JPH088165B2 - Current lead - Google Patents
Current leadInfo
- Publication number
- JPH088165B2 JPH088165B2 JP62080401A JP8040187A JPH088165B2 JP H088165 B2 JPH088165 B2 JP H088165B2 JP 62080401 A JP62080401 A JP 62080401A JP 8040187 A JP8040187 A JP 8040187A JP H088165 B2 JPH088165 B2 JP H088165B2
- Authority
- JP
- Japan
- Prior art keywords
- current
- current lead
- heat
- superconductor
- support
- 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
Links
Classifications
-
- Y02E40/642—
Landscapes
- Superconductors And Manufacturing Methods Therefor (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
Description
【発明の詳細な説明】 〈産業上の利用分野〉 この発明は超電導マグネット等に電流を供給するため
の電流リードに関する。The present invention relates to a current lead for supplying a current to a superconducting magnet or the like.
〈従来の技術と発明が解決しようとする問題点〉 従来、超電導マグネット等の超電導素子に電流を供給
するために、電流供給源と超電導素子との間に介在させ
る電流リードとしては、棒状あるいはパイプ状に形成さ
れた銅導体を用いたものが知られた。<Problems to be Solved by Conventional Techniques and Inventions> Conventionally, in order to supply a current to a superconducting element such as a superconducting magnet, a current supply source and a current lead interposed between the superconducting element have a rod shape or a pipe shape. It is known to use a copper conductor formed in a strip shape.
しかしながら、銅導体は常電導体で、しかも熱良伝導
体であるため、通電により発生した熱および高温端子側
の熱が、超電導マグネットを浸漬している液体ヘリウ
ム,液体窒素等の冷媒に伝導し、この伝導熱により冷媒
が蒸発するという弊害があった。However, since the copper conductor is a normal conductor and also a good conductor of heat, the heat generated by energization and the heat on the high temperature terminal side are conducted to the refrigerant such as liquid helium and liquid nitrogen in which the superconducting magnet is immersed. However, there is a problem that the refrigerant evaporates due to the conduction heat.
そこで、この液体ヘリウムへの伝導熱を最少限に抑え
るため、従来の電流リードにあっては、第3図に示すよ
うに、その表面に、螺旋フィン(110)を取り付け、こ
れをステンレス製の外筒管(120)の内部に収納した構
造のものとし、伝導熱にて蒸発したヘリウムガス(13
0)を超電導マグネット接続端子(140)側からリード内
に取り込んで、電流リード(100)を冷却しながら電流
を高温側端子(150)より超電導マグネットに供給する
という方法が行なわれ、さらに、液体ヘリウムへの伝導
熱をより少なくするため、電流リードの構造改善等、種
々の試験研究がなされているが、現時点では通電電流10
00Aあたり1Wの熱伝導は避け難いものとされていた。Therefore, in order to suppress the conduction heat to the liquid helium to a minimum, in the conventional current lead, as shown in FIG. 3, a spiral fin (110) is attached to the surface of the conventional current lead, which is made of stainless steel. The structure is such that it is housed inside the outer tube (120), and the helium gas (13
0) is taken into the lead from the superconducting magnet connection terminal (140) side, and current is supplied from the high temperature side terminal (150) to the superconducting magnet while cooling the current lead (100). In order to reduce the conduction heat to helium, various tests and researches have been conducted such as improving the structure of the current lead.
Heat conduction of 1W per 00A was said to be inevitable.
なお、1Wの熱伝導に対し例えば超電導マグネットの冷
媒として液体ヘリウムを用いた場合には、約1.4l/hrの
ヘリウムガスが蒸発する。When liquid helium is used as the refrigerant of the superconducting magnet for heat conduction of 1 W, about 1.4 l / hr of helium gas evaporates.
〈発明の目的〉 この発明は上記従来の電流リードの問題点に鑑みなさ
れたもので、伝導熱による液体ヘリウム、液体窒素等の
冷媒の蒸発量を低く抑えることができる電流リードを提
供することを目的とする。<Object of the Invention> The present invention has been made in view of the problems of the conventional current leads described above, and it is an object of the present invention to provide a current lead capable of suppressing the evaporation amount of a refrigerant such as liquid helium or liquid nitrogen due to conduction heat to be low. To aim.
〈問題点を解決するための手段〉 上記の目的を達成するためのこの発明の電流リード
は、電流供給源と超電導素子との間に介在させる電流リ
ードであって、セラミックス超電導体と、絶縁体あるい
は非磁性金属体からなる支持体との複合体よりなるもの
である。<Means for Solving the Problems> The current lead of the present invention for achieving the above object is a current lead interposed between a current supply source and a superconducting element, and includes a ceramic superconductor and an insulator. Alternatively, it is a composite with a support made of a non-magnetic metal body.
〈作用〉 この発明は、電流リードをセラミックス超電導体と絶
縁体あるいは非磁性金属体からなる支持体との複合体に
て形成したものゆえ、臨界温度以下では通電による発熱
がほとんどなく、また高温部からの熱伝導による冷媒へ
の熱伝導を少なくでき、液体ヘリウム、液体窒素等の冷
媒の蒸発量を少なくできる。<Operation> Since the present invention forms the current lead by a composite of a ceramic superconductor and a support made of an insulator or a non-magnetic metal body, there is almost no heat generation due to energization below the critical temperature, and the high temperature part It is possible to reduce the heat conduction to the refrigerant due to the heat conduction from, and to reduce the evaporation amount of the refrigerant such as liquid helium and liquid nitrogen.
〈実施例〉 この発明の実施例について添付図面を参照しながら以
下に詳述する。<Embodiment> An embodiment of the present invention will be described in detail below with reference to the accompanying drawings.
第1図はこの発明の電流リード(1)を2個一対にし
て使用した場合を示す断面図、第2図は第1図のII−II
線切断断面図である。FIG. 1 is a cross-sectional view showing a case where two current leads (1) of the present invention are used as a pair, and FIG. 2 is II-II of FIG.
It is a line cutting sectional view.
上記電流リード(1)は、酸化物セラミックスからな
る超電導体(1a)および、この超電導体(1a)を支持す
るFRP等の絶縁体、あるいは銅、アルミニウム、ステン
レス等の非磁性金属体からなる支持体(1b)よりなる複
合体にて形成されている。The current lead (1) is a support made of a superconductor (1a) made of oxide ceramics, an insulator such as FRP supporting the superconductor (1a), or a non-magnetic metal body such as copper, aluminum or stainless steel. It is formed of a complex composed of the body (1b).
なお、支持体(1b)として非磁性金属体を用いた場合
には、超電導体(1a)を支持する支持体としての役目を
果すとともに、超電導体(1a)の安定化材としての役目
を果し、好適な実施となる。When a non-magnetic metal body is used as the support (1b), it serves not only as a support for supporting the superconductor (1a) but also as a stabilizer for the superconductor (1a). However, this is a suitable implementation.
電流リード(1)は、例えば、非磁性金属体からなる
支持体(1b)の上に超電導体(1a)の粉末を圧粉、接
着、押出、電着等の方法により一体化するか、超電導体
(1a)のみを先に成型しておき、これを支持体(1b)に
接着するか、またはバインドして複合一体化する。な
お、接着にて両者を複合一体化する場合は、接着剤とし
て、エポキシ系樹脂等の有機材料を用いて接着し、複合
化するのが容易である。The current lead (1) is formed, for example, by integrating the powder of the superconductor (1a) on a support (1b) made of a nonmagnetic metal body by a method such as powder compaction, adhesion, extrusion, electrodeposition, or superconductivity. Only the body (1a) is molded in advance, and the body (1a) is bonded to the support (1b) or bound to form a composite body. In the case where the both are combined and integrated by adhesion, it is easy to use an organic material such as an epoxy resin as an adhesive agent for adhesion to form a composite.
上記電流リード(1)は、単独でも使用可能である
が、一対にして用いる実施が別々に設ける場合よりコン
パクトとなり(第1図参照)好適な実施となる。The current lead (1) can be used alone, but it is preferable to use it in a pair as it is more compact than that provided separately (see FIG. 1).
以下に一対の電流リードを用いる実施についてさらに
詳細に述べると、電流リード(1)(1)間にスペーサ
(2)を長手方向に介在させ、適宜間隔毎にその周囲を
サポート(3)で支持する。To describe in more detail below the implementation using a pair of current leads, a spacer (2) is longitudinally interposed between the current leads (1) and (1), and the periphery thereof is supported by a support (3) at appropriate intervals. To do.
なお、スペーサ(2)は電流リード(1)の支持体
(1b)が金属体にて形成されている場合はGFRP等の絶縁
体を用い、支持体(1b)が絶縁体の場合は、絶縁体、金
属体のいずれでもよく、また省略も可能である。サポー
タ(3)としては、絶縁性を有するディスク状のものを
嵌め込むか、バインド用の絶縁テープを巻き付ける。The spacer (2) is made of an insulator such as GFRP when the support (1b) of the current lead (1) is made of a metal body, and is insulated when the support (1b) is an insulator. It may be a body or a metal body, and may be omitted. As the supporter (3), a disk-shaped one having an insulating property is fitted or an insulating tape for binding is wound.
なお、正負一対の電流リード(1)を用いた上例の場
合には、電流リード(1)の周囲に磁界が印加された状
態で通電すると、電流リード(1)(1)間と外部磁界
との間で作用するローレンツ力は互いに押し合う方向に
働くこととなり、スペーサ(2)は両電流リード(1)
(1)間の圧縮力に耐え得る強度を有するとともに十分
な絶縁距離を備えたものであることが必要となるが、サ
ポータ(3)はさほど堅固なものでなくてもよく、省略
または非常に小型のものでよいためコンパクトに実施で
き好適なものとなる。In the case of the above example using a pair of positive and negative current leads (1), if current is applied with a magnetic field applied around the current leads (1), the current between the current leads (1) (1) and the external magnetic field The Lorentz forces acting between and act on the spacers (2) in such a direction that they push each other, and the spacer (2) acts on both current leads (1).
It is necessary that the supporter (3) has a strength capable of withstanding the compressive force between (1) and a sufficient insulation distance, but the supporter (3) does not have to be so rigid, and may be omitted or extremely Since it can be small in size, it can be implemented compactly, which is preferable.
逆に無磁化の状態で通電する場合には、電流リード
(1)自身により磁界が発生することとなり、しかも各
電流リード(1)に流れる電流の向きが反対方向である
ため、ローレンツの力は両者を互に反発させる方向に作
用する。したがって、上記電流リード(1)の周囲に磁
界を印加した状態で通電する場合と異なり、この場合に
は、スペーサ(2)よりもサポータ(3)を堅固な構造
としておく必要がある。また(4)はクライオスタート
のトップフランジに電流リード(1)を取り付けるため
のフランジであって、クライオスタートトップフランジ
と電流リード(1)とを絶縁する機能を保持させておく
ものである。(5)は高温側接続端子、(6)は超電導
マグネット側接続端子である。On the contrary, when energized in the non-magnetized state, the magnetic field is generated by the current lead (1) itself, and moreover, the direction of the current flowing through each current lead (1) is in the opposite direction, so the Lorentz force is It acts to repel each other. Therefore, unlike the case where the current is applied in the state where a magnetic field is applied around the current lead (1), in this case, the supporter (3) needs to have a firm structure rather than the spacer (2). Further, (4) is a flange for attaching the current lead (1) to the top flange of the cryostart, and keeps the function of insulating the cryostart top flange and the current lead (1). (5) is a high temperature side connecting terminal, and (6) is a superconducting magnet side connecting terminal.
上記セラミックス超電導体はセラミックス超電導体用
原料を焼結する等によって製造され、その原料として
は、超電導体を構成する元素を含有するものであれば単
体、化合物の何れの形態でも使用し得る。上記元素とし
ては、周期律表I族、II族およびIII族元素並に酸素、
フッ素が例示される。The ceramic superconductor is manufactured by sintering a raw material for a ceramic superconductor, and the raw material may be either a simple substance or a compound as long as it contains an element constituting the superconductor. Examples of the above-mentioned elements include oxygen in the groups I, II and III of the periodic table,
An example is fluorine.
より詳細には、周期律表I族元素のうち、Ia族元素と
しては、Li、Na、K、Rb、Cs等が挙げられ、Ib族元素と
しては、Cu、AgおよびAuが挙げられる。また、周期律表
II族元素のうち、IIa族元素としては、Be、Mg、Ca、S
r、BaおよびRaが挙げられ、IIb族元素としては、Zn、Cd
等が挙げられる。周期律表III族元素のうち、IIIa族元
素としては、Sc、Yやランタノイド系元素であるLa、C
e、Gd、Lu等、アクチノイド系元素であるAc、Th、Pa、C
f等が挙げられる。また、IIIb族元素としては、Al、G
a、In、Tl等が挙げられる。More specifically, among the group I elements of the periodic table, examples of the group Ia elements include Li, Na, K, Rb, and Cs, and the group Ib elements include Cu, Ag, and Au. Also, the periodic table
Of the II group elements, the IIa group elements include Be, Mg, Ca, S
r, Ba, and Ra, and the IIb group elements include Zn and Cd.
Etc. Of the III group elements of the periodic table, IIIa group elements include Sc, Y and lanthanoid series elements such as La and C.
Actinides such as e, Gd, Lu, etc. Ac, Th, Pa, C
f and the like. Further, as the group IIIb element, Al, G
a, In, Tl and the like.
上記元素のうち、Ib族元素から選ばれた元素、特に酸
化物からなるIIa族元素、IIIa族元素およびランタノイ
ド系元素から選ばれた元素、並びに酸素およびフッ素か
ら選ばれた元素からなるセラミックス超電導体が好まし
い。尚、Ib族元素としてはCuおよびAgが好ましい。Of the above elements, a ceramic superconductor composed of an element selected from the group Ib, particularly an element selected from the group IIa composed of oxides, a group IIIa and a lanthanoid series element, and an element selected from oxygen and fluorine. Is preferred. Note that Cu and Ag are preferable as the Group Ib element.
なお、酸化物セラミックス超電導体(1a)を用いた電
流リード(1)の場合の、高温部からの伝熱による冷媒
への熱伝導量を計測した結果、例えば4.2K〜300Kの場合
で、熱伝導積分値超電導▲∫300k 4.2kλ▼dT(λは熱伝
導率である)は約1990×10-3(W/cm)であった。In addition, in the case of the current lead (1) using the oxide ceramics superconductor (1a), as a result of measuring the amount of heat conduction to the refrigerant due to heat transfer from the high temperature part, for example, in the case of 4.2K to 300K, Conduction integral value Superconductivity ▲ ∫ 300k 4.2k λ ▼ dT (λ is thermal conductivity) was about 1990 × 10 -3 (W / cm).
これは、概ねガラス,石英に近似し、電解銅の1620
(W/cm),燐脱酸銅の461(W/cm)に比べ、1/800あるい
は1/230の減少を示したものとなり、冷媒への伝導熱量
を非常に少なくできたことが判明した。This is approximately similar to glass and quartz, and is 1620 of electrolytic copper.
(W / cm), compared with 461 (W / cm) of phosphorous deoxidized copper, it was reduced by 1/800 or 1/230, and it was revealed that the heat of conduction to the refrigerant could be extremely reduced. .
また、超電導体(1a)と複合される支持体(1b)とし
て例えば、4ふっ化エチレン樹脂,GFRP等を用いた場合
の熱伝導は700×10-3〜1000×10-3(W/cm)と非常に小
さく良好なものとなる。さらに金属体を用いた場合でも
従来のもののように金属体に電流を通電するわけではな
く安定化材あるいは支持体としての働きを有するもので
ある。したがって、その断面積等を従来のもののように
通電電流容量を確保するために特に大きくする必要はな
く、安定化材、支持体としての働きをなす大きさで十分
であり、液体ヘリウム等の冷媒への伝導熱量は大幅に減
らすことができる。Further, when the support (1b) to be combined with the superconductor (1a) is, for example, tetrafluoroethylene resin, GFRP, etc., the heat conduction is 700 × 10 −3 to 1000 × 10 −3 (W / cm 2 ) Is very small and good. Furthermore, even when a metal body is used, it does not pass an electric current through the metal body as in the conventional one, but it functions as a stabilizer or a support. Therefore, it is not necessary to make the cross-sectional area and the like particularly large in order to secure the current carrying capacity unlike the conventional ones, and a size that acts as a stabilizing material and a support is sufficient, and a refrigerant such as liquid helium is sufficient. The amount of heat transferred to can be greatly reduced.
〈発明の効果〉 以上のようにこの発明によれば、電流リードをセラミ
ックス超電導体と、絶縁体あるいは非磁性金属体からな
る支持体との複合体にて形成したものゆえ、臨界温度以
下では通電による発熱はほとんどなくなり、また高温部
からの熱伝導による冷媒への伝導熱量は大幅に減少され
るため、冷媒の蒸発量を最少限にでき、従来の常電導の
ものに比べ構造が非常に簡単で、コンパクトな構造で形
成できるという特有の効果を奏する。<Effects of the Invention> As described above, according to the present invention, the current lead is formed of a composite of a ceramics superconductor and a support made of an insulating material or a non-magnetic metal material. The heat generated by the heat is almost eliminated, and the amount of heat transferred to the refrigerant due to heat conduction from the high temperature part is greatly reduced, so that the evaporation amount of the refrigerant can be minimized and the structure is much simpler than that of the normal conducting type. Therefore, it has a unique effect that it can be formed with a compact structure.
第1図は電流リードの1実施例を示す断面図、第2図は
前面II−II線切欠断面図、第3図は従来例を示す断面図
である。 (1)……電流リード、(1a)……超電導体、(1b)…
…支持体、FIG. 1 is a sectional view showing one embodiment of a current lead, FIG. 2 is a sectional view taken along the line II-II of the front surface, and FIG. 3 is a sectional view showing a conventional example. (1) ... Current lead, (1a) ... Superconductor, (1b) ...
... support,
Claims (1)
る電流リードであって、セラミックス超電導体と、絶縁
体あるいは非磁性金属体からなる支持体との複合体より
なることを特徴とする電流リード。1. A current lead interposed between a current supply source and a superconducting element, comprising a composite of a ceramics superconductor and a support made of an insulating material or a non-magnetic metal material. Current lead.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62080401A JPH088165B2 (en) | 1987-03-31 | 1987-03-31 | Current lead |
| US07/174,468 US4965246A (en) | 1987-03-31 | 1988-03-28 | Current-carrying lead formed of a ceramic superconductive material carried by a support |
| EP88105209A EP0285147B2 (en) | 1987-03-31 | 1988-03-30 | Current-carrying lead |
| DE3879739T DE3879739T3 (en) | 1987-03-31 | 1988-03-30 | Live wire. |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62080401A JPH088165B2 (en) | 1987-03-31 | 1987-03-31 | Current lead |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63245909A JPS63245909A (en) | 1988-10-13 |
| JPH088165B2 true JPH088165B2 (en) | 1996-01-29 |
Family
ID=13717267
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62080401A Expired - Lifetime JPH088165B2 (en) | 1987-03-31 | 1987-03-31 | Current lead |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH088165B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03283678A (en) * | 1990-03-30 | 1991-12-13 | Fuji Electric Co Ltd | Current lead of superconducting magnet apparatus |
| JPH04165680A (en) * | 1990-10-30 | 1992-06-11 | Fuji Electric Co Ltd | Current lead superconducting device |
| JP7710977B2 (en) * | 2021-12-21 | 2025-07-22 | 株式会社東芝 | High-temperature superconducting coil device and stacked-type high-temperature superconducting coil device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5998505A (en) * | 1982-11-26 | 1984-06-06 | Japanese National Railways<Jnr> | Super conductive current lead |
-
1987
- 1987-03-31 JP JP62080401A patent/JPH088165B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63245909A (en) | 1988-10-13 |
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