrapped around a drum, and the drum being energized to separate the superconducting wire 1.
An example of an insulated superconducting wire 5 is shown in which the fibers of the nonwoven fabric 1 are self-fused to the surface of the superconducting wire by heating to about 80° C. The self-fusing surface 6 of the fibers is strongly adhered, and the insulating tape 3 is not easily peeled off from the superconducting wire 4. Although various heating methods can be used for self-fusion, the above method is effective.
第4図は第3図に示した絶縁超電導線5を用いて製作し
た超電導発電機用の鞍形超電導界磁巻線7を示す。第4
図のv−V線に沿う断面を第5図に示す。絶縁超電導線
5が密巻きされており、バインド用テープ8によってコ
イル9の支持を行い、鞍形超電導界磁巻線7を形成して
いる。FIG. 4 shows a saddle-shaped superconducting field winding 7 for a superconducting generator manufactured using the insulated superconducting wire 5 shown in FIG. 3. Fourth
FIG. 5 shows a cross section taken along the line v--v in the figure. An insulated superconducting wire 5 is tightly wound, a coil 9 is supported by a binding tape 8, and a saddle-shaped superconducting field winding 7 is formed.
第5図の密巻きされている巻線の一部分の詳細を第1図
に示す。超電導線4に自己融着されている不織布1は繊
維間の目が粗いために液体ヘリウムの出入が容易であり
、超電導線4の冷却性は非常に良い。巻線の径方向には
径方向クーリングチャンネル10が形成され、周方向ク
ーリングチャンネル11が、軸方向には軸方向クーリン
グチャンネル12aが形成されている。又、絶縁超電導
線5の四隅には軸方向のクーリングチャンネル12bが
形成されている。このように、クーリングチャンネルが
多く形成されているので液体ヘリウムの流れは良く、冷
却性の良好な超電導界磁巻線が得られる。A detail of a portion of the tightly wound winding of FIG. 5 is shown in FIG. Since the nonwoven fabric 1 that is self-fused to the superconducting wire 4 has coarse mesh between the fibers, liquid helium can easily enter and exit the nonwoven fabric 1, and the cooling performance of the superconducting wire 4 is very good. A radial cooling channel 10 is formed in the radial direction of the winding, a circumferential cooling channel 11 is formed, and an axial cooling channel 12a is formed in the axial direction. Furthermore, axial cooling channels 12b are formed at the four corners of the insulated superconducting wire 5. In this way, since many cooling channels are formed, the flow of liquid helium is good, and a superconducting field winding with good cooling performance can be obtained.
本実施例の効果を従来例と比較検討した結果を第6図に
示す。同図は縦軸に従来例を1.0 とした場合の巻線
電流密度をとり、横軸に従来例を1.0 とした場合
の磁界をとって、磁界と巻線電流密度との関係を示した
ものである。同図から明らかなように、本実施例の超電
導界磁巻線の特性Pは、従来例の特性Qに比べて巻線電
流密度が大きく優れており、線材の特性Rは近い特性に
なっている。すなわち、従来の超電導界磁巻線は巻線電
流密度が1パーユニツト(P、U、)でクエンチを起す
のに対し、本実施例の超電導界磁巻線では巻線電流密度
が1.3P、U、でクエンチを起すようになる。このよ
うに本実施例の超電導界磁巻線の特性が向上したのは、
超電導線に縦、横方向の溝を設けた不織布絶縁テープを
巻回し、自己融着によって超電導線が液体ヘリウムと直
接触れる面積が増大したことと、巻線導体間に径方向9
周方向及び軸方向のクーリングチャンネルを多く形成し
たことにより、巻線導体間に液体ヘリウムが流れ易くな
って冷却性が大幅に向上したことによるものである。FIG. 6 shows the results of comparing the effects of this embodiment with the conventional example. The figure shows the relationship between the magnetic field and the winding current density, with the vertical axis representing the winding current density when the conventional example is set to 1.0, and the horizontal axis representing the magnetic field when the conventional example is set to 1.0. This is what is shown. As is clear from the figure, the characteristic P of the superconducting field winding of this example is much superior to the characteristic Q of the conventional example in terms of winding current density, and the characteristic R of the wire is similar. There is. That is, while the conventional superconducting field winding quenches when the winding current density is 1 per unit (P, U,), the superconducting field winding of this embodiment has a winding current density of 1.3 P, U, will cause quenching. The characteristics of the superconducting field winding of this example were improved in this way because
The superconducting wire is wound with a non-woven insulating tape with vertical and horizontal grooves, and self-fusion increases the area in which the superconducting wire comes into direct contact with liquid helium, and the radial 9-9 area between the wound conductors increases.
This is because by forming many cooling channels in the circumferential direction and the axial direction, liquid helium can easily flow between the winding conductors, greatly improving cooling performance.
なお、本実施例では合成繊維の不織布としてポリエステ
ルを使用したが、ポリイミド、ポリアミド及びポリエチ
レンを使用しても同様の効果がある。In this example, polyester was used as the synthetic nonwoven fabric, but the same effect can be obtained by using polyimide, polyamide, or polyethylene.
また、本実施例では不織布の絶縁テープを使用したが、
繊維を網込んだ絶縁テープを使用してもよい。In addition, in this example, non-woven insulating tape was used, but
Insulating tape interwoven with fibers may also be used.
巻線の剛性、及び、冷却性を一段と向上することができ
る。セラミックステープ13は両側に縦。The rigidity and cooling performance of the winding can be further improved. Ceramic tape 13 is vertical on both sides.
横の溝14が設けられており、貫通孔15によって連通
されている。このセラミックステープ13に接着剤を塗
り、超電導線の外周に無掛けで巻回して絶縁超電導線を
形成し、これを巻回して鞍形の超電導界磁巻線を製作す
る。A horizontal groove 14 is provided and communicated by a through hole 15. This ceramic tape 13 is coated with adhesive and wound around the outer periphery of the superconducting wire to form an insulated superconducting wire, which is then wound to produce a saddle-shaped superconducting field winding.
第8図は鞍形超電導界磁巻線の断面のその一部分を示す
。クーリングチャンネルは本発明の超電導界磁巻線と同
様に、径方向クーリングチャンネル16、周方向クーリ
ングチャンネル17.軸方向クーリングチャンネル18
a、18bが形成される。FIG. 8 shows a portion of a cross section of a saddle-shaped superconducting field winding. Similar to the superconducting field winding of the present invention, the cooling channels include a radial cooling channel 16, a circumferential cooling channel 17. Axial cooling channel 18
a, 18b are formed.
セラミックスは剛性が大きいために巻線の動きを微小に
することができ、又、熱伝導率が大きく、冷部に効果的
なり−リングチャンネルを多く形成することができるの
で、クエンチの少ない安定度の高い高電流密度の超電導
界磁巻線を得ることかできる。Ceramics has high rigidity, so it is possible to minimize the movement of the winding wire, and it also has high thermal conductivity, making it effective for cold parts - many ring channels can be formed, resulting in stability with less quenching. It is possible to obtain superconducting field windings with high current densities.
c′発明の効果〕
本発明によれば、超電導界磁巻線の冷却性が向上するの
で微小の巻線導体の動きがあってもクエンチは起さず、
また、超電導線の全表面が絶縁テープで覆われているの
で、電磁力及び遠心力等で巻線導体間が短絡を起すよう
なこともなく、安定度の高い高電流密度の超電導界磁巻
線が得られる。c′ Effect of the invention] According to the present invention, the cooling performance of the superconducting field winding is improved, so even if there is minute movement of the winding conductor, quenching does not occur.
In addition, since the entire surface of the superconducting wire is covered with insulating tape, there is no short circuit between the winding conductors due to electromagnetic force, centrifugal force, etc., and the superconducting field winding has a highly stable high current density. A line is obtained.
第1図は本発明の超電導界磁巻線の一実施例の断面図、
第2図は本発明の超電導界磁巻線に用いる溝付き絶縁テ
ープの断面図、第3図は本発明の超電導界磁巻線に用い
る絶縁超電導線の斜視図、第4図は本発明の超電導界磁
巻線の斜視図、第5図は第4図の■−■線に沿う断面図
、第6図は本発明の超電導界磁巻線の実施例と従来例の
コイル電流密度と磁界との関係を示す特性図、第7図は
ワンステップ先行発明の超電導界磁巻線に使用するセラ
ミックステープの斜視図、第8図はワンステップ先行発
明の超電導界磁巻線の一部分断面図である。
1・・・不織布、2・・・溝、3・・・溝付き絶縁テー
プ。FIG. 1 is a sectional view of an embodiment of the superconducting field winding of the present invention;
FIG. 2 is a sectional view of a grooved insulating tape used in the superconducting field winding of the present invention, FIG. 3 is a perspective view of an insulated superconducting wire used in the superconducting field winding of the present invention, and FIG. A perspective view of a superconducting field winding, FIG. 5 is a sectional view taken along the line ■-■ in FIG. 4, and FIG. 6 is a coil current density and magnetic field of an embodiment of the superconducting field winding of the present invention and a conventional example Figure 7 is a perspective view of the ceramic tape used in the superconducting field winding of the one-step prior invention, and Figure 8 is a partial cross-sectional view of the superconducting field winding of the one-step prior invention. be. 1... Nonwoven fabric, 2... Groove, 3... Grooved insulation tape.
Claims (1)
導線を巻回した超電導巻線において、前記繊維状テープ
はポリエステム繊維、ポリイミド繊維、ポリアミド繊維
及びポリエチレン繊維等の合成繊維から成り、前記繊維
状テープには縦及び横方向に溝を設け、前記繊維状テー
プを裸またはエナメルコーティングした超電導線の表面
に巻回して径方向、周方向及び軸方向のクーリングチャ
ンネルを形成させたことを特徴とする超電導巻線。 2、特許請求の範囲第1項において、 溝付きの前記絶縁テープを前記超電導線に自己融着させ
ることを特徴とする超電導巻線。 3、特許請求の範囲第1項において、 繊維状の前記溝付き絶縁テープの代りにセラミックステ
ープを用い前記セラミックステープの表、裏の両面に縦
及び横方向の溝を設け、前記溝は連通することを特徴と
する超電導巻線。[Claims] 1. A superconducting wire in which an insulated superconducting wire is wound with a fibrous tape wound around the surface of the superconducting wire, wherein the fibrous tape is made of polyester fiber, polyimide fiber, polyamide fiber, polyethylene fiber, etc. The fibrous tape is made of synthetic fibers, the fibrous tape is provided with grooves in the longitudinal and lateral directions, and the fibrous tape is wound around the surface of the bare or enamel-coated superconducting wire to create radial, circumferential and axial cooling channels. A superconducting winding characterized by forming a superconducting wire. 2. The superconducting winding according to claim 1, wherein the grooved insulating tape is self-fused to the superconducting wire. 3. In claim 1, a ceramic tape is used instead of the fibrous grooved insulating tape, vertical and horizontal grooves are provided on both sides of the ceramic tape, and the grooves communicate with each other. A superconducting winding wire characterized by:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28883686A JPS63144761A (en) | 1986-12-05 | 1986-12-05 | Superconducting winding |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28883686A JPS63144761A (en) | 1986-12-05 | 1986-12-05 | Superconducting winding |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63144761A true JPS63144761A (en) | 1988-06-16 |
Family
ID=17735378
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP28883686A Pending JPS63144761A (en) | 1986-12-05 | 1986-12-05 | Superconducting winding |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63144761A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02254964A (en) * | 1989-03-28 | 1990-10-15 | Chiyoudendou Hatsuden Kanren Kiki Zairyo Gijutsu Kenkyu Kumiai | Rotor for superconducting rotary electric machine |
-
1986
- 1986-12-05 JP JP28883686A patent/JPS63144761A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02254964A (en) * | 1989-03-28 | 1990-10-15 | Chiyoudendou Hatsuden Kanren Kiki Zairyo Gijutsu Kenkyu Kumiai | Rotor for superconducting rotary electric machine |
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