JP2601318B2 - Superconducting magnetic circuit - Google Patents

Superconducting magnetic circuit

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Publication number
JP2601318B2
JP2601318B2 JP14327688A JP14327688A JP2601318B2 JP 2601318 B2 JP2601318 B2 JP 2601318B2 JP 14327688 A JP14327688 A JP 14327688A JP 14327688 A JP14327688 A JP 14327688A JP 2601318 B2 JP2601318 B2 JP 2601318B2
Authority
JP
Japan
Prior art keywords
superconducting
magnetic circuit
hollow container
loop
magnetic flux
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
JP14327688A
Other languages
Japanese (ja)
Other versions
JPH01312807A (en
Inventor
調 秋田
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.)
Central Research Institute of Electric Power Industry
Original Assignee
Central Research Institute of Electric Power Industry
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 Central Research Institute of Electric Power Industry filed Critical Central Research Institute of Electric Power Industry
Priority to JP14327688A priority Critical patent/JP2601318B2/en
Publication of JPH01312807A publication Critical patent/JPH01312807A/en
Application granted granted Critical
Publication of JP2601318B2 publication Critical patent/JP2601318B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は超電導体による磁気遮蔽効果を利用した交流
磁束伝達用磁気回路に関するものである。
Description: TECHNICAL FIELD The present invention relates to a magnetic circuit for transmitting AC magnetic flux using a magnetic shielding effect of a superconductor.

(従来技術) 変圧器のように1次コイルにより発生させた磁束を2
次コイルに伝達してエネルギの伝達などを行う装置にお
いては、1次コイルの発生磁束のすべてを2次コイルに
伝達できるのが理想である。
(Prior art) A magnetic flux generated by a primary coil like a transformer
In a device that transmits energy to the secondary coil, it is ideal that all of the magnetic flux generated by the primary coil can be transmitted to the secondary coil.

しかし周知のように1次コイルと2次コイルのみで
は、1次コイルの発生磁束の多くが2次コイルに鎖交す
ることなく拡逃散するためエネルギ伝達効率の大きな低
下を招く。そこで一般にはこれを防止するため1次コイ
ルと2次コイルを貫通する鉄心による磁気回路を設ける
ことが行われている。
However, as is well known, when only the primary coil and the secondary coil are used, much of the magnetic flux generated in the primary coil spreads and escapes without interlinking with the secondary coil, so that the energy transfer efficiency is greatly reduced. In order to prevent this, a magnetic circuit is generally provided by an iron core penetrating the primary coil and the secondary coil.

しかしこの方法では磁気飽和などにより周知のように
2テスラ以上の磁束の伝達は不可能である。このためエ
ネルギの伝達量にはおのずからなる限界があり、しかも
伝達磁束が交流磁束の場合には鉄損の発生をまぬがれ得
ないためエネルギの伝達効率は更に低下する。
However, in this method, it is impossible to transmit a magnetic flux of 2 Tesla or more as is well known due to magnetic saturation and the like. For this reason, the amount of transmitted energy is naturally limited, and when the transmitted magnetic flux is an alternating magnetic flux, the generation of iron loss cannot be avoided, so that the energy transmission efficiency is further reduced.

そこで本発明者は先に超電導状態において発揮される
マイナス効果などにより、超電導体が極めてすぐれた磁
気遮蔽効果を呈することを利用した磁気回路を提案した
(特願昭63−22113号参照)。
The present inventor has previously proposed a magnetic circuit utilizing a superconductor exhibiting an extremely excellent magnetic shielding effect due to a negative effect exhibited in a superconducting state (see Japanese Patent Application No. 63-22113).

この磁気回路は超電導材により例えば第1図に示す一
部切欠き斜視図にようなループ状中空容器(1)を形成
し、これを超電導状態におくことにより磁気遮蔽効果を
発揮させて磁気遮蔽材により包囲された閉磁路空間(1
a)を作り、例えばその内部の一端部に設けた1次コイ
ル(2)による発生磁束を、拡逃散しないように封じこ
めながら他端に設けた2次コイル(3)に伝達するよう
にしたものである。
In this magnetic circuit, a loop-shaped hollow container (1) as shown in, for example, a partially cutaway perspective view shown in FIG. 1 is formed of a superconducting material, and a magnetic shielding effect is exerted by leaving the container in a superconducting state. Magnetic circuit space (1
a), for example, the magnetic flux generated by the primary coil (2) provided at one end inside is transmitted to the secondary coil (3) provided at the other end while being enclosed so as not to spread and escape. Things.

この方法によれば原理上鉄心を用いる磁気回路のよう
に飽和などにもとづく磁束伝達量の制限がなく、しかも
磁束の拡逃散が著しく少ない。これに加えて鉄損の発生
もないので、鉄心を用いる磁気回路に比べて多量のエネ
ルギを効率よく伝達できる。
According to this method, in principle, there is no limitation on the amount of magnetic flux transmission based on saturation or the like as in a magnetic circuit using an iron core, and the spread and escape of the magnetic flux are extremely small. In addition, since there is no generation of iron loss, a large amount of energy can be efficiently transmitted as compared with a magnetic circuit using an iron core.

なお第1図において(4)は伝達磁束によりループ状
中空容器(1)の周方向に生ずる電流Iの発生を防ぎ、
伝達磁束の減衰を防ぐための絶縁層である。
In FIG. 1, (4) prevents generation of a current I generated in the circumferential direction of the loop-shaped hollow container (1) by the transmitted magnetic flux.
This is an insulating layer for preventing attenuation of the transmission magnetic flux.

(従来技術の問題点) しかし超電導材によるループ状容器、特に大型ものを
作るのは難しく、しかも機械的強度を持たせるため或る
程度以上の肉厚を必要とすることから容器が高価なもの
となるのは勿論、特に伝達すべき磁束が交流の場合には
ループ状中空容器内に損失を生ずるのを防ぐことができ
ないため、その分だけエネルギーの伝達効率を低下する
ことになる。
(Problems of the prior art) However, it is difficult to make a loop-shaped container made of a superconducting material, particularly a large container, and the container is expensive because it requires a certain thickness or more to have mechanical strength. Of course, in particular, when the magnetic flux to be transmitted is an alternating current, it is not possible to prevent the loss in the loop-shaped hollow container, so that the energy transmission efficiency is reduced accordingly.

(発明の目的) 本発明は製作し易くしかも交流損失の少ない交流磁束
伝達用の超電導磁気回路の提供を目的としてなされたも
のである。
(Object of the Invention) The present invention has been made to provide a superconducting magnetic circuit for transmitting an AC magnetic flux which is easy to manufacture and has a small AC loss.

(問題点を解決するための本発明の手段) 本発明の特徴とするところは、交流用超電導線即ち直
径を極力細くした超電導フィラメントを例えば銅ニッケ
ル合金による超電導率母材中に埋め込み、更にこの線に
出来るだけ短いピッチの撚りをかけて低交流損失化を図
った公知の交流用超電導線をテープ状に織成し、これを
ループ状中空容器を形成するように巻いて構成するよう
にした点にある。次に実施例によって本発明を具体的に
説明する。
(Means of the present invention for solving the problems) The feature of the present invention is that an AC superconducting wire, that is, a superconducting filament having a diameter as small as possible is embedded in a superconductivity base material made of, for example, a copper-nickel alloy. A known AC superconducting wire woven in the form of a tape in which the wire is twisted with a pitch as short as possible to reduce the AC loss, and this is wound and formed to form a loop-shaped hollow container. is there. Next, the present invention will be specifically described with reference to examples.

(実施例) 第2図は本発明の一実施例説明図である。第2図
(a)に示すように交流用超電導線を縦糸(5)及び横
糸(6)として、巻回に容易な幅をもった超電導材テー
プ(7)を織成する。なおこの場合超電動線はエナメル
などにより絶縁してもよい。一方これとは別に第2図
(b)に示すように中空状直管(8a)および中空状曲管
(8b)の差し込み接続によって形成され、かつ直管(8
a)または曲管内に所要ターン数の1次コイル(2)と
2次コイル(3)が収容固定され、しかもコイル(2)
(3)のそれぞれの両端が所要の絶縁が施された接続導
線(2a)(3a)として管外に引出されるようにした絶縁
性のループ状中空容器形成材(8)を用意する。
(Example) FIG. 2 is an explanatory view of an example of the present invention. As shown in FIG. 2 (a), a superconducting material tape (7) having a width which is easy to wind is woven using the AC superconducting wire as the warp (5) and the weft (6). In this case, the super electric wire may be insulated by enamel or the like. On the other hand, as shown in FIG. 2 (b), the straight pipe (8a) and the hollow curved pipe (8b) are formed by insertion connection.
a) Or, the required number of turns of the primary coil (2) and the secondary coil (3) are accommodated and fixed in a curved tube, and the coil (2)
An insulating loop-shaped hollow container forming material (8) is prepared, which is drawn out of the tube as connection conductors (2a) and (3a), both ends of which are provided with required insulation.

そして第2図(c)に示すように別に用意した超電導
材テープ(7)より幅の広い絶縁性テープ(9)例えば
ガラス繊維製テープと、超電導材テープ(7)とを重ね
合わせながら所要の幅宛オーバーラップ(10)させて中
空容器形成材(8)の周面の全長に亘って螺施状に巻
く。そして最後に表面の保護を中空容器形成材料(8)
とこの上に巻かれた超電導材テープ(7)間のずれや巻
つけの緩みなどの防止のため、樹脂材例えばエポキシ樹
脂を含浸し固化させて第2図(d)のように形成したも
ので、このような超電導磁気回路は例えば中空容器形成
材(8)の表面に所要の面積を持たせた布状超電導材
(7)、または布状超電導材(7)と周回電流発生防止
用の布状絶縁材(9)を重ね合わせたものをエポキシ樹
脂接着材により貼りつけても形成できる。
Then, as shown in FIG. 2 (c), an insulating tape (9) wider than the separately prepared superconducting material tape (7), for example, a glass fiber tape and a superconducting material tape (7) are superimposed on each other and required. The hollow container forming material (8) is spirally wound over the entire length of the peripheral surface of the hollow container forming material (8) so as to overlap the width (10). And finally, the surface is protected by the hollow container forming material (8).
In order to prevent the gap between the superconducting material tapes (7) wound thereon and the looseness of the winding, etc., a resin material such as an epoxy resin is impregnated and solidified to form as shown in FIG. 2 (d). Such a superconducting magnetic circuit is, for example, a cloth-shaped superconducting material (7) having a required area on the surface of a hollow container forming material (8), or a cloth-shaped superconducting material (7) and a circuit for preventing generation of a circulating current. It can also be formed by laminating a cloth-like insulating material (9) with an epoxy resin adhesive.

また例えば半田のような低電導率材を含浸させた超電
導材テープ(7)または超電導材テープ(7)と絶縁性
テープ(9)を重ね合わせたものを、エポキシ樹脂など
により接着し形成しながらループ状の中空容器を形成す
るように巻いて形成できるなどの任意適宜の方法を用い
て形成できる。
Further, for example, a superconducting tape (7) impregnated with a low-conductivity material such as solder, or a superconducting tape (7) and an insulating tape (9) superposed on each other are adhered to each other with an epoxy resin or the like. It can be formed by using any appropriate method such as forming by winding to form a loop-shaped hollow container.

なお第2図の例を含めて磁気遮蔽に用いる超電導体が
低温で性能を発揮する場合には、超電導材で作られたル
ープ状中空容器を低温容器中に収容するなどして冷却し
なければならない。
In the case where the superconductor used for magnetic shielding including the example of FIG. 2 performs at a low temperature, the loop-shaped hollow container made of the superconducting material must be cooled by being housed in a low-temperature container or the like. No.

(発明の効果) 以上のように本発明では交流用超電導材を巻いて磁気
回路となるループ状中空容器を形成し、しかも超電導テ
ープと絶縁性テープの重ね巻きする方法により中空容器
の周回方法に流れる電流の発生を防止する。従って低交
流損失であって、磁気回路中の軸方向に発生する伝達す
べき磁束を弱めることのない超電導磁気回路を構成で
き、しかも超電導材を金型などにより成形したり、その
一部に絶縁層を設けたりして作るものに比べ製作が容易
である。
(Effects of the Invention) As described above, in the present invention, a loop-shaped hollow container serving as a magnetic circuit is formed by winding a superconducting material for alternating current, and a superconducting tape and an insulating tape are overlapped and wound. Prevent the generation of flowing current. Therefore, a superconducting magnetic circuit that has low AC loss and does not weaken the magnetic flux to be transmitted generated in the axial direction in the magnetic circuit can be configured. It is easier to manufacture than one made by providing layers.

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

第1図は従来の超電導磁気回路の説明図、第2図は本発
明の一実施例回路図である。 (1)……超電導材によるループ状中空容器、(2)…
…1次コイル、(3)……2次コイル、(4)……周回
電流防止用絶縁層、(5)……交流用超電導線による縦
糸、(6)……交流用超電導線による横糸、(7)……
超電導材テープ、(8)……絶縁性ループ状中空容器、
(9)……周回電流防止用絶縁性テープ、(10)……オ
ーバーラップ部、(11)……樹脂材。
FIG. 1 is an explanatory diagram of a conventional superconducting magnetic circuit, and FIG. 2 is a circuit diagram of one embodiment of the present invention. (1) ... loop-shaped hollow container made of superconducting material, (2) ...
... primary coil, (3) ... secondary coil, (4) ... insulating layer for preventing circulating current, (5) ... warp by AC superconducting wire, (6) ... weft by AC superconducting wire, (7) ...
Superconducting material tape, (8) ... hollow insulating hollow container,
(9) ... Insulating tape for preventing circulating current, (10) ... Overlap, (11) ... Resin material.

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】交流用超電線を縦糸および横糸として織成
した布状超電導材を用いてループ状中空容器を形成して
磁気回路とすることを特徴とする超電導磁気回路。
1. A superconducting magnetic circuit, wherein a loop-shaped hollow container is formed using a cloth-like superconducting material in which AC superconducting wires are woven as warps and wefts to form a magnetic circuit.
【請求項2】絶縁性ループ状中空容器面を布状超電導材
により被覆して形成することを特徴とする特許請求の範
囲第1項記載の超電導磁気回路。
2. The superconducting magnetic circuit according to claim 1, wherein the surface of the insulating loop-shaped hollow container is covered with a cloth-like superconducting material.
【請求項3】絶縁性テープを布状超電導材と重ね合わせ
てループ状中空容器を形成することを特徴とする特許請
求の範囲第1項,第2項記載の超電導磁気回路。
3. The superconducting magnetic circuit according to claim 1, wherein a loop-shaped hollow container is formed by laminating an insulating tape with a cloth superconducting material.
JP14327688A 1988-06-10 1988-06-10 Superconducting magnetic circuit Expired - Lifetime JP2601318B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14327688A JP2601318B2 (en) 1988-06-10 1988-06-10 Superconducting magnetic circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14327688A JP2601318B2 (en) 1988-06-10 1988-06-10 Superconducting magnetic circuit

Publications (2)

Publication Number Publication Date
JPH01312807A JPH01312807A (en) 1989-12-18
JP2601318B2 true JP2601318B2 (en) 1997-04-16

Family

ID=15334981

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14327688A Expired - Lifetime JP2601318B2 (en) 1988-06-10 1988-06-10 Superconducting magnetic circuit

Country Status (1)

Country Link
JP (1) JP2601318B2 (en)

Also Published As

Publication number Publication date
JPH01312807A (en) 1989-12-18

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