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JPS6331091B2 - - Google Patents
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JPS6331091B2 - - Google Patents

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Publication number
JPS6331091B2
JPS6331091B2 JP56027050A JP2705081A JPS6331091B2 JP S6331091 B2 JPS6331091 B2 JP S6331091B2 JP 56027050 A JP56027050 A JP 56027050A JP 2705081 A JP2705081 A JP 2705081A JP S6331091 B2 JPS6331091 B2 JP S6331091B2
Authority
JP
Japan
Prior art keywords
current
power supply
transition
detector
superconducting device
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.)
Expired
Application number
JP56027050A
Other languages
Japanese (ja)
Other versions
JPS57141904A (en
Inventor
Hisahide Nakayama
Katsuji Murai
Kunishige Kuroda
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.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP2705081A priority Critical patent/JPS57141904A/en
Publication of JPS57141904A publication Critical patent/JPS57141904A/en
Publication of JPS6331091B2 publication Critical patent/JPS6331091B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F6/00Superconducting magnets; Superconducting coils
    • H01F6/02Quenching; Protection arrangements during quenching

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Protection Of Static Devices (AREA)

Description

【発明の詳細な説明】 本発明は超電導装置の電源制御装置に係り、特
に超電導々体の常電導転移(以下、転移という)
を未然に防ぎながら超電導装置に対する通電々流
を制御する電源制御装置に関する。
[Detailed Description of the Invention] The present invention relates to a power supply control device for a superconducting device, and particularly to a normal conduction transition (hereinafter referred to as transition) of a superconductor.
The present invention relates to a power supply control device that controls current flow to a superconducting device while preventing such problems from occurring.

超電導装置に通電中、何らかの原因で導体の一
部に転移が発生し、転移領域が超電導状態に回復
せずに拡つてゆくと、導体内で発生する有限の抵
抗分によるジユール損失のため、流体ヘリウムの
沸騰などによる装置(導体や容器等)の破損が生
じるおそれがある。従来、このような転移に対し
ては、超電導装置内のエネルギーを装置外で消費
させて導体の保護を行うことなどが考えられてき
た。
When a superconducting device is energized, if a transition occurs in a part of the conductor for some reason and the transition region expands without recovering to the superconducting state, fluid loss due to the finite resistance generated within the conductor occurs. There is a risk of damage to equipment (conductors, containers, etc.) due to boiling of helium. Conventionally, it has been considered to protect the conductor by consuming energy within the superconducting device outside the device in order to prevent such transitions.

しかし、上記のような方法では、超電導装置が
転移した後でないと動作が期待できないので、転
移に先立つ現象を検出して転移を防止する方法が
最近考えられている。しかし、従来の制御装置は
転移後または転移が予測された場合通電停止また
は遮断を行うだけで、所定のパターンの通電々流
制御を望む場合、その要求に対応できないという
欠点を持つていた。
However, with the above-mentioned methods, operation cannot be expected until after the superconducting device has transferred, so methods have recently been considered to prevent the transfer by detecting phenomena that precede the transfer. However, conventional control devices only stop or cut off the energization after transition or when transition is predicted, and have the disadvantage that they cannot meet the demand for energization control in a predetermined pattern.

本発明は以上の点に鑑み発明されたもので、そ
の目的とするところは、超電導装置の転移を防止
し、所定の通電々流パターンと実際の通電々流パ
ターンとの偏差を最小にする超電導装置の電源制
御装置の提供にある。
The present invention was invented in view of the above points, and its purpose is to prevent the transition of a superconducting device and to minimize the deviation between a predetermined energizing current pattern and an actual energizing current pattern. The purpose of the present invention is to provide a power supply control device for the device.

超電導々体に、転移が発生する原因は電磁的な
ものと機械的なものが考えられており、導体中の
磁束の移動と導体の動き(変形)にともない、分
流現象や渦電流や磁化により導体中に熱を発生
し、最終的には導体の温度上昇をもたらすといわ
れている。
The causes of transitions in superconductors are thought to be electromagnetic and mechanical, and are caused by shunt phenomena, eddy currents, and magnetization due to the movement of magnetic flux in the conductor and the movement (deformation) of the conductor. It is said that heat is generated in the conductor, ultimately causing the temperature of the conductor to rise.

本発明は以上の点に着目し、 (1) 導体の温度上昇の検出器 (2) 液体ヘリウム中の泡の検出器 (3) 導体の動きによつて発生する音波の検出器 (4) 導体の動きによつて発生する電場を求めるた
めの導体の速度検出器 (5) 導体などに発生する渦電流損を求めるための
磁場検出器 などの出力信号から転移発生を予測して通電々流
の制御を行い、所定の通電々流パターンに対する
実際の通電々流パターンの偏差を求め、転移が発
生しない範囲で偏差を最小にする制御の実現を計
る点にある。
The present invention focuses on the above points and provides (1) a detector for temperature rise in a conductor, (2) a detector for bubbles in liquid helium, (3) a detector for sound waves generated by the movement of a conductor, and (4) a detector for a conductor. conductor speed detector to determine the electric field generated by the movement of the conductor (5); magnetic field detector to determine the eddy current loss generated in the conductor, etc.; The purpose of this method is to perform control, find the deviation of the actual current flow pattern from a predetermined current flow pattern, and realize control that minimizes the deviation within a range where transition does not occur.

第1図は本発明の実施例を示したものである。
超電導コイル10は容器11内に設置され、液化
装置12によつて作られる液体ヘリウム13によ
つて冷却されている。
FIG. 1 shows an embodiment of the present invention.
The superconducting coil 10 is placed in a container 11 and is cooled by liquid helium 13 produced by a liquefier 12 .

超電導コイル10は電源20によつて通電さ
れ、電源20は電源制御装置30の制御信号31
によつてその出力を制御される。
The superconducting coil 10 is energized by a power supply 20, and the power supply 20 receives a control signal 31 from a power supply control device 30.
Its output is controlled by

超電導コイル10の転移の原因となる現象を検
出する各種検出器は超電導コイル10、あるいは
容器11に設置する。検出器には、液体ヘリウム
13に発生する泡を検出する気泡検出器40、超
電導々体内部の歪や導体の動きにより発生する音
波をとらえる音波検出器50、導体の動く速度と
磁束密度から導体に発生する電界を求めるための
速度検出器60、磁気検出器70等を使用する。
このうち磁気検出器70は導体に発生する渦電流
損を求めるためにも使用する。
Various detectors for detecting phenomena that cause the transition of the superconducting coil 10 are installed in the superconducting coil 10 or the container 11. The detectors include a bubble detector 40 that detects bubbles generated in liquid helium 13, a sonic detector 50 that captures sound waves generated by strain inside the superconductor and movement of the conductor, and a sonic detector 50 that detects sound waves generated by strain inside the superconductor and movement of the conductor. A speed detector 60, a magnetic detector 70, etc. are used to determine the electric field generated in the magnetic field.
Of these, the magnetic detector 70 is also used to determine the eddy current loss generated in the conductor.

これらの検出器信号値は転移の原因となる物理
量(気泡量、導体内に発生する電界の大きさ等)
に対応する。転移の原因となる物理量が閾値を越
えると、超電導装置に急激な転移が発生する。
These detector signal values are the physical quantities that cause the transition (the amount of bubbles, the size of the electric field generated within the conductor, etc.)
corresponds to When the physical quantity that causes the transition exceeds a threshold value, a rapid transition occurs in the superconducting device.

したがつて、超電導々体に通電中発生する転移
を防止するためには、これらの検出器信号のいず
れか、または組合せたものが、その各々に対して
あらかじめ設定しておいた警報レベルに達した場
合、通電々流を減少させるように電源の制御を行
い、転移の原因となる量を減少させればよい。
Therefore, in order to prevent transitions that occur while energizing a superconductor, one or a combination of these detector signals must reach a preset alarm level for each of them. In such a case, the power source may be controlled to reduce the current flow to reduce the amount that causes the transfer.

第2図を用いて上記を説明する。横軸は時間、
縦軸は転移原因に対応する物理量(例えば液体ヘ
リウム中の気泡量)である。時刻t1に、何らかの
理由で転移が発生したとする。この転移が増大し
て、時刻t3で閾値LTに越えると超電導々体全体に
転移が拡がり装置に危険を招く(同図Aの曲線)。
これを避けるため、警報レベルLAをLTより小さ
く設定し、その物理量が時刻t2でLAを越えれば装
置の通電々流を減少させるようにする。その物理
量はLTに達することなく転移の成長を防止する
ことができる(同図Bの曲線)。時刻t2で転移を
検出してから実際に通電電流の減少が行われるま
での間の時間遅れの影響(転移が消滅し始める前
にLTに致ることなど)は警報レベルの設定を低
くすることにより解決できる。
The above will be explained using FIG. The horizontal axis is time;
The vertical axis represents a physical quantity (for example, the amount of bubbles in liquid helium) corresponding to the cause of the transition. Assume that a transition occurs for some reason at time t1 . When this transition increases and exceeds the threshold L T at time t 3 , the transition spreads throughout the superconductor, posing a danger to the device (curve A in the figure).
In order to avoid this, the alarm level L A is set lower than L T , and if the physical quantity exceeds L A at time t 2 , the current flowing through the device is reduced. The physical quantity can prevent the growth of metastasis without reaching L T (curve B in the same figure). The effect of the time delay between detecting the transition at time t2 and actually reducing the applied current (such as reaching L T before the transition begins to disappear) can be avoided by setting the alarm level low. This can be resolved by doing so.

第3図は超電導装置の電流、転移原因に対応す
る物理量の変化、など検出器信号の時間的相関関
係を示す図である。
FIG. 3 is a diagram showing the temporal correlation of detector signals such as the current of the superconducting device and changes in physical quantities corresponding to causes of transition.

あらかじめ電源制御装置に与えられている電流
設定パターンはAである。この電流設定パターン
Aに従つて超電導装置に通電中、時刻t4において
転移が発生してそれに対応する物理量Cが増加
し、時刻t5に致つて警報レベルLAを越えたとす
る。この時検出器は検出器信号Dを出力し、電源
制御装置は電源に対し、転移原因に対応する物理
量がLAを越えない範囲で電流設定パターンAと
の偏差が常に最小となるように時刻t5〜t6の間制
御信号を送り、また時刻t6で転移が消滅した場
合、電源制御装置は電源に対して速やかにもとの
設定電流パターンAに戻るように指示し、結果と
して実線の電流パターンが得る。
The current setting pattern given to the power supply control device in advance is A. Assume that while the superconducting device is being energized according to this current setting pattern A, a transition occurs at time t4 , the corresponding physical quantity C increases, and exceeds the alarm level LA at time t5 . At this time, the detector outputs a detector signal D, and the power supply control device sends the power supply a time signal so that the deviation from the current setting pattern A is always minimized within the range where the physical quantity corresponding to the cause of the transition does not exceed L A. A control signal is sent between t 5 and t 6 , and if the transition disappears at time t 6 , the power supply control device instructs the power supply to immediately return to the original set current pattern A, and as a result, the solid line The current pattern is obtained.

電源制御装置のこのような機能は、アナログ、
デイジタルのいずれの回路形式によつても容易に
実現可能である。
These functions of power control equipment include analog,
It can be easily implemented using any digital circuit type.

以上のように、転移を防止しつつ、所定の設定
電流パターンとの偏差を最小にする超電導装置の
電源制御装置が得られる。
As described above, it is possible to obtain a power supply control device for a superconducting device that minimizes deviation from a predetermined set current pattern while preventing transition.

さらに超電導装置の実際の電流パターンと設定
電流パターンとの偏差の積分値が零になるよう制
御する方法は、通電々流の減少をよぎなくした転
移原因が消滅した後、設定電流パターンよりも電
流を大きくすればよい。第4図に従つてその方法
を説明する。図で時刻t6までは第3図と同じであ
るが、時刻t4に発生した転移原因が時刻t6で消滅
した後は通電々流の減少による偏差を零とするた
め、設定電流パターンAより多い電流を流すので
ある。当然、電流増加による転移原因に対応する
物理量C′(導体の発熱等に起因する)が警報レベ
ルLAを越える場合は、新たに電流増加による検
出器信号D′が発生するので、電源制御装置は電
源の出力を抑えて転移の発生を防ぐ。この電流増
加は転移を避けるために生じた設定電流パターン
による偏差の積分値を打消す時刻t7まで持続す
る。
Furthermore, the method of controlling the superconducting device so that the integral value of the deviation between the actual current pattern and the set current pattern becomes zero is to Just make it bigger. The method will be explained according to FIG. The diagram is the same as Figure 3 until time t 6 , but after the cause of the transition that occurred at time t 4 disappears at time t 6 , the set current pattern A It allows more current to flow. Naturally, if the physical quantity C' corresponding to the cause of transition due to the increase in current (due to heat generation in the conductor, etc.) exceeds the alarm level L A , a new detector signal D' due to the increase in current is generated, so the power supply control device suppresses the power output to prevent metastasis from occurring. This current increase continues until time t7 , when the integral value of the deviation due to the set current pattern, which occurs to avoid transition, is canceled out.

本実施例によれば転移を避けるために生じた電
流設定パターンに対する偏差の積分値を零にし
て、全体としての電流値を、あらかじめ設定した
電流パターンのそれと一致させることができる。
According to this embodiment, the integral value of the deviation with respect to the current setting pattern that occurs in order to avoid transition can be made zero, and the overall current value can be made to match that of the preset current pattern.

本発明によれば、超電導装置の転移を防止し、
所定の通電々流パターンと実際の通電々流パター
ンとの偏差を最小にする超電導装置の電源制御装
置が得られ、あらかじめ設定した電流パターンの
全電流値と一致させることができ、超電導装置の
最適でかつ経済的な運転方法が確立される。
According to the present invention, transition of a superconducting device is prevented,
A power supply control device for a superconducting device that minimizes the deviation between a predetermined energizing galvanic current pattern and an actual energizing galvanic current pattern can be obtained, and can match the total current value of a preset current pattern, thereby achieving an optimal superconducting device. A fast and economical driving method will be established.

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

第1図は本発明を応用した超電導装置の図、第
2図は検出器信号に現れる転移の原因となる量の
変化を示す図、第3図は超電導装置の電流と検出
器信号との関係を示す図(偏差を最小とする制御
の場合)、第4図は第3図と同様であるが、偏差
の積分を零とする制御の場合を示す図である。 10……超電導コイル、11……容器、12…
…液化装置、13……液体ヘリウム、20……電
源、30……電源制御装置、31……制御信号、
40……気泡検出器、50……音波検出器、60
……速度検出器、70……磁気検出器。
Fig. 1 is a diagram of a superconducting device to which the present invention is applied, Fig. 2 is a diagram showing changes in the amount that causes the transition that appears in the detector signal, and Fig. 3 is the relationship between the current of the superconducting device and the detector signal. FIG. 4 is the same as FIG. 3, but shows the case of control where the integral of the deviation is zero. 10... superconducting coil, 11... container, 12...
...Liquifier, 13...Liquid helium, 20...Power source, 30...Power control device, 31...Control signal,
40...Bubble detector, 50...Sound wave detector, 60
...Speed detector, 70...Magnetic detector.

Claims (1)

【特許請求の範囲】[Claims] 1 超電導装置の所定の電流パターンに従つた電
流が供給されるように電源を制御し、該超電導装
置の常電導転移現象の前兆を検出する検出器から
の信号が警報レベルに到達したとき、常電導転移
現象が発生しない範囲でかつ、該電流パターンと
の偏差が最小となる電流が該超電導装置に供給さ
れるよう該電源を制御する電源制御装置におい
て、常電導転移現象が抑えられた時点から、該電
流パターンに従つた電流に加え、電流減少時に生
じた該偏差の積分値とほぼ等しい量の電流を供給
した後、該電流パターンに従つた電流を該超電導
装置に供給するよう該電源を制御する機能を設け
たことを特徴とする超電導装置の電源制御装置。
1 The power source is controlled so that a current is supplied according to a predetermined current pattern of the superconducting device, and when the signal from the detector that detects the sign of the normal conduction transition phenomenon of the superconducting device reaches an alarm level, In a power supply control device that controls the power supply so that a current is supplied to the superconducting device within a range where the conductive transition phenomenon does not occur and the deviation from the current pattern is minimal, from the time when the normal conductive transition phenomenon is suppressed. , in addition to the current according to the current pattern, the power supply is supplied with an amount of current approximately equal to the integral value of the deviation that occurs when the current decreases, and then the power supply is configured to supply the current according to the current pattern to the superconducting device. A power supply control device for a superconducting device characterized by having a control function.
JP2705081A 1981-02-27 1981-02-27 Power source controlling device of super conduction device Granted JPS57141904A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2705081A JPS57141904A (en) 1981-02-27 1981-02-27 Power source controlling device of super conduction device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2705081A JPS57141904A (en) 1981-02-27 1981-02-27 Power source controlling device of super conduction device

Publications (2)

Publication Number Publication Date
JPS57141904A JPS57141904A (en) 1982-09-02
JPS6331091B2 true JPS6331091B2 (en) 1988-06-22

Family

ID=12210239

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2705081A Granted JPS57141904A (en) 1981-02-27 1981-02-27 Power source controlling device of super conduction device

Country Status (1)

Country Link
JP (1) JPS57141904A (en)

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2618955B1 (en) * 1987-07-29 1990-05-11 Hitachi Ltd SUPERCONDUCTING ENERGY STORAGE DEVICE
US4989989A (en) * 1989-08-31 1991-02-05 Westinghouse Electric Corp. Hydraulic sensor for quench detection and location in superconductors
JP4705844B2 (en) * 2005-12-09 2011-06-22 株式会社日立製作所 Superconducting coil abnormality detection device
JP5175593B2 (en) * 2008-03-31 2013-04-03 株式会社東芝 Superconducting coil device, superconducting coil abnormality detecting device, and superconducting coil device operating method
JP5877397B2 (en) * 2011-09-08 2016-03-08 国立研究開発法人物質・材料研究機構 Superconducting coil protection method and superconducting magnet device
GB201801604D0 (en) * 2018-01-31 2018-03-14 Tokamak Energy Ltd magnetic quench induction system
JP7313933B2 (en) * 2019-07-01 2023-07-25 株式会社東芝 Superconducting magnet device and control method for superconducting magnet device
JP7377087B2 (en) * 2019-12-10 2023-11-09 住友重機械工業株式会社 Superconducting magnet device and superconducting magnet control method

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6041211B2 (en) * 1977-09-03 1985-09-14 ヤマハ発動機株式会社 multi-cylinder internal combustion engine

Also Published As

Publication number Publication date
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