JPS59218712A - Protective circuit for superconductive coil - Google Patents
Protective circuit for superconductive coilInfo
- Publication number
- JPS59218712A JPS59218712A JP9239183A JP9239183A JPS59218712A JP S59218712 A JPS59218712 A JP S59218712A JP 9239183 A JP9239183 A JP 9239183A JP 9239183 A JP9239183 A JP 9239183A JP S59218712 A JPS59218712 A JP S59218712A
- Authority
- JP
- Japan
- Prior art keywords
- resistor
- liquid nitrogen
- coil
- resistance value
- superconducting coil
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/003—Methods and means for discharging superconductive storage
Abstract
Description
【発明の詳細な説明】 〔発明の属する技術分野〕 この発明は、超電導コイルの保護回路に関する。[Detailed description of the invention] [Technical field to which the invention pertains] The present invention relates to a protection circuit for superconducting coils.
従来技術としての保護回路は、通常の抵抗器を用いるの
で、抵抗値はほとんど変化しない。このため、超電導コ
イルのエネルギ゛−をすみやかに放出しようとするとき
には、放電抵抗器の抵抗値を大きくすることが必要であ
る。このため、コイル電流を放電抵抗器へ移すときの発
生電圧が高くなる。そのため、コイル電流をしゃ断する
開閉器に高電圧の直流電流しゃ断能力が必要となる他、
電流しゃ断時の過渡電圧による絶縁破壊の恐れがあった
。Since the conventional protection circuit uses a normal resistor, the resistance value hardly changes. Therefore, when trying to quickly release the energy of the superconducting coil, it is necessary to increase the resistance value of the discharge resistor. Therefore, the voltage generated when transferring the coil current to the discharge resistor increases. Therefore, the switch that cuts off the coil current needs to have high voltage DC current cutting ability.
There was a risk of insulation breakdown due to transient voltage when the current was cut off.
この発明は、電流しゃ断時の、放電抵抗値を低くして、
電流しゃ断時の発生電圧を低く抑えるが、抵抗器が抵抗
自体の発熱で温度が上がると、抵抗値が大きくなり、す
みやかなエネルギー放出を可能ならしめる、保護回路を
提供することにある。This invention lowers the discharge resistance value when the current is cut off,
The purpose of the present invention is to provide a protection circuit that suppresses the voltage generated when current is cut off, but when the temperature of the resistor rises due to the heat generated by the resistor itself, the resistance value increases, making it possible to quickly release energy.
温度による抵抗変化の大きい、銅、アルミニウム等の金
属で抵抗器を構成し、電流を通電する以前は、液体窒素
で冷却しておき、抵抗の発熱で、液体窒素を蒸散でせる
ことにより、液体窒素から常温付近までの温度変化を実
現することで、抵抗器の抵抗値を大幅に変化させる。The resistor is made of a metal such as copper or aluminum, which has a large resistance change depending on temperature, and is cooled with liquid nitrogen before applying current.The heat generated by the resistor evaporates the liquid nitrogen. By achieving a temperature change from nitrogen to around room temperature, the resistance value of the resistor can be significantly changed.
抵抗器を液体窒素温度から、常温まで変化させることで
、比較的容易に、抵抗値を大幅に変化させることができ
る。By changing the temperature of the resistor from liquid nitrogen temperature to room temperature, the resistance value can be significantly changed relatively easily.
第1図は、この発明による、超電導コイルの保護回路で
ある。図において、1は超電導コイル、2はクライオス
タット、3は抵抗器、4は液体窒素容器、5はコイル電
流を抵抗器へ移すため、コイル電流をしゃ断する開閉器
、6は、コイルを励磁する電源である。第2図は、無酸
素鋼の温度と電気抵抗率の関係を表わしたものである。FIG. 1 shows a protection circuit for a superconducting coil according to the present invention. In the figure, 1 is a superconducting coil, 2 is a cryostat, 3 is a resistor, 4 is a liquid nitrogen container, 5 is a switch that cuts off the coil current in order to transfer the coil current to the resistor, and 6 is a power source that excites the coil. It is. FIG. 2 shows the relationship between temperature and electrical resistivity of oxygen-free steel.
図から読みとれるように、液体窒素温度(’77K)と
常温(300K)では、抵抗率はおよそ1桁変化する。As can be seen from the figure, the resistivity changes by approximately one order of magnitude between liquid nitrogen temperature ('77K) and room temperature (300K).
すなわち、常温の抵抗値に対して、初期抵抗値は約1割
であるため、コイル電流しゃ断時の発生電圧も、最終発
生電圧値に対して、約1割となる。That is, since the initial resistance value is about 10% of the resistance value at room temperature, the voltage generated when the coil current is cut off is also about 10% of the final generated voltage value.
このため、直流のしゃ断電圧が250V程度であるノー
ヒユーズしゃ断器を用いて、抵抗による発生電圧が10
00〜2000 Vとなる保護回路を構成することがで
きる。Therefore, by using a no-fuse breaker with a DC breaking voltage of about 250V, the voltage generated by the resistance can be reduced to 10V.
A protection circuit with a voltage of 00 to 2000 V can be constructed.
第3図は、この発明による、他の実施例である。 FIG. 3 shows another embodiment according to the invention.
7は通常の抵抗器で、液体窒素で冷却した抵抗器3と並
列にして用いる。このようにして用いると合成抵抗の抵
抗値の変化幅は小さくなるが、液体窒素冷却による抵抗
器への熱入力を少なくすることができ、全体として抵抗
器の構成が容易となる。7 is an ordinary resistor, which is used in parallel with resistor 3 cooled with liquid nitrogen. When used in this manner, the range of change in the resistance value of the combined resistor becomes smaller, but the heat input to the resistor due to liquid nitrogen cooling can be reduced, and the resistor structure as a whole becomes easier.
数値例を示すと次のようになる。通電電流1000A1
蓄積エネルギl MJの超電導コイルのエネルギーを最
大発生電圧1000Vで放出させるとき、合成抵抗値は
1Ω、である。通常抵抗器の抵抗値を1.5Ω、液体窒
素冷却の抵抗値を0.3Ωから3Ωまで変化きせるよう
にすると、初期の合成抵抗値は0.25Ωで、100O
Aの通電による発生電圧は、250Vとなるので、例え
ば、ノーヒユーズしゃ断器を用いてしゃ断することが可
能である。このときの液体窒素冷却抵抗器への熱負伺は
全体の1/3の333KJとなる。抵抗器は、銅で作る
ものとして、液体窒素温度から、loo′c″!、でn
′A度変化略せる場合の熱容量は、90 J/g 1し
たがって、3.7kgの材料が必要となる。常温におけ
る抵抗率を1.8X10’Ωmとして、3Ωとなるよう
にするには、断面積1.55+++ffl長ざ250m
となる。これは、直径1.45 mmのイ伺線を直径2
00間のコイル状に1往復無誘導巻きに巻くと長さ30
0団となる大きさである。A numerical example is shown below. Carrying current 1000A1
When the energy of a superconducting coil with stored energy l MJ is released at a maximum generated voltage of 1000 V, the combined resistance value is 1 Ω. If the resistance value of the normal resistor is 1.5Ω and the resistance value of the liquid nitrogen cooling is changed from 0.3Ω to 3Ω, the initial combined resistance value is 0.25Ω, which is 100Ω.
Since the voltage generated by energizing A is 250V, it is possible to break it off using, for example, a no-fuse breaker. The heat load on the liquid nitrogen cooling resistor at this time is 333 KJ, which is 1/3 of the total. Assuming that the resistor is made of copper, from the liquid nitrogen temperature, loo′c″!, n
The heat capacity when the A degree change can be omitted is 90 J/g 1. Therefore, 3.7 kg of material is required. Assuming that the resistivity at room temperature is 1.8X10'Ωm, to make it 3Ω, the cross-sectional area is 1.55+++ffl, and the length is 250m.
becomes. This means that a line with a diameter of 1.45 mm is made with a diameter of 2
When wound in a coil shape between 00 and 1 round trip with non-inductive winding, the length is 30
It is large enough to have 0 groups.
抵抗値の温度変化の大きなものとしては、白熱電球があ
り、タングステア線を真空中に封じ切って抵抗器とする
ことによっても同様な効果が得られる。An incandescent light bulb has a resistance value that changes significantly with temperature, and a similar effect can be obtained by sealing a tungsteer wire in a vacuum and using it as a resistor.
第1図にこの発明による超電導コイルの保護回路図、第
2図は、温度による抵抗率変化の例を示す特性図、第3
図は、この発明の他の実施例を示す超電導コイルの保護
回路図である。
1・・・超電導コイル 2・・・クライオスタット
3.7・・・抵抗器Fig. 1 is a protection circuit diagram of a superconducting coil according to the present invention, Fig. 2 is a characteristic diagram showing an example of resistivity change due to temperature, and Fig. 3 is a characteristic diagram showing an example of resistivity change due to temperature.
The figure is a protection circuit diagram of a superconducting coil showing another embodiment of the present invention. 1...Superconducting coil 2...Cryostat 3.7...Resistor
Claims (4)
ルと直列に接続してコイル電流を減少させる放電抵抗器
において、抵抗値の温度変化が大きい材料を用いること
を特徴とする超電導コイルの保護回路。(1) A protection circuit for a superconducting coil characterized by using a material whose resistance value changes greatly with temperature in a discharge resistor that is connected in series with the superconducting coil to reduce the coil current when the superconducting coil transitions to normal conductivity. .
特徴とする特許請求の範囲第1項記載の超電導コイルの
保護6回路。(2) The six superconducting coil protection circuits according to claim 1, wherein the discharge resistor is cooled with liquid nitrogen.
を並列に接続して構成したことを特徴とする特許請求の
範囲第1項記載の超電導コイルの保−回路。(3) The superconducting coil protection circuit according to claim 1, wherein the discharge resistor is constructed by connecting a resistor and a resistor cooled with liquid nitrogen in parallel.
に設置するタングステン線を並列に接続して構成したこ
とを特徴とする特許請求の範囲第1項記載の超電導コイ
ルの保護回路。(4) A protection circuit for a superconducting coil according to claim 1, wherein the discharge resistor is constructed by connecting the resistor and a tungsten wire placed in a vacuum or an inert gas in parallel.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9239183A JPS59218712A (en) | 1983-05-27 | 1983-05-27 | Protective circuit for superconductive coil |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9239183A JPS59218712A (en) | 1983-05-27 | 1983-05-27 | Protective circuit for superconductive coil |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59218712A true JPS59218712A (en) | 1984-12-10 |
JPH0554244B2 JPH0554244B2 (en) | 1993-08-12 |
Family
ID=14053115
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9239183A Granted JPS59218712A (en) | 1983-05-27 | 1983-05-27 | Protective circuit for superconductive coil |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59218712A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04136777A (en) * | 1990-09-28 | 1992-05-11 | Agency Of Ind Science & Technol | Squid element having resistance layer |
JPH0485706U (en) * | 1990-11-30 | 1992-07-24 | ||
CN114038640A (en) * | 2021-09-18 | 2022-02-11 | 盛雷城精密电阻(江西)有限公司 | Ultrahigh frequency radio frequency resistor and production method thereof |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS52104749A (en) * | 1976-02-28 | 1977-09-02 | Furukawa Electric Co Ltd | Holding device for superconductive electromagnet coil |
JPS5483390A (en) * | 1977-12-16 | 1979-07-03 | Toshiba Corp | Protective device for superconductive coil |
JPS54137658A (en) * | 1978-04-19 | 1979-10-25 | Hitachi Ltd | Energy remover for superconductive coil |
-
1983
- 1983-05-27 JP JP9239183A patent/JPS59218712A/en active Granted
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS52104749A (en) * | 1976-02-28 | 1977-09-02 | Furukawa Electric Co Ltd | Holding device for superconductive electromagnet coil |
JPS5483390A (en) * | 1977-12-16 | 1979-07-03 | Toshiba Corp | Protective device for superconductive coil |
JPS54137658A (en) * | 1978-04-19 | 1979-10-25 | Hitachi Ltd | Energy remover for superconductive coil |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH04136777A (en) * | 1990-09-28 | 1992-05-11 | Agency Of Ind Science & Technol | Squid element having resistance layer |
JPH0485706U (en) * | 1990-11-30 | 1992-07-24 | ||
CN114038640A (en) * | 2021-09-18 | 2022-02-11 | 盛雷城精密电阻(江西)有限公司 | Ultrahigh frequency radio frequency resistor and production method thereof |
CN114038640B (en) * | 2021-09-18 | 2023-05-23 | 盛雷城精密电阻(江西)有限公司 | Ultrahigh frequency radio frequency resistor and production method thereof |
Also Published As
Publication number | Publication date |
---|---|
JPH0554244B2 (en) | 1993-08-12 |
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