JPH08110359A - Method for measuring momentary value of polyphase voltage - Google Patents

Method for measuring momentary value of polyphase voltage

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Publication number
JPH08110359A
JPH08110359A JP27296594A JP27296594A JPH08110359A JP H08110359 A JPH08110359 A JP H08110359A JP 27296594 A JP27296594 A JP 27296594A JP 27296594 A JP27296594 A JP 27296594A JP H08110359 A JPH08110359 A JP H08110359A
Authority
JP
Japan
Prior art keywords
voltage
polyphase
fundamental wave
value
wave voltage
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
JP27296594A
Other languages
Japanese (ja)
Inventor
Hiroshi Yokose
宏 横瀬
Yoshio Yokose
義雄 横瀬
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.)
Individual
Original Assignee
Individual
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Filing date
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Application filed by Individual filed Critical Individual
Priority to JP27296594A priority Critical patent/JPH08110359A/en
Publication of JPH08110359A publication Critical patent/JPH08110359A/en
Pending legal-status Critical Current

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Abstract

PURPOSE: To establish a method for accurately measuring the momentary value of the maximum value of a fundamental wave voltage in a polyphase voltage containing high harmonic voltages and at the same time obtain the momentary value of the polyphase fundamental wave voltage by utilizing the value for applying to the control of an AC electrical equipment. CONSTITUTION: By converting a polyphase voltage 1 onto α-βplane by α βconversion 2, a rotary vector whose amplitude is equal to that of the polyphase voltage can be obtained. By converting the rotary vector onto α'-β' plane of rotary coordinates 3 which rotate at the same angular velocity as the polyphase voltage 1 and averaging the components of α' axis and β' axis on the rotary coordinates independently on time axis by time averaging 4, the influence of high harmonic voltage can be eliminated. By performing amplitude calculation 5 using two components of α' axis and β' axis which are averaged on time axis, a momentary value 8 of the maximum value of the fundamental wave voltage in the polyphase voltage can be obtained. Further, the momentary value of a polyphase fundamental wave voltage 9 is obtained by a rotary coordinate inverse conversion 6 and αβ inverse conversion 7.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は高調波電圧を含む多相電
圧の制御、例えばパワ−・アクティブ・フィルター、お
よび交流電圧の振幅の制御に必要な多相電圧中の基本波
電圧の最大値の瞬時値および多相基本波電圧の瞬時値の
検出方法に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the control of multi-phase voltages including harmonic voltages, for example power active filters, and the maximum value of the fundamental wave voltage in the multi-phase voltages required for controlling the amplitude of alternating voltage. The present invention relates to a method for detecting the instantaneous value of and the instantaneous value of the polyphase fundamental wave voltage.

【0002】[0002]

【従来の技術】特開平1−311286に示されるよう
に正弦波交流電圧の最大値の瞬時値の計測方法は、整流
器により直流電圧に変換して零クロスの点からの任意時
間後の値を測定することで最大値の瞬時値を計算する方
法、また、特開平3−39659、特開平3−2525
60、特開平3−39661等のように、被測定交流電
圧の任意の一定間隔の3点のデータから最大値の瞬時値
を計算する方法が取られていた。しかし、パワー・アク
ティブ・フィルター、および交流電圧の振幅制御におい
ては、交流電圧の最大値および基本波電圧の瞬時値を使
った制御が必要とされ、また取り扱う交流電圧の殆どが
高調波電圧を含んでいるために、被測定交流電圧が正弦
波であると仮定した上記の測定方法では高調波電圧によ
る誤差を発生する。
2. Description of the Related Art As disclosed in Japanese Patent Laid-Open No. 1-311286, a method of measuring an instantaneous value of a maximum value of a sine wave AC voltage is converted into a DC voltage by a rectifier, and a value after an arbitrary time from a point of zero crossing A method of calculating the instantaneous value of the maximum value by measuring, and further, JP-A-3-39659 and JP-A-3-2525.
No. 60, JP-A-3-39661, etc., a method of calculating the instantaneous value of the maximum value from the data of three points of the measured AC voltage at arbitrary fixed intervals has been adopted. However, in the power active filter and the amplitude control of the AC voltage, control using the maximum value of the AC voltage and the instantaneous value of the fundamental wave voltage is required, and most of the AC voltage handled includes harmonic voltage. Therefore, the above-mentioned measurement method assuming that the measured AC voltage is a sine wave causes an error due to the harmonic voltage.

【0003】[0003]

【発明が解決しようとする課題】そこで、本発明の目的
は高調波電圧を含む多相電圧中の基本波電圧の最大値の
瞬時値の測定方法を開発すると共に、多相基本波電圧の
瞬時値を出力することのできるシステムを提供すること
により、交流電気機器の制御方法を改良することにあ
る。
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to develop a method of measuring the instantaneous value of the maximum value of the fundamental wave voltage in the polyphase voltage including the harmonic voltage, and to determine the instantaneous value of the polyphase fundamental wave voltage. An object of the present invention is to improve a control method of an AC electric device by providing a system capable of outputting a value.

【0004】[0004]

【課題を解決するための手段】本発明多相電圧中の基本
波電圧の最大値の瞬時値と多相基本波電圧の瞬時値の測
定方法は図1に示す如く、多相電圧1をαβ変換2、回
転座標変換3により静止ベクトルに変換して、時間平均
4により高調波電圧を除去して、多相電圧中の基本波電
圧の最大値の瞬時値である最大値の瞬時値8を振幅計算
5により求める。また、時間平均4により高調波電圧を
除去した値を回転座標逆変換6とαβ逆変換7の変換を
行うことにより、多相基本波電圧9の瞬時値を得る。以
下、これを3相電圧を使って説明する。今、3相電圧の
基本波電圧をVa(t),Vb(t),Vc(t)とし
て、これに高調波電圧Vha(t),Vhb(t),V
hc(t)が含まれているとすれば、これらの電圧のα
β変換は、
As shown in FIG. 1, the method for measuring the instantaneous value of the maximum value of the fundamental wave voltage in the polyphase voltage and the instantaneous value of the polyphase fundamental wave voltage according to the present invention is as follows. Conversion 2 and rotation coordinate conversion 3 convert to a static vector, time average 4 removes the harmonic voltage, and the maximum instantaneous value 8 which is the maximum instantaneous value of the fundamental wave voltage in the multi-phase voltage Calculated by amplitude calculation 5. Further, the value obtained by removing the harmonic voltage by the time average 4 is converted by the rotational coordinate reverse conversion 6 and the αβ reverse conversion 7 to obtain the instantaneous value of the multiphase fundamental wave voltage 9. Hereinafter, this will be described using a three-phase voltage. Now, assuming that the fundamental wave voltage of the three-phase voltage is Va (t), Vb (t), Vc (t), the harmonic voltage Vha (t), Vhb (t), V
If hc (t) is included, α of these voltages
β conversion is

【数1】 で表す事ができる。これより3相電圧の最大値の瞬時値
Vem(t)は、
[Equation 1] Can be expressed as From this, the instantaneous value Vem (t) of the maximum value of the three-phase voltage is

【数2】 で求めることができる。ただし第(1)式中の右辺第1
項は3相電圧の基本波電圧であり、また同第2項に含ま
れている高調波電圧は、
[Equation 2] Can be obtained by However, the first on the right side of the equation (1)
The term is the fundamental wave voltage of the three-phase voltage, and the harmonic voltage included in the second term is

【数3】 で表せるとする。ここで、第(1)式が図1に示したα
β変換2に相当し、多相電圧の最大値の瞬時値は第
(2)式で求まる。ところが、多相電圧に高調波電圧が
含まれているために、第(2)式の計算値は高調波電圧
も含めて求まるので、多相電圧中の基本波電圧の最大値
の瞬時値とは一致しなくなる。これを補正するために、
図1に示した次の方法で、高調波電圧により発生する誤
差の補正を行なう。
(Equation 3) Can be expressed as Here, the expression (1) is α shown in FIG.
Corresponding to β conversion 2, the instantaneous value of the maximum value of the multiphase voltage is obtained by the equation (2). However, since the polyphase voltage includes the harmonic voltage, the calculated value of the equation (2) can be obtained by including the harmonic voltage. Therefore, the instantaneous value of the maximum value of the fundamental wave voltage in the polyphase voltage is calculated. Will not match. To compensate for this,
The following method shown in FIG. 1 corrects the error generated by the harmonic voltage.

【0005】第(1)式の計算値Vαx(t)とVβx
(t)は、それぞれα−β平面上のα軸とβ軸の成分で
ある。この成分をα軸とβ軸上のベクトルの成分と考え
て、これ等を合成すると回転ベクトルを得る。更に、多
相電圧1中の基本波電圧の角周波数と同一速度で回転す
る回転座標α’−β’平面を考えて、上記の回転ベクト
ルをこの平面上に変換すると、
Calculated values Vαx (t) and Vβx of the equation (1)
(T) are components of the α axis and the β axis on the α-β plane, respectively. Considering this component as a vector component on the α axis and the β axis, and combining these components, a rotation vector is obtained. Furthermore, considering a rotation coordinate α′-β ′ plane that rotates at the same speed as the angular frequency of the fundamental wave voltage in the multiphase voltage 1, and converting the above rotation vector onto this plane,

【数4】 になる。ところが、第(4)式で変換されたベクトルは
図2のように回転座標α’−β’平面上でベクトル軌跡
を描く。このベクトル軌跡が高調波電圧によって発生す
る誤差になる。そこで、この誤差を除去するためにα’
軸の成分Vαx’(t)とβ’軸の成分Vβx’(t)
を、次式のように時間平均すると、
[Equation 4] become. However, the vector converted by the equation (4) draws a vector locus on the rotation coordinate α′-β ′ plane as shown in FIG. This vector locus becomes an error generated by the harmonic voltage. Therefore, in order to remove this error, α '
Axis component Vαx '(t) and β'axis component Vβx' (t)
Is time-averaged as

【数5】 となる。これは図1の時間平均4により、平均値Vα
m’(t)とVβm’(t)を求めることになる。これ
らの時間平均した2値を使って、ベクトルの大きさVo
p(t)を求めると、
(Equation 5) Becomes This is the average value Vα according to the time average 4 in FIG.
m ′ (t) and Vβm ′ (t) will be obtained. By using these two time-averaged values, the vector magnitude Vo
When p (t) is calculated,

【数6】 となり、この値が多相電圧中の基本波電圧の最大値の瞬
時値8を与える。これをベクトル表示したのが図2の中
にVop(t)と記した時間平均した多相電圧のベクト
ル12である。
(Equation 6) This value gives the instantaneous value 8 of the maximum value of the fundamental wave voltage in the multiphase voltage. The vector display of this is a time-averaged multi-phase voltage vector 12 indicated by Vop (t) in FIG.

【0006】上記のように時間平均4により得た平均値
Vαm’(t)とVβm’(t)は高調波電圧を除去し
たα’軸とβ’軸の成分である。この成分は第(1)式
の右辺第2項の高調波電圧を除去した残りの3相電圧中
の基本波電圧に等しい。したがって、上記の平均値Vα
m’(t)とVβm’(t)を回転座標からα−β平面
に変換して、更に多相座標に変換すると、3相基本波電
圧を求めることができる。この変換の内、回転座標から
α−β平面への変換は、
As described above, the average values Vαm '(t) and Vβm' (t) obtained by the time average 4 are components of the α'axis and the β'axis from which the harmonic voltage is removed. This component is equal to the fundamental wave voltage in the remaining three-phase voltage after removing the harmonic voltage of the second term on the right side of the equation (1). Therefore, the above average value Vα
By converting m ′ (t) and Vβm ′ (t) from the rotating coordinates into the α-β plane and further into the polyphase coordinates, the three-phase fundamental voltage can be obtained. Of these transformations, the transformation from rotational coordinates to the α-β plane is

【数7】 により行える。第(7)式は図1の回転座標逆変換6を
求める計算である。更に、α−β平面から多相座標への
変換は、
(Equation 7) Can be done by Expression (7) is a calculation for obtaining the inverse rotation coordinate transformation 6 of FIG. Furthermore, the conversion from α-β plane to polyphase coordinates is

【数8】 のように表せる。第(8)式は3相基本波電圧Va1
(t),Vb1(t),Vc1(t)を表しており、図
1のαβ逆変換7の計算によって得ることができる。
(Equation 8) Can be expressed as Formula (8) is the three-phase fundamental wave voltage Va1.
(T), Vb1 (t), and Vc1 (t) are represented and can be obtained by calculation of the αβ inverse transform 7 of FIG.

【0007】[0007]

【作用】本発明に依れば高調波電圧を含む多相電圧中の
基本波電圧の最大値の瞬時値と多相基本波電圧の瞬時値
の測定方法は、図1の多相電圧1をαβ変換2により回
転ベクトルに変換して、上記多相電圧中の基本波電圧と
同一角周波数で回転する回転座標に回転座標変換4で変
換して得たベクトルを、時間平均4で時間平均すること
により高調波電圧を除去したベクトルが求まる。このベ
クトルの大きさを振幅計算5により最大値の瞬時値8と
して得る。一方、上記時間平均4で求めたベクトルの成
分を、回転座標逆変換6によりαβ座標に変換した後
に、αβ逆変換7により多相座標に変換すると、高調波
電圧を除去した多相基本波電圧9を得る。更に、上記の
多相電圧中の基本波電圧の最大値の瞬時値と多相基本波
電圧の瞬時値の測定方法を、交流電気機器の制御に応用
すると、有効な制御システムを構成できる。
According to the present invention, the method for measuring the instantaneous value of the maximum value of the fundamental wave voltage and the instantaneous value of the polyphase fundamental wave voltage in the multiphase voltage including the harmonic voltage is as follows. The vector obtained by converting into the rotation vector by the αβ conversion 2 and converted into the rotation coordinate that rotates at the same angular frequency as the fundamental wave voltage in the multiphase voltage by the rotation coordinate conversion 4 is time averaged by the time average 4. As a result, a vector with the harmonic voltage removed can be obtained. The magnitude of this vector is obtained as the maximum instantaneous value 8 by the amplitude calculation 5. On the other hand, when the vector component obtained by the time average 4 is converted into αβ coordinates by the rotating coordinate inverse transform 6 and then converted into polyphase coordinates by the αβ inverse transform 7, the harmonic voltage is removed to obtain the polyphase fundamental wave voltage. Get 9. Furthermore, an effective control system can be configured by applying the above-described method of measuring the maximum value of the fundamental wave voltage in the polyphase voltage and the instantaneous value of the polyphase fundamental wave voltage to the control of the AC electric equipment.

【0008】[0008]

【実施例】図1は本発明の多相電圧の瞬時値の測定法の
概略図で、多相電圧中の基本波電圧の最大値の瞬時値を
求める方法と、多相基本波電圧の瞬時値を求める方法を
示している。まず、多相電圧中の基本波電圧の最大値の
瞬時値を求める方法は、多相電圧1をαβ変換2で計算
して回転ベクトルを得る。この回転ベクトルの大きさは
多相電圧の振幅に等しく、このベクトルの大きさを測る
ことで、高調波電圧を含んだ多相電圧の最大値の瞬時値
を求める事ができる。しかし、多くの場合は、高調波電
圧を除いた最大値の瞬時値を必要とする。ここでは高調
波電圧を除去するために、回転ベクトルを回転座標上へ
変換して静止させた後に、時間平均する方法を使用す
る。この操作は図1の回転座標変換3と時間平均4で行
う。これにより得た結果を振幅計算5で計算すると、高
調波電圧を含まない最大値の瞬時値を得る事ができる。
FIG. 1 is a schematic diagram of a method for measuring an instantaneous value of a polyphase fundamental voltage according to the present invention. A method for obtaining an instantaneous value of the maximum value of the fundamental wave voltage in the polyphase voltage and an instantaneous value of the polyphase fundamental wave voltage. It shows how to find the value. First, in the method of obtaining the instantaneous value of the maximum value of the fundamental wave voltage in the multiphase voltage, the multiphase voltage 1 is calculated by the αβ conversion 2 to obtain the rotation vector. The magnitude of this rotation vector is equal to the amplitude of the multi-phase voltage, and by measuring the magnitude of this vector, the instantaneous value of the maximum value of the multi-phase voltage including the harmonic voltage can be obtained. However, in many cases, the maximum instantaneous value excluding the harmonic voltage is required. Here, in order to remove the harmonic voltage, a method of converting the rotation vector onto the rotation coordinate and making it stand still, and then performing time averaging is used. This operation is performed by the rotational coordinate conversion 3 and the time average 4 in FIG. When the obtained result is calculated by the amplitude calculation 5, the maximum instantaneous value that does not include the harmonic voltage can be obtained.

【0009】次に多相基本波電圧の瞬時値の求め方につ
いて説明する。図1において時間平均4の出力は、高調
波電圧を含んでいないので、この出力をα−β平面へ変
換して、更に多相座標へ戻すと、多相基本波電圧の瞬時
値を得る事ができる。この操作は図1の回転座標逆変換
6がα−β平面への変換を受け持ち、αβ逆変換7で多
相座標に変換された多相基本波電圧9を得る。
Next, how to obtain the instantaneous value of the polyphase fundamental wave voltage will be described. In FIG. 1, the output of time average 4 does not include the harmonic voltage, so if this output is converted to the α-β plane and returned to the polyphase coordinates, the instantaneous value of the polyphase fundamental wave voltage is obtained. You can In this operation, the inverse rotation coordinate transformation 6 in FIG. 1 takes charge of the transformation into the α-β plane, and the αβ inverse transformation 7 obtains the polyphase fundamental wave voltage 9 transformed into the polyphase coordinates.

【0010】以上に示した多相電圧中の基本波電圧の最
大値の瞬時値と多相基本波電圧の瞬時値の測定方法を、
商用3相電圧の測定に使用した実験結果を次に示す。測
定した3相電圧は、3相200Vの商用電圧で、これに
含まれている高調波電圧は、第5調波電圧が約1.9
%、第7調波電圧が約1.2%で、この他高次の高調波
電圧を含んでいるが、測定誤差範囲内であるため省略し
た。また第3調波電圧の含有量は計器用変圧器を△結線
としたゝめ、第5調波電圧と第7調波電圧に対して無視
できるオーダであった。さらに基本波電圧の不平衡成分
も、最大値の測定値に影響を与えない大きさであった。
図3の商用3相電圧14は測定した商用3相電圧の各相
の電圧波形を示している。この電圧を第(1)式と第
(2)式で最大値の瞬時値の計算をした結果が、図3の
2段目の最大値の瞬時値15の曲線である。図に示すよ
うに、その測定値は第6調波成分を最も多く含み、約±
2.6%の大きさの誤差を発生している。同様に図3の
3段目に示した曲線は、第(6)式を使って求めた商用
3相電圧中の基本波電圧の最大値の瞬時値16の特性で
ある。この曲線は高調波電圧の除去を行っているため
に、その誤差は±0.28%と第(2)式を使って求め
た結果に比べて高精度な結果を得た。以上に最大値の瞬
時値の測定例を示したが、図3の最下段の波形は、第
(8)式を使って図3の最上段に示した商用3相電圧か
ら得た3相基本波電圧17の波形を示したものである。
この波形は歪率±0.8%以内に収まっており、高精度
な3相基本波電圧波形である。
The above-described method for measuring the instantaneous value of the maximum value of the fundamental wave voltage in the polyphase voltage and the instantaneous value of the polyphase fundamental wave voltage is
The experimental results used for measuring the commercial three-phase voltage are shown below. The measured three-phase voltage is a commercial voltage of three-phase 200V, and the harmonic voltage contained in this is a fifth harmonic voltage of about 1.9.
%, The 7th harmonic voltage is about 1.2%, and other high-order harmonic voltages are included, but they are omitted because they are within the measurement error range. The content of the 3rd harmonic voltage was in the order that can be ignored for the 5th harmonic voltage and the 7th harmonic voltage, because the transformer for the instrument was Δ-connected. Furthermore, the unbalanced component of the fundamental wave voltage was of a magnitude that did not affect the maximum measured value.
The commercial three-phase voltage 14 in FIG. 3 indicates the voltage waveform of each phase of the measured commercial three-phase voltage. The result of calculating the instantaneous value of the maximum value of this voltage by the equations (1) and (2) is the curve of the instantaneous value 15 of the maximum value in the second stage of FIG. As shown in the figure, the measured value contains the sixth harmonic component most, and is about ±
There is an error of 2.6%. Similarly, the curve shown in the third row of FIG. 3 is the characteristic of the instantaneous value 16 of the maximum value of the fundamental wave voltage in the commercial three-phase voltage obtained by using the equation (6). Since the harmonic voltage is removed from this curve, the error is ± 0.28%, which is a highly accurate result compared with the result obtained by using the equation (2). The measurement example of the maximum instantaneous value is shown above, but the waveform at the bottom of FIG. 3 shows the basic three-phase voltage obtained from the commercial three-phase voltage shown at the top of FIG. The waveform of the wave voltage 17 is shown.
This waveform is within a distortion rate of ± 0.8% and is a highly accurate three-phase fundamental wave voltage waveform.

【0011】[0011]

【発明の効果】以上に説明した如く、本発明によれば高
調波電圧を含む多相電圧をαβ変換した後に、回転座標
上で時間平均すると高調波電圧を除去できることを利用
して、多相電圧中の基本波電圧の最大値の瞬時値を正確
に求めることが出来る。また、上記の高調波電圧除去の
方法を利用して、多相基本波電圧の瞬時値を求めること
も出来る。そのため、この方法を交流電気機器の制御に
利用することにより、良質な制御システムを構成でき
る。
As described above, according to the present invention, it is possible to remove the harmonic voltage by averaging the multiphase voltage including the harmonic voltage on the rotating coordinates after αβ conversion. The instantaneous value of the maximum value of the fundamental wave voltage in the voltage can be accurately obtained. Further, it is also possible to obtain the instantaneous value of the multiphase fundamental wave voltage by utilizing the above method of removing the harmonic voltage. Therefore, a high-quality control system can be constructed by using this method for controlling AC electric equipment.

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

【図1】本発明の多相電圧中の基本波電圧の最大値の瞬
時値と多相基本波電圧の瞬時値の測定方法の実施例を示
す図
FIG. 1 is a diagram showing an embodiment of a method for measuring an instantaneous value of a maximum value of a fundamental wave voltage in a polyphase voltage and an instantaneous value of a polyphase fundamental wave voltage of the present invention.

【図2】高調波電圧により発生する誤差と本発明の時間
平均による誤差の除去方法
FIG. 2 is a diagram showing a method of removing an error caused by a harmonic voltage and an error by time averaging according to the present invention.

【図3】本発明の方法を使って商用3相電圧中の基本波
電圧の最大値の瞬時値と3相基本波電圧の瞬時値を測定
した例
FIG. 3 is an example in which the instantaneous value of the maximum value of the fundamental wave voltage in a commercial three-phase voltage and the instantaneous value of the three-phase fundamental wave voltage are measured using the method of the present invention.

【符号の説明】[Explanation of symbols]

1 被測定多相電圧 2 第(1)式を使ったαβ変換の計算 3 第(4)式を使った回転座標変換の計算 4 第(5)式を使ったα’軸とβ’軸の成分の時間平
均の計算 5 第(6)式を使った最大値の瞬時値の計算 6 第(7)式を使った回転座標逆変換の計算 7 第(8)式を使ったαβ座標から多相座標への変換
の計算 8 多相電圧中の基本波電圧の最大値の瞬時値 9 多相基本波電圧の瞬時値 10 高調波電圧が描くベクトル軌跡 11 時間tにおける多相電圧のベクトル 12 時間平均した多相電圧のベクトル 13 時間tiにおける多相電圧のベクトル 14 商用3相電圧の波形 15 第(2)式で求めた商用3相電圧の最大値の瞬時
値Vem(t) 16 第(6)式で求めた商用3相電圧中の基本波電圧
の最大値の瞬時値Vop(t) 17 第(8)式で求めた3相基本波電圧
1 Measured multi-phase voltage 2 Calculation of αβ conversion using formula (1) 3 Calculation of rotational coordinate conversion using formula (4) 4 Calculation of α'axis and β'axis using formula (5) Calculation of time average of components 5 Calculation of instantaneous value of maximum value using formula (6) 6 Calculation of inverse rotation coordinate conversion using formula (7) 7 Calculation from αβ coordinates using formula (8) Calculation of conversion to phase coordinates 8 Instantaneous value of maximum value of fundamental wave voltage in polyphase voltage 9 Instantaneous value of polyphase fundamental wave voltage 10 Vector locus drawn by harmonic voltage 11 Vector of polyphase voltage at t 12 hours Averaged vector of multi-phase voltage 13 Vector of multi-phase voltage at time ti 14 Waveform of commercial three-phase voltage 15 Instantaneous value Vem (t) 16 No. (6) of the maximum value of commercial three-phase voltage obtained by the equation (2) The instantaneous value Vop (t) 17 of the maximum value of the fundamental wave voltage in the commercial three-phase voltage obtained by the equation) was obtained by the equation (8). Phase fundamental voltage

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】αβ変換を使って高調波電圧を含む多相電
圧中の基本波電圧の最大値の瞬時値と多相基本波電圧の
瞬時値を求める方法に於いて、上記高調波電圧を含む多
相電圧をαβ変換によりα−β平面上で回転する回転ベ
クトルに変換して、上記の高調波電圧を含む多相電圧中
の基本波電圧の角周波数と同一角速度で回転する回転座
標のα’−β’平面上へ変換した後に、α’軸とβ’軸
の2成分の時間平均により高調波電圧を消去した値を求
め、その値から多相電圧中の基本波電圧の最大値の瞬時
値を求めると共に、上記時間平均した2成分を使って、
逆変換により多相基本波電圧の瞬時値を求めることを特
徴とする多相電圧中の基本波電圧の最大値の瞬時値と多
相基本波電圧の瞬時値の測定方法。
1. A method for obtaining an instantaneous value of a maximum value of a fundamental wave voltage in a polyphase voltage including a harmonic wave voltage and an instantaneous value of the polyphase fundamental wave voltage by using αβ conversion, wherein By converting the multi-phase voltage containing to the rotation vector that rotates on the α-β plane by αβ conversion, the rotation frequency of the rotation frequency that rotates at the same angular velocity as the angular frequency of the fundamental wave voltage in the multi-phase voltage including the above harmonic voltage After converting to the α'-β 'plane, the value obtained by eliminating the harmonic voltage by the time average of the two components of the α'axis and β'axis is obtained, and from that value, the maximum value of the fundamental wave voltage in the multiphase voltage In addition to finding the instantaneous value of, using the two components averaged over time,
A method for measuring the instantaneous value of the maximum value of the fundamental wave voltage in the polyphase voltage and the instantaneous value of the polyphase fundamental wave voltage, wherein the instantaneous value of the polyphase fundamental wave voltage is obtained by inverse conversion.
JP27296594A 1994-10-11 1994-10-11 Method for measuring momentary value of polyphase voltage Pending JPH08110359A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP27296594A JPH08110359A (en) 1994-10-11 1994-10-11 Method for measuring momentary value of polyphase voltage

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP27296594A JPH08110359A (en) 1994-10-11 1994-10-11 Method for measuring momentary value of polyphase voltage

Publications (1)

Publication Number Publication Date
JPH08110359A true JPH08110359A (en) 1996-04-30

Family

ID=17521263

Family Applications (1)

Application Number Title Priority Date Filing Date
JP27296594A Pending JPH08110359A (en) 1994-10-11 1994-10-11 Method for measuring momentary value of polyphase voltage

Country Status (1)

Country Link
JP (1) JPH08110359A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2001002870A1 (en) * 1999-07-02 2001-01-11 General Electric Company Method and apparatus for real time measurement of three phase electrical parameters

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2001002870A1 (en) * 1999-07-02 2001-01-11 General Electric Company Method and apparatus for real time measurement of three phase electrical parameters
JP2003504599A (en) * 1999-07-02 2003-02-04 ゼネラル・エレクトリック・カンパニイ Method and apparatus for real-time measurement of three-phase electrical parameters
JP4993153B2 (en) * 1999-07-02 2012-08-08 ゼネラル・エレクトリック・カンパニイ Method and apparatus for real-time measurement of three-phase electrical parameters

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