JPH06176632A - Superconductor - Google Patents
SuperconductorInfo
- Publication number
- JPH06176632A JPH06176632A JP4323866A JP32386692A JPH06176632A JP H06176632 A JPH06176632 A JP H06176632A JP 4323866 A JP4323866 A JP 4323866A JP 32386692 A JP32386692 A JP 32386692A JP H06176632 A JPH06176632 A JP H06176632A
- Authority
- JP
- Japan
- Prior art keywords
- stabilizing member
- superconducting
- loss
- magnetic field
- superconducting 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.)
- Withdrawn
Links
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
Landscapes
- Superconductors And Manufacturing Methods Therefor (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、超伝導コイル等を形成
するための超伝導導体に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a superconducting conductor for forming a superconducting coil or the like.
【0002】[0002]
【従来の技術】超伝導状態の超伝導線材に大電流を流し
ているときに、何らかの原因で超伝導線材の温度が上昇
すると、超伝導状態がら常伝導状態に移行してしまうこ
とがある。この現象はクエンチと呼ばれる。2. Description of the Related Art When a large current is applied to a superconducting wire in a superconducting state and the temperature of the superconducting wire rises for some reason, the superconducting state may shift to a normal conducting state. This phenomenon is called quench.
【0003】クエンチが生じると、その部分でジュール
発熱が生じ、超伝導線材が損傷することがある。このよ
うな損傷を防止するために超伝導線材にたとえば純アル
ミニウム等の良導電体からなる安定化部材を併設するこ
とにより、超伝導線材の一部にクエンチが生じた場合、
上記安定化部材により電流をバイパスさせる手段があ
る。When quenching occurs, Joule heat is generated at that portion and the superconducting wire may be damaged. In order to prevent such damage, by attaching a stabilizing member made of a good conductor such as pure aluminum to the superconducting wire, if a quench occurs in part of the superconducting wire,
There is a means for bypassing the current by the stabilizing member.
【0004】図2はそのような構造をもつ超伝導導体の
断面図である。図示の如く超伝導導体1を構造部材2で
囲み、その外側を絶縁部材3で覆い、超伝導線材1に安
定化部材5を併置した構成となっている。このように一
体型の安定化部材5を用いたものでは、超伝導導体を速
い磁場変化状態で使用する場合、安定化部材5の中に誘
導電流が発生し、交流損失が増加する。この交流損失の
増加をおさえる対策として安定化部材5の多層化が考え
られている。FIG. 2 is a sectional view of a superconducting conductor having such a structure. As shown in the figure, the superconducting conductor 1 is surrounded by a structural member 2, the outer side of which is covered with an insulating member 3, and a stabilizing member 5 is arranged on the superconducting wire 1. In the case of using the integrated stabilizing member 5 as described above, when the superconducting conductor is used in a rapid magnetic field changing state, an induced current is generated in the stabilizing member 5 and the AC loss increases. As a measure for suppressing this increase in AC loss, multilayering of the stabilizing member 5 is considered.
【0005】図3はその一例を示す断面図である。図3
に示すように安定化部材5を複数層に分割して多層型安
定化部材6となしたものであり、各層の安定化部材6の
表面には比較的電気抵抗の大きい材料、たとえばCuN
i等が被覆されている。しかし、図3のように構成され
たものでは、X方向の磁場成分に対する交流損失は低減
されるが、Y方向の磁場成分に対する交流損失は低減さ
れないという不具合がある。FIG. 3 is a sectional view showing an example thereof. Figure 3
The stabilizing member 5 is divided into a plurality of layers to form a multilayer stabilizing member 6, as shown in FIG.
i, etc. are covered. However, the configuration as shown in FIG. 3 has a drawback that the AC loss for the magnetic field component in the X direction is reduced, but the AC loss for the magnetic field component in the Y direction is not reduced.
【0006】[0006]
【発明が解決しようとする課題】上記したように図3に
示す構成のものでは、超伝導導体が経験する磁場変化の
うち、X方向の磁場成分に対する交流損失の低減には効
果があるが、Y方向の磁場成分に対しては低減効果がな
い。このため交流損失(ジュール発熱)が大きくなり、
超伝導線材のクエンチ現象を引き起こす可能性が高くな
ると共に、冷却系への負荷が過大となり、超伝導コイル
システムの効率が低下するという問題があった。As described above, the structure shown in FIG. 3 is effective in reducing the AC loss with respect to the magnetic field component in the X direction among the magnetic field changes experienced by the superconducting conductor. There is no reduction effect on the magnetic field component in the Y direction. As a result, AC loss (Joule heat generation) increases,
There is a problem that the quenching phenomenon of the superconducting wire increases and the load on the cooling system becomes excessive and the efficiency of the superconducting coil system decreases.
【0007】本発明は、いずれの方向の磁場成分に対す
る交流損失をも低減することができ、超伝導線材のクエ
ンチ現象を引き起こすおそれがない上、冷却負荷の増大
を招くことがなく、効率のよい超伝導コイルシステムを
実現可能な超伝導導体を提供することにある。The present invention can reduce the AC loss with respect to the magnetic field component in any direction, does not cause the quench phenomenon of the superconducting wire, and does not cause an increase in cooling load, and is efficient. It is to provide a superconducting conductor that can realize a superconducting coil system.
【0008】[0008]
【課題を解決するための手段】上記課題を解決し目的を
達成するために、本発明は、超伝導線材に接して設けら
れる安定化部材が、小さな矩形状に区切られており、か
つその表面を、比較的電気抵抗の高い材料で覆われてい
るようにした。In order to solve the above-mentioned problems and to achieve the object, the present invention provides a stabilizing member provided in contact with a superconducting wire in the form of a small rectangle, and its surface. To be covered with a material having a relatively high electric resistance.
【0009】[0009]
【作用】上記手段を講じた結果、次のような作用が生じ
る。安定化部材が、小さい矩形状に区切られているた
め、超伝導導体が変動磁場中で使用される場合に、経験
する磁場成分のうち、X方向およびY方向の両成分のい
ずれに対しても交流損失を低減することができる。As a result of taking the above-mentioned means, the following effects occur. Since the stabilizing member is divided into small rectangular shapes, when the superconducting conductor is used in a fluctuating magnetic field, both of the X-direction and Y-direction components of the magnetic field component to be experienced are experienced. AC loss can be reduced.
【0010】[0010]
【実施例】図1は本発明の一実施例に係る超伝導導体の
構成を示す断面図である。図1に示すように本実施例の
超伝導線材1は断面コの字状の構造部材2によって囲ま
れており、構造部材2の外側は絶縁部材3にて被覆され
ている。構造部材2の内側には超伝導線材1に接するよ
うに安定化部材10が設けられている。この安定化部材
10は、図1の紙面に垂直な方向の超伝導導体の電流の
流れ方向にみた断面積が、極めて微小面積となるように
小さな矩形状に区切られたものとなっている。上記、安
定化部材10は例えば純アルミニウムのような良導電体
でできており、かつその表面には比較的高電気抵抗を有
する材料、たとえばCuNiを用いた絶縁被覆11(含
塗装)が施されている。酸化被膜等もこれに含まれる。1 is a sectional view showing the structure of a superconducting conductor according to an embodiment of the present invention. As shown in FIG. 1, the superconducting wire 1 of this embodiment is surrounded by a structural member 2 having a U-shaped cross section, and the outside of the structural member 2 is covered with an insulating member 3. A stabilizing member 10 is provided inside the structural member 2 so as to contact the superconducting wire 1. The stabilizing member 10 is divided into small rectangular shapes so that the cross-sectional area of the superconducting conductor in the direction perpendicular to the plane of FIG. The stabilizing member 10 is made of a good conductor such as pure aluminum, and the surface thereof is coated with an insulating coating 11 (including coating) using a material having a relatively high electric resistance, for example, CuNi. ing. This includes oxide films and the like.
【0011】本実施例の超伝導導体は、安定化部材10
が小さな矩形状に区切られて配置されているため、超伝
導導体が変動磁場中で使用される場合に、X方向および
Y方向のいずれの磁場成分に対しても、安定化部材10
中に発生する交流損失(ジュール発熱)による超伝導線
材1のクエンチ現象の発生を防止することができる。ま
た、冷却系の負荷軽減にも寄与するため、超伝導コイル
システムの効率を向上させ得る。なお、本発明は上記実
施例に限定されるものではなく、本発明の要旨を逸脱し
ない範囲で種々変形実施可能であるのは勿論である。The superconducting conductor of this embodiment has a stabilizing member 10.
Are arranged in a small rectangular shape, so that when the superconducting conductor is used in a fluctuating magnetic field, the stabilizing member 10 can be applied to both magnetic field components in the X direction and the Y direction.
It is possible to prevent the quench phenomenon of the superconducting wire rod 1 from occurring due to the AC loss (Joule heat generation) generated therein. Further, since it also contributes to reducing the load on the cooling system, the efficiency of the superconducting coil system can be improved. The present invention is not limited to the above-mentioned embodiments, and it goes without saying that various modifications can be made without departing from the gist of the present invention.
【0012】[0012]
【発明の効果】本発明によれば、超伝導線材に接して設
けられる安定化部材が小さな矩形状に区切られているた
め、いずれの方向の磁場成分に対する交流損失をも低減
することができ、超伝導線材のクエンチ現象を引き起こ
すおそれがない上、冷却負荷の増大を招くことがなく、
効率のよい超伝導コイルシステムを実現可能な超伝導導
体を提供できる。According to the present invention, since the stabilizing member provided in contact with the superconducting wire is divided into small rectangular shapes, it is possible to reduce the AC loss with respect to the magnetic field component in any direction. There is no risk of quenching the superconducting wire, and it does not increase the cooling load.
A superconducting conductor capable of realizing an efficient superconducting coil system can be provided.
【図1】本発明の一実施例に係る超伝導導体の構成を示
す断面図。FIG. 1 is a sectional view showing a configuration of a superconducting conductor according to an embodiment of the present invention.
【図2】従来の超伝導導体の断面図。FIG. 2 is a cross-sectional view of a conventional superconducting conductor.
【図3】従来の安定化部材の多層化をはかった超伝導導
体の一例の断面図。FIG. 3 is a cross-sectional view of an example of a conventional superconducting conductor in which a stabilizing member is multilayered.
【符号の説明】 1…超伝導線材 2…構造部材 3絶縁部材 10安定化部材 11絶縁被覆[Explanation of Codes] 1 ... Superconducting wire 2 ... Structural member 3 Insulating member 10 Stabilizing member 11 Insulating coating
Claims (1)
が、小さな矩形状に区切られており、かつその表面を、
比較的電気抵抗の高い材料で覆われていることを特徴と
する超伝導導体。1. A stabilizing member provided in contact with a superconducting wire is divided into small rectangular shapes, and the surface thereof is
A superconducting conductor characterized by being covered with a material having a relatively high electric resistance.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4323866A JPH06176632A (en) | 1992-12-03 | 1992-12-03 | Superconductor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4323866A JPH06176632A (en) | 1992-12-03 | 1992-12-03 | Superconductor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH06176632A true JPH06176632A (en) | 1994-06-24 |
Family
ID=18159472
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4323866A Withdrawn JPH06176632A (en) | 1992-12-03 | 1992-12-03 | Superconductor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH06176632A (en) |
-
1992
- 1992-12-03 JP JP4323866A patent/JPH06176632A/en not_active Withdrawn
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
A300 | Withdrawal of application because of no request for examination |
Free format text: JAPANESE INTERMEDIATE CODE: A300 Effective date: 20000307 |