JP2016092152A - Protection device and method for protecting superconducting coil - Google Patents

Protection device and method for protecting superconducting coil Download PDF

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JP2016092152A
JP2016092152A JP2014223674A JP2014223674A JP2016092152A JP 2016092152 A JP2016092152 A JP 2016092152A JP 2014223674 A JP2014223674 A JP 2014223674A JP 2014223674 A JP2014223674 A JP 2014223674A JP 2016092152 A JP2016092152 A JP 2016092152A
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superconducting coil
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JP6486651B2 (en
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智則 渡部
Tomonori Watabe
智則 渡部
長屋 重夫
Shigeo Nagaya
重夫 長屋
敦士 石山
Atsushi Ishiyama
敦士 石山
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Chubu Electric Power Co Inc
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Abstract

PROBLEM TO BE SOLVED: To provide a protection device and a method for protecting a superconducting coil capable of simplifying the configuration, and capable of stopping the operation smoothly while protecting a superconducting coil at the time of normal conducting transition.SOLUTION: A single pancake coil 17 as a superconducting coil is formed by winding superconducting wires 11 without insulating therebetween, and a plurality of pickup coils 23, as magnetic field variation detection elements, are arranged in the vicinity of the inner peripheral part of the single pancake coil 17. An abnormality detection mechanism 27 interrupts a current supplied from a power supply 20 to the single pancake coil 17 by opening an on/off switch 22, when any pickup coil 23 detects magnetic field variation due to normal conducting transition.SELECTED DRAWING: Figure 1

Description

本発明は、例えば希土類系酸化物超電導体により形成された超電導線材を巻回してなる超電導コイルの使用時にクエンチ(常電導転移)等の異常が生じたとき、十分な保護機能を発揮しつつ、運転を停止することができる超電導コイルの保護装置及び保護方法に関する。   In the present invention, for example, when an abnormality such as quench (normal conduction transition) occurs when using a superconducting coil formed by winding a superconducting wire formed of a rare earth oxide superconductor, while exhibiting a sufficient protection function, The present invention relates to a protection device and a protection method for a superconducting coil capable of stopping operation.

一般に、希土類系酸化物超電導体による超電導線材を用いた超電導コイルにおいては、使用時にクエンチ等の異常が発生してもその異常状態が周囲に拡大し難いことから異常検出が困難で、異常検出までに局部的に高温部(ヒートスポット)が生じ、超電導コイルの特性が低下する。この超電導線材として例えば、基板上に中間層を介して希土類系酸化物超電導体による超電導層が形成され、その超電導層上に銀等の保護層を介して銅等による安定化層が形成されたものが知られている。そして、常電導転移が生じたとき、超電導層から安定化層にも電流が流れるようにすることで発熱を抑え、超電導線材の損傷を防止することが考えられる。   In general, in superconducting coils using superconducting wires made of rare earth oxide superconductors, even if an abnormality such as a quench occurs during use, it is difficult to detect the abnormality, so it is difficult to detect the abnormality. Therefore, a high temperature part (heat spot) is locally generated and the characteristics of the superconducting coil are deteriorated. As this superconducting wire, for example, a superconducting layer made of a rare earth oxide superconductor is formed on a substrate via an intermediate layer, and a stabilizing layer made of copper or the like is formed on the superconducting layer via a protective layer such as silver. Things are known. When normal conduction transition occurs, it can be considered that current is caused to flow from the superconducting layer to the stabilizing layer, thereby suppressing heat generation and preventing damage to the superconducting wire.

しかしながら、超電導コイルには電力が貯蔵されていることから、異常発生時には迅速に通電を停止するとともに、貯蔵電力を消費することが必要である。このため、超電導コイルには別途保護回路を設け、異常時にはその保護回路に電流を誘導し、保護回路中の抵抗負荷により超電導コイルの貯蔵電力を消費し、運転を停止するようになっている。   However, since electric power is stored in the superconducting coil, it is necessary to quickly stop energization and consume the stored electric power when an abnormality occurs. For this reason, a separate protection circuit is provided for the superconducting coil. When an abnormality occurs, a current is induced in the protection circuit, and the stored power of the superconducting coil is consumed by the resistive load in the protection circuit, and the operation is stopped.

この種の超電導コイル装置が、例えば特許文献1に記載されている。この超電導コイル装置は、超電導コイルが常電導転移したときにそのエネルギー(貯蔵電力)を消費するための保護回路と、超電導コイルに並列に接続され、前記保護回路とは別個の抵抗とを備えた装置である。そして、超電導コイルが常電導転移したとき、超電導コイルのもつエネルギーを保護回路で消費するとともに、保護回路とは別個の抵抗でエネルギーを消費して常電導転移部の拡散を図るようになっている。   This type of superconducting coil device is described in Patent Document 1, for example. This superconducting coil device includes a protection circuit for consuming energy (stored power) when the superconducting coil is in a normal conduction transition, and a resistance connected to the superconducting coil in parallel and separate from the protection circuit. Device. And, when the superconducting coil makes a normal conducting transition, the energy of the superconducting coil is consumed by the protection circuit, and the energy is consumed by a resistance different from the protection circuit to diffuse the normal conducting transition part. .

特開平5−67524号公報JP-A-5-67524

前述した特許文献1に記載されている従来構成の超電導コイル装置においては、超電導コイルとは別に超電導コイルのもつ貯蔵電力を消費する保護回路を設けなければならず、またその保護回路には超電導コイルのインダクタンスに見合う抵抗を設定し、超電導コイルに接続しなければならない。そのため、超電導コイル装置の部品点数が多くなるとともに、構成が複雑になるという欠点があった。   In the conventional superconducting coil device described in Patent Document 1 described above, a protection circuit that consumes stored power of the superconducting coil must be provided separately from the superconducting coil, and the protection circuit includes a superconducting coil. A resistance that matches the inductance of the superconducting coil must be set. For this reason, there are disadvantages that the number of parts of the superconducting coil device increases and the configuration becomes complicated.

さらに、この超電導コイル装置では、保護回路とは別の抵抗で発生する電圧を検出し、超電導コイルと電源との間に設けられた開閉スイッチを開いて超電導コイルへの通電を遮断するように構成されている。この抵抗に発生する電圧変動は、常電導転移による異常が微小である場合には非常に小さく、電圧変動の検出がノイズの影響を受けやすく、検出精度が低いという問題もあった。   Furthermore, this superconducting coil device is configured to detect a voltage generated by a resistance different from that of the protection circuit, and to open the open / close switch provided between the superconducting coil and the power source to cut off the energization to the superconducting coil. Has been. The voltage fluctuation generated in the resistor is very small when the abnormality due to the normal conduction transition is very small, and there is a problem that detection of the voltage fluctuation is easily affected by noise and detection accuracy is low.

そこで、本発明の目的とするところは、構成を簡易にでき、常電導転移時に超電導コイルを保護しながら円滑に運転を停止することができる超電導コイルの保護装置及び保護方法を提供することにある。   Therefore, an object of the present invention is to provide a protection device and a protection method for a superconducting coil that can be simplified in configuration and can be smoothly stopped while protecting the superconducting coil at the time of normal conduction transition. .

上記の目的を達成するために、請求項1に記載の発明の超電導コイルの保護装置は、超電導線材をコイル状に巻回するとともに、前記超電導線材の両端部に電極を取付け、両電極間に電源を接続して通電するようにした超電導コイルであって、前記超電導コイルは超電導線材間を絶縁することなく巻回して形成されるとともに、超電導コイルにはその磁界が及ぶ範囲に磁界変動検出素子を備え、該磁界変動検出素子が磁界変動を検出したとき電源から供給される電流を遮断する異常検出機構を備えたものである。   In order to achieve the above object, the superconducting coil protection device according to the first aspect of the present invention winds a superconducting wire in a coil shape, attaches electrodes to both ends of the superconducting wire, and A superconducting coil connected to a power source and energized, wherein the superconducting coil is formed without being wound between the superconducting wires, and the superconducting coil has a magnetic field fluctuation detecting element in a range covered by the magnetic field. And an abnormality detection mechanism for cutting off the current supplied from the power supply when the magnetic field fluctuation detection element detects a magnetic field fluctuation.

請求項2に記載の発明の超電導コイルの保護装置は、請求項1に係る発明において、前記磁界変動検出素子はピックアップコイルである。
請求項3に記載の発明の超電導コイルの保護装置は、請求項1又は請求項2に係る発明において、前記磁界変動検出素子は、超電導コイルの内周部に配置されている。
A superconducting coil protection device according to a second aspect of the present invention is the superconducting coil protection device according to the first aspect, wherein the magnetic field fluctuation detecting element is a pickup coil.
A protection device for a superconducting coil according to a third aspect of the present invention is the invention according to the first or second aspect, wherein the magnetic field fluctuation detecting element is disposed on an inner peripheral portion of the superconducting coil.

請求項4に記載の発明の超電導コイルの保護装置は、請求項1から請求項3のいずれか一項に係る発明において、前記磁界変動検出素子は複数個配置されている。
請求項5に記載の発明の超電導コイルの保護装置は、請求項1から請求項4のいずれか一項に係る発明において、前記超電導線材は、基板上に中間層を介して希土類系酸化物超電導体による超電導層が形成され、その超電導層上に保護層が形成され、それらの外周部に安定化層が形成されて構成されている。
A superconducting coil protection device according to a fourth aspect of the present invention is the superconducting coil protection device according to any one of the first to third aspects, wherein a plurality of the magnetic field fluctuation detecting elements are arranged.
According to a fifth aspect of the present invention, there is provided the superconducting coil protection device according to any one of the first to fourth aspects, wherein the superconducting wire is a rare earth oxide superconducting material via an intermediate layer on a substrate. A superconducting layer is formed by a body, a protective layer is formed on the superconducting layer, and a stabilizing layer is formed on the outer peripheral portion thereof.

請求項6に記載の発明の超電導コイルの保護方法は、請求項1から請求項5のいずれか一項に記載の超電導コイルの保護装置を使用し、電源から超電導コイルに電流を供給して超電導コイルが運転状態にある場合において、磁界変動検出素子が磁界変動を検出したとき、電源から供給される電流を遮断するとともに、超電導コイルの貯蔵電力に基づく電流を超電導線材間に流して超電導コイル全体で貯蔵電力を消費して運転を停止することを特徴とする。   According to a sixth aspect of the present invention, there is provided a superconducting coil protection method using the superconducting coil protection device according to any one of the first to fifth aspects, wherein a current is supplied from a power source to the superconducting coil. When the coil is in an operating state, when the magnetic field fluctuation detecting element detects a magnetic field fluctuation, the current supplied from the power supply is cut off, and a current based on the stored power of the superconducting coil is passed between the superconducting wires to make the entire superconducting coil The storage power is consumed and the operation is stopped.

請求項7に記載の発明の超電導コイルの保護方法は、請求項6に係る発明において、前記磁界変動検出素子は超電導コイルの内周部に配置され、その磁界変動検出素子が磁界変動を検出したとき、電源から供給される電流を遮断する。   According to a seventh aspect of the present invention, there is provided the superconducting coil protection method according to the sixth aspect of the invention, wherein the magnetic field fluctuation detecting element is disposed on an inner periphery of the superconducting coil, and the magnetic field fluctuation detecting element detects a magnetic field fluctuation. When the current supplied from the power supply is cut off.

請求項8に記載の発明の超電導コイルの保護方法は、請求項6又は請求項7に係る発明において、前記磁界変動検出素子は複数個配置され、それらの磁界変動検出素子のうちいずれかの磁界変動検出素子が磁界変動を検出したとき、電源から供給される電流を遮断する。   The superconducting coil protection method according to an eighth aspect of the present invention is the invention according to the sixth or seventh aspect, wherein a plurality of the magnetic field fluctuation detection elements are arranged, and any one of the magnetic field fluctuation detection elements is arranged. When the fluctuation detecting element detects a magnetic field fluctuation, the current supplied from the power supply is cut off.

本発明の超電導コイルの保護装置によれば、構成を簡易にでき、常電導転移時に超電導コイルを保護しながら円滑に運転を停止することができるという効果を奏する。   According to the protection device for a superconducting coil of the present invention, the configuration can be simplified, and the operation can be smoothly stopped while protecting the superconducting coil at the time of normal conduction transition.

実施形態における異常検出機構を備えた超電導コイルの保護装置を模式的に示す概略図。Schematic which shows typically the protection apparatus of the superconducting coil provided with the abnormality detection mechanism in embodiment. シングルパンケーキコイルに4つのピックアップコイルを配置した状態を示す概略斜視図。The schematic perspective view which shows the state which has arrange | positioned four pick-up coils to the single pancake coil. 超電導線材を示す断面図。Sectional drawing which shows a superconducting wire. 超電導コイルに通電した状態での電流の流れを示す概略平面図。The schematic plan view which shows the flow of the electric current in the state which supplied with electricity to the superconducting coil. 超電導コイルの異常検出機構が異常を検出したときの超電導コイル内の電流の流れを示す概略平面図。The schematic plan view which shows the flow of the electric current in a superconducting coil when the abnormality detection mechanism of a superconducting coil detects abnormality. 時間と、コイルの磁界、コイルの電圧又はコイルの電流との関係を示すグラフ。The graph which shows the relationship between time and the magnetic field of a coil, the voltage of a coil, or the current of a coil. 本発明の別例を示し、ダブルパンケーキコイルに3つのピックアップコイルを配置した状態を示す概略斜視図。The schematic perspective view which shows the other example of this invention and shows the state which has arrange | positioned the three pickup coils to the double pancake coil. 本発明のさらなる別例を示し、異形形状のシングルパンケーキコイルに2つのピックアップコイルを配置した状態を示す概略平面図。The schematic top view which shows the further another example of this invention, and shows the state which has arrange | positioned the two pick-up coils to the irregular shaped single pancake coil.

以下、本発明の実施形態を図1〜図5に基づいて詳細に説明する。
図3に示すように、テープ状をなす超電導線材11は、基板12上に中間層13を介して超電導層14が形成され、その超電導層14上に保護層15が設けられ、それらの外周部に銅製の安定化層16が被覆されて構成されている。
Hereinafter, embodiments of the present invention will be described in detail with reference to FIGS.
As shown in FIG. 3, a superconducting wire 11 in the form of a tape has a superconducting layer 14 formed on a substrate 12 via an intermediate layer 13, and a protective layer 15 is provided on the superconducting layer 14, and the outer peripheral portions thereof. The copper stabilization layer 16 is coated on the surface.

前記基板12は、ニッケル合金(ハステロイ)、銀、銀合金等の金属により、例えば厚さ50〜100μm、幅4〜10mmに形成される。中間層13は、ガドリニウム・ジルコニウム酸化物(Gd・Zr酸化物)、ランタン(La)・マンガン(Mn)系酸化物、酸化マグネシウム(MgO)、イットリウム安定化ジルコニウム(YSZ)、バリウム・ジルコニウム酸化物(Ba・Zr酸化物)、酸化セリウム(CeO)等の化合物により、例えば厚さ500nmに形成される。 The substrate 12 is formed of a metal such as nickel alloy (Hastelloy), silver, or silver alloy, for example, to a thickness of 50 to 100 μm and a width of 4 to 10 mm. The intermediate layer 13 is made of gadolinium / zirconium oxide (Gd / Zr oxide), lanthanum (La) / manganese (Mn) oxide, magnesium oxide (MgO), yttrium stabilized zirconium (YSZ), barium / zirconium oxide. For example, it is formed to a thickness of 500 nm by a compound such as (Ba · Zr oxide) or cerium oxide (CeO 2 ).

超電導層14は、希土類系酸化物超電導体のCVD法(化学蒸着法)により、例えば厚さ約1μmに形成される。希土類元素としては、ランタン(La)、ネオジム(Nd)、サマリウム(Sm)、ユウロピウム(Eu)、ガドリニウム(Gd)、ジスプロシウム(Dy)、ホルミウム(Ho)、エルビウム(Er)、イットリウム(Y)、イッテルビウム(Yb)等が挙げられる。希土類系酸化物としては、RE・Ba・Cu・O等が挙げられる。但し、REは希土類元素を表す。この超電導層14として具体的には、イットリウム・バリウム・銅酸化物(Y・Ba・Cu酸化物)、ランタン・バリウム・銅酸化物(La・Ba・Cu酸化物)等が挙げられる。   The superconducting layer 14 is formed to a thickness of, for example, about 1 μm by a rare earth oxide superconductor CVD method (chemical vapor deposition method). As rare earth elements, lanthanum (La), neodymium (Nd), samarium (Sm), europium (Eu), gadolinium (Gd), dysprosium (Dy), holmium (Ho), erbium (Er), yttrium (Y), And ytterbium (Yb). Examples of rare earth oxides include RE, Ba, Cu, and O. However, RE represents a rare earth element. Specific examples of the superconducting layer 14 include yttrium / barium / copper oxide (Y / Ba / Cu oxide) and lanthanum / barium / copper oxide (La / Ba / Cu oxide).

前記保護層15は、銀、銀合金等の金属によって形成され、超電導層14を被覆して保護するように構成されている。この保護層15は、例えば銀等の金属のスパッタリングによって2〜8μm程度の厚さに形成される。   The protective layer 15 is formed of a metal such as silver or a silver alloy, and is configured to cover and protect the superconducting layer 14. The protective layer 15 is formed to a thickness of about 2 to 8 μm by sputtering of a metal such as silver.

前記安定化層16は銅により形成され、超電導状態が不安定になって抵抗が生じた場合でも、超電導層14に流れている電流を保護層15から安定化層16に迂回させて後述する超電導コイルの超電導特性を安定化させる機能を有している。安定化層16を形成する銅には銅合金も含まれる。この安定化層16の厚さは通電電流の大きさに応じて厚くなるが、実用的には5〜30μmであることが好ましい。安定化層16の厚さが5μmより薄い場合には、安定化層16を流れる電流量が低下し、安定化層16としての機能が十分に発揮できなくなって好ましくない。その一方、安定化層16の厚さが30μmより厚い場合には、超電導線材11の剛性が高くなって取扱いが難しくなる傾向にあり、超電導コイルの形成が困難になったりして好ましくない。   The stabilization layer 16 is made of copper, and even when the superconducting state becomes unstable and resistance is generated, the current flowing in the superconducting layer 14 is diverted from the protective layer 15 to the stabilizing layer 16 to be described later. It has the function of stabilizing the superconducting characteristics of the coil. The copper forming the stabilizing layer 16 includes a copper alloy. The thickness of the stabilization layer 16 increases depending on the magnitude of the energization current, but is practically preferably 5 to 30 μm. When the thickness of the stabilization layer 16 is less than 5 μm, the amount of current flowing through the stabilization layer 16 is lowered, and the function as the stabilization layer 16 cannot be sufficiently exhibited, which is not preferable. On the other hand, when the thickness of the stabilization layer 16 is greater than 30 μm, the superconducting wire 11 has a high rigidity and tends to be difficult to handle, which is not preferable because it makes it difficult to form a superconducting coil.

この安定化層16は、銅めっきによって形成されることが好ましい。銅めっきは電気めっきの常法に従って行われるが、硫酸銅等のめっき液を用い、電極間に所要の電流を流すことにより行われる。この銅めっきにより、安定化層16を容易かつ安定した状態で形成することができる。   This stabilization layer 16 is preferably formed by copper plating. Copper plating is performed according to a conventional method of electroplating, and is performed by using a plating solution such as copper sulfate and passing a required current between the electrodes. By this copper plating, the stabilization layer 16 can be formed easily and stably.

図2に示すように、超電導コイルとしてのシングルパンケーキコイル(単にコイルともいう)17は、前述したテープ状の超電導線材11をコイル状(渦巻状)に1段で巻回して形成される。この超電導線材11をコイル状に巻回する際には、超電導線材11間に電気絶縁材料は介在されておらず、超電導線材11間が直接接触した状態つまり超電導線材11の安定化層16間が直接接触した状態で巻回される。前記コイル17の内周側における超電導線材11の端部及び外周側における超電導線材11の端部には、銅等の導電性の良い金属により形成された一対の電極18、19が接続されている。なお、図1〜図5の各図においては、コイル17は理解を容易にするため模式的に描かれ、各層の厚さや超電導線材11の厚さは実際より厚く描かれている。   As shown in FIG. 2, a single pancake coil (also simply referred to as a coil) 17 as a superconducting coil is formed by winding the tape-shaped superconducting wire 11 in a coil shape (spiral shape) in one step. When the superconducting wire 11 is wound in a coil shape, no electrical insulating material is interposed between the superconducting wires 11 and the superconducting wires 11 are in direct contact with each other, that is, between the stabilization layers 16 of the superconducting wire 11. It is wound in direct contact. A pair of electrodes 18 and 19 made of a metal having good conductivity such as copper are connected to the end of the superconducting wire 11 on the inner peripheral side of the coil 17 and the end of the superconducting wire 11 on the outer peripheral side. . 1 to 5, the coil 17 is schematically drawn for easy understanding, and the thickness of each layer and the thickness of the superconducting wire 11 are drawn thicker than actual.

図1に示すように、シングルパンケーキコイル17の両電極18、19間には電源20が接続線21により接続され、電源20からの電流がコイル17へ供給されるようになっている。前記接続線21には開閉スイッチ22が設けられ、コイル17にクエンチ、停電、冷凍機停止等による異常事態(常電導転移)が発生したとき、コイル17へ電流の供給を遮断できるようになっている。   As shown in FIG. 1, a power source 20 is connected between both electrodes 18 and 19 of the single pancake coil 17 by a connection line 21, and a current from the power source 20 is supplied to the coil 17. The connection line 21 is provided with an open / close switch 22 so that when an abnormal situation (normal conduction transition) occurs due to a quench, a power failure, a chiller stop, or the like, the current supply to the coil 17 can be cut off. Yes.

前記シングルパンケーキコイル17の内周部近傍には、磁界変動検出素子としての4つのピックアップコイル(シングルコイル)23が周方向に間隔をおいて配置されている。これらのピックアップコイル23は、コイル17が常電導転移に基づいて磁界変動を生じたとき、その磁界変動を検出する。コイル17の内周部は外周部に比べて磁界が強いことから、ピックアップコイル23による磁界変動の検出精度を高めることができる。   In the vicinity of the inner periphery of the single pancake coil 17, four pickup coils (single coils) 23 as magnetic field fluctuation detection elements are arranged at intervals in the circumferential direction. These pickup coils 23 detect the magnetic field fluctuation when the coil 17 causes a magnetic field fluctuation based on the normal conducting transition. Since the inner peripheral portion of the coil 17 has a stronger magnetic field than the outer peripheral portion, the detection accuracy of the magnetic field fluctuation by the pickup coil 23 can be increased.

前記4つのピックアップコイル23はそれぞれ入力線24により制御装置25に接続され、その制御装置25は出力線26により前記開閉スイッチ22に接続されている。そして、4つのピックアップコイル23のいずれかが磁界変動を検出したとき、その信号が入力線24を介して制御装置25に入力され、制御装置25から制御信号が出力線26を介して開閉スイッチ22に送られて開閉スイッチ22が開放され、電源20からコイル17に供給される電流を遮断するように構成されている。   Each of the four pickup coils 23 is connected to a control device 25 by an input line 24, and the control device 25 is connected to the open / close switch 22 by an output line 26. When any of the four pickup coils 23 detects a magnetic field variation, the signal is input to the control device 25 via the input line 24, and the control signal is transmitted from the control device 25 via the output line 26 to the open / close switch 22. The open / close switch 22 is opened and the current supplied from the power source 20 to the coil 17 is cut off.

異常検出機構27は、前記4つのピックアップコイル23、制御装置25、開閉スイッチ22等により構成されている。また、シングルパンケーキコイル17の保護装置10は、シングルパンケーキコイル17、両電極18、19、電源20、異常検出機構27等により構成されている。   The abnormality detection mechanism 27 includes the four pickup coils 23, the control device 25, the open / close switch 22, and the like. The protection device 10 for the single pancake coil 17 includes a single pancake coil 17, both electrodes 18, 19, a power source 20, an abnormality detection mechanism 27, and the like.

次に、上記のように構成されたシングルパンケーキコイル17の保護装置10について作用を説明する。
さて、本実施形態のシングルパンケーキコイル17を常法に従い冷却して超電導状態とし、その超電導状態でコイル17の両電極18、19間に電源20から所定の電流を通電すると、図4の二点鎖線の矢印に示すように電流は一方の電極19から超電導線材11中の超電導層14を通って他方の電極18へと流れる。このとき、電気抵抗のない超電導状態で通電を継続することができ、高電流密度で大電流を通電でき、電力を貯蔵できるとともに、コイル17の周囲に強磁場を発生することができる。
Next, an effect | action is demonstrated about the protection apparatus 10 of the single pancake coil 17 comprised as mentioned above.
When the single pancake coil 17 of the present embodiment is cooled according to a conventional method to be in a superconducting state and a predetermined current is supplied from the power source 20 between the electrodes 18 and 19 of the coil 17 in the superconducting state, As indicated by the dotted line arrow, current flows from one electrode 19 to the other electrode 18 through the superconducting layer 14 in the superconducting wire 11. At this time, energization can be continued in a superconducting state without electrical resistance, a large current can be energized with a high current density, electric power can be stored, and a strong magnetic field can be generated around the coil 17.

この超電導状態において、シングルパンケーキコイル17を構成する超電導線材11の一部が何らかの理由で超電導状態を逸脱して常電導状態に移行する常電導転移が発生する場合がある。このとき、超電導層14を流れていた電流は安定化層16へ流れ、さらに超電導線材11間を流れて、コイル17の巻回数が見かけ上減少するため、コイル17から発せられる磁界は急激に低下するように変動する。この磁界変動を前記4つのピックアップコイル23のいずれかが検出する。いずれかのピックアップコイル23によって検出された磁界変動に基づく入力信号は制御装置25に送られ、制御装置25から制御信号が開閉スイッチ22に送られて直ちに開閉スイッチ22が図1の二点鎖線に示すように開放される。そのため、電源20からコイル17へ供給される電流は遮断されると同時に、図5の二点鎖線の矢印に示すようにコイル17内に貯蔵された電力による電流は、外周に位置する超電導線材11の超電導層14から安定化層16へ流れた後、その内周側に隣接する超電導線材11へと流れ、さらにコイル17の中心に向って瞬時に流れる。   In this superconducting state, a part of the superconducting wire 11 constituting the single pancake coil 17 may deviate from the superconducting state and shift to the normal conducting state for some reason. At this time, the current flowing in the superconducting layer 14 flows to the stabilizing layer 16 and further flows between the superconducting wires 11, and the number of turns of the coil 17 is apparently reduced, so that the magnetic field generated from the coil 17 rapidly decreases. To fluctuate. Any of the four pickup coils 23 detects this magnetic field fluctuation. An input signal based on the magnetic field fluctuation detected by any one of the pickup coils 23 is sent to the control device 25, and the control signal is sent from the control device 25 to the open / close switch 22, and the open / close switch 22 immediately changes to the two-dot chain line in FIG. Open as shown. Therefore, the current supplied from the power source 20 to the coil 17 is interrupted, and at the same time, as indicated by the two-dot chain line arrow in FIG. After flowing from the superconducting layer 14 to the stabilizing layer 16, it flows to the superconducting wire 11 adjacent to the inner peripheral side, and further flows instantaneously toward the center of the coil 17.

すなわち、シングルパンケーキコイル17内では急激な電流変化によって誘導電圧が生じ、超電導線材11間に電流が流れてコイル17全体の安定化層16が結合した状態になり、見かけ上銅のバルクのような負荷となってコイル17全体が発熱して貯蔵電力が消費される。その結果、コイル17とは別に保護回路を設けて貯蔵電力を消費させずとも、超電導線材11の局部的な発熱を抑制でき、コイル17の損傷を回避することができる。   That is, an induced voltage is generated in the single pancake coil 17 due to an abrupt current change, and a current flows between the superconducting wires 11 so that the stabilization layer 16 of the entire coil 17 is coupled, which looks like a copper bulk. The entire coil 17 generates heat and the stored power is consumed. As a result, local heat generation of the superconducting wire 11 can be suppressed and damage to the coil 17 can be avoided without providing a protection circuit separately from the coil 17 and consuming stored power.

以上詳述した実施形態によって得られる効果を以下にまとめて記載する。
(1)本実施形態のシングルパンケーキコイル17の保護装置10において、コイル17は超電導線材11間を絶縁することなく巻回して形成されるとともに、コイル17には磁界変動検出素子を有する異常検出機構27が備えられている。そのため、この磁界変動検出素子がクエンチ等の異常発生に伴う磁界変動を検出したとき電源20から供給される電流を遮断して電源20等への過電流の流入を抑制することができるとともに、保護回路を用いることなく、コイル17内の局所的温度上昇を抑えながらコイル17の運転を停止することができる。
The effects obtained by the embodiment described in detail above are collectively described below.
(1) In the protection device 10 for the single pancake coil 17 of the present embodiment, the coil 17 is formed by winding the superconducting wire 11 without being insulated, and the coil 17 has an abnormality detection having a magnetic field fluctuation detection element. A mechanism 27 is provided. Therefore, when this magnetic field fluctuation detecting element detects a magnetic field fluctuation accompanying an abnormality such as a quench, the current supplied from the power source 20 can be cut off to suppress the inflow of overcurrent to the power source 20 and the like. Without using a circuit, the operation of the coil 17 can be stopped while suppressing a local temperature rise in the coil 17.

従って、本実施形態の保護装置10によれば、構成を簡易にでき、常電導転移時にシングルパンケーキコイル17を保護しながら円滑に運転を停止することができる。
(2)前記磁界変動検出素子はピックアップコイル23である。このため、簡易構造で汎用の検出素子により、磁界変動を精度良く検出することができる。
Therefore, according to the protection device 10 of the present embodiment, the configuration can be simplified, and the operation can be stopped smoothly while protecting the single pancake coil 17 at the time of normal conduction transition.
(2) The magnetic field fluctuation detecting element is a pickup coil 23. For this reason, magnetic field fluctuations can be detected with high accuracy by a general-purpose detection element having a simple structure.

(3)前記ピックアップコイル23は、シングルパンケーキコイル17の内周部に配置されている。このコイル17の内周部においては、通電時に強い磁界が発生しており、磁界変動の検出精度を一層向上させることができる。   (3) The pickup coil 23 is disposed on the inner periphery of the single pancake coil 17. In the inner peripheral portion of the coil 17, a strong magnetic field is generated when energized, and the detection accuracy of the magnetic field fluctuation can be further improved.

(4)前記ピックアップコイル23は複数個配置されている。そのため、複数のピックアップコイル23のいずれかが磁界変動を検出したとき、コイル17の運転を迅速に停止することができる。   (4) A plurality of the pickup coils 23 are arranged. Therefore, when any of the plurality of pickup coils 23 detects a magnetic field variation, the operation of the coil 17 can be stopped quickly.

(5)前記超電導線材11は、基板12上に中間層13を介して希土類系酸化物超電導体による超電導層14が形成され、その超電導層14上に保護層15が設けられ、それらの外周部に安定化層16が形成されて構成されている。このため、コイル17は、超電導特性を良好に発揮できるとともに、常電導転移時にはその運転を速やかに停止することができる。   (5) In the superconducting wire 11, a superconducting layer 14 made of a rare earth oxide superconductor is formed on a substrate 12 via an intermediate layer 13, and a protective layer 15 is provided on the superconducting layer 14, and the outer peripheral portions thereof. In addition, a stabilization layer 16 is formed. For this reason, the coil 17 can exhibit a superconducting characteristic favorably, and can stop the operation | movement rapidly at the time of a normal conduction transition.

(6)シングルパンケーキコイル17の保護方法は、シングルパンケーキコイル17が運転状態にある場合において、磁界変動検出素子が磁界変動を検出したとき、電源20から供給される電流を遮断し、巻回されている超電導線材11間に電流を流してコイル17全体で貯蔵電力を消費して運転を停止するものである。従って、常電導転移時にコイル17に損傷を与えることなく保護しながら運転を円滑に停止することができる。   (6) The method for protecting the single pancake coil 17 is that when the single pancake coil 17 is in an operating state, when the magnetic field fluctuation detecting element detects a magnetic field fluctuation, the current supplied from the power source 20 is cut off, A current is passed between the superconducting wires 11 being rotated, the stored power is consumed in the entire coil 17, and the operation is stopped. Accordingly, it is possible to smoothly stop the operation while protecting the coil 17 without damaging it during the normal conducting transition.

次に、実施例を挙げて前記実施形態をさらに具体的に説明する。
(実施例1)
まず、この実施例1では、幅4mm、厚さ50μmのニッケル合金(ハステロイ)製の基板12上にランタン・マンガン系酸化物及び酸化マグネシウムの中間層13を介してイットリウム系の超電導物質による超電導層14を形成した。次いで、その上に銀のスパッタリングによる保護層15を形成し、その外周に銅めっきによる安定化層16を形成し、厚さ約100μmのイットリウム系の超電導線材11(液体窒素中、自己磁場での臨界電流130A)を作製した。そして、この超電導線材11を1段に30回巻回して、内径60mm、外径66mmのシングルパンケーキコイル17を製作した。
Next, the embodiment will be described more specifically with reference to examples.
Example 1
First, in Example 1, a superconducting layer made of a yttrium-based superconducting material via a lanthanum / manganese-based oxide and magnesium oxide intermediate layer 13 on a nickel alloy (Hastelloy) substrate 12 having a width of 4 mm and a thickness of 50 μm. 14 was formed. Next, a protective layer 15 by sputtering of silver is formed thereon, a stabilization layer 16 by copper plating is formed on the outer periphery thereof, and a yttrium-based superconducting wire 11 having a thickness of about 100 μm (in liquid nitrogen in a self-magnetic field). A critical current 130A) was produced. Then, this superconducting wire 11 was wound 30 times in one stage to produce a single pancake coil 17 having an inner diameter of 60 mm and an outer diameter of 66 mm.

そして、得られたシングルパンケーキコイル17を液体窒素中にて、0.5A/sの速度で励磁電流(通電電流)を125Aまで通電した際のコイルの磁界(最大磁界、mT)の変化とコイルの両電極18,19間の電圧(V)の変化を測定し、その結果を図6に示した。なお、図6における実線はコイル17の磁界(mT)の変化、破線はコイル17の電流(10A)の変化及び二点鎖線はコイル17の電圧(V)の変化を示す。 And the change of the magnetic field (maximum magnetic field, mT) of the coil when energizing the obtained single pancake coil 17 in liquid nitrogen at a speed of 0.5 A / s up to 125 A energizing current (energizing current) The change in voltage (V) between both electrodes 18 and 19 of the coil was measured, and the result is shown in FIG. In FIG. 6, a solid line indicates a change in the magnetic field (mT) of the coil 17, a broken line indicates a change in the current (10 2 A) of the coil 17, and a two-dot chain line indicates a change in the voltage (V) of the coil 17.

図6に示した結果より、シングルパンケーキコイル17の磁界はコイル電流が臨界電流付近に到ると、増大傾向が鈍化した。さらにコイル電流を増加させると、突然磁界が減少すると同時に、コイル電圧が急上昇した。従って、超電導線材11間が絶縁されていないシングルパンケーキコイル17において、常電導転移により通電状態が崩れると、コイル17の磁界が急速に低下することを確認できた。   From the results shown in FIG. 6, the increasing tendency of the magnetic field of the single pancake coil 17 slowed down when the coil current reached near the critical current. When the coil current was further increased, the magnetic field suddenly decreased and at the same time the coil voltage rose rapidly. Therefore, in the single pancake coil 17 in which the superconducting wire 11 is not insulated, it was confirmed that the magnetic field of the coil 17 rapidly decreased when the energized state collapsed due to the normal conducting transition.

次いで、図1に示すように、コイル17の内周面近傍に4つのピックアップコイル23を配置し、そのピックアップコイル23が磁界変動を検出すると直ちに開閉スイッチ22を開放するようにした。ピックアップコイル23は、直径0.25mmの銅線を内径5mmで巻いて作製した。   Next, as shown in FIG. 1, four pickup coils 23 are arranged in the vicinity of the inner peripheral surface of the coil 17, and the opening / closing switch 22 is opened as soon as the pickup coil 23 detects a magnetic field variation. The pickup coil 23 was produced by winding a copper wire having a diameter of 0.25 mm with an inner diameter of 5 mm.

そして、超電導状態でシングルパンケーキコイル17を運転していたところ、ピックアップコイル23によりコイル電流87.5Aで磁界が急激に低下したことが検出され、その結果開閉スイッチ22が開放されてコイル17の運転が停止した。その後、コイル17の状態を目視により確認したところ、外観に変化は見られなかった。さらに、コイル17に通電して励磁したところ、前記図6と同様に、電流の上昇に伴って磁界が上昇する結果が得られたことから、コイル17に劣化箇所は認められなかった。従って、この実施例1では、コイル17とは別に保護回路を設けることなく、コイル17の貯蔵電力に基づく発熱によるコイル17の損傷を抑えることができ、超電導特性を維持できることが判明した。   Then, when the single pancake coil 17 was operated in the superconducting state, it was detected by the pickup coil 23 that the magnetic field suddenly decreased with the coil current 87.5A, and as a result, the open / close switch 22 was opened and the coil 17 Operation stopped. Then, when the state of the coil 17 was confirmed by visual observation, no change was seen in the appearance. Furthermore, when the coil 17 was energized and excited, as in the case of FIG. 6, a result that the magnetic field increased as the current increased was obtained. Therefore, in Example 1, it was found that, without providing a protection circuit separately from the coil 17, damage to the coil 17 due to heat generation based on the stored power of the coil 17 can be suppressed, and the superconducting characteristics can be maintained.

ここで、コイル17の発熱量をPEEC(Partial Element Equivalent Circuit、部分要素等価回路)解析と熱解析を連成した解析プログラムを用いて解析し、評価した。なお、PEEC解析は、積分方程式による電磁場解析の手法の1つで、電磁界と回路を結合した解析に適した三次元の全波モデル化手法であって、公知の手法であるため、その説明を省略する。   Here, the calorific value of the coil 17 was analyzed and evaluated using an analysis program in which PEEC (Partial Element Equivalent Circuit) analysis and thermal analysis were coupled. The PEEC analysis is one of electromagnetic field analysis methods based on integral equations, and is a three-dimensional full-wave modeling method suitable for analysis combining an electromagnetic field and a circuit. Is omitted.

まず、コイル17の内径を60mm、超電導線材11の巻数を60とし、巻回された超電導線材11間の接触抵抗を70、350及び700μΩ・cmの3通りに設定した場合のコイル17の温度上昇について解析した。コイル17のインダクタンスは432μH、通電電流は30A、貯蔵エネルギーは194.5mJで、断熱状態であるとして温度上昇を解析した。その結果、接触抵抗の大きさにかかわらず、コイル17の温度上昇は0.017Kであった。従って、コイル17の温度上昇は僅かであり、超電導線材11間が絶縁されていないシングルパンケーキコイル17の熱的安定性が示された。 First, the temperature of the coil 17 when the inner diameter of the coil 17 is 60 mm, the number of turns of the superconducting wire 11 is 60, and the contact resistance between the wound superconducting wire 11 is set to three types of 70, 350, and 700 μΩ · cm 2. The rise was analyzed. The inductance of the coil 17 was 432 μH, the energization current was 30 A, the stored energy was 194.5 mJ, and the temperature rise was analyzed as being in an adiabatic state. As a result, the temperature rise of the coil 17 was 0.017K regardless of the contact resistance. Therefore, the temperature rise of the coil 17 is slight, and the thermal stability of the single pancake coil 17 in which the superconducting wire 11 is not insulated is shown.

次に、コイル17の内径を60mm、超電導線材11間の接触抵抗を70μΩ・cmとし、超電導線材11の巻数を120、240及び360とした場合の温度上昇を解析した。解析条件と温度上昇を表1に示した。 Next, the temperature rise was analyzed when the inner diameter of the coil 17 was 60 mm, the contact resistance between the superconducting wires 11 was 70 μΩ · cm 2, and the number of turns of the superconducting wire 11 was 120, 240, and 360. The analysis conditions and temperature rise are shown in Table 1.

表1に示した結果より、超電導線材11の巻数が増加すると、接触抵抗による消費エネルギーは一定の増加を示すが、コイル17の温度上昇は小さいものであった。従って、超電導線材11間が絶縁されていないシングルパンケーキコイル17は、常電導転移による異常事態に対して高い熱的安定性を有することが明らかになり、保護抵抗を用いることなく、コイル17を保護しつつその運転を停止することが可能となった。 From the results shown in Table 1, when the number of turns of the superconducting wire 11 is increased, the energy consumption due to contact resistance shows a certain increase, but the temperature rise of the coil 17 is small. Therefore, it becomes clear that the single pancake coil 17 in which the superconducting wire 11 is not insulated has high thermal stability against an abnormal situation due to normal conduction transition, and the coil 17 can be connected without using protective resistance. It became possible to stop the operation while protecting.

なお、前記実施形態を次のように変更して具体化することも可能である。
・前記超電導コイルとしてダブルパンケーキコイルを使用してもよい。すなわち、図7に示すように、ダブルパンケーキコイル28は、テープ状の超電導線材11が図示しない内周枠の周りに巻回されて形成されたコイル28a,28bがセパレート枠29を介して上下2段に積層されて形成されている。ダブルパンケーキコイル28の内周部には、例えば3つのピックアップコイル23が配置される。
It should be noted that the embodiment described above can be modified and embodied as follows.
-A double pancake coil may be used as the superconducting coil. That is, as shown in FIG. 7, the double pancake coil 28 has coils 28a and 28b formed by winding a tape-like superconducting wire 11 around an inner peripheral frame (not shown). It is formed in two layers. For example, three pickup coils 23 are arranged on the inner peripheral portion of the double pancake coil 28.

・前記磁界変動検出素子として、ホール素子、ファラデー素子等を使用してもよい。
・図8に示すように、シングルパンケーキコイル17として異形形状のものを使用してもよい。この場合には、ピックアップコイル23を、周囲と比べて強い磁界が発生し磁界変動の検出精度を高めることができるコイル17の屈曲部の内周部に配置することが好ましい。
A Hall element, a Faraday element, or the like may be used as the magnetic field fluctuation detection element.
As shown in FIG. 8, a single pancake coil 17 having a deformed shape may be used. In this case, it is preferable to arrange the pickup coil 23 on the inner peripheral portion of the bent portion of the coil 17 that generates a magnetic field stronger than the surroundings and can improve the detection accuracy of the magnetic field fluctuation.

・前記超電導線材11として、ビスマス系酸化物の超電導線材を使用してもよい。このビスマス系酸化物の超電導体としては、ビスマス(Bi)を含む酸化物により形成される超電導物質であり、例えばBi2223すなわちBiSrCaCu10−α(αは0〜0.15)、Bi2212すなわちBiSrCaCu8−α(αは0〜0.15)等が用いられる。このビスマス系酸化物の超電導体が展伸性を有する金属材料のシース層中に分散されて構成される。 As the superconducting wire 11, a bismuth oxide superconducting wire may be used. The superconductor of this bismuth-based oxide is a superconducting material formed of an oxide containing bismuth (Bi). For example, Bi2223, that is, Bi 2 Sr 2 Ca 2 Cu 3 O 10-α (α is 0 to 0. 15), Bi2212, that is, Bi 2 Sr 2 CaCu 2 O 8-α (α is 0 to 0.15) or the like is used. This bismuth-based oxide superconductor is configured to be dispersed in a sheath layer of a metal material having stretchability.

10…保護装置、11…超電導線材、12…基板、13…中間層、14…超電導層、15…保護層、16…安定化層、17…超電導コイルとしてのシングルパンケーキコイル、19…電極、20…電源、23…磁界変動検出素子としてのピックアップコイル、27…異常検出機構、28…超電導コイルとしてのダブルパンケーキコイル。   DESCRIPTION OF SYMBOLS 10 ... Protection apparatus, 11 ... Superconducting wire, 12 ... Substrate, 13 ... Intermediate layer, 14 ... Superconducting layer, 15 ... Protective layer, 16 ... Stabilization layer, 17 ... Single pancake coil as superconducting coil, 19 ... Electrode, DESCRIPTION OF SYMBOLS 20 ... Power supply, 23 ... Pick-up coil as a magnetic field fluctuation detection element, 27 ... Abnormality detection mechanism, 28 ... Double pancake coil as a superconducting coil.

Claims (8)

超電導線材をコイル状に巻回するとともに、前記超電導線材の両端部に電極を取付け、両電極間に電源を接続して通電するようにした超電導コイルであって、
前記超電導コイルは超電導線材間を絶縁することなく巻回して形成されるとともに、超電導コイルにはその磁界が及ぶ範囲に磁界変動検出素子を備え、該磁界変動検出素子が磁界変動を検出したとき電源から供給される電流を遮断する異常検出機構を備えた超電導コイルの保護装置。
A superconducting coil in which a superconducting wire is wound in a coil shape, electrodes are attached to both ends of the superconducting wire, and a power source is connected between both electrodes to energize,
The superconducting coil is formed by winding the superconducting wires without insulation, and the superconducting coil is provided with a magnetic field fluctuation detecting element in a range covered by the magnetic field, and when the magnetic field fluctuation detecting element detects a magnetic field fluctuation, a power source is provided. Superconducting coil protection device equipped with an abnormality detection mechanism that cuts off the current supplied from the coil.
前記磁界変動検出素子はピックアップコイルである請求項1に記載の超電導コイルの保護装置。   The superconducting coil protection device according to claim 1, wherein the magnetic field fluctuation detection element is a pickup coil. 前記磁界変動検出素子は、超電導コイルの内周部に配置されている請求項1又は請求項2に記載の超電導コイルの保護装置。   The protection device for a superconducting coil according to claim 1, wherein the magnetic field fluctuation detection element is disposed on an inner periphery of the superconducting coil. 前記磁界変動検出素子は複数個配置されている請求項1から請求項3のいずれか一項に記載の超電導コイルの保護装置。   The protection device for a superconducting coil according to any one of claims 1 to 3, wherein a plurality of the magnetic field fluctuation detection elements are arranged. 前記超電導線材は、基板上に中間層を介して希土類系酸化物超電導体による超電導層が形成され、その超電導層上に保護層が形成され、それらの外周部に安定化層が形成されて構成されている請求項1から請求項4のいずれか一項に記載の超電導コイルの保護装置。   The superconducting wire is composed of a superconducting layer formed of a rare earth oxide superconductor through an intermediate layer on a substrate, a protective layer formed on the superconducting layer, and a stabilization layer formed on the outer periphery thereof. The superconducting coil protection device according to any one of claims 1 to 4, wherein the protection device is a superconducting coil. 請求項1から請求項5のいずれか一項に記載の超電導コイルの保護装置を使用し、電源から超電導コイルに電流を供給して超電導コイルが運転状態にある場合において、磁界変動検出素子が磁界変動を検出したとき、電源から供給される電流を遮断するとともに、超電導コイルの貯蔵電力に基づく電流を超電導線材間に流して超電導コイル全体で貯蔵電力を消費して運転を停止することを特徴とする超電導コイルの保護方法。   When the superconducting coil protection device according to any one of claims 1 to 5 is used and a current is supplied from a power source to the superconducting coil and the superconducting coil is in an operating state, the magnetic field fluctuation detection element is a magnetic field. When the fluctuation is detected, the current supplied from the power supply is cut off, and the current based on the stored power of the superconducting coil is passed between the superconducting wires to consume the stored power in the entire superconducting coil and stop the operation. To protect the superconducting coil. 前記磁界変動検出素子は超電導コイルの内周部に配置され、その磁界変動検出素子が磁界変動を検出したとき、電源から供給される電流を遮断する請求項6に記載の超電導コイルの保護方法。   7. The method of protecting a superconducting coil according to claim 6, wherein the magnetic field fluctuation detecting element is disposed on an inner periphery of the superconducting coil, and when the magnetic field fluctuation detecting element detects a magnetic field fluctuation, the current supplied from the power source is cut off. 前記磁界変動検出素子は複数個配置され、それらの磁界変動検出素子のうちいずれかの磁界変動検出素子が磁界変動を検出したとき、電源から供給される電流を遮断する請求項6又は請求項7に記載の超電導コイルの保護方法。   A plurality of the magnetic field fluctuation detection elements are arranged, and when any of the magnetic field fluctuation detection elements detects a magnetic field fluctuation, the current supplied from the power source is cut off. 2. A method for protecting a superconducting coil according to 1.
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