JPH1114675A - Power system harmonic measurement method - Google Patents

Power system harmonic measurement method

Info

Publication number
JPH1114675A
JPH1114675A JP9180573A JP18057397A JPH1114675A JP H1114675 A JPH1114675 A JP H1114675A JP 9180573 A JP9180573 A JP 9180573A JP 18057397 A JP18057397 A JP 18057397A JP H1114675 A JPH1114675 A JP H1114675A
Authority
JP
Japan
Prior art keywords
harmonic
injection
current
measurement
power system
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.)
Pending
Application number
JP9180573A
Other languages
Japanese (ja)
Inventor
Isao Koda
勲 香田
Masakazu Tsukamoto
政和 塚本
Soji Nishimura
荘治 西村
Yasukazu Natsuda
育千 夏田
Toshihiko Shikata
俊彦 志方
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Chubu Electric Power Co Inc
Nissin Electric Co Ltd
Original Assignee
Chubu Electric Power Co Inc
Nissin Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Chubu Electric Power Co Inc, Nissin Electric Co Ltd filed Critical Chubu Electric Power Co Inc
Priority to JP9180573A priority Critical patent/JPH1114675A/en
Priority to US09/099,381 priority patent/US6208945B1/en
Publication of JPH1114675A publication Critical patent/JPH1114675A/en
Pending legal-status Critical Current

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Classifications

    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/40Arrangements for reducing harmonics

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  • Supply And Distribution Of Alternating Current (AREA)

Abstract

(57)【要約】 【課題】 電力系統に基本波の非整数倍周波数の電流を
注入して測定結果から測定調波についてのアドミタンス
を求める際に、注入電流量を電力系統の負荷に悪影響を
与えない最適量に設定して正確に求め得るようにする。 【解決手段】 電力系統1の注入点4に、測定調波の
上,下両側それぞれの基本波の非整数倍周波数の電流を
徐々に増加しながら注入し、注入電流に基づく注入点4
の注入周波数の歪み電圧がほぼ所定の上限電圧に上昇し
たときに注入電流の増加を停止して高調波測定に移行
し、測定調波の上,下両側それぞれの注入電流に基づく
注入点4の電圧及び注入点4より上位,下位の少なくと
も一方の電流の計測結果から系統1の注目側の注入電流
についての等価回路のアドミタンスを算出し、測定調波
の上,下両側の注入電流についての算出したアドミタン
スに基づく補間処理により、注目側の測定調波について
の等価回路のアドミタンスを求めて決定する。
(57) [Summary] [PROBLEMS] To determine the admittance of a measured harmonic from a measurement result by injecting a current of a non-integer multiple frequency of a fundamental wave into a power system, the amount of injected current has an adverse effect on a load of the power system. Set the optimum amount not to be given so that it can be obtained accurately. SOLUTION: A current of a non-integer multiple frequency of a fundamental wave of each of upper and lower sides of a measurement harmonic is injected into an injection point 4 of a power system 1 while gradually increasing the current, and the injection point 4 based on the injection current is obtained.
When the distortion voltage at the injection frequency rises to a substantially predetermined upper limit voltage, the injection current stops increasing, and the operation shifts to harmonic measurement, where the injection point 4 based on the injection current on both the upper and lower sides of the measurement harmonic is measured. The admittance of an equivalent circuit for the injection current on the target side of the system 1 is calculated from the measurement result of the voltage and at least one of the currents higher and lower than the injection point 4, and the injection currents on the upper and lower sides of the measurement harmonic are calculated. The admittance of the equivalent circuit for the measured harmonic on the side of interest is obtained and determined by interpolation processing based on the admittance obtained.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、電力系統の高調波
(測定調波)についてのアドミタンス又は等価回路を求
める電力系統の高調波測定方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method of measuring harmonics of a power system for obtaining an admittance or an equivalent circuit of a harmonic (measurement harmonic) of the power system.

【0002】[0002]

【従来の技術】電力系統の送,配電系統等の高調波抑制
技術においては、高調波ロスを利用したいわゆる系統切
り換え技術により高調波を低減することが、重要視され
てきた。
2. Description of the Related Art In a technique for suppressing harmonics in power transmission and distribution systems of a power system, it has been regarded as important to reduce harmonics by a so-called system switching technique utilizing harmonic loss.

【0003】そして、系統切り換え等によって生じる高
調波の周波数は、系統電源の基本波の周波数fsの整数
倍であり、代表的な第5調波(5次高調波)の周波数は
5・fsである。
The frequency of a harmonic generated by system switching or the like is an integer multiple of the frequency fs of the fundamental wave of the system power supply, and the typical frequency of the fifth harmonic (fifth harmonic) is 5 · fs. is there.

【0004】また、高調波の低減はコンデンサ設備に付
属するフィルタ設備により、高調波の電圧レベルの予測
等に基づき、そのフィルタを設置して行われる。
[0004] The reduction of harmonics is performed by installing a filter based on prediction of the voltage level of the harmonics by a filter facility attached to the capacitor facility.

【0005】このとき、高調波の電圧レベルの予測等を
行うには、電力系統のフィルタ設備の接続点より上位
(上流),下位(下流)の高調波に対する特性を把握し
てその等価回路を求める必要がある。
At this time, in order to predict the voltage level of the harmonic, for example, the characteristics of the higher (upstream) and lower (downstream) harmonics from the connection point of the filter equipment of the power system are grasped, and the equivalent circuit thereof is determined. Need to ask.

【0006】この等価回路は、一般に、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、そのうちのア
ドミタンスが特性の把握の上からは最も重要である。
This equivalent circuit can be generally regarded as a parallel circuit of an admittance and a current source, of which the admittance is the most important from the viewpoint of the characteristics.

【0007】そして、電気学会論文誌B,101巻8
号,p.451−458,(昭56−8)には、配電線
の第5調波についての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に対する
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 Transactions of the Institute of Electrical Engineers of Japan, B, 101, 8
No., p. 451-458, (Showa 56-8) discloses that when obtaining an equivalent circuit for the fifth harmonic of a distribution line, the voltage and current of the fundamental wave of the system are measured, and the admittance of the equivalent circuit with respect to harmonics is obtained from the results. , The size and phase of the current source are calculated and estimated.

【0008】[0008]

【発明が解決しようとする課題】前記文献等に記載のよ
うに電力系統の高調波についての等価回路をその基本波
についての電圧,電流の計測結果で求める場合、精度よ
く求めることができない問題点がある。
As described in the above-mentioned documents and the like, when an equivalent circuit for harmonics of a power system is obtained from the measurement results of the voltage and current of the fundamental wave, it cannot be obtained with high accuracy. There is.

【0009】なお、例えば前記フィルタ装置の接続点に
基本波(周波数fs)の整数倍周波数n・fs(nは整
数)の高調波の電流を注入し、そのときの系統各所の電
流,電圧等の計測結果からその高調波についての等価回
路を求めようとしても、電力系統にその高調波が存在す
るため、注入した高調波変化に基づく電流,電圧等の変
化を明確にすることができず、その高調波についての電
力系統のアドミタンスや等価回路を正確に求めることが
できなかった。
[0009] For example, a harmonic current of an integral multiple frequency n · fs (n is an integer) of a fundamental wave (frequency fs) is injected into a connection point of the filter device, and current, voltage, etc. at various points in the system at that time. Even when trying to find an equivalent circuit for the higher harmonics from the measurement results, since the higher harmonics exist in the power system, it is not possible to clarify changes in current, voltage, etc. based on changes in the injected harmonics. The admittance and the equivalent circuit of the power system with respect to the harmonic cannot be obtained accurately.

【0010】したがって、従来は電力系統の前記フィル
タ装置の接続点等の上位,下位の高調波についてのアド
ミタンスや等価回路を個別に精度よく求めることができ
ず、この結果、系統切り換え等の際の高調波の電圧レベ
ルの精度の高い予測ができなかった。
Therefore, conventionally, it is not possible to individually and accurately obtain the admittance and the equivalent circuit for the higher and lower harmonics such as the connection point of the filter device in the power system, and as a result, when switching the system, etc. Precise prediction of the voltage level of harmonics could not be made.

【0011】ところで、n次高調波を測定調波とする
と、電力系統(実系統)には、本来、測定調波の上,下
両側の基本波の非整数倍周波数の成分が存在しないた
め、これらの周波数の電流の注入に基づく測定結果か
ら、つぎのようにして電力系統の測定調波についてのア
ドミタンスや等価回路を求めることが考えられる。
By the way, assuming that the n-th harmonic is the measurement harmonic, the power system (real system) does not originally have a non-integer multiple frequency component of the fundamental wave above and below the measurement harmonic. From the measurement results based on the injection of the currents at these frequencies, it is conceivable to determine the admittance and the equivalent circuit for the measured harmonics of the power system as follows.

【0012】すなわち、測定調波の上,下両側の基本波
の非整数倍周波数の電流を電力系統に注入し、その測定
の結果から電力系統の測定調波の上,下両側での注入電
流についての等価回路のアドミタンスを求める。
That is, a current having a frequency that is a non-integer multiple of the fundamental wave on both the upper and lower sides of the measured harmonic is injected into the power system, and based on the measurement result, the injected current on the upper and lower sides of the measured harmonic of the power system is measured. Find the admittance of the equivalent circuit for.

【0013】そして、この測定調波の上,下両側でのア
ドミタンスに平均等の補間処理を施し、その中間の測定
調波についての電力系統のアドミタンスを求める。
Then, the admittance on both the upper and lower sides of the measured harmonic is subjected to interpolation processing such as averaging, and the admittance of the power system for the intermediate measured harmonic is obtained.

【0014】さらに、等価回路を求めるときは、求めた
アドミタンスと電力系統の測定調波についての電流,電
圧の測定結果とにより、電力系統の測定調波についての
電流源を求め、アドミタンスと電流源との並列回路から
なる等価回路を求める。
Further, when obtaining an equivalent circuit, a current source for the measured harmonics of the power system is obtained from the obtained admittance and the measurement results of the current and the voltage for the measured harmonics of the power system, and the admittance and the current source are obtained. To find an equivalent circuit consisting of a parallel circuit with

【0015】この場合、基本波の非整数倍周波数の電流
についての電力系統のアドミタンスが測定結果から正確
に求まるため、測定調波についてのアドミタンスや等価
回路を正確に求めることができる。
In this case, the admittance of the power system with respect to the current having a non-integer multiple frequency of the fundamental wave is accurately obtained from the measurement result, so that the admittance and the equivalent circuit of the measured harmonic can be accurately obtained.

【0016】ところで、測定精度等の面からは、前記基
本波の非整数倍周波数の電流の注入量を多くすることが
望ましいが、電力系統の負荷条件が系統や時間帯等によ
って異なり、注入量を適切に設定することは極めて困難
である。
From the viewpoint of measurement accuracy and the like, it is desirable to increase the amount of current injection at a frequency that is a non-integer multiple of the fundamental wave. However, the load conditions of the power system differ depending on the system, time zone, and the like. It is extremely difficult to properly set.

【0017】そして、適当に設定した一定量(設定量)
の電流を電力系統に注入して測定するのみでは、前記負
荷条件の変化にしたがって、電力系統の注入周波数に対
する電圧歪みの程度が変わるため、場合によっては注入
不足になって所期の精度で測定できない事態が生じる。
Then, an appropriately set constant amount (set amount)
Simply injecting the current into the power system and measuring it, the degree of voltage distortion with respect to the injection frequency of the power system changes according to the change in the load condition, and in some cases, the injection becomes insufficient and the measurement is performed with the desired accuracy. The situation that cannot be done arises.

【0018】さらに、注入周波数が電力系統の共振点に
一致又は近接していれば、注入に基づく電力系統の歪み
電圧が共振によって著しく拡大されるため、電力系統に
前記基本波の非整数倍周波数の過大な歪み電圧が生じ、
電力系統の負荷に悪影響を与えるおそれがある。
Further, if the injection frequency coincides with or is close to the resonance point of the power system, the distortion voltage of the power system due to the injection is significantly increased by the resonance. Causes an excessive distortion voltage of
The load on the power system may be adversely affected.

【0019】そして、電力系統の負荷条件は時々刻々変
化して不明であり、その共振周波数を把握することがで
きないため、前記基本波の非整数倍周波数の電流を電力
系統の負荷に悪影響を与えない最適量注入し、その測定
結果から測定調波についてのアドミタンスや等価回路を
正確に求めることができない。
Since the load condition of the power system changes every moment and is unknown and its resonance frequency cannot be grasped, the current of a non-integer multiple frequency of the fundamental wave adversely affects the load of the power system. It is not possible to accurately determine the admittance and the equivalent circuit of the measured harmonic from the measurement result obtained by injecting no optimal amount.

【0020】本発明は、測定調波の上,下両側の基本波
の非整数倍周波数の電流の注入量を、電力系統の負荷に
悪影響を与えない最適量に設定し、その注入結果から測
定調波についてのアドミタンスや等価回路が正確に求め
られるようにすることを課題とする。
According to the present invention, the injection amount of the current having a non-integer multiple frequency of the fundamental wave on the upper and lower sides of the measurement harmonic is set to an optimum amount which does not adversely affect the load on the power system, and the measurement is performed from the injection result. It is an object to accurately determine an admittance and an equivalent circuit for harmonics.

【0021】[0021]

【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、この出願の請求項1の電力系統の高調波測定方法
においては、電力系統の基本波の整数倍周波数の高調波
を測定調波とし、電力系統の高調波注入点に、測定調波
の上,下両側それぞれの基本波の非整数倍周波数の電流
を、徐々に増加しながら注入し、測定調波の上,下両側
それぞれの注入電流に基づく高調波注入点の注入周波数
の歪み電圧を計測し、この歪み電圧がほぼ所定の上限電
圧に上昇したときに注入電流の増加を停止して高調波測
定に移行し、測定調波の上,下両側それぞれの注入電流
に基づく高調波注入点の電圧及び電力系統の高調波注入
点より上位,下位の少なくとも一方の電流の計測結果か
ら前記上位,前記下位の少なくとも一方からなる電力系
統の注目側の測定調波の上,下両側の注入電流について
の等価回路のアドミタンスを算出し、測定調波の上,下
両側の注入電流についての算出したアドミタンスに基づ
く補間処理により、注目側の測定調波についての等価回
路のアドミタンスを求めて決定する。
In order to solve the above-mentioned problems, a method for measuring harmonics of a power system according to claim 1 of the present application measures harmonics of an integral multiple of a fundamental wave of a power system. Inject into the power system harmonic injection point currents at non-integer multiples of the fundamental wave on each of the upper and lower sides of the measurement harmonic, while gradually increasing the current. The distortion voltage at the injection frequency at the harmonic injection point based on the injection current is measured, and when the distortion voltage rises to a substantially predetermined upper limit voltage, the injection current stops increasing, and the operation shifts to harmonic measurement. From the measurement results of the voltage at the harmonic injection point based on the injection currents on both the upper and lower sides of the wave and at least one of the currents higher and lower than the harmonic injection point of the power system, the power consisting of the upper and / or lower power Measurement of the line of interest Calculate the admittance of the equivalent circuit for the injection currents on both the upper and lower sides of the wave, and perform interpolation processing based on the calculated admittances for the injection currents on the upper and lower sides of the measurement harmonic to obtain the equivalent of the measured harmonics on the target side. Determined for admittance of the circuit.

【0022】したがって、測定調波の上,下両側それぞ
れの基本波の非整数倍周波数の電流が、徐々に増加しな
がら電力系統に注入してその注入周波数の歪み電圧を計
測することのくり返しに基づき、事前に、電力系統に過
大な歪み電圧が発生する直前の電流量,すなわち注入に
よって電力系統の負荷に悪影響を与えない最適注入量に
設定される。
Therefore, the current of a non-integer multiple frequency of the fundamental wave on each of the upper and lower sides of the measured harmonic is gradually increased and injected into the power system to repeatedly measure the distortion voltage at the injected frequency. Based on this, the current amount immediately before the generation of an excessive distortion voltage in the power system, that is, the optimum injection amount that does not adversely affect the load of the power system due to the injection is set.

【0023】そして、この最適注入量の電流注入によ
り、電力系統の負荷に悪影響を与えることなく、測定調
波の上,下両側それぞれの基本波の非整数倍周波数の注
入電流についての電力系統の注目側のアドミタンスが精
度よく求まり、この結果から注目側の測定調波について
のアドミタンスが正確に求まる。
The current injection at the optimum injection amount does not adversely affect the load on the power system, and the power system is capable of injecting a non-integer multiple frequency of the fundamental wave on each of the upper and lower sides of the measured harmonic. The admittance of the attention side is accurately determined, and the admittance of the measurement harmonic of the attention side is accurately determined from the result.

【0024】また、請求項2に係る電力系統の高調波測
定方法においては、電力系統の基本波の整数倍周波数の
高調波を測定調波とし、電力系統の高調波注入点に、測
定調波の上,下両側それぞれの基本波の非整数倍周波数
の電流を徐々に増加しながら注入し、測定調波の上,下
両側それぞれの注入電流に基づく高調波注入点の注入周
波数の歪み電圧を計測し、この歪み電圧がほぼ所定の上
限電圧に上昇したときに注入電流の増加を停止して高調
波測定に移行し、測定調波の上,下両側それぞれの注入
電流に基づく高調波注入点の電圧及び電力系統の高調波
注入点より上位,下位の少なくとも一方の電流の計測結
果から前記上位,前記下位の少なくとも一方からなる電
力系統の注目側の測定調波の上,下両側の注入電流につ
いての等価回路のアドミタンスを算出し、測定調波の
上,下両側の前記注入電流についての算出したアドミタ
ンスに基づく補間処理により、注目側の測定調波につい
ての等価回路のアドミタンスを求めて決定し、この決定
したアドミタンスと,高調波注入点の電力系統の測定調
波の電圧及び電流の計測結果とにより、注目側の測定調
波についての等価回路の電流源を求めて決定し、決定し
たアドミタンスと電流源との並列回路により注目側の測
定調波についての等価回路を求める。
According to a second aspect of the present invention, there is provided a method for measuring harmonics in an electric power system, wherein a harmonic having an integral multiple of a fundamental wave of the electric power system is used as a measurement harmonic, and the measured harmonic is added to a harmonic injection point of the electric power system. The current at a non-integer multiple of the fundamental wave on each of the upper and lower sides is gradually increased and injected, and the distortion voltage of the injection frequency at the harmonic injection point based on the injected current on the upper and lower sides of the measured harmonic is reduced. When the distortion voltage rises to a predetermined upper limit voltage, the injection current stops increasing, and the operation shifts to harmonic measurement. The harmonic injection point is based on the injection current at both the upper and lower sides of the measured harmonic. From the measurement results of at least one of the higher and lower currents of the voltage and the harmonic injection point of the power system, the injection currents on the upper and lower sides of the measurement harmonic on the attention side of the power system consisting of the upper and lower ones About the equivalent circuit The admittance of the equivalent circuit for the measured harmonic on the side of interest is determined and determined by interpolation processing based on the calculated admittance of the injection current on the upper and lower sides of the measured harmonic by calculating the dominance and determining the admittance. Based on the measurement results of the voltage and current of the measured harmonic of the power system at the harmonic injection point, the current source of the equivalent circuit for the measured harmonic of interest is determined and determined, and the admittance between the determined admittance and the current source is determined. An equivalent circuit for the measured harmonic on the side of interest is determined by a parallel circuit.

【0025】したがって、この場合は、請求項1の場合
と同様にして求めた電力系統の注目側の測定調波につい
てのアドミタンスと、電力系統の測定調波の電圧,電流
の計測結果とにより、電力系統の注目側の前記アドミタ
ンスに並列な測定調波の電流源が求められ、電力系統の
注目側のアドミタンスと電流源との並列回路からなる測
定調波についての等価回路が、電力系統の負荷に悪影響
を与えることなく、正確に求められる。
Therefore, in this case, the admittance of the measured harmonic on the target side of the power system obtained in the same manner as in claim 1 and the measurement results of the voltage and current of the measured harmonic of the power system are obtained by: A current source of the measurement harmonic in parallel with the admittance on the power system's attention side is required, and an equivalent circuit for the measurement harmonic consisting of a parallel circuit of the admittance and the current source on the power system's attention side is a load of the power system. Is accurately determined without adversely affecting the system.

【0026】[0026]

【発明の実施の形態】本発明の実施の1形態につき、図
1ないし図6を参照して説明する。電力系統の高調波等
価回路を測定する際は、図1に示すように、電力系統1
の系統電源2と負荷3との間の適当な位置,例えば高調
波電流低減用のフィルタ装置が接続される位置を高調波
注入点4とし、この注入点4にマイクロコンピュータ構
成の計測装置5からの電流を注入する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described with reference to FIGS. When measuring the harmonic equivalent circuit of the power system, as shown in FIG.
An appropriate position between the system power supply 2 and the load 3, for example, a position where a filter device for reducing harmonic current is connected is designated as a harmonic injection point 4. Inject current.

【0027】ところで、電力系統1には周波数fsの基
本波のほかに、基本波の整数倍の周波数n・fsの高調
波が存在し、これらの整数倍周波数の高調波に対して、
高調波注入点4からみた系統1の下位(負荷側)はほぼ
負荷3が接続された状態にあり、上位(電源側)は例え
ば配電トランスのトランスインピーダンスを含む線路イ
ンピーダンス6を介して系統電源2が接続された状態に
ある。
By the way, in addition to the fundamental wave of the frequency fs, the power system 1 has harmonics of the frequency n · fs which are integral multiples of the fundamental wave.
The lower part (load side) of the system 1 viewed from the harmonic injection point 4 is almost in a state where the load 3 is connected, and the upper part (power supply side) is connected to the system power supply 2 via a line impedance 6 including a transimpedance of a distribution transformer, for example. Is connected.

【0028】このとき、上位,下位をノートンの定理で
表現した高調波等価回路は、それぞれアドミタンスと電
流源との並列回路とみなせる。
At this time, the harmonic equivalent circuit expressing the upper and lower parts by Norton's theorem can be regarded as a parallel circuit of admittance and current source, respectively.

【0029】なお、下位の電流源は実際に存在するので
はなく、負荷による電流歪み等で等価的に形成されるも
のである。
It should be noted that the lower current source does not actually exist but is formed equivalently due to current distortion caused by a load.

【0030】また、上位の線路インピーダンス6等は電
力系統1の線路特性から予め把握されており、既知であ
る。
The upper line impedance 6 and the like are previously known from the line characteristics of the power system 1 and are known.

【0031】そして、n次高調波を測定調波とし、この
測定調波についての高調波注入点4の上位,下位の時々
刻々変化するアドミタンス(回路定数)を求める場合、
注入点4の電圧(系統電圧)を変圧器7により計測し、
高調波注入点4の上位,下位の少なくとも一方,例えば
上位の電流を変流器8により計測する。
When the n-th order harmonic is used as a measurement harmonic, and the admittance (circuit constant) that changes every moment in the upper and lower harmonic injection points 4 for the measurement harmonic is obtained,
The voltage at the injection point 4 (system voltage) is measured by the transformer 7,
At least one of the upper and lower parts of the harmonic injection point 4, for example, the upper part of the current is measured by the current transformer 8.

【0032】さらに、変圧器7の電圧の計測信号をPL
L回路構成の同期信号作成部9に供給し、この作成部9
により、制御部10の制御信号に基づいて系統電源2の
例えば60Hzの基本波に同期した同期制御信号を形成
する。
Further, the measurement signal of the voltage of the transformer 7 is
The signal is supplied to a synchronizing signal generator 9 having an L circuit configuration.
As a result, a synchronization control signal synchronized with a fundamental wave of, for example, 60 Hz of the system power supply 2 is formed based on the control signal of the control unit 10.

【0033】そして、この同期制御信号が供給される注
入源信号作成部11は、制御部10の制御に基づき、測
定調波の上,下両側の基本波の非整数倍周波数の注入信
号として、測定調波(n次高調波)とn±1次高調波そ
れぞれとの間の基本波に同期した基本波の非整数倍周波
数の注入信号を形成する。
Then, based on the control of the control unit 10, the injection source signal creating unit 11 to which the synchronization control signal is supplied, as an injection signal of a non-integer multiple frequency of the fundamental wave above and below the measurement harmonic, An injection signal of a non-integer multiple frequency of the fundamental wave synchronized with the fundamental wave between the measurement harmonic (nth harmonic) and each of the n ± 1st harmonics is formed.

【0034】つぎに、この注入信号を増幅器12により
電流増幅して測定調波の上,下両側それぞれの注入電流
を形成し、この注入電流を注入回路13,開閉器14を
介して高調波注入点4に注入し、この注入に基づく高調
波注入点4の系統電圧を変圧器7により計測するととも
に、高調波注入点4の上位,下位の少なくとも一方,例
えば上位の系統電流を変流器8により計測する。
Next, the injection signal is amplified by an amplifier 12 to form an injection current on each of the upper and lower sides of the measured harmonic, and this injection current is passed through an injection circuit 13 and a switch 14 to obtain a harmonic injection. Injection is made at a point 4, the system voltage at the harmonic injection point 4 based on the injection is measured by the transformer 7, and at least one of the upper and lower harmonic currents of the harmonic injection point 4, for example, the upper system current is converted to the current transformer 8. Measured by

【0035】また、高調波注入点4の注入電流は、変流
器15により計測する。なお、電流注入期間は後述の周
波数分析等に基づく測定精度を考慮して、例えば基本波
の10周期に設定される。
The injection current at the harmonic injection point 4 is measured by the current transformer 15. The current injection period is set to, for example, 10 periods of the fundamental wave in consideration of measurement accuracy based on frequency analysis and the like described later.

【0036】そして、変圧器7の電圧の計測信号及び変
流器8,15の電流の計測信号をA/D変換部16に供
給し、この変換部16により、同期信号作成部9の同期
制御信号に基づくサンプリングタイミング制御部17の
基本波に同期したサンプリングパルスで各計測信号を計
測データに変換する。
The measurement signal of the voltage of the transformer 7 and the measurement signal of the current of the current transformers 8 and 15 are supplied to the A / D converter 16, which controls the synchronization of the synchronization signal generator 9. Each measurement signal is converted into measurement data by a sampling pulse synchronized with the fundamental wave of the sampling timing control unit 17 based on the signal.

【0037】つぎに、これらの計測データを信号処理部
18に供給し、この処理部18により、DET処理,F
FT処理等のデジタル周波数分析処理又はアナログ周波
数分析処理を実行し、この分析の結果に基づき、電力系
統1の高調波注入点4の上位,下位の少なくとも一方、
例えば下位を注目側として、この注目側の測定調波の
上,下両側の注入周波数についてのアドミタンスを求め
る。
Next, these measurement data are supplied to a signal processing unit 18, which performs DET processing, F
A digital frequency analysis process such as an FT process or an analog frequency analysis process is executed, and based on a result of this analysis, at least one of the upper and lower harmonic injection points 4 of the power system 1;
For example, with the lower side as the target side, the admittances of the injection frequencies on the upper and lower sides of the measurement harmonic on the target side are obtained.

【0038】さらに、この上,下両側の注入周波数につ
いてのアドミタンスに基づく補間処理により、その中間
の値をとる測定調波についての注目側のアドミタンスを
求めて決定する。
Further, the admittance on the target side of the measured harmonic having an intermediate value is obtained and determined by interpolation processing based on the admittance of the upper and lower injection frequencies.

【0039】また、注目側の測定調波についての等価回
路を求めるときは、決定したアドミタンスと電力系統1
の測定調波の電流,電圧の測定結果とにより、決定した
アドミタンスに並列な電流源も求める。
When obtaining an equivalent circuit for the measured harmonic on the side of interest, the determined admittance and power system 1
A current source in parallel with the determined admittance is also obtained from the measured harmonic current and voltage measurement results.

【0040】つぎに、測定調波の上,下両側それぞれの
注入電流の注入手法について説明する。まず、電力系統
1のn次高調波についての高調波注入点4の上位,下位
の等価回路は、図2の等価回路19,20に示すよう
に、アドミタンスYn1 ,Yn2と電流源Gn1 ,Gn
2 との並列回路とみなすことができる。
Next, a method of injecting an injection current on both upper and lower sides of the measurement harmonic will be described. First, as shown in the equivalent circuits 19 and 20 of FIG. 2, the admittances Yn 1 and Yn 2 and the current source Gn 1 are shown in the upper and lower equivalent circuits of the harmonic injection point 4 for the n-th harmonic of the power system 1. , Gn
It can be regarded as a parallel circuit with 2 .

【0041】また、n次高調波の上,下両側の基本波の
非整数倍周波数についての電力系統1の等価回路は、本
来、この周波数の成分がないため、アドミタンスのみに
なる。
Further, the equivalent circuit of the power system 1 for the non-integer multiple of the fundamental wave on the upper and lower sides of the n-th harmonic has only admittance because there is no component of this frequency.

【0042】そして、電力系統1を高調波の注入による
電圧歪みを起し易い1KVAベースの小容量負荷回路モ
デルとし、測定調波をn=5の5次高調波とし、さら
に、その上,下両側の基本波の非整数倍周波数の注入電
流を、基本波に同期した5.5次調波,4.5次調波の
中間次数調波の電流とした場合、種々の実験から、電流
注入により基本波電圧に対して0.3%程度の電圧歪み
を与えれば、電力系統1の負荷に悪影響を与えることな
く、測定結果から注目側の測定調波についてのアドミタ
ンスYn1 ,Yn2 や等価回路19,20を求め得るこ
とが判明した。
Then, the power system 1 is a 1KVA-based small-capacity load circuit model that easily causes voltage distortion due to the injection of harmonics, and the measured harmonic is the fifth harmonic of n = 5. In the case where the injection current of a non-integer multiple frequency of the fundamental wave on both sides is a 5.5th harmonic and a 4.5th harmonic intermediate order harmonic synchronized with the fundamental wave, the current injection was performed based on various experiments. Gives a voltage distortion of about 0.3% with respect to the fundamental voltage, the admittance Yn 1 , Yn 2 and the equivalent of the measured harmonic on the attention side can be obtained from the measurement result without adversely affecting the load of the power system 1. It has been found that circuits 19 and 20 can be obtained.

【0043】一方、電力系統1の共振点が5.5次,
4.5次の中間次数調波又はそれらの近傍の周波数にな
るときは、5.5次,4.5次の中間次数調波の電流を
注入すると、電力系統1に前記の0.3%をこえる大き
な歪み電圧が発生する。
On the other hand, the resonance point of the power system 1 is 5.5 order,
When a 4.5th intermediate order harmonic or a frequency in the vicinity thereof is reached, 5.5% or 4.5th intermediate order harmonic current is injected, and the above 0.3% A large distortion voltage exceeding the above occurs.

【0044】そこで、基本波電圧の0.3%の歪み電圧
を所定の上限電圧(しきい値)とし、注入電流毎に制御
部10により図3の注入流量決定処理を実行し、そのス
テップS1 〜S5 の処理によって中間次数調波の注入電
流量を決定する。
Then, the distortion voltage of 0.3% of the fundamental wave voltage is set as a predetermined upper limit voltage (threshold value), and the control unit 10 executes the injection flow rate determination processing of FIG. determining the amount of injected current of the intermediate order harmonics by treatment 1 to S 5.

【0045】すなわち、測定調波の上,下両側の注入電
流の高調波次数又は周波数がキーボード操作等で制御部
10に与えられると、制御部10は、最初に、例えば測
定調波の下側の4.5次調波の周波数〔基本波を60H
zとしたときは270Hz{=(240+300)/
2}〕を注入周波数とし、ステップS1 により、注入周
波数の初期注入量(スタートレベル)の注入信号を形成
するように、注入源信号作成部11の信号利得を制御
し、高調波注入点4に4.5次調波の初期注入量の電流
を注入する。
That is, when the harmonic order or frequency of the injection current on both the upper and lower sides of the measurement harmonic is given to the control unit 10 by keyboard operation or the like, the control unit 10 firstly operates, for example, on the lower side of the measurement harmonic. 4.5th harmonic frequency [fundamental wave is 60H
270Hz {= (240 + 300) /
2}] is set as the injection frequency, and in step S 1 , the signal gain of the injection source signal generator 11 is controlled so as to form an injection signal of the initial injection amount (start level) of the injection frequency, and the harmonic injection point 4 is set. Is injected with the current of the initial injection amount of the 4.5th harmonic.

【0046】つぎに、ステップS2 に移行し、変圧器7
の計測信号に基づくA/D変換部16の電圧の計測デー
タを信号処理部18により分析して処理し、4.5次調
波の電流注入に基づく電力系統1の歪み電圧を検出す
る。
Next, the process proceeds to step S 2, transformer 7
The signal processing unit 18 analyzes and processes the measured data of the voltage of the A / D conversion unit 16 based on the measurement signal of (1), and detects the distortion voltage of the power system 1 based on the 4.5th harmonic current injection.

【0047】この検出結果(歪み電圧)が制御部10に
伝送され、ステップS3 により制御部10が伝送された
歪み電圧と前記上限電圧とを比較し、伝送された歪み電
圧が上限電圧に達するまでステップS4 を介してステッ
プS2 に戻り、注入電流量を小量ずつ,例えば一定量Δ
Iずつ増加して電力系統1に注入することをくり返す。
[0047] The detection result (distorted voltage) is transmitted to the control unit 10, the control unit 10 compares the upper limit voltage distortion voltage transmitted by the step S 3, the transmitted distortion voltage reaches the upper limit voltage until the process returns to step S 2 via step S 4, the injected current amount small portions, for example, a fixed amount Δ
The process of increasing by I and injecting into the power system 1 is repeated.

【0048】そして、注入電流に基づく歪み電圧が上限
電圧に上昇すると、ステップS3 からステップS5 に移
行し、注入電流量を一定量ΔI減少してその直前の大き
さに戻し、注入電流をほぼ基本波の0.3%の歪み電圧
が生じる大きさ(注入量)に決定して電流量決定処理を
終了する。
When the distortion voltage based on the injection current rises to the upper limit voltage, the process proceeds from step S 3 to step S 5 , where the injection current is reduced by a fixed amount ΔI and returned to the immediately preceding magnitude, and the injection current is reduced. The magnitude (implantation amount) at which a distortion voltage of about 0.3% of the fundamental wave is generated is determined, and the current amount determination processing ends.

【0049】この終了後、高調波測定に移行し、決定し
た注入量の4.5次調波の電流を高調波注入点4に注入
し、変圧器7及び変流器8,15の計測結果から4.5
次調波についての電力系統1の注目側のアドミタンスを
求める。
After completion of the above operation, the operation proceeds to the harmonic measurement, and the current of the 4.5th harmonic of the determined injection amount is injected into the harmonic injection point 4, and the measurement results of the transformer 7 and the current transformers 8, 15 are obtained. From 4.5
The admittance of the attention side of the power system 1 for the next harmonic is determined.

【0050】さらに、4.5次調波についてのアドミタ
ンスが求まると、制御部10は測定調波の上側の5.5
次調波の周波数〔基本波が60Hzであれば330Hz
{=300+360)/2}〕を注入周波数に設定して
図3の注入量決定処理を再び実行し、前記4.5次調波
の場合と同様にして、5.5次調波の注入電流を徐々に
大きくしながら高調波注入点4に注入する。
Further, when the admittance of the 4.5th harmonic is obtained, the control unit 10 sets the upper 5.5 of the measured harmonic.
Next harmonic frequency [330Hz if fundamental wave is 60Hz
{= 300 + 360) / 2}] is set as the injection frequency, and the injection amount determination processing of FIG. 3 is executed again. As in the case of the 4.5th harmonic, the injection current of the 5.5th harmonic is set. Is gradually injected into the harmonic injection point 4.

【0051】そして、この5.5次調波の注入電流に基
づく電力系統1の歪み電圧がほぼ基本波電圧の0.3%
まで大きくなると、注入電流をこの大きさに決定して高
調波測定に移行し、5.5次調波についての注目側のア
ドミタンスを求める。
The distortion voltage of the power system 1 based on the 5.5th harmonic injection current is approximately 0.3% of the fundamental wave voltage.
When it becomes larger, the injection current is determined to this value, and the operation shifts to harmonic measurement, and the admittance of the attention side for the 5.5th harmonic is obtained.

【0052】したがって、測定調波(5次高調波)の
上,下両側の5.5次調波,4.5次調波の注入電流
が、それぞれ、注入によって電力系統1にほぼ基本波電
圧の0.3%の歪み電圧が生じる直前の最適注入量に自
動的に設定され、この最適電流量の電流注入に基づき、
電力系統1の注目側の5.5次調波,4.5次調波につ
いてのアドミタンスが求められる。
Therefore, the injection currents of the 5.5th harmonic and the 4.5th harmonic on the upper and lower sides of the measured harmonic (the 5th harmonic) are respectively substantially applied to the power system 1 by the injection. Is automatically set to the optimal injection amount immediately before the 0.3% distortion voltage occurs. Based on the current injection of the optimal current amount,
The admittance of the 5.5th harmonic and the 4.5th harmonic on the target side of the power system 1 is obtained.

【0053】この場合、注入電流の周波数が電力系統1
の共振点の周波数又はその近傍の周波数であっても、電
力系統1に過大な電圧歪みが発生せず、電力系統1の負
荷に悪影響を与えることなく、注入周波数についての注
目側のアドミタンスが正確に求まる。
In this case, the frequency of the injected current is
At the resonance point or at a frequency near the resonance point, excessive voltage distortion does not occur in the power system 1 and the load on the power system 1 is not adversely affected. Is determined.

【0054】ところで、注入電流の初期注入量及び変化
量ΔIは同一の一定量であってもよく、例えば線形又は
非線形に増大又は減少変化する量であってもよい。
Incidentally, the initial injection amount and the change amount ΔI of the injection current may be the same fixed amount, and may be, for example, an amount that increases or decreases linearly or non-linearly.

【0055】また、最適注入量は、注入電流を零から増
加して決定してもよいが、つぎに説明するように共振点
での電圧拡大率を考慮した注入量から増加して決定する
ことが実用上からは好ましい。
The optimum injection amount may be determined by increasing the injection current from zero. However, as described below, the optimum injection amount is determined by increasing the injection amount in consideration of the voltage expansion rate at the resonance point. Is preferable in practical use.

【0056】すなわち、電力系統1を例えば10MVA
ベースとし、その高調波注入点4の下位を注目側とする
と、そのn次高調波の等価回路は、図4に示すように、
図2のアドミタンスYn2 ,電流源IGn2 の並列回路を
アドミタンスYnとして表わすことができ、このアドミ
タンスYnは容量成分SCと抵抗負荷成分Yとを並列合
成したn次アドミタンスからなる。
That is, the power system 1 is set to, for example, 10 MVA.
Assuming that the lower side of the harmonic injection point 4 is the target side, the equivalent circuit of the n-th harmonic is, as shown in FIG.
The parallel circuit of the admittance Yn 2 and the current source IGn2 in FIG. 2 can be represented as admittance Yn, and this admittance Yn is composed of an n-order admittance in which a capacitance component SC and a resistance load component Y are combined in parallel.

【0057】このとき、系統電源2のn次高調波の電圧
をEnとし、主に配電トランスのインピーダンスに基づ
くn次高調波についての配線インピーダンス6をjXL
nとすると、高調波注入点4のn次高調波の電圧Vnは
つぎの数1の式で示される。
At this time, the voltage of the nth harmonic of the system power supply 2 is set to En, and the wiring impedance 6 for the nth harmonic mainly based on the impedance of the distribution transformer is set to jXL.
Assuming that n, the voltage Vn of the nth harmonic at the harmonic injection point 4 is expressed by the following equation (1).

【0058】[0058]

【数1】Vn=En/(1+jXLn・Yn)## EQU1 ## Vn = En / (1 + jXLn.Yn)

【0059】さらに、電圧拡大率はVn/Enで示さ
れ、数1の式に基づき、電圧拡大率Vn/Enは1/
(1+jXLn・Yn)の絶対値から求まる。
Further, the voltage expansion rate is represented by Vn / En, and based on the equation (1), the voltage expansion rate Vn / En is 1 /
It is obtained from the absolute value of (1 + jXLn · Yn).

【0060】そして、5次高調波(n=5)につき、抵
抗負荷成分Yを1000%負荷(1MW負荷)にして容
量成分SCを0〜100%(0〜10MVA)に可変す
ると、電圧拡大率V5 /E5 は、図5の実測結果に示す
ようにほぼ1から25の範囲で変化し、共振すると、2
5倍に拡大されることがわかる。
For the fifth harmonic (n = 5), when the resistance load component Y is changed to a load of 1000% (1 MW load) and the capacitance component SC is changed to 0 to 100% (0 to 10 MVA), the voltage expansion rate becomes V 5 / E 5 changes in the range of approximately 1 to 25 as shown in the actual measurement results in FIG.
It can be seen that it is magnified 5 times.

【0061】つぎに、n次高調波の上,下両側の電力系
統1に存在しない中間次数調波をn±m次調波(0<m
<1)とし、このn±m次調波の電流In±mを高調波
注入点4に注入する際は、図4と同様の電力系統1の等
価回路が図6に示すようになる。
Next, an intermediate order harmonic that does not exist in the power system 1 on both the upper and lower sides of the nth harmonic is converted into an n ± mth harmonic (0 <m).
When the current In ± m of the n ± m-th harmonic is injected into the harmonic injection point 4, the equivalent circuit of the power system 1 similar to that of FIG. 4 is as shown in FIG.

【0062】この図6において、高調波注入点4の下位
の注目側のアドミタンスYn±mは容量成分SC’と抵
抗成分Y’との並列合成からなり、配線インピーダンス
6をjXLn±mとすると、高調波注入点4の電圧Vn
±mはつぎの数2の式で示される。
In FIG. 6, the admittance Yn ± m on the attention side below the harmonic injection point 4 is composed of a parallel combination of the capacitance component SC ′ and the resistance component Y ′. If the wiring impedance 6 is jXLn ± m, Voltage Vn at harmonic injection point 4
± m is expressed by the following equation (2).

【0063】[0063]

【数2】Vn±m=(jXLn±m・In±m)/(1
+jXLn±m・Yn±m)
Vn ± m = (jXLn ± m · In ± m) / (1
+ JXLn ± m ・ Yn ± m)

【0064】そして、数1,数2の式において、In=
In±m,Vn=Vn±m,XLn=XLn±m,Yn
=Yn±mとすると、両式の分母が等しくなり、数2の
式はつぎの数3の式で表すことができる。
In the equations (1) and (2), In =
In ± m, Vn = Vn ± m, XLn = XLn ± m, Yn
Assuming that = Yn ± m, the denominator of both equations becomes equal, and the equation of Equation 2 can be expressed by the following Equation 3.

【0065】[0065]

【数3】Vn±m=(jXLn・In)・電圧拡大率## EQU3 ## Vn ± m = (jXLn · In) · Voltage expansion rate

【0066】この数3の式は、例えば5次高調波(n=
5)の上,下近傍の中間次数調波の電流を注入する際、
電圧拡大率が25(最大)であれば、電圧拡大率が1
(最小)のときの1/25の電流量で電圧拡大率が1の
ときと同じ電圧歪みが生じることを表わし、電力系統1
の状態によっては同じ大きさの電流を注入しても電圧歪
みに過不足が生じることを示す。
The equation (3) is, for example, the fifth harmonic (n =
5) When injecting the current of the middle order harmonic near the upper and lower sides,
If the voltage expansion rate is 25 (maximum), the voltage expansion rate is 1
(Minimum), the same voltage distortion as when the voltage expansion rate is 1 occurs at a current amount of 1/25, and the power system 1
Indicates that even if a current of the same magnitude is injected, excessive or insufficient voltage distortion occurs.

【0067】そこで、測定調波を5次高調波とし、基本
波電圧の0.3%を注入の上限電圧(しきい値)とする
際は、測定調波の上,下両側の中間次数調波の注入電流
の初期注入量を、注入による歪み電圧が前記0.3%の
1/25になる量に設定し、この注入量から増加して注
入電流の大きさを決定する。
Therefore, when the measured harmonic is the fifth harmonic and the upper limit voltage (threshold) for injection is 0.3% of the fundamental wave voltage, the intermediate harmonics on both upper and lower sides of the measured harmonic are used. The initial injection amount of the wave injection current is set to an amount such that the distortion voltage due to the injection becomes 1/25 of the 0.3%, and the amount of the injection current is determined by increasing the injection amount.

【0068】つぎに、決定した注入電流の注入結果に基
づく注目側のアドミタンスの具体的な求め方について説
明する。
Next, a specific method of obtaining the admittance of the attention side based on the injection result of the determined injection current will be described.

【0069】説明を簡単にするため、高調波注入点4に
注入される中間次数調波の電流をIxとし、この電流I
xの注入に基づく高調波注入点4の電圧をVxとし、高
調波注入点4の上位,下位それぞれを流れる電流をIx
1 ,Ix2 とし、この電流Ix1 ,Ix2 に基づく電力
系統1の高調波注入点4より上位,下位のアドミタンス
をYx1 ,Yx2 とすると、アドミタンスYx1 ,Yx
2 は、つぎの数4,数5の2式それぞれから求まる。
For simplicity of explanation, the current of the intermediate order harmonic injected into the harmonic injection point 4 is defined as Ix, and this current I
Let Vx be the voltage at the harmonic injection point 4 based on the injection of x, and let Ix be the current flowing through each of the upper and lower harmonic injection points 4.
1, and Ix 2, higher than the current Ix 1, Ix 2 harmonic injection point 4 of the power system 1 based on, when the lower admittance and Yx 1, Yx 2, admittance Yx 1, Yx
2 is obtained from each of the following equations (4) and (5).

【0070】[0070]

【数4】Yx1 =Ix1 /Vx## EQU4 ## Yx 1 = Ix 1 / Vx

【0071】[0071]

【数5】Yx2 =Ix2 /Vx## EQU5 ## Yx 2 = Ix 2 / Vx

【0072】そして、電流Ix1 ,Ix2 はいずれか一
方を測定すれば、Ix1 =Ix−Ix2 ,Ix2 =Ix
−Ix1 の演算により他方が求まる。
If one of the currents Ix 1 and Ix 2 is measured, Ix 1 = Ix−Ix 2 and Ix 2 = Ix
The other is obtained by calculation of -ix 1.

【0073】したがって、電力系統1の高調波注入点4
より下位を注目側とする場合、信号処理部18は、A/
D変換部17の計測データの周波数分析により電圧Vx
及び電流Ix,Ix1 を求める。
Therefore, the harmonic injection point 4 of the power system 1
When the lower side is set as the attention side, the signal processing unit 18 outputs the A /
The voltage Vx is obtained by analyzing the frequency of the
And current Ix, seek Ix 1.

【0074】このとき、注入電流が電力系統1の基本波
に同期した整数周期の電流であり、基本波に同期したサ
ンプリングにより、サンプリングの開始,終了の連続性
が保たれるため、サンプリングエッジによるDFT誤差
等の周波数分析の誤差は生じない。
At this time, the injection current is an integer period current synchronized with the fundamental wave of the power system 1, and the sampling start and end continuity is maintained by the sampling synchronized with the fundamental wave. No frequency analysis error such as a DFT error occurs.

【0075】さらに、電流Ix,Ix1 に基づき、信号
処理部18はIx2 =Ix−Ix1の演算から注目側の
測定調波の上,下両側の中間次数調波の電流Ix2 を求
める。
[0075] Furthermore, based current Ix, the Ix 1, the signal processing unit 18 Ix 2 = on the calculation of the Ix-Ix 1 attention side of the measuring harmonics, determine the current Ix 2 intermediate degree harmonics of the lower sides .

【0076】そして、電流Ix2 ,電圧Vxに基づき、
数5の式から注目側の測定調波の上,下両側の中間次数
調波についてのアドミタンスYx2 を求める。
Then, based on the current Ix 2 and the voltage Vx,
The admittance Yx 2 for the intermediate order harmonics on the upper and lower sides of the measurement harmonic on the side of interest is calculated from the equation (5).

【0077】このとき、電流Ixが電力系統1に存在し
ない周波数の電流であるため、注入電力量が微小であっ
ても、アドミタンスYx2 は電力系統1の高調波の影響
を受けることなく正確に求まる。
At this time, since the current Ix is a current having a frequency that does not exist in the power system 1, the admittance Yx 2 can be accurately obtained without being affected by harmonics of the power system 1 even if the amount of injected power is minute. I get it.

【0078】なお、電流Ix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 a harmonic current of the measured harmonic is injected instead of the current Ix, the admittance based on the injected harmonic current cannot be obtained because the harmonic exists in the power system 1. .

【0079】つぎに、注目側の測定調波についてのアド
ミタンスYn2 は、その上,下両側の電流Ix2 につい
てのアドミタンスをYx2 (u),Yx2 (d)とする
と、アドミタンスYx2 (u),Yx2 (d)の中間値
として求まる。
Next, the admittance Yn 2 of the measured harmonic on the target side is given by admittance Yx 2 (d) where the admittance of the current Ix 2 on both the upper and lower sides is Yx 2 (u), Yx 2 (d). u), Yx 2 (d).

【0080】そのため、信号処理部18はアドミタンス
Yx2 (u),Yx2 (d)に基づき、単純平均或いは
最小二乗法等により補間演算を実行し、測定調波につい
ての図2の等価回路20のアドミタンスYn2 を求めて
決定する。
For this reason, the signal processing section 18 executes an interpolation operation by a simple average or a least square method based on the admittances Yx 2 (u) and Yx 2 (d), and obtains an equivalent circuit 20 of FIG. Is determined by obtaining the admittance Yn 2 of

【0081】このとき、アドミタンスYx2 (u),Y
2 (d)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、測定調波についてのアドミタ
ンスYn2 も正確に求まる。
At this time, the admittance Yx 2 (u), Y
Since x 2 (d) is accurately calculated without being affected by the harmonics of the power system 1, the admittance Yn 2 of the measured harmonic is also accurately obtained.

【0082】なお、高調波注入点4の上位の電流Ix1
を計測する代わりに、その下位の電流Ix2 を計測して
もよく、この場合は、計測された電流から直ちに注目側
の電流Ix2 が求まる。
The higher current Ix 1 at the harmonic injection point 4
Instead of measuring may measure the current Ix 2 of the lower, in this case, immediately noticed side current Ix 2 is obtained from the measured current.

【0083】また、高調波注入点4の上位を注目側とす
る場合にも、計測又はIx−Ix2の演算から得られた
電流Ix1 と電流Ix,電圧Vxとに基づき、前記と同
様にして測定調波についてのアドミタンスを、電力系統
1の高調波の影響を受けることなく正確に求めることが
できる。
Also, in the case where the upper side of the harmonic injection point 4 is the target side, based on the current Ix 1 , the current Ix, and the voltage Vx obtained from the measurement or the calculation of Ix−Ix 2 in the same manner as described above. Thus, the admittance of the measured harmonic can be accurately obtained without being affected by harmonics of the power system 1.

【0084】なお、高調波注入点4の上位,下位の両方
を注目側とし、それぞれの測定調波についてのアドミタ
ンスを求めることもでき、この場合、上位,下位の両方
に変流器を設け、上位,下位を流れる電流Ix1 ,Ix
2 をそれぞれ計測してもよい。
It is also possible to determine the admittance of each measured harmonic by setting both the upper and lower harmonics of the harmonic injection point 4 as the attention side. In this case, current transformers are provided for both the upper and lower harmonics. Currents Ix 1 , Ix flowing in the upper and lower parts
2 may be measured respectively.

【0085】そして、注目側の測定調波についてのアド
ミタンスが求まれば、注目側の測定調波に対する挙動等
を把握することができる。
When the admittance of the measurement harmonic on the target side is obtained, the behavior of the measurement harmonic on the target side can be grasped.

【0086】ところで、この実施の形態においては、ア
ドミタンスだけでなく、このアドミタンスと電流源との
並列回路からなる測定調波についての等価回路をより完
全に求めるため、信号処理部18は測定調波についての
注目側のアドミタンスを求めて決定した後、つぎに説明
するように、測定調波についての注目側の電流源を算出
してその等価回路を求める。
By the way, in this embodiment, in order to more completely find an equivalent circuit for a measured harmonic composed of a parallel circuit of the admittance and the current source, not only the admittance but also the signal processing unit 18 After determining and determining the admittance of the target side for the target, the current source of the target side for the measured harmonic is calculated and its equivalent circuit is determined, as described below.

【0087】すなわち、測定調波についての注目側のア
ドミタンスYn2 が求まると、中間次数調波の電流注入
の終了後、開閉器14が開放した状態での変圧器7,変
流器8の計測信号に基づくA/D変換部17の計測デー
タの周波数分析により、電力系統1の測定調波の電圧
(高調波電圧),電流(高調波電流)を求める。
That is, when the admittance Yn 2 on the side of interest for the measured harmonic is determined, the measurement of the transformer 7 and the current transformer 8 with the switch 14 opened after the end of the current injection of the intermediate order harmonic is completed. The frequency (harmonic voltage) and current (harmonic current) of the measured harmonic of the power system 1 are obtained by frequency analysis of the measurement data of the A / D converter 17 based on the signal.

【0088】そして、測定調波の高調波電圧をVn,高
調波電流をIn(上位から下位の向きを正)とすると、
図2の等価回路図からも明らかなように、高調波注入点
4の下位,上位につき、つぎの数6,数7の2式それぞ
れが成立する。
Then, assuming that the harmonic voltage of the measured harmonic is Vn and the harmonic current is In (the direction from upper to lower is positive),
As is clear from the equivalent circuit diagram of FIG. 2, the following two equations (6) and (7) hold for the lower and upper harmonic injection points 4 respectively.

【0089】[0089]

【数6】IGn1 =In+Vn・Yn1 ## EQU6 ## I Gn1 = In + Vn · Yn 1

【0090】[0090]

【数7】IGn2 =Vn・Yn2 −In## EQU7 ## I Gn2 = Vn · Yn 2 -In

【0091】そこで、注目側が高調波注入点4の下位で
ある場合、信号処理部18は数7の式の演算から注目側
の測定調波の電流源IGn2 を求めて、図2の測定調波に
ついての注目側の等価回路20を決定する。
Therefore, when the target side is below the harmonic injection point 4, the signal processing unit 18 obtains the current source I Gn2 of the measurement harmonic on the target side from the calculation of the equation (7), and obtains the measurement tone of FIG. The attention side equivalent circuit 20 for the wave is determined.

【0092】なお、注目側が高調波注入点4の上位であ
る場合は、数6の式の演算から電流源IGn1 を求めて等
価回路19を決定する。
When the target side is higher than the harmonic injection point 4, the equivalent circuit 19 is determined by obtaining the current source I Gn1 from the calculation of the equation (6).

【0093】この場合、注目側の測定調波についての等
価回路19,20が個別にしかも精度よく求められる。
In this case, the equivalent circuits 19 and 20 for the measurement harmonic on the side of interest are individually and accurately obtained.

【0094】なお、注目側の等価回路19,20の決定
された各回路定数Yn1 ,Yn2 ,IGn1 ,IGn2 等の
情報は、計測装置5の記憶部(図示せず)に記憶される
とともに表示部(図示せず)に例えば等価回路図の形式
で画面表示される。
[0094] Incidentally, each circuit constant Yn 1, Yn 2, I Gn1 , I Gn2 information such as determined attention side of the equivalent circuits 19 and 20 are stored in the storage unit of the measuring device 5 (not shown) At the same time, a screen is displayed on a display unit (not shown) in the form of, for example, an equivalent circuit diagram.

【0095】また、系統切換え等による高調波の低減を
行う場合は、前記の各測定がくり返されて注目側の最新
の等価回路19,20の状態が把握され、この結果等か
ら系統切り換えに伴う高調波の発生を予測し、高調波注
入点4に接続したフィルタ装置(図示せず)のフィルタ
容量が最適に設定される。
When harmonics are reduced by system switching or the like, the above-described measurements are repeated to grasp the state of the latest equivalent circuits 19 and 20 on the side of interest. The generation of accompanying harmonics is predicted, and the filter capacity of a filter device (not shown) connected to the harmonic injection point 4 is optimally set.

【0096】そして、この実施の形態においては、測定
調波の上,下両側の中間次数調波の注入電流を徐々に注
入量を増大して実際に電力系統1に注入し、この注入の
結果に基づき、両注入電流を注入による歪み電圧が電力
系統1の負荷に悪影響を与える直前の大きさになる最適
電流量に決定し、この最適電流量の注入結果に基づいて
測定調波についての電力系統1のアドミタンスYn1
Yn2 又は等価回路19,20を求めたため、電力系統
1のいわゆる高調波注入による障害を招来することな
く、電力系統1の高調波についての回路特性を正確に求
めることができる。
In this embodiment, the injection current of the intermediate order harmonics on the upper and lower sides of the measurement harmonic is actually gradually injected into the electric power system 1 while the injection amount is increased. , The two injection currents are determined to be the optimum amount of current at which the distortion voltage caused by the injection adversely affects the load of the power system 1, and the power for the measured harmonic is determined based on the result of the injection of the optimum current amount. Admittance Yn 1 of system 1,
Since Yn 2 or the equivalent circuits 19 and 20 have been obtained, the circuit characteristics of the power system 1 with respect to harmonics can be accurately obtained without causing a failure due to so-called harmonic injection of the power system 1.

【0097】なお、測定調波の上,下両側の注入電流
は、基本波に同期していない基本波の非整数倍の適当な
周波数の電流であってもよく、また、それぞれ複数であ
ってもよい。
The injection currents on the upper and lower sides of the measurement harmonic may be currents having an appropriate frequency which is a non-integer multiple of the fundamental wave which is not synchronized with the fundamental wave. Is also good.

【0098】そして、測定調波の上,下両側の注入電流
がそれぞれ複数になる場合は、例えば、上,下両側それ
ぞれにつき、注入電流毎にアドミタンスを求め、その平
均値等を求めて測定調波についてのアドミタンスを求め
ればよい。また、上限電圧の大きさ等は電力系統1の状
態等に応じて設定すればよい。
When the injection currents on the upper and lower sides of the measurement harmonic are plural, for example, the admittance is obtained for each injection current on both the upper and lower sides, and the average value and the like are obtained. What is necessary is to find the admittance of the wave. The magnitude of the upper limit voltage may be set according to the state of the power system 1 or the like.

【0099】[0099]

【発明の効果】本発明は、以下に記載する効果を奏す
る。まず、請求項1の場合は、測定調波の上,下両側そ
れぞれの基本波の非整数倍周波数の電流を、徐々に増加
しながら電力系統1に注入してその注入周波数の歪み電
圧を計測することのくり返しに基づき、事前に、電力系
統1に過大な歪み電圧が発生する直前の電流量,すなわ
ち注入によって電力系統1の負荷に悪影響を与えない最
適注入量に設定することができる。
The present invention has the following effects. First, in the case of claim 1, a current of a non-integer multiple frequency of each of the fundamental waves on both upper and lower sides of the measurement harmonic is injected into the power system 1 while gradually increasing, and a distortion voltage at the injection frequency is measured. Based on the repetition, the current amount immediately before an excessive distortion voltage is generated in the power system 1, that is, the optimum injection amount that does not adversely affect the load of the power system 1 due to the injection can be set.

【0100】そして、この最適注入量の電流注入によ
り、電力系統1の負荷に悪影響を与えることなく、測定
調波の上,下両側それぞれの基本波の非整数倍周波数の
電流注入についての電力系統1の注目側のアドミタンス
を精度よく求めることができ、この結果から電力系統1
の注目側の測定調波についてのアドミタンスを、高調波
注入による障害を招来することなく、正確に求めること
ができる。
The current injection at the optimum injection amount does not adversely affect the load of the power system 1 and the power system for current injection at a non-integer multiple frequency of the fundamental wave on each of the upper and lower sides of the measured harmonic. 1, the admittance of the attention side of the power system 1 can be accurately obtained.
The admittance of the measurement harmonic on the side of interest can be accurately determined without causing an obstacle due to harmonic injection.

【0101】また、請求項2の場合は、請求項1の場合
と同様にして求めた電力系統1の注目側の測定調波につ
いてのアドミタンスと、電力系統1の測定調波の電圧,
電流の計測結果とにより、電力系統1の注目側の前記ア
ドミタンスに並列な測定調波の電流源を求めることがで
き、電力系統1の注目側のアドミタンスと電流源との並
列回路からなる測定調波についての等価回路を、電力系
統1の負荷に悪影響を与えることなく、正確に求めるこ
とができる。
Also, in the case of claim 2, the admittance of the measured harmonic on the target side of the power system 1 obtained in the same manner as in the case of claim 1 and the voltage of the measured harmonic of the power system 1,
Based on the current measurement result, a current source of a measurement harmonic parallel to the admittance on the target side of the power system 1 can be obtained, and a measurement source including a parallel circuit of the admittance and the current source on the target side of the power system 1 can be obtained. An equivalent circuit for the wave can be obtained accurately without adversely affecting the load of the power system 1.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明の実施の1形態の回路ブロック図であ
る。
FIG. 1 is a circuit block diagram of one embodiment of the present invention.

【図2】図1の電力系統の高調波等価回路図である。FIG. 2 is a harmonic equivalent circuit diagram of the power system of FIG.

【図3】図1の注入電流決定処理のフローチャートであ
る。
FIG. 3 is a flowchart of an injection current determination process of FIG. 1;

【図4】図1の注入電流の決定説明用の第1の等価回路
図である。
FIG. 4 is a first equivalent circuit diagram for explaining the determination of an injection current in FIG. 1;

【図5】共振特性の測定図である。FIG. 5 is a measurement diagram of resonance characteristics.

【図6】図1の注入電流の決定説明用の第2の等価回路
図である。
FIG. 6 is a second equivalent circuit diagram for explaining the determination of the injection current in FIG. 1;

【符号の説明】[Explanation of symbols]

1 電力系統 4 高調波注入点 5 計測装置 19,20 等価回路 Reference Signs List 1 power system 4 harmonic injection point 5 measuring device 19, 20 equivalent circuit

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 志方 俊彦 京都市右京区梅津高畝町47番地 日新電機 株式会社内Continued on the front page (72) Inventor Shoji Nishimura, 47, Umezu Takaune-cho, Ukyo-ku, Kyoto-shi Nissin Electric Co., Ltd. Inventor Toshihiko Shikata 47, Umezu Takaune-cho, Ukyo-ku, Kyoto Nissin Electric Co., Ltd.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 電力系統の基本波の整数倍周波数の高調
波を測定調波とし、 前記電力系統の高調波注入点に前記測定調波の上,下両
側それぞれの前記基本波の非整数倍周波数の電流を徐々
に増加しながら注入し、 前記測定調波の上,下両側それぞれの注入電流に基づく
前記高調波注入点の注入周波数の歪み電圧を計測し、 前記歪み電圧がほぼ所定の上限電圧に上昇したときに前
記注入電流の増加を停止して高調波測定に移行し、 前記測定調波の上,下両側それぞれの前記注入電流に基
づく前記高調波注入点の電圧及び前記電力系統の前記高
調波注入点より上位,下位の少なくとも一方の電流の計
測結果から前記上位,前記下位の少なくとも一方からな
る前記電力系統の注目側の前記測定調波の上,下両側の
前記注入電流についての等価回路のアドミタンスを算出
し、 前記測定調波の上,下両側の注入電流についての算出し
たアドミタンスに基づく補間処理により、前記注目側の
前記測定調波についての等価回路のアドミタンスを求め
て決定することを特徴とする電力系統の高調波測定方
法。
1. A harmonic having an integral multiple of a fundamental frequency of a power system as a measurement harmonic, and a non-integer multiple of the fundamental wave on each of the upper and lower sides of the measurement harmonic at a harmonic injection point of the power system. Injecting while gradually increasing the frequency current, measuring the distortion voltage of the injection frequency at the harmonic injection point based on the injection currents on both the upper and lower sides of the measurement harmonic, wherein the distortion voltage is substantially a predetermined upper limit. When the voltage rises to a voltage, the increase of the injection current is stopped, and the operation shifts to harmonic measurement. The voltage of the harmonic injection point based on the injection current on each of the upper and lower sides of the measurement harmonic and the power system From the measurement results of at least one of the higher and lower currents from the harmonic injection point, the measured values of the injection current on the upper and lower sides of the measurement harmonic on the attention side of the power system, which is composed of at least the upper and lower ones, Equivalent circuit Calculating an admittance, and determining and determining an admittance of an equivalent circuit for the measurement harmonic on the side of interest by performing an interpolation process based on the calculated admittance for the injection currents above and below the measurement harmonic. Power system harmonic measurement method.
【請求項2】 電力系統の基本波の整数倍周波数の高調
波を測定調波とし、 前記電力系統の高調波注入点に、前記測定調波の上,下
両側それぞれの前記基本波の非整数倍周波数の電流を徐
々に増加しながら注入し、 前記測定調波の上,下両側それぞれの注入電流にもとづ
く前記高調波注入点の注入周波数の歪み電圧を計測し、 前記歪み電圧がほぼ所定の上限電圧に上昇したときに前
記注入電流の増加を停止して高調波測定に移行し、 前記測定調波の上,下両側それぞれの前記注入電流に基
づく前記高調波注入点の電圧及び前記電力系統の前記高
調波注入点より上位,下位の少なくとも一方の電流の計
測結果から前記上位,前記下位の少なくとも一方からな
る前記電力系統の注目側の前記測定調波の上,下両側の
前記注入電流についての等価回路のアドミタンスを算出
し、 前記測定調波の上,下両側の前記注入電流についての算
出したアドミタンスに基づく補間処理により、前記注目
側の前記測定調波についての等価回路のアドミタンスを
求めて決定し、 前記測定調波についての決定したアドミタンスと,前記
高調波注入点の前記電力系統の前記測定調波の電圧及び
電流の計測結果とにより、前記注目側の前記測定調波に
ついての前記等価回路の電流源を求めて決定し、 決定した前記アドミタンスと前記電流源との並列回路に
より前記注目側の前記測定調波についての前記等価回路
を求めることを特徴とする電力系統の高調波測定方法。
2. A harmonic which is an integral multiple of a fundamental frequency of a power system as a measurement harmonic, and a non-integer of the fundamental wave on each of upper and lower sides of the measurement harmonic is added to a harmonic injection point of the power system. Injecting while gradually increasing the current of the double frequency, measuring the distortion voltage of the injection frequency at the harmonic injection point based on the injection current on each of the upper and lower sides of the measurement harmonic, wherein the distortion voltage is substantially predetermined. When the voltage rises to the upper limit voltage, the injection current stops increasing and shifts to harmonic measurement. The voltage at the harmonic injection point based on the injection currents on the upper and lower sides of the measurement harmonic and the power system From the measurement results of at least one of the higher and lower currents above the harmonic injection point of the injection current on the upper and lower sides of the measurement harmonic on the side of interest of the power system comprising at least the upper and lower ones The equivalent of The admittance of the path is calculated, and the admittance of the equivalent circuit for the measurement harmonic on the side of interest is determined and determined by interpolation processing based on the calculated admittance of the injection current on the upper and lower sides of the measurement harmonic. The determined admittance of the measured harmonic and the measurement result of the voltage and current of the measured harmonic of the power system at the harmonic injection point, the equivalent circuit of the measured harmonic on the side of interest. A method for measuring harmonics in a power system, comprising determining and determining a current source, and determining the equivalent circuit for the measurement harmonic on the side of interest using a parallel circuit of the determined admittance and the current source.
JP9180573A 1997-06-19 1997-06-19 Power system harmonic measurement method Pending JPH1114675A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP9180573A JPH1114675A (en) 1997-06-19 1997-06-19 Power system harmonic measurement method
US09/099,381 US6208945B1 (en) 1997-06-19 1998-06-18 Harmonic component measuring method for power system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9180573A JPH1114675A (en) 1997-06-19 1997-06-19 Power system harmonic measurement method

Publications (1)

Publication Number Publication Date
JPH1114675A true JPH1114675A (en) 1999-01-22

Family

ID=16085647

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9180573A Pending JPH1114675A (en) 1997-06-19 1997-06-19 Power system harmonic measurement method

Country Status (1)

Country Link
JP (1) JPH1114675A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114301055A (en) * 2022-02-17 2022-04-08 河海大学 Method and system for obtaining inter-harmonic power flow of power system based on broadband measurement

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114301055A (en) * 2022-02-17 2022-04-08 河海大学 Method and system for obtaining inter-harmonic power flow of power system based on broadband measurement

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