WO2006115126A1 - 超電導コイルのクエンチ検出方法と装置および超電導電力貯蔵装置 - Google Patents
超電導コイルのクエンチ検出方法と装置および超電導電力貯蔵装置 Download PDFInfo
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- WO2006115126A1 WO2006115126A1 PCT/JP2006/308141 JP2006308141W WO2006115126A1 WO 2006115126 A1 WO2006115126 A1 WO 2006115126A1 JP 2006308141 W JP2006308141 W JP 2006308141W WO 2006115126 A1 WO2006115126 A1 WO 2006115126A1
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- Prior art keywords
- voltage
- coil
- superconducting coil
- superconducting
- taenchi
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Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/02—Quenching; Protection arrangements during quenching
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/006—Supplying energising or de-energising current; Flux pumps
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02H—EMERGENCY PROTECTIVE CIRCUIT ARRANGEMENTS
- H02H7/00—Emergency protective circuit arrangements specially adapted for specific types of electric machines or apparatus or for sectionalised protection of cable or line systems, and effecting automatic switching in the event of an undesired change from normal working conditions
- H02H7/001—Emergency protective circuit arrangements specially adapted for specific types of electric machines or apparatus or for sectionalised protection of cable or line systems, and effecting automatic switching in the event of an undesired change from normal working conditions for superconducting apparatus, e.g. coils, lines, machines
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—ELECTRIC POWER NETWORKS; CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J3/00—Circuit arrangements for AC mains or AC distribution networks
- H02J3/18—Arrangements for adjusting, eliminating or compensating reactive power in networks
- H02J3/1821—Arrangements for adjusting, eliminating or compensating reactive power in networks using shunt compensators
- H02J3/1835—Arrangements for adjusting, eliminating or compensating reactive power in networks using shunt compensators with stepless control
- H02J3/1842—Arrangements for adjusting, eliminating or compensating reactive power in networks using shunt compensators with stepless control having reactive elements actively controlled by bridge converters, e.g. active filters or static compensators [STATCOM]
- H02J3/185—Arrangements for adjusting, eliminating or compensating reactive power in networks using shunt compensators with stepless control having reactive elements actively controlled by bridge converters, e.g. active filters or static compensators [STATCOM] the reactive elements being purely inductive, e.g. superconductive magnetic energy storage [SMES] systems
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- 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
- Y02E40/20—Active power filtering [APF]
-
- 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
Definitions
- the present invention relates to a superconducting coil, in particular, a superconducting coil suitable for detecting a superconducting coil for which an induced voltage is continuously generated for power system control or instantaneous voltage drop compensation.
- the present invention relates to a method and apparatus and a superconducting power storage device.
- the simplest Taenchi detection method is a method of monitoring the absolute value of the voltage across the superconducting coil. This method detects changes in the output voltage of the current source due to the resistance of the superconducting coil. It is a simple force Because it is necessary to set the detection voltage so that the induced voltage at the time of excitation and demagnetization of the superconducting coil is not erroneously detected, it is small enough that the excitation voltage is about several volts and the detection voltage can be simultaneously set to several volts or more. Often applied to superconducting coils. In general, a superconducting coil is short-circuited at both ends by a protective resistor or semiconductor element, so the maximum voltage input to the Taenti detector is determined by the resistance or the voltage across the semiconductor element.
- the detection voltage at the time of turning is set smaller than the induced voltage at the time of excitation and demagnetization of the superconducting coil.
- a widely used method is to divide the superconducting coil and to obtain the difference voltage between both sections. Is a method of monitoring. When the superconducting coil is composed of a plurality of element coils, it may be divided at the midpoint of the element coil group. In this method, the difference voltage between the two sections with equal division of the inductance is monitored, so it is possible to detect the occurrence of a minute abnormal voltage by eliminating the induced voltage. In practice, it is necessary to make fine adjustments on the quench detector side to compensate for the inductance difference in each divided section.
- the voltage at the midpoint of the superconducting coil may be higher than the voltage at both ends of the coil depending on the type of Taenti. Therefore, a protection circuit that circulates the coil current is configured for each section divided at the midpoint, and the maximum voltage is generally limited by providing a resistor and a semiconductor element for each circuit.
- Patent Document 1 Japanese Patent Laid-Open No. 6-333739
- Patent Document 2 JP-A-9-260130
- Patent Document 3 Japanese Patent Publication No. 5-58246
- Patent Document 4 Japanese Patent Publication No. 6-56811
- fly Pinch detection needs to detect an abnormal voltage that is 4 orders of magnitude smaller than the induced voltage and at the same time have a withstand voltage of several tens of kV.
- a voltage signal is resistance-divided and input to a high-voltage isolation amplifier as in general high-voltage measurement, it will be difficult to ensure sufficient sensitivity as the detection voltage decreases. There is.
- the element coils operated by separate power sources are close to each other! In this case, it is necessary to cancel the mutual induction from the element coil operated by another power source. Furthermore, voltage sharing may differ between element coils due to potential oscillation, and it may be difficult to completely cancel the induced voltage with the conventional method of taking the differential voltage. In this case, in order to avoid misjudgment of Taenti, the detection voltage is set to a certain level, which causes a problem that a minute voltage cannot be detected.
- the present invention provides a superconducting coil in which a plurality of element coils are connected to a plurality of current sources and repeatedly operated in a pulse or an alternating current, and several kV is continuously applied as an induced voltage. It is an object of the present invention to provide a superconducting coil quench detection method and apparatus, and a superconducting power storage device capable of detecting a detection voltage at the time of turning. Means for solving the problem
- a superconducting coil Taenchi detection device includes a pickup coil provided in or near the superconducting coil, a voltage generated in the superconducting coil when the superconducting coil is energized, and a voltage induced in the pickup coil. And an overvoltage protection circuit that outputs a voltage signal that is less than or equal to a predetermined value and a Taenchi detector that receives the voltage signal and detects the Taenchi of the superconducting coil. Toss The
- the superconducting coil Taenti detection method is a superconducting coil Taenchi that detects a resistance component in the superconducting coil by measuring a voltage with an inductive component canceled out of the generated voltage of the superconducting coil.
- overvoltage protection is performed so that the maximum value of the voltage to be measured does not exceed a predetermined voltage.
- the superconducting power storage device includes a pickup coil provided in or near the superconducting coil, and a difference between a voltage generated in the superconducting coil and a voltage induced in the pickup coil when the superconducting coil is turned.
- a superconducting coil quench detection device comprising: an overvoltage protection circuit that inputs a voltage of a predetermined value and outputs a voltage signal equal to or less than a predetermined value; and a taenti detector that receives the voltage signal and detects the taenchi of the superconducting coil. It is characterized by having.
- FIG. 1 (a) is a circuit diagram showing a superconducting coil Taenchi detection device according to a first embodiment of the present invention, and (b) is a circuit diagram of a modification of (a).
- FIG. 2 (a) is a circuit diagram showing a superconducting coil Taenchi detection device according to a second embodiment of the present invention, and (b) is a circuit diagram of a modification of (a).
- FIG. 3 (a) is a circuit diagram showing a superconducting coil Taenchi detection device according to a third embodiment of the present invention, and (b) is a circuit diagram of a modification of (a).
- FIG. 4 (a) is a circuit diagram showing a superconducting coil Taenti detection device according to a fourth embodiment of the present invention, and (b) is a circuit diagram of a modification of (a).
- FIG. 5 (a) is a circuit diagram showing a superconducting coil Taenchi detection device according to a fifth embodiment of the present invention
- FIG. 5 (b) is a circuit diagram of a modification of (a).
- FIG. 6 (a) is a circuit diagram showing a superconducting coil Taenchi detection device according to a sixth embodiment of the present invention, and (b) is a circuit diagram of a modification of (a).
- 7] (a) is a circuit diagram showing a superconducting coil Taenchi detection device according to a seventh embodiment of the present invention, and (b) is a circuit diagram of a modification of (a).
- FIG. 8 is a circuit diagram showing a quench detection apparatus for a superconducting coil according to an eighth embodiment (a) of the present invention and its modification (b).
- (a) is a circuit diagram showing a superconducting coil Taenchi detection device according to an eighth embodiment of the present invention, and (b) is a circuit diagram of a modification of (a).
- FIG. 10 (a) is a circuit diagram showing a superconducting power storage device equipped with a superconducting coil Taenchi detection device according to a tenth embodiment of the present invention, and (b) is a circuit diagram of a modification of (a). is there. Explanation of symbols
- FIG. 1 (a) is a circuit diagram showing a first embodiment of the present invention.
- the tungsten detector according to the present embodiment includes a pickup coil 2 provided in the vicinity of the superconducting coil 1 connected to the current source 10 through the current limiting resistor 5, a voltage VA between the terminals of the superconducting coil 1 and the pickup coil.
- pick-up coil 2 is arranged at a position where the magnetic field generated by superconducting coil 1 can be sensed. Then, the voltage obtained by eliminating the inductive component in the subtractor 17 from the excitation demagnetizing voltage of the superconducting coil 1 is input to the Taenti detector 3 through the overvoltage protection circuit 4.
- the overvoltage protection circuit 4 shorts the input signals when the input voltage reaches the threshold value. This prevents an excessive voltage from being applied to the Taenti detector 3 and protects the Taenti detector 3.
- the threshold is selected, for example, within a range of less than 600V.
- V can be calculated by multiplying the signal of the pickup coil 2 by a constant, or the current signal force inductive component of the current limiting resistor 5 can be reduced without using the pickup coil 2. It may be calculated. In this case, the calculation and calculation conditions are selected by looking at each output when the superconducting coil 1 is energized at a current value smaller than the rated value.
- a graph showing the relationship between voltage V and time T at each position on the circuit is also shown.
- the force-current waveform showing the case of sine wave AC energization may be arbitrary.
- the signal input to Taenti detector 3 may have a potential of 600V or more with respect to the ground, so you can leave the Taent detector 3 floating without grounding it! And, you can increase the withstand voltage for the earth!
- a voltage signal is converted into an optical signal by optical converters 6a and 6b and transmitted, and then converted into a voltage signal by voltage change and input to overvoltage protection circuit 4. It is good also as a structure.
- the optical converters 6a and 6b for converting the voltage signal into the optical signal may be buoyant with the potential without being grounded with respect to the ground. The withstand voltage may be increased.
- the overvoltage protection circuit 4 has a protection voltage of less than 600V because it is within the range of low-voltage work, and it is more desirable that the maximum input voltage of the instrument be less than 200V.
- the Taenti detector 3 detects Taenchi, it performs a stop operation to stop energization of the superconducting coil 1 at an early stage. Specifically, the current source 10 is disconnected, and switching is performed so that a current flows through a protective resistor (not shown) parallel to the current source 10.
- a zero level voltage signal with the inductive component canceled is input to the Taenti detector 3 without reducing the signal by resistance voltage division or the like, and at the same time, maximum voltage is applied by applying overvoltage protection.
- an isolating amplifier for high voltage is not required on the detector side, and it is possible to detect even abnormal voltages below IV with high accuracy. Therefore, it is possible to avoid the problem that it is difficult to obtain sufficient detection sensitivity for an abnormal voltage of less than IV when an insulation amplifier for high voltage is used.
- FIG. 2 is a block diagram showing a second embodiment of the method and apparatus for detecting the superconducting coil according to the present invention.
- FIG. 2 (a) and Fig. 2 (b) show that superconducting coil 1 and pickup coil 2 are configured by combining superconducting wire 7 and subconductor 8.
- the sub conductor 8 operates as the pickup coil 2.
- the superconducting wire 7 and the subconductor 8 are electrically insulated from each other, but are electrically connected at one place, and the superconducting wire 7 and the subconductor 8 are at the same potential at the connection position.
- the superconducting wire 7 may be a bundled wire obtained by bundling a plurality of superconducting wires, or may be a stranded wire.
- the shape and material of the subconductor 8 are not limited, and may be the same shape as the superconducting wire 7, or the subconductor 8 may be a shape covering the periphery of the superconducting wire 7.
- the subconductor 8 may be a superconducting wire different from the superconducting wire 7.
- Inductive voltage of superconducting coil 1 by measuring the voltage (difference voltage) ⁇ between superconducting wire 7 and subconductor 8 at the end opposite to the side where superconducting wire 7 and subconductor 8 are at the same potential Cancel this voltage
- the signal is used as an input signal to Taenti detector 3.
- superconducting wire 7 and subconductor 8 are set to the same potential in one place. However, when superconducting coil 1 is also configured with a plurality of element coil forces and there are a plurality of independent electric circuits, it is independent.
- the superconducting wire 7 and the secondary conductor 8 may be connected for each circuit.
- the superconducting wire 7 and the subconductor 8 may be completely electrically insulated, and the respective voltages may be detected individually, and the induced voltage may be subtracted on the Taenti detector 3 side.
- the subconductor 8 wound in a coil shape together with the superconducting wire 7 is provided, so that the induced voltage of the pick-up coil 2 is increased.
- the potential oscillation effect agrees well with that of the superconducting coil 1, and the induced voltage can be canceled satisfactorily even when the potential vibration is significant. It is possible to realize a Taenti detection device with high accuracy.
- FIG. 3 is a block diagram showing a third embodiment of the present invention.
- FIG. 3 (a) and Fig. 3 (b) shows the same as in Fig. 2 (a) and Fig. 2 (b).
- 8 shows the cross-sectional shape when superconducting coil 1 and pickup coil 2 are configured in combination with 8.
- the superconducting coil 1 and the pick-up coil 2 are constructed by jointing the superconducting wire 7 and the subconductor 8 together.
- the figures surrounded by dotted lines in the lower left corners of FIGS. 3 (a) and 3 (b) are enlarged cross-sectional views of a part of the figures enclosed by dotted lines in the upper left corners.
- the secondary conductor 8 that forms the pick-up coil 2 together with the superconducting wire 7 that forms the superconducting coil 1 is composed of a high mechanical strength member made of stainless steel, copper alloy, or aluminum alloy.
- the shape of the sub-conductor 8 can be various.
- an insulating coating 20 As a means for electrically insulating the superconducting wire 7 and the subconductor 8 from each other, either one or both of the superconducting wire 7 and the conductor 8 are covered with an insulating coating 20.
- the insulation coating 20 may be coated with an insulating material, or an insulating tape or prepreg may be applied! /.
- the secondary conductor 8 serves as a coil reinforcement and also serves as the pickup coil 2. Therefore, it is possible to realize a high-precision Taenthi detection device with high efficiency and low cost.
- the superconducting coil 1 is composed of two element coils 9 and is energized in series by one current source 10.
- the number of element coils 9 is not limited to two and may be three or more.
- the number of current sources may be one or more, but it is desirable to operate each power supply in synchronization.
- Each element coil 9 has the coil structure described in the third embodiment, and a signal ⁇ obtained by canceling the induced voltage in each set of element coil 9 and pickup coil 2 is input to the Taenti detector 3. And monitor the difference between the voltage signals.
- the superconducting coil 1 when the superconducting coil 1 is composed of a plurality of element coils 9, the voltage obtained by canceling the inductive component is measured for each element coil 9, and the difference voltage ⁇ between them is measured. To monitor. As a result, it avoids the problem that the detection sensitivity is not sufficient when the induced voltage that remains minutely without cancellation is larger than the quench detection voltage, and realizes highly accurate Taenchi detection. In addition, when the number of element coils is large, it is possible to realize an efficient Taenchi detector with a reduced number of Taenchi detectors.
- the superconducting wire 1 and the pick-up coil 2 are formed by co-wiring the superconducting wire 7 and the subconductor 8, and the superconducting coil 1 and the pick-up coil are formed.
- the semiconductor element 11 is connected between 2 and the voltage ⁇ across the semiconductor element 11 is input to the Taenti detector 3 to monitor Taenti.
- the semiconductor element 11 is normally open. When the superconducting coil 1 is turned, it closes and is electrically short-circuited at the connecting portion between the superconducting coil 1 and the pickup coil 2. At this time, the semiconductor element 11 is selected so that the differential voltage ⁇ V between the superconducting coil 1 and the pickup coil 2 does not exceed 600V! /.
- the voltage signal is short-circuited by closing the switch by the semiconductor element 11, so that the maximum voltage input to the Taenti detector is set to the semiconductor element.
- the semiconductor element 11 is connected to the input terminal of the coil voltage signal from which the induced voltage is canceled. After progress, the maximum value of the detection voltage ⁇ V can be limited by the voltage across the forward direction of the semiconductor element 11. Therefore, a highly accurate Taenti detection device can be realized without using a high-voltage amplifier. Can do.
- the present embodiment is a cryostat in which the superconducting coil 1 and the pickup coil 2 are housed in the fifth embodiment (FIG. 5).
- the semiconductor device 11 is provided inside.
- FIG. 5 the illustration of the cryostat 12 is omitted.
- the superconducting coil 1, the pick-up coil 2, the current limiting resistor 5, and the current source 10 are in the cryostat 12, and the semiconductor element 11 is outside the cryostat 12. Arranged in
- connection of the semiconductor element 11 requires a current capacity that can cope with the current that flows when the semiconductor element 11 is closed.
- the semiconductor element 11 since the semiconductor element 11 is provided inside the cryostat 12, the current circuit that flows when the semiconductor element 11 is closed is housed inside the cryostat 12. Therefore, it is sufficient to take out only the signal line for measurement outside the cryostat 12, and the problem of having to take out a thick electric cable with current carrying capacity can be avoided.
- the semiconductor element 11 is provided inside the cryostat 12, a compact superconducting coil device in which the signal line for detecting the tentiency that is taken out of the cryostat 12 is thinned. As well as a compact Taenti detector.
- a diode 13 is connected between the terminals of the superconducting coil 1 and the pickup coil 2 as shown in FIGS. 7 (a) and 7 (b).
- the diode 13 may be a surge absorber or a varistor instead of a diode, or an element such as an arrester, or another switch element that does not require control.
- the diode 13 is installed in a temperature environment similar to that of the superconducting coil 1 to take advantage of the temperature dependence of the forward voltage. Thus, the forward voltage may be increased.
- a plurality of semiconductor elements may be connected in series or in parallel. In that case, different types of elements may be combined.
- diode 13 which is a semiconductor element that does not need to be controlled from the outside is used, reliability of opening / closing control of the semiconductor element is required when superconducting coil 1 is turned. To avoid the problem.
- this embodiment uses a diode that does not require external control of opening and closing, a highly reliable Taenti detection device that operates passively can be realized.
- a thyristor 14 is connected between the terminals of the superconducting coil 1 and the pickup coil 2.
- Thyristor 14 may be a GTO, or an IGBT instead of a thyristor! / ⁇ may be an IEGT! / ⁇ may be another element that can be controlled.
- a plurality of these semiconductor elements may be configured in series or in parallel. In that case, different types of elements may be combined.
- the semiconductor element that can be controlled from the outside as described above since the semiconductor element that can be controlled from the outside as described above is used, the problem that the opening and closing cannot be freely controlled when a passively operating semiconductor element is used can be avoided.
- the present embodiment uses a semiconductor element that can be controlled from the outside to open and close, so that a taenti detection device capable of freely setting the interlock operation of the current source 10 is realized. can do.
- a resistor 15 is connected between the terminals of the superconducting coil 1 and the pickup coil 2 as shown in FIGS.
- the resistance value of the resistor 15 is selected so that the voltage ⁇ generated at both ends of the resistor 15 when the superconducting coil 1 is turned is less than 600V.
- the abnormal signal of the superconducting coil 1 is divided by the impedance of the pickup coil 2 and the resistor 15, so that the detection signal is reduced, but the high voltage is easily applied. It is possible to avoid input to the anchor detector 3. Therefore, if the problem does not become a problem even if the abnormal signal is reduced by the resistance voltage division, it is bothersome to take special measures against overvoltage.
- the abnormal signal from the superconducting coil 1 is divided by the impedance of the pickup coil 2 and the resistance of the resistor 15 and input to the Taenti detector 3. It is possible to realize a taenti detector that avoids voltage.
- the superconducting coil 1 constitutes a superconducting power storage device 16.
- the superconducting power storage device 16 may be used for instantaneous voltage drop compensation, or for system control such as system stability, load fluctuation compensation, or frequency adjustment.
- the superconducting power storage device is provided with the Taenti detection device of the first to ninth embodiments, so that a plurality of element coils are repeatedly operated by a plurality of current sources, or a pulse operation or an AC operation. Even in this case, it is possible to avoid the problem that it is difficult to detect a minute voltage, and to realize taenchi detection with high accuracy.
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Abstract
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Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US11/918,673 US7898778B2 (en) | 2005-04-19 | 2006-04-18 | Superconducting coil quench detection method and device, and superconducting power storage unit |
| EP06745423.1A EP1876609A4 (en) | 2005-04-19 | 2006-04-18 | METHOD AND DEVICE FOR DETECTING SUPER-CONDUCTIVE COIL INHIBITION AND SUPER-CONDUCTIVE ENERGY STORAGE UNIT |
| JP2007514611A JP4929165B2 (ja) | 2005-04-19 | 2006-04-18 | 超電導コイルのクエンチ検出方法と装置および超電導電力貯蔵装置 |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2005-121104 | 2005-04-19 | ||
| JP2005121104 | 2005-04-19 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| WO2006115126A1 true WO2006115126A1 (ja) | 2006-11-02 |
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Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/JP2006/308141 Ceased WO2006115126A1 (ja) | 2005-04-19 | 2006-04-18 | 超電導コイルのクエンチ検出方法と装置および超電導電力貯蔵装置 |
Country Status (4)
| Country | Link |
|---|---|
| US (1) | US7898778B2 (ja) |
| EP (1) | EP1876609A4 (ja) |
| JP (1) | JP4929165B2 (ja) |
| WO (1) | WO2006115126A1 (ja) |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2006332513A (ja) * | 2005-05-30 | 2006-12-07 | Toshiba Corp | 超電導コイル装置 |
| JP2012023168A (ja) * | 2010-07-14 | 2012-02-02 | Hitachi Ltd | 超電導コイル、超電導マグネットおよびその運転方法 |
| WO2013035669A1 (ja) | 2011-09-08 | 2013-03-14 | 独立行政法人物質・材料研究機構 | 超伝導コイルの保護方法、および超伝導磁石装置 |
| WO2014064994A1 (ja) * | 2012-10-24 | 2014-05-01 | 住友重機械工業株式会社 | 超電導コイルのクエンチ検出装置 |
| JP2022549132A (ja) * | 2019-09-23 | 2022-11-24 | オックスフォード インストルメンツ ナノテクノロジー ツールス リミテッド | クエンチ保護装置 |
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| JP5180783B2 (ja) * | 2008-11-12 | 2013-04-10 | 三菱重工業株式会社 | 超電導コイルクエンチの検出装置及び検出方法 |
| US20110152102A1 (en) * | 2009-12-22 | 2011-06-23 | John H Claassen | Device and method of measuring electrical dissipation in a superconducting coil |
| GB201200614D0 (en) | 2012-01-16 | 2012-02-29 | Rolls Royce Plc | Cryogenic power control |
| KR101444814B1 (ko) | 2013-06-25 | 2014-09-26 | 한국전기연구원 | 전도냉각형 초전도 코일의 ?치시 온도 예측 방법 |
| DE102016208226A1 (de) * | 2016-05-12 | 2017-11-16 | Bruker Biospin Ag | Kryogenfreies Magnetsystem mit magnetokalorischer Wärmesenke |
| KR102338894B1 (ko) * | 2018-01-30 | 2021-12-13 | 토카막 에너지 리미티드 | 극저온 시스템의 모니터 장치 |
| GB201904528D0 (en) | 2019-04-01 | 2019-05-15 | Tokamak Energy Ltd | Partial insulation with diagnostic pickup coils |
| CN113764750A (zh) * | 2021-09-07 | 2021-12-07 | 上海海事大学 | 高温超导储能监测系统 |
| FR3151936B1 (fr) * | 2023-08-03 | 2026-01-02 | Airbus | Procede ameliore de detection d’un phenomene de quench, systeme executant le procede, et aeronef. |
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| JPH0656811B2 (ja) | 1988-04-14 | 1994-07-27 | 三菱電機株式会社 | 超電導コイルのクエンチ検出装置 |
| US4978922A (en) * | 1989-08-31 | 1990-12-18 | Westinghouse Electric Corp. | Superconducting sensor for quench detection in a superconductor |
| US4996472A (en) * | 1989-08-31 | 1991-02-26 | Westinghouse Electric Corp. | Passive superconducting quench detection sensor |
| US5067044A (en) | 1990-03-05 | 1991-11-19 | Westinghouse Electric Corp. | Sensor for detecting a quench in a superconductor using an optical coupling |
| JPH04346207A (ja) * | 1991-05-23 | 1992-12-02 | Showa Electric Wire & Cable Co Ltd | 交流用超電導コイルの監視装置 |
| JPH06333739A (ja) | 1993-05-21 | 1994-12-02 | Hitachi Ltd | 超電導コイルシステム |
| JP3419986B2 (ja) | 1996-03-27 | 2003-06-23 | 財団法人鉄道総合技術研究所 | 超電導コイル通電線の保護方法及びその装置 |
| JPH11288809A (ja) * | 1998-03-31 | 1999-10-19 | Toshiba Corp | 超電導マグネット装置 |
| DE29923845U1 (de) * | 1999-11-19 | 2001-06-13 | Siemens AG, 80333 München | Anordnung zur elektrischen Energieversorgung |
| JP4220518B2 (ja) | 2003-12-12 | 2009-02-04 | 株式会社日立製作所 | エンジンの制御装置 |
-
2006
- 2006-04-18 US US11/918,673 patent/US7898778B2/en active Active
- 2006-04-18 EP EP06745423.1A patent/EP1876609A4/en not_active Withdrawn
- 2006-04-18 WO PCT/JP2006/308141 patent/WO2006115126A1/ja not_active Ceased
- 2006-04-18 JP JP2007514611A patent/JP4929165B2/ja not_active Expired - Fee Related
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| JPS61289611A (ja) * | 1985-06-18 | 1986-12-19 | Toshiba Corp | クエンチ検出器の保護装置 |
| JPS633405A (ja) * | 1986-06-24 | 1988-01-08 | Mitsubishi Electric Corp | 超電導装置用保護回路 |
| JPH05316633A (ja) * | 1992-05-08 | 1993-11-26 | Kansai Electric Power Co Inc:The | 超電導コイルのクエンチ検出装置 |
| JPH08138927A (ja) * | 1994-11-02 | 1996-05-31 | Kansai Electric Power Co Inc:The | 超電導コイルクエンチ検出装置 |
| JPH0984252A (ja) * | 1995-09-12 | 1997-03-28 | Mitsubishi Electric Corp | 超電導コイルクエンチ検出装置 |
Non-Patent Citations (1)
| Title |
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Cited By (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2006332513A (ja) * | 2005-05-30 | 2006-12-07 | Toshiba Corp | 超電導コイル装置 |
| JP2012023168A (ja) * | 2010-07-14 | 2012-02-02 | Hitachi Ltd | 超電導コイル、超電導マグネットおよびその運転方法 |
| WO2013035669A1 (ja) | 2011-09-08 | 2013-03-14 | 独立行政法人物質・材料研究機構 | 超伝導コイルの保護方法、および超伝導磁石装置 |
| US9543754B2 (en) | 2011-09-08 | 2017-01-10 | National Institute For Materials Science | Superconducting coil protection method and superconducting magnet device |
| WO2014064994A1 (ja) * | 2012-10-24 | 2014-05-01 | 住友重機械工業株式会社 | 超電導コイルのクエンチ検出装置 |
| JP2014086584A (ja) * | 2012-10-24 | 2014-05-12 | Sumitomo Heavy Ind Ltd | 超電導コイルのクエンチ検出装置 |
| CN104756205A (zh) * | 2012-10-24 | 2015-07-01 | 住友重机械工业株式会社 | 超导线圈的失超检测装置 |
| US9568569B2 (en) | 2012-10-24 | 2017-02-14 | Sumitomo Heavy Industries, Ltd. | Device for detecting quench in superconducting coil |
| CN104756205B (zh) * | 2012-10-24 | 2017-08-22 | 住友重机械工业株式会社 | 超导线圈的失超检测装置 |
| JP2022549132A (ja) * | 2019-09-23 | 2022-11-24 | オックスフォード インストルメンツ ナノテクノロジー ツールス リミテッド | クエンチ保護装置 |
| JP7624000B2 (ja) | 2019-09-23 | 2025-01-29 | オックスフォード インストルメンツ ナノテクノロジー ツールス リミテッド | クエンチ保護装置 |
Also Published As
| Publication number | Publication date |
|---|---|
| EP1876609A4 (en) | 2014-08-20 |
| EP1876609A1 (en) | 2008-01-09 |
| JPWO2006115126A1 (ja) | 2008-12-18 |
| JP4929165B2 (ja) | 2012-05-09 |
| US7898778B2 (en) | 2011-03-01 |
| US20090046399A1 (en) | 2009-02-19 |
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