JPH0793059B2 - AC superconducting wire - Google Patents

AC superconducting wire

Info

Publication number
JPH0793059B2
JPH0793059B2 JP62043757A JP4375787A JPH0793059B2 JP H0793059 B2 JPH0793059 B2 JP H0793059B2 JP 62043757 A JP62043757 A JP 62043757A JP 4375787 A JP4375787 A JP 4375787A JP H0793059 B2 JPH0793059 B2 JP H0793059B2
Authority
JP
Japan
Prior art keywords
superconducting
wires
wire
superconducting wire
resin
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
JP62043757A
Other languages
Japanese (ja)
Other versions
JPS63211517A (en
Inventor
靖三 田中
要 松本
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.)
THE FURUKAW ELECTRIC CO., LTD.
Original Assignee
THE FURUKAW ELECTRIC CO., 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 THE FURUKAW ELECTRIC CO., LTD. filed Critical THE FURUKAW ELECTRIC CO., LTD.
Priority to JP62043757A priority Critical patent/JPH0793059B2/en
Publication of JPS63211517A publication Critical patent/JPS63211517A/en
Publication of JPH0793059B2 publication Critical patent/JPH0793059B2/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50/60Hzの交流用超電導線の構造に関するもの
である。
The present invention relates to a structure of a 50/60 Hz AC superconducting wire.

(従来の技術とその問題点) 従来50/60Hzの交流用超電導線としては例えば第3図
(a)に示すような超電導素線(1)を7本撚り合せた
もの、同図(b)のようにステンレス鋼、キユプロニツ
ケルなどの非超電導線(3)の囲りに超電導素線(1)
を6本撚り合せたもの、あるいは同図(c)のように超
電導素線(1)を13本平角撚線状にし、これらをいずれ
もエポキシ樹脂などの樹脂(2)により含浸したものが
ある。従来の超電導線の太さは電流容量のみで決定され
ており、例えば電流容量を増すために、7本から19本、
36本と素線数を増すことによつて電流容量の増大化がな
されていた。しかし超電導線の太さが大きくなると交流
損失により発熱し、電流容量が増大せず、また超電導素
線が隣接し過ぎるため超電導線内での発熱密度および分
布を低くできないなどの問題があつた。
(Prior art and its problems) As a conventional 50/60 Hz AC superconducting wire, for example, seven superconducting element wires (1) as shown in FIG. 3 (a) are twisted together, and FIG. Such as stainless steel, Kyupro Nikkeru, and other non-superconducting wires (3) surrounded by superconducting element wires (1)
6 twisted together, or as shown in FIG. 7C, there are 13 superconducting wires (1) formed into a flat rectangular twisted wire and impregnated with a resin (2) such as epoxy resin. . The thickness of the conventional superconducting wire is determined only by the current capacity. For example, in order to increase the current capacity, 7 to 19 wires,
The current capacity has been increased by increasing the number of strands to 36. However, when the thickness of the superconducting wire becomes large, heat is generated due to AC loss, the current capacity does not increase, and since the superconducting element wires are too close to each other, the heat density and distribution in the superconducting wire cannot be lowered.

(発明が解決しようとする問題点) 本発明は上記の問題を検討した結果、超電導線内部での
発熱密度を低下させ電流容量の大きい超電導線の構造を
開発したものである。
(Problems to be Solved by the Invention) As a result of examining the above problems, the present invention has developed a structure of a superconducting wire having a large current capacity by reducing the heat generation density inside the superconducting wire.

(問題点を解決するための手段および作用) 本発明は、超電導素線が集合され、素線の空隙の一部ま
たは全部が樹脂含浸されており、集合された超電導線の
中心から1.0mm以内に液体ヘリウムが接する自由表面が
あり、樹脂を除く超電導線のうち超電導素線の占める割
合が30〜50%でありかつ超電導素線が3本以上隣接しな
いことを特徴とする交流用超電導線である。
(Means and Actions for Solving Problems) In the present invention, superconducting wires are assembled, and a part or all of the voids of the wires are resin-impregnated, and within 1.0 mm from the center of the assembled superconducting wires. Is a free surface in contact with liquid helium, and the ratio of superconducting element wires to the superconducting element wires excluding resin is 30 to 50%, and three or more superconducting element wires are not adjacent to each other. is there.

以下に本発明の態様について第1図および第2図の超電
導線の断面図を用いて説明する。第1図(a)に示すよ
うに例えばNbTiなどのフイラメントを多数キユプロニツ
ケル中に埋込んだ外径0.1mm程度の超電導素線(1)
と、ステンレス鋼またはキユプロニツケルなどからなる
非超電導線(3)を予め外周にポリエステルで絶縁被覆
し、超電導素線が3本以上隣接しないように非超電導線
と集合して相互の空隙をエポキシ樹脂などの樹脂で含浸
して超電導線(4)としたものである。この際含浸する
樹脂は空隙を埋める程度としてもよく、また同図(b)
のように超電導線の等価直径にわたる全周を含浸しても
よい。これは多数の超電導線を集合した場合にはコイル
の振動が大きくなるので、これを防止するため樹脂層の
厚みを大きくした方がよいからである。
Aspects of the present invention will be described below with reference to the sectional views of the superconducting wire shown in FIGS. As shown in FIG. 1 (a), a superconducting wire with an outer diameter of about 0.1 mm, in which a number of filaments such as NbTi are embedded in a Kyupro nickel (1)
And a non-superconducting wire (3) made of stainless steel or Kyupro Nikel, etc. is preliminarily insulated and coated with polyester on the outer circumference, and the non-superconducting wires are assembled so that three or more superconducting element wires are not adjacent to each other and the mutual voids are made of epoxy resin, etc. This is a superconducting wire (4) impregnated with the above resin. At this time, the resin to be impregnated may be enough to fill the voids, and FIG.
As described above, the entire circumference of the equivalent diameter of the superconducting wire may be impregnated. This is because when a large number of superconducting wires are assembled, the vibration of the coil becomes large, and therefore it is better to increase the thickness of the resin layer in order to prevent this.

また本発明において集合された超電導線の中心から1.0m
m以内に液体ヘリウムが接する自由表面があることと
は、例えば丸線の場合第1図(b)に示す超電導線の直
径(A)、平角線の場合厚さ(B)、六角線の場合第2
図のように等価直径(C)が夫々2.0mm以内とするもの
で、これを越えると交流Ig/直流Icが50%以下となり実
質的効力が消失するからである。
In addition, 1.0 m from the center of the superconducting wires assembled in the present invention
The fact that there is a free surface in contact with liquid helium within m means, for example, in the case of a round wire, the diameter (A) of the superconducting wire shown in Fig. 1 (b), in the case of a rectangular wire the thickness (B), and in the case of a hexagonal wire. Second
As shown in the figure, the equivalent diameters (C) are 2.0 mm or less, respectively, and when the equivalent diameters (C) are exceeded, AC Ig / DC Ic becomes 50% or less and the effective effect disappears.

さらに本発明において、樹脂を除く超電導線のうち超電
導素線の占める割合を30〜50%としたのは、30%未満で
は導体の電流密度が低下し、50%を越えると超電導素線
が3本以上隣接する構造となり発熱源密度が上がり冷却
する速度よりも発熱速度が大きくクエンチ(超電導から
常電導へ転移)するからである。なお第1図(c)およ
び第2図のものは超電導線と非超電導線を集合したもの
である。
Further, in the present invention, the ratio of the superconducting wire to the superconducting wire excluding the resin is set to 30 to 50% because the current density of the conductor is reduced below 30%, and the superconducting wire exceeds 3% when the ratio exceeds 50%. This is because more than two adjacent structures are formed and the heat source density is increased and the heat generation rate is higher than the cooling rate and quenching (transition from superconducting to normal conducting). 1 (c) and 2 are a collection of superconducting wires and non-superconducting wires.

また本発明において超電導体としてはNbTi合金線のほか
Nb3Sn化合物線も適用できるが、この場合の素線絶縁は
セラミツクスを用い、またコイルスペーサーや巻枠をア
ルミナなどに替える必要がある。
Further, in the present invention, in addition to NbTi alloy wire as the superconductor
Nb 3 Sn compound wire can also be applied, but in this case, it is necessary to use ceramics for the wire insulation and replace the coil spacer and winding frame with alumina or the like.

(実施例) 以下に本発明の一実施例について説明する。(Example) An example of the present invention will be described below.

直径0.5μmのNbTiフイラメント7000本を9−1キユプ
ロニツケル中に埋込んだ外径0.1mmの超電導素線と同一
直径0.1mmのステンレス鋼からなる非超電導線の外周を
予めポリエステルで10μm絶縁被覆した。これらの素線
を用いて次の超電導線を作製した。超電導線の諸元を第
1表に示す。
A 7,000 NbTi filaments with a diameter of 0.5 μm were embedded in 9-1 Kyupro Nikel and a non-superconducting wire made of stainless steel with a diameter of 0.1 mm and a superconducting wire with a diameter of 0.1 mm was preliminarily insulation-coated with polyester to a thickness of 10 μm. The following superconducting wire was produced using these strands. Table 1 shows the specifications of the superconducting wire.

上記の超電導線を用いて次の交流コイルを作製した。こ
の諸元を第2表に示す。
The following alternating current coil was produced using the above superconducting wire. The specifications are shown in Table 2.

上記のコイルをエポキシ樹脂で真空含浸し、スペーサー
部の樹脂を取り除いて液体ヘリウムの流路(ダクト)と
した。したがつて素線間には第1図および第2図に示す
ように樹脂(2)が充満している。これらのコイルを用
いて50Hzで通電試験を行つた。この結果を第3表に示
す。
The coil was vacuum-impregnated with an epoxy resin, and the resin in the spacer portion was removed to form a liquid helium flow channel (duct). Therefore, the resin (2) is filled between the wires as shown in FIGS. 1 and 2. An energization test was performed at 50 Hz using these coils. The results are shown in Table 3.

第3表から明らかなように本発明によるものは電流容量
が大きく設計でき交流Ig/直流Ic95〜100%を達成でき
る。
As is clear from Table 3, the present invention can be designed with a large current capacity and can achieve AC Ig / DC Ic 95 to 100%.

(効果) 以上に説明したように本発明によれば超電導内部の発熱
密度を低下せしめ、このため電流容量の大きい超電導線
が得られるもので工業上極めて顕著な効果を奏するもの
である。
(Effects) As described above, according to the present invention, the heat generation density inside the superconducting material is reduced, so that a superconducting wire having a large current capacity can be obtained, and an extremely remarkable effect is industrially exhibited.

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

第1図乃至第3図は本発明の一実施例を示す超電導線の
断面図である。 1……超電導素線、2……樹脂、3……非超電導線、4
……超電導線、5……補強線。
1 to 3 are sectional views of superconducting wires showing an embodiment of the present invention. 1 ... Superconducting element wire, 2 ... Resin, 3 ... Non-superconducting wire, 4
…… Superconducting wire, 5 …… Reinforcing wire.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】超電導素線が集合され、素線間の空隙の一
部または全部が樹脂含浸されており、集合された超電導
線の中心から1.0mm以内に液体ヘリウムが接する自由表
面があり、樹脂を除く超電導線のうち超電導素線の占め
る割合が30〜50%でありかつ超電導素線が3本以上隣接
しないことを特徴とする交流用超電導線。
1. Superconducting wires are assembled, and a part or all of the voids between the wires are impregnated with resin, and there is a free surface within 1.0 mm from the center of the assembled superconducting wires that liquid helium contacts. A superconducting wire for alternating current, wherein the ratio of superconducting element wires to the superconducting element wires excluding resin is 30 to 50% and three or more superconducting element wires are not adjacent to each other.
JP62043757A 1987-02-26 1987-02-26 AC superconducting wire Expired - Lifetime JPH0793059B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62043757A JPH0793059B2 (en) 1987-02-26 1987-02-26 AC superconducting wire

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62043757A JPH0793059B2 (en) 1987-02-26 1987-02-26 AC superconducting wire

Publications (2)

Publication Number Publication Date
JPS63211517A JPS63211517A (en) 1988-09-02
JPH0793059B2 true JPH0793059B2 (en) 1995-10-09

Family

ID=12672632

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62043757A Expired - Lifetime JPH0793059B2 (en) 1987-02-26 1987-02-26 AC superconducting wire

Country Status (1)

Country Link
JP (1) JPH0793059B2 (en)

Also Published As

Publication number Publication date
JPS63211517A (en) 1988-09-02

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