JPH0287424A - Complexed superconductive conductor - Google Patents
Complexed superconductive conductorInfo
- Publication number
- JPH0287424A JPH0287424A JP63237682A JP23768288A JPH0287424A JP H0287424 A JPH0287424 A JP H0287424A JP 63237682 A JP63237682 A JP 63237682A JP 23768288 A JP23768288 A JP 23768288A JP H0287424 A JPH0287424 A JP H0287424A
- Authority
- JP
- Japan
- Prior art keywords
- superconductive
- superconducting
- current circuit
- high resistance
- induction current
- 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
- 239000004020 conductor Substances 0.000 title abstract description 5
- 239000000463 material Substances 0.000 claims abstract description 19
- 239000002131 composite material Substances 0.000 claims description 15
- 239000002887 superconductor Substances 0.000 claims description 9
- 230000000087 stabilizing effect Effects 0.000 claims description 8
- 239000002184 metal Substances 0.000 abstract description 7
- 229910052751 metal Inorganic materials 0.000 abstract description 7
- 229910000679 solder Inorganic materials 0.000 abstract description 6
- 229910002482 Cu–Ni Inorganic materials 0.000 abstract description 3
- 229910045601 alloy Inorganic materials 0.000 abstract description 3
- 239000000956 alloy Substances 0.000 abstract description 3
- 239000011159 matrix material Substances 0.000 abstract description 3
- 230000004907 flux Effects 0.000 abstract description 2
- 230000006698 induction Effects 0.000 abstract 4
- 239000003381 stabilizer Substances 0.000 abstract 1
- 230000008878 coupling Effects 0.000 description 13
- 238000010168 coupling process Methods 0.000 description 13
- 238000005859 coupling reaction Methods 0.000 description 13
- 239000010949 copper Substances 0.000 description 6
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 5
- 229910052802 copper Inorganic materials 0.000 description 5
- 230000000694 effects Effects 0.000 description 3
- 229910052734 helium Inorganic materials 0.000 description 2
- 239000001307 helium Substances 0.000 description 2
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 2
- 239000007788 liquid Substances 0.000 description 2
- 229910000990 Ni alloy Inorganic materials 0.000 description 1
- 238000005219 brazing Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 238000010791 quenching Methods 0.000 description 1
Classifications
-
- Y—GENERAL 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
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment
Abstract
Description
【発明の詳細な説明】
〔発明の目的〕
(産業上の利用分野)
本発明は超電導材を安定化ハウジング材中に埋込み構成
する複合化超電導4体に関する。DETAILED DESCRIPTION OF THE INVENTION OBJECTS OF THE INVENTION (Industrial Field of Application) The present invention relates to a composite superconducting body in which a superconducting material is embedded in a stabilizing housing material.
(従来の技術)
一般に複合化超電導4体において鎖交磁界が変動すると
超電源フィラメント同土間に誘起される誘起電流による
交流損失が発生する。このメカニズムによる交流損失を
結合損失という。交流損失形態の種類にはこれ以外にピ
ンニング損失及びうず電流損失があるが、鎖交磁界の変
動率がある程度大きくなると上記3種類の交流損失のう
ち結合損失がほとんど支配的になることは周知のとおり
である。(Prior Art) In general, when the interlinkage magnetic field fluctuates in the four composite superconductors, alternating current loss occurs due to the induced current induced between the superpower filaments and the earthen floor. AC loss due to this mechanism is called coupling loss. Other types of AC loss include pinning loss and eddy current loss, but it is well known that coupling loss becomes predominant among the three types of AC loss when the fluctuation rate of the interlinking magnetic field increases to a certain extent. That's right.
すなわち、従来の複合化超電専々体は第3図に示すよう
に銅マトリックス■中に超電導フィラメン)・0を多数
埋込んだ超電導材0)を2分割の安定化ハウジング材(
通常材料は銅)■の中に配置し各接合節は半田■で接合
した構造をなしている。In other words, as shown in Figure 3, the conventional composite superelectric body consists of a superconducting material (0) in which a large number of superconducting filaments (0) and (0) are embedded in a copper matrix (2), and a stabilizing housing material (0) divided into two.
The structure is such that the material is usually copper) and each joint is connected with solder.
そのため上記誘起電流0が流れる電流路の抵抗は銅の比
抵抗だけでほぼ決るため、結合損失は非常に大きなもの
となる。Therefore, the resistance of the current path through which zero induced current flows is almost determined only by the resistivity of copper, resulting in a very large coupling loss.
よってこのような複合化超電導4体を用いた超電導マグ
ネットにおいては以下のような不具合がある。Therefore, a superconducting magnet using such four composite superconducting bodies has the following problems.
例えば、水冷マグネットを内側に、そして超電導マグネ
ットを外側に同心円状に配し合わせて中心部に高磁界を
発生するハイブリットマグネットにおいては、水冷マグ
ネットがそのトラブルのためしゃ断する場合、超電導マ
グネットに発生する結合損失のため超電導マグネットが
クエンチする可能性が非常に大きい。For example, in a hybrid magnet that generates a high magnetic field in the center by concentrically arranging a water-cooled magnet on the inside and a superconducting magnet on the outside, if the water-cooled magnet shuts off due to a problem, the problem occurs in the superconducting magnet. There is a great possibility that the superconducting magnet will quench due to coupling loss.
また、超電導マグネット単独として用いる場合でも何ら
かの外的な要因のため超電導マグネットが誤しゃ断され
ると、結合損失の発生にもとづく液体ヘリウムの蒸発が
過大となり、破裂板を吹かせてしまい、液体ヘリウムの
多大な消費を引起すことのみならず、超電導マグネット
システム全体のシステムダウンを引起すことが多かった
。In addition, even when a superconducting magnet is used alone, if the superconducting magnet is accidentally cut off due to some external factor, the evaporation of liquid helium due to the occurrence of coupling loss will be excessive, causing the rupture disc to blow, and the liquid helium will evaporate excessively due to coupling loss. This not only causes a large amount of consumption, but also often causes the entire superconducting magnet system to go down.
(発明が解決しようとする課題)
従来の複合化超電導4体においては誘起電流の電流回路
の抵抗値が小さいことが結合損失を大きくしている主た
る原因である。そこで結合損失の小さい複合化超電導4
体の発明が要望されている。(Problems to be Solved by the Invention) In the conventional composite superconductor 4 body, the main reason for the large coupling loss is that the resistance value of the current circuit for the induced current is small. Therefore, composite superconductor 4 with low coupling loss
There is a demand for physical inventions.
本発明は誘起電流回路の抵抗値を従来より大幅に大きく
とれるような複合化超電導4体を提供することを目的と
する。An object of the present invention is to provide a composite superconductor 4 body which allows the resistance value of the induced current circuit to be significantly larger than that of the prior art.
(課題を解決するための手段) 上記目的を達成するために、本発明においては。 (Means for solving problems) In order to achieve the above object, in the present invention.
超電導材を安定化ハウジング材中に埋込こみ構成する複
合化超電導4体において、超電導材から安定化ハウジン
グへの誘起電流回路に高抵抗部材を配設したことを特徴
とする複合化超電導4体を提供する。A composite superconductor 4 body comprising a superconducting material embedded in a stabilizing housing material, characterized in that a high resistance member is disposed in an induced current circuit from the superconducting material to the stabilizing housing. I will provide a.
(作 用)
このようにすると高抵抗部材が誘起電流を抑1tllし
結合損失を大幅に低減する。(Function) In this way, the high-resistance member suppresses the induced current and significantly reduces the coupling loss.
(実施例)
実施例1
以下、本発明の第1の実施例について、第1図を参照し
て説明する。(Examples) Example 1 A first example of the present invention will be described below with reference to FIG. 1.
第1図は本発明による複合化超電尋々体の切断端面を示
すもので銅マトリックス■中に多数の超電導フィラメン
ト0を埋込み、超電導材Ω)を形成すると共にその周囲
にCu−Ni合金等による高抵抗金属シース■を配置し
これを2分割された安定化ハウジング材ω内に半田■に
より接合して構成する。結合損失を発生する誘起電流■
は矢印で示す。Figure 1 shows a cut end surface of a composite superconductor body according to the present invention, in which a large number of superconducting filaments 0 are embedded in a copper matrix 1, forming a superconducting material Ω), and surrounding it a Cu-Ni alloy etc. A high-resistance metal sheath (2) is placed inside the stabilized housing material (ω), which is divided into two parts, and is joined by solder (2). Induced current that causes coupling loss■
is indicated by an arrow.
次にこの実施例1の作用を説明する。Next, the operation of this first embodiment will be explained.
上記のように構成すると、超電導フィラメント■同士間
を流れる誘起電流■の電流回照内には。With the above configuration, the induced current (■) flowing between the superconducting filaments (■) is within the current circulation.
第3図に示す従来の複合化超電導4体と異なり。This is different from the conventional composite superconductor 4 body shown in Figure 3.
高抵抗全屈シース■が介在するため誘起電流の電流回路
の抵抗は大幅に増大する。Due to the presence of the high-resistance fully bent sheath (2), the resistance of the induced current circuit increases significantly.
例えば、4.2に温度下での銅の比抵抗は磁場条件ある
いはハードネスの状態にもよるがおおよそ1O−8Ω・
口のオーダである一方、Cu−Ni合金のそれは104
Ω・口のオーダである。よってわずかの厚みのCu −
Ni合金のシースを高抵抗部材である高抵抗金凡シース
■として採用することにより、上記抵抗は大幅に増大す
ることがわかる。For example, as shown in 4.2, the specific resistance of copper at temperature is approximately 1O-8Ω・depending on the magnetic field conditions and hardness condition.
On the other hand, that of Cu-Ni alloy is 104
It is on the order of Ω/mouth. Therefore, a small thickness of Cu −
It can be seen that by employing the Ni alloy sheath as the high resistance metal sheath (2), which is a high resistance member, the above resistance increases significantly.
そのため複合化超電導4体に鎖交する磁界変動にもとづ
く誘起電流■は抑制され、大幅に結合損失を低減できる
効果がある。Therefore, the induced current (2) based on magnetic field fluctuations interlinking with the four composite superconducting bodies is suppressed, which has the effect of significantly reducing coupling loss.
ここで高抵抗金属シース(3)内に超電導材■を配置し
、いっしょに線引することにより上記導体構成は容易に
実現できる。The above conductor structure can be easily realized by placing the superconducting material (3) inside the high-resistance metal sheath (3) and drawing it together.
尚、半田を他のろう材に代えてもよい。Note that the solder may be replaced with another brazing material.
実施例2 第2図は本発明の第2の実施例を示すもので上。Example 2 FIG. 2 shows a second embodiment of the present invention.
下の安定化ハウジング材(1)同士の接合面に高抵抗部
材である高抵抗金属テープ(3a)を挿入し半田■で各
々接合し構成したものである。この場合も誘起電流■の
電流回路には第3図に示す従来の複合化超電導4体と異
なり、大きな抵抗層が介在するため誘起電流■が抑制さ
れ、結合損失が大幅に低減する効果がある。A high-resistance metal tape (3a), which is a high-resistance member, is inserted into the joint surfaces of the lower stabilizing housing materials (1), and each is joined with solder (2). In this case as well, unlike the conventional composite superconductor 4 shown in Figure 3, the current circuit for the induced current ■ has a large resistance layer, which suppresses the induced current ■ and has the effect of significantly reducing coupling loss. .
ここで高抵抗金属テープ(3a)は2分割の安定化ハウ
ジング材ωを半田■で接合する際、いっしょに接合する
ことにより上記導体構成は容易に実現できる。Here, the above-described conductor structure can be easily realized by joining the high-resistance metal tape (3a) together when the two halves of the stabilizing housing material ω are joined together with solder (2).
以上説明したように本発明によれば簡単な構成により、
鎖交磁束変動にもとづく結合損失を大幅に低減すること
が可能な複合化超電導4体を提供できる。As explained above, according to the present invention, with a simple configuration,
It is possible to provide four composite superconducting bodies that can significantly reduce coupling loss due to flux linkage fluctuations.
第1図は本発明の複合化超電導4体の第1の実施例を示
す切口端面図、第2図は第2の実施例を示す切口端面図
、第3図は従来例を示す切口端而図である。FIG. 1 is a cut end view showing a first embodiment of the four composite superconducting bodies of the present invention, FIG. 2 is a cut end view showing the second embodiment, and FIG. 3 is a cut end view showing a conventional example. It is a diagram.
Claims (1)
複合化超電導々体において、超電導材から安定化ハウジ
ングへの誘起電流回路に高抵抗部材を配設したことを特
徴とする複合化超電導々体。A composite superconductor comprising a superconducting material embedded in a stabilizing housing material, characterized in that a high resistance member is disposed in an induced current circuit from the superconducting material to the stabilizing housing. .
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63237682A JPH0287424A (en) | 1988-09-22 | 1988-09-22 | Complexed superconductive conductor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP63237682A JPH0287424A (en) | 1988-09-22 | 1988-09-22 | Complexed superconductive conductor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0287424A true JPH0287424A (en) | 1990-03-28 |
Family
ID=17018946
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP63237682A Pending JPH0287424A (en) | 1988-09-22 | 1988-09-22 | Complexed superconductive conductor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0287424A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5442137A (en) * | 1990-11-22 | 1995-08-15 | Kabushiki Kaisha Toshiba | Superconductor wire and method of manufacturing the same |
-
1988
- 1988-09-22 JP JP63237682A patent/JPH0287424A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5442137A (en) * | 1990-11-22 | 1995-08-15 | Kabushiki Kaisha Toshiba | Superconductor wire and method of manufacturing the same |
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