JPH1123626A - Current injector for measuring harmonic - Google Patents
Current injector for measuring harmonicInfo
- Publication number
- JPH1123626A JPH1123626A JP19780997A JP19780997A JPH1123626A JP H1123626 A JPH1123626 A JP H1123626A JP 19780997 A JP19780997 A JP 19780997A JP 19780997 A JP19780997 A JP 19780997A JP H1123626 A JPH1123626 A JP H1123626A
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- Japan
- Prior art keywords
- harmonic
- current
- injection
- harmonics
- frequency
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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- Supply And Distribution Of Alternating Current (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、電力系統の高調波
特性の測定に用いられる電流注入装置に関し、詳しくは
その小型化に関する。[0001] 1. Field of the Invention [0002] The present invention relates to a current injection device used for measuring harmonic characteristics of a power system, and more particularly, to miniaturization thereof.
【0002】[0002]
【従来の技術】従来、電力の送,配電においては、高調
波を低減することが重要である。2. Description of the Related Art Conventionally, in power transmission and distribution, it is important to reduce harmonics.
【0003】そして、n次(nは1,2,3,…の整
数)の高調波は系統基本周波数fs の整数倍であり、代
表的な5次,7次の高調波は5×fs ,7×fs であ
る。[0003] Then, n order (n is 1, 2, 3, ... integer) harmonic is an integer multiple of the system fundamental frequency f s, a typical fifth order, seventh order harmonics 5 × f s, 7 is a × f s.
【0004】この高調波の低減は高調波レベル(電圧レ
ベル)を予測し、その周波数のフィルタ設備をコンデン
サ設備に付設等して行われる。[0004] The reduction of the harmonics is performed by predicting the harmonic level (voltage level) and attaching filter equipment of the frequency to the capacitor equipment.
【0005】そして、高調波レベルを予測する場合、電
力系統の例えば前記フィルタ設備の接続点より下位(下
流)又は上位(上流)の高調波特性を把握し、その等価
回路(高調波等価回路)を求める必要がある。When predicting the harmonic level, the lower (downstream) or upper (upstream) harmonic characteristics of the power system, for example, from the connection point of the filter equipment are grasped, and an equivalent circuit thereof (harmonic equivalent circuit) is obtained. ).
【0006】この高調波等価回路は、例えばノートンの
定理で表示した場合、アドミタンスと電流源との並列回
路とみなすことができる。When this harmonic equivalent circuit is represented by, for example, Norton's theorem, it can be regarded as a parallel circuit of admittance and a current source.
【0007】そして、電気学会論文誌B101巻8号,
P.451−458,(昭56−8)には、配電系統の
第5調波についての高調波等価回路を求める際、系統の
基本波の電圧,電流を計測し、その結果から高調波等価
回路のアドミタンス,電流源の大きさ,位相等を算出し
て推定することが記載されている。[0007] The Institute of Electrical Engineers of Japan, B101 Vol.
P. 451-458, (Showa 56-8), when obtaining a harmonic equivalent circuit for the fifth harmonic of the distribution system, measures the voltage and current of the fundamental wave of the system, and from the results, determines the harmonic equivalent circuit. It describes that the admittance, the magnitude of the current source, the phase, and the like are calculated and estimated.
【0008】しかし、前記論文誌に記載の高調波測定方
法の場合、系統の計測の基本波電圧・電流を計測し、そ
の計測結果から高調波アドミタンス,高調波電流源の大
きさ,位相等を推定して高調波特性を測定するため、精
度の高い測定が行えない。However, in the case of the harmonic measurement method described in the above-mentioned journal, the fundamental voltage and current of the system are measured, and the harmonic admittance, the size and phase of the harmonic current source, etc. are measured from the measurement results. Since the harmonic characteristics are measured by estimation, high-precision measurement cannot be performed.
【0009】すなわち、前記の測定方法にあっては、測
定対象の高調波のアドミタンスや電流源を実測して求め
たわけではなく、基本波の計測情報に基づき、基本波の
大きさ(ベクトル値)から測定対象の高調波の大きさ
(べクトル値)を推定するに過ぎないため、その高調波
特性を精度よく求めて測定することができない。That is, in the above-described measuring method, the magnitude (vector value) of the fundamental wave is not determined by actually measuring the admittance or current source of the harmonic to be measured, but based on the measurement information of the fundamental wave. Since only the magnitude (vector value) of the harmonic to be measured is estimated from the above, it is not possible to accurately obtain and measure the harmonic characteristic.
【0010】そのため、従来は電力系統の例えばフィル
タ設備の接続点より下位の高調波特性を正確に把握して
適当なフィルタ設備を設けたりすることができず、高調
波レベルを良好に低減することができなかった。For this reason, conventionally, it is not possible to accurately grasp the lower harmonic characteristics of the power system, for example, from the connection point of the filter equipment, and to provide an appropriate filter equipment, thereby reducing the harmonic level satisfactorily. I couldn't do that.
【0011】そこで、本出願人は特願平8−31019
2号の出願により、系統の高調波注入点に測定対象の高
調波(測定調波)の上下の系統基本周波数の非整数倍の
2周波数の電流(中間高調波の電流)をそれぞれ注入
し、各中間高調波の電圧,電流の実測結果から、系統の
高調波注入点より下位または上位の各中間高調波それぞ
れについての等価回路のアドミタンスを求め、それらを
用いた補間処理により、高調波注入点より下位又は上位
の測定対象の高調波についての等価回路のアドミタンス
を決定してその高調波特性を測定することを既に発明し
ている。Therefore, the present applicant has filed Japanese Patent Application No. 8-31019.
According to the application of No. 2, currents of two frequencies (intermediate harmonic currents) which are non-integer multiples of the system fundamental frequency above and below the harmonic (measurement harmonic) to be measured are respectively injected into the system harmonic injection points, From the measured results of the voltage and current of each intermediate harmonic, the admittance of the equivalent circuit for each intermediate harmonic lower or higher than the harmonic injection point of the system is obtained, and interpolation is performed using these to determine the harmonic injection point. It has already been invented to determine the admittance of the equivalent circuit for the higher or lower harmonics to be measured and measure its harmonic characteristics.
【0012】この場合、測定対象の高調波の上下の各中
間高調波の電流が系統に本来存在しない系統基本周波数
の非整数倍周波数の電流であり、それらの等価回路のア
ドミタンスが、系統に存在する各高調波の影響を受ける
ことなく、実測により精度よく求まるため、この結果を
用いて系統の例えば5次,7次の高調波の特性を精度よ
く測定して把握することができる。In this case, the current of each intermediate harmonic above and below the harmonic to be measured is a current of a non-integer multiple of the system fundamental frequency that does not originally exist in the system, and the admittance of their equivalent circuit is present in the system. Since it is accurately determined by actual measurement without being affected by each harmonic, the characteristics of, for example, the fifth and seventh harmonics of the system can be accurately measured and grasped using this result.
【0013】[0013]
【発明が解決しようとする課題】前記既出願の高調波測
定方法を実施する場合、注入装置が必要となり、計測装
置全体が大型化されることが懸念されるため、小型の注
入装置で各中間高調波の電流をどのようにして形成して
系統に注入するかが重要な課題である。In order to carry out the harmonic measurement method of the above-mentioned application, an injection device is required, and there is a concern that the entire measurement device becomes large. An important issue is how to generate and inject harmonic currents into the system.
【0014】本発明は、各中間高調波の電流を短時間に
注入し得るようにして、電流注入装置を小容量化し、小
型化することを課題とする。It is an object of the present invention to reduce the capacity and size of a current injection device so that current of each intermediate harmonic can be injected in a short time.
【0015】[0015]
【課題を解決するための手段】前記の課題を解決するた
めに、本発明の高調波測定用の電流注入装置は、出力周
波数が各中間高調波の周波数に連続的に変化するインバ
ータと、各中間高調波のほぼ中間に共振点を設定した共
振回路からなり、インバータの出力から各中間高調波の
電流を抽出するフィルタ部と、フィルタ部から出力され
た各中間高調波の電流を系統に注入する結合トランスと
を備える。したがって、インバータの出力が連続的に各
中間高調波の周波数に変化する。In order to solve the above-mentioned problems, a current injection device for measuring harmonics according to the present invention comprises: an inverter whose output frequency continuously changes to the frequency of each intermediate harmonic; It consists of a resonance circuit with a resonance point set almost in the middle of the intermediate harmonics. The filter section extracts the current of each intermediate harmonic from the output of the inverter, and the current of each intermediate harmonic output from the filter section is injected into the system. And a coupling transformer. Therefore, the output of the inverter continuously changes to the frequency of each intermediate harmonic.
【0016】さらに、インバータの各中間高調波の周波
数成分にフィルタ部が共振し、この共振による周波数の
選択に基づき、フィルタ部が系統基本周波数の成分や各
中間高調波の逓倍周波数の成分等の不要な周波数成分を
排除してインバータの出力から各中間高調波の電流を抽
出する。Further, the filter unit resonates with the frequency components of the respective intermediate harmonics of the inverter, and based on the selection of the frequency by the resonance, the filter unit converts the components of the system fundamental frequency, the components of the multiplied frequency of the respective intermediate harmonics, and the like. Unnecessary frequency components are eliminated and the current of each intermediate harmonic is extracted from the output of the inverter.
【0017】そして、フィルタ部の各中間高調波の電流
が結合トランスを介して系統に注入される。Then, the current of each intermediate harmonic of the filter section is injected into the system via the coupling transformer.
【0018】この場合、各中間高調波の電流を1台の電
流注入装置から系統に注入することができる。In this case, the current of each intermediate harmonic can be injected into the system from one current injection device.
【0019】しかも、この電流注入装置の出力が各中間
高調波の周波数に連続的に変化し、各中間高調波の電流
の注入が短時間で終了するため、電流注入装置はいわゆ
る短時間定格を満足すればよく、小容量,小型に形成す
ることができる。Moreover, the output of the current injection device continuously changes to the frequency of each intermediate harmonic, and the injection of the current of each intermediate harmonic is completed in a short time. It suffices to be satisfied, and a small capacity and small size can be formed.
【0020】[0020]
【発明の実施の形態】本発明の実施の1形態について、
図1ないし図3を参照して説明する。まず、図2は測定
の対象となる電力系統1の単線表記の等価回路を示し、
この電力系統1の配電用変電所2の低圧2次側(660
0V側)の高調波特性を測定するため、配電用変電所2
の配電トランス3の2次側から引出された配電母線4に
高調波注入・計測点aが設定される。DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described.
This will be described with reference to FIGS. First, FIG. 2 shows a single-line equivalent circuit of the power system 1 to be measured.
The low-voltage secondary side (660) of the distribution substation 2 of this power system 1
0V side) to measure the harmonic characteristics of the distribution substation 2
The harmonic injection / measurement point a is set on the distribution bus 4 drawn out from the secondary side of the distribution transformer 3.
【0021】この注入・計測点aに配電用変電所2の低
圧トランス5の高圧側(6600V),低圧側(220
V)を介して高調波測定用の電流注入装置6が接続さ
れ、この電流注入装置6及びA/D変換器7,信号処理
装置8,演算処理装置9,表示装置10,記録装置11
により、高調波測定装置12が形成される。At the injection / measurement point a, the high-voltage side (6600 V) and the low-voltage side (220
V), a current injection device 6 for harmonic measurement is connected, and the current injection device 6 and the A / D converter 7, the signal processing device 8, the arithmetic processing device 9, the display device 10, and the recording device 11 are connected.
Thereby, the harmonic measuring device 12 is formed.
【0022】ところで、電力系統1には系統基本周波数
fs の整数倍の周波数n×fs (nは1,2,…の整
数)の種々の高調波が存在し、これらの高調波に対し
て、高調波注入点aからみたその右側の下位(下流)の
等価回路13は、例えばノートンの定理で表現すると、
アドミタンス14と電流源15との並列回路とみなすこ
とができる。By the way, (the n 1, 2, ... integer) frequency n × f s is an integer multiple of the system fundamental frequency f s is in the power system 1 there are various harmonics, for these harmonics Thus, the equivalent circuit 13 on the lower side (downstream) on the right side of the harmonic injection point a can be expressed by, for example, Norton's theorem.
It can be regarded as a parallel circuit of the admittance 14 and the current source 15.
【0023】なお、電流源15は、通常、実際に電流源
が存在するのではなく、負荷による電流歪み等に起因し
て発生したものである。The current source 15 usually does not actually exist, but is generated due to current distortion or the like due to a load.
【0024】そして、例えば代表的な第5調波(n=
5),第7調波(n=7)を測定対象の高調波(着目高
調波)とし、この着目高調波についての等価回路13の
時々刻々変化する回路定数を求めてその高調波特性を測
定する場合、まず、電流注入装置6から高調波注入・計
測点aに、着目高調波の周波数の上,下近傍の系統基本
周波数の非整数倍周波数の複数の中間高調波の電流を個
別に注入する。Then, for example, a typical fifth harmonic (n =
5), the seventh harmonic (n = 7) is set as a harmonic to be measured (harmonic of interest), and a constantly changing circuit constant of the equivalent circuit 13 for the harmonic of interest is obtained, and its harmonic characteristics are determined. When measuring, first, currents of a plurality of intermediate harmonics of a non-integer multiple of the system fundamental frequency above and below the frequency of the target harmonic are individually applied to the harmonic injection / measurement point a from the current injection device 6. inject.
【0025】このとき、各中間高調波の電流は電力系統
1に本来存在しない周波数の電流であり、高調波注入・
計測点aからみたその下位側及び上位側の各中間高調波
についての等価回路は、理想的な場合、ノートンの定理
で表現すると、それぞれアドミタンスのみとなる。At this time, the current of each intermediate harmonic is a current of a frequency that does not originally exist in the power system 1,
In an ideal case, the equivalent circuit for each of the lower and upper intermediate harmonics from the measurement point a has only admittance when expressed by Norton's theorem.
【0026】そして、高調波注入・計測点aに注入され
た各中間高調波の電流は、その下位側及び上位側の各中
間高調波についてのアドミタンスに応じて下位側,上位
側に分流する。The current of each intermediate harmonic injected into the harmonic injection / measurement point a is divided into lower and upper sides according to the admittance of each of the lower and upper intermediate harmonics.
【0027】そのため、高調波注入・計測点aの各中間
高調波の注入電流I(m),注入電圧V(m)を注入ラインに
設けた計器用変流器16の計測電流,計器用変圧器17
の計測電圧から検出し、高調波注入・計測点aの上位に
分流した各中間高調波の電流Ix(m)を高調波注入・計測
点aの上位に測圧計器変流器18の計測電流から検出す
ると、高調波注入・計測点aの下位に分流した各中間高
調波の電流Iy(m)は、Iy(m)=I(m)−Ix(m)の演算か
ら求まる。For this reason, the injection current I ( m ) and the injection voltage V ( m ) of each intermediate harmonic at the harmonic injection / measurement point a are measured by the measurement current of the current transformer 16 provided on the injection line, Table 17
The current I x ( m ) of each intermediate harmonic shunted above the harmonic injection / measurement point a is detected by the pressure measuring instrument current transformer 18 above the harmonic injection / measurement point a. Upon detecting the current, the current I y of each intermediate harmonics diverted to a lower harmonic injection and measurement point a (m) is determined from the calculation of I y (m) = I ( m) -I x (m) .
【0028】そして、高調波注入・計測点aからみた各
中間高調波についての下位の等価回路のアドミタンスを
Yy(m)とすると、高調波注入・計測点aからみた下位及
び上位の各中間高調波の電圧がそれぞれの注入電圧
V(m)に等しくなることから、アドミタンスYy(m)はYy
(m)=(I(m)−Ix(m))/V(m)の演算から求まる。If the admittance of the lower equivalent circuit for each intermediate harmonic as viewed from the harmonic injection / measurement point a is Y y ( m ), the lower and upper intermediate circuits as viewed from the harmonic injection / measurement point a will be described. since the voltage of the higher harmonics is equal to the respective injection voltage V (m), admittance Y y (m) is Y y
(M) = obtained from calculation of (I (m) -I x ( m)) / V (m).
【0029】さらに、説明を簡単にするため、着目高調
波を挟むその上,下の2中間高調波についてのアドミタ
ンスYy(m)をY1(m),Y2(m)とすると、着目高調波につ
いての等価回路13のアドミタンス14が、最も簡単に
はY(n)=(Y1(m)+Y2(m))/2の補間演算からY(n)
として求まる。For the sake of simplicity, the admittances Y y ( m ) of the two intermediate harmonics above and below the harmonic of interest are denoted by Y 1 ( m ) and Y 2 ( m ). admittance 14 of the equivalent circuit 13 for the harmonics, the simplest Y (n) = (Y 1 (m) + Y 2 (m)) / 2 interpolation operation from Y (n)
Is obtained as
【0030】また、電流注入装置6の電流注入が終了し
た後、計器用変圧器17の計測電圧,計器用変流器18
の計測電流から配電母線4を下位方向に流れる着目高調
波の電圧V(n),電流I(n)を求めることにより、IG(n)
=Y(n)×V(n)−I(n)の演算から等価回路13の電流
源15がIG(n)として求まる。After the current injection by the current injection device 6 is completed, the measured voltage of the instrument transformer 17 and the current transformer 18 are measured.
Voltage from the measured current interest harmonics flowing distribution bus 4 in the downward direction V (n), by determining the current I (n), I G ( n)
= Current source 15 of the equivalent circuit 13 from the operation of Y (n) × V (n ) -I (n) is obtained as I G (n).
【0031】そして、着目高調波についての等価回路1
3のアドミタンス14,電流源15が求まると、高調波
注入・計測点aより下位の着目高調波についての特性を
測定して把握することができる。Then, an equivalent circuit 1 for the harmonic of interest
When the admittance 14 and the current source 15 of 3 are obtained, it is possible to measure and grasp the characteristic of the target harmonic lower than the harmonic injection / measurement point a.
【0032】そして、電流注入装置6は各中間高調波の
電流を設定時間ずつ連続的に順次に注入して高調波特性
の測定を短時間に終了するため、図1に示すように構成
され、低圧トランス5の低圧側に結合トランス19の第
1の巻線19aが接続され、この結合トランス19の第
2の巻線19bに電圧型のインバータ20が接続され
る。The current injection device 6 is configured as shown in FIG. 1 in order to sequentially and sequentially inject the current of each intermediate harmonic for a set time and finish the measurement of the harmonic characteristics in a short time. The first winding 19a of the coupling transformer 19 is connected to the low voltage side of the low voltage transformer 5, and the voltage type inverter 20 is connected to the second winding 19b of the coupling transformer 19.
【0033】このインバータ20は例えばタイマ動作に
より、ROM等のメモリに保持された各中間高調波の1
又は数周期のデータを設定された順に設定時間ずつ読出
し、読出したデータに基づき出力部のブリッジ構成の半
導体スイッチング素子を駆動し、図3に示すように連続
的に各中間高調波の周波数に変化するインバータ出力
(電圧出力)を形成する。なお、図3のt1 ,t2 はイ
ンバータ出力の周波数の変化タイミングを示す。The inverter 20 operates, for example, by a timer operation to generate one of the intermediate harmonics held in a memory such as a ROM.
Alternatively, data of several cycles are read out in a set time sequence for each set time, and based on the read data, a semiconductor switching element having a bridge configuration of an output unit is driven, and continuously changes to the frequency of each intermediate harmonic as shown in FIG. To generate an inverter output (voltage output). Note that t 1 and t 2 in FIG. 3 indicate timings at which the frequency of the inverter output changes.
【0034】そして、インバータ20の出力は、この形
態では、その電流が例えば12Aから60Aに増大する
ように、巻数比1:5のステップアップトランス21に
より変圧され、このトランス21を介した設定電流のイ
ンバータ出力がコンデンサ22,抵抗23,コイル24
の直列共振回路が形成するフィルタ部25を通って結合
トランス19の第3の巻線19cに供給される。In this embodiment, the output of the inverter 20 is transformed by a step-up transformer 21 with a turns ratio of 1: 5 so that the current increases from 12 A to 60 A, for example. Output of the capacitor 22, the resistor 23, the coil 24
Is supplied to the third winding 19c of the coupling transformer 19 through the filter unit 25 formed by the series resonance circuit of FIG.
【0035】このとき、本実施の形態にあっては、実際
の高調波計測に最も重要な第5調波又は第7調波を着目
高調波とし、その近傍周波数の各中間高調波の電流のみ
を結合トランス19,低圧トランス5を介して高調波注
入・計測点aに注入するため、フィルタ部25は共振点
が各中間高調波のほぼ中間の第6調波の前後に設定さ
れ、その共振特性がほぼ第5調波ないし第7調波の範囲
をカバーする平坦なQ特性に設定される。At this time, in the present embodiment, the fifth harmonic or the seventh harmonic, which is the most important for the actual harmonic measurement, is set as the target harmonic, and only the current of each intermediate harmonic near the target harmonic is measured. Is injected into the harmonic injection / measurement point a via the coupling transformer 19 and the low-voltage transformer 5, so that the resonance point of the filter unit 25 is set before and after the sixth harmonic, which is substantially intermediate between the intermediate harmonics. The characteristic is set to a flat Q characteristic covering substantially the range of the fifth to seventh harmonics.
【0036】そのため、低圧トランス5から高調波注入
点aに、不要な中間高調波の逓倍周波数成分を排除し
て、着目高調波を挟むその上下の各中間高調波の電流
が、途切れることなく設定時間ずつ順次に注入され、1
台の注入装置で短時間に測定が終了する。For this reason, unnecessary high frequency components of intermediate harmonics are eliminated from the low-voltage transformer 5 to the harmonic injection point a, and the current of each intermediate harmonic above and below the harmonic of interest is set without interruption. Injected sequentially by time, 1
The measurement is completed in a short time with one injection device.
【0037】したがって、インバータ20等は短時間定
格を満足すればよく、小容量,小型に形成することがで
きるとともに、それらの放熱フィンの省略等も図ること
ができる。Therefore, the inverter 20 and the like only need to satisfy the rating for a short time, can be formed with a small capacity and a small size, and can omit the radiation fins thereof.
【0038】しかも、フィルタ部25の直列共振回路の
コンデンサ22が電力系統1の商用周波数電圧(系統基
本波の電圧)を分担し、この点から、トランス19,2
1等の小容量,小型化を図ることができる。Moreover, the capacitor 22 of the series resonance circuit of the filter unit 25 shares the commercial frequency voltage (voltage of the system fundamental wave) of the power system 1, and from this point, the transformers 19, 2
It is possible to reduce the capacity and size of the first and the like.
【0039】そのため、電流注入装置6を小容量かつ小
型,軽量に形成することができ、可搬型の装置に形成す
ることも可能になる。Therefore, the current injection device 6 can be formed to have a small capacity, a small size, and a light weight, and can be formed as a portable device.
【0040】つぎに、電流注入装置6から高調波注入・
計測点aに注入された各中間高調波の電流に基づく高調
波特性の具体的な測定方法を説明する。Next, harmonic injection from the current injection device 6 is performed.
A specific method of measuring the harmonic characteristics based on the current of each intermediate harmonic injected into the measurement point a will be described.
【0041】まず、説明を簡単にするため、電流注入装
置6から高調波注入・計測点aに、着目高調波(周波数
n×fs )を挟むその上,下の2周波数f1 ,f2 (f
1 <n×fs <f2 )の中間高調波の電流Iy1(m),I
y2(m)(=Iyi(m),i=1,2)が順次に注入されて測
定が行われるとする。Firstly, in order to simplify the description, the current injection device 6 to harmonic injection and measurement points a, thereon sandwiching the interest harmonic (frequency n × f s), 2 frequency f 1 below, f 2 (F
1 <n × f s <intermediate harmonic currents I y1 of f 2) (m), I
It is assumed that measurement is performed by sequentially injecting y2 ( m ) (= Iyi ( m ), i = 1, 2).
【0042】この場合、電流Iy1(m),Iy2(m)それぞれ
の注入時、計器用変流器16により高調波注入・計測点
aの注入電流を計測し、かつ、計器用変圧器17,計器
用変流器18により高調波注入・計測点aの電圧(系統
電圧),その上位を流れる電流を計測し、それらの計測
信号を測定装置12のA/D変換器7によりそれぞれデ
ジタルの計測データに変換する。In this case, at the time of injecting each of the currents Iy 1 ( m ) and Iy 2 ( m ), the injection current at the harmonic injection / measurement point a is measured by the current transformer 16 for the instrument, and 17, the voltage at the harmonic injection / measurement point a (system voltage) and the current flowing therethrough are measured by the current transformer 18 for the instrument, and the measured signals are digitally converted by the A / D converter 7 of the measuring device 12. To the measured data.
【0043】さらに、A/D変換器7の各計測データを
信号処理装置8のFFT解析等により処理し、高調波注
入・計測点aに注入された電流I1(m),I2(m)(=Ii(
m),i=1,2)それぞれにつき、高調波注入・計測点
aの電圧V1(m),V2(m)(=Vi(m))及び高調波注入・
計測点aの上位への分流Ix1(m),Ix2(m)(=
Ixi(m),i=1,2)の計測結果を得る。Further, each measurement data of the A / D converter 7 is processed by FFT analysis or the like of the signal processing device 8, and the currents I 1 ( m ) and I 2 ( m ) injected into the harmonic injection / measurement point a. ) (= I i (
m ), i = 1, 2), the voltages V 1 ( m ) and V 2 ( m ) (= V i ( m )) at the harmonic injection / measurement point a and the harmonic injection /
The shunt I x1 ( m ), I x2 ( m ) (=
A measurement result of I xi ( m ), i = 1, 2) is obtained.
【0044】そして、信号処理装置8の計測出力を後段
の演算処理装置9に供給し、この処理装置9により、計
測された電流Ixi(m)に基づき、Iyi(m)=Ii(m)−Ixi
(m)の演算から高調波注入点aの下位への分流Iy1(m),
Iy2(m)を求め、Yyi(m)=Iyi(m)/Vi(m)の演算から
電流Iy1(m),Iy2(m)それぞれについてのアドミタンス
Yy1(m),Yy2(m)(=Yyi(m))を求める。Then, the measurement output of the signal processing device 8 is supplied to a subsequent processing device 9, and based on the measured current I xi ( m ), I yi ( m ) = I i ( m ) -I xi
From the calculation of ( m ), the shunt I y1 ( m ) to the lower order of the harmonic injection point a,
I y2 (m) asking, Y yi (m) = I yi (m) / V current from the calculation of i (m) I y1 (m ), I y2 (m) admittance Y y1 (m) for each, Y y2 ( m ) (= Y yi ( m )) is obtained.
【0045】このとき、電流Iyi(m)が電力系統1に存
在しない周波数の電流であるため、電流注入装置6の注
入電力量が微小であっても、アドミタンスYyi(m)は電
力系統1の高調波等の影響を受けることなく正確に求ま
る。At this time, since the current I yi ( m ) is a current having a frequency that does not exist in the power system 1, the admittance Y yi ( m ) is maintained even if the amount of power injected by the current injection device 6 is very small. It is accurately obtained without being affected by harmonics of 1 or the like.
【0046】なお、中間高調波の電流Ii(m)の代わりに
測定調波の高調波電流を注入しても、この高調波が電力
系統1に存在しているため、注入した高調波電流に基づ
くアドミタンスを求めることはできない。Even if the harmonic current of the measured harmonic is injected instead of the intermediate harmonic current I i ( m ), since this harmonic exists in the power system 1, the injected harmonic current is Admittance based on criterion cannot be sought.
【0047】また、高調波注入・計測点aの下位を流れ
る電流を計測し、その計測電流から電流Iyi(m)を求め
てもよい。Alternatively, the current flowing below the harmonic injection / measurement point a may be measured, and the current I yi ( m ) may be obtained from the measured current.
【0048】そして、演算処理装置9は例えばYy(n)=
(Yy1(m)+Yy2(m))/2の補間演算を実行し、高調波
注入・計測点aより下位の着目高調波についてのアドミ
タンスYy1(n)を求めて決定する。Then, the arithmetic processing unit 9 calculates, for example, Y y ( n ) =
An interpolation operation of (Y y1 ( m ) + Y y2 ( m )) / 2 is executed to determine and determine the admittance Y y1 ( n ) of the focused harmonic lower than the harmonic injection / measurement point a.
【0049】このとき、アドミタンスYy1(m),Yy2(m)
が電力系統1の高調波の影響を受けることなく正確に算
出されるため、着目高調波についてのアドミタンスYy(
n)(アドミタンス14)が正確に求まる。At this time, the admittances Y y1 ( m ) and Y y2 ( m )
Is accurately calculated without being affected by the harmonics of the power system 1, the admittance Y y (
n ) (admittance 14) is accurately obtained.
【0050】つぎに、電流注入装置6の電流注入の終了
直後、計器用変圧器17の計測電圧,計器用変流器18
の計測電流の周波数分析から系統母線4の着目高調波の
電圧V(n),下位方向の電流Iy(n)を求める。Next, immediately after the current injection by the current injection device 6 is completed, the measured voltage of the instrument transformer 17 and the current transformer 18 are measured.
Voltage of interest harmonics of the system bus 4 from the frequency analysis of the measured current V (n), obtains a lower direction of the current I y (n).
【0051】そして、アドミタンスYy(n)及び電圧
V(n),電流Iy(n)に基づき、IGy(n)=Yy(n)×V(n)
−Iy(n)の演算から電流源IGy(n)(電流源15)を求
め、等価回路13を同定して高調波注入・計測点aより
下位の着目高調波についての高調波特性の完全な測定を
行う。Then, based on the admittance Y y ( n ), the voltage V ( n ) and the current I y ( n ), I Gy ( n ) = Y y ( n ) × V ( n )
The current source I Gy ( n ) (current source 15) is obtained from the calculation of −I y ( n ), the equivalent circuit 13 is identified, and the harmonic characteristics of the target harmonic lower than the harmonic injection / measurement point a are obtained. Make a complete measurement of.
【0052】ところで、高調波注入・計測点aより上位
の高調波特性も、前記と同様にして同時に測定すること
ができる。Incidentally, the higher harmonic characteristics than the higher harmonic injection / measurement point a can be simultaneously measured in the same manner as described above.
【0053】この場合、計測電流Ixi(m),計測電圧V(
m)に基づいて得られた中間高調波の分流Ix1(m),Ix2(
m)(=Ixi(m))から、高調波注入・計測点aの上位の
中間調 波についてのアドミタンスYx1(m),Yx2(m)
(=Yxi(m))はYxi(m)=Ixi(m) /Vi(m)の演算によ
り求まる。In this case, the measurement current I xi ( m ) and the measurement voltage V (
m ), I x1 ( m ), I x2 (
m ) (= I xi ( m )), the admittances Y x1 ( m ) and Y x2 ( m ) of the intermediate harmonic higher than the harmonic injection / measurement point a
(= Y xi ( m )) is obtained by the calculation of Y xi ( m ) = I xi ( m ) / V i ( m ).
【0054】また、Yx(n)=(Yx1(m)+Yx2(m))/2
の補間演算から、アドミタンスYy(n)と同様の高調波注
入・計測点aより上位の着目高調波についての等価回路
のアドミタンスYx(n)が求まる。Further, Y x ( n ) = (Y x1 ( m ) + Y x2 ( m )) / 2
From interpolation operation, admittance Y y admittance of an equivalent circuit of the interest harmonics higher than a similar harmonic injection and measurement points a and (n) Y x (n) is obtained.
【0055】さらに、アドミタンスYx(n)及び電圧
V(n),電流Ix(n)に基づき、IGx(n)=Yx(n)×V(n)
+Ix(n)の演算から、電流源15と同様の高調波注入点
aより上位 の着目高調波についての等価回路の電流源
IGx(n)が求まる。Further, based on the admittance Y x ( n ), the voltage V ( n ), and the current I x ( n ), I Gx ( n ) = Y x ( n ) × V ( n )
From the calculation of + I x ( n ), the current source IGx ( n ) of the equivalent circuit for the target harmonic higher than the harmonic injection point a similar to the current source 15 is obtained.
【0056】そして、アドミタンスYx(n),電流源IGx
(n)により、等価回路13と同様の高調波注入・計測点
aより上位の着目高調波についての等価回路を同定し、
高調波注入・計測点aより上位の高調波特性を測定でき
る。The admittance Y x ( n ) and the current source I Gx
( n ), an equivalent circuit for the focused harmonic higher than the harmonic injection / measurement point a similar to the equivalent circuit 13 is identified,
Higher harmonic characteristics higher than the harmonic injection / measurement point a can be measured.
【0057】つぎに、前記実施の形態においては、高調
波注入・計測点aを高調波の注入と計測とに兼用した
が、高調波注入点と高調波計測点とを別個に設定にし、
高調波注入点に電流注入装置6を接続し、高調波計測点
側に計器用変圧器17,計器用変流器18を設け、高調
波計測点より下位,上位の着目高調波についての等価回
路を同定して高調波特性を測定してもよく、この場合、
電流注入装置を小型,軽量にして可搬性を向上すること
により、高調波注入点への電流注入装置の運搬等が極め
て容易に行える利点がある。Next, in the above embodiment, the harmonic injection / measurement point a is used for both injection and measurement of the harmonic, but the harmonic injection point and the harmonic measurement point are set separately.
The current injection device 6 is connected to the harmonic injection point, an instrument transformer 17 and an instrument current transformer 18 are provided on the harmonic measurement point side, and an equivalent circuit for the target harmonic lower and higher than the harmonic measurement point is provided. May be identified to measure the harmonic characteristics. In this case,
By improving the portability by reducing the size and weight of the current injection device, there is an advantage that the current injection device can be transported to the harmonic injection point very easily.
【0058】また、高調波計測点と高調波注入点とを別
個に設ける場合、高調波注入点を系統の分枝した各母線
等に複数設定して電流注入装置6を複数にし、各電流注
入装置6から各中間高調波の電流を注入して高調波特性
を測定することができ、この場合は、各電流注入装置6
が一層小型,軽量になる利点がある。When a harmonic measuring point and a harmonic injection point are separately provided, a plurality of harmonic injection points are set on each of the buses or the like branched in the system, and a plurality of current injection devices 6 are provided. The harmonic characteristic can be measured by injecting the current of each intermediate harmonic from the device 6, and in this case, the current injection device 6
However, there is an advantage that it becomes smaller and lighter.
【0059】そして、高調波注入点及び高調波計測点の
数や位置等をどのように設定した場合にも本発明を適用
することができるのは勿論である。The present invention can of course be applied to any case where the number and position of the harmonic injection points and the harmonic measurement points are set.
【0060】つぎに、例えば着目高調波の上,下の中間
高調波をそれぞれ複数にする場合や複数の着目高調波に
ついて一括して測定する場合には、インバータ20の出
力周波数を3種以上の多数の周波数に連続的に切換るよ
うにすればよいのは勿論である。Next, for example, when a plurality of intermediate harmonics above and below the target harmonic are respectively provided, or when a plurality of target harmonics are collectively measured, the output frequency of the inverter 20 is set to three or more types. Of course, it is only necessary to continuously switch to a large number of frequencies.
【0061】つぎに、インバータ20は出力周波数がタ
イマ制御等で設定された各中間高調波の周波数に連続的
に変化するものであれば、どのような構成であってもよ
い。The inverter 20 may have any configuration as long as the output frequency continuously changes to the frequency of each intermediate harmonic set by timer control or the like.
【0062】また、インバータ20の後段のステップア
ップトランス21は、インバータ20の出力電流が十分
大きいような場合は省くことができる。The step-up transformer 21 after the inverter 20 can be omitted when the output current of the inverter 20 is sufficiently large.
【0063】さらに、直列共振回路25の共振特性は、
取出す中間高調波の周波数範囲等に応じて設定すればよ
く、各中間高調波の電流が極力同じ共振特性で抽出され
るように、必要な周波数範囲でいわゆるQ値が平坦であ
ることが望ましい。Further, the resonance characteristics of the series resonance circuit 25 are as follows.
What is necessary is just to set according to the frequency range of the extracted intermediate harmonic, etc., and it is desirable that the so-called Q value is flat in the required frequency range so that the current of each intermediate harmonic is extracted with the same resonance characteristics as much as possible.
【0064】つぎに、等価回路13等をアドミタンスと
電流源との並列回路とする代わりに、インピーダンスと
電圧源との直列回路として高調波特性を測定する場合に
も同様に適用することができるのは勿論である。Next, instead of using the equivalent circuit 13 or the like as a parallel circuit of admittance and a current source, the present invention can be similarly applied to a case where a harmonic characteristic is measured as a series circuit of an impedance and a voltage source. Of course.
【0065】[0065]
【発明の効果】本発明は、以下に記載する効果を奏す
る。インバータ20の出力が連続的に各中間高調波の周
波数に変化する。そして、インバータ20の各中間高調
波の周波数成分にフィルタ部25が共振し、この共振に
よる周波数の選択に基づき、フィルタ部25により系統
基本周波数の成分や各中間高調波の逓倍周波数の成分等
の不要な周波数成分を排除してインバータ20の出力か
ら各中間高調波の電流を抽出することができる。The present invention has the following effects. The output of the inverter 20 continuously changes to the frequency of each intermediate harmonic. Then, the filter unit 25 resonates with the frequency component of each intermediate harmonic of the inverter 20, and based on the selection of the frequency by this resonance, the filter unit 25 causes the component of the system fundamental frequency, the component of the multiplied frequency of each intermediate harmonic, and the like. Unnecessary frequency components can be eliminated, and the current of each intermediate harmonic can be extracted from the output of the inverter 20.
【0066】さらに、フィルタ部25の各中間高調波の
電流を結合トランス19を介して系統に注入することが
できる。Further, the current of each intermediate harmonic of the filter unit 25 can be injected into the system via the coupling transformer 19.
【0067】この場合、各中間高調波の電流を1台の電
流注入装置6から系統に注入することができる。In this case, the current of each intermediate harmonic can be injected from one current injection device 6 into the system.
【0068】しかも、この電流注入装置6の出力が各中
間高調波の周波数に連続的に変化し、各中間高調波の電
流の注入が短時間に終了するため、電流注入装置6はい
わゆる短時間定格を満足すればよく、小容量,小型に形
成することができる。Moreover, the output of the current injection device 6 continuously changes to the frequency of each intermediate harmonic, and the injection of the current of each intermediate harmonic is completed in a short time. It suffices to satisfy the rating, and it can be formed with small capacity and small size.
【0069】したがって、小容量で小型の電流注入装置
6により、精度の高い高調波特性の測定が行える。Therefore, the high-accuracy harmonic characteristics can be measured by the small-capacity and small-sized current injection device 6.
【図1】本発明の実施の1形態の回路結線図である。FIG. 1 is a circuit connection diagram according to an embodiment of the present invention.
【図2】図1の電流注入装置を用いた高調波測定の1例
の回路結線図である。FIG. 2 is a circuit connection diagram of an example of harmonic measurement using the current injection device of FIG.
【図3】図1のインバータの出力波形図である。FIG. 3 is an output waveform diagram of the inverter of FIG. 1;
1 電力系統 19 結合トランス 20 インバータ 25 フィルタ部 DESCRIPTION OF SYMBOLS 1 Power system 19 Coupling transformer 20 Inverter 25 Filter part
───────────────────────────────────────────────────── フロントページの続き (72)発明者 西村 荘治 京都市右京区梅津高畝町47番地 日新電機 株式会社内 (72)発明者 夏田 育千 京都市右京区梅津高畝町47番地 日新電機 株式会社内 (72)発明者 蓑輪 義文 京都市右京区梅津高畝町47番地 日新電機 株式会社内 ──────────────────────────────────────────────────続 き Continuing on the front page (72) Inventor Shoji Nishimura, 47, Takane-cho, Umezu, Ukyo-ku, Kyoto-shi Inside Nisshin Electric Co., Ltd. (72) Inventor Yoshifumi Minowa 47, Umezu Takaune-cho, Ukyo-ku, Kyoto-shi Nissin Electric Co., Ltd.
Claims (1)
本周波数の非整数倍の周波数の電流を中間高調波の電流
としてそれぞれ注入し、系統の計測電流,計測電圧の周
波数解析により系統の前記各中間高調波の電流,電圧を
検出して系統の前記各中間高調波についての等価回路の
アドミタンス又はインピーダンスを求め、該各等価回路
のアドミタンス又はインピーダンスから着目高調波につ
いての系統の等価回路のアドミタンス又はインピーダン
スを補間演算して決定し、系統の前記測定対象の高調波
についての高調波特性を測定する際に、系統に前記各中
間高調波の電流を注入する高調波測定用の電流注入装置
において、 出力周波数が前記各中間高調波の周波数に連続的に変化
するインバータと、 前記各中間高調波のほぼ中間に共振点を設定した共振回
路からなり、前記インバータの出力から前記各中間高調
波の電流を出力するフィルタ部と、 該フィルタ部から出力された前記各中間高調波の電流を
系統に注入する結合トランスとを備えたことを特徴とす
る高調波測定用の電流注入装置。1. A current having a frequency that is a non-integer multiple of the system fundamental frequency above and below the harmonic to be measured is injected into the system as an intermediate harmonic current, and the measured current and measured voltage of the system are analyzed by frequency analysis. The admittance or impedance of the equivalent circuit for each of the intermediate harmonics of the system is determined by detecting the current and voltage of each of the intermediate harmonics, and the equivalent circuit of the system for the target harmonic is determined from the admittance or impedance of each of the equivalent circuits. The admittance or impedance is determined by interpolation, and when measuring the harmonic characteristics of the harmonics to be measured in the system, the current injection for harmonic measurement is performed by injecting the current of each intermediate harmonic into the system. In the device, an inverter whose output frequency continuously changes to the frequency of each of the intermediate harmonics, and a resonance point is set substantially at the center of each of the intermediate harmonics. And a coupling transformer for injecting the current of each of the intermediate harmonics output from the filter unit into a system. A current injection device for measuring harmonics.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
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JP19780997A JP2940604B2 (en) | 1997-07-07 | 1997-07-07 | Current injection device for harmonic measurement |
US09/110,997 US6326796B1 (en) | 1997-07-07 | 1998-07-06 | Harmonic measuring method and a current injection device for harmonic measurement |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
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JP19780997A JP2940604B2 (en) | 1997-07-07 | 1997-07-07 | Current injection device for harmonic measurement |
Publications (2)
Publication Number | Publication Date |
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JPH1123626A true JPH1123626A (en) | 1999-01-29 |
JP2940604B2 JP2940604B2 (en) | 1999-08-25 |
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JP19780997A Expired - Fee Related JP2940604B2 (en) | 1997-07-07 | 1997-07-07 | Current injection device for harmonic measurement |
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Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100748492B1 (en) * | 2001-02-13 | 2007-08-13 | 엘지전자 주식회사 | Initialization method for phase change type optical disc |
CN102791805A (en) * | 2010-03-15 | 2012-11-21 | 大正制药株式会社 | Pigment composition |
CN110208602A (en) * | 2019-06-06 | 2019-09-06 | 福州大学 | One kind being conducive to transformer ultra harmonics transmission characteristic counting circuit and its calculation method |
CN111537794A (en) * | 2020-05-21 | 2020-08-14 | 国网江苏省电力有限公司电力科学研究院 | Topological system, control method and storage medium of three-port impedance frequency sweeping device |
-
1997
- 1997-07-07 JP JP19780997A patent/JP2940604B2/en not_active Expired - Fee Related
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100748492B1 (en) * | 2001-02-13 | 2007-08-13 | 엘지전자 주식회사 | Initialization method for phase change type optical disc |
CN102791805A (en) * | 2010-03-15 | 2012-11-21 | 大正制药株式会社 | Pigment composition |
CN110208602A (en) * | 2019-06-06 | 2019-09-06 | 福州大学 | One kind being conducive to transformer ultra harmonics transmission characteristic counting circuit and its calculation method |
CN111537794A (en) * | 2020-05-21 | 2020-08-14 | 国网江苏省电力有限公司电力科学研究院 | Topological system, control method and storage medium of three-port impedance frequency sweeping device |
CN111537794B (en) * | 2020-05-21 | 2023-02-28 | 国网江苏省电力有限公司电力科学研究院 | Topological system, control method and storage medium of three-port impedance frequency sweeping device |
Also Published As
Publication number | Publication date |
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JP2940604B2 (en) | 1999-08-25 |
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