JP2013037767A - Magnetization rush current suppression device - Google Patents

Magnetization rush current suppression device Download PDF

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JP2013037767A
JP2013037767A JP2011170227A JP2011170227A JP2013037767A JP 2013037767 A JP2013037767 A JP 2013037767A JP 2011170227 A JP2011170227 A JP 2011170227A JP 2011170227 A JP2011170227 A JP 2011170227A JP 2013037767 A JP2013037767 A JP 2013037767A
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phase
voltage
transformer
magnetic flux
residual magnetic
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JP5740240B2 (en
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Tadashi Koshizuka
正 腰塚
Kei Kawasaki
圭 川崎
Minoru Saito
実 齋藤
Shiro Maruyama
志郎 丸山
Tokuyuki Nagayama
徳幸 長山
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Toshiba Corp
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Abstract

PROBLEM TO BE SOLVED: To provide a magnetization rush current suppression device which can control the closing phase for suppressing magnetization rush current of a circuit breaker that opens/closes connection of a three-phase AC power system including a power supply and a grounded transformer for converting the three-phase AC voltage into a single-phase AC voltage.SOLUTION: A magnetization rush current suppression device 6 which suppresses a magnetization rush current of a circuit breaker 2 that opens/closes the connection of a power supply bus 1 and a grounded deformation Woodbridge connection transformer 3 for each phase calculates the steady-state flux of the transformer 3 by measuring the three-phase AC voltage of the power supply bus 1, and calculates the residual flux of three-phases of the transformer 3 after interruption by measuring the single-phase AC voltage of the transformer 3. The circuit breaker 2 in a phase having the maximum value of residual flux is closed in a phase where the steady-state flux matches the residual flux, and the circuit breakers 2 in two remaining phases are closed in a phase where the phase voltage of the closed phase becomes the zero point upon elapsing a preset time.

Description

本発明は、遮断器を投入する際に生じる励磁突入電流を抑制する励磁突入電流抑制装置に関する。   The present invention relates to a magnetizing inrush current suppressing device that suppresses an magnetizing inrush current generated when a circuit breaker is turned on.

一般に、変圧器鉄心に残留磁束がある状態で電源投入により無負荷励磁を行うと、大きな励磁突入電流が流れることが知られている。この励磁突入電流の大きさは変圧器の定格負荷電流の数倍になる。このように大きな励磁突入電流が流れると、系統電圧が変動し、その電圧変動が大きい場合、需要者に影響を与えることがある。   In general, it is known that when no-load excitation is performed by turning on the power in a state where there is a residual magnetic flux in the transformer core, a large excitation inrush current flows. The magnitude of this magnetizing inrush current is several times the rated load current of the transformer. When such a large magnetizing inrush current flows, the system voltage fluctuates, and if the voltage fluctuation is large, the consumer may be affected.

このため、励磁突入電流を抑制する方法として、投入抵抗と接点とが直列に接続された抵抗体付き遮断器を用いることが知られている。抵抗体付き遮断器は、遮断器主接点と並列に接続する。この抵抗体付き遮断器は、遮断器主接点に先行して投入する。これにより、励磁突入電流が抑制される。   For this reason, as a method for suppressing the magnetizing inrush current, it is known to use a breaker with a resistor in which a making resistor and a contact are connected in series. The breaker with resistor is connected in parallel with the breaker main contact. This breaker with a resistor is inserted prior to the main contact of the breaker. Thereby, the magnetizing inrush current is suppressed.

また、他の抑制方法として、直接接地系の三相変圧器を3台の単相型遮断器で投入する際、任意の1相を先行投入し、その後に残りの2相を投入させるようにして励磁突入電流を抑制する方法が知られている。   As another suppression method, when a three-phase transformer with direct grounding is inserted with three single-phase circuit breakers, an arbitrary one phase is introduced first, and then the remaining two phases are introduced. There is a known method for suppressing the magnetizing inrush current.

さらに、非有効接地系の三相変圧器を三相一括操作型遮断器で投入する際の励磁突入電流を抑制する方法として、変圧器が遮断された時の鉄心に残留する磁束の値を計測し、変圧器投入時の励磁突入電流を遮断器の投入位相を制御することが知られている。   Furthermore, as a method of suppressing the inrush current when a non-effective grounding type three-phase transformer is turned on with a three-phase batch operation type circuit breaker, the value of the magnetic flux remaining in the iron core when the transformer is cut off is measured. In addition, it is known to control the closing phase of the circuit breaker with the magnetizing inrush current when the transformer is turned on.

一方、三相交流電圧を単相交流電圧に変換する方法として、スコット結線、ウッドブリッジ結線変圧器、又は変形ウッドブリッジ結線等が知られている。これらの結線の変圧器は、例えば、単相電気炉又は単相交流電気車などに給電する場合に用いられる。   On the other hand, as a method for converting a three-phase AC voltage into a single-phase AC voltage, a Scott connection, a Woodbridge connection transformer, a modified Woodbridge connection, or the like is known. These connection transformers are used, for example, when power is supplied to a single-phase electric furnace or a single-phase AC electric vehicle.

特開2002−75145号公報JP 2002-75145 A 特開2008−160100号公報JP 2008-160100 A 特開2008−140580号公報JP 2008-140580 A

John H.Brunke、外1名,“Elimination of Transformer Inrush Currents by Controlled Switching -Part I: Theoretical Considerations”, IEEE TRANSACTIONS ON POWER DELIVERY, IEEE,2001年4月,Vol.16,No.2,p.276−280John H. Brunke, 1 other, “Elimination of Transformer Inrush Currents by Controlled Switching -Part I: Theoretical Considerations”, IEEE TRANSACTIONS ON POWER DELIVERY, IEEE, April 2001, Vol. 16, no. 2, p. 276-280

しかしながら、上述のような励磁突入電流を抑制する方法では、以下のような問題がある。   However, the method for suppressing the magnetizing inrush current as described above has the following problems.

抵抗体付き遮断器による励磁突入電流抑制方法では、通常の遮断器に対して抵抗体付き遮断器を付加する必要があるため、遮断器全体としてみた場合、大型化してしまう。   In the method of suppressing the magnetizing inrush current by the breaker with resistor, it is necessary to add the breaker with resistor to the normal breaker, so that the size of the breaker as a whole is increased.

また、いずれの励磁突入電流を抑制する方法も、上述のような三相交流電圧を単相交流電圧に変換する変圧器を投入することは想定されていない。   Further, none of the methods for suppressing the magnetizing inrush current is assumed to introduce a transformer for converting the above three-phase AC voltage into a single-phase AC voltage.

例えば、残留磁束を計測し、遮断器の投入位相を制御する方法では、電力系統に用いられる三相変圧器に対する制御方法を、三相交流電圧を単相交流電圧に変換する変圧器にそのまま適用することはできない。これらの結線の変圧器の場合は、三相交流側の相電圧又は線間電圧を計測しても、変圧器鉄心の磁束をそのまま算出することができないからである。   For example, in the method of measuring the residual magnetic flux and controlling the closing phase of the circuit breaker, the control method for the three-phase transformer used in the power system is directly applied to the transformer that converts the three-phase AC voltage to the single-phase AC voltage. I can't do it. In the case of these connection transformers, the magnetic flux of the transformer core cannot be calculated as it is even if the phase voltage or the line voltage on the three-phase AC side is measured.

本発明の実施形態の目的は、電源を備えた三相交流の電力系統と三相交流電圧を単相交流電圧に変換する接地された変圧器との接続を開閉する遮断器の励磁突入電流を抑制するための投入位相の制御をすることのできる励磁突入電流抑制装置を提供することにある。   An object of an embodiment of the present invention is to provide an excitation inrush current of a circuit breaker that opens and closes a connection between a three-phase AC power system having a power source and a grounded transformer that converts a three-phase AC voltage into a single-phase AC voltage An object of the present invention is to provide a magnetizing inrush current suppression device capable of controlling a closing phase for suppression.

本発明の実施形態の観点に従った励磁突入電流抑制装置は、電源を備えた三相交流の電力系統と三相交流電圧を単相交流電圧に変換する接地された変圧器との接続を相毎に開閉する遮断器の励磁突入電流を抑制する励磁突入電流抑制装置であって、前記変圧器の単相交流電圧を計測する変圧器側単相交流電圧計測手段と、前記変圧器側単相交流電圧計測手段により計測された前記変圧器の単相交流電圧を、前記変圧器の三相交流電圧に変換する変圧器側電圧変換手段と、前記変圧器側電圧変換手段により変換された三相交流電圧に基づいて、前記遮断器による前記変圧器の遮断後の前記変圧器の三相の残留磁束を演算する残留磁束演算手段と、前記遮断器よりも前記電源側の三相交流電圧を計測する電源側三相交流電圧計測手段と、前記電源側三相交流電圧計測手段により計測された三相交流電圧に基づいて、前記変圧器の三相の定常磁束を演算する定常磁束演算手段と、前記残留磁束演算手段により演算された前記三相の残留磁束のうち絶対値が最大の相を判断する相判断手段と、前記相判断手段により判断された前記相において、前記残留磁束演算手段により演算された前記残留磁束と前記定常磁束演算手段により演算された前記定常磁束とが一致するような第1の位相を判断する第1の位相判断手段と、前記第1の位相判断手段により判断された前記第1の位相で、前記相判断手段により判断された前記相の前記遮断器を投入する第1の投入手段と、前記第1の位相判断手段により判断された前記第1の位相よりも後に、前記相判断手段により判断された前記相の前記電源側の交流電圧が、前記相判断手段により判断された前記相の残留磁束と同極性から逆極性に遷移する零点となるような第2の位相を判断する第2の位相判断手段と、前記第2の位相判断手段により判断された前記第2の位相で、投入されていない他の2相の前記遮断器を投入する第2の投入手段とを備えている。   An inrush current suppression device according to an embodiment of the present invention has a connection between a three-phase AC power system having a power source and a grounded transformer that converts a three-phase AC voltage into a single-phase AC voltage. An excitation inrush current suppressing device that suppresses an excitation inrush current of a circuit breaker that opens and closes every time, a transformer-side single-phase AC voltage measuring unit that measures a single-phase AC voltage of the transformer, and the transformer-side single-phase Transformer-side voltage conversion means for converting the single-phase AC voltage of the transformer measured by the AC voltage measurement means into the three-phase AC voltage of the transformer, and the three-phase converted by the transformer-side voltage conversion means Based on the AC voltage, the residual magnetic flux calculating means for calculating the three-phase residual magnetic flux of the transformer after the transformer is interrupted by the circuit breaker, and measuring the three-phase AC voltage on the power supply side from the circuit breaker Power supply side three-phase AC voltage measuring means, and the power supply Based on the three-phase AC voltage measured by the three-phase AC voltage measuring means, the steady-state magnetic flux calculating means for calculating the three-phase steady-state magnetic flux of the transformer, and the three-phase residual calculated by the residual magnetic flux calculating means The phase determination means for determining the phase having the maximum absolute value of the magnetic flux, and the residual magnetic flux calculated by the residual magnetic flux calculation means and the steady magnetic flux calculation means in the phase determined by the phase determination means. The first phase determining means for determining a first phase that matches the steady magnetic flux and the first phase determined by the first phase determining means are determined by the phase determining means. And a power supply for the phase determined by the phase determination means after the first phase determined by the first phase determination means. ~ side Second phase determining means for determining a second phase such that the AC voltage becomes a zero point at which a transition is made from the same polarity to the opposite polarity as the residual magnetic flux of the phase determined by the phase determining means; And a second closing means for closing the other two-phase circuit breakers that are not turned on at the second phase determined by the phase determining means.

本発明の第1の実施形態に係る励磁突入電流抑制装置の適用された電力系統システムの構成を示す構成図。The block diagram which shows the structure of the electric power system system to which the magnetizing inrush current suppression apparatus which concerns on the 1st Embodiment of this invention was applied. 第1の実施形態に係る変形ウッドブリッジ結線変圧器の構成を示す構成図。The block diagram which shows the structure of the deformation | transformation wood bridge connection transformer which concerns on 1st Embodiment. 第1の実施形態に係るウッドブリッジ結線変圧器の構成を示す構成図。The block diagram which shows the structure of the wood bridge connection transformer which concerns on 1st Embodiment. 第1の実施形態に係る変形ウッドブリッジ結線変圧器の1次側相電圧をベクトルで示すベクトル図。The vector diagram which shows the primary side phase voltage of the deformation | transformation wood bridge connection transformer which concerns on 1st Embodiment with a vector. 第1の実施形態に係る変形ウッドブリッジ結線変圧器の2次側電圧をベクトルで示すベクトル図。The vector diagram which shows the secondary side voltage of the deformation | transformation wood bridge connection transformer which concerns on 1st Embodiment with a vector. 第1の実施形態に係る変圧器電圧計測部により計測された2組の単相交流電圧の電圧波形を示す波形図。The wave form diagram which shows the voltage waveform of two sets of single phase alternating current voltage measured by the transformer voltage measurement part which concerns on 1st Embodiment. 第1の実施形態に係る変圧器電圧変換部による変換後の1次側相電圧の電圧波形を示す波形図。The wave form diagram which shows the voltage waveform of the primary side phase voltage after the conversion by the transformer voltage conversion part which concerns on 1st Embodiment. 第1の実施形態に係る変形ウッドブリッジ結線変圧器の1次側相電圧の電圧波形を示す波形図。The wave form diagram which shows the voltage waveform of the primary side phase voltage of the deformation | transformation wood bridge connection transformer which concerns on 1st Embodiment. 第1の実施形態に係る励磁突入電流抑制装置による遮断器の遮断前後の1次側相電圧を示す波形図。The wave form diagram which shows the primary side phase voltage before and behind interruption | blocking of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 1st Embodiment. 第1の実施形態に係る励磁突入電流抑制装置による遮断器の遮断前後の1次側相磁束を示す波形図。The wave form diagram which shows the primary side phase magnetic flux before and behind interruption | blocking of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 1st Embodiment. 第1の実施形態に係る励磁突入電流抑制装置による遮断器の投入前後の1次側相電圧を示す波形図。The wave form diagram which shows the primary side phase voltage before and behind turning on of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 1st Embodiment. 第1の実施形態に係る励磁突入電流抑制装置による遮断器の投入前後の1次側相磁束を示す波形図。The wave form diagram which shows the primary side phase magnetic flux before and behind the injection | throwing-in of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 1st Embodiment. 第1の実施形態に係る励磁突入電流抑制装置による遮断器の投入前後の1次側相電流(励磁突入電流)を示す波形図。The wave form diagram which shows the primary side phase current (excitation inrush current) before and behind the injection | throwing-in of the circuit breaker by the inrush current suppression apparatus which concerns on 1st Embodiment. 本発明の第2の実施形態に係る励磁突入電流抑制装置の適用された電力系統システムの構成を示す構成図。The block diagram which shows the structure of the electric power system system to which the magnetizing inrush current suppression apparatus which concerns on the 2nd Embodiment of this invention was applied. 第2の実施形態に係る励磁突入電流抑制装置による遮断器の遮断前後の1次側相電圧を示す波形図。The wave form diagram which shows the primary side phase voltage before and behind interruption | blocking of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 2nd Embodiment. 第2の実施形態に係る励磁突入電流抑制装置による遮断器の遮断前後の1次側相磁束を示す波形図。The wave form diagram which shows the primary side phase magnetic flux before and behind interruption | blocking of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 2nd Embodiment. 第2の実施形態に係る励磁突入電流抑制装置による遮断器の投入前後の1次側相電圧を示す波形図。The wave form diagram which shows the primary side phase voltage before and after turning on of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 2nd Embodiment. 第2の実施形態に係る励磁突入電流抑制装置による遮断器の投入前後の1次側相磁束を示す波形図。The wave form diagram which shows the primary side phase magnetic flux before and after injection | throwing-in of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 2nd Embodiment. 第2の実施形態に係る励磁突入電流抑制装置による遮断器の投入前後の1次側相電流(励磁突入電流)を示す波形図。The wave form diagram which shows the primary side phase current (excitation inrush current) before and behind the injection | throwing-in of the circuit breaker by the excitation inrush current suppression apparatus which concerns on 2nd Embodiment. 本発明の第3の実施形態に係る励磁突入電流抑制装置の適用された電力系統システムの構成を示す構成図。The block diagram which shows the structure of the electric power grid | system system to which the magnetizing inrush current suppression apparatus which concerns on the 3rd Embodiment of this invention was applied. 本発明の第4の実施形態に係る励磁突入電流抑制装置の適用された電力系統システムの構成を示す構成図。The block diagram which shows the structure of the electric power grid | system system to which the magnetizing inrush current suppression apparatus which concerns on the 4th Embodiment of this invention was applied. 第4の実施形態に係る励磁突入電流抑制装置による遮断器の遮断前後の1次側相磁束の残留磁束を示す波形図。The wave form diagram which shows the residual magnetic flux of the primary side phase magnetic flux before and behind interruption | blocking of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 4th Embodiment. 第4の実施形態に係る励磁突入電流抑制装置による遮断器の遮断前後の2次側巻線磁束の残留磁束を示す波形図。The wave form diagram which shows the residual magnetic flux of the secondary side winding magnetic flux before and behind interruption | blocking of the circuit breaker by the magnetizing inrush current suppression apparatus which concerns on 4th Embodiment.

以下図面を参照して、本発明の実施形態を説明する。   Embodiments of the present invention will be described below with reference to the drawings.

(第1の実施形態)
図1は、本発明の第1の実施形態に係る励磁突入電流抑制装置6の適用された電力系統システムの構成を示す構成図である。なお、以降の図における同一部分には同一符号を付してその詳しい説明を省略し、異なる部分について主に述べる。以降の実施形態も同様にして重複する説明を省略する。
(First embodiment)
FIG. 1 is a configuration diagram showing a configuration of a power system to which the magnetizing inrush current suppressing device 6 according to the first embodiment of the present invention is applied. In addition, the same code | symbol is attached | subjected to the same part in subsequent figures, the detailed description is abbreviate | omitted, and a different part is mainly described. In the following embodiments, the same description is omitted.

本実施形態に係る電力系統システムは、電源母線(電力系統の母線)1と、遮断器2と、変形ウッドブリッジ結線変圧器3と、電源母線1に設けられた三相分の電源電圧検出器4U,4V,4Wと、変形ウッドブリッジ結線変圧器3の2次側に設けられた2相分の変圧器2次側電圧検出器5M,5Tと、励磁突入電流抑制装置6とを備えている。   The power system according to this embodiment includes a power supply bus (power system bus) 1, a circuit breaker 2, a modified Woodbridge connection transformer 3, and a power supply voltage detector for three phases provided on the power supply bus 1. 4U, 4V, 4W, two-phase transformer secondary voltage detectors 5M, 5T provided on the secondary side of the modified Woodbridge connection transformer 3, and the magnetizing inrush current suppression device 6 are provided. .

電源母線1は、U相、V相、及びW相からなる三相交流の電源を備えた電力系統の母線である。   The power supply bus 1 is a bus of an electric power system provided with a three-phase AC power supply composed of a U phase, a V phase, and a W phase.

変形ウッドブリッジ結線変圧器3は、遮断器2を介して、電源母線1に接続されている。変形ウッドブリッジ結線変圧器3は、有効接地系又は非有効接地系に設置されている。変形ウッドブリッジ結線変圧器3は、電源母線1から供給される三相交流電圧を2組の単相交流電圧に変換する。変形ウッドブリッジ結線変圧器3は、三相交流側を1次側とし、単相交流側を2次側とする。なお、変形ウッドブリッジ結線変圧器3は、変成原理の同じウッドブリッジ結線変圧器を用いてもよい。従って、以下(以降の実施形態も含む)においても、変形ウッドブリッジ結線変圧器3は、特に区別しない限り、ウッドブリッジ結線変圧器に置き換えられるものとする。   The modified wood bridge connection transformer 3 is connected to the power supply bus 1 via the circuit breaker 2. The modified wood bridge connection transformer 3 is installed in an effective grounding system or a non-effective grounding system. The modified wood bridge connection transformer 3 converts the three-phase AC voltage supplied from the power bus 1 into two sets of single-phase AC voltages. In the modified Woodbridge connection transformer 3, the three-phase AC side is the primary side, and the single-phase AC side is the secondary side. The modified wood bridge connection transformer 3 may be a wood bridge connection transformer having the same transformation principle. Therefore, in the following (including the following embodiments), the modified woodbridge connection transformer 3 is replaced with a woodbridge connection transformer unless otherwise specified.

遮断器2は、電源母線1と変形ウッドブリッジ結線変圧器3との間に設けられている。遮断器2は、U相、V相、及びW相の各相の主接点を個別に操作する各相操作型の遮断器である。遮断器2が投入されることにより、変形ウッドブリッジ結線変圧器3は、電源母線1による電源投入がされる。遮断器2が開放されることにより、変形ウッドブリッジ結線変圧器3は、電源母線1から遮断(電気的な接続の切り離し)される。   The circuit breaker 2 is provided between the power supply bus 1 and the modified wood bridge connection transformer 3. The circuit breaker 2 is a phase operation type circuit breaker that individually operates the main contact of each phase of the U phase, the V phase, and the W phase. When the breaker 2 is turned on, the modified wood bridge connection transformer 3 is turned on by the power bus 1. When the circuit breaker 2 is opened, the modified wood bridge connection transformer 3 is disconnected (disconnected from the electrical connection) from the power supply bus 1.

3つの電源電圧検出器4U,4V,4Wは、それぞれ電源母線1のU相、V相、W相のそれぞれの相電圧(対地電圧)を計測するための計測用機器である。電源電圧検出器4U,4V,4Wは、例えば、計器用変圧器(VT, Voltage Transformer)である。電源電圧検出器4U,4V,4Wは、検出値を検出信号として、励磁突入電流抑制装置6に出力する。   The three power supply voltage detectors 4U, 4V, and 4W are measuring devices for measuring the phase voltages (ground voltages) of the U-phase, V-phase, and W-phase of the power supply bus 1, respectively. The power supply voltage detectors 4U, 4V, 4W are, for example, instrument transformers (VT, Voltage Transformer). The power supply voltage detectors 4U, 4V, 4W output the detected value as a detection signal to the magnetizing inrush current suppressing device 6.

2相分の変圧器2次側電圧検出器5M,5Tは、それぞれ変形ウッドブリッジ結線変圧器3の2次側の各端子(主座、T座)のそれぞれの端子電圧(単相交流電圧)VT,VMを計測するための計測用機器である。変圧器2次側電圧検出器5M,5Tは、例えば、計器用変圧器である。変圧器2次側電圧検出器5M,5Tは、検出値を検出信号として、励磁突入電流抑制装置6に出力する。   The transformer secondary voltage detectors 5M and 5T for two phases are respectively terminal voltages (single-phase AC voltages) of the respective terminals (main and T seats) on the secondary side of the modified Woodbridge connection transformer 3. This is a measuring device for measuring VT and VM. The transformer secondary side voltage detectors 5M and 5T are, for example, instrument transformers. The transformer secondary side voltage detectors 5M and 5T output the detected value as a detection signal to the excitation inrush current suppression device 6.

励磁突入電流抑制装置6は、電源電圧検出器4U,4V,4W及び変圧器2次側電圧検出器5M,5Tのそれぞれから受信した検出信号に基づいて、遮断器2の主接点に対して投入指令を出力する。これにより、遮断器2は投入される。   The magnetizing inrush current suppression device 6 is applied to the main contact of the circuit breaker 2 based on the detection signals received from the power supply voltage detectors 4U, 4V, 4W and the transformer secondary side voltage detectors 5M, 5T. Outputs a command. Thereby, the circuit breaker 2 is turned on.

図2は、本実施形態に係る変形ウッドブリッジ結線変圧器3の構成を示す構成図である。   FIG. 2 is a configuration diagram showing the configuration of the modified Woodbridge connection transformer 3 according to the present embodiment.

変形ウッドブリッジ結線変圧器3は、主座変圧器(M座変圧器)302とT座変圧器301とを備えている。   The modified wood bridge connection transformer 3 includes a main seat transformer (M seat transformer) 302 and a T seat transformer 301.

主座変圧器302は、2次側に等しい巻数の巻線2個を持つ。T座変圧器301は、2次側で1:0.366:0.366の巻数比となる巻線を持つ単巻変圧器と接続される。変形ウッドブリッジ結線変圧器3は、主座変圧器302及びT座変圧器301の2次側同士が2つのデルタ結線された巻線で背中合わせになるように接続されている。   The main transformer 302 has two windings with the same number of turns on the secondary side. The T-seat transformer 301 is connected to a single-turn transformer having windings with a turns ratio of 1: 0.366: 0.366 on the secondary side. The modified wood bridge connection transformer 3 is connected so that the secondary sides of the main transformer 302 and the T seat transformer 301 are back-to-back with two delta-connected windings.

次に、変圧器3がウッドブリッジ結線である場合について説明する。   Next, a case where the transformer 3 is a wood bridge connection will be described.

図3は、本実施形態に係るウッドブリッジ結線変圧器3の構成を示す構成図である。   FIG. 3 is a configuration diagram showing the configuration of the woodbridge connection transformer 3 according to the present embodiment.

ウッドブリッジ結線変圧器3のT座変圧器301は、変形ウッドブリッジ結線で用いた単巻変圧器の代わりに、2次側に1:0.366:0.366の巻数比となる巻線を持つ。その他の点は、変形ウッドブリッジ結線変圧器3と同様の構成である。   The T-seat transformer 301 of the wood bridge connection transformer 3 has a winding having a turns ratio of 1: 0.366: 0.366 on the secondary side instead of the single-turn transformer used in the modified wood bridge connection. Have. Other points are the same as those of the modified wood bridge connection transformer 3.

図4は、本実施形態に係る変形ウッドブリッジ結線変圧器3の1次側相電圧Vu,Vv,Vwをベクトルで示すベクトル図である。図5は、本実施形態に係る変形ウッドブリッジ結線変圧器3の2次側電圧Vt,Vmをベクトルで示すベクトル図ある。   FIG. 4 is a vector diagram showing the primary side phase voltages Vu, Vv, Vw of the modified Woodbridge connection transformer 3 according to the present embodiment as vectors. FIG. 5 is a vector diagram showing the secondary side voltages Vt and Vm of the modified Woodbridge connection transformer 3 according to the present embodiment as vectors.

1次側のVW相間の電圧Vvwは、主座変圧器302の2次側端子c−a間に印加される電圧(主座の2次側電圧)Vmと同位相になる。また、1次側のU相電圧Vuは、T座変圧器301の2次側端子b−d間に印加される電圧(T座の2次側電圧)Vtと同位相になる。よって、T座の2次側電圧Vtは、主座の2次側電圧Vmよりも90度位相が進む。   The voltage Vvw between the VW phases on the primary side has the same phase as the voltage (secondary voltage on the main seat) Vm applied between the secondary terminals ca of the main transformer 302. Further, the primary-side U-phase voltage Vu has the same phase as the voltage (t-secondary secondary voltage) Vt applied between the secondary terminals b-d of the T-seat transformer 301. Therefore, the phase of the secondary voltage Vt of the T seat is advanced by 90 degrees relative to the secondary voltage Vm of the main seat.

励磁突入電流抑制装置6は、電源電圧計測部601と、定常磁束算出部602と、変圧器電圧計測部603と、変圧器電圧変換部610と、残留磁束算出部604と、位相検出部605と、投入指令出力部606とを備えている。   The excitation inrush current suppression device 6 includes a power supply voltage measurement unit 601, a steady magnetic flux calculation unit 602, a transformer voltage measurement unit 603, a transformer voltage conversion unit 610, a residual magnetic flux calculation unit 604, and a phase detection unit 605. And a charging command output unit 606.

電源電圧計測部601は、電源電圧検出器4U,4V,4Wにより検出された検出信号に基づいて、電源母線1の各相電圧Vv,Vu,Vwを計測する。電源電圧計測部601は、計測した各相電圧を定常磁束算出部602に出力する。   The power supply voltage measuring unit 601 measures the phase voltages Vv, Vu, Vw of the power supply bus 1 based on the detection signals detected by the power supply voltage detectors 4U, 4V, 4W. The power supply voltage measurement unit 601 outputs the measured phase voltages to the steady magnetic flux calculation unit 602.

定常磁束算出部602は、電源電圧計測部601により計測された各相電圧Vv,Vu,Vwをそれぞれ積分する。定常磁束算出部602は、この積分された値を、定常時の磁束(定常磁束)φTu,φTv,φTwとする。定常磁束算出部602は、遮断器2が投入されるまで、定常磁束φTu,φTv,φTwを演算する。定常磁束算出部602は、演算した定常磁束φTu,φTv,φTwを位相検出部605に出力する。   The steady magnetic flux calculation unit 602 integrates each phase voltage Vv, Vu, Vw measured by the power supply voltage measurement unit 601. The steady magnetic flux calculation unit 602 sets the integrated value as a steady state magnetic flux (steady magnetic flux) φTu, φTv, φTw. The steady magnetic flux calculation unit 602 calculates steady magnetic fluxes φTu, φTv, and φTw until the breaker 2 is turned on. The steady magnetic flux calculation unit 602 outputs the calculated steady magnetic fluxes φTu, φTv, and φTw to the phase detection unit 605.

変圧器電圧計測部603は、変圧器2次側電圧検出器5T,5Mにより検出された検出信号に基づいて、変形ウッドブリッジ結線変圧器3の2次側の各組の単相交流電圧Vt,Vmを計測する。変圧器電圧計測部603は、計測した2組の単相交流電圧Vt,Vmを変圧器電圧変換部610に出力する。   The transformer voltage measuring unit 603 is configured to generate a single-phase AC voltage Vt, a secondary phase of each set of the modified Woodbridge connection transformer 3 on the basis of the detection signals detected by the transformer secondary voltage detectors 5T and 5M. Vm is measured. The transformer voltage measurement unit 603 outputs the measured two sets of single-phase AC voltages Vt and Vm to the transformer voltage conversion unit 610.

変圧器電圧変換部610は、変圧器電圧計測部603により計測された2組の単相交流電圧Vt,Vmを、次式により、1次側相電圧VDu,VDv,VDwに変換する。1次側相電圧VDuは、変換後のU相電圧である。1次側相電圧VDvは、変換後のV相電圧である。1次側相電圧VDwは、変換後のW相電圧である。変圧器電圧変換部610は、変換した1次側相電圧VDu,VDv,VDwを残留磁束算出部604に出力する。   The transformer voltage conversion unit 610 converts the two sets of single-phase AC voltages Vt and Vm measured by the transformer voltage measurement unit 603 into primary side phase voltages VDu, VDv, and VDw according to the following equations. Primary side phase voltage VDu is a U-phase voltage after conversion. Primary side phase voltage VDv is a V-phase voltage after conversion. Primary side phase voltage VDw is a W-phase voltage after conversion. The transformer voltage conversion unit 610 outputs the converted primary side phase voltages VDu, VDv, and VDw to the residual magnetic flux calculation unit 604.

VDu=Vt/√3 …式(1)
VDv=(1/2)(−Vt/√3+Vm) …式(2)
VDw=−(1/2)(Vt/√3+Vm) …式(3)
なお、p.u.(定格に対する割合)表示で、1次側相電圧VDu,VDv,VDwに変換する演算をする場合、上記の式(1)〜(3)の中の√3で割る演算は不要である。
VDu = Vt / √3 Formula (1)
VDv = (1/2) (− Vt / √3 + Vm) (2)
VDw = − (1/2) (Vt / √3 + Vm) (3)
P. u. When performing calculations to convert to primary side phase voltages VDu, VDv, VDw in the (ratio to rating) display, the calculation divided by √3 in the above formulas (1) to (3) is not necessary.

図6〜図8を参照して、本実施形態に係る変圧器電圧変換部610による演算処理について説明する。   With reference to FIGS. 6-8, the arithmetic processing by the transformer voltage conversion part 610 which concerns on this embodiment is demonstrated.

図6は、変圧器電圧計測部603により計測された2組の単相交流電圧Vt,Vmの電圧波形を示す波形図である。図7は、変圧器電圧変換部610による変換後の1次側相電圧VDu,VDv,VDwの電圧波形を示す波形図である。図8は、変形ウッドブリッジ結線変圧器3の1次側相電圧Vu,Vv,Vwの電圧波形を示す波形図である。   FIG. 6 is a waveform diagram showing voltage waveforms of two sets of single-phase AC voltages Vt and Vm measured by the transformer voltage measuring unit 603. FIG. 7 is a waveform diagram showing voltage waveforms of primary side phase voltages VDu, VDv, and VDw after conversion by transformer voltage conversion unit 610. FIG. 8 is a waveform diagram showing voltage waveforms of the primary side phase voltages Vu, Vv, Vw of the modified Woodbridge connection transformer 3.

変圧器電圧変換部610は、図6に示す2組の単相交流電圧Vt,Vmを、図7に示す1次側相電圧VDu,VDv,VDwに変換する。これにより、変圧器電圧変換部610は、pu値(定格に対する割合)で換算して、図8に示す1次側相電圧Vu,Vv,Vwと同一の電圧波形を求めることができる。   The transformer voltage conversion unit 610 converts the two sets of single-phase AC voltages Vt and Vm shown in FIG. 6 into primary side phase voltages VDu, VDv, and VDw shown in FIG. Thereby, the transformer voltage conversion unit 610 can obtain the same voltage waveform as the primary side phase voltages Vu, Vv, and Vw shown in FIG. 8 by converting the pu value (ratio to the rating).

残留磁束算出部604は、遮断器2による変形ウッドブリッジ結線変圧器3の遮断直後に、変圧器電圧変換部610により変換された各相電圧VDu,VDv,VDwをそれぞれ積分する。残留磁束算出部604は、この積分された値を、変形ウッドブリッジ結線変圧器3の鉄心の残留磁束(1次側相磁束)φZu,φZv,φZwとする。残留磁束算出部604は、演算した残留磁束φZu,φZv,φZwを位相検出部605に出力する。   The residual magnetic flux calculation unit 604 integrates each phase voltage VDu, VDv, VDw converted by the transformer voltage conversion unit 610 immediately after the circuit breaker 2 cuts off the modified Woodbridge connection transformer 3. The residual magnetic flux calculation unit 604 sets the integrated value as the residual magnetic flux (primary side phase magnetic flux) φZu, φZv, φZw of the iron core of the modified Woodbridge connection transformer 3. The residual magnetic flux calculation unit 604 outputs the calculated residual magnetic fluxes φZu, φZv, φZw to the phase detection unit 605.

位相検出部605は、定常磁束算出部602により演算された定常磁束φTu,φTv,φTw及び残留磁束算出部604により演算された残留磁束φZu,φZv,φZwに基づいて、2段階の投入目標位相Tc1,Tc2をそれぞれ同定(判断)する。1段階目の投入目標位相Tc1は、先行して1相の遮断器2を投入するための位相である。2段階目の投入目標位相Tc2は、後から残りの2相の遮断器2を投入するための位相である。位相検出部605は、同定した2段階の投入目標位相Tc1,Tc2をそれぞれ投入指令出力部606に出力する。   The phase detection unit 605 is based on the steady magnetic fluxes φTu, φTv, φTw calculated by the steady magnetic flux calculation unit 602 and the residual magnetic fluxes φZu, φZv, φZw calculated by the residual magnetic flux calculation unit 604, and has two stages of target target phases Tc1. , Tc2 are identified (determined). The first target closing phase Tc1 is a phase for leading the one-phase circuit breaker 2 in advance. The second target closing phase Tc2 is a phase for turning on the remaining two-phase circuit breaker 2 later. The phase detection unit 605 outputs the identified two-step input target phases Tc1 and Tc2 to the input command output unit 606, respectively.

具体的には、位相検出部605は、三相の残留磁束φZu,φZv,φZwのうち絶対値が最大の相を検出(判断)する。位相検出部605は、検出した相において、残留磁束と定常磁束が一致するような位相を1段階目の投入目標位相Tc1として同定する。位相検出部605は、投入目標位相Tc1から予め設定されている時間経過後に、残留磁束の絶対値が最大の相(検出した相)の相電圧が、同相の残留磁束と同極性から逆極性に遷移する零点となるような位相を2段階目の投入目標位相Tc2として同定する。2段階目の投入目標位相Tc2の同定は、1段階目の投入目標位相Tc1時点の定常磁束の値に基づいて、励磁突入電流抑制装置6で内部的に演算してもよいし、電源電圧検出器4U,4V,4Wによる計測値で実際に零点となる相電圧を検出してもよい。また、予め設定する時間は、この設定時間後の次に来る零点が、投入した相の残留磁束と同極性から逆極性に遷移する零点になるように設定してもよい。これにより、位相検出部605は、単に、設定時間経過後に次に来る零点の位相を投入目標位相Tc2として同定すればよい。   Specifically, the phase detector 605 detects (determines) the phase having the maximum absolute value among the three-phase residual magnetic fluxes φZu, φZv, and φZw. The phase detection unit 605 identifies the phase in which the residual magnetic flux and the steady magnetic flux match in the detected phase as the first target phase Tc1. The phase detector 605 changes the phase voltage of the phase having the maximum absolute value of the residual magnetic flux (detected phase) from the same polarity to the opposite polarity to the residual magnetic flux of the same phase after a preset time has elapsed from the input target phase Tc1. The phase that becomes the zero point for transition is identified as the second stage target phase Tc2. The identification of the second stage closing target phase Tc2 may be performed internally by the magnetizing inrush current suppression device 6 based on the value of the steady magnetic flux at the time of the first stage closing target phase Tc1, or the power supply voltage detection The phase voltage that actually becomes the zero point may be detected from the measurement values obtained by the devices 4U, 4V, and 4W. Further, the preset time may be set so that the next zero point after this set time becomes a zero point that changes from the same polarity as the residual magnetic flux of the input phase to the opposite polarity. Thereby, the phase detection unit 605 may simply identify the phase of the zero point that comes next after the set time has elapsed as the input target phase Tc2.

投入指令出力部606は、位相検出部605により検出された2段階の投入目標位相Tc1,Tc2で、遮断器2の各相の主接点を駆動する操作機構に対して2段階に投入指令を出力する。これにより、遮断器2の全ての相は、2段階に分けて投入される。投入指令出力部606は、1段階目の投入目標位相Tc1で、残留磁束の絶対値が最大の相(位相検出部605で検出した相)の遮断器2を投入する。投入指令出力部606は、2段階目の投入目標位相Tc2で、残りの2相の遮断器2を投入する。   The closing command output unit 606 outputs the closing command in two stages to the operation mechanism that drives the main contact of each phase of the circuit breaker 2 with the two-stage closing target phases Tc1 and Tc2 detected by the phase detection unit 605. To do. Thereby, all the phases of the circuit breaker 2 are thrown into two stages. The closing command output unit 606 switches on the circuit breaker 2 of the phase in which the absolute value of the residual magnetic flux is the maximum (phase detected by the phase detecting unit 605) at the first target closing phase Tc1. The closing command output unit 606 switches on the remaining two-phase circuit breaker 2 at the second-stage closing target phase Tc2.

次に、図9〜図13を参照して、励磁突入電流抑制装置6による励磁突入電流の抑制について説明する。   Next, with reference to FIGS. 9-13, suppression of the magnetizing inrush current by the magnetizing inrush current suppressing device 6 will be described.

図9及び図10は、励磁突入電流抑制装置6による遮断器2の遮断Tp前後の状態の一例を示している。図9は、1次側相電圧Vu,Vv,Vwを示す波形図である。図10は、1次側相磁束φu,φv,φwを示す波形図である。図11〜図13は、励磁突入電流抑制装置6による遮断器2の投入Tc1,Tc2前後の状態の一例を示している。図11は、1次側相電圧Vu,Vv,Vwを示す波形図である。図12は、1次側相磁束φu,φv,φwを示す波形図である。図13は、1次側相電流(励磁突入電流)Iu,Iv,Iwを示す波形図である。   9 and 10 show an example of the state before and after the circuit breaker Tp of the circuit breaker 2 by the magnetizing inrush current suppressing device 6. FIG. 9 is a waveform diagram showing primary side phase voltages Vu, Vv, Vw. FIG. 10 is a waveform diagram showing primary side phase magnetic fluxes φu, φv, and φw. 11 to 13 show an example of the state before and after the closing Tc1 and Tc2 of the circuit breaker 2 by the magnetizing inrush current suppressing device 6. FIG. FIG. 11 is a waveform diagram showing primary side phase voltages Vu, Vv, Vw. FIG. 12 is a waveform diagram showing primary side phase magnetic fluxes φu, φv, and φw. FIG. 13 is a waveform diagram showing primary side phase currents (excitation inrush currents) Iu, Iv, Iw.

ここで、遮断Tp前又は投入Tc1,Tc2後の1次側相磁束φu,φv,φwは、定常磁束φTu,φTv,φTwを示している。また、遮断Tp後と投入Tc1,Tc2前の間の1次側相磁束φu,φv,φwは、残留磁束φZu,φZv,φZwを示している。   Here, primary side phase magnetic fluxes φu, φv, φw before interruption Tp or after input Tc1, Tc2 indicate steady magnetic fluxes φTu, φTv, φTw. Further, the primary side phase magnetic fluxes φu, φv, φw after the interruption Tp and before the input Tc1, Tc2 indicate the residual magnetic fluxes φZu, φZv, φZw.

変形ウッドブリッジ結線変圧器3の1次側に図9に示す三相交流電圧Vu,Vv,Vwが印加されている場合、遮断器2が開極した後(遮断Tp後)は、図10に示す残留磁束φZu,φZv,φZwが残る。このとき、絶対値が最大の残留磁束は、U相の残留磁束φZuである。   When the three-phase AC voltages Vu, Vv, and Vw shown in FIG. 9 are applied to the primary side of the modified wood bridge connection transformer 3, after the circuit breaker 2 is opened (after the circuit break Tp), FIG. The residual magnetic fluxes φZu, φZv, φZw shown remain. At this time, the residual magnetic flux having the maximum absolute value is the U-phase residual magnetic flux φZu.

従って、励磁突入電流抑制装置6は、図12に示すように、U相の定常磁束φTuがU相の残留磁束φZuと略一致する位相を、U相の遮断器2を投入するための1段階目の投入目標位相Tc1として同定する。励磁突入電流抑制装置6は、同定した1段階目の投入目標位相Tc1で、U相の遮断器2を投入する。   Therefore, as shown in FIG. 12, the magnetizing inrush current suppressing device 6 is a one-stage for turning on the U-phase circuit breaker 2 so that the U-phase steady magnetic flux φTu substantially coincides with the U-phase residual magnetic flux φZu. It is identified as the eye insertion target phase Tc1. The magnetizing inrush current suppression device 6 inputs the U-phase circuit breaker 2 at the identified first target closing target phase Tc1.

次に、励磁突入電流抑制装置6は、図11に示すように、U相の遮断器2を投入してから予め設定された時間経過後に、U相電圧VuがU相の残留磁束φZuと同極性(プラス)から逆極性(マイナス)に遷移する略零点となる位相を残りのV相及びW相の遮断器2を投入するための2段階目の投入目標位相Tc2として同定する。励磁突入電流抑制装置6は、同定した2段階目の投入目標位相Tc2で、V相及びW相の遮断器2を投入する。   Next, as shown in FIG. 11, the magnetizing inrush current suppressing device 6 has the U-phase voltage Vu equal to the U-phase residual magnetic flux φZu after a preset time has elapsed since the U-phase circuit breaker 2 was turned on. The phase that is a substantially zero point that transitions from the polarity (plus) to the opposite polarity (minus) is identified as the second stage target phase Tc2 for putting the remaining V-phase and W-phase circuit breakers 2 on. The magnetizing inrush current suppressing device 6 turns on the V-phase and W-phase circuit breakers 2 at the identified second-stage closing target phase Tc2.

2段階目の投入目標位相Tc2を同定するための“予め設定された時間”は、投入されていないV相及びW相の残留磁束φZv,φZwを充分に近づけるための時間である。この時間は、主に変圧器3の特性に基づいて設定される。   The “preset time” for identifying the second target phase Tc2 to be applied is a time for sufficiently approaching the residual magnetic fluxes φZv and φZw of the V phase and W phase that are not applied. This time is set mainly based on the characteristics of the transformer 3.

このように励磁突入電流抑制装置6が遮断器2を投入することにより、図13に示すように、各相の遮断器電流(励磁突入電流)Iu,Iv,Iwが抑制される。各相の遮断器電流Iu,Iv,Iwは、最大で10[A]程度である。これは、変圧器の励磁電流レベルである。   In this way, when the magnetizing inrush current suppressing device 6 turns on the circuit breaker 2, as shown in FIG. 13, the circuit breaker current (exciting inrush current) Iu, Iv, Iw of each phase is suppressed. The circuit breaker currents Iu, Iv, and Iw of each phase are about 10 [A] at the maximum. This is the transformer excitation current level.

本実施形態によれば、絶対値が最大の残留磁束の相の遮断器2を残留磁束と定常磁束が一致するような位相で投入し、所定時間経過後に、既に投入した相の相電圧が零点となるような位相で、残りの相の遮断器2を投入することで、励磁突入電流Iu,Iv,Iwを抑制することができる。   According to the present embodiment, the phase breaker 2 having the maximum absolute value of the residual magnetic flux is applied in such a phase that the residual magnetic flux and the steady magnetic flux coincide with each other, and the phase voltage of the already applied phase is zero after a predetermined time has elapsed. The inrush currents Iu, Iv, and Iw can be suppressed by turning on the circuit breaker 2 of the remaining phase at such a phase.

これにより、変形ウッドブリッジ結線変圧器3の2次側に電圧検出器5M,5Tが設置されていれば、1次側に電圧検出器が設置されていなくても、励磁突入電流抑制装置6は、励磁突入電流Iu,Iv,Iwを抑制するように、遮断器2を投入することができる。   As a result, if the voltage detectors 5M and 5T are installed on the secondary side of the modified Woodbridge connection transformer 3, the excitation inrush current suppressing device 6 can be used even if the voltage detector is not installed on the primary side. The circuit breaker 2 can be turned on so as to suppress the magnetizing inrush currents Iu, Iv, Iw.

また、2段階の投入目標位相Tc1,Tc2は、残留磁束の絶対値が最大となる相を判断した後は、1つの相の相電圧と定常磁束を監視すれば、他の2つの相を監視しなくても同定できる。従って、2段階の投入目標位相Tc1,Tc2を同定するための励磁突入電流抑制装置6における演算負荷を軽減することができる。   In addition, after determining the phase in which the absolute value of the residual magnetic flux is maximum, the two target target phases Tc1 and Tc2 are monitored for the other two phases by monitoring the phase voltage and steady magnetic flux of one phase. You can identify without. Therefore, it is possible to reduce the calculation load in the inrush current suppression device 6 for identifying the two target input phases Tc1 and Tc2.

(第2の実施形態)
図14は、本発明の第2の実施形態に係る励磁突入電流抑制装置6Aの適用された電力系統システムの構成を示す構成図である。
(Second Embodiment)
FIG. 14: is a block diagram which shows the structure of the electric power grid | system system to which the magnetizing inrush current suppression apparatus 6A which concerns on the 2nd Embodiment of this invention was applied.

励磁突入電流抑制装置6Aは、図1に示す第1の実施形態に係る励磁突入電流抑制装置6において、位相検出部605を位相検出部605Aに代えたものである。その他の点は、第1の実施形態と同様である。   The excitation inrush current suppression device 6A is obtained by replacing the phase detection unit 605 with a phase detection unit 605A in the excitation inrush current suppression device 6 according to the first embodiment shown in FIG. Other points are the same as in the first embodiment.

位相検出部605Aは、1段階目の投入目標位相Tc1の同定方法が異なる点以外は、第1の実施形態に位相検出部605と同様である。   The phase detection unit 605A is the same as the phase detection unit 605 in the first embodiment, except that the identification method of the input target phase Tc1 at the first stage is different.

位相検出部605Aは、三相の残留磁束φZu,φZv,φZwのうち絶対値が最大の相を検出する。位相検出部605Aは、検出した相において、定常磁束が残留磁束の極性と一致した波高値(波形の最大値)となるような位相を1段階目の投入目標位相Tc1として同定する。この同定した1段階目の投入目標位相Tc1の時点での同相の相電圧は、零点である。   The phase detector 605A detects the phase having the maximum absolute value among the three-phase residual magnetic fluxes φZu, φZv, and φZw. In the detected phase, the phase detector 605A identifies the phase at which the steady magnetic flux has a peak value (maximum value of the waveform) that matches the polarity of the residual magnetic flux as the first target phase Tc1. The phase voltage of the in-phase at the time of the identified first target input phase Tc1 is zero.

次に、図15〜図19を参照して、励磁突入電流抑制装置6Aによる励磁突入電流の抑制について説明する。   Next, with reference to FIG. 15 to FIG. 19, suppression of the magnetizing inrush current by the magnetizing inrush current suppressing device 6A will be described.

図15及び図16は、励磁突入電流抑制装置6Aによる遮断器2の遮断Tp前後の状態の一例を示している。図15は、1次側相電圧Vu,Vv,Vwを示す波形図である。図16は、1次側相磁束φu,φv,φwを示す波形図である。図17〜図19は、励磁突入電流抑制装置6Aによる遮断器2の投入Tc1,Tc2前後の状態の一例を示している。図17は、1次側相電圧Vu,Vv,Vwを示す波形図である。図18は、1次側相磁束φu,φv,φwを示す波形図である。図19は、1次側相電流(励磁突入電流)Iu,Iv,Iwを示す波形図である。   FIG.15 and FIG.16 has shown an example of the state before and behind interruption | blocking Tp of the circuit breaker 2 by the magnetizing inrush current suppression apparatus 6A. FIG. 15 is a waveform diagram showing primary side phase voltages Vu, Vv, Vw. FIG. 16 is a waveform diagram showing primary side phase magnetic fluxes φu, φv, and φw. FIGS. 17-19 has shown an example of the state before and after closing | fastening Tc1 and Tc2 of the circuit breaker 2 by the magnetizing inrush current suppression apparatus 6A. FIG. 17 is a waveform diagram showing primary side phase voltages Vu, Vv, Vw. FIG. 18 is a waveform diagram showing primary side phase magnetic fluxes φu, φv, and φw. FIG. 19 is a waveform diagram showing primary side phase currents (excitation inrush currents) Iu, Iv, Iw.

変形ウッドブリッジ結線変圧器3の1次側に図15に示す三相交流電圧Vu,Vv,Vwが印加されている場合、遮断器2が開極した後(遮断Tp後)は、図16に示す残留磁束φZu,φZv,φZwが残る。このとき、絶対値が最大の残留磁束は、U相の残留磁束φZuである。   When the three-phase AC voltages Vu, Vv, and Vw shown in FIG. 15 are applied to the primary side of the modified Woodbridge connection transformer 3, after the circuit breaker 2 is opened (after the circuit break Tp), FIG. The residual magnetic fluxes φZu, φZv, φZw shown remain. At this time, the residual magnetic flux having the maximum absolute value is the U-phase residual magnetic flux φZu.

従って、励磁突入電流抑制装置6Aは、図18に示すように、U相の定常磁束φTuがU相の残留磁束φZuと同一の極性で略波高値となる位相を、U相の遮断器2を投入するための1段階目の投入目標位相Tc1として同定する。1段階目の投入目標位相Tc1は、図17に示すように、U相電圧Vuが零点の位相でもある。従って、この場合は、U相電圧Vuが零点の位相を1段階目の投入目標位相Tc1として同定してもよい。励磁突入電流抑制装置6Aは、同定した1段階目の投入目標位相Tc1で、U相の遮断器2を投入する。   Accordingly, as shown in FIG. 18, the magnetizing inrush current suppressing device 6A sets the phase at which the U-phase steady-state magnetic flux φTu has the same polarity as the U-phase residual magnetic flux φZu and has a peak value, as shown in FIG. It is identified as the first target injection phase Tc1 for input. The first stage input target phase Tc1 is also a phase where the U-phase voltage Vu is zero as shown in FIG. Therefore, in this case, the phase at which the U-phase voltage Vu is zero may be identified as the first target phase Tc1. The magnetizing inrush current suppressing device 6A inputs the U-phase circuit breaker 2 at the identified first target closing target phase Tc1.

U相の遮断器2を投入後、励磁突入電流抑制装置6Aは、第1の実施形態と同様に、2段階目の投入目標位相Tc2を同定し、残りのV相及びW相の遮断器2を投入する。   After turning on the U-phase circuit breaker 2, the magnetizing inrush current suppressing device 6 </ b> A identifies the second turn-on target phase Tc <b> 2 as in the first embodiment, and the remaining V-phase and W-phase circuit breakers 2. .

このように励磁突入電流抑制装置6Aが遮断器2を投入することにより、図19に示すように、各相の遮断器電流(励磁突入電流)Iu,Iv,Iwが抑制される。各相の遮断器電流Iu,Iv,Iwは、数10[A]程度である。これは、変圧器の励磁電流レベルよりも多いが、通常の励磁突入電流レベルよりも少ない。   Thus, when the exciting inrush current suppressing device 6A turns on the circuit breaker 2, the circuit breaker currents (exciting inrush currents) Iu, Iv, and Iw of each phase are suppressed as shown in FIG. The circuit breaker currents Iu, Iv, and Iw of each phase are about several tens [A]. This is greater than the transformer excitation current level, but less than the normal excitation inrush current level.

本実施形態によれば、定常磁束φTu,φTv,φTwの波高値を検出して、1段階目の投入目標位相Tc1を同定するため、第1の実施形態よりも、1段階目の投入目標位相Tc1を同定する演算負荷を軽減することができる。また、1段階目の投入目標位相Tc1から2段階目の投入目標位相Tc2までの時間(位相)は、波高値から零点までの時間となるため、常に一定にすることができる。これにより、2段階目の投入目標位相Tc2を同定する精度を高め、演算負荷を軽減することができる。   According to the present embodiment, since the peak values of the steady magnetic fluxes φTu, φTv, and φTw are detected and the first-stage input target phase Tc1 is identified, the first-stage input target phase is more than that of the first embodiment. The calculation load for identifying Tc1 can be reduced. In addition, the time (phase) from the first stage target target phase Tc1 to the second stage target target phase Tc2 is the time from the peak value to the zero point, and can be always constant. As a result, the accuracy of identifying the second stage input target phase Tc2 can be improved, and the calculation load can be reduced.

(第3の実施形態)
図20は、本発明の第3の実施形態に係る励磁突入電流抑制装置6Bの適用された電力系統システムの構成を示す構成図である。
(Third embodiment)
FIG. 20 is a configuration diagram showing a configuration of a power system to which the magnetizing inrush current suppressing device 6B according to the third embodiment of the present invention is applied.

励磁突入電流抑制装置6Bは、図1に示す第1の実施形態に係る励磁突入電流抑制装置6において、位相検出部605の代わりに、位相検出部605Bを設け、計測情報保持部607、開極位相制御部608、及び開極指令出力部609を追加した構成である。その他の構成は、第1の実施形態に係る励磁突入電流抑制装置6と同様である。   The magnetizing inrush current suppressing device 6B includes a phase detecting unit 605B instead of the phase detecting unit 605 in the magnetizing inrush current suppressing device 6 according to the first embodiment shown in FIG. In this configuration, a phase control unit 608 and an opening command output unit 609 are added. Other configurations are the same as those of the magnetizing inrush current suppressing device 6 according to the first embodiment.

励磁突入電流抑制装置6Bの運用前に、計測情報保持部607は、遮断器2を複数回遮断したときにおける、変圧器電圧変換部610により算出された1次側相電圧VDu,VDv,VDwの電圧遮断位相と、残留磁束算出部604により算出された残留磁束φZu,φZv,φZwの磁束信号とを計測する。計測情報保持部607は、計測された電圧遮断位相及び磁束信号に基づいて、遮断位相と残留磁束との関係などの残留磁束の特性に関する情報を計測情報として保持する。   Before the operation of the magnetizing inrush current suppression device 6B, the measurement information holding unit 607 is configured to output the primary side phase voltages VDu, VDv, and VDw calculated by the transformer voltage conversion unit 610 when the circuit breaker 2 is interrupted a plurality of times. The voltage cutoff phase and the magnetic flux signals of the residual magnetic fluxes φZu, φZv, and φZw calculated by the residual magnetic flux calculation unit 604 are measured. The measurement information holding unit 607 holds, as measurement information, information on the characteristics of the residual magnetic flux, such as the relationship between the cutoff phase and the residual magnetic flux, based on the measured voltage cutoff phase and magnetic flux signal.

開極位相制御部608には、計測情報保持部607に保持された計測情報及び電源電圧計測部601により計測された電源母線1の各相電圧Vu,Vv,Vwが入力される。開極位相制御部608は、計測情報から各相の残留磁束φZu,φZv,φZwを推定する。開極位相制御部608は、推定した各相の残留磁束φZu,φZv,φZw及び各相電圧に基づいて、遮断位相が常に同じになるように、遮断器2の主接点の開極位相を制御する。開極位相制御部608は、制御した開極位相を開極指令出力部609に出力する。   The opening phase control unit 608 receives the measurement information held in the measurement information holding unit 607 and the phase voltages Vu, Vv, Vw of the power supply bus 1 measured by the power supply voltage measurement unit 601. The opening phase control unit 608 estimates the residual magnetic flux φZu, φZv, φZw of each phase from the measurement information. The opening phase control unit 608 controls the opening phase of the main contact of the circuit breaker 2 based on the estimated residual magnetic fluxes φZu, φZv, φZw of each phase and the phase voltages so that the breaking phase is always the same. To do. The opening phase control unit 608 outputs the controlled opening phase to the opening command output unit 609.

開極指令出力部609は、開極位相制御部608から受信した開極位相に基づいて、遮断器2の主接点を駆動する操作機構に対して開極指令を出力する。これにより、遮断器2は、開放される。   The opening command output unit 609 outputs the opening command to the operation mechanism that drives the main contact of the circuit breaker 2 based on the opening phase received from the opening phase control unit 608. Thereby, the circuit breaker 2 is opened.

位相検出部605Bには、計測情報保持部607に保持されている計測情報及び定常磁束算出部602により算出された各相の定常磁束φTu,φTv,φTwが入力される。位相検出部605Bは、計測情報保持部607に保持されている計測情報から各相の残留磁束φZu,φZv,φZwを推定する。位相検出部605Bは、各相の残留磁束φZu,φZv,φZw及び各相の定常磁束φTu,φTv,φTwに基づいて、遮断器2を投入する2段階の投入目標位相Tc1,Tc2を同定する。2段階の投入目標位相Tc1,Tc2を同定する方法については、第1の実施形態又は第2の実施形態と同様である。   The phase detection unit 605B receives the measurement information held in the measurement information holding unit 607 and the steady magnetic flux φTu, φTv, φTw of each phase calculated by the steady magnetic flux calculation unit 602. The phase detector 605B estimates the residual magnetic flux φZu, φZv, φZw of each phase from the measurement information held in the measurement information holding unit 607. The phase detection unit 605B identifies the two-stage application target phases Tc1 and Tc2 for applying the circuit breaker 2 based on the residual magnetic fluxes φZu, φZv, φZw of each phase and the steady magnetic fluxes φTu, φTv, φTw of each phase. The method for identifying the two target input phases Tc1 and Tc2 is the same as that in the first embodiment or the second embodiment.

ここで、開極位相制御部608は、常に遮断位相が同じになるように、位相制御をしている。従って、位相検出部605Bは、計測情報保持部607に保持されている情報に変更がなければ(計測情報を更新していなければ)、常に2段階の投入目標位相Tc1,Tc2は同じでよい。   Here, the opening phase control unit 608 performs phase control so that the cutoff phase is always the same. Therefore, if the information held in the measurement information holding unit 607 is not changed (the measurement information is not updated), the phase detection unit 605B may always have the same two-step input target phases Tc1 and Tc2.

本実施形態によれば、第1の実施形態と同様の作用効果に加え、以下の作用効果を得ることができる。   According to the present embodiment, in addition to the same functions and effects as those of the first embodiment, the following functions and effects can be obtained.

電力系統に遮断器2及び変形ウッドブリッジ結線変圧器3などを一旦設置した後は、この電力系統の回路条件は、常に同じである。このため、遮断器2が遮断するときの位相を常に同じにしておけば、変形ウッドブリッジ結線変圧器3の残留磁束φZu,φZv,φZwの値も常に同じになるはずである。   After the circuit breaker 2 and the modified Woodbridge connection transformer 3 are once installed in the power system, the circuit conditions of the power system are always the same. Therefore, if the phase when the circuit breaker 2 is interrupted is always the same, the residual magnetic fluxes φZu, φZv, φZw of the modified Woodbridge connection transformer 3 should always be the same.

励磁突入電流抑制装置6Bは、遮断器2で変形ウッドブリッジ結線変圧器3を遮断する際、遮断位相が常に同じになるように遮断器2の開極位相を制御して遮断する。即ち、励磁突入電流抑制装置6Bは、各相の残留磁束φZu,φZv,φZwを常に同じ値とすることができる。従って、励磁突入電流抑制装置6Bは、遮断器2を投入させて変形ウッドブリッジ結線変圧器3を励磁させるときも、励磁突入電流の抑制をするための投入位相を常に同じ位相にすることができる。   When the breaker 2 cuts off the modified Woodbridge connection transformer 3, the magnetizing inrush current suppression device 6 </ b> B controls the breaking phase of the breaker 2 so that the breaking phase is always the same. That is, the magnetizing inrush current suppressing device 6B can always set the residual magnetic fluxes φZu, φZv, φZw of each phase to the same value. Therefore, the exciting inrush current suppressing device 6B can always make the closing phase for suppressing the exciting inrush current even when the breaker 2 is turned on to excite the deformed wood bridge connection transformer 3. .

従って、変圧器2次側電圧検出器5M,5Tが常時接続されていない場合でも、励磁突入電流抑制装置6Bは、計測情報保持部607に保持されている計測情報に基づいて、遮断器2が遮断した後の変形ウッドブリッジ結線変圧器3の残留磁束φZu,φZv,φZwの情報を常に得ることができる。従って、変圧器2次側電圧検出器5M,5Tは、計測情報保持部607による計測時のみ接続し、通常の運用状態では取り外すこともできる。もちろん、変圧器1次側電圧検出器5M,5Tは、恒久的に設置されていても良い。   Therefore, even when the transformer secondary voltage detectors 5M and 5T are not always connected, the magnetizing inrush current suppression device 6B is configured so that the circuit breaker 2 is based on the measurement information held in the measurement information holding unit 607. Information on the residual magnetic fluxes φZu, φZv, φZw of the deformed wood bridge connection transformer 3 after being interrupted can always be obtained. Therefore, the transformer secondary side voltage detectors 5M and 5T can be connected only during measurement by the measurement information holding unit 607, and can be removed in a normal operation state. Of course, the transformer primary side voltage detectors 5M and 5T may be permanently installed.

(第4の実施形態)
図21は、本発明の第4の実施形態に係る励磁突入電流抑制装置6Cの適用された電力系統システムの構成を示す構成図である。
(Fourth embodiment)
FIG. 21 is a configuration diagram showing a configuration of a power system to which the magnetizing inrush current suppressing device 6C according to the fourth embodiment of the present invention is applied.

励磁突入電流抑制装置6Cは、図20に示す第3の実施形態に係る励磁突入電流抑制装置6Bにおいて、残留磁束算出部604を残留磁束算出部604Cに代え、計測情報保持部607を計測情報保持部607Cに代え、位相検出部605Bを位相検出部605Cに代え、変圧器電圧変換部610及び定常磁束算出部602を取り除いた構成である。その他の構成については、第3の実施形態と同様である。   In the magnetizing inrush current suppressing device 6C according to the third embodiment shown in FIG. 20, the magnetizing inrush current suppressing device 6C replaces the residual magnetic flux calculating unit 604 with the residual magnetic flux calculating unit 604C and holds the measurement information holding unit 607 in the measuring information holding. Instead of the unit 607C, the phase detection unit 605B is replaced with the phase detection unit 605C, and the transformer voltage conversion unit 610 and the steady magnetic flux calculation unit 602 are removed. Other configurations are the same as those in the third embodiment.

残留磁束算出部604Cは、遮断器2による変形ウッドブリッジ結線変圧器3の遮断直後に、変圧器電圧計測部603により計測された2組の単相交流電圧Vt,Vmをそれぞれ積分する。残留磁束算出部604Cは、この積分された値を、変形ウッドブリッジ結線変圧器3の鉄心の残留磁束(2次側磁束)φZt,φZmとする。残留磁束算出部604Cは、演算した残留磁束φZt,φZmを位相検出部605Cに出力する。   The residual magnetic flux calculation unit 604C integrates the two sets of single-phase AC voltages Vt and Vm measured by the transformer voltage measurement unit 603 immediately after the breaker 2 cuts off the modified Woodbridge connection transformer 3. The residual magnetic flux calculation unit 604C sets the integrated value as the residual magnetic flux (secondary magnetic flux) φZt and φZm of the iron core of the modified Woodbridge connection transformer 3. The residual magnetic flux calculator 604C outputs the calculated residual magnetic fluxes φZt and φZm to the phase detector 605C.

励磁突入電流抑制装置6Cの運用前に、計測情報保持部607Cは、遮断器2を複数回遮断したときにおける、変圧器電圧計測部603により計測された2次側電圧Vm,Vtの電圧遮断位相と、残留磁束算出部604Cにより算出された残留磁束φZt,φZmの磁束信号とを計測する。計測情報保持部607Cは、計測された電圧遮断位相及び磁束信号に基づいて、遮断位相と残留磁束との関係などの残留磁束の特性に関する情報を計測情報として保持する。   Prior to the operation of the magnetizing inrush current suppressing device 6C, the measurement information holding unit 607C has the voltage cutoff phases of the secondary side voltages Vm and Vt measured by the transformer voltage measuring unit 603 when the circuit breaker 2 is interrupted a plurality of times. And the magnetic flux signals of the residual magnetic fluxes φZt and φZm calculated by the residual magnetic flux calculation unit 604C. The measurement information holding unit 607C holds, as measurement information, information on the characteristics of the residual magnetic flux, such as the relationship between the cutoff phase and the residual magnetic flux, based on the measured voltage cutoff phase and magnetic flux signal.

開極位相制御部608には、計測情報保持部607Cに保持された計測情報及び電源電圧計測部601により計測された電源母線1の各相電圧Vu,Vv,Vwが入力される。開極位相制御部608は、計測情報から変形ウッドブリッジ結線変圧器3の2次側巻線の残留磁束φZm,φZtを推定する。開極位相制御部608Cは、推定した残留磁束φZm,φZt及び各相電圧に基づいて、遮断位相が常に同じになるように、遮断器2の主接点の開極位相を制御する。開極位相制御部608Cは、制御した開極位相を開極指令出力部609に出力する。   The opening phase control unit 608 receives the measurement information held in the measurement information holding unit 607C and the phase voltages Vu, Vv, Vw of the power supply bus 1 measured by the power supply voltage measurement unit 601. The opening phase control unit 608 estimates the residual magnetic fluxes φZm and φZt of the secondary winding of the modified Woodbridge connection transformer 3 from the measurement information. The opening phase control unit 608C controls the opening phase of the main contact of the circuit breaker 2 so that the interruption phase is always the same based on the estimated residual magnetic fluxes φZm and φZt and the phase voltages. The opening phase control unit 608C outputs the controlled opening phase to the opening command output unit 609.

開極指令出力部609は、開極位相制御部608から受信した開極位相に基づいて、遮断器2の主接点を駆動する操作機構に対して開極指令を出力する。これにより、遮断器2は、開放される。   The opening command output unit 609 outputs the opening command to the operation mechanism that drives the main contact of the circuit breaker 2 based on the opening phase received from the opening phase control unit 608. Thereby, the circuit breaker 2 is opened.

位相検出部605Cには、計測情報保持部607Cに保持されている計測情報及び電源電圧計測部601により計測された電源母線1の各相電圧Vu,Vv,Vwが入力される。位相検出部605Cは、遮断器2を投入する2段階の投入目標位相Tc1,Tc2を同定する。2段階の投入目標位相Tc1,Tc2を同定する方法については、第1の実施形態又は第2の実施形態と同様である。   The phase detection unit 605C receives the measurement information held in the measurement information holding unit 607C and the phase voltages Vu, Vv, Vw of the power supply bus 1 measured by the power supply voltage measurement unit 601. The phase detection unit 605C identifies the two-stage closing target phases Tc1 and Tc2 at which the circuit breaker 2 is turned on. The method for identifying the two target input phases Tc1 and Tc2 is the same as that in the first embodiment or the second embodiment.

次に、図22及び図23を参照して、励磁突入電流抑制装置6Cによる励磁突入電流の抑制について説明する。   Next, with reference to FIG.22 and FIG.23, suppression of the excitation inrush current by the excitation inrush current suppression apparatus 6C is demonstrated.

図22及び図23は、励磁突入電流抑制装置6Cによる遮断器2の遮断Tp前後の状態の一例を示している。図22は、変形ウッドブリッジ変圧器3の1次側相磁束φu,φv,φwの残留磁束φZu,φZv,φZwを示す波形図である。図23は、変形ウッドブリッジ変圧器3の2次側巻線磁束φt,φmの残留磁束φZt,φZmを示す波形図である。図22及び図23は、p.u.表示で示している。   22 and 23 show an example of a state before and after the circuit breaker Tp of the circuit breaker 2 by the magnetizing inrush current suppressing device 6C. FIG. 22 is a waveform diagram showing the residual magnetic fluxes φZu, φZv, φZw of the primary side phase magnetic fluxes φu, φv, φw of the modified Woodbridge transformer 3. FIG. 23 is a waveform diagram showing the residual magnetic fluxes φZt and φZm of the secondary winding magnetic fluxes φt and φm of the modified Woodbridge transformer 3. 22 and 23 show p. u. Shown in the display.

ここで、変形ウッドブリッジ変圧器3の2次側のT座の単相電圧Vtと1次側のU相電圧Vuとは、同位相である。   Here, the single-phase voltage Vt at the T-seat on the secondary side of the modified Woodbridge transformer 3 and the U-phase voltage Vu on the primary side have the same phase.

図22及び図23に示すように、これらを積分したT座の2次側巻線磁束φtと1次側U相磁束φuも同位相となる。また、p.u.表示すれば、T座の2次側巻線磁束φtの残留磁束φZtと1次側U相磁束φuの残留磁束φZuは、同じになる。   As shown in FIGS. 22 and 23, the secondary winding magnetic flux φt and the primary U-phase magnetic flux φu of the T seat obtained by integrating them are also in the same phase. P. u. In other words, the residual magnetic flux φZt of the secondary winding magnetic flux φt of the T seat is the same as the residual magnetic flux φZu of the primary U-phase magnetic flux φu.

従って、開極位相制御部608が、常にT座の2次側巻線磁束φtが最大の絶対値(波高値)となるように同じ位相で開極位相を制御することで、位相検出部605Cは、1次側U相電圧Vuの計測のみに基づいて、2段階の投入目標位相Tc1,Tc2の同定をすることができる。   Accordingly, the opening phase control unit 608 controls the opening phase with the same phase so that the secondary winding magnetic flux φt of the T seat always has the maximum absolute value (peak value), so that the phase detection unit 605C. Can identify the input target phases Tc1 and Tc2 in two stages based only on the measurement of the primary U-phase voltage Vu.

具体的には、開極位相制御部608は、T座の2次側巻線磁束φtが波高値となる位相で、遮断器2を開放するように位相を制御する。これにより、T座の2次側巻線の残留磁束φZtは、最大(定常磁束φtの波高値)となる。従って、1次側U相の残留磁束φZuも、1次側V相の残留磁束φZv及び1次側W相の残留磁束φZwよりも大きくなるはずである。開極位相制御部608がこのように遮断器2を開放させることで、位相検出部605Cは、U相電圧VuがT座の2次側巻線の残留磁束φZtと同極性から逆極性に遷移する略零点となる位相を1段階目の投入目標位相Tc1として同定すればよい。   Specifically, the opening phase control unit 608 controls the phase so that the circuit breaker 2 is opened at a phase where the secondary winding magnetic flux φt of the T seat has a peak value. As a result, the residual magnetic flux φZt of the secondary winding of the T seat becomes the maximum (the peak value of the steady magnetic flux φt). Therefore, the residual magnetic flux φZu of the primary U phase should be larger than the residual magnetic flux φZv of the primary V phase and the residual magnetic flux φZw of the primary W phase. When the opening phase control unit 608 opens the circuit breaker 2 in this way, the phase detection unit 605C causes the U-phase voltage Vu to transition from the same polarity to the reverse polarity as the residual magnetic flux φZt of the secondary winding of the T seat. What is necessary is just to identify the phase used as the substantially zero point to be 1st step | paragraph input target phase Tc1.

本実施形態によれば、第3の実施形態による作用効果と同様の作用効果を得ることができる。   According to the present embodiment, it is possible to obtain the same effects as the effects according to the third embodiment.

なお、各実施形態において、電源電圧検出器4U,4V,4Wにより、電源母線1の各相電圧を計測したが、電源母線1の各線間電圧を計測してもよい。各線間電圧を相電圧に変換することで、各実施形態と同様の構成にすることができる。   In each embodiment, each phase voltage of the power supply bus 1 is measured by the power supply voltage detectors 4U, 4V, 4W, but each line voltage of the power supply bus 1 may be measured. By converting each line voltage into a phase voltage, a configuration similar to each embodiment can be obtained.

また、各実施形態において、三相交流電圧を単相交流電圧に変換する変圧器として、変形ウッドブリッジ結線又はウッドブリッジ結線による変圧器について説明したが、他の結線による変圧器でもよい。例えば、有効接地系に適用される変圧器としては、ルーフデルタ結線変圧器でもよい。   Moreover, in each embodiment, although the transformer by a deformation | transformation wood bridge connection or a wood bridge connection was demonstrated as a transformer which converts a three-phase alternating current voltage into a single phase alternating voltage, the transformer by another connection may be used. For example, a roof delta connection transformer may be used as the transformer applied to the effective grounding system.

さらに、各実施形態において、励磁突入電流抑制装置6等での位相制御における各種パラメータは、より精度を高めるため等により補正をしてもよい。例えば、遮断器2の投入において、主接点間に発生するプレアークと呼ばれる先行放電や、操作機構の動作ばらつきなどに起因する投入時間のばらつきが存在する。このプレアークによる投入ばらつきや、遮断器投入時のばらつきは、あらかじめその特性を取得しておくことにより、位相制御を行う際にこの特性による補正をする。このような補正をすることで、これらのばらつきがあっても、励磁突入電流をより確実に抑制することができる。   Furthermore, in each embodiment, various parameters in the phase control in the excitation inrush current suppressing device 6 and the like may be corrected to improve accuracy. For example, when the circuit breaker 2 is turned on, there is a variation in closing time due to a preceding discharge called a pre-arc generated between the main contacts and a variation in operation of the operation mechanism. The characteristics of the throwing variation due to the pre-arc and the variation when the circuit breaker is thrown are acquired in advance, and correction is performed based on this characteristic when performing phase control. By performing such correction, the inrush current can be more reliably suppressed even if these variations occur.

また、各実施形態において、定常磁束及び残留磁束を演算する場合に、相電圧から線間電圧、又は線間電圧から各種巻線電圧などのように、電圧を変換してから磁束を求めたが、磁束を求めた後に、磁束を変換してもよい。例えば、各相電圧から各線間の磁束を求める場合、先に各相の磁束を求めた後に、各線間の磁束を求めてもよい。また、その他の演算においても、結果が同じになるのであれば、演算の順序や演算をさせる場所(励磁突入電流抑制装置の内部や外部を問わず、コンピュータや各種検出器等)は、適宜変更することができる。   Further, in each embodiment, when calculating the steady magnetic flux and the residual magnetic flux, the magnetic flux is obtained after converting the voltage from the phase voltage to the line voltage, or from the line voltage to various winding voltages, etc. After obtaining the magnetic flux, the magnetic flux may be converted. For example, when obtaining the magnetic flux between each line from each phase voltage, the magnetic flux between each line may be obtained after obtaining the magnetic flux of each phase first. Also, in other calculations, if the results are the same, the order of calculations and the place where the calculations are performed (regardless of the inside or outside of the magnetizing inrush current suppression device, the computer, various detectors, etc.) can be changed as appropriate. can do.

さらに、第1から第3の実施形態において、定常磁束φTu,φTv,φTwを演算する構成としたが、定常磁束φTu,φTv,φTwは、実際に演算しなくてもよい。具体的には、定常磁束φTu,φTv,φTwが相電圧Vv,Vu,Vwよりも90度遅れることを考慮することで、実質的な演算とみなすことができる。これ以外の演算についても、このような演算については同様である。また、第4の実施形態も同様に、このような演算については演算しなくてもよい。   Furthermore, in the first to third embodiments, the steady magnetic fluxes φTu, φTv, and φTw are calculated. However, the steady magnetic fluxes φTu, φTv, and φTw do not have to be actually calculated. Specifically, it can be regarded as a substantial calculation by considering that the steady magnetic fluxes φTu, φTv, φTw are delayed by 90 degrees from the phase voltages Vv, Vu, Vw. The same applies to other operations. Similarly, in the fourth embodiment, such a calculation need not be performed.

また、第4の実施形態において、残留磁束算出部604Cは、T座の残留磁束φZtを演算すれば、必ずしも主座の残留磁束φZmを演算しなくてもよい。   In the fourth embodiment, the residual magnetic flux calculation unit 604C does not necessarily calculate the residual magnetic flux φZm of the main seat as long as the residual magnetic flux φZt of the T seat is calculated.

なお、本発明のいくつかの実施形態を説明したが、これらの実施形態は、例として提示したものであり、発明の範囲を限定することは意図していない。これら新規な実施形態は、その他の様々な形態で実施されることが可能であり、発明の要旨を逸脱しない範囲で、種々の省略、置き換え、変更を行うことができる。これら実施形態やその変形は、発明の範囲や要旨に含まれるとともに、特許請求の範囲に記載された発明とその均等の範囲に含まれる。   In addition, although some embodiment of this invention was described, these embodiment is shown as an example and is not intending limiting the range of invention. These novel embodiments can be implemented in various other forms, and various omissions, replacements, and changes can be made without departing from the scope of the invention. These embodiments and modifications thereof are included in the scope and gist of the invention, and are included in the invention described in the claims and the equivalents thereof.

1…電源母線、2…遮断器、3…変形ウッドブリッジ結線変圧器、4U,4V,4W…電源電圧検出器、5M,5T…変圧器2次側電圧検出器、6…励磁突入電流抑制装置、601…電源電圧計測部、602…定常磁束算出部、603…変圧器電圧計測部、604…残留磁束算出部、605…位相検出部、606…投入指令出力部、610…変圧器電圧変換部。   DESCRIPTION OF SYMBOLS 1 ... Power supply bus line, 2 ... Circuit breaker, 3 ... Deformation wood bridge connection transformer, 4U, 4V, 4W ... Power supply voltage detector, 5M, 5T ... Transformer secondary side voltage detector, 6 ... Excitation inrush current suppression device 601 ... Power supply voltage measurement unit 602 ... Stationary magnetic flux calculation unit 603 ... Transformer voltage measurement unit 604 ... Residual magnetic flux calculation unit 605 ... Phase detection unit 606 ... Input command output unit 610 ... Transformer voltage conversion unit .

Claims (10)

電源を備えた三相交流の電力系統と三相交流電圧を単相交流電圧に変換する接地された変圧器との接続を相毎に開閉する遮断器の励磁突入電流を抑制する励磁突入電流抑制装置であって、
前記変圧器の単相交流電圧を計測する変圧器側単相交流電圧計測手段と、
前記変圧器側単相交流電圧計測手段により計測された前記変圧器の単相交流電圧を、前記変圧器の三相交流電圧に変換する変圧器側電圧変換手段と、
前記変圧器側電圧変換手段により変換された三相交流電圧に基づいて、前記遮断器による前記変圧器の遮断後の前記変圧器の三相の残留磁束を演算する残留磁束演算手段と、
前記遮断器よりも前記電源側の三相交流電圧を計測する電源側三相交流電圧計測手段と、
前記電源側三相交流電圧計測手段により計測された三相交流電圧に基づいて、前記変圧器の三相の定常磁束を演算する定常磁束演算手段と、
前記残留磁束演算手段により演算された前記三相の残留磁束のうち絶対値が最大の相を判断する相判断手段と、
前記相判断手段により判断された前記相において、前記残留磁束演算手段により演算された前記残留磁束と前記定常磁束演算手段により演算された前記定常磁束とが一致するような第1の位相を判断する第1の位相判断手段と、
前記第1の位相判断手段により判断された前記第1の位相で、前記相判断手段により判断された前記相の前記遮断器を投入する第1の投入手段と、
前記第1の位相判断手段により判断された前記第1の位相よりも後に、前記相判断手段により判断された前記相の前記電源側の交流電圧が、前記相判断手段により判断された前記相の残留磁束と同極性から逆極性に遷移する零点となるような第2の位相を判断する第2の位相判断手段と、
前記第2の位相判断手段により判断された前記第2の位相で、投入されていない他の2相の前記遮断器を投入する第2の投入手段と
を備えたことを特徴とする励磁突入電流抑制装置。
Inrush current suppression that suppresses the excitation inrush current of the circuit breaker that opens and closes the connection between the three-phase AC power system with power supply and the grounded transformer that converts the three-phase AC voltage into a single-phase AC voltage. A device,
Transformer-side single-phase AC voltage measuring means for measuring the single-phase AC voltage of the transformer,
Transformer-side voltage conversion means for converting the single-phase AC voltage of the transformer measured by the transformer-side single-phase AC voltage measurement means into a three-phase AC voltage of the transformer;
Based on the three-phase AC voltage converted by the transformer-side voltage conversion means, residual magnetic flux calculating means for calculating the three-phase residual magnetic flux of the transformer after the transformer is interrupted by the circuit breaker;
A power source side three-phase AC voltage measuring means for measuring the power source side three-phase AC voltage from the circuit breaker;
Based on the three-phase AC voltage measured by the power-source-side three-phase AC voltage measuring means, the steady-state magnetic flux calculating means for calculating the three-phase steady-state magnetic flux of the transformer,
Phase determining means for determining a phase having the maximum absolute value among the three-phase residual magnetic fluxes calculated by the residual magnetic flux calculating means;
In the phase determined by the phase determining means, a first phase is determined such that the residual magnetic flux calculated by the residual magnetic flux calculating means matches the steady magnetic flux calculated by the steady magnetic flux calculating means. First phase determining means;
First closing means for closing the circuit breaker of the phase determined by the phase determining means at the first phase determined by the first phase determining means;
After the first phase determined by the first phase determining means, the AC voltage on the power source side of the phase determined by the phase determining means is the phase of the phase determined by the phase determining means. A second phase determining means for determining a second phase that becomes a zero point that transitions from the same polarity to the opposite polarity as the residual magnetic flux;
An inrush current of excitation characterized by comprising: a second closing means for turning on the other two-phase circuit breakers that are not turned on at the second phase determined by the second phase determining means. Suppression device.
電源を備えた三相交流の電力系統と三相交流電圧を単相交流電圧に変換する接地された変圧器との接続を相毎に開閉する遮断器の励磁突入電流を抑制する励磁突入電流抑制装置であって、
前記変圧器の単相交流電圧を計測する変圧器側単相交流電圧計測手段と、
前記変圧器側単相交流電圧計測手段により計測された前記変圧器の単相交流電圧を、前記変圧器の三相交流電圧に変換する変圧器側電圧変換手段と、
前記変圧器側電圧変換手段により変換された三相交流電圧に基づいて、前記遮断器による前記変圧器の遮断後の前記変圧器の三相の残留磁束を演算する残留磁束演算手段と、
前記遮断器よりも前記電源側の三相交流電圧を計測する電源側三相交流電圧計測手段と、
前記電源側三相交流電圧計測手段により計測された三相交流電圧に基づいて、前記変圧器の三相の定常磁束を演算する定常磁束演算手段と、
前記残留磁束演算手段により演算された前記三相の残留磁束のうち絶対値が最大の相を判断する相判断手段と、
前記相判断手段により判断された前記相において、前記定常磁束演算手段により演算された前記定常磁束が残留磁束演算手段により演算された前記残留磁束と極性が一致する波高値となるような第1の位相を判断する第1の位相判断手段と、
前記第1の位相判断手段により判断された前記第1の位相で、前記相判断手段により判断された前記相の前記遮断器を投入する第1の投入手段と、
前記第1の位相判断手段により判断された前記第1の位相よりも後に、前記相判断手段により判断された前記相の前記電源側の交流電圧が、前記相判断手段により判断された前記相の残留磁束と同極性から逆極性に遷移する零点となるような第2の位相を判断する第2の位相判断手段と、
前記第2の位相判断手段により判断された前記第2の位相で、投入されていない他の2相の前記遮断器を投入する第2の投入手段と
を備えたことを特徴とする励磁突入電流抑制装置。
Inrush current suppression that suppresses the excitation inrush current of the circuit breaker that opens and closes the connection between the three-phase AC power system with power supply and the grounded transformer that converts the three-phase AC voltage into a single-phase AC voltage. A device,
Transformer-side single-phase AC voltage measuring means for measuring the single-phase AC voltage of the transformer,
Transformer-side voltage conversion means for converting the single-phase AC voltage of the transformer measured by the transformer-side single-phase AC voltage measurement means into a three-phase AC voltage of the transformer;
Based on the three-phase AC voltage converted by the transformer-side voltage conversion means, residual magnetic flux calculating means for calculating the three-phase residual magnetic flux of the transformer after the transformer is interrupted by the circuit breaker;
A power source side three-phase AC voltage measuring means for measuring the power source side three-phase AC voltage from the circuit breaker;
Based on the three-phase AC voltage measured by the power-source-side three-phase AC voltage measuring means, the steady-state magnetic flux calculating means for calculating the three-phase steady-state magnetic flux of the transformer,
Phase determining means for determining a phase having the maximum absolute value among the three-phase residual magnetic fluxes calculated by the residual magnetic flux calculating means;
In the phase determined by the phase determining means, a first peak value such that the steady magnetic flux calculated by the steady magnetic flux calculating means has a peak value whose polarity coincides with the residual magnetic flux calculated by the residual magnetic flux calculating means. First phase determining means for determining a phase;
First closing means for closing the circuit breaker of the phase determined by the phase determining means at the first phase determined by the first phase determining means;
After the first phase determined by the first phase determining means, the AC voltage on the power source side of the phase determined by the phase determining means is the phase of the phase determined by the phase determining means. A second phase determining means for determining a second phase that becomes a zero point that transitions from the same polarity to the opposite polarity as the residual magnetic flux;
An inrush current of excitation characterized by comprising: a second closing means for turning on the other two-phase circuit breakers that are not turned on at the second phase determined by the second phase determining means. Suppression device.
前記遮断器を少なくとも1回開放操作したときの前記変圧器の残留磁束及び前記遮断器の遮断位相を計測した情報を保持する計測情報保持手段と、
前記計測情報保持手段に保持された情報に基づいて、同一の遮断位相で前記遮断器を開放するための開放手段とを備え、
前記投入手段は、前記開放手段による前記遮断位相に基づいて、前記遮断器を投入すること
を特徴とする請求項1又は請求項2に記載の励磁突入電流抑制装置。
Measurement information holding means for holding information measuring the residual magnetic flux of the transformer and the breaking phase of the breaker when the breaker is opened at least once;
Based on the information held in the measurement information holding means, comprising an opening means for opening the circuit breaker at the same breaking phase,
The magnetizing inrush current suppressing device according to claim 1 or 2, wherein the closing unit switches on the circuit breaker based on the breaking phase by the opening unit.
電源を備えた三相交流の電力系統と三相交流電圧を第1の相と第2の相からなる2組の単相交流電圧に変換する接地された変圧器との接続を相毎に開閉する遮断器の励磁突入電流を抑制する励磁突入電流抑制装置であって、
前記変圧器の単相交流電圧を計測する変圧器側単相交流電圧計測手段と、
前記変圧器側単相交流電圧計測手段により計測された前記変圧器の単相交流電圧に基づいて、前記遮断器による前記変圧器の遮断後の前記変圧器の単相交流側巻線の前記第1の相の残留磁束を演算する残留磁束演算手段と、
前記遮断器を少なくとも1回開放操作したときの前記変圧器の残留磁束及び前記遮断器の遮断位相を計測した情報を保持する計測情報保持手段と、
前記計測情報保持手段に保持された情報に基づいて、前記残留磁束演算手段により演算された前記第1の相の残留磁束が最大となるような遮断位相で前記遮断器を開放するための開放手段と、
前記遮断器よりも前記電源側の三相交流電圧を計測する電源側三相交流電圧計測手段と、
前記電源側三相交流電圧計測手段により計測された三相交流電圧のうち前記第1の相と同位相の相電圧が、前記残留磁束演算手段により演算された前記第1の相の残留磁束と同極性から逆極性に遷移する零点となるような第1の位相を判断する第1の位相判断手段と、
前記第1の位相判断手段により判断された前記第1の位相で、前記第1の相と同位相の前記相の前記遮断器を投入する第1の投入手段と、
前記第1の位相判断手段により判断された前記第1の位相よりも後に、前記第1の相と同位相の前記相の相電圧が、前記残留磁束演算手段により演算された前記第1の相の残留磁束と同極性から逆極性に遷移する零点となるような第2の位相を判断する第2の位相判断手段と、
前記第2の位相判断手段により判断された前記第2の位相で、投入されていない他の2相の前記遮断器を投入する第2の投入手段と
を備えたことを特徴とする励磁突入電流抑制装置。
Open and close connections for each phase with a three-phase AC power system equipped with a power supply and a grounded transformer that converts the three-phase AC voltage into two sets of single-phase AC voltages consisting of the first and second phases An inrush current suppression device for suppressing an inrush current of a circuit breaker that
Transformer-side single-phase AC voltage measuring means for measuring the single-phase AC voltage of the transformer,
Based on the single-phase AC voltage of the transformer measured by the transformer-side single-phase AC voltage measuring means, the first of the single-phase AC side windings of the transformer after the transformer is shut off by the circuit breaker. Residual magnetic flux calculating means for calculating the residual magnetic flux of one phase;
Measurement information holding means for holding information measuring the residual magnetic flux of the transformer and the breaking phase of the breaker when the breaker is opened at least once;
Based on the information held in the measurement information holding means, an opening means for opening the circuit breaker at a breaking phase that maximizes the residual magnetic flux of the first phase calculated by the residual magnetic flux calculating means. When,
A power source side three-phase AC voltage measuring means for measuring the power source side three-phase AC voltage from the circuit breaker;
Of the three-phase AC voltage measured by the power supply-side three-phase AC voltage measuring means, the phase voltage having the same phase as the first phase is the residual magnetic flux of the first phase calculated by the residual magnetic flux calculating means. First phase determination means for determining a first phase that becomes a zero point that transitions from the same polarity to a reverse polarity;
First closing means for closing the circuit breaker of the phase in the same phase as the first phase at the first phase determined by the first phase determining means;
After the first phase determined by the first phase determining means, the phase voltage of the phase having the same phase as the first phase is calculated by the residual magnetic flux calculating means. Second phase determining means for determining a second phase that is a zero point that transitions from the same polarity to the opposite polarity as the residual magnetic flux of
An inrush current of excitation characterized by comprising: a second closing means for turning on the other two-phase circuit breakers that are not turned on at the second phase determined by the second phase determining means. Suppression device.
前記第2の位相判断手段は、前記第1の位相判断手段により判断された前記第1の位相後、予め設定された時間後の零点を、前記第2の位相として判断すること
を特徴とする請求項1から請求項4のいずれか1項に記載の励磁突入電流抑制装置。
The second phase determining means determines a zero point after a preset time after the first phase determined by the first phase determining means as the second phase. The excitation inrush current suppression device according to any one of claims 1 to 4.
電源を備えた三相交流の電力系統と三相交流電圧を単相交流電圧に変換する接地された変圧器との接続を相毎に開閉する遮断器の励磁突入電流を抑制する励磁突入電流抑制方法であって、
前記変圧器の単相交流電圧を計測し、
計測した前記変圧器の単相交流電圧を、前記変圧器の三相交流電圧に変換し、
変換した前記変圧器の三相交流電圧に基づいて、前記遮断器による前記変圧器の遮断後の前記変圧器の三相の残留磁束を演算し、
前記遮断器よりも前記電源側の三相交流電圧を計測し、
計測した前記電源側の三相交流電圧に基づいて、前記変圧器の三相の定常磁束を演算し、
演算した前記三相の残留磁束のうち絶対値が最大の相を判断し、
判断した前記相において、演算した前記残留磁束と演算した前記定常磁束とが一致するような第1の位相を判断し、
判断した前記第1の位相で、判断した前記相の前記遮断器を投入し、
判断した前記第1の位相よりも後に、判断した前記相の前記電源側の交流電圧が、判断した前記相の残留磁束と同極性から逆極性に遷移する零点となるような第2の位相を判断し、
判断した前記第2の位相で、投入されていない他の2相の前記遮断器を投入すること
を含むことを特徴とする励磁突入電流抑制方法。
Inrush current suppression that suppresses the excitation inrush current of the circuit breaker that opens and closes the connection between the three-phase AC power system with power supply and the grounded transformer that converts the three-phase AC voltage into a single-phase AC voltage. A method,
Measure the single-phase AC voltage of the transformer,
The measured single-phase AC voltage of the transformer is converted into a three-phase AC voltage of the transformer,
Based on the converted three-phase AC voltage of the transformer, the three-phase residual magnetic flux of the transformer after the transformer is shut off by the circuit breaker,
Measure the three-phase AC voltage on the power supply side than the breaker,
Based on the measured three-phase AC voltage on the power source side, the three-phase steady-state magnetic flux of the transformer is calculated,
Judge the phase with the maximum absolute value among the calculated residual magnetic fluxes of the three phases,
In the determined phase, a first phase is determined such that the calculated residual magnetic flux and the calculated steady magnetic flux match,
At the determined first phase, turn on the circuit breaker of the determined phase;
After the determined first phase, a second phase is set such that the AC voltage on the power supply side of the determined phase becomes a zero point that transitions from the same polarity to the opposite polarity as the determined residual magnetic flux of the phase. Judgment
A method of suppressing a magnetizing inrush current, comprising: turning on the other two-phase circuit breakers that are not turned on at the determined second phase.
電源を備えた三相交流の電力系統と三相交流電圧を単相交流電圧に変換する接地された変圧器との接続を相毎に開閉する遮断器の励磁突入電流を抑制する励磁突入電流抑制方法であって、
前記変圧器の単相交流電圧を計測し、
計測した前記変圧器の単相交流電圧を、前記変圧器の三相交流電圧に変換し、
変換した前記変圧器の三相交流電圧に基づいて、前記遮断器による前記変圧器の遮断後の前記変圧器の三相の残留磁束を演算し、
前記遮断器よりも前記電源側の三相交流電圧を計測し、
計測した前記電源側の三相交流電圧に基づいて、前記変圧器の三相の定常磁束を演算し、
演算した前記三相の残留磁束のうち絶対値が最大の相を判断し、
判断した前記相において、演算した前記定常磁束が演算した前記残留磁束と極性が一致する波高値となるような第1の位相を判断し、
判断した前記第1の位相で、判断した前記相の前記遮断器を投入し、
判断した前記第1の位相よりも後に、判断した前記相の前記電源側の交流電圧が、判断した前記相の残留磁束と同極性から逆極性に遷移する零点となるような第2の位相を判断し、
判断した前記第2の位相で、投入されていない他の2相の前記遮断器を投入すること
を含むことを特徴とする励磁突入電流抑制方法。
Inrush current suppression that suppresses the excitation inrush current of the circuit breaker that opens and closes the connection between the three-phase AC power system with power supply and the grounded transformer that converts the three-phase AC voltage into a single-phase AC voltage. A method,
Measure the single-phase AC voltage of the transformer,
The measured single-phase AC voltage of the transformer is converted into a three-phase AC voltage of the transformer,
Based on the converted three-phase AC voltage of the transformer, the three-phase residual magnetic flux of the transformer after the transformer is shut off by the circuit breaker,
Measure the three-phase AC voltage on the power supply side than the breaker,
Based on the measured three-phase AC voltage on the power source side, the three-phase steady-state magnetic flux of the transformer is calculated,
Judge the phase with the maximum absolute value among the calculated residual magnetic fluxes of the three phases,
In the determined phase, a first phase is determined such that the calculated steady-state magnetic flux has a peak value whose polarity matches the calculated residual magnetic flux,
At the determined first phase, turn on the circuit breaker of the determined phase;
After the determined first phase, a second phase is set such that the AC voltage on the power supply side of the determined phase becomes a zero point that transitions from the same polarity to the opposite polarity as the determined residual magnetic flux of the phase. Judgment
A method of suppressing a magnetizing inrush current, comprising: turning on the other two-phase circuit breakers that are not turned on at the determined second phase.
前記遮断器を少なくとも1回開放操作したときの前記変圧器の残留磁束及び前記遮断器の遮断位相を計測した情報を保持し、
保持した情報に基づいて、同一の遮断位相で前記遮断器を開放し、
前記遮断器の投入は、開放した前記遮断位相に基づいて行うこと
を含むことを特徴とする請求項6又は請求項7に記載の励磁突入電流抑制方法。
Holding information measuring the residual magnetic flux of the transformer and the breaking phase of the breaker when the breaker is opened at least once;
Based on the information held, the circuit breaker is opened at the same breaking phase,
The method of suppressing an inrush current according to claim 6 or 7, characterized in that the circuit breaker is turned on based on the opened cut-off phase.
電源を備えた三相交流の電力系統と三相交流電圧を第1の相と第2の相からなる2組の単相交流電圧に変換する接地された変圧器との接続を相毎に開閉する遮断器の励磁突入電流を抑制する励磁突入電流抑制方法であって、
前記変圧器の単相交流電圧を計測し、
計測した前記変圧器の単相交流電圧に基づいて、前記遮断器による前記変圧器の遮断後の前記変圧器の単相交流側巻線の前記第1の相の残留磁束を演算し、
前記遮断器を少なくとも1回開放操作したときの前記変圧器の残留磁束及び前記遮断器の遮断位相を計測した情報を保持し、
保持した情報に基づいて、演算した前記第1の相の残留磁束が最大となるような遮断位相で前記遮断器を開放し、
前記遮断器よりも前記電源側の三相交流電圧を計測し、
計測した前記電源側の三相交流電圧のうち前記第1の相と同位相の相電圧が、演算した前記第1の相の残留磁束と同極性から逆極性に遷移する零点となるような第1の位相を判断し、
判断した前記第1の位相で、前記第1の相と同位相の前記相の前記遮断器を投入し、
判断した前記第1の位相よりも後に、前記第1の相と同位相の前記相の相電圧が、演算した前記第1の相の残留磁束と同極性から逆極性に遷移する零点となるような第2の位相を判断し、
判断した前記第2の位相で、投入されていない他の2相の前記遮断器を投入すること
を含むことを特徴とする励磁突入電流抑制方法。
Open and close connections for each phase with a three-phase AC power system equipped with a power supply and a grounded transformer that converts the three-phase AC voltage into two sets of single-phase AC voltages consisting of the first and second phases An inrush current suppression method for suppressing an inrush current of a circuit breaker
Measure the single-phase AC voltage of the transformer,
Based on the measured single-phase AC voltage of the transformer, the residual magnetic flux of the first phase of the single-phase AC side winding of the transformer after the transformer is interrupted by the circuit breaker,
Holding information measuring the residual magnetic flux of the transformer and the breaking phase of the breaker when the breaker is opened at least once;
Based on the retained information, the circuit breaker is opened at a breaking phase such that the calculated residual magnetic flux of the first phase is maximized,
Measure the three-phase AC voltage on the power supply side than the breaker,
Of the measured three-phase AC voltage on the power supply side, the phase voltage having the same phase as the first phase becomes the zero point at which the calculated residual magnetic flux of the first phase changes from the same polarity to the opposite polarity. Determine the phase of 1 and
At the determined first phase, the circuit breaker of the phase that is in phase with the first phase is turned on,
After the determined first phase, the phase voltage of the phase that is in phase with the first phase becomes a zero point that transitions from the same polarity to the opposite polarity as the calculated residual magnetic flux of the first phase. Determine the second phase,
A method of suppressing a magnetizing inrush current, comprising: turning on the other two-phase circuit breakers that are not turned on at the determined second phase.
前記第2の位相の判断は、判断した前記第1の位相後、予め設定された時間後の零点を、前記第2の位相として判断すること
を特徴とする請求項6から請求項9のいずれか1項に記載の励磁突入電流抑制方法。
10. The determination of the second phase is performed by determining a zero point after a predetermined time after the determined first phase as the second phase. The method for suppressing an inrush current according to claim 1.
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Publication number Priority date Publication date Assignee Title
US9490627B2 (en) 2012-06-11 2016-11-08 Kabushiki Kaisha Toshiba Magnetizing inrush current suppressing device
US10074971B2 (en) 2012-07-19 2018-09-11 Kabushiki Kaisha Toshiba Excitation inrush current suppressing apparatus and excitation inrush current suppressing method
US10424912B2 (en) 2014-06-09 2019-09-24 Mitsubishi Electric Corporation Phase control device
US11437205B2 (en) * 2018-12-27 2022-09-06 Hitachi Energy Switzerland Ag Method and device for monitoring operation of a switching device for controlled switching applications

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US6704214B1 (en) * 2003-02-19 2004-03-09 Eaton Corporation Excitation control system and method employing de-excitation trip logic
JP2005204368A (en) * 2004-01-13 2005-07-28 Tm T & D Kk Phase control switching apparatus
WO2008065757A1 (en) * 2006-11-29 2008-06-05 Kabushiki Kaisha Toshiba Apparatus and method for compressing exciting inrush current of transformer
JP2010130849A (en) * 2008-11-28 2010-06-10 Toshiba Corp Excitation rush current restrainer of transformer and method

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JPS6346713A (en) * 1986-08-12 1988-02-27 Railway Technical Res Inst Transformer for two phase/three phase conversion
US6704214B1 (en) * 2003-02-19 2004-03-09 Eaton Corporation Excitation control system and method employing de-excitation trip logic
JP2005204368A (en) * 2004-01-13 2005-07-28 Tm T & D Kk Phase control switching apparatus
WO2008065757A1 (en) * 2006-11-29 2008-06-05 Kabushiki Kaisha Toshiba Apparatus and method for compressing exciting inrush current of transformer
JP2010130849A (en) * 2008-11-28 2010-06-10 Toshiba Corp Excitation rush current restrainer of transformer and method

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9490627B2 (en) 2012-06-11 2016-11-08 Kabushiki Kaisha Toshiba Magnetizing inrush current suppressing device
US10074971B2 (en) 2012-07-19 2018-09-11 Kabushiki Kaisha Toshiba Excitation inrush current suppressing apparatus and excitation inrush current suppressing method
US10424912B2 (en) 2014-06-09 2019-09-24 Mitsubishi Electric Corporation Phase control device
US11437205B2 (en) * 2018-12-27 2022-09-06 Hitachi Energy Switzerland Ag Method and device for monitoring operation of a switching device for controlled switching applications

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