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JPH0618090B2 - AC superconducting conductor - Google Patents
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JPH0618090B2 - AC superconducting conductor - Google Patents

AC superconducting conductor

Info

Publication number
JPH0618090B2
JPH0618090B2 JP62263829A JP26382987A JPH0618090B2 JP H0618090 B2 JPH0618090 B2 JP H0618090B2 JP 62263829 A JP62263829 A JP 62263829A JP 26382987 A JP26382987 A JP 26382987A JP H0618090 B2 JPH0618090 B2 JP H0618090B2
Authority
JP
Japan
Prior art keywords
superconducting
normal
outer peripheral
loss
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.)
Expired - Lifetime
Application number
JP62263829A
Other languages
Japanese (ja)
Other versions
JPH01107421A (en
Inventor
邦茂 黒田
龍▲吉▼ ▲高▼橋
伸洋 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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP62263829A priority Critical patent/JPH0618090B2/en
Publication of JPH01107421A publication Critical patent/JPH01107421A/en
Publication of JPH0618090B2 publication Critical patent/JPH0618090B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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

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  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は超電導化された交流機器に好適な超電導導体に
関する。
The present invention relates to a superconducting conductor suitable for a superconducting AC device.

〔従来の技術〕[Conventional technology]

従来の交流機器に使用される超電導導体は、銅やアルミ
ニウムなどの常電導金属体中に、超電導体をフイラメン
ト状にして、その外周部に集中して配置する方式で開発
されてきた。第3図以下、従来例を具体的に第3図に従
つて、構造,効能について述べる。
Superconducting conductors used in conventional AC devices have been developed by a method in which a superconducting conductor is made into a filament shape in a normal conducting metal body such as copper or aluminum and concentrated on the outer peripheral portion thereof. FIG. 3 Hereinafter, the structure and efficacy will be described in detail with reference to FIG.

該図に示す如く、従来の交流超電導導体1はNb−T
i,Nb3Snなどの超電導フイラメント4に、第1の
常電導金属5と第2の常電導金属6を2重に被覆した超
電導素線2を外周部に配置し、第3の常電導金属7に第
4の常電導金属8を被覆した常電導素線3を中心部に配
置し、それらの最外層を第5の常電導金属9で被覆し構
成されている。通常、第1〜5の常電導金属は導,アル
ミニウム,キユプロニツケルの2種、または3種の組合
せで使用されており、特に、第1と第3の常電導金属
5,7は低抵抗金属が、そして第2,4,5の常電導金
属6,8,9は高抵抗金属が良く用いられている。磁化
損失を低減するために、超電導素線2は細線化され、1
μm程度の直径を有し、常電導素線3も渦損失を低減す
るためほぼそれと同寸法に細線化される。高抵抗金属は
超電導素線2間の結合電流を、そして常電導素線3間の
渦電流を遮断するために使用され、最終的に交流超電導
導体1の交流損失を低減するのに大きく寄与する。ま
た、交流超電導導体1は中心軸廻りにツイスト(撚り)
され、前記結合電流の遮断がより効果的になるよう工夫
されている。
As shown in the figure, the conventional AC superconducting conductor 1 is Nb-T.
A superconducting element wire 2 in which a first normal conducting metal 5 and a second normal conducting metal 6 are doubly coated is placed on a superconducting filament 4 such as i, Nb 3 Sn or the like, and a third normal conducting metal is provided. 7, the normal conducting wire 3 coated with the fourth normal conducting metal 8 is arranged in the central portion, and the outermost layer thereof is covered with the fifth normal conducting metal 9. Usually, the first to fifth normal-conducting metals are used in a combination of two or three kinds of conductive, aluminum and Kyupro-Nickel, and especially, the first and third normal-conducting metals 5 and 7 are low resistance metals. A high resistance metal is often used for the second, fourth and fifth normal conducting metals 6, 8 and 9. In order to reduce the magnetization loss, the superconducting wire 2 is thinned to 1
The normal conducting wire 3 has a diameter of about μm and is thinned to almost the same size as that of the normal conducting wire 3 in order to reduce eddy loss. The high resistance metal is used to block the coupling current between the superconducting wires 2 and the eddy current between the normal conducting wires 3, and finally contributes largely to reduce the AC loss of the AC superconducting conductor 1. . Also, the AC superconducting conductor 1 is twisted around the central axis.
It is devised so that the blocking of the coupling current becomes more effective.

導体の電流容量を増大するために、ここで示した交流超
電導導体1を複数本束ね円心状、または平角状に撚線成
形したものが使用されている。また、用途に応じ、交流
超電導導体1の外周に絶縁層が被覆される場合がある。
In order to increase the current capacity of the conductor, a plurality of alternating-current superconducting conductors 1 shown here are bundled and formed into a concentric or rectangular shape by stranded wire. In addition, the outer periphery of the AC superconducting conductor 1 may be covered with an insulating layer depending on the application.

この交流超電導導体1に電流が流れると、表皮作用によ
つて導体の外周部に片寄り、しかも零抵抗である超電導
フイラメント4に集中して流れ、中心部の常電導素線群
のみならず外周部の超電導素線群の間に介在する常電導
体に流れず、ジユール発熱を十分に抑制でき、交流損失
の大幅な低減が期待される。さらに、外周部の超電導素
線群に電流が流れれば、この電流によつて発生する自己
磁界は、中心部において零となり、常電導素線群には渦
損失の発生は全くなく、交流損失低減効果が一層高めら
れる。以下がこの種導体に関する効能である。
When a current flows through this AC superconducting conductor 1, it is biased to the outer peripheral portion of the conductor by the skin action and flows concentratedly in the superconducting filament 4 which has zero resistance, and not only the normal conductive wire group in the central portion but also the outer peripheral portion. The current does not flow into the normal conductor that is interposed between the superconducting element wires in the above section, so that it is possible to sufficiently suppress the heat generation of the jule and it is expected that the AC loss will be greatly reduced. Furthermore, if a current flows in the superconducting wire group in the outer peripheral part, the self-magnetic field generated by this current will be zero in the central part, and there will be no eddy loss in the normal conducting wire group, and there will be no AC loss. The reduction effect is further enhanced. The following are the effects for this seed conductor.

しかし、上記効能は、この種導体が単線である場合に限
定される。交流損失を下げるために超電導フイラメント
を超極細線化するため、製法上昇線の直線も著るしく細
く(<1mm)なり、その電流容量も小さく(<数+A)
実用上極めて不便である。そのため前述の如く大電流化
するためには、この単線を複数本束ね撚線されるのが普
通である。ところが撚線をすると、着目した単線に、隣
接する他の単線からの磁界が垂直に印加される(近接効
果)ことになり必ずしも上記効能が期待されるとはいえ
ない。尚、交流用の超電導線に関しては、例えば特開昭
60−158510号公報,特開昭62−67156号公報等に開示さ
れている。
However, the above effects are limited to the case where the seed conductor is a single wire. Since the superconducting filament is made into ultra-fine wire to reduce AC loss, the straight line of the manufacturing process rise line is also extremely thin (<1 mm), and its current capacity is also small (<number + A).
It is extremely inconvenient for practical use. Therefore, in order to increase the current as described above, it is usual that a plurality of these single wires are bundled and twisted. However, when the stranded wire is used, the magnetic field from another adjacent single wire is vertically applied to the focused single wire (proximity effect), and the above effect cannot be always expected. Regarding superconducting wires for alternating current, see
It is disclosed in JP-A-60-158510 and JP-A-62-67156.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

上記従来技術は、実用的な大電流化に対する配慮がなさ
れておらず、撚線に伴なう近接効果による損失増大に問
題があつた。
The prior art described above does not consider practically large current, and has a problem of increasing loss due to the proximity effect associated with twisted wires.

本発明は上述の点に鑑み成されたもので、その目的とす
るところは、大電流化にも対処できるようにして、交流
損失を従来よりも下げられるような単線としての交流用
超電導導体を提供するにある。
The present invention has been made in view of the above points, and an object thereof is to provide an AC superconducting conductor as a single wire that can reduce AC loss as compared with the related art so as to be able to cope with a large current. To provide.

〔問題点を解決するための手段〕[Means for solving problems]

上記目的は、超電導体の周りに常電導金属の低抵抗層と
該低抵抗層より高抵抗を有する常電導金属の高抵抗層を
順次被覆した多数の超電導素線からなる極細多心の交流
用超電導導体において、前記超電導素線を超電導導体の
中央部と外周部に配置し、前記中央部と外周部の中間及
び外周部の外側に前記常電導金属の高抵抗層を設けるこ
とによって達成される。
The above-mentioned object is for an ultrafine multi-core alternating current consisting of a large number of superconducting element wires which are successively coated with a low-resistance layer of a normal-conductive metal and a high-resistance layer of a normal-conductive metal having a higher resistance than the low-resistance layer around a superconductor. In a superconducting conductor, it is achieved by arranging the superconducting element wire in a central portion and an outer peripheral portion of the superconducting conductor, and providing a high resistance layer of the normal conducting metal in the middle of the central portion and the outer peripheral portion and outside the outer peripheral portion. .

〔作用〕[Action]

交流超電導導体の交流損失を損失機構によつて内訳する
と、超電導フイラメント内の磁化損失が約80%で大部
分を占め、常電導体内の渦損失が約5%で、残りの約1
5%が常電導金属を介した超電導フイラメント間の結合
損失であるといわれている。しかも、電流による損失よ
りも磁界による損失が約2桁(約100倍)大きくなる
といわれている。この2つの事実を前提に、交流超電導
導体に交流電流が流れ、垂直な交流磁界が作用している
場合(大電流用撚線導体)を考えると、一本の構成単位
である導体で超電導フイラメントの配置の仕方を工夫す
れば交流損失を低減できる可能性がある。
Breaking down the AC loss of the AC superconducting conductor by the loss mechanism, the magnetization loss in the superconducting filament accounts for about 80%, the eddy loss in the normal conductor is about 5%, and the remaining about 1%.
It is said that 5% is the coupling loss between superconducting filaments via the normal conducting metal. Moreover, it is said that the loss due to the magnetic field is about two orders of magnitude (about 100 times) larger than the loss due to the current. Based on these two facts, considering the case where an AC current flows through an AC superconducting conductor and a vertical AC magnetic field is acting (a large-current stranded conductor), a superconducting filament is a conductor that is one structural unit. There is a possibility that AC loss can be reduced by devising the arrangement method of.

従来の交流超電導導体において、超電導フイラメント、
すなわち超電導素線2の本数を2分し、その一部を外周
部に、残りを中心部に配置しその中間部に常電導金属を
配置した構成に改めると、外部印加磁界に対して、外周
部の超電導素線群は外部磁界を浴びるが、フィラメント
本数を低減した分だけ損失(磁化損失)は減少し、中心
部の超電導素線群の損失は外周部による遮蔽効果のため
ほぼ零となる。従つて、全体の交流損失は確実に低減さ
れる。外周部に配置する超電導素線群の本数を極力減ら
し、効率よく外部磁界を遮蔽するようにするなら、更
に、全体の交流損失を低減することができる。そのため
の手段として、外周部と中心部の間に距離を十分とり、
かつ、この中間部に常電導(低抵抗)金属を配置する方
法と、外周部の超電導素線のツイスト・ピツチをやや長
くし、結合を強くする方法の2つが考えられる。
In conventional AC superconducting conductors, superconducting filaments,
That is, when the number of superconducting wires 2 is divided into two, a part of the superconducting wires 2 is placed in the outer peripheral portion, the rest is placed in the central portion, and a normal conducting metal is placed in the middle portion, the outer peripheral portion is exposed to an externally applied magnetic field. The superconducting wire group in the central part is exposed to the external magnetic field, but the loss (magnetization loss) is reduced by the number of filaments reduced, and the loss in the superconducting wire group in the central part becomes almost zero due to the shielding effect by the outer peripheral part. . Therefore, the overall AC loss is reliably reduced. If the number of superconducting element wires arranged in the outer peripheral portion is reduced as much as possible and the external magnetic field is efficiently shielded, the total AC loss can be further reduced. As a means for that, take a sufficient distance between the outer peripheral part and the central part,
There are two possible methods: a method of arranging a normal-conducting (low-resistance) metal in this intermediate portion, and a method of lengthening the twist pitch of the superconducting element wire in the outer peripheral portion to make the coupling stronger.

〔実施例〕〔Example〕

本発明の一実施例を第1図に示し、その構成,作用,効
果について説明する。本発明における交流超電導導体1
の構成は以下の通りである。超電導(Nb−Ti)フイ
ラメント4の外側に、第1の常電導金属(銅)と第2の
常電導金属(キユプロ・ニツケル)6を2重に被覆した
超電導素線2を中心部に857本と外周部に643本密
に配置し、その中間部に第6の常電導金属(キユプロ・
ニツケル)10の層を設け、最外周には第5の常電導金
属(キユプロニツケル40μm厚)9を配置した。
One embodiment of the present invention is shown in FIG. 1, and its configuration, action and effect will be described. AC superconducting conductor 1 according to the present invention
The configuration is as follows. On the outside of the superconducting (Nb-Ti) filament 4, there are 857 superconducting element wires 2 in which the first normal conducting metal (copper) and the second normal conducting metal (Kyupro Nickel) 6 are double-coated in the central portion. 643 are densely arranged on the outer periphery and the sixth normal conducting metal (Kyupro.
Nickel) 10 was provided, and a fifth normal conducting metal (Kyupro Nickel 40 μm thick) 9 was arranged on the outermost periphery.

この具体的製法については後述する。また、比較のため
に本実施例と同一諸元を有する従来導体を別途作製して
おいた。本実施例では直径1μmの超電導フイラメント
4を7本1組で第1の常電導金属5の中に埋め込んだ
が、1本毎に3層構造体にする方法がより一般的であ
る。この構成について、ここでは特に問題にしないこと
とする。
This specific manufacturing method will be described later. For comparison, a conventional conductor having the same specifications as this embodiment was separately prepared. In the present embodiment, a set of seven superconducting filaments 4 each having a diameter of 1 μm is embedded in the first normal conducting metal 5, but a method of forming a three-layer structure for each one is more general. This configuration will not be a particular problem here.

次に、各構成部の作用について説明する。外周部と中心
部には超電導素線2が配置され、交流電流を搬送する役
目を果す。その中間部の常電導金属10の層は中心部と
外周部の超電導素線群を電気的に結合させないようにす
るとともに、多少とも距離をかせぎ磁気的結合を弱め交
流損失を低減する機能をもつ。最外層の常電導金属9は
交流超電導導体1を強固に形状維持する役目の他に、そ
れが高抵抗金属である場合、渦電流と結合電流を流れに
くくし、それが低抵抗金属である場合、その内側の超電
導素線群での渦電流や結合電流を減らし、全体としての
交流損失を低減する機能をもつ。超電導素線2を構成す
る第2の常電導金属6も常電導金属9と同様な機能を有
する。また、中心部と外周部の超電導素線群は、比較の
ための実験で用いた従来例の導体と同じ4mmピツチでツ
イストを行なつた。ツイストは、前述の通り超電導素線
2間の電気的結合を断ち交流損失を低減する作用を有す
る。
Next, the operation of each component will be described. Superconducting wires 2 are arranged at the outer peripheral portion and the central portion, and serve to carry an alternating current. The layer of the normal-conductivity metal 10 in the middle portion has a function of not electrically coupling the superconducting element wires in the central portion and the outer peripheral portion, and also having a function of slightly increasing the distance to weaken the magnetic coupling and reduce the AC loss. . In addition to the role of firmly maintaining the shape of the AC superconducting conductor 1, the outermost normal-conducting metal 9 is a high-resistance metal, which makes it difficult for eddy currents and coupling currents to flow and is a low-resistance metal. , It has the function of reducing eddy currents and coupling currents in the superconducting element wires inside it, and reducing AC loss as a whole. The second normal conducting metal 6 forming the superconducting element wire 2 also has the same function as the normal conducting metal 9. Further, the superconducting wire groups at the central portion and the outer peripheral portion were twisted with the same 4 mm pitch as the conductor of the conventional example used in the comparative experiment. As described above, the twist has a function of cutting off the electrical coupling between the superconducting element wires 2 and reducing the AC loss.

更に、本発明の交流超電導導体1の効果について述べ
る。従来例と本発明にかかる交流超電導導体の交流損失
測定を行なつた結果を第4図に示す。実線が本発明の、
そして点線が従来導体の交流損失を示す。すなわち、交
流磁界1.0Tにおいて比較すると、従来例の導体1に
比べ交流損失は1/2.3に減少した。この結果は交流
損失低減に本発明が有効であることを示唆している。
Further, the effect of the AC superconducting conductor 1 of the present invention will be described. FIG. 4 shows the result of the AC loss measurement of the AC superconducting conductor according to the conventional example and the present invention. The solid line is the present invention,
The dotted line shows the AC loss of the conventional conductor. That is, when compared with an AC magnetic field of 1.0 T, the AC loss was reduced to 1 / 2.3 as compared with the conductor 1 of the conventional example. This result suggests that the present invention is effective in reducing AC loss.

本実施例において、中心部の超電導素線群と外周部の超
電導素線群のツイスト・ピツチを異なる値に選ぶことに
よつて、更に交流損失を低減することが可能である。既
に述べた如く、外部印加磁界を効率よく遮蔽し、中心部
の超電導素線群と中間部の常電導金属層10の磁界を小
さくするためには外周部の超電導素線群のツイスト・ピ
ツチを長くし、結合電流を流れ易くすればよい。結合電
流の増加は結合損失の増大につながるが、ツイスト・ピ
ツチを無限大にするわけでなく、結合損失が全損失の1
/5以下であることを考えれば、大勢に影響を及ぼすこ
とはない。また、中心部と外周部の超電導素線群を同一
のピツチでツイストすると、外周部は中心部に比べイン
ダクタンスが大きくなり、交流電流が流れにくく、超電
導素線に均等に交流電流が流れなくなる可能性がある。
従つて、外周部のツイストピツチを長くし、インピーダ
ンスを下げ、中心部のそれと等しくする必要がある。こ
のツイスト・ピツチの選択は、中心部と外周部にふくま
れる超電導素線2の本数の違いを考慮した上で、交流損
失を低減する方向で行なわれなければならない。よつ
て、中心部に比べ外周部のツイスト・ピツチが長いとは
限らないし、ツイストの方向を同一方向にする必然性も
ない。
In this embodiment, the AC loss can be further reduced by selecting different values for the twist pitches of the superconducting element wire group in the central part and the superconducting element wire group in the outer peripheral part. As described above, in order to efficiently shield the externally applied magnetic field and reduce the magnetic fields of the superconducting element wire group in the central part and the normal conducting metal layer 10 in the middle part, the twist pitch of the superconducting element wire group in the outer peripheral part is used. The length may be increased so that the coupling current can easily flow. An increase in the coupling current leads to an increase in the coupling loss, but it does not make the twist pitch infinite, and the coupling loss is one of the total losses.
Considering that it is / 5 or less, it will not affect many people. Also, if the superconducting wire group in the central part and the outer peripheral part are twisted with the same pitch, the outer peripheral part has a larger inductance than the central part, and it is difficult for the alternating current to flow, and it is possible that the alternating current does not flow evenly in the superconducting wire. There is a nature.
Therefore, it is necessary to lengthen the twist pitch at the outer peripheral portion and lower the impedance to make it equal to that at the central portion. The selection of the twist pitch should be made in the direction of reducing the AC loss in consideration of the difference in the number of the superconducting wires 2 included in the central portion and the outer peripheral portion. Therefore, the twist pitch of the outer peripheral portion is not always longer than that of the central portion, and it is not necessary to make the twist directions the same.

本発明の他の実施例を第2図に従つて説明する。構成上
第1図と異なる部分は中間部の常電導金属層10であ
る。すなわち第1図では単一常電導金属パイプを用いた
が、第2図では、これを多層にし、異種常電導金属や常
電導素線3が組合されている。その詳細を第2図(c)
に、4通りの構成で示した。a断面は内側と外側に第6
の常電導金属11を配置し、その中間に第7の常電導金
属12を配置したものであり、b断面はこれと逆の配列
をしたものである。またc断面は内側に第8の常電導金
属13を配置し、その外側に常電導素線3を密に配置
し、d断面はそれと逆に配列したものである。
Another embodiment of the present invention will be described with reference to FIG. The structure is different from that shown in FIG. 1 in the normal conducting metal layer 10 in the middle part. That is, in FIG. 1, a single normal-conducting metal pipe is used, but in FIG. 2, the normal-conducting metal pipe is made into a multi-layer, and different kinds of normal-conducting metals and normal-conducting element wires 3 are combined. The details are shown in Fig. 2 (c).
The four configurations are shown in FIG. a cross section is 6th inside and outside
The normal-conducting metal 11 is arranged, and the seventh normal-conducting metal 12 is arranged in the middle of the normal-conducting metal 11, and the section b is the reverse arrangement. The c-section has the eighth normal-conducting metal 13 arranged on the inner side, the normal-conducting element wires 3 densely arranged on the outer side thereof, and the d-section has the opposite arrangement.

これは交流超電導導体1の安定性向上のために低抵抗金
属の量を増加する必要がある場合の対策法であり、低抵
抗金属をパイプ状のまま配置すると渦損失や結合損失が
増加するために細分化、または多層化を図つたものであ
る。細分化と多層化の方法は当然上記以外にも種々考え
られる。
This is a countermeasure when it is necessary to increase the amount of low-resistance metal in order to improve the stability of the AC superconducting conductor 1. Since placing a low-resistance metal in a pipe shape increases eddy loss and coupling loss. It is intended for subdivision or multi-layering. Naturally, various methods other than the above can be considered for the method of subdividing and multilayering.

本実施例から期待される効果は、前記実施例と同様、損
失の低減と安定性の一層の向上にある。
The effects expected from this embodiment are reduction of loss and further improvement of stability, as in the above-mentioned embodiments.

本発明を具体化するための製法に関する極く基本的な実
施例を以下説明する。
A very basic example of a manufacturing method for embodying the present invention will be described below.

第5図は本発明の第1の製造方法を示したものである。
(a)は製造の出発時点を示したものであり、中央部と
なる超電導線14は丸線状ですでにツイストが加えられ
ている。外周部となる超電導線15,15′は平角線状
であるが、その寸法やツイストピツチ等により必要な数
が決る。これらの超電導線を(b)に示すように、中心
部となる超電導線14に外周部となる超電導線15,1
5′を巻き付ける。そして、例えば、ダイスに通し互い
に密着させ、(c)に示したように一本の交流超電導導
体1とした。
FIG. 5 shows the first manufacturing method of the present invention.
(A) shows the starting point of manufacture, and the superconducting wire 14 at the center is a round wire and has already been twisted. The superconducting wires 15 and 15 ′ that are the outer peripheral portions are rectangular wire shapes, but the required number is determined by their dimensions and twist pitches. As shown in (b) of these superconducting wires, the superconducting wire 14 serving as the central portion and the superconducting wires 15, 1 serving as the outer peripheral portion are formed.
Wrap 5 '. Then, for example, they are passed through a die and brought into close contact with each other to form one AC superconducting conductor 1 as shown in (c).

第6図は本発明の第2の製造方法を示したものである。
(a)は製造の出発時点を示したものであり、中心部と
なる超電導線14は丸線状ですでにツイストが加えられ
ており、外周部となる超電導線16はパイプ状でこれに
もツイストが加えられている。これらの超電導線を
(b)に示すように、外周部となる超電導線16の中に
中央部となる超電導線14を挿入する。そしてダイスに
通し互いに密着させ、(c)に示したように一本の交流
超電導導体1とした。上記の2つの製法では、密着加工
した後、特にツイストは加えなかつたが、密着加工した
後さらにツイストを加えて所望のツイストピツチとして
もよいのは勿論である。また、中央部と外周部のツイス
トの方向が同じである必要はなく、互いに逆向きでもよ
い。いうまでもなく、中央部と外周部の中間及び最外周
部に常電導金属層9と10を設けることは上記両製法に
おいて極めて容易である。
FIG. 6 shows a second manufacturing method of the present invention.
(A) shows the starting point of manufacturing, in which the superconducting wire 14 at the center is a round wire and has already been twisted, and the superconducting wire 16 at the outer peripheral part is a pipe, and A twist has been added. As shown in (b) of these superconducting wires, the central superconducting wire 14 is inserted into the outer peripheral superconducting wire 16. Then, they were passed through a die and brought into close contact with each other to form one AC superconducting conductor 1 as shown in (c). In the above-mentioned two manufacturing methods, the twist is not particularly added after the contact processing, but it is needless to say that a twist may be further added after the contact processing to obtain a desired twist pitch. Further, the twist directions of the central portion and the outer peripheral portion do not have to be the same, and may be opposite to each other. Needless to say, it is extremely easy to provide the normal-conducting metal layers 9 and 10 in the middle of the central portion and the outer peripheral portion and in the outermost peripheral portion in both the above manufacturing methods.

第1図で説明した実施例は第5図で説明した製法に従つ
たもので、外周部の超電導線16は中間の常電導金属層
10の外側に超電導素線2と予め巻きつけ、その外側に
最外層となる常電導金属層を被覆したものであり、中央
部の超電導線14は通常の極細多心線の製法に従つたも
のである。超電導フイラメント数(超電導素線2の
数)、ツイストピツチは既に述べた通りである。
The embodiment described with reference to FIG. 1 is based on the manufacturing method described with reference to FIG. 5, and the superconducting wire 16 at the outer peripheral portion is pre-wound with the superconducting element wire 2 on the outside of the intermediate normal-conducting metal layer 10 and the outside thereof. The outermost normal conducting metal layer is coated on the superconducting wire 14, and the superconducting wire 14 in the central portion is obtained by the usual method for manufacturing an ultrafine multifilamentary wire. The number of superconducting filaments (the number of superconducting wires 2) and twist pitch are as described above.

〔発明の効果〕〔The invention's effect〕

以上説明した本発明によれば、最も交流損失の少ない従
来導体に比べ更に交流損失を低減できる交流用超電導導
体を提供することができ、大電流化しても損失の低減が
可能なために、超電導の交流応用分野における工業的効
果は甚大である。
According to the present invention described above, it is possible to provide an AC superconducting conductor that can further reduce the AC loss as compared with the conventional conductor having the smallest AC loss, and it is possible to reduce the loss even if the current is increased. The industrial effects in the field of AC application are enormous.

【図面の簡単な説明】[Brief description of drawings]

第1図(a)は本発明の一実施例の交流超電導導体を示
す断面図、第1図(b)はその超電導素線の詳細断面
図、第2図(a)は本発明の他の実施例を示す交流超電
導導体の断面図、第2図(b)はその超電導素線の詳細
断面図、第2図(c)は常電導金属層の各種組合せの状
態を示す導体断面図、第2図(d)はその常電導素線の
詳細断面図、第3図(a)は従来の交流超電導導体を示
す断面図、第3図(b)はその超電導素線の詳細断面
図、第3図(c)はその常電導素線の断面図、第4図は
同一諸えを有する従来、及び本発明の交流超電導導体の
実測された交流損失特性を示す特性図、第5図(a),
(b),(c)と第6図(a),(b),(c)は本発
明の交流超電導導体を具体化する製法に関する実施例を
それぞれ示す工程順の図である。 1……交流用超電導導体、2……超電導素線、3……常
電導素線、4……超電導フイラメント、5……第1の常
電導金属、6……第2の常電導金属、7……第3の常電
導金属、8……第4の常電導金属、9……第5の常電導
金属、10……常電導金属層、11……第6の常電導金
属、12……第7の常電導金属、13……第8の常電導
金属、14……中央部となる超電導線、15,15′…
…外周部となる超電導線、16……外周部となるパイプ
状超電導線。
FIG. 1 (a) is a sectional view showing an AC superconducting conductor of an embodiment of the present invention, FIG. 1 (b) is a detailed sectional view of the superconducting element wire, and FIG. 2 (a) is another embodiment of the present invention. FIG. 2 (b) is a detailed cross-sectional view of the superconducting element wire, FIG. 2 (c) is a cross-sectional view of conductors showing various combinations of normal-conducting metal layers, and FIG. 2 (d) is a detailed sectional view of the normal conducting wire, FIG. 3 (a) is a sectional view showing a conventional AC superconducting conductor, and FIG. 3 (b) is a detailed sectional view of the superconducting wire. FIG. 3 (c) is a cross-sectional view of the normal conducting wire, FIG. 4 is a characteristic diagram showing actually measured AC loss characteristics of the AC superconducting conductor of the present invention having the same specifications, and FIG. 5 (a). ),
6 (b) and 6 (c) and FIGS. 6 (a), 6 (b) and 6 (c) are process order diagrams showing examples of the manufacturing method for embodying the AC superconducting conductor of the present invention. 1 ... AC superconducting conductor, 2 ... Superconducting element wire, 3 ... Normal conducting element wire, 4 ... Superconducting filament, 5 ... First normal conducting metal, 6 ... Second normal conducting metal, 7 ...... Third normal conducting metal, 8 ...... Fourth normal conducting metal, 9 ...... Fifth normal conducting metal, 10 ...... Normal conducting metal layer, 11 ...... Sixth normal conducting metal, 12 ...... Seventh normal conducting metal, 13 ... Eighth normal conducting metal, 14 ... Central superconducting wire, 15, 15 '...
… Superconducting wire that becomes the outer peripheral portion, 16… Pipe-shaped superconducting wire that becomes the outer peripheral portion.

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭50−39492(JP,A) 特開 昭60−158510(JP,A) 特開 昭62−67156(JP,A) 特公 昭43−5063(JP,B1) 特公 昭51−13867(JP,B1) ─────────────────────────────────────────────────── ─── Continuation of the front page (56) Reference JP-A-50-39492 (JP, A) JP-A-60-158510 (JP, A) JP-A-62-67156 (JP, A) JP-B 43- 5063 (JP, B1) JP-B-51-13867 (JP, B1)

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】超電導体の周りに常電導金属の低抵抗層と
該低抵抗層より高抵抗を有する常電導金属の高抵抗層を
順次被覆した多数の超電導素線からなる極細多心の交流
用超電導導体において、前記超電導素線を超電導導体の
中央部と外周部に配置し、前記中央部と外周部の中間及
び外周部の外側に前記常電導金属の高抵抗層を設けたこ
とを特徴とする交流用超電導導体。
1. An ultrafine multi-core alternating current composed of a large number of superconducting element wires in which a low-resistance layer of a normal-conductive metal and a high-resistance layer of a normal-conductive metal having a higher resistance than the low-resistance layer are sequentially coated around a superconductor. In the superconducting conductor for use, the superconducting element wire is arranged in a central portion and an outer peripheral portion of the superconducting conductor, and the high resistance layer of the normal conducting metal is provided between the central portion and the outer peripheral portion and outside the outer peripheral portion. Superconducting conductor for alternating current.
【請求項2】特許請求の範囲第1項記載のものにおい
て、中央部と外周部の前記超電導素線群を異なるピッチ
で撚線したことを特徴とする交流用超電導導体。
2. A superconducting conductor for alternating current according to claim 1, wherein the superconducting element wire groups in the central portion and the outer peripheral portion are twisted at different pitches.
JP62263829A 1987-10-21 1987-10-21 AC superconducting conductor Expired - Lifetime JPH0618090B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62263829A JPH0618090B2 (en) 1987-10-21 1987-10-21 AC superconducting conductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62263829A JPH0618090B2 (en) 1987-10-21 1987-10-21 AC superconducting conductor

Publications (2)

Publication Number Publication Date
JPH01107421A JPH01107421A (en) 1989-04-25
JPH0618090B2 true JPH0618090B2 (en) 1994-03-09

Family

ID=17394802

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62263829A Expired - Lifetime JPH0618090B2 (en) 1987-10-21 1987-10-21 AC superconducting conductor

Country Status (1)

Country Link
JP (1) JPH0618090B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100758149B1 (en) * 2006-08-21 2007-09-12 순천향대학교 산학협력단 Superconductor total loss measuring device and device for transferring it

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE1282116B (en) * 1964-04-17 1968-11-07 Siemens Ag Superconducting wire for the transport of high currents
JPS5640924A (en) * 1979-09-10 1981-04-17 Hitachi Denshi Ltd Direct current constant voltage power source
JPH0796698B2 (en) * 1985-09-18 1995-10-18 株式会社フジクラ Manufacturing method of multi-core superconducting conductor for alternating current

Also Published As

Publication number Publication date
JPH01107421A (en) 1989-04-25

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