JPS60147656A - Superconductor capable of detecting superconduction breakdown - Google Patents

Superconductor capable of detecting superconduction breakdown

Info

Publication number
JPS60147656A
JPS60147656A JP59005062A JP506284A JPS60147656A JP S60147656 A JPS60147656 A JP S60147656A JP 59005062 A JP59005062 A JP 59005062A JP 506284 A JP506284 A JP 506284A JP S60147656 A JPS60147656 A JP S60147656A
Authority
JP
Japan
Prior art keywords
superconducting
breakdown
superconduction
superconductive
detecting
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
Application number
JP59005062A
Other languages
Japanese (ja)
Inventor
Takashi Yasukochi
安河内 昂
Masatami Iwamoto
岩本 雅民
Katsuyoshi Toyoda
豊田 勝義
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP59005062A priority Critical patent/JPS60147656A/en
Publication of JPS60147656A publication Critical patent/JPS60147656A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N60/00Superconducting devices
    • H10N60/20Permanent superconducting devices

Landscapes

  • Measurement Of Resistance Or Impedance (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)
  • Superconductive Dynamoelectric Machines (AREA)

Abstract

PURPOSE:To detect surely superconduction breakdown even in case of a large- sized superconductive coil by inserting one superconduction breakdown detecting superconductive stand, which is not subjected to stabilizing treatment, at least to one primary stranded wire. CONSTITUTION:A superconduction breakdown detecting superconductive strand 9 which is not subjected to stabilizing treatment is inserted into the stranded wire where 3 superconductive strands 8 subjected to stabilizing treatment with a metal such as copper or the like are stranded, and this stranded wire is convered together with bundled conductors 11, where primary stranded wires 10 are stranded, with a casing 12 for airtightness or reinforcing, and a very low- temperature cooling medium for cooling is filled up in gaps of bundled conductors 11, thus constituting a superconductor 2. A current approximating the transition current value is flowed to the superconductive strand 9. If superconduction breakdown is caused in a part of the primary stranded wires 10, the cooling medium around the superconductive strand 9 is gasified, and the superconductive strand 9 causes superconduction breakdown to generate a large voltage, and it is detected by a superconduction breakdown detector 3.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は、超電導破壊を感度良(検出できる新規な超
電導4体に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] This invention relates to four novel superconductors that can detect superconductor breakdown with high sensitivity.

〔従来技術〕[Prior art]

従来、超電導コイルの超電導破壊を検出する装置として
第1図に示すものがあった。図において、lは超電導コ
イルであり、超電導々体コをコイル状に巻いて作られる
。3は超電導破壊検出器であり、その端子3aおよび3
bが超電導コイルlの電流入出力部に取り付けられグは
超電導破壊検出器3によって作動される遮断器であり、
Sは超電導コイルlの両端間に接続された保護抵抗であ
り、そして乙は ”’ 4電源である。
Conventionally, there has been a device shown in FIG. 1 as a device for detecting superconducting breakdown in superconducting coils. In the figure, l is a superconducting coil, which is made by winding a superconducting conductor into a coil shape. 3 is a superconducting breakdown detector, and its terminals 3a and 3
b is a circuit breaker attached to the current input/output part of the superconducting coil l, and g is a circuit breaker operated by the superconducting breakdown detector 3;
S is a protective resistor connected between both ends of the superconducting coil l, and B is a power source.

次に動作について説明する。超電導コイル/の電流入出
力部に取り付けられた端子3a、3b間には、超電導々
体コが超電導状態を保っている限り、定常状態では電圧
が!検出されない。しかし、超電導々体コの一部が超電
導破壊を起して常電導状態に転移すると、常電導部に抵
抗が生じるので端子3a、Jb間に電圧が発生する。こ
の電圧を超電導破壊検出器3で検出し、遮断器ダを開い
て電源6と超電導コイル/間の回路を遮断する。そのた
めに超電導コイル/に流れていた電流は、保護抵抗6を
流れることにより減衰する。
Next, the operation will be explained. As long as the superconducting conductor maintains its superconducting state, there is a voltage between the terminals 3a and 3b attached to the current input/output part of the superconducting coil in a steady state! Not detected. However, when a part of the superconducting conductor undergoes superconductivity breakdown and transitions to a normal conducting state, resistance is generated in the normal conducting part, so that a voltage is generated between the terminals 3a and Jb. This voltage is detected by the superconducting breakdown detector 3, and the circuit breaker is opened to interrupt the circuit between the power source 6 and the superconducting coil. Therefore, the current flowing through the superconducting coil is attenuated by flowing through the protective resistor 6.

なお、超電導破壊検出器3は、超電導破壊電圧とノイズ
を区別するため、例えば/ mVの信号がlOミリ秒以
上続いた場合に超電導破壊と判断するように設定されて
いる。
In order to distinguish between superconducting breakdown voltage and noise, the superconducting breakdown detector 3 is set to determine that superconducting breakdown has occurred, for example, when a signal of /mV continues for 10 milliseconds or more.

従来の超電導破壊検出装置は以上のように構成されてい
るので、大型の超電導コイルの場合には下記のように誤
動作するという欠点があった。
Since the conventional superconducting breakdown detection device is configured as described above, it has the disadvantage of malfunctioning as described below when using a large superconducting coil.

(1)超電導コイルのインダクタシスL=70ヘンリー
、電源リップル率(ΔI /sec ) −= 、 O
−eアンペッツ秒とすると、lOミリ秒の間に端子間電
圧Δt O,Oi の電圧が発生し、誤動作する。
(1) Inductance L of superconducting coil = 70 Henry, power supply ripple rate (ΔI/sec) −=, O
-e ampet seconds, an inter-terminal voltage Δt O,Oi is generated for 10 milliseconds, resulting in malfunction.

(2)超電導コイルの磁場がSテスラの部分で超区尋々
体が電磁力によりioミリ秒の間に/mの長さに渡って
一μm移動したとすると、端子間には、やはり/ mV
の電圧が発生し、(1)と同様、誤動作する。
(2) If the magnetic field of the superconducting coil is S tesla and the superconductor is moved by 1 μm over a length of /m in io milliseconds due to electromagnetic force, then there is also /m between the terminals. mV
voltage is generated, and as in (1), malfunction occurs.

〔発明の概要〕[Summary of the invention]

この発明は、上記のような従来のもの〜欠点を除去する
ためになされたもので、1次撚線内に少な(とも7本の
超電導破壊検出用超電導素線を挿入したので、大型の超
電導コイルに於ても、確実に超電導破壊を検出できる超
電導4体を提供することを目的としている。
This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and because a small number (7 in total) of superconducting strands for detecting superconducting breakdown were inserted into the primary stranded wire, large-sized superconducting The purpose of this invention is to provide four superconducting bodies that can reliably detect superconducting breakdown even in coils.

〔発明の実施例〕[Embodiments of the invention]

以下、この発明の一実施例を図について説明する。第一
図において、コは超電導4体、gは銅などの金属で安定
化処理を施した超電導素線、ワは安定化処理を施してな
い超電導破壊検出用超電導素線であり、10は安定化処
理を施した超亀辱素mgを3本撚り台上た/本撚腺、l
/は7次撚線10を何本か束状に撚り合せた束状導体、
/、2は束状導体/lの周囲を気密又は補強のために囲
ったケーシングである。13は束状導体//の間隙であ
り、冷却用の極低温冷媒が満されている。
An embodiment of the present invention will be described below with reference to the drawings. In Figure 1, C indicates four superconducting bodies, g indicates a superconducting strand stabilized with a metal such as copper, W indicates a superconducting strand for detecting superconducting breakdown that has not been stabilized, and 10 indicates a stable superconducting strand. 3 strands of ultra-transparent mg treated with oxidation treatment were placed on a twisting table/this twisted gland, l
/ is a bundled conductor made by twisting several 7th order stranded wires into a bundle,
/, 2 is a casing surrounding the bundled conductor /l for airtightness or reinforcement. 13 is a gap between the bundled conductors //, and is filled with a cryogenic refrigerant for cooling.

第3図は、第2図のうち、超電導破壊検出用超電4素i
?を含んだ1次撚線10のみを示す。
Figure 3 shows the four superconducting elements i for superconducting breakdown detection in Figure 2.
? Only the primary stranded wire 10 containing .

以上のように構成されたこの発明において、超電導検出
用超電導素線デには臨界電流値に近い電流を流しておく
。ここで、1次撚線10の極く一部例えは第3図の斜腺
部が超電導破壊を起したとすると、超電導々体全体とし
ては電圧が検出されないが、超電導破壊検出用超電導素
線りの囲りの冷媒はガス化しかつ超電導破壊検出用超電
導素線りが安定化されていないため、超電導破壊検出用
超電導素線デは直ちに超電導破壊を引き起し、大きな電
圧が発生ずる。従って、この電圧を第1図に示した超電
導破壊検出器3で検知する事により超電導破壊をその初
期状態から確実に検出できるなお、上記実施例では、第
3図のように、7本の超電導破壊検出用超電導素線デを
1次撚線/θ内に挿入した場合について示したが、第q
図のようにコ本の超電導破壊検出用超電導素線9aおよ
び9bの各々を折り返し形で挿入すると、励磁・減磁の
時にも訪導起電力を生ずる事がない。又、第3−図のよ
うに中間に多数のリード線/4’a、/!bおよび/’
Icを着けると、超電導破壊位置も検出する事ができる
。上記第を図、第S図では、簡単のため3本の超電導素
線ざから成る1次撚線10を2本の平行線で代表して示
しである。
In the present invention configured as described above, a current close to a critical current value is caused to flow through the superconducting element wire for superconductivity detection. Here, if a superconducting breakdown occurs in a very small part of the primary stranded wire 10 (for example, the oblique part in FIG. Since the refrigerant surrounding the refrigerant gasifies and the superconducting strands for detecting superconducting breakdown are not stabilized, the superconducting strands for detecting superconducting breakdown immediately cause superconducting breakdown and a large voltage is generated. Therefore, by detecting this voltage with the superconducting breakdown detector 3 shown in Fig. 1, superconducting breakdown can be reliably detected from its initial state. The case where the superconducting wire for destruction detection is inserted into the primary stranded wire /θ has been shown, but the qth
If each of the superconducting strands 9a and 9b for detecting superconducting breakdown is inserted in a folded manner as shown in the figure, no stray electromotive force will be generated even during excitation and demagnetization. Also, as shown in Figure 3, there are many lead wires /4'a, /! in the middle. b and /'
By wearing an Ic, it is also possible to detect the location of superconducting breakdown. In the above-mentioned figures No. 1 and S, for simplicity, the primary stranded wire 10 consisting of three superconducting strands is represented by two parallel lines.

第3図の実施例はケーシング内外内に冷媒を封入する場
合を想定したものである。しかしながら、第6図のよう
に連通口/3を設りた場合、ケーシング/Jは単に補強
のみの機能を有し、ケーシング内外に同一冷媒が満され
、相互に連通している、〔先明の効果〕 以上のように、この発明では1次撚線内に超電導破壊検
出用超電導素線を挿入した〜め、大型の超亀寺コイルに
於ても、確実に、積置よ(、超電導破壊を検出すること
が可能になった。
The embodiment shown in FIG. 3 is based on the assumption that a refrigerant is sealed inside and outside the casing. However, when the communication port /3 is provided as shown in Fig. 6, the casing /J has only a reinforcing function, and the inside and outside of the casing are filled with the same refrigerant and are in communication with each other. [Effects] As described above, in this invention, superconducting strands for detecting superconducting destruction are inserted into the primary stranded wires. Destruction can now be detected.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の超電導破壊検出装置を示す図、は他の実
施例を示す斜視図である。 lは超電導コイル、コは超電導4体、3は超電導破壊検
出器、3aと3bは端子、りは遮断器、左は保護抵抗、
乙は電諒、gは安定化処理を施した超電導素線、りは超
電導破壊検出用超電導素線、lθは1次撚線、//は束
状導体、12はケーシング、/3は冷媒充填用間隙、/
4’はリード線、/Sは連辿口である。なお、図中、同
一符号は同−又は相当部分を示す。 代理人 大 岩 増 雄 序1図 ス 艮 胆図 昂4図 昂5図
FIG. 1 is a diagram showing a conventional superconducting breakdown detection device, and FIG. 1 is a perspective view showing another embodiment. l is a superconducting coil, C is 4 superconductors, 3 is a superconducting breakdown detector, 3a and 3b are terminals, ri is a circuit breaker, left is a protective resistor,
O is a wire, g is a superconducting wire subjected to stabilization treatment, ri is a superconducting wire for superconducting breakdown detection, lθ is a primary stranded wire, // is a bundled conductor, 12 is a casing, /3 is a refrigerant filling Gap, /
4' is a lead wire, and /S is a continuous trace port. In addition, in the figures, the same reference numerals indicate the same or corresponding parts. Agent: Masu Oiwa Yuzu 1 figure Suuen Itu Gong 4 figure Kong 5 figure

Claims (1)

【特許請求の範囲】 (1)安定化処理を施した超電導素線を3本撚り合せて
1次撚線を作り、この1次撚線を何本か束状に撚り合せ
て作った束状導体をケーシング内に収容した超電導4体
において、1本の1次撚線内に、安定化処理を施してな
い少なくとも1本の超電導破壊検出用超電導素線を挿入
したことを特徴とする超電導破壊検出可能な超電導4体
。 (,2) i本の超電導破壊検出用超電導素線を7次撚
線の端から端まで挿入した特許請求の範囲第1項記載の
超電導4体。 (3) 2本の超電導破壊検出用超電導素線の各々を折
り返して1次撚線の各端から挿入した特許請求の範囲第
1項記載の超電導4体。 (リ 1本の超電導破壊検出用超電導素線の中間に多数
のリード線を着けた特許請求の範囲第2項記載の超電導
4体。
[Claims] (1) A bundle made by twisting three stabilized superconducting strands together to make a primary strand, and twisting several of these primary strands together into a bundle. A superconducting breakdown characterized in that in four superconducting bodies in which conductors are housed in a casing, at least one superconducting strand for detecting superconducting breakdown that has not been subjected to stabilization treatment is inserted into one primary stranded wire. Four detectable superconductors. (, 2) The superconductor 4 body according to claim 1, wherein i superconducting strands for superconducting breakdown detection are inserted from end to end of the seventh strand. (3) The four superconducting bodies according to claim 1, wherein each of the two superconducting strands for detecting superconducting breakdown is folded back and inserted from each end of the primary strand. (li) The superconductor 4 body according to claim 2, in which a large number of lead wires are attached to the middle of one superconducting element wire for detecting superconducting breakdown.
JP59005062A 1984-01-13 1984-01-13 Superconductor capable of detecting superconduction breakdown Pending JPS60147656A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59005062A JPS60147656A (en) 1984-01-13 1984-01-13 Superconductor capable of detecting superconduction breakdown

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59005062A JPS60147656A (en) 1984-01-13 1984-01-13 Superconductor capable of detecting superconduction breakdown

Publications (1)

Publication Number Publication Date
JPS60147656A true JPS60147656A (en) 1985-08-03

Family

ID=11600905

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59005062A Pending JPS60147656A (en) 1984-01-13 1984-01-13 Superconductor capable of detecting superconduction breakdown

Country Status (1)

Country Link
JP (1) JPS60147656A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2674671A1 (en) * 1991-03-28 1992-10-02 Alsthom Gec SUPERCONDUCTING CONDUCTOR HAVING IMPROVED PROTECTION AGAINST PARTIAL TRANSITIONS.

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2674671A1 (en) * 1991-03-28 1992-10-02 Alsthom Gec SUPERCONDUCTING CONDUCTOR HAVING IMPROVED PROTECTION AGAINST PARTIAL TRANSITIONS.

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