JPS61272903A - Saddle type superconductive field winding - Google Patents
Saddle type superconductive field windingInfo
- Publication number
- JPS61272903A JPS61272903A JP11416585A JP11416585A JPS61272903A JP S61272903 A JPS61272903 A JP S61272903A JP 11416585 A JP11416585 A JP 11416585A JP 11416585 A JP11416585 A JP 11416585A JP S61272903 A JPS61272903 A JP S61272903A
- Authority
- JP
- Japan
- Prior art keywords
- winding
- saddle
- tape
- conductors
- semicured
- 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
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/06—Coils, e.g. winding, insulating, terminating or casing arrangements therefor
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Superconductive Dynamoelectric Machines (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の利用分野〕
本発明は超電導発電機に使用する鞍形超電導界磁巻線に
係り、特に、支持及び冷却を改良した高電流密度の鞍形
超電導界磁巻線に関する。Detailed Description of the Invention [Field of Application of the Invention] The present invention relates to a saddle-shaped superconducting field winding for use in a superconducting generator, and more particularly to a saddle-shaped superconducting field winding with improved support and cooling. Regarding lines.
第3図に超電導発電機に組込まれた超電導回転子の従来
例を示す、超電導回転子は円筒状トルクチューブ1、鞍
形超電導界磁巻線2A、2B、ヘリウム容器3.ダンパ
4および、回転軸5A。FIG. 3 shows a conventional example of a superconducting rotor incorporated in a superconducting generator. The superconducting rotor includes a cylindrical torque tube 1, saddle-shaped superconducting field windings 2A and 2B, a helium container 3. damper 4 and rotating shaft 5A.
5Bから構成される、これら回転軸5A、5Bは軸受6
A、6Bにより、それぞれ、支承されている。そして、
反駆動側軸端には液体ヘリウム導入ロア、ガスヘリウム
排出口8が設けられ、液体ヘリウム導入ロアより供給さ
れる液体ヘリウム9により鞍形超電導界磁巻線2A、2
Bは冷却されて、約4.2” Kの極低温状態に維持さ
れる。この鞍11Bを介して直流電源12から電流が供
給されて行われる。なお、13は固定子巻線、14は固
定子鉄心、15はフレームである。鞍形超電導界磁巻線
2A、2Bは第4図及び第5図に示すように、円筒状ト
ルクチューブ1の外周側に設けられた鞍形の溝に挿入さ
れ、その挿入された鞍形超電導界磁巻線2A’、2Bの
外周上にはバインド線16が巻付けられ、このバインド
線の外周上には。5B, these rotating shafts 5A and 5B have bearings 6
It is supported by A and 6B, respectively. and,
A liquid helium introduction lower and a gas helium discharge port 8 are provided at the non-drive side shaft end, and the saddle-shaped superconducting field windings 2A, 2 are supplied with liquid helium 9 supplied from the liquid helium introduction lower.
B is cooled and maintained at an extremely low temperature of about 4.2" K. Current is supplied from the DC power supply 12 through this saddle 11B. Note that 13 is a stator winding, and 14 is a stator winding. The stator core 15 is a frame.The saddle-shaped superconducting field windings 2A and 2B are inserted into saddle-shaped grooves provided on the outer circumferential side of the cylindrical torque tube 1, as shown in FIGS. 4 and 5. A bind wire 16 is wound on the outer periphery of the inserted saddle-shaped superconducting field windings 2A', 2B, and on the outer periphery of this bind wire.
同心内のFRP層17が設けられ、この外周上に補強円
筒(図示せず)が焼嵌められる。鞍形超電導界磁巻線2
A、2Bの冷却は、トルクチューブlの内周側に充填さ
れている液体ヘリウム9が遠心力で鞍形超電導界磁巻線
の方へ押しやられ、鞍形超電導界磁巻線の内周側に設け
られたクーリングチャンネル18を流れて行われる。A concentric FRP layer 17 is provided, onto which a reinforcing cylinder (not shown) is shrink-fitted. Saddle-shaped superconducting field winding 2
The cooling of A and 2B is achieved by pushing the liquid helium 9 filled in the inner circumferential side of the torque tube l toward the saddle-shaped superconducting field winding by centrifugal force, The water flows through a cooling channel 18 provided in the air.
超電導界磁巻線2A、2Bには、第6図に示すように、
超電導線が鞍形に巻回され、巻線全体にエポキシ樹脂が
含浸されている。このため、巻線導体の動きを抑えるこ
とはできるが、巻線外周面しか冷却できないので、冷却
性が悪くなる欠点がある。第6図および第7図で、超電
導線19間に含浸されたエポキシ樹脂20は、加熱硬化
時に収縮して歪が発生し歪応力として残る。この超電導
界磁巻線2A、2Bを回転子に取付け、液体ヘリウムで
冷却して回転励磁を行うと、超電導界磁巻線には熱収縮
応力、電磁応力及び遠心応力が加わり、含浸エポキシ樹
脂20の歪は局部的に開放されてクラック21を発生す
ることがある。エポキシ樹脂は分子間の結合力が大きい
ため、クラッチ発生エネルギも大きく、クラック発生時
には、超電導界磁巻線をクエンチさせるのに十分な熱を
発生する。このクエンチ発生熱は巻線の冷却性が悪いた
め、超電導線19に伝導し、局部的に温度上昇してクエ
ンチを起す、このため、巻線の電流密度を十分に大きく
できない欠点がある。As shown in FIG. 6, the superconducting field windings 2A and 2B include
A superconducting wire is wound into a saddle shape, and the entire winding is impregnated with epoxy resin. Therefore, although the movement of the winding conductor can be suppressed, only the outer circumferential surface of the winding can be cooled, so there is a drawback that the cooling performance deteriorates. In FIGS. 6 and 7, the epoxy resin 20 impregnated between the superconducting wires 19 contracts during heating and curing to generate strain, which remains as strain stress. When these superconducting field windings 2A and 2B are attached to a rotor, cooled with liquid helium, and rotationally excited, thermal contraction stress, electromagnetic stress, and centrifugal stress are applied to the superconducting field windings, and the impregnated epoxy resin 20 The strain may be locally released and cause a crack 21. Since epoxy resin has a large intermolecular bonding force, the clutch generation energy is large, and when a crack occurs, sufficient heat is generated to quench the superconducting field winding. This quench-generated heat is conducted to the superconducting wire 19 due to the poor cooling properties of the winding, causing a local temperature rise and quenching.Therefore, there is a drawback that the current density in the winding cannot be sufficiently increased.
このように、樹脂含浸巻線は冷却性及びクラック発生の
問題があるので、巻線の動きはある程度犠牲にしても、
樹脂を含浸しないで冷却性をよくする方法も採用されて
いる0例えば、米国特許3.816,780のように、
トルクチューブの外周上に超電導線を鞍形に巻回して一
層ごとにバンドで締付ける方法がある。この方法による
と。In this way, resin-impregnated windings have problems with cooling performance and crack generation, so even if the movement of the windings is sacrificed to some extent,
Methods to improve cooling performance without impregnating with resin have also been adopted. For example, as in U.S. Patent No. 3,816,780,
There is a method of winding superconducting wire in a saddle shape around the outer circumference of a torque tube and tightening each layer with a band. According to this method.
鞍形に巻線す際に十分な張力をかけることができず、巻
線に弛みが生じ易い、このため、巻線導体は電磁力及び
遠心力で動き易く、摩擦熱及びうず電流積の発生により
、超電導界磁巻線の性能は低下する。When winding the wire in a saddle shape, it is not possible to apply sufficient tension, and the winding wire tends to loosen.As a result, the winding conductor tends to move due to electromagnetic force and centrifugal force, causing frictional heat and eddy current products. As a result, the performance of the superconducting field winding decreases.
本発明の目的は、巻線の動きを少なくシ、冷却性をよく
して安定性のある高電流密度な鞍形超電導界磁巻線を提
供することにある。SUMMARY OF THE INVENTION An object of the present invention is to provide a saddle-shaped superconducting field winding with reduced winding movement, improved cooling performance, and stable high current density.
本発明の要点は、エポキシ樹脂含浸セミキュアテープを
巻線導体間に縫うように挿入してレーストラック状超電
導巻線を形成し、これを半円柱及び半円筒型を使用して
プレスにより鞍形巻線とし、この鞍形巻線をトルクチュ
ーブに複数個積み重ねてバインド支持により鞍形超電導
界磁巻線を形成することにある。The main point of the present invention is to form a racetrack-shaped superconducting winding by threading an epoxy resin-impregnated semi-cured tape between the winding conductors, and press this into a saddle shape using a semi-cylindrical and semi-cylindrical mold. A saddle-shaped superconducting field winding is formed by stacking a plurality of saddle-shaped windings on a torque tube and supporting them by binding.
第1図、第2図及び第8図ないし第12@に本発明の一
実施例を示す。An embodiment of the present invention is shown in FIGS. 1, 2, and 8 to 12@.
第8図はレーストラック状の超電導巻線で、この巻線か
ら本発明の鞍形超電導巻線を形成する。FIG. 8 shows a racetrack-shaped superconducting winding from which a saddle-shaped superconducting winding of the present invention is formed.
巻線はダブルパンケーキ巻線方式で行ない1巻線部体1
9間にはエポキシ樹脂を含浸して半硬化させたセミキュ
アガスチーブ22を巻線の導体間を縫うように挿入して
巻線導体19を抑え、接続部なしの複数列で二層のレー
ストラック状超電導巻線23を製作する。断面部で、セ
ミキュアテープ22が挿入されていない所は空間24が
形成され、セミキュアテープ22を挿入した所は、巻線
導体間を縫うように挿入されている。このように形成さ
れたレーストラック状巻線を第11図に示すように半円
柱状の型台25に乗せ、レーストラック状巻線23の上
側に半円筒状の型26を乗せて上方向(矢印)より力を
加えてプレスを行ない、同時に、プレス状態でセミキュ
アガラステープを加熱硬化することにより、弛みのない
鞍形超電導巻線を形成することができる。レーストラッ
ク状の巻線し易く、緊密に巻けること、及び、プレスに
より鞍形を形成する時に、巻線のコーナ部が曲げられて
巻線全体が緊密に締るので、前述のような、鞍形巻線を
製作するのには好適である。前述の鞍形超電導巻線27
を第1図に示す、セミキュアテープは上・下巻線とも巻
回方向にある間隔をあけて多数列挿入されている。第2
図の断面部では上層巻線の導体間にセミキュアガラステ
ープ22が巻線導体間を縫う−ように二列隣接して挿入
されており、その−列目と二列目のセミキュアガラステ
−プ22は巻線導体19を一本ずらして挿入されている
。このため1巻線導体19はセミキュアガラステープ2
2によって組込まれるようになって良く抑えられ、前述
の方法で巻線をプレスした時に列から飛び出すことはな
い、上層巻線及び下層巻線とも、セミキュアガラステー
プの挿入しないところは、空間24が形成される。この
ようにして形成した鞍形超電導巻線のトルクチューブへ
の支持を第12図に示す、複数列、二層に巻回した鞍形
超電導巻線27A、27Bをトルクチューブの鞍形スロ
ットに複数個積み重ねてバンド28をかけ、鞍形超電導
界磁巻線2A、2Bの形成する。鞍形超電導界磁巻線2
A、2Bの側面とトルクチューブ1との間の隙間には接
着剤29を詰めて巻線の動きをなくす、このように構成
することにより、鞍形超電導界磁巻線2A、2Bは電磁
力及び遠心力が加わってもほとんど動かなくなる0巻線
内部の空間24は液体ヘリウムの通るクーリングチャン
ネルとなるので冷却性が非常によく1巻線の微小の動き
による発生熱を速やかに除去できる効果がある。Winding is done using the double pancake winding method, with 1 winding body 1
9, a semi-cured gas tube 22 impregnated with epoxy resin and semi-hardened is inserted between the winding conductors to hold down the winding conductor 19, and a two-layer lace is formed in multiple rows without connecting parts. A track-shaped superconducting winding 23 is manufactured. In the cross section, a space 24 is formed where semi-cure tape 22 is not inserted, and where semi-cure tape 22 is inserted, it is inserted so as to thread between the winding conductors. The racetrack winding thus formed is placed on a semi-cylindrical mold base 25 as shown in FIG. By pressing with more force (arrow) and at the same time heating and curing the semi-cured glass tape in the pressed state, a saddle-shaped superconducting winding with no slack can be formed. It is easy to wind the wire in a racetrack shape and it can be wound tightly, and when the saddle shape is formed by pressing, the corners of the winding are bent and the entire winding is tightly tightened. It is suitable for producing shaped windings. The aforementioned saddle-shaped superconducting winding 27
As shown in FIG. 1, multiple rows of semi-cured tape are inserted in both the upper and lower windings at certain intervals in the winding direction. Second
In the cross section shown in the figure, two adjacent rows of semi-cured glass tape 22 are inserted between the conductors of the upper winding, threading between the winding conductors, and the semi-cured glass tape 22 in the second and second rows is inserted between the conductors of the upper winding. - The loop 22 is inserted with the winding conductor 19 shifted by one line. Therefore, the first winding conductor 19 is made of semi-cured glass tape 2.
2, the semi-cured glass tape is not inserted into the space 24 for both the upper layer winding and the lower layer winding. is formed. The saddle-shaped superconducting windings formed in this manner are supported on the torque tube as shown in FIG. The superconducting field windings 2A and 2B are formed by stacking them and applying a band 28. Saddle-shaped superconducting field winding 2
The gaps between the side surfaces of A and 2B and the torque tube 1 are filled with adhesive 29 to eliminate movement of the windings. With this configuration, the saddle-shaped superconducting field windings 2A and 2B are free from electromagnetic force. The space 24 inside the 0th winding, which hardly moves even when centrifugal force is applied, becomes a cooling channel through which liquid helium passes, so the cooling performance is very good and the heat generated by the minute movement of the 1st winding can be quickly removed. be.
(発明の効果〕
本発明によれば、回転励磁による電磁力及び遠心力で巻
線導体に微小な動きがあっても摩擦等の発生熱は速やか
に除去されるので巻線の超電導性は安定する。(Effects of the Invention) According to the present invention, even if there is minute movement in the winding conductor due to electromagnetic force and centrifugal force due to rotational excitation, heat generated due to friction etc. is quickly removed, so the superconductivity of the winding is stable. do.
第゛1図は本発明の一実施例の鞍形超電導巻線の斜視図
、第2図は第1図のn−n矢視断面図、第3図は従来の
超電導回転子を使用した超電導発電機の縦断面図、第4
図は第3図のM枠部の斜視図。
第5図は第4図の■−■矢視断面図、第6図は従来の鞍
形超電導界磁巻線の斜視図、第7図は第6図の■−■断
面図、第8図は本発明の鞍形超電導巻線を形成する前の
レーストラック状超電導巻線の平面図、第9図は第8図
の[−1に、矢視断面図。
第10図は第8図のX−X矢視断面図、第11図は本0
発明の鞍形超電導巻線を形成方法の斜視図。
第12図は本発明の鞍形超電導巻線を複数個積み重ねて
形成した鞍形超電導界磁巻線の斜視図である。
2A、2B・・・鞍形超電導界磁巻線t19・・・巻線
導体、22・・・樹脂含浸セミキュアガラステープ、第
152]
第252]
24 IQ
第3図
第4図
第5121
第 b 口
ZA・ZF3
第71iJ
第6回
第9 図
2卒
第1o口
寮IZ団Fig. 1 is a perspective view of a saddle-shaped superconducting winding according to an embodiment of the present invention, Fig. 2 is a sectional view taken along the nn arrow in Fig. 1, and Fig. 3 is a superconducting coil using a conventional superconducting rotor. Vertical cross-sectional view of the generator, No. 4
The figure is a perspective view of the M frame portion in FIG. 3. Fig. 5 is a sectional view taken along the line ■-■ in Fig. 4, Fig. 6 is a perspective view of a conventional saddle-shaped superconducting field winding, Fig. 7 is a sectional view taken along -■ in Fig. 6, and Fig. 8 9 is a plan view of the racetrack-shaped superconducting winding before forming the saddle-shaped superconducting winding of the present invention, and FIG. 9 is a cross-sectional view taken along arrows [-1] in FIG. Fig. 10 is a sectional view taken along the line X-X in Fig. 8, and Fig. 11 is a book 0
FIG. 2 is a perspective view of a method of forming a saddle-shaped superconducting winding of the invention. FIG. 12 is a perspective view of a saddle-shaped superconducting field winding formed by stacking a plurality of saddle-shaped superconducting windings according to the present invention. 2A, 2B...Saddle-shaped superconducting field winding t19...Wound conductor, 22...Resin-impregnated semi-cured glass tape, No. 152] No. 252] 24 IQ Fig. 3 Fig. 4 Fig. 5121 No. b口ZA・ZF3 71iJ 6th 9th Figure 2 Graduate 1st Oguchi Dormitory IZ Group
Claims (1)
る鞍形超電導界磁巻線において、 樹脂含浸セミキュアテープを巻線導体間に挿入して網込
んだ複数列のレーストラック状の超電導巻線をプレスし
て鞍形に形成し、この鞍形超電導巻線を複数個積み重ね
て形成し、この鞍形超電導巻線を複数個積み重ねて形成
することを特徴とする鞍形超電導界磁巻線。[Claims] 1. In a saddle-shaped superconducting field winding formed by winding a superconducting wire in a saddle shape in a plurality of cases and in a plurality of stages, a resin-impregnated semicured tape is inserted between the winding conductors to form a mesh. The method is characterized in that a row of racetrack-shaped superconducting windings are pressed to form a saddle shape, a plurality of saddle-shaped superconducting windings are stacked, and a plurality of saddle-shaped superconducting windings are stacked to form a saddle shape. saddle-shaped superconducting field winding.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11416585A JPS61272903A (en) | 1985-05-29 | 1985-05-29 | Saddle type superconductive field winding |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11416585A JPS61272903A (en) | 1985-05-29 | 1985-05-29 | Saddle type superconductive field winding |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61272903A true JPS61272903A (en) | 1986-12-03 |
Family
ID=14630791
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11416585A Pending JPS61272903A (en) | 1985-05-29 | 1985-05-29 | Saddle type superconductive field winding |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61272903A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008028097A (en) * | 2006-07-20 | 2008-02-07 | Mitsubishi Electric Corp | Superconducting electromagnet |
JP2010219118A (en) * | 2009-03-13 | 2010-09-30 | Sumitomo Electric Ind Ltd | Superconducting coil, rotary device, and method for manufacturing superconducting coil |
JP2014057087A (en) * | 2013-11-05 | 2014-03-27 | Sumitomo Electric Ind Ltd | Rotary device |
US8886266B2 (en) | 2010-06-21 | 2014-11-11 | Sumitomo Electric Industries, Ltd. | Superconducting coil, rotating device, and superconducting coil manufacturing method |
-
1985
- 1985-05-29 JP JP11416585A patent/JPS61272903A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008028097A (en) * | 2006-07-20 | 2008-02-07 | Mitsubishi Electric Corp | Superconducting electromagnet |
JP2010219118A (en) * | 2009-03-13 | 2010-09-30 | Sumitomo Electric Ind Ltd | Superconducting coil, rotary device, and method for manufacturing superconducting coil |
US8886266B2 (en) | 2010-06-21 | 2014-11-11 | Sumitomo Electric Industries, Ltd. | Superconducting coil, rotating device, and superconducting coil manufacturing method |
JP2014057087A (en) * | 2013-11-05 | 2014-03-27 | Sumitomo Electric Ind Ltd | Rotary device |
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