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JP2017005859A - Isolated operation detection device for distributed power source - Google Patents

Isolated operation detection device for distributed power source Download PDF

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JP2017005859A
JP2017005859A JP2015117197A JP2015117197A JP2017005859A JP 2017005859 A JP2017005859 A JP 2017005859A JP 2015117197 A JP2015117197 A JP 2015117197A JP 2015117197 A JP2015117197 A JP 2015117197A JP 2017005859 A JP2017005859 A JP 2017005859A
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怜史 宇田
Satoshi Uda
怜史 宇田
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Nissin Electric Co Ltd
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Abstract

【課題】 単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とを両立させることができる単独運転検出装置を提供する。【解決手段】 この単独運転検出装置10aは、インバータ6を制御して、それから、配電系統2の基本波と同じ周波数の3相の基本波電流に、当該基本波の非整数倍次数mの次数間高調波電流Imを単相で重畳させて出力させる機能を有している制御装置30aと、連系線22上の測定点24における非整数倍次数mの次数間高調波電圧Vmを測定して、当該電圧Vmの変化から分散電源8が単独運転になったことを検出する単独運転監視装置32とを備えている。かつ制御装置30aは、測定点24を流れる次数間高調波電流Imの大きさの、所定時間前の値からの変化率を算出して、インバータ6から出力する次数間高調波電流Imを、前記算出した変化率に反比例させて増大させる次数間高調波電流補正回路72を有している。【選択図】 図3PROBLEM TO BE SOLVED: To provide an isolated operation detection device capable of achieving both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs. The isolated operation detection device 10a controls an inverter 6, and then converts the fundamental wave current of the same frequency as the fundamental wave of the power distribution system 2 to a non-integer multiple order m of the fundamental wave. A control device 30a having a function of superimposing and outputting the interharmonic current Im in a single phase, and measuring the interharmonic voltage Vm of the non-integer multiple order m at the measurement point 24 on the interconnection line 22. And an isolated operation monitoring device 32 for detecting that the distributed power supply 8 has been operated independently from the change in the voltage Vm. The control device 30a calculates the rate of change of the magnitude of the inter-order harmonic current Im flowing through the measurement point 24 from the value before a predetermined time, and calculates the inter-order harmonic current Im output from the inverter 6 as described above. An inter-order harmonic current correction circuit 72 that increases in inverse proportion to the calculated rate of change is provided. [Selection] Figure 3

Description

この発明は、直流電力を出力する電源と当該直流電力を交流電力に変換して出力するインバータとを有する分散電源を備えている分散電源保有設備が配電系統に接続された構成のシステム(これは分散電源連系システムと呼ぶこともできる。以下同様)に適用されて、前記分散電源が単独運転になったことを検出する単独運転検出装置に関する。   The present invention relates to a system in which a distributed power supply facility having a distributed power source having a power source that outputs DC power and an inverter that converts the DC power into AC power and outputs the power is connected to a distribution system (this is The present invention relates to an isolated operation detection device that can be referred to as a distributed power supply interconnection system (hereinafter the same applies) and detects that the distributed power supply is in an isolated operation.

配電系統には、例えば、太陽電池、蓄電池等の直流電力を出力する電源と当該直流電力を交流電力に変換して出力するインバータとを有する発電設備が接続されることが盛んになってきた。このような発電設備は、分散電源と呼ばれる。   For example, a power generation facility having a power source that outputs DC power, such as a solar battery or a storage battery, and an inverter that converts the DC power into AC power and outputs the power has become popular. Such a power generation facility is called a distributed power source.

分散電源を配電系統に接続して運転(これを連系運転と呼ぶ)している場合に、系統事故等によって電力会社の変電所の遮断器が開放されて上位系統からの電力供給が停止したとき、分散電源が運転(即ち単独運転)を続けていると、上位系統からの電力供給が停止したにもかかわらず配電線に電圧が印加され続けることになるので、感電事故等が発生する恐れがある。そこで、第1ステップとして、このような上位系統からの電力供給の停止、即ち分散電源の単独運転を確実に検出する必要がある。更に第2ステップとして、当該分散電源を配電系統から切り離す(解列する)必要がある。この出願は、この第1ステップの装置に関する。   When operating with a distributed power supply connected to the distribution system (this is called interconnection operation), the circuit breaker of the power company's substation was opened due to a system failure, etc., and the power supply from the upper system was stopped. If the distributed power supply continues to operate (ie, single operation), the voltage will continue to be applied to the distribution line even though the power supply from the higher-level system is stopped. There is. Therefore, as a first step, it is necessary to reliably detect such a stop of power supply from the host system, that is, a single operation of the distributed power source. Furthermore, as the second step, it is necessary to disconnect (disconnect) the distributed power source from the distribution system. This application relates to the apparatus of this first step.

分散電源の単独運転を検出する従来の単独運転検出装置を有する分散電源保有設備が配電系統に接続された構成のシステムの一例を図1に示す。   FIG. 1 shows an example of a system having a configuration in which a distributed power source possessing facility having a conventional isolated operation detection device for detecting isolated operation of a distributed power source is connected to a distribution system.

配電系統2に連系線22を介して分散電源保有設備36が接続されている。分散電源保有設備36は、直流電力を出力する電源4と当該直流電力を交流電力に変換して出力するインバータ6とを有する分散電源8を備えている。直流電力を出力する電源4は、例えば、太陽電池、蓄電池、その他の電池等である。交流電源とそれからの交流電力を直流電力に変換するコンバータとを有しているものでも良い。   A distributed power supply facility 36 is connected to the power distribution system 2 via the interconnection line 22. The distributed power supply facility 36 includes a distributed power supply 8 having a power supply 4 that outputs DC power and an inverter 6 that converts the DC power into AC power and outputs the AC power. The power source 4 that outputs DC power is, for example, a solar battery, a storage battery, or other batteries. It may have an AC power source and a converter that converts AC power from the AC power source into DC power.

インバータ6の出力部は、この例では、LCフィルタ14、絶縁変圧器16、電磁接触器18、遮断器20および連系線22を経由して配電系統2に接続されている。但しこのような構成に限られるものではない(後述する本発明の実施形態においても同様)。   In this example, the output unit of the inverter 6 is connected to the power distribution system 2 via the LC filter 14, the insulation transformer 16, the electromagnetic contactor 18, the circuit breaker 20, and the interconnection line 22. However, the present invention is not limited to such a configuration (the same applies to the embodiments of the present invention described later).

インバータ6に制御信号CSを供給してインバータ6を制御(例えばPWM制御)する制御装置30が設けられている。インバータ6の入力側の直流電圧Vdcは電圧検出器9を介して、出力側の交流電流Iacは計器用変流器12を介して、連系線22の測定点24における電圧Vs は計器用変圧器26を介して、制御装置30にそれぞれ取り込まれる。この交流電流Iacも、測定点24を流れる後述する電流Is と同様に、基本波電流I1 に次数間高調波電流Im が重畳されたものである。 A control device 30 is provided that controls the inverter 6 by supplying a control signal CS to the inverter 6 (for example, PWM control). The DC voltage V dc on the input side of the inverter 6 passes through the voltage detector 9, the AC current I ac on the output side passes through the current transformer 12, and the voltage V s at the measurement point 24 of the interconnection line 22 is These are taken into the control device 30 via the instrument transformer 26. The AC current I ac, similar to the current I s to be described later through the measurement point 24, in which interharmonic current I m to the fundamental wave current I 1 is superimposed.

制御装置30は、前記インバータ6を制御して、インバータ6から、配電系統2の基本波(例えば60Hzまたは50Hz)と同じ周波数の3相の基本波電流I1 に、当該基本波の1倍よりも大きい非整数倍次数m(例えば2.25次〜2.75次)の次数間高調波電流Im を単相で重畳させて出力させる機能を有している。即ち、連系線22に次数間高調波電流Im を単相注入する電流注入機能を有している。 The control device 30 controls the inverter 6 so that a three-phase fundamental current I 1 having the same frequency as the fundamental wave of the distribution system 2 (for example, 60 Hz or 50 Hz) is supplied from the inverter 6 by a factor of 1 of the fundamental wave. and an order between the harmonic current I m of the non-integer multiple order m is large (e.g., 2.25 order 2.75 order) have a function to output the superimposed single-phase. That has a current injection function of the single-phase injection of interharmonic current I m to tie line 22.

従って、連系線22の測定点24を流れる電流Is は、基本波電流I1 に次数間高調波電流Im を重畳させたものである。また、このような電流が流れることによって発生する電圧、即ち測定点24における電圧Vs は、基本波電圧V1 に次数間高調波電圧Vm を重畳させたものである。 Accordingly, the current I s flowing through the measurement point 24 of the tie-line 22 is overlapped with the fundamental wave current I interharmonic current I m to 1. Further, the voltage generated by the flow of such a current, that is, the voltage V s at the measurement point 24 is obtained by superimposing the inter-order harmonic voltage V m on the fundamental wave voltage V 1 .

分散電源8が単独運転になったことを検出する単独運転検出装置10は、この例では、上記のような機能を有する制御装置30および単独運転監視装置32を備えている。   In this example, the isolated operation detection device 10 that detects that the distributed power source 8 has been operated independently includes the control device 30 and the isolated operation monitoring device 32 having the functions described above.

なお、図1中のインバータ6付近から遮断器20付近までの破線で囲んだ要素を含む装置34は、通常、パワーコンディショナ(略称PCS)と呼ばれている。後述する本発明の実施形態においても同様である。   In addition, the apparatus 34 including the element enclosed with the broken line from the inverter 6 vicinity in FIG. 1 to the circuit breaker 20 vicinity is normally called the power conditioner (abbreviation PCS). The same applies to embodiments of the present invention described later.

制御装置30の構成の一例を図2に示す。この例では、簡単に言えば、3相/2相変換器38の出力部から2相/3相変換器60の入力部までの間を2相で扱っている。   An example of the configuration of the control device 30 is shown in FIG. In this example, simply speaking, the range from the output part of the 3-phase / 2-phase converter 38 to the input part of the 2-phase / 3-phase converter 60 is handled in two phases.

この制御装置30は、基本波電流I1 の指令値I1 ′を上記測定点における電圧Vs の波形を用いて作り出す。即ち、3相の上記電圧Vs を3相/2相変換器38によって2相の電圧に変換し、その基本波電圧V1 から電圧位相演算器40によって位相情報を算出し、それを基本波電流指令値発生器44に与える。また、直流電圧一定制御器42において上記直流電圧Vdcが一定になる情報を算出し、それを基本波電流指令値発生器44に与える。基本波電流指令値発生器44は、上記情報に基づいて、インバータ6から出力する基本波電流I1 の指令値I1 ′を発生させる。 This control device 30 generates a command value I 1 ′ of the fundamental current I 1 using the waveform of the voltage V s at the measurement point. That is, the three-phase voltage V s is converted into a two-phase voltage by the three-phase / two-phase converter 38, phase information is calculated from the fundamental wave voltage V 1 by the voltage phase calculator 40, and the fundamental wave is converted to the fundamental wave. The current command value generator 44 is given. Further, the DC voltage constant controller 42 calculates information that makes the DC voltage V dc constant, and supplies it to the fundamental wave current command value generator 44. The fundamental wave command value generator 44 generates a command value I 1 ′ of the fundamental current I 1 output from the inverter 6 based on the above information.

一方、次数間高調波電流指令値発生器46によって、インバータ6から出力する上記次数間高調波電流Im の指令値Im ′を発生させ、上記両指令値I1 ′、Im ′を加算器48で加算する。 On the other hand, the inter-order harmonic current command value generator 46 generates the command value I m ′ of the inter-order harmonic current I m output from the inverter 6 and adds the both command values I 1 ′ and I m ′. Adder 48

加算器48からの信号は、増幅器52によってフィードフォワード係数jωLを掛けて電圧信号に変換する一方、減算器50によって上記直流電流Iacを減算した後に増幅器54によってフィードバック係数Kp を掛けて電圧信号に変換し、両電圧信号を加算器56によって加算すると共に加算器58によって、上記3相/2相変換器38からの2相に変換した電圧を加算した後、2相/3相変換器60によって3相に変換して上記制御信号CSが形成され、それがインバータ6に与えられる。 The signal from the adder 48 is converted into a voltage signal by multiplying the feed forward coefficient jωL by the amplifier 52, while being subtracted from the DC current I ac by the subtractor 50 and then multiplied by the feedback coefficient K p by the amplifier 54. The two voltage signals are added by the adder 56 and the voltage converted into the two phases from the three-phase / two-phase converter 38 is added by the adder 58, and then the two-phase / three-phase converter 60 is added. Is converted into three phases to form the control signal CS, which is supplied to the inverter 6.

制御装置30は、上記のような構成によって、インバータ6を、それから出力する基本波電流I1 が指令値I1 ′どおりになるように制御する。即ち、配電系統2側のインピーダンスが変化しても、一定の基本波電流I1 が出力されるように制御する。 With the configuration as described above, the control device 30 controls the inverter 6 so that the fundamental current I 1 output therefrom is in accordance with the command value I 1 ′. That is, even if the impedance on the power distribution system 2 side changes, control is performed so that a constant fundamental wave current I 1 is output.

単独運転監視装置32は、上記測定点24における電圧Vs に含まれている上記非整数倍次数mの次数間高調波電圧Vm を測定して、当該次数間高調波電圧Vm の変化から、分散電源8が単独運転になったことを検出してそれを表す単独運転検出信号S1 を出力する。例えば、次数間高調波電圧Vm またはその変化率を所定の判定値と比較して、次数間高調波電圧Vm またはその変化率が当該判定値を超えると単独運転検出信号S1 を出力する。その後は、例えば、当該単独運転検出信号S1 に基づいて、インバータ6をゲートブロックして出力を止め、かつ電磁接触器18を開放する等して、分散電源8を配電系統2から切り離せば良い。 The isolated operation monitoring device 32 measures the inter-order harmonic voltage V m of the non-integer multiple order m included in the voltage V s at the measurement point 24, and determines the change in the inter-order harmonic voltage V m . Then, it detects that the distributed power source 8 has become an isolated operation, and outputs an isolated operation detection signal S 1 representing it. For example, the inter-order harmonic voltage V m or the rate of change thereof is compared with a predetermined determination value, and when the inter-order harmonic voltage V m or the rate of change exceeds the determination value, the isolated operation detection signal S 1 is output. . Thereafter, for example, based on the isolated operation detection signal S 1 , the distributed power supply 8 may be disconnected from the distribution system 2 by gate-blocking the inverter 6 to stop the output and opening the electromagnetic contactor 18. .

なお、上記のように連系線に次数間高調波電流を注入して、連系線上の測定点における次数間高調波電圧の変化から、分散電源の単独運転を検出する方式の単独運転検出装置の一例が、特許文献1に記載されている。   In addition, as described above, an independent operation detection device that detects the independent operation of the distributed power source from the change in the harmonic voltage between the orders at the measurement points on the interconnection line by injecting the interharmonic current into the interconnection line. An example is described in Patent Document 1.

特開2000−287362号公報JP 2000-287362 A

上述した従来の単独運転検出装置10の場合、配電系統2内の遮断器(図示省略。図11中の遮断器154参照)が開放されて単独運転が発生すると、測定点24から見た配電系統2側のインピーダンスが増大するので、測定点24における電圧Vs に含まれている次数間高調波電圧Vm も増大するけれども、同時に連系線22に流れる電流Is に含まれている次数間高調波電流Im が減少するので、次数間高調波電圧Vm は上記インピーダンスの増大ほどには大きくならず、単独運転発生時の次数間高調波電圧Vm の変化が小さいという課題がある。 In the case of the conventional isolated operation detection device 10 described above, when the circuit breaker (not shown; see the circuit breaker 154 in FIG. 11) in the distribution system 2 is opened and the isolated operation occurs, the distribution system viewed from the measurement point 24. Since the impedance on the second side increases, the inter-order harmonic voltage V m included in the voltage V s at the measurement point 24 also increases, but at the same time, between the orders included in the current I s flowing through the interconnection line 22. Since the harmonic current I m decreases, the inter-order harmonic voltage V m does not increase as much as the increase in the impedance, and there is a problem that the change in the inter-order harmonic voltage V m at the time of isolated operation is small.

これを詳述すると、上述したように制御装置30は通常、配電系統2側のインピーダンスが変化してもインバータ6から出力する基本波電流I1 が一定の値を保つように動作する(これは定電流制御と呼ばれる)。そのための制御要素として、増幅器54で設定するフィードバック係数Kp が大きく寄与しており、その値は通常、分散電源8の本来の出力である基本波電流I1 に主眼をおいて設定される。 More specifically, as described above, the control device 30 normally operates so that the fundamental wave current I 1 output from the inverter 6 maintains a constant value even if the impedance on the distribution system 2 side changes (this is Called constant current control). As a control element for that purpose, the feedback coefficient K p set by the amplifier 54 greatly contributes, and its value is usually set with a focus on the fundamental current I 1 which is the original output of the distributed power supply 8.

一方、次数間高調波電流Im は基本波の非整数倍次数m(例えば2.25次〜2.75次)であるため、次数間高調波電流の指令値Im ′も基本波電流の指令値I1 ′よりも高調波の波形となる。仮に次数間高調波電流Im の制御に対応させるために、フィードバック係数Kp を大きくしてフィードバックの制御量を大きくしようとすると、分散電源8の本来の出力である基本波電流I1 にとってはフィードバック量が大きくなり過ぎて基本波電流I1 が不安定になるため、そのようにフィードバック係数Kp を大きくすることはできない。 Meanwhile, since the harmonic current I m between orders is a non-integer multiple order m of the fundamental wave (for example, 2.25 order 2.75 order), the command value I m interharmonic current 'also of fundamental wave current The waveform is higher than the command value I 1 ′. To tentatively correspond to the control interharmonic current I m, when trying to enlarge the control amount of feedback by increasing the feedback coefficient K p, for the fundamental current I 1 which is the original output of the distributed power supply 8 Since the fundamental wave current I 1 becomes unstable because the feedback amount becomes too large, the feedback coefficient K p cannot be increased as such.

そのために通常は、上記のように基本波電流I1 に主眼をおいてフィードバック係数Kp を設定しており、次数間高調波電流Im にとってはフィードバック係数Kp が小さくフィードバック量が少ないので、単独運転が発生して測定点24から見た配電系統2側のインピーダンスが増大すると、次数間高調波電流Im は一定を保つことができず減少する。次数間高調波電流Im が減少すると、当該次数間高調波電流Im によって発生する次数間高調波電圧Vm も減少するので、上記のように、次数間高調波電圧Vm は上記インピーダンスの増大ほどには大きくならず、単独運転発生時の次数間高調波電圧Vm の変化は小さい(後述する図14、図18およびその説明も参照)。 Usually Therefore, and set the feedback coefficient K p focuses on the fundamental wave current I 1, as described above, since the feedback coefficient K p is the feedback amount is small small for interharmonic current I m, If the impedance of the power distribution system 2 side alone operation viewed from the measurement point 24 occurs is increased, the harmonic current I m between orders is reduced can not be kept constant. When the harmonic current I m is reduced between orders, since interharmonic voltage V m generated by the interharmonic current I m also decreases, as described above, the harmonic voltage V m between orders of the impedance It does not increase as much as the increase, and the change in the inter-order harmonic voltage V m when the isolated operation occurs is small (see also FIGS. 14 and 18 described later and the description thereof).

単独運転発生時の次数間高調波電圧Vm の変化が小さいと、単独運転監視装置32における単独運転の検出が難しくなる。即ち、単独運転監視装置32における判定値を小さくして検出感度を上げると、系統電圧の瞬時低下や系統周波数の変動のような系統擾乱発生時に誤検出(即ち、単独運転でないのに単独運転と判定する不要検出)の可能性が高くなる。逆に単独運転監視装置32における判定値を大きくして検出感度を下げると、今度は単独運転の確実な検出が困難になる。従って、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とを両立させることが難しい。 If the change in the inter-order harmonic voltage V m when the isolated operation occurs is small, it is difficult to detect the isolated operation in the isolated operation monitoring device 32. That is, if the detection value in the isolated operation monitoring device 32 is reduced to increase the detection sensitivity, erroneous detection occurs when a system disturbance such as an instantaneous decrease in the system voltage or fluctuation in the system frequency occurs (that is, it is not an isolated operation but an isolated operation. The possibility of unnecessary detection) is increased. Conversely, if the detection value is lowered by increasing the determination value in the isolated operation monitoring device 32, it will be difficult to reliably detect the isolated operation. Therefore, it is difficult to achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs.

そこでこの発明は、上記のような点を改善して、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とを両立させることができる単独運転検出装置を提供することを主たる目的としている。   Accordingly, the main object of the present invention is to provide an isolated operation detection device that can improve the above-described points and achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs. It is said.

この発明に係る単独運転検出装置は、直流電力を出力する電源と当該直流電力を交流電力に変換して出力するインバータとを有する分散電源を備えている分散電源保有設備が配電系統に接続された構成のシステムに適用されて、前記分散電源が単独運転になったことを検出する単独運転検出装置であって、前記インバータを制御して、前記インバータから、前記配電系統の基本波と同じ周波数の3相の基本波電流に、当該基本波の1倍よりも大きい非整数倍次数の次数間高調波電流を単相で重畳させて出力させる機能を有している制御装置と、前記分散電源保有設備と前記配電系統との連系線上の測定点における前記非整数倍次数の次数間高調波電圧を測定して、当該次数間高調波電圧の変化から、前記分散電源が単独運転になったことを検出する単独運転監視装置とを備えており、かつ前記制御装置は、前記連系線上の測定点を流れる前記次数間高調波電流の大きさの、所定時間前の値からの変化率を算出して、前記インバータから出力する前記次数間高調波電流を、前記算出した変化率に反比例させて増大させる次数間高調波電流補正回路を有している、ことを特徴としている。   In the isolated operation detection device according to the present invention, a distributed power supply facility having a distributed power source having a power source that outputs DC power and an inverter that converts the DC power into AC power and outputs the power is connected to the distribution system. An isolated operation detection device that is applied to a system having a configuration and detects that the distributed power supply is in an isolated operation, and controls the inverter so that the inverter has the same frequency as the fundamental wave of the distribution system. A control device having a function of superimposing a non-integer multiple order harmonic current greater than 1 times the fundamental wave in a single phase on a three-phase fundamental current and outputting the same; Measure the harmonic voltage between the orders of the non-integer multiple order at the measurement point on the interconnection line between the facility and the power distribution system, and the distributed power source has become an independent operation from the change in the harmonic voltage between the orders Inspect And the control device calculates a rate of change of the magnitude of the interharmonic current flowing through the measurement point on the interconnection line from a value before a predetermined time. And an inter-order harmonic current correction circuit for increasing the inter-order harmonic current output from the inverter in inverse proportion to the calculated rate of change.

この単独運転検出装置によれば、単独運転が発生すると、測定点から見た配電系統側のインピーダンスが増大して、測定点を流れる次数間高調波電流が減少するけれども、制御装置内の次数間高調波電流補正回路は、上記次数間高調波電流の変化率を算出して、インバータから出力する次数間高調波電流を、上記算出した変化率に反比例させて増大させるので、測定点を流れる次数間高調波電流の減少が小さく抑えられる。その結果、単独運転発生時の測定点における次数間高調波電圧の変化が大きくなるので、単独運転監視装置における判定値の選定が容易になる。その結果、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とを両立させることができる。   According to this isolated operation detection device, when isolated operation occurs, the impedance on the distribution system side as viewed from the measurement point increases, and the interharmonic current flowing through the measurement point decreases. The harmonic current correction circuit calculates the rate of change of the harmonic current between the orders, and increases the harmonic current between orders output from the inverter in inverse proportion to the calculated rate of change. Reduction of inter-harmonic current is kept small. As a result, the change in the harmonic voltage between the orders at the measurement point when the isolated operation occurs increases, so that the determination value can be easily selected in the isolated operation monitoring device. As a result, it is possible to achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs.

前記次数間高調波電流補正回路は、前記連系線上の測定点を流れる電流から、前記配電系統の基本波およびその整数倍の高調波を除去した電流を出力するコムフィルタと、前記コムフィルタから出力される前記電流の瞬時値を用いて、当該電流の瞬時逆相電流の振幅を演算して出力する瞬時逆相演算器と、前記瞬時逆相演算器からの前記瞬時逆相電流の振幅の、所定時間前からの変化率を演算して出力する変化率演算器と、前記変化率演算器からの前記変化率の逆数である補正ゲインを演算して出力する補正ゲイン演算器と、前記インバータに前記次数間高調波電流を出力させるために与える次数間高調波電流の指令値を、前記補正ゲイン演算器からの前記補正ゲインで増大させる指令値補正器とを有していても良い。   The inter-order harmonic current correction circuit outputs a current obtained by removing a fundamental wave of the distribution system and an integral multiple of the harmonic from the current flowing through the measurement point on the interconnection line, and the comb filter Using the instantaneous value of the current that is output, the instantaneous negative phase calculator that calculates and outputs the amplitude of the instantaneous negative phase current of the current, and the amplitude of the instantaneous negative phase current from the instantaneous negative phase calculator A change rate calculator that calculates and outputs a change rate from a predetermined time before, a correction gain calculator that calculates and outputs a correction gain that is the reciprocal of the change rate from the change rate calculator, and the inverter And a command value corrector that increases a command value of the interharmonic current to be given to output the interharmonic current with the correction gain from the correction gain calculator.

前記次数間高調波電流補正回路は、前記補正ゲイン演算器からの前記補正ゲインの変化率を、定常時の値を1に保ちつつ拡大して出力する補正ゲイン拡大器を更に有しており、前記指令値補正器は、前記インバータに与える前記次数間高調波電流の指令値を、前記補正ゲイン拡大器からの拡大させた補正ゲインで増大させるものである、という構成を採用しても良い。   The inter-order harmonic current correction circuit further includes a correction gain expander that expands and outputs the rate of change of the correction gain from the correction gain calculator while maintaining a steady-state value of 1, The command value corrector may employ a configuration in which the command value of the inter-order harmonic current given to the inverter is increased by an enlarged correction gain from the correction gain expander.

請求項1に記載の発明によれば、単独運転が発生すると、測定点から見た配電系統側のインピーダンスが増大して、測定点を流れる次数間高調波電流が減少するけれども、制御装置内の次数間高調波電流補正回路は、上記次数間高調波電流の変化を算出して、インバータから出力する次数間高調波電流を、上記算出した変化率に反比例させて増大させるので、測定点を流れる次数間高調波電流の減少が小さく抑えられる。その結果、単独運転発生時の測定点における次数間高調波電圧の変化が大きくなるので、単独運転監視装置における判定値の選定が容易になる。その結果、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とを両立させることができる。   According to the first aspect of the present invention, when an independent operation occurs, the impedance on the distribution system side as viewed from the measurement point increases and the interharmonic current flowing through the measurement point decreases. The interharmonic current correction circuit calculates a change in the interharmonic current and increases the interharmonic current output from the inverter in inverse proportion to the calculated rate of change, so that it flows through the measurement point. The decrease in interharmonic current is kept small. As a result, the change in the harmonic voltage between the orders at the measurement point when the isolated operation occurs increases, so that the determination value can be easily selected in the isolated operation monitoring device. As a result, it is possible to achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs.

請求項2に記載の発明によれば次の更なる効果を奏する。即ち、次数間高調波電流補正回路は、瞬時逆相演算器およびその前処理としてのコムフィルタ等を有していて、次数間高調波電流の変化率を、瞬時逆相電流の振幅の変化率として検出することによって、離散フーリエ変換器等を用いる場合に比べて高速で検出することができるので、単独運転発生時にインバータから出力される次数間高調波電流の減少をより速やかに抑制することができる。その結果、単独運転発生時の測定点における次数間高調波電圧の変化がより大きくなるので、単独運転監視装置における判定値の選定がより容易になる。その結果、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とをより確実に両立させることができる。   According to invention of Claim 2, there exists the following further effect. That is, the inter-order harmonic current correction circuit includes an instantaneous anti-phase calculator and a comb filter as a pre-processing thereof, and the rate of change of the inter-order harmonic current is expressed as the rate of change of the amplitude of the instantaneous anti-phase current. Since it can be detected at a higher speed than when using a discrete Fourier transformer or the like, it is possible to more quickly suppress a decrease in interharmonic current output from the inverter when an isolated operation occurs. it can. As a result, the change in the inter-order harmonic voltage at the measurement point when the isolated operation occurs becomes larger, so that it becomes easier to select the determination value in the isolated operation monitoring device. As a result, it is possible to more reliably achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs.

請求項3に記載の発明によれば次の更なる効果を奏する。即ち、拡大させた補正ゲインを用いることによって、単独運転発生時にインバータから出力される次数間高調波電流の減少をより確実に抑制することができる。その結果、単独運転発生時の測定点における次数間高調波電圧の変化がより一層大きくなるので、単独運転監視装置における判定値の選定がより一層容易になる。その結果、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とをより確実に両立させることができる。   According to invention of Claim 3, there exists the following further effect. That is, by using the enlarged correction gain, it is possible to more reliably suppress the decrease in the inter-order harmonic current output from the inverter when the single operation occurs. As a result, the change in the harmonic voltage between the orders at the measurement point when the isolated operation occurs is further increased, so that the selection of the judgment value in the isolated operation monitoring device is further facilitated. As a result, it is possible to more reliably achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs.

従来の単独運転検出装置を有する分散電源保有設備が配電系統に接続された構成のシステムの一例を示す単線接続図である。It is a single line connection figure which shows an example of the system of the structure by which the distributed power supply equipment which has the conventional isolated operation detection apparatus was connected to the power distribution system. 図1中の制御装置の構成の一例を示すブロック図である。It is a block diagram which shows an example of a structure of the control apparatus in FIG. 本発明の実施形態に係る単独運転検出装置を有する分散電源保有設備が配電系統に接続された構成のシステムの一例を示す単線接続図である。1 is a single line connection diagram illustrating an example of a system having a configuration in which a distributed power supply facility having an isolated operation detection device according to an embodiment of the present invention is connected to a power distribution system. 図3中の単独運転監視装置の構成の一例を示すブロック図である。It is a block diagram which shows an example of a structure of the independent operation monitoring apparatus in FIG. 図3中の制御装置の構成の一例を示すブロック図である。It is a block diagram which shows an example of a structure of the control apparatus in FIG. 図5中の補正ゲイン演算回路の構成の一例を示すブロック図である。FIG. 6 is a block diagram illustrating an example of a configuration of a correction gain calculation circuit in FIG. 5. 図5中の次数間高調波電流指令値発生器の構成の一例を示すブロック図である。It is a block diagram which shows an example of a structure of the harmonic current command value generator between orders in FIG. 図6中のコムフィルタの構成の一例を示すブロック図およびその特性の一例を示す図である。FIG. 7 is a block diagram showing an example of the configuration of a comb filter in FIG. 6 and an example of its characteristics. 図6中の瞬時逆相演算器の構成の一例を示すブロック図である。It is a block diagram which shows an example of a structure of the instantaneous reverse phase calculator in FIG. 単独運転発生時の図6中の瞬時逆相電流の振幅の変化率およびその逆数である補正ゲインの変化の一例を示す概略図である。It is the schematic which shows an example of the change of the correction gain which is the rate of change of the amplitude of the instantaneous reverse phase current in FIG. 単独運転発生時のシミュレーションに用いた系統モデルを示す単線接続図である。It is a single line connection figure which shows the system | strain model used for the simulation at the time of islanding generation | occurrence | production. 単独運転発生時の図6中の瞬時逆相電流の振幅の変化率dIn およびその逆数である補正ゲインG1 をシミュレーションした結果の一例を示す図である。Is a diagram showing an example of independent operation simulating the correction gain G 1 is the change rate dI n and its inverse of the amplitude of the instantaneous anti-phase current in Figure 6 in the event the result. 図6中の瞬時逆相電流に代えて、単独運転発生時の瞬時正相電流の振幅の変化率dIp およびその逆数である補正ゲインG1 をシミュレーションした結果の一例を示す図である。Instead of the instantaneous anti-phase current in FIG. 6 is a diagram showing an example of a simulation result of the correction gain G 1 is the change rate dI p and its inverse of the amplitude of the instantaneous positive-phase current during isolated operation occurs. 従来の単独運転検出装置を有する場合に、単独運転発生時をシミュレーションしたときの測定点における次数間高調波電流および次数間高調波電圧の変化の一例を示す図である。It is a figure which shows an example of the change of the harmonic current between orders and the harmonic voltage between orders in a measurement point when it has a conventional islanding operation detection apparatus, and the time of an islanding operation is simulated. 本発明の第1の実施形態の単独運転検出装置を有する場合に、単独運転発生時をシミュレーションしたときの測定点における次数間高調波電流および次数間高調波電圧の変化の一例を示す図である。It is a figure which shows an example of the change of the harmonic current between orders and the harmonic voltage between orders in a measurement point when it has the islanding operation detection apparatus of the 1st Embodiment of this invention, and the time of an islanding operation is simulated. . 図5中の補正ゲイン演算回路の構成の他の例を示すブロック図である。FIG. 6 is a block diagram showing another example of the configuration of the correction gain calculation circuit in FIG. 5. 図16中の拡大させた補正ゲインG4 を説明するための概略図である。FIG. 17 is a schematic diagram for explaining an enlarged correction gain G 4 in FIG. 16. 従来の単独運転検出装置を有する場合に、インピーダンス変化の生じにくい条件において単独運転発生時をシミュレーションしたときの測定点における次数間高調波電流および次数間高調波電圧の変化の一例を示す図である。It is a figure which shows an example of the change of the harmonic current between orders and the harmonic voltage between orders in a measurement point when simulating the time of an isolated operation generation | occurrence | production on the conditions which are hard to produce an impedance change when it has the conventional isolated operation detection apparatus. . 本発明の第1の実施形態の単独運転検出装置を有する場合に、インピーダンス変化の生じにくい条件において単独運転発生時をシミュレーションしたときの測定点における次数間高調波電流および次数間高調波電圧の変化の一例を示す図である。Changes in inter-order harmonic current and inter-order harmonic voltage at measurement points when a single operation occurrence is simulated under conditions where impedance change does not easily occur when the isolated operation detection device according to the first embodiment of the present invention is provided. It is a figure which shows an example. 本発明の第2の実施形態の単独運転検出装置を有する場合に、インピーダンス変化の生じにくい条件において単独運転発生時をシミュレーションしたときの測定点における次数間高調波電流および次数間高調波電圧の変化の一例を示す図である。Changes in inter-order harmonic current and inter-harmonic voltage at measurement points when simulating the occurrence of isolated operation under conditions where impedance change is unlikely to occur when the isolated operation detection device of the second embodiment of the present invention is provided It is a figure which shows an example.

(1)単独運転検出装置の第1の実施形態
図3に、本発明の実施形態に係る単独運転検出装置を有する分散電源保有設備が配電系統に接続された構成のシステムの一例を示す。図1、図2に示した従来例と同一または相当する部分には同一符号を付し、以下においては当該従来例との相違点を主に説明する。
(1) First Embodiment of Isolated Operation Detection Device FIG. 3 shows an example of a system having a configuration in which a distributed power supply facility having an isolated operation detection device according to an embodiment of the present invention is connected to a distribution system. Parts identical or corresponding to those in the conventional example shown in FIGS. 1 and 2 are denoted by the same reference numerals, and differences from the conventional example will be mainly described below.

この実施形態の単独運転検出装置10aは、前述した従来の制御装置30に対応する制御装置30aと、前述した単独運転監視装置32とを有している。この制御装置30aには、計器用変流器28を介して、連系線22上の測定点24を流れる電流Is が取り込まれる。この電流Is は、前述したように、基本波電流I1 に次数間高調波電流Im が重畳されたものである。 The isolated operation detection device 10a of this embodiment includes a control device 30a corresponding to the above-described conventional control device 30 and the isolated operation monitoring device 32 described above. The control unit 30a, via a current transformer 28, the current I s flowing through the measurement points 24 on the tie-line 22 is fetched. The current I s are those as described above, the fundamental wave current I interharmonic current I m to 1 superimposed.

制御装置30aは、連系線22上の測定点24を流れる次数間高調波電流Im の大きさの、所定時間前の値からの変化率を算出して、インバータ6から出力する次数間高調波電流Im を、前記算出した変化率に反比例させて増大させる次数間高調波電流補正回路72を有している。これを以下に詳述する。 Control device 30a, the size of interharmonic current I m flowing through the measurement points 24 on the tie-line 22, to calculate the rate of change from the value before the predetermined time, harmonic between orders to be output from the inverter 6 wave current I m, and has a interharmonic current correction circuit 72 to increase in inverse proportion to the calculated rate of change. This will be described in detail below.

それに先立って、単独運転監視装置32の構成の一例を図4を参照して説明する。この単独運転監視装置32は、上記測定点24における電圧Vs に含まれている上記次数間高調波電圧Vm の変化率dVm を判定する場合の例であり、離散フーリエ変換器62、絶対値演算器64、移動平均演算器66、変化率演算器68および比較器70を備えている。 Prior to that, an example of the configuration of the isolated operation monitoring device 32 will be described with reference to FIG. This isolated operation monitoring device 32 is an example in which the rate of change dV m of the inter-order harmonic voltage V m included in the voltage V s at the measurement point 24 is determined. A value calculator 64, a moving average calculator 66, a change rate calculator 68, and a comparator 70 are provided.

離散フーリエ変換器62は、上記電圧Vs から、離散フーリエ変換によって、上記次数間高調波電圧Vm を抽出して出力する。 The discrete Fourier transformer 62 extracts the inter-order harmonic voltage V m from the voltage V s by discrete Fourier transform and outputs it.

絶対値演算器64は、離散フーリエ変換器62から与えられる次数間高調波電圧Vm の絶対値|Vm |を演算して出力する。 The absolute value calculator 64 calculates and outputs the absolute value | V m | of the inter-order harmonic voltage V m given from the discrete Fourier transformer 62.

移動平均演算器66は、絶対値演算器64から与えられる絶対値|Vm |について、現在より所定時間過去における所定時間の移動平均値Vmav を演算して出力する。例えば現在より1秒過去における1秒間の移動平均値Vmav を算出する。 The moving average calculator 66 calculates and outputs a moving average value V mav for a predetermined time in the past for the absolute value | V m | given from the absolute value calculator 64. For example, the moving average value V mav for one second in the past from the present is calculated.

変化率演算器68は、上記絶対値|Vm |の変化率dVm を、次式に従って演算して出力する。即ち、変化率dVm は、この例では、Vmav に対する|Vm |の比率である。 The change rate calculator 68 calculates and outputs the change rate dV m of the absolute value | V m | according to the following equation. That is, the change rate dV m is a ratio of | V m | to V mav in this example.

[数1]
dVm =|Vm |/Vmav
[Equation 1]
dV m = | V m | / V mav

比較器70は、変化率演算器68から与えられる変化率dVm を所定の判定値J1 と比較して、前者dVm が後者J1 を超えたときに、前記分散電源8が単独運転になったことを表す単独運転検出信号S1 を出力する。 The comparator 70 compares the rate of change dV m given from the rate of change calculator 68 with a predetermined judgment value J 1, and when the former dV m exceeds the latter J 1 , the distributed power source 8 is put into a single operation. An isolated operation detection signal S 1 indicating that the failure has occurred is output.

但し、単独運転監視装置32は、次数間高調波電圧Vm の変化率dVm を判定する代わりに、例えば前記特許文献1にも記載されているように、次数間高調波電圧Vm の大きさが所定の判定値を超えたときに、単独運転検出信号S1 を出力するという構成を採用しても良い。 However, instead of determining the rate of change dV m of the inter-order harmonic voltage V m , the isolated operation monitoring device 32 has a large inter-order harmonic voltage V m as described in, for example, Patent Document 1 described above. Saga when exceeds a predetermined judgment value, may be adopted that outputs the isolated operation detecting signal S 1.

また、上記単独運転検出信号S1 をそのまま単独運転監視装置32から出力しても良いけれども、当該信号S1 が所定時間(例えば20m秒程度)継続していることを判定した後に出力するようにしても良い。そのようにすると、単独運転発生以外の何らかの原因による電圧Vs 等の瞬時の変動による誤検出を防止することが容易になる。 The isolated operation detection signal S 1 may be output from the isolated operation monitoring device 32 as it is. However, the isolated operation detection signal S 1 is output after determining that the signal S 1 continues for a predetermined time (for example, about 20 milliseconds). May be. By doing so, it becomes easy to prevent erroneous detection due to instantaneous fluctuations of the voltage V s or the like due to some cause other than the occurrence of isolated operation.

制御装置30aは、この実施形態では図5に示すように、図2に示したものに比べて、3相/2相変換器74および補正ゲイン演算回路76を更に有しており、かつ次数間高調波電流指令値発生器46a内に指令値補正器124〜126(図7参照)を設けており、これらがこの実施形態では、上述した次数間高調波電流補正回路72を構成している。これらを以下に詳述する。   In this embodiment, as shown in FIG. 5, the control device 30a further includes a three-phase / two-phase converter 74 and a correction gain calculation circuit 76 as compared with the one shown in FIG. Command value correctors 124 to 126 (see FIG. 7) are provided in the harmonic current command value generator 46a, and in this embodiment, these constitute the inter-order harmonic current correction circuit 72 described above. These are described in detail below.

3相/2相変換器74は、上記連系線22の測定点24を流れる3相の電流Is (即ち、Isu、Isv、Isw)を、次式に従って直交変換して、2相のα成分電流Isαおよびβ成分電流Isβに変換する。前述したように、次数間高調波電流の指令値Im ′等は2相で扱っているので、それに対応させるためである。 The three-phase / two-phase converter 74 orthogonally converts the three-phase current I s (that is, I su , I sv , I sw ) flowing through the measurement point 24 of the interconnection line 22 according to the following formula, The phase α component current I s α and β component current I s β are converted. As described above, the command value I m ′ and the like of the inter-order harmonic current is handled in two phases, so that it corresponds to it.

[数2]
sα=√(2/3){Isu−(1/2)Isv−(1/2)Isw
sβ=√(2/3){(√3/2)Isv−(√3/2)Isw
[Equation 2]
I s α = √ (2/3) {I su − (1/2) I sv − (1/2) I sw }
I s β = √ (2/3) {(√3 / 2) I sv − (√3 / 2) I sw }

ちなみに、前述した2相/3相変換器60は、次式に従って2相から3相への変換を行って、3相の制御信号CS(即ちCSu 、CSv 、CSw )を出力する。Vαは加算器58から2相/3相変換器60に与えられるα成分電圧、Vβはβ成分電圧である。 Incidentally, the two-phase / three-phase converter 60 described above performs conversion from two phases to three phases according to the following equation, and outputs three-phase control signals CS (ie, CS u , CS v , CS w ). Vα is an α component voltage supplied from the adder 58 to the 2-phase / 3-phase converter 60, and Vβ is a β component voltage.

[数3]
CSu =√(2/3)・Vα
CSv =√(2/3){−(1/2)・Vα+(√3/2)・Vβ}
CSw =√(2/3){−(1/2)・Vα−(√3/2)・Vβ}
[Equation 3]
CS u = √ (2/3) · Vα
CS v = √ (2/3) {− (1/2) · Vα + (√3 / 2) · Vβ}
CS w = √ (2/3) {− (1/2) · Vα− (√3 / 2) · Vβ}

補正ゲイン演算回路76の構成の一例を図6に示す。この補正ゲイン演算回路76は、コムフィルタ78、80、瞬時逆相演算器82、ローパスフィルタ84、変化率演算器86および補正ゲイン演算器94を備えている。   An example of the configuration of the correction gain calculation circuit 76 is shown in FIG. The correction gain calculation circuit 76 includes comb filters 78 and 80, an instantaneous reverse phase calculation unit 82, a low-pass filter 84, a change rate calculation unit 86, and a correction gain calculation unit 94.

コムフィルタ78、80は、それぞれ、上記直交変換して得られたα成分電流Isα、β成分電流Isβから、配電系統2の基本波およびその整数倍の高調波を除去した電流を出力する。 The comb filters 78 and 80 respectively obtain the currents obtained by removing the fundamental wave of the distribution system 2 and the harmonics of the integral multiple thereof from the α component current I s α and β component current I s β obtained by the orthogonal transformation. Output.

コムフィルタ78、80の構成および特性の一例を図8に示す。コムフィルタ78、80は、それぞれ、遅延器130で1サイクル前の基本波を算出し、それを減算器132によって現在値から減算し、増幅器134でゲインを1/2にして出力する。これによって、図8(B)に示すように、配電系統2の基本波およびその整数倍の高調波を除去することができる。測定点を流れる電流Is に含まれている次数間高調波電流Im は、その次数が前述したように配電系統2の基本波の1倍よりも大きい非整数倍次数mであるので、コムフィルタ78、80で除去されずに通過する。 An example of the configuration and characteristics of the comb filters 78 and 80 is shown in FIG. Each of the comb filters 78 and 80 calculates a fundamental wave one cycle before by the delay unit 130, subtracts it from the current value by the subtracter 132, and outputs the gain by halving by the amplifier 134. As a result, as shown in FIG. 8B, the fundamental wave of the power distribution system 2 and its integral multiple harmonics can be removed. Interharmonics current I m which is included in the current I s flowing through the measuring points, because the order is a non-integer multiple order m is greater than 1 times the fundamental wave of the power distribution system 2 as described above, comb The filters 78 and 80 pass through without being removed.

上記非整数倍次数(換言すれば帯小数次数)mは、単独運転の検出精度を高めるためには、例えば、連系する配電系統2の電圧が7kV以下の高圧の場合は、1<m<2.75(但しm≠2)の範囲内が好ましく、配電系統2の電圧が7kVを超える特別高圧の場合は、1<m<3.6(但しm≠2、m≠3)の範囲内が好ましいことが実験によって確かめられている。この実施形態では、一例として2.25次〜2.75次の範囲内を用いている。   The non-integer multiple order (in other words, the sub-order number) m is, for example, 1 <m <when the voltage of the interconnected distribution system 2 is a high voltage of 7 kV or less, in order to increase the detection accuracy of isolated operation. 2.75 (however, m ≠ 2) is preferable, and in the case of extra high voltage where the voltage of distribution system 2 exceeds 7 kV, it is within the range of 1 <m <3.6 (where m ≠ 2, m ≠ 3) Has been confirmed by experiments. In this embodiment, the range of 2.25 to 2.75 order is used as an example.

再び図6を参照して、瞬時逆相演算器82は、コムフィルタ78、80から出力される電流Isα、Isβの瞬時値を用いて、次式に従って、当該電流の瞬時逆相電流の振幅|In |を演算して出力する。ここで、Inαは瞬時逆相電流のα成分、Inα′はその90度前の成分、Inβは瞬時逆相電流のβ成分、Inβ′はその90度前の成分である。 Referring again to FIG. 6, the instantaneous reverse phase calculator 82 uses the instantaneous values of the currents I s α and I s β output from the comb filters 78 and 80, and instantaneous instantaneous phase of the current according to the following equation: The current amplitude | I n | is calculated and output. Here, I n α is the α component of the instantaneous reverse phase current, I n α ′ is the component 90 degrees before, I n β is the β component of the instantaneous reverse phase current, and I n β ′ is the component 90 degrees before It is.

[数4]
nα=(1/2)(Isα+Isβ′)
nβ=(1/2)(Isβ−Isα′)
|In |=√(Inα2 +Inβ2
[Equation 4]
I n α = (1/2) (I s α + I s β ′)
I n β = (1/2) (I s β−I s α ′)
| I n | = √ (I n α 2 + I n β 2 )

交流電流の逆相成分(または正相成分)は、通常は、実効値を用いて対称座標法に従って算出されるのであるが、ここではそうせずに、上記の電流の瞬時値を用いて、対称座標法を近似的に定義して、上記式に従って瞬時逆相電流(具体的にはそのα成分およびβ成分)および瞬時逆相電流の振幅|In |を算出する。瞬時逆相電流は、上記のように瞬時値を用いて算出するので、実効値を用いる場合よりも高速で算出することができる。これについては、後で更に詳しく説明する。 The reverse phase component (or normal phase component) of the alternating current is normally calculated according to the symmetric coordinate method using the effective value, but here, instead of using the instantaneous value of the current, The symmetrical coordinate method is defined approximately, and the instantaneous negative phase current (specifically, its α component and β component) and the amplitude of the instantaneous negative phase current | I n | are calculated according to the above formula. Since the instantaneous reverse phase current is calculated using the instantaneous value as described above, it can be calculated at a higher speed than when the effective value is used. This will be described in more detail later.

瞬時逆相演算器82の構成の一例を図9に示す。上記β成分電流Isβを遅延器138で90度遅延させてβ成分電流Isβ′を算出し、それを加算器140でα成分電流Isαに加算し、増幅器144でゲインを1/2にして、瞬時逆相電流のα成分Inαを算出して座標変換器148に供給する。これが上記数4中の第1行目の演算である。かつ、上記α成分電流Isαを遅延器136で90度遅延させてα成分電流Isα′を算出し、それを減算器142でβ成分電流Isβから減算し、増幅器146でゲインを1/2にして、瞬時逆相電流のβ成分Inβを算出して座標変換器148に供給する。これが上記数4中の第2行目の演算である。 An example of the configuration of the instantaneous reverse phase calculator 82 is shown in FIG. The β component current I s β is delayed by 90 degrees by the delay unit 138 to calculate the β component current I s β ′, which is added to the α component current I s α by the adder 140, and the gain is set to 1 by the amplifier 144. Then, the α component I n α of the instantaneous reverse phase current is calculated and supplied to the coordinate converter 148. This is the operation of the first row in the above equation 4. Further, the α component current I s α is delayed by 90 degrees by the delay unit 136 to calculate the α component current I s α ′, subtracted from the β component current I s β by the subtractor 142, and gained by the amplifier 146. and 1/2, and supplies the coordinate converter 148 calculates the instantaneous negative sequence current beta component I n beta. This is the operation of the second row in the above equation 4.

座標変換器148は、上記数4中の第3行目の演算を行って、瞬時逆相電流の振幅|In |を演算して出力する。この振幅|In |は、上記測定点24を流れる電流Is に含まれている上記次数間高調波電流Im の大きさ(振幅)を表している。これを以下で更に説明する。 The coordinate converter 148 performs the calculation on the third row in the above equation 4, calculates the amplitude | I n | of the instantaneous reverse phase current, and outputs it. The amplitude | I n | represents the magnitude of the interharmonic current I m which is included in the current I s flowing through the measurement point 24 (amplitude). This is further explained below.

即ち、この実施形態のように、連系線22に非整数倍次数mの次数間高調波電流Im を単相注入すると、単相注入は不平衡な注入であるため、次の非特許文献1にも記載されているように(特に945−946頁参照)、当該次数間高調波電流Im を、測定点24を流れる当該非整数倍次数mの正相電流または逆相電流として算出することができる。その内で、この実施形態では逆相電流を扱っている。その理由は後で詳しく説明する。 That is, when the interphase harmonic current Im of non-integer multiple order m is single-phase injected into the interconnection line 22 as in this embodiment, the single-phase injection is an unbalanced injection. as also described in 1 (see especially 945-946 pages), the harmonic current I m among the orders is calculated as a positive phase current, or reverse-phase current of the flow measurement point 24 non-integer multiple order m be able to. Among them, this embodiment deals with a reverse phase current. The reason will be described in detail later.

非特許文献1:山本文雄、外3名、「分散電源の単独運転検出装置の開発−次数間高調波注入方式−」、電気設備学会誌、社団法人電気設備学会、平成16年12月10日、第24巻、第12号、頁943(57)−952(66)   Non-Patent Document 1: Yamamoto Fumio, 3 others, “Development of an independent operation detection device for distributed power sources-Harmonic injection method between orders”, The Journal of the Institute of Electrical Engineers of Japan, The Institute of Electrical Engineers of Japan, December 10, 2004 24, No. 12, pp. 943 (57) -952 (66)

上記次数間高調波電流Im は、その次数が上記のような系統基本波の非整数倍次数mであるため、配電系統2には自然には殆ど存在せず、従って、測定点24を流れる電流Is (この例ではそれを3相/2相変換器74で上記α成分電流Isαおよびβ成分電流Isβに変換した電流)を上記コムフィルタ78、80を通すことによって、瞬時逆相演算器82には、自設備で注入した上記非整数倍次数mのα成分電流Isαおよびβ成分電流Isβのみが供給され、そこで上記瞬時逆相電流の振幅|In |が算出される。従って、この振幅|In |は、上記測定点24を流れる電流Is に含まれている上記次数間高調波電流Im の大きさ(振幅)を表している。 The Interharmonics current I m, because its degree is non-integral multiple order m of the system fundamental wave as described above, almost absent in nature in the distribution system 2, thus, flows through the measurement point 24 By passing the current I s (current converted into the α component current I s α and β component current I s β by the three-phase / two-phase converter 74 in this example) through the comb filters 78, 80, an instantaneous Only the α component current I s α and β component current I s β of the non-integer multiple order m injected by the own equipment are supplied to the negative phase computing unit 82, where the amplitude | I n | Is calculated. Therefore, the amplitude | I n | represents between the orders are included in the current I s flowing through the measurement point 24 the magnitude of the harmonic current I m (amplitude).

再び図6を参照して、ローパスフィルタ84は、上記算出した振幅|In |から直流成分等のノイズを除去するためのものであり、それを設けるのが好ましいけれども、必須のものではない。ローパスフィルタ84の時定数は100m秒程度以下のものが好ましい。上記処理によって、上記振幅|In |を100m秒程度以下の高速で算出することができる。 Referring to FIG. 6 again, the low-pass filter 84 is for removing noise such as a DC component from the calculated amplitude | I n |, and although it is preferable to provide it, it is not essential. The time constant of the low-pass filter 84 is preferably about 100 milliseconds or less. By the above process, the amplitude | I n | can be calculated at a high speed of about 100 msec or less.

変化率演算器86は、瞬時逆相演算器82から出力されてローパスフィルタ84を通過した上記瞬時逆相電流の振幅|In |の、所定時間前からの変化率dIn を演算して出力する。この変化率dIn の演算には、この例のように、移動平均を用いるのが好ましい。 The rate-of-change calculator 86 calculates and outputs the rate of change dI n from a predetermined time before the amplitude | I n | of the instantaneous anti-phase current output from the instantaneous anti-phase calculator 82 and passed through the low-pass filter 84. To do. The calculation of the change rate dI n, as in this example, it is preferable to use a moving average.

より具体的には、変化率演算器86は、この例では、ローパスフィルタ84からの上記振幅|In |を遅延器88によって所定時間(例えば1秒程度)遅延し、移動平均演算器90によってその所定時間(例えば0.5秒間程度)の移動平均Inav を算出し、更に除算器92で次式に従って上記変化率dIn を算出する。 More specifically, in this example, the change rate calculator 86 delays the amplitude | I n | from the low-pass filter 84 by a delay unit 88 for a predetermined time (for example, about 1 second), and the moving average calculator 90 calculating a moving average I nav of the predetermined time (for example, about 0.5 seconds), and calculates the change rate dI n accordance with still following expressions divider 92.

[数5]
dIn =|In |/Inav
[Equation 5]
dI n = | I n | / I nav

遅延器88で所定時間遅延することによって、単独運転発生時の変化率dIn を大きくすることができる。この変化率dIn は、上記と同様の理由から、測定点24を流れる電流Is に含まれている上記次数間高調波電流Im の大きさの変化率を表している。 By delaying a predetermined time by the delaying unit 88, it is possible to increase the change rate dI n when islanding occurs. The rate of change dI n represents the same reason as described above, the magnitude of the rate of change of the interharmonic current I m which is included in the current I s flowing through the measurement points 24.

補正ゲイン演算器94は、変化率演算器86からの変化率dIn の逆数である補正ゲインG1 を演算して出力する。より具体的には、補正ゲイン演算器94は、この例では、定数1.0を発生させる定数設定器96と、次式に従って補正ゲインG1 を演算して出力する除算器98とを有している。 Correction gain calculator 94, the correction gain G 1 is the reciprocal of the rate of change dI n from the change rate calculator 86 calculates and outputs. More specifically, in this example, the correction gain calculator 94 includes a constant setting unit 96 that generates a constant 1.0, and a divider 98 that calculates and outputs the correction gain G 1 according to the following equation. ing.

[数6]
1 =1/dIn
[Equation 6]
G 1 = 1 / dI n

単独運転発生時の図6中の瞬時逆相電流の振幅の変化率dIn およびその逆数である補正ゲインG1 の変化の概略例を図10に示す。図10(A)に示すように、常時は上記振幅|In |に変化は殆どないのでその変化率dIn はほぼ1であり、単独運転が発生すると前述したように連系線22を流れる電流Is 中に含まれている次数間高調波電流Im が減少するので、上記変化率dIn は1より小さくなり、やがて1/N(Nは1.0より大きい数)付近に落ち着く。図10(B)に示すように、補正ゲインG1 はこの変化率dIn の逆で変化する。即ち、変化率dIn の変化を打ち消すように変化する。 FIG. 10 shows a schematic example of the change rate dI n of the amplitude of the instantaneous reverse phase current in FIG. 6 and the change of the correction gain G 1 which is the reciprocal number when the isolated operation occurs. As shown in FIG. 10A, since there is almost no change in the amplitude | I n | at all times, the rate of change dI n is almost 1, and when the single operation occurs, it flows through the interconnection line 22 as described above. since the current I s interharmonic current I m that is being included in the decreases, the change rate dI n is smaller than 1, finally 1 / n (n is greater than 1.0 number) settled in the vicinity. As shown in FIG. 10 (B), the correction gain G 1 varies in reverse the change rate dI n. That is, changes so as to cancel the change in the change rate dI n.

上記補正ゲイン演算回路76(より具体的にはその補正ゲイン演算器94)からの上記補正ゲインG1 は、図5に示すように次数間高調波電流指令値発生器46aに与えられる。次数間高調波電流指令値発生器46aは、上記インバータ6に次数間高調波電流Im を出力させるために与える上記次数間高調波電流の指令値Im ′を、上記補正ゲイン演算器94からの補正ゲインG1 で増大させる指令値補正器(図7中の指令値補正器124〜126参照)を有している。この次数間高調波電流指令値発生器46aの構成の一例を図7に示す。 The correction gain G 1 from the correction gain calculation circuit 76 (more specifically, the correction gain calculation unit 94) is applied to the inter-order harmonic current command value generator 46a as shown in FIG. Interharmonics current command value generator 46a is a command value of the interharmonic current I m 'to give in order to output the interharmonic current I m to the inverter 6, from the correction gain calculator 94 has the correction gain G 1 command value corrector that increases with the (reference command value corrector 124 to 126 in FIG. 7). An example of the configuration of the inter-order harmonic current command value generator 46a is shown in FIG.

インバータ6から出力する上記非整数倍次数mの次数間高調波電流Im の周波数fm を周波数設定器100で設定し、それを位相生成回路102の増幅器103で数7に従って角周波数ωm に変換し、それを積算器104で数8に従って離散時間系で角度θm に変換する。nはデータ番号である。 The frequency f m interharmonic current I m of the non-integer multiple order m output from the inverter 6 is set by the frequency setting unit 100, which in the angular frequency omega m according to Equation 7 by an amplifier 103 of the phase generator 102 Then, it is converted into an angle θ m in a discrete time system by the accumulator 104 according to Equation 8. n is a data number.

[数7]
ωm =2πfm
[Equation 7]
ω m = 2πf m

[数8]
θm =Σωm [n]
[Equation 8]
θ m = Σω m [n]

更に、剰余演算器105で、角度θm を2πで割ったときの余りを算出して、角度θm を0〜2πの範囲にする。 Further, the remainder calculator 105 calculates the remainder when the angle θ m is divided by 2π, and sets the angle θ m in the range of 0 to 2π.

初期位相設定器112〜114で、次数間高調波電流Im のu、v、w相の初期位相θmu、θmv、θmwを設定し、それらを加算器108〜110で上記角度θm に加算する。例えば、この実施形態ではuv相への単相注入であるので、θmu=0、θmv=πに設定する。なお、図7の例では、注入相を任意に選べるように、w相回路もu、v相回路と同様に設けて3相回路として、注入相以外のw相回路の出力は0にしている。注入相を固定(例えばuv相に固定)するのであれば、それ以外の相(例えばw相)の回路を設けなくても良く、その相(w相)は0信号を3相/2相変換器128に与えれば良い。以下の説明においても同様である。 In the initial phase setter 112 to 114, u interharmonic current I m, v, w-phase of the initial phase θ mu, θ mv, θ Set mw, the angle theta m them in adder 108 to 110 Add to. For example, in this embodiment, since it is a single-phase injection into the uv phase, θ mu = 0 and θ mv = π are set. In the example of FIG. 7, the w-phase circuit is also provided in the same manner as the u and v-phase circuits so that the injection phase can be arbitrarily selected, and the output of the w-phase circuit other than the injection phase is set to 0. . If the injection phase is fixed (for example, fixed to the uv phase), it is not necessary to provide a circuit for the other phase (for example, w phase), and the phase (w phase) converts the 0 signal to 3 phase / 2 phase. What is necessary is to give to the container 128. The same applies to the following description.

各加算器108〜110からの信号を用いて、正弦波関数発生器116〜118で非整数倍次数mの正弦波信号を発生させ、増幅器120〜122で次式に従ってその振幅を設定して、u、v、w相の次数間高調波電流Imu、Imv、Imwを発生させる。但し、w相回路の出力が0であるのは上記のとおりであり、この例では次数間高調波電流Imuが上記次数間高調波電流の指令値Im ′、次数間高調波電流Imvが同指令値−Im ′である。 Using the signals from the adders 108 to 110, the sine wave function generators 116 to 118 generate non-integer multiple order m sine wave signals, and the amplifiers 120 to 122 set their amplitudes according to the following equations: The harmonic currents I mu , I mv , and I mw of the u, v, and w phases are generated. However, the output of the w-phase circuit is 0 as described above. In this example, the interharmonic current I mu is the interharmonic current command value I m ′ and the interharmonic current I mv. Is the command value −I m ′.

[数9]
mu=Gmu・sin(θm +θmu
mv=Gmv・sin(θm +θmv
mw=Gmw・sin(θm +θmw
[Equation 9]
I mu = G mu · sin (θ m + θ mu )
I mv = G mv · sin (θ m + θ mv )
I mw = G mw · sin (θ m + θ mw )

上記周波数設定器100から増幅器120〜122までは、次数間高調波電流の指令値Im ′の発生回路と呼ぶこともできる。 The frequency setter 100 to the amplifiers 120 to 122 can also be referred to as a generation circuit for the command value I m ′ of the interharmonic current.

指令値補正器124〜126は、この例では乗算器であり、これらで上記次数間高調波電流の指令値Im ′(具体的には上記次数間高調波電流Imv、Imw)に上記補正ゲインG1 を掛けて、即ち指令値Im ′を補正ゲインG1 で増大させて、3相/2相変換器128に与える。但し、w相の指令値補正器126を設けなくても良いのは前述のとおりである。 The command value correctors 124 to 126 are multipliers in this example, and the command value correctors 124 to 126 are added to the command value I m ′ (specifically, the inter-order harmonic currents I mv and I mw ) of the inter-order harmonic current. is multiplied by the correction gain G 1, i.e., the command value I m 'is increased by the correction gain G 1, it gives the 3-phase / 2-phase converter 128. However, as described above, the w-phase command value corrector 126 may not be provided.

3相/2相変換器128は、上記3相/2相変換器74の場合と同様に、3相の入力を前記数2と同様の式に従って2相に直交変換して、補正後の次数間高調波電流の指令値Im ′のα成分Imαおよびβ成分Imβに変換して出力し、これらを図5に示す加算器48(これも前述したように2相分ある)に与える。図5中における加算器48以降は図2の場合と同様であり、これによって、インバータ6から出力する次数間高調波電流Im を上記補正ゲインG1 で増大させることができる。 The three-phase / two-phase converter 128 converts the three-phase input into two phases according to the same equation as the equation 2 in the same manner as in the case of the three-phase / two-phase converter 74, and the corrected order. An inter-harmonic current command value I m ′ is converted into an α component I m α and a β component I m β and output, and these are added to an adder 48 shown in FIG. 5 (also for two phases as described above). To give. Figure adder 48 after at 5 is the same as that of FIG. 2, thereby, the interharmonic current I m that is output from the inverter 6 can be increased by the correction gain G 1.

以上のようにこの単独運転検出装置10aによれば、単独運転が発生すると、測定点24から見た配電系統2側のインピーダンスが増大して、測定点24を流れる次数間高調波電流Im が減少するけれども、制御装置30a内の次数間高調波電流補正回路72は、上記次数間高調波電流Im の変化率(具体的にはこの実施形態では、次数間高調波電流Im の変化率を表す瞬時逆相電流の変化率dIn )を算出して、インバータ6から出力する次数間高調波電流Im を、上記算出した変化率に反比例させて増大させる(具体的にはこの実施形態では、上記変化率dIn の逆数である補正ゲインG1 で増大させる)ので、測定点24を流れる次数間高調波電流Im の減少が小さく抑えられる。その結果、単独運転発生時の測定点24における次数間高調波電圧Vm の変化が大きくなるので、単独運転監視装置32における判定値J1 の選定が容易になる。 According to the independent operation detecting apparatus 10a as described above, when the isolated operation occurs, the impedance viewed from the measurement point 24 the power distribution system 2 side is increased, the interharmonic current I m flowing through the measuring point 24 Although decreasing, interharmonic current correction circuit 72 in the control device 30a, in this embodiment, the rate of change of the interharmonic current I m (specifically, the rate of change of interharmonic current I m to calculate the instantaneous rate of change of the negative sequence current dI n) representing the a interharmonic current I m output from the inverter 6, the embodiment in (specifically to increase in inverse proportion to the rate of change calculated above so it is allowed) since increasing the correction gain G 1 is the inverse of the change rate dI n, reduction of interharmonic current I m flowing through the measuring point 24 is suppressed. As a result, the change in the inter-order harmonic voltage V m at the measurement point 24 at the time of isolated operation is increased, so that the determination value J 1 can be easily selected by the isolated operation monitoring device 32.

即ち、判定値J1 をあまり小さくせずに済むので、系統電圧の瞬時低下や系統周波数の変動のような系統擾乱発生時に誤検出(即ち、単独運転でないのに単独運転と判定する不要検出)が起こるのを防止することができる。しかも、単独運転発生時は次数間高調波電圧Vm の変化が大きくなって上記判定値J1 を確実に超えるので、単独運転を確実に検出することができる。また、増幅器54で設定するフィードバック係数Kp については、従来技術の課題の所で説明したけれども、この単独運転検出装置10aでは当該フィードバック係数Kp はこれまでと同様に分散電源8の本来の出力である基本波電流I1 に主眼をおいて設定すれば良いので、基本波電流I1 の制御が不安定になるのを防止することができる。 That is, since the judgment value J 1 does not need to be made too small, erroneous detection is performed when a system disturbance such as an instantaneous drop in system voltage or a change in system frequency occurs (that is, unnecessary detection that determines that the system is operating independently but not operating independently). Can be prevented. In addition, when the single operation occurs, the change in the inter-order harmonic voltage V m becomes large and reliably exceeds the determination value J 1 , so that the single operation can be reliably detected. Further, although the feedback coefficient K p set by the amplifier 54 has been described in the problem of the prior art, in this isolated operation detection device 10a, the feedback coefficient K p is the original output of the distributed power source 8 as before. since the fundamental wave current I 1 may be set focuses it, it is possible to prevent the control of the fundamental wave current I 1 becomes unstable.

以上の結果、この単独運転検出装置10aによれば、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とを両立させることができる。   As a result, according to this isolated operation detection device 10a, it is possible to achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs.

更にこの実施形態では、次数間高調波電流補正回路72は、瞬時逆相演算器82およびその前処理としてのコムフィルタ78、80等を有していて、次数間高調波電流Im の変化率を、瞬時逆相電流の振幅の変化率dIn として検出することによって、離散フーリエ変換器等を用いる場合に比べて高速で検出することができるので、単独運転発生時にインバータ6から出力される次数間高調波電流Im の減少をより速やかに抑制することができる。その結果、単独運転発生時の測定点24における次数間高調波電圧Vm の変化がより大きくなるので、単独運転監視装置32における判定値J1 の選定がより容易になる。その結果、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とをより確実に両立させることができる。 Further, in this embodiment, interharmonic current correction circuit 72 have the comb filter 78, 80 or the like as an instantaneous anti-phase calculator 82 and its pre-treatment, the rate of change of interharmonic current I m and by detecting the amplitude of the change rate dI n instantaneous negative sequence current, can be detected at high speed as compared with the case of using a discrete Fourier transformer or the like, output from the inverter 6 during isolated operation occurs order it can be more rapidly suppressed decrease between harmonic current I m. As a result, since the change in the inter-order harmonic voltage V m at the measurement point 24 when the isolated operation occurs becomes larger, the selection of the judgment value J 1 in the isolated operation monitoring device 32 becomes easier. As a result, it is possible to more reliably achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs.

これをより詳しく説明すると、上記のような非整数倍次数mの次数間高調波電流Im の抽出には、従来から離散フーリエ変換器がよく用いられているけれども、離散フーリエ変換器を用いる場合は、サンプル数を多くして(例えば系統基本波の30周期ぶん程度)周波数分解能を高める必要があるので、次数間高調波電流Im の抽出が遅くなる。そうなると、次数間高調波電流Im の変化を検出してインバータ6から出力する次数間高調波電流Im を増大させる動作が遅くなり、単独運転発生時の測定点24における次数間高調波電圧Vm の変化を大きくする動作も遅くなり、ひいては単独運転監視装置32における単独運転検出が遅くなる。これに対して、この実施形態では瞬時値を用いて瞬時逆相電流の振幅を演算するので、高速演算が可能であり、従って上記の次数間高調波電流Im 等の変化の検出が遅くなるという課題発生を防止することができる。 This will be explained in more detail, the extraction of interharmonic current I m of the non-integer multiple order m as described above, although conventionally the discrete Fourier transformer is often used, when using a discrete Fourier transformer since it is necessary to increase the frequency resolution (30 degree period sentence of example systems fundamental) by increasing the number of samples, the extraction of interharmonic current I m becomes slow. If this happens, it is slow operation to increase the interharmonic current I m which detects a change in interharmonic current I m output from the inverter 6, interharmonic voltage at the measurement point 24 at the time of islanding occurs V The operation for increasing the change of m is also delayed, and the isolated operation detection in the isolated operation monitoring device 32 is delayed. On the other hand, in this embodiment, since the amplitude of the instantaneous reverse phase current is calculated using the instantaneous value, high speed calculation is possible, and therefore detection of the change in the inter-order harmonic current Im etc. is delayed. The generation | occurrence | production of a problem can be prevented.

また、次数間高調波電流Im の逆相成分の算出に、実効値を用いる通常の対称座標法を用いると、実効値の算出に系統基本波の1サイクル以上の測定を必要とするので、この場合も、離散フーリエ変換器を用いる場合ほどではないとしても、演算が遅くなり、上記と同様の課題が生じる。これに対して、この実施形態では瞬時値を用いて瞬時逆相電流の振幅を演算するので、高速演算が可能であり、従って上記の次数間高調波電流Im 等の変化の検出が遅くなるという課題発生を防止することができる。 Further, the calculation of the reverse phase component of interharmonic current I m, the use of conventional symmetric coordinate method using an effective value, since it requires the measurement of one or more cycles of the system fundamental wave for calculation of the effective value, In this case as well, even if not as much as when a discrete Fourier transformer is used, the calculation is slowed down and the same problem as described above occurs. On the other hand, in this embodiment, since the amplitude of the instantaneous reverse phase current is calculated using the instantaneous value, high speed calculation is possible, and therefore detection of the change in the inter-order harmonic current Im etc. is delayed. The generation | occurrence | production of a problem can be prevented.

また、上述したように、非整数倍次数mの次数間高調波電流Im を単相注入した場合、当該次数間高調波電流Im を、測定点24を流れる非整数倍次数mの正相電流または逆相電流として算出することができるけれども、正相電流よりもこの実施形態のように逆相電流を扱うのが好ましい。具体的には瞬時逆相電流を扱うのが好ましい。瞬時値を扱うことの利点は上述したとおりである。瞬時正相電流を扱うよりも、瞬時逆相電流を扱う方が好ましいこと等を、以下のシミュレーション結果を用いて説明する。 As described above, if the interharmonic current I m of the non-integer multiple order m and single phase injected harmonic current I m between the orders, positive phase of non-integer multiple order m flowing measuring point 24 Although it can be calculated as a current or a negative phase current, it is preferable to handle the negative phase current as in this embodiment rather than the positive phase current. Specifically, it is preferable to handle instantaneous reverse phase current. The advantages of handling instantaneous values are as described above. The fact that it is preferable to handle the instantaneous negative phase current rather than the instantaneous positive phase current will be described using the following simulation results.

(2)シミュレーションの例
シミュレーションには、図11に示す系統モデルを用いた。これは、図3に示したシステムの配電系統2をより具体化したものである。即ち、上位系統156に変電所の遮断器154を介して高圧配電線152が接続されており、それに変圧器150および連系線22を介して前述した分散電源保有設備36が接続されている。高圧配電線152には、変圧器160および負荷162を有する高圧需要家設備158が接続されている。そしてここでは、標準の高圧系統を想定して、シミュレーションの条件は次のとおりとした。
(2) Example of simulation The system model shown in FIG. 11 was used for the simulation. This is a more specific example of the power distribution system 2 of the system shown in FIG. In other words, the high-voltage distribution line 152 is connected to the upper system 156 via the circuit breaker 154 of the substation, and the above-described distributed power supply facility 36 is connected to the upper system 156 via the transformer 150 and the interconnection line 22. A high voltage customer facility 158 having a transformer 160 and a load 162 is connected to the high voltage distribution line 152. Here, assuming the standard high-voltage system, the simulation conditions were as follows.

上位系統156:60Hz系、3相6.6kV、インピーダンスj8%(10MVAベース)
高圧配電線152:インピーダンス30+j40%(10MVAベース)、亘長5km相当
変圧器150、160:3相6.6kV/210V、110kVA、インピーダンス(%Z)2.5%(自己容量ベース)、リアクタンス(X)/抵抗(R)比=1.11
分散電源8(太陽光発電):容量100kW
高圧需要家負荷162:抵抗負荷100kW、モータ負荷30kVar、力率改善コンデンサ30kVar(クオリティファクタQf=0.3)
単独運転発生時のインピーダンス変化:20倍
注入する次数間高調波電流Im :次数m=2.73次、定格電流の2%をインバータ6から出力
Host system 156: 60 Hz system, 3-phase 6.6 kV, impedance j8% (10 MVA base)
High-voltage distribution line 152: impedance 30 + j40% (10 MVA base), equivalent to 5 km in length Transformer 150, 160: three-phase 6.6 kV / 210 V, 110 kVA, impedance (% Z) 2.5% (self-capacitance base), reactance ( X) / resistance (R) ratio = 1.11
Distributed power supply 8 (solar power generation): Capacity 100 kW
High voltage customer load 162: resistance load 100 kW, motor load 30 kVar, power factor improving capacitor 30 kVar (quality factor Qf = 0.3)
Impedance change at the time of isolated operation: 20 times Injected harmonic current I m : Order m = 2.73, 2% of rated current is output from inverter 6

上記系統モデルにおいて、分散電源8と需要家負荷162とが同容量でバランスしている状態で、変電所の遮断器154が開放されて分散電源8の単独運転が発生した時のシミュレーション結果を図12〜図15に示す。   In the system model described above, the simulation results when the distributed power source 8 is operated independently by opening the circuit breaker 154 in the substation in a state where the distributed power source 8 and the customer load 162 are balanced with the same capacity are shown in FIG. 12 to FIG.

まず、図12、図13について説明する。遮断器154が開放されて単独運転が発生した時、分散電源8の出力に対して需要家負荷162とのQバランス(無効電力のバランス)が僅かでも違うと、パワーコンディショナ34は出力周波数を上下させることによって無効電力のバランスを取ろうとするために、遮断器154から下流側の単独運転系統における基本波電圧V1 の周波数が変化する。この周波数変化(上下)の方向は需要家負荷162を構成するL、Cの優劣に依存しており、周波数変化の大きさはQバランスの崩れ方に依存している。 First, FIGS. 12 and 13 will be described. When the circuit breaker 154 is opened and a single operation occurs, if the Q balance (reactive power balance) with the consumer load 162 is slightly different from the output of the distributed power supply 8, the power conditioner 34 changes the output frequency. In order to balance reactive power by raising and lowering, the frequency of the fundamental voltage V 1 in the isolated operation system downstream from the circuit breaker 154 changes. The direction of this frequency change (up and down) depends on the superiority or inferiority of L and C constituting the customer load 162, and the magnitude of the frequency change depends on how the Q balance is broken.

分散電源8からの基本波電流I1 は、先に図2(および図5)を参照して説明したように、基本波電圧V1 の位相情報に基づいて作成した指令値I1 ′に従って出力されるので、上記のように基本波電圧V1 の周波数が変化すると基本波電流I1 の周波数も変化する。この周波数変化は、基本波電流I1 のものであるから、対称成分で見れば正相分の変化として表れ、逆相分では発生しない。 As described above with reference to FIG. 2 (and FIG. 5), the fundamental wave current I 1 from the distributed power supply 8 is output according to the command value I 1 ′ created based on the phase information of the fundamental wave voltage V 1. Therefore, when the frequency of the fundamental wave voltage V 1 changes as described above, the frequency of the fundamental wave current I 1 also changes. Since this frequency change is of the fundamental wave current I 1 , it appears as a change in the normal phase when viewed from the symmetrical component, and does not occur in the reverse phase.

従って、単独運転発生時の図6中の瞬時逆相電流の振幅の変化率dIn およびその逆数である補正ゲインG1 は、上記基本波電流I1 の周波数変化の影響を受けないので、図12に示すように、先に図10を参照して説明したものと同様に正しく変化している。従って、前述した作用効果を奏して、単独運転発生時にインバータ6から出力する次数間高調波電流Im の大きさをうまく補正することができる。 Accordingly, the rate of change dI n of the amplitude of the instantaneous reverse-phase current in FIG. 6 and the correction gain G 1 that is the reciprocal thereof in FIG. 6 when the single operation occurs are not affected by the frequency change of the fundamental current I 1 . As shown in FIG. 12, the change is the same as that described above with reference to FIG. Therefore, it is possible to exhibit the operational effect described above, to successfully correct the magnitude of interharmonic current I m output from the inverter 6 during isolated operation occurs.

一方、仮に図6に示した補正ゲイン演算回路76において、瞬時逆相電流に代えて、瞬時正相電流を扱い、瞬時逆相電流の変化率dIn の代わりに瞬時正相電流の振幅の変化率dIp を算出し、その逆数を補正ゲインG1 とした場合、上記基本波電流I1 の周波数変化に伴う正相分の変動の影響を受けるので、図13に示すように、単独運転発生時の次数間高調波電流の変化率および補正ゲインを正しく算出することはできない。即ち、図13(A)に示すように、単独運転発生時に、本来は配電系統2側のインピーダンスが増加しているので次数間高調波電流は減るのであるが、それとは反対に瞬時正相電流の変化率dIp が増加しており、その結果、図13(B)に示すように補正ゲインG1 が減少している。これは、本当は次数間高調波電流Im を増やさなければならない状況であるのにそれを減らすという逆方向の動作である。しかもこの瞬時正相電流の変化率dIp およびその逆数の補正ゲインG1 の変動の仕方は、前述したQバランスの崩れ方によって様々に変化するので、これらを用いても、単独運転発生時にインバータ6から出力する次数間高調波電流Im の大きさをうまく補正することはできない。 On the other hand, if the correction gain calculating circuit 76 shown in FIG. 6, instead of the instantaneous anti-phase currents, treats instantaneous positive-phase current, the amplitude variation of the instantaneous positive phase current instead of the rate of change dI n instantaneous negative sequence current When the rate dI p is calculated and the reciprocal thereof is set as the correction gain G 1 , it is affected by the fluctuation of the positive phase accompanying the frequency change of the fundamental wave current I 1 , so that an isolated operation occurs as shown in FIG. The rate of change of the harmonic current between orders and the correction gain cannot be calculated correctly. That is, as shown in FIG. 13 (A), when an isolated operation occurs, the impedance on the distribution system 2 side is originally increased, so that the harmonic current between the orders decreases, but on the contrary, the instantaneous positive phase current of and increased the rate of change dI p. as a result, the correction gain G 1 is being reduced as shown in FIG. 13 (B). This is the reverse operation of reducing it to a situation that must really increase the interharmonic current I m. In addition, the variation rate of the instantaneous positive phase current change rate dI p and the reciprocal correction gain G 1 vary depending on how the Q balance is lost. 6 can not be successfully corrected the magnitude of interharmonic current I m to be output from.

以上の理由から、瞬時正相電流を扱うよりも、この実施形態のように瞬時逆相電流を扱う方が好ましい。   For the above reasons, it is preferable to handle the instantaneous negative phase current as in this embodiment rather than the instantaneous positive phase current.

次に、図14、図15について説明する。シミュレーションの条件は前述したとおりである。なお、上記図中には、参考までに、次数間高調波電圧Vm の変化を当該電圧Vm の大きさで判定する場合の判定値J2 の一例を記入している。但しこれに限られるものではない。後述する他の図においても同様である。 Next, FIGS. 14 and 15 will be described. The simulation conditions are as described above. In the figure, for reference, an example of a determination value J 2 in the case where the change in the inter-order harmonic voltage V m is determined based on the magnitude of the voltage V m is shown. However, it is not limited to this. The same applies to other figures described later.

図14は、図1〜図2を参照して説明した従来の単独運転検出装置10を有する場合に、単独運転発生時をシミュレーションしたときの測定点24における次数間高調波電流Im および次数間高調波電圧Vm の変化の一例を示す図である。変電所の遮断器154が開放されて単独運転が発生すると、系統インピーダンスの増大に伴って次数間高調波電流Im が1/3程度に減少しており、それの影響で、次数間高調波電圧Vm の変化は、本来のインピーダンス変化(これは前記シミュレーション条件に示すように20倍)より遥かに小さく、6〜7倍程度に制限されている。系統条件によっては、次数間高調波電圧Vm の変化はこれよりも小さくなる場合もある(例えば図18およびその説明参照)。従って、前述したように、単独運転発生時にのみ次数間高調波電圧Vm が判定値J2 を確実に超えるような判定値J2 の選定が難しくなり、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とを両立させることが難しくなる。 Figure 14 is a diagram when having 1 to FIG. 2 reference conventional independent operation detecting apparatus 10 described and islanding operation between orders at the measuring point 24 when the simulated time of occurrence harmonic current I m and between orders is a diagram showing an example of a change in the harmonic voltage V m. When breaker 154 of the substation is opened islanding occurs, and decreased to about 1/3 of the harmonic current I m between orders with increasing system impedance, in its effects, interharmonic The change in the voltage V m is much smaller than the original impedance change (this is 20 times as shown in the simulation conditions) and is limited to about 6 to 7 times. Depending on the system conditions, the change in inter-order harmonic voltage V m may be smaller than this (see, for example, FIG. 18 and its description). Therefore, as described above, it becomes difficult to select the judgment value J 2 so that the interharmonic voltage V m surely exceeds the judgment value J 2 only when the single operation occurs. It becomes difficult to achieve both prevention of erroneous detection at the time of occurrence.

図15は、図3〜図10を参照して説明した本発明の第1の実施形態の単独運転検出装置10aを有する場合に、単独運転発生時をシミュレーションしたときの測定点24における次数間高調波電流Im および次数間高調波電圧Vm の変化の一例を示す図である。変電所の遮断器154が開放されて単独運転が発生すると、系統インピーダンスの増大に伴って次数間高調波電流Im が減少するけれども2/3程度に留められており、それによって次数間高調波電圧Vm の変化は12倍程度まで増大している。従って、前述したように、単独運転発生時にのみ次数間高調波電圧Vm が判定値J2 を確実に超えるような判定値J2 の選定が容易になり、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とを両立させることができる。 FIG. 15 shows the inter-order harmonics at the measurement point 24 when simulating the occurrence of isolated operation when the isolated operation detection device 10a of the first embodiment of the present invention described with reference to FIGS. is a diagram showing an example of a change in the wave currents I m and interharmonic voltage V m. When breaker 154 of the substation is opened by islanding operation occurs, is fastened to 2/3 but the harmonic current I m decreases between orders with increasing system impedance, whereby interharmonic The change in the voltage V m increases to about 12 times. Therefore, as described above, it becomes easy to select the judgment value J 2 so that the interharmonic voltage V m surely exceeds the judgment value J 2 only when the single operation occurs. It is possible to achieve both prevention of erroneous detection when a disturbance occurs.

(3)単独運転検出装置の第2の実施形態
次に、単独運転検出装置10aの第2の実施形態を、先の第1の実施形態との相違点を主に説明する。
(3) Second Embodiment of Isolated Operation Detection Device Next, the second embodiment of the isolated operation detection device 10a will be described mainly with respect to differences from the previous first embodiment.

この実施形態では、上記制御装置30a内の次数間高調波電流補正回路72は、より具体的にはそれを構成する補正ゲイン演算回路76は、図16に示す例のように、上記補正ゲイン演算器94からの上記補正ゲインG1 の変化率を、定常時の値を1に保ちつつ拡大して補正ゲインG4 として出力する補正ゲイン拡大器164を更に有している。 In this embodiment, the inter-order harmonic current correction circuit 72 in the control device 30a is more specifically the correction gain calculation circuit 76 constituting the same, as in the example shown in FIG. The correction gain expander 164 further expands the rate of change of the correction gain G 1 from the adjuster 94 while maintaining the steady-state value at 1, and outputs it as the correction gain G 4 .

そして、上記補正ゲインG1 の代わりとして、拡大させた上記補正ゲインG4 を、図7に示す次数間高調波電流指令値発生器46a内の指令値補正器124〜126に与えて、インバータ6に与える次数間高調波電流の指令値Im ′を、補正ゲイン拡大器164からの拡大させた補正ゲインG4 で増大させるようにしている。 Then, instead of the correction gain G 1 , the enlarged correction gain G 4 is given to the command value correctors 124 to 126 in the inter-order harmonic current command value generator 46a shown in FIG. the command value I m 'interharmonic current applied to, so that increase in the correction gain G 4 which is enlarged from the correction gain expander 164.

補正ゲイン拡大器164は、この例では、上記補正ゲイン演算器94からの補正ゲインG1 をゲインG2 で増幅する増幅器166と、定数(G2 −1.0)を設定する定数設定器170と、増幅器166の出力から定数設定器170の出力を減算して次式で表される補正ゲインG4 を出力する減算器168とを有している。 In this example, the correction gain expander 164 includes an amplifier 166 that amplifies the correction gain G 1 from the correction gain calculator 94 with a gain G 2 , and a constant setting unit 170 that sets a constant (G 2 −1.0). And a subtractor 168 that subtracts the output of the constant setting unit 170 from the output of the amplifier 166 and outputs a correction gain G 4 expressed by the following equation.

[数10]
4 =G2 ・G1 −(G2 −1)
[Equation 10]
G 4 = G 2 · G 1 − (G 2 −1)

上記補正ゲインG4 を用いる理由を図17を参照して説明する。図17(A)中の補正ゲインG1 は、図10(B)に示した補正ゲインG1 と同じものである。この補正ゲインG1 の変化率を拡大するために、それに単純にゲインG2 を掛けると、図17(A)に示す補正ゲインG3 (=G2 ・G1 )となり、定常時の値が1でなくG2 になってしまう。これに対して、上記補正ゲインG4 にすると、図17(B)に示すように、定常時の値を1に保ちつつ、補正ゲインG4 の変化率を拡大することができる。補正ゲインG4 の定常時の値を1に保つと、定常時にインバータ6から出力する次数間高調波電流Im の大きさを変えずに済み、ひいては定常時の測定点24における次数間高調波電圧Vm の大きさを変えずに済むので、単独運転監視装置32における判定値J1 (またはJ2 )も変えずに済み、単独運転監視装置32における次数間高調波電圧Vm の変化の検出が容易になる。 The reason for using the correction gain G 4 with reference to FIG. 17 will be described. The correction gain G 1 in FIG. 17A is the same as the correction gain G 1 shown in FIG. If the gain G 2 is simply multiplied to increase the rate of change of the correction gain G 1, the correction gain G 3 (= G 2 · G 1 ) shown in FIG. It becomes G 2 instead of 1. In contrast, when the above correction gain G 4, as shown in FIG. 17 (B), while keeping the value of the steady state 1, it is possible to enlarge the rate of change of the correction gain G 4. Correcting Keeping the value in the steady state gain G 4 to 1, requires without changing the size of the interharmonic current I m output from the inverter 6 during steady, interharmonic at the measurement point 24 in the steady state and thus Since it is not necessary to change the magnitude of the voltage V m , it is not necessary to change the judgment value J 1 (or J 2 ) in the isolated operation monitoring device 32, and the change in the inter-order harmonic voltage V m in the isolated operation monitoring device 32 can be avoided. Detection is easy.

しかも、拡大させた補正ゲインG4 を用いることによって、単独運転発生時にインバータ6から出力される次数間高調波電流Im の減少をより確実に抑制することができる。その結果、単独運転発生時の測定点24における次数間高調波電圧Vm の変化がより一層大きくなるので、単独運転監視装置32における判定値の選定がより一層容易になる。その結果、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とをより確実に両立させることができる。 Moreover, by using the correction gain G 4 which is enlarged, it is possible to more reliably suppress the decrease of interharmonic current I m which is output from the inverter 6 during isolated operation occurs. As a result, since the change in the inter-order harmonic voltage V m at the measurement point 24 when the isolated operation occurs is further increased, the selection of the judgment value in the isolated operation monitoring device 32 is further facilitated. As a result, it is possible to more reliably achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs.

(2)シミュレーションの他の例
上記第2の実施形態のように拡大させた補正ゲインG4 を用いる場合の効果を、以下のシミュレーション結果を用いて説明する。この場合も図11に示した系統モデルを用いた。シミュレーション条件は、単独運転発生時にインピーダンス変化の生じにくい次の条件とした。
(2) the effect of using the correction gain G 4 which is enlarged as in other examples the second embodiment of the simulation will be described with reference to the following simulation results. Also in this case, the system model shown in FIG. 11 was used. The simulation conditions were the following conditions in which impedance change hardly occurs when an isolated operation occurs.

上位系統156:60Hz系、3相6.6kV、インピーダンスj8%(10MVAベース)
高圧配電線152:インピーダンス180+j240%(10MVAベース)、亘長30km相当
変圧器150:3相6.6kV/210V、110kVA、インピーダンス(%Z)7.5%(自己容量ベース)、リアクタンス(X)/抵抗(R)比=1.11
変圧器160:3相6.6kV/210V、120kVA、インピーダンス(%Z)7.5%(自己容量ベース)、リアクタンス(X)/抵抗(R)比=1.11
分散電源8(太陽光発電):容量100kW
高圧需要家負荷162:抵抗負荷100kW、モータ負荷60kVar、力率改善コンデンサ60kVar(クオリティファクタQf=0.6)
単独運転発生時のインピーダンス変化:2.3倍
注入する次数間高調波電流Im :次数m=2.73次、定格電流の2%をインバータ6から出力
Host system 156: 60 Hz system, 3-phase 6.6 kV, impedance j8% (10 MVA base)
High-voltage distribution line 152: impedance 180 + j 240% (10 MVA base), equivalent to 30 km in length Transformer 150: 3-phase 6.6 kV / 210 V, 110 kVA, impedance (% Z) 7.5% (self-capacitance base), reactance (X) / Resistance (R) ratio = 1.11
Transformer 160: 3-phase 6.6 kV / 210 V, 120 kVA, impedance (% Z) 7.5% (self-capacitance base), reactance (X) / resistance (R) ratio = 1.11.
Distributed power supply 8 (solar power generation): Capacity 100 kW
High voltage customer load 162: resistance load 100 kW, motor load 60 kVar, power factor improving capacitor 60 kVar (quality factor Qf = 0.6)
Impedance change at the time of isolated operation: 2.3 times Injected order harmonic current I m : Order m = 2.73, 2% of rated current is output from inverter 6

上記系統モデルにおいて、分散電源8と需要家負荷162とが同容量でバランスしている状態で、変電所の遮断器154が開放されて分散電源8の単独運転が発生した時のシミュレーション結果を図18〜図20に示す。   In the system model described above, the simulation results when the distributed power source 8 is operated independently by opening the circuit breaker 154 in the substation in a state where the distributed power source 8 and the customer load 162 are balanced with the same capacity are shown in FIG. 18 to 20.

図18は、前述した従来の単独運転検出装置10を有している場合であり、単独運転時に次数間高調波電流Im は1/2程度に減少しており、その影響で、次数間高調波電圧Vm の変化は、本来のインピーダンス変化(これは前記シミュレーション条件に示すように2.3倍)に比べて小さく、2倍未満に制限されている。従って、単独運転発生時にのみ次数間高調波電圧Vm が判定値J2 を確実に超えるような判定値J2 の選定が非常に難しい。 Figure 18 is the result when the conventional independent operation detecting apparatus 10 described above, the interharmonic current I m when the single operation has been reduced to about 1/2, with the effect, harmonics between orders The change in the wave voltage V m is smaller than the original impedance change (which is 2.3 times as shown in the simulation conditions) and is limited to less than 2 times. Therefore, it is very difficult to select the judgment value J 2 so that the inter-order harmonic voltage V m surely exceeds the judgment value J 2 only when the single operation occurs.

図19は、前述した第1の実施形態の単独運転検出装置10aを有している場合であり、単独運転時の次数間高調波電流Im の減少が抑制されており、それに伴って、次数間高調波電圧Vm の変化も2倍近くまで大きくなっている。従って、判定値J2 の選定が容易になる。 Figure 19 is a case having a first embodiment of the independent operation detecting apparatus 10a described above, a decrease in interharmonic current I m when islanding operation is suppressed, with it, the order The change of the inter-harmonic voltage V m is also increased to nearly twice. Accordingly, the determination value J 2 can be easily selected.

図20は、上記第2の実施形態の単独運転検出装置10aを有している場合であり、単独運転時の次数間高調波電流Im は、ごく短時間減少するもののすぐに回復して、ほぼ一定の大きさで出力できている。その結果、次数間高調波電圧Vm の変化は、本来のインピーダンスの変化(2.3倍)と同程度に大きくなっている。従って、単独運転発生時にインピーダンス変化が生じにくい系統においても、単独運転発生時にのみ次数間高調波電圧Vm が判定値J2 を確実に超えるような判定値J2 の選定がより容易になり、単独運転の確実な検出と、系統擾乱発生時の誤検出の防止とをより確実に両立させることができる。 Figure 20 is the result when the independent operation detecting apparatus 10a of the second embodiment, interharmonic current I m when islanding operation is to recover quickly but decreases very short time, The output is almost constant. As a result, the change in the inter-order harmonic voltage V m is as large as the original change in impedance (2.3 times). Therefore, even in a system in which an impedance change is unlikely to occur when an isolated operation occurs, it becomes easier to select the determination value J 2 so that the inter-order harmonic voltage V m surely exceeds the determination value J 2 only when the isolated operation occurs. It is possible to more reliably achieve both reliable detection of isolated operation and prevention of erroneous detection when a system disturbance occurs.

2 配電系統
4 直流電力を出力する電源
6 インバータ
8 分散電源
10、10a 単独運転検出装置
22 連系線
24 測定点
30、30a 制御装置
32 単独運転監視装置
36 分散電源保有設備
46、46a 次数間高調波電流指令値発生器
72 次数間高調波電流補正回路
76 補正ゲイン演算回路
78、80 コムフィルタ
82 瞬時逆相演算器
86 変化率演算器
94 補正ゲイン演算器
124〜126 指令値補正器
164 補正ゲイン拡大器
m 非整数倍次数
m 次数間高調波電流
m 次数間高調波電圧
dIn 瞬時逆相電流の振幅の変化率
1 、G4 補正ゲイン
2 Power distribution system 4 Power supply that outputs DC power 6 Inverter 8 Distributed power supply 10, 10a Independent operation detection device 22 Interconnection line 24 Measuring point 30, 30a Control device 32 Independent operation monitoring device 36 Distributed power supply equipment 46, 46a Interharmonic Wave current command value generator 72 Interharmonic current correction circuit 76 Correction gain calculation circuit 78, 80 Comb filter 82 Instantaneous antiphase calculator 86 Change rate calculator 94 Correction gain calculator 124-126 Command value corrector 164 Correction gain Expander m Non-integer multiple order I m Harmonic current between m orders V m Harmonic voltage between orders m dIn n Rate of change in instantaneous negative phase current amplitude G 1 , G 4 correction gain

Claims (3)

直流電力を出力する電源と当該直流電力を交流電力に変換して出力するインバータとを有する分散電源を備えている分散電源保有設備が配電系統に接続された構成のシステムに適用されて、前記分散電源が単独運転になったことを検出する単独運転検出装置であって、
前記インバータを制御して、前記インバータから、前記配電系統の基本波と同じ周波数の3相の基本波電流に、当該基本波の1倍よりも大きい非整数倍次数の次数間高調波電流を単相で重畳させて出力させる機能を有している制御装置と、
前記分散電源保有設備と前記配電系統との連系線上の測定点における前記非整数倍次数の次数間高調波電圧を測定して、当該次数間高調波電圧の変化から、前記分散電源が単独運転になったことを検出する単独運転監視装置とを備えており、
かつ前記制御装置は、前記連系線上の測定点を流れる前記次数間高調波電流の大きさの、所定時間前の値からの変化率を算出して、前記インバータから出力する前記次数間高調波電流を、前記算出した変化率に反比例させて増大させる次数間高調波電流補正回路を有している、ことを特徴とする分散電源の単独運転検出装置。
The distributed power supply facility comprising a distributed power source having a power source that outputs DC power and an inverter that converts the DC power into AC power and outputs the same is applied to a system having a configuration in which the distributed power source is connected to a distribution system. An isolated operation detection device for detecting that the power supply has been operated independently,
By controlling the inverter, a single-phase harmonic current having a non-integer multiple order larger than 1 times the fundamental wave is simply applied from the inverter to a three-phase fundamental current having the same frequency as the fundamental wave of the distribution system. A control device having a function of superimposing and outputting in phase;
Measure the harmonic voltage between the orders of the non-integer multiple order at the measurement point on the connection line between the distributed power supply facility and the distribution system, and the distributed power supply operates independently from the change in the harmonic voltage between the orders. With an isolated operation monitoring device that detects that
The control device calculates a rate of change from a value before a predetermined time of the magnitude of the interharmonic current flowing through the measurement point on the interconnection line, and outputs the interharmonic harmonic output from the inverter. An isolated operation detection apparatus for a distributed power source, comprising: an inter-order harmonic current correction circuit that increases current in inverse proportion to the calculated rate of change.
前記次数間高調波電流補正回路は、
前記連系線上の測定点を流れる電流から、前記配電系統の基本波およびその整数倍の高調波を除去した電流を出力するコムフィルタと、
前記コムフィルタから出力される前記電流の瞬時値を用いて、当該電流の瞬時逆相電流の振幅を演算して出力する瞬時逆相演算器と、
前記瞬時逆相演算器からの前記瞬時逆相電流の振幅の、所定時間前からの変化率を演算して出力する変化率演算器と、
前記変化率演算器からの前記変化率の逆数である補正ゲインを演算して出力する補正ゲイン演算器と、
前記インバータに前記次数間高調波電流を出力させるために与える次数間高調波電流の指令値を、前記補正ゲイン演算器からの前記補正ゲインで増大させる指令値補正器とを有している請求項1記載の分散電源の単独運転検出装置。
The inter-harmonic current correction circuit is
A comb filter that outputs a current obtained by removing a fundamental wave of the distribution system and a harmonic of an integral multiple thereof from a current flowing through a measurement point on the interconnection line;
Using the instantaneous value of the current output from the comb filter, the instantaneous negative phase calculator for calculating and outputting the amplitude of the instantaneous negative phase current of the current,
A change rate calculator that calculates and outputs the rate of change of the amplitude of the instantaneous negative phase current from the instantaneous negative phase calculator from a predetermined time; and
A correction gain calculator that calculates and outputs a correction gain that is the reciprocal of the change rate from the change rate calculator;
A command value corrector that increases a command value of an interharmonic current to be supplied to the inverter to output the interharmonic current with the correction gain from the correction gain calculator. The isolated operation detection apparatus for a distributed power source according to 1.
前記次数間高調波電流補正回路は、前記補正ゲイン演算器からの前記補正ゲインの変化率を、定常時の値を1に保ちつつ拡大して出力する補正ゲイン拡大器を更に有しており、
前記指令値補正器は、前記インバータに与える前記次数間高調波電流の指令値を、前記補正ゲイン拡大器からの拡大させた補正ゲインで増大させるものである請求項2記載の分散電源の単独運転検出装置。
The inter-order harmonic current correction circuit further includes a correction gain expander that expands and outputs the rate of change of the correction gain from the correction gain calculator while maintaining a steady-state value of 1,
The distributed operation of the distributed power supply according to claim 2, wherein the command value corrector increases the command value of the inter-order harmonic current to be supplied to the inverter with an increased correction gain from the correction gain expander. Detection device.
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