JPH05226707A - Current limiting conductor - Google Patents
Current limiting conductorInfo
- Publication number
- JPH05226707A JPH05226707A JP4029585A JP2958592A JPH05226707A JP H05226707 A JPH05226707 A JP H05226707A JP 4029585 A JP4029585 A JP 4029585A JP 2958592 A JP2958592 A JP 2958592A JP H05226707 A JPH05226707 A JP H05226707A
- Authority
- JP
- Japan
- Prior art keywords
- oxide superconductor
- current limiting
- current
- quenching
- superconductor
- 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
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)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
- Emergency Protection Circuit Devices (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は、超電導体を用いた短
絡電流などの過大電流を限流する限流器等に用いられる
限流導体に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a current limiting conductor used in a current limiting device for limiting an excessive current such as a short circuit current using a superconductor.
【0002】[0002]
【従来の技術】図10は例えば特開平2−281765
号公報に示された従来の酸化物超電導体を用いた限流素
子である。図において、1は基板、2は基板1上に配置
された酸化物超電導体であり、この例では、ドクターブ
レード法でシートに成形し、つづら折り状に打ち抜いて
作られたY系の酸化物超電導体である。また分かりやす
くするため網掛表示している。2aは酸化物超電導体2
の一方の折り返し部分、2bは酸化物超電導体2の他方
の折り返し部分、2cは中央部を示す。例えば、幅約
1.3mm、厚さ約0.9mmの断面の酸化物超電導体
を一辺の長さ約30mmで折り曲げた構造である。図1
1は図10をA方向からみた側面図である。2. Description of the Related Art FIG. 10 shows, for example, JP-A-2-281765.
It is a current limiting element using a conventional oxide superconductor disclosed in Japanese Patent Laid-Open Publication No. 2003-242242. In the figure, 1 is a substrate, and 2 is an oxide superconductor arranged on the substrate 1. In this example, a Y-based oxide superconductor formed by a doctor blade method into a sheet and punched into a zigzag shape. It is the body. In addition, the display is shaded for clarity. 2a is an oxide superconductor 2
One of the folded portions, 2b, is the other folded portion of the oxide superconductor 2, and 2c is the central portion. For example, it has a structure in which an oxide superconductor having a cross section with a width of about 1.3 mm and a thickness of about 0.9 mm is bent to have a side length of about 30 mm. Figure 1
FIG. 1 is a side view of FIG. 10 viewed from the direction A.
【0003】次に動作について説明する。酸化物超電導
体2が超電導状態にある定格電流を流す場合は、電流は
酸化物超電導体2を流れる。しかし、回路において短絡
事故などが起こり過大電流が流れると酸化物超電導体2
はクエンチして常電導体となり抵抗を有する。酸化物超
電導体2に発生した抵抗で電流が抑制され限流効果を示
す。Next, the operation will be described. When the oxide superconductor 2 carries a rated current in a superconducting state, the current flows through the oxide superconductor 2. However, if a short circuit accident occurs in the circuit and an excessive current flows, the oxide superconductor 2
Quenches into a normal conductor and has resistance. The current generated is suppressed by the resistance generated in the oxide superconductor 2, and the current limiting effect is exhibited.
【0004】[0004]
【発明が解決しようとする課題】従来の限流導体は以上
のように構成されており断面積が全長に渡ってほぼ一定
であるが、臨界電流密度にはばらつきがある。そのため
酸化物超電導体2がクエンチするとき全長の一部分がク
エンチしてそこから全体に広がっていくため時間がかか
るという問題があった。また、入力エネルギーの度合い
によっては溶断の恐れもある。The conventional current limiting conductor is constructed as described above and its cross-sectional area is substantially constant over the entire length, but the critical current density varies. Therefore, when the oxide superconductor 2 is quenched, there is a problem that a part of the entire length of the oxide superconductor is quenched and spreads from there to the whole, which takes time. Further, there is a risk of fusing depending on the degree of input energy.
【0005】この発明は、係る問題を解決するためにな
されたもので、限流導体の局所的クエンチを抑えクエン
チ伝搬をよくするとともに溶断を防止できる限流導体を
得ることを目的とする。The present invention has been made to solve the above problems, and an object of the present invention is to obtain a current limiting conductor capable of suppressing local quenching of the current limiting conductor, improving quench propagation, and preventing fusing.
【0006】[0006]
【課題を解決するための手段】この発明における限流導
体は、つづら折り状に形成された超電導体の厚みおよび
幅の少なくとも一方を他の部分より小さくした箇所を複
数箇所有するものである。The current-limiting conductor according to the present invention has a plurality of locations in which at least one of the thickness and the width of the superconductor formed in a zigzag shape is smaller than the other portions.
【0007】[0007]
【作用】この発明における限流導体は、つづら折り状に
形成された超電導体の少なくとも一部の厚みまたは幅を
他の部分より小さくし断面積を小さくした箇所を複数箇
所有するため、臨界電流値が他の部分より小さくなり、
この部分からクエンチが起こり素早く超電導体全体へク
エンチが伝搬する。また、局所的なクエンチが抑えられ
溶断も防止される。The current-limiting conductor according to the present invention has a plurality of places where the thickness or width of at least a part of the superconductor formed in a zigzag shape is made smaller than the other parts and the cross-sectional area is made smaller. Smaller than other parts,
Quenching occurs from this portion, and the quenching propagates quickly to the entire superconductor. In addition, local quenching is suppressed and fusing is also prevented.
【0008】[0008]
【実施例】実施例1.図1に図10のA方向から見たこ
の発明の一実施例による限流導体の側面図を示す。図に
おいて、1は基板、2は基板1上につづら折り状に配置
された酸化物超電導体、2aは酸化物超電導体2の一方
の折り返し部分、2bは酸化物超電導体2の他方の折り
返し部分で、2cは中央部を示す。この例では、折り返
し部分2a,2bは、中央部2cより厚みが薄い。EXAMPLES Example 1. FIG. 1 shows a side view of a current limiting conductor according to an embodiment of the present invention viewed from the direction A in FIG. In the figure, 1 is a substrate, 2 is an oxide superconductor arranged in a zigzag shape on the substrate 1, 2a is one folded portion of the oxide superconductor 2, and 2b is the other folded portion of the oxide superconductor 2. 2c shows the central part. In this example, the folded-back portions 2a and 2b are thinner than the central portion 2c.
【0009】次に動作について説明する。酸化物超電導
体2が超電導状態にある定格電流を流す場合は、電流は
酸化物超電導体2を流れる。しかし、回路において短絡
事故などが起こり過大電流が流れると酸化物超電導体2
はクエンチして常電導体となり抵抗を有する。酸化物超
電導体2に発生した抵抗で電流が抑制され限流効果を示
す。このときクエンチは中央部2cより厚みが薄い折り
返し部分2a,2bで起こり、この両端の折り返し部分
2a,2bから中央部2cに向かって伝搬する。したが
ってクエンチが全体に素早く広がるとともに局所的クエ
ンチが抑えられる。Next, the operation will be described. When the oxide superconductor 2 carries a rated current in a superconducting state, the current flows through the oxide superconductor 2. However, if a short circuit accident occurs in the circuit and an excessive current flows, the oxide superconductor 2
Quenches into a normal conductor and has resistance. The current generated is suppressed by the resistance generated in the oxide superconductor 2, and the current limiting effect is exhibited. At this time, quenching occurs in the folded-back portions 2a and 2b which are thinner than the central portion 2c, and propagates from the folded-back portions 2a and 2b at both ends toward the central portion 2c. Therefore, the quench quickly spreads throughout and the local quench is suppressed.
【0010】図2から図4に他の実施例を示す。これら
の図に示すように中央部2cより厚みが薄い折り返し部
分2a,2bを有するならば実施例1と同様の効果が得
られる。2 to 4 show another embodiment. As shown in these figures, if the folded portions 2a and 2b are thinner than the central portion 2c, the same effect as that of the first embodiment can be obtained.
【0011】また、上記各実施例では折り返し部分2
a,2bの両方が中央部2cより厚みが薄い形状になっ
ていたが折り返し部分2a,2bのいずれか一方だけで
もよい。さらに、全列に厚みが薄い部分を設けなくても
1列おき等であってもよい。Further, in each of the above embodiments, the folded-back portion 2
Although both a and 2b are thinner than the central portion 2c, only one of the folded portions 2a and 2b may be used. Furthermore, it is also possible to provide every other row without providing a thin portion in all rows.
【0012】なお、上記各実施例では共に折り返し部分
2a,2bの厚みを薄くする場合について示したが、図
5に示すように、中央部2cの厚みを他の部分より薄く
してもよい。In each of the above embodiments, the thickness of the folded portions 2a, 2b is shown to be thin, but the central portion 2c may be thinner than the other portions as shown in FIG.
【0013】実施例2.図6にこの発明の第二の実施例
による限流導体を示す。図において、1は基板、2は基
板1上に配置された酸化物超電導体、2aは酸化物超電
導体2の一方の折り返し部分、2bは酸化物超電導体2
の他方の折り返し部分で、2cは中央部を示す。この例
では折り返し部分2a,2bは、中央部2cより幅が狭
い。Embodiment 2. FIG. 6 shows a current limiting conductor according to a second embodiment of the present invention. In the figure, 1 is a substrate, 2 is an oxide superconductor arranged on the substrate 1, 2a is one folded portion of the oxide superconductor 2, and 2b is an oxide superconductor 2.
In the other folded-back portion, 2c indicates the central portion. In this example, the folded-back portions 2a and 2b are narrower than the central portion 2c.
【0014】次に動作について説明する。酸化物超電導
体2が超電導状態にある定格電流を流す場合は、電流は
酸化物超電導体2を流れる。しかし、回路において短絡
事故などが起こり過大電流が流れると酸化物超電導体2
はクエンチして常電導体となり抵抗を有する。酸化物超
電導体2に発生した抵抗で電流が抑制され限流効果を示
す。このときクエンチは中央部2cより幅の狭い折り返
し部分2a,2bで起こり、この両端の折り返し部分2
a,2bから中央部2cに向かって伝搬する。したがっ
てクエンチが全体に素早く広がるとともに局所的クエン
チが抑えられ溶断を防止できる。Next, the operation will be described. When the oxide superconductor 2 carries a rated current in a superconducting state, the current flows through the oxide superconductor 2. However, if a short circuit accident occurs in the circuit and an excessive current flows, the oxide superconductor 2
Quenches into a normal conductor and has resistance. The current generated is suppressed by the resistance generated in the oxide superconductor 2, and the current limiting effect is exhibited. At this time, the quench occurs at the folded portions 2a and 2b which are narrower than the central portion 2c, and the folded portions 2 at both ends are
Propagate from a, 2b toward the central portion 2c. Therefore, quenching spreads quickly to the whole, local quenching is suppressed, and fusing can be prevented.
【0015】図7、図8に他の実施例を示す。図7は中
央部2cから折り返し部分2a,2bに少し近づいたと
ころから徐々に幅を狭くした構造になっている。図8は
中央部2cから折り返し部分2a,2bに向かって徐々
に幅を狭くした構造になっている。何れも図6に示す実
施例2と同様の効果が得られる。Another embodiment is shown in FIGS. FIG. 7 shows a structure in which the width is gradually narrowed from a position slightly closer to the folded-back portions 2a and 2b from the central portion 2c. FIG. 8 shows a structure in which the width is gradually reduced from the central portion 2c toward the folded-back portions 2a and 2b. In any case, the same effect as that of the second embodiment shown in FIG. 6 can be obtained.
【0016】なお、上記各実施例では両方の折り返し部
分2a,2bの幅を狭くした構造になっていたが、折り
返し部分2a,2bのいずれか一方だけでもよい。さら
に、全列に設けなくて1列おき等であってもよい。In each of the above embodiments, the width of both of the folded back portions 2a and 2b is narrowed, but only one of the folded back portions 2a and 2b may be used. Further, it may not be provided in all the rows and may be arranged every other row.
【0017】また、上記各実施例では共に折り返し部分
2a,2bの幅を狭くする場合について示したが、図9
に示すように、中央部2cの幅を他の部分より狭くして
もよい。In each of the above embodiments, the width of the folded portions 2a and 2b is narrowed, but FIG.
As shown in, the width of the central portion 2c may be narrower than the other portions.
【0018】なお、上記図1から図9に示す各実施例で
は超電導体2の厚みおよび幅の一方を他の部分より小さ
くした場合について示したが、厚みおよび幅の両方を小
さくしてもよい。In each of the embodiments shown in FIGS. 1 to 9 described above, one of the thickness and the width of the superconductor 2 is made smaller than the other portion, but both the thickness and the width may be made smaller. ..
【0019】さらに、上記各実施例ではドクターブレー
ド法で作られたシート状の酸化物超電導体を用いた場合
について説明を行ったが、バルク材でもよく、またはP
VD法、CVD法、スパッタ法、電着法などで作られた
薄膜などでもよい。Further, in each of the above embodiments, the case where the sheet-shaped oxide superconductor made by the doctor blade method is used is explained, but a bulk material may be used, or P
A thin film formed by a VD method, a CVD method, a sputtering method, an electrodeposition method or the like may be used.
【0020】[0020]
【発明の効果】以上のように、この発明によれば、つづ
ら折り状に形成された超電導体の厚みおよび幅の少なく
とも一方を他の部分より小さくした箇所を複数箇所有す
るので、臨界電流値が他の部分より小さい箇所が複数箇
所できることとなり、これらの部分からクエンチが起こ
り素早く超電導体全体へクエンチが伝搬する。また、局
所的なクエンチが抑えられ溶断も防止される。As described above, according to the present invention, since there are a plurality of places where at least one of the thickness and the width of the superconductor formed in a zigzag shape is smaller than the other portions, the critical current value is different. A plurality of places smaller than the portion of will be formed, and quenching will occur from these portions and the quenching will propagate quickly to the entire superconductor. In addition, local quenching is suppressed and fusing is also prevented.
【図1】この発明の実施例1による限流導体を示す側面
図である。FIG. 1 is a side view showing a current limiting conductor according to a first embodiment of the present invention.
【図2】この発明の他の実施例による限流導体を示す側
面図である。FIG. 2 is a side view showing a current limiting conductor according to another embodiment of the present invention.
【図3】この発明の他の実施例による限流導体を示す側
面図である。FIG. 3 is a side view showing a current limiting conductor according to another embodiment of the present invention.
【図4】この発明の他の実施例による限流導体を示す側
面図である。FIG. 4 is a side view showing a current limiting conductor according to another embodiment of the present invention.
【図5】この発明の他の実施例による限流導体を示す側
面図である。FIG. 5 is a side view showing a current limiting conductor according to another embodiment of the present invention.
【図6】この発明の実施例2による限流導体を示す上面
図である。FIG. 6 is a top view showing a current limiting conductor according to a second embodiment of the present invention.
【図7】この発明の他の実施例による限流導体を示す上
面図である。FIG. 7 is a top view showing a current limiting conductor according to another embodiment of the present invention.
【図8】この発明の他の実施例による限流導体を示す上
面図である。FIG. 8 is a top view showing a current limiting conductor according to another embodiment of the present invention.
【図9】この発明の他の実施例による限流導体を示す上
面図である。FIG. 9 is a top view showing a current limiting conductor according to another embodiment of the present invention.
【図10】従来の限流導体を示す上面図である。FIG. 10 is a top view showing a conventional current limiting conductor.
【図11】従来の限流導体を示す側面図である。FIG. 11 is a side view showing a conventional current limiting conductor.
1 基板 2 酸化物超電導体 2a 一方の折り返し部分 2b 他方の折り返し部分 2c 中央部 1 Substrate 2 Oxide superconductor 2a One folded portion 2b Other folded portion 2c Central part
───────────────────────────────────────────────────── フロントページの続き (72)発明者 松野 繁 尼崎市塚口本町8丁目1番1号 三菱電機 株式会社材料デバイス研究所内 (72)発明者 木ノ内 伸一 尼崎市塚口本町8丁目1番1号 三菱電機 株式会社材料デバイス研究所内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Shigeru Matsuno 8-1-1 Tsukaguchihonmachi, Amagasaki City Mitsubishi Electric Corporation Material Devices Research Center (72) Inventor Shinichi Kinouchi 8-1-1 Tsukaguchihonmachi, Amagasaki Mitsubishi Electric Devices Co., Ltd. Material Device Research Center
Claims (1)
みおよび幅の少なくとも一方を他の部分より小さくした
箇所を複数箇所有することを特徴とする限流導体。1. A current limiting conductor having a plurality of locations in which at least one of the thickness and the width of a superconductor formed in a zigzag shape is smaller than other portions.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4029585A JPH05226707A (en) | 1992-02-17 | 1992-02-17 | Current limiting conductor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4029585A JPH05226707A (en) | 1992-02-17 | 1992-02-17 | Current limiting conductor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH05226707A true JPH05226707A (en) | 1993-09-03 |
Family
ID=12280156
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4029585A Pending JPH05226707A (en) | 1992-02-17 | 1992-02-17 | Current limiting conductor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH05226707A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5828078A (en) * | 1995-07-24 | 1998-10-27 | Hughes Electronics | Electrostatic discharge protection using high temperature superconductors |
EP1309014A1 (en) * | 2001-10-31 | 2003-05-07 | Abb Research Ltd. | Superconducting resistive current limiter |
EP2983218A1 (en) * | 2014-08-06 | 2016-02-10 | Karlsruher Institut für Technologie | Design of superconducting devices by optimization of the superconductor's local critical current |
-
1992
- 1992-02-17 JP JP4029585A patent/JPH05226707A/en active Pending
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5828078A (en) * | 1995-07-24 | 1998-10-27 | Hughes Electronics | Electrostatic discharge protection using high temperature superconductors |
EP1309014A1 (en) * | 2001-10-31 | 2003-05-07 | Abb Research Ltd. | Superconducting resistive current limiter |
US6900718B2 (en) | 2001-10-31 | 2005-05-31 | Abb Research Ltd | Resistive superconducting current limiter |
EP2983218A1 (en) * | 2014-08-06 | 2016-02-10 | Karlsruher Institut für Technologie | Design of superconducting devices by optimization of the superconductor's local critical current |
US10153071B2 (en) | 2014-08-06 | 2018-12-11 | Karlsruher Institut Fuer Technologie | Superconducting devices by optimization of the superconductor's local critical current |
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