JP3326763B2 - How to measure complex power - Google Patents

How to measure complex power

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Publication number
JP3326763B2
JP3326763B2 JP32639894A JP32639894A JP3326763B2 JP 3326763 B2 JP3326763 B2 JP 3326763B2 JP 32639894 A JP32639894 A JP 32639894A JP 32639894 A JP32639894 A JP 32639894A JP 3326763 B2 JP3326763 B2 JP 3326763B2
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JP
Japan
Prior art keywords
power
vrx
resistor
calculated
load
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.)
Expired - Fee Related
Application number
JP32639894A
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Japanese (ja)
Other versions
JPH08184617A (en
Inventor
功 山口
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.)
Tokai University Educational Systems
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Tokai University Educational Systems
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Description

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

【0001】[0001]

【産業上の利用分野】本発明は有効電力と無効電力より
なる複素電力を計測する計測方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a measuring method for measuring complex power consisting of active power and reactive power.

【0002】[0002]

【従来の技術】従来の電力計は有効電力のみを測定する
計器であるが、接続法を変更して無効電力計としても使
用されている。従来の電力計による有効電力の測定にお
いては正の有効電力、即ち消費電力の測定であって、負
の消費電力、即ち受給電力の場合は計器の指針が逆振れ
するため、正常な指針の振れとなるように接続を変えて
測定している。
2. Description of the Related Art A conventional wattmeter is an instrument for measuring only active power, but is also used as a reactive power meter by changing a connection method. In the measurement of active power by a conventional wattmeter, the measurement of the positive active power, that is, the power consumption, is negative. The measurement is performed by changing the connection so that

【0003】[0003]

【発明が解決しようとする課題】上述の従来の電力計に
よる無効電力の測定では無効電力値そのものは測定出来
るが、その無効電力が進みか遅れかの判定は出来ない。
即ち、一般に複素電力を Pl =Pa +jPr と表示
するとき、従来の電力計では有効電力Pa と無効電力P
r を同時に測定することは出来ず、更にPr の正負の判
定が出来ない。
In the above-described measurement of reactive power by the conventional wattmeter, the reactive power itself can be measured, but it cannot be determined whether the reactive power is advanced or delayed.
That is, generally, when the complex power is expressed as Pl = Pa + jPr, the active power Pa and the reactive power P
r cannot be measured at the same time, and furthermore, the positive / negative judgment of Pr cannot be made.

【0004】三相電力回路では、三相電源又は三相負荷
の不平衡により、各相の電源が分担している複素電力及
び各相負荷の複素電力も不平衡となり、複素電力の正確
な測定が出来ない。特に、三相不平衡負荷側の構成素子
値が未知である場合は電源側からみた等価回路はブラッ
クボックスと考えざるを得ない。その場合の三相電力測
定値は物理的に何を表しているのか判明出来ない。
In a three-phase power circuit, due to the unbalance of the three-phase power supply or the three-phase load, the complex power shared by the power supplies of each phase and the complex power of each phase load also become unbalanced, and the complex power is accurately measured. Can not do. In particular, when the component values on the three-phase unbalanced load side are unknown, the equivalent circuit viewed from the power supply side must be considered as a black box. In such a case, it is impossible to determine what the three-phase power measurement value physically represents.

【0005】具体的には、三相リニアモータ(LIM)
は構造に起因する端効果のため、電源側からはパラメー
タ値が未知なブラックボックスと見なされている。この
LIMを詳細に解析する上で、三相等価回路のパラメー
タ値算定は現在注目されているものの、動作時の電力と
して、複素量の電力 Pl =Pa +jPr を測定しな
ければならない。特に、LIMの運転制御には複素量の
電力測定が不可欠であり、更に実際のLIMの運転は低
周波インバータ電源が用いられ、その低周波での電力測
定は従来の電力計では誤差が増大する。
Specifically, a three-phase linear motor (LIM)
Is regarded as a black box whose parameter value is unknown from the power supply side due to the end effect caused by the structure. In analyzing this LIM in detail, the calculation of the parameter values of the three-phase equivalent circuit is currently receiving attention, but it is necessary to measure the complex power Pl = Pa + jPr as the power during operation. In particular, complex power measurement is indispensable for the operation control of the LIM, and the actual operation of the LIM uses a low-frequency inverter power supply, and the power measurement at the low frequency increases the error in the conventional power meter. .

【0006】本発明は上述の複素電力を測定出来る測定
方法、即ち抵抗、コンデンサのみで構成され、電圧の実
効値測定から複素電力を算出する測定方法を提供するも
のである。
The present invention provides a measuring method capable of measuring the above-described complex power, that is, a measuring method comprising only a resistor and a capacitor and calculating the complex power from the effective value measurement of the voltage.

【0007】[0007]

【課題を解決するための手段】負荷Zl と並列に抵抗R
a1とRa2の第一直列回路、及び抵抗Rb とコンデンサC
b の第二直列回路を接続し、前記負荷Zl と前記第一、
及び第二直列回路の抵抗Ra 及びRb 側の接続点pと前
記電源の一端sとの間に抵抗rを接続し、前記負荷Zl
の両端子間の実効値電圧Vl 、前記抵抗Ra1の実効値電
圧Va 、前記抵抗Rb の実効値電圧Vb 、前記抵抗rの
実効値電圧Vr 、前記電源の一端sと前記抵抗Ra1とR
a2との接続点a間の実効値電圧Vsa、及び前記電源の一
端sと前記抵抗Rb とコンデンサCb との接続点b間の
実効値電圧Vsbを測定し、Vl 値から既知の第二直列回
路のRb 及びCb を使用してVbx及びVbyを算出してお
き、これらの実測値及び算出値から(1)式によりVrx
を算出し、 Vrx=(Vsa2 −Vr 2 −Va 2 )/2Va ・・・(1) 次に2個の電圧Vr 、Vb の実部、虚部とVsbについ
て、 (Vrx+Vbx)2 +(Vry+Vby)2 =Vsb2 ・・・(2) が成り立ち、Vr の虚部Vryを(3)式より算出し、 Vry={(Vsb2 −Vr 2 −Vb 2 )/2−VrxVbx}/Vby ・・・(3) このVrx、Vryを使用して、負荷電流Ir は、 Ir =Vr /r=Vrx/r+jVry/r ・・・(4) であるから、負荷電力Pl は Pl =Vl ×Ir =Vl Vrx/r+jVl Vry/r ・・・(5) で、複素電力を算出する。
The resistor R is connected in parallel with the load Zl.
The first series circuit of a1 and R a2, and the resistor Rb and capacitor C
b and the load Zl and the first,
A resistor r is connected between a connection point p on the side of the resistors Ra and Rb of the second series circuit and one end s of the power supply, and the load Zl is connected.
Effective voltage Vl between both terminals of the effective value voltage Va of the resistor R a1, effective voltage Vb of the resistor Rb, the effective value voltage Vr of the resistor r, end s and the resistor R a1 and R of the power supply
An effective value voltage Vsa between the connection point a of the power supply a2 and a connection point b between the one end s of the power supply and the resistor Rb and the capacitor Cb is measured. Vbx and Vby are calculated using Rb and Cb of the above equation, and Vrx and Vby are calculated from the measured values and the calculated values according to equation (1).
Vrx = (Vsa 2 −Vr 2 −Va 2 ) / 2 Va (1) Next, for the real part, imaginary part and Vsb of the two voltages Vr and Vb, (Vrx + Vbx) 2 + (Vry + Vby) ) 2 = Vsb 2 (2) holds, and the imaginary part Vry of Vr is calculated from equation (3), and Vry = {(Vsb 2 −Vr 2 −Vb 2 ) / 2−VrxVbx} / Vby. (3) Using these Vrx and Vry, the load current Ir is given by: Ir = Vr / r = Vrx / r + jVry / r (4) Therefore, the load power Pl is Pl = Vl.times.Ir = Vl. Vrx / r + jVl Vry / r (5) The complex power is calculated.

【0008】[0008]

【作用】上述のように、実測可能な実効値電圧を測定
し、一回の測定後に所定の計算式により電圧の実部及び
虚部を算出し、更にこれらの算出値から複素電力値を算
出する。
As described above, the measurable RMS voltage is measured, and after one measurement, the real part and the imaginary part of the voltage are calculated by a predetermined formula, and the complex power value is calculated from these calculated values. I do.

【0009】[0009]

【実施例】図1の示すように、負荷Zl と並列に抵抗R
a1とRa2の第一直列回路、及び抵抗Rb とコンデンサC
b の第二直列回路を接続し、負荷Zl と第一、及び第二
直列回路の抵抗Ra1及びRb 側の接続点pと電源の一端
sとの間に抵抗rを接続する。ただし、負荷に影響しな
い程度にRa1とRa2の直列抵抗及びRb とCb の直列イ
ンピーダンスは大きくとり、直列抵抗rは負荷インピー
ダンスに比べて無視出来る程度の値とする。このときの
各電圧ベクトルはVa を基準ベクトルにとれば、図2の
ように表示することが出来る。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS As shown in FIG.
The first series circuit of a1 and R a2, and the resistor Rb and capacitor C
b, and a resistor r is connected between the load Zl and a connection point p of the first and second resistors R a1 and Rb on the side of the first series circuit and one end s of the power supply. However, the series impedance of the series resistance and Rb and Cb of a degree that does not affect the load R a1 and R a2 are made large, the series resistance r is the value of negligible compared to the load impedance. Each voltage vector at this time can be displayed as shown in FIG. 2 if Va is used as a reference vector.

【0010】いま、抵抗Rb の電圧ベクトルを Vb =
Vbx+jVby 抵抗rの電圧ベクトルを Vr =Vrx+
jVry 、端子s−a間の電圧ベクトルと端子s−b間
の電圧ベクトルをそれぞれ Vsa=Vsax +jVsay
、Vsb=Vsbx +jVsby と表す。
Now, the voltage vector of the resistor Rb is expressed as Vb =
Vbx + jVby The voltage vector of the resistor r is given by Vr = Vrx +
jVry, the voltage vector between the terminals sa and s and the voltage vector between the terminals sb are respectively Vsa = Vsax + jVsay
, Vsb = Vsbx + jVsby.

【0011】又、Va 、Vr 、Vsaの実効値をVa 、V
r 、Vsaと表すと、3個の電圧Va、Vr 、VsaからVr
の実部Vrxは余弦定理を用いて Vrx=(Vsa2 −Vr 2 −Va 2 )/2Va ・・・(1) の関係式より実効測定値Vsa、Vr 、Va (Ra1とRa2
は既知であるから、Vaは端子p、q間の負荷電圧の実
効値測定値Vl よりVa =Vl Ral/(Ra1+Ra2
と計算出来、測定不要)から求められる。
The effective values of Va, Vr, and Vsa are represented by Va, V
r, Vsa, the three voltages Va, Vr, Vsa to Vr
Vrx is the real part Vrx using the cosine theorem = (Vsa 2 -Vr 2 -Va 2 ) / 2Va ··· effective measurements from relational expression (1) Vsa, Vr, Va (R a1 and R a2
Is known, Va is Va = Vl Ral / ( Ra1 + Ra2 ) from the measured effective value Vl of the load voltage between the terminals p and q.
Can be calculated and measurement is unnecessary).

【0012】次に2個の電圧Vr 、Vb の実部、虚部と
Vsbについて、 (Vrx+Vbx)2 +(Vry+Vby)2 =Vsb2 ・・・(2) が成り立ち、Vr の虚部Vryを(3)式より算出し、 Vry={(Vsb2 −Vr 2 −Vb 2 )/2−VrxVbx}/Vby ・・・(3)
Next, with respect to the real part, imaginary part and Vsb of the two voltages Vr and Vb, (Vrx + Vbx) 2 + (Vry + Vby) 2 = Vsb 2. 3) calculated from the equation, Vry = {(Vsb 2 -Vr 2 -Vb 2) / 2-VrxVbx} / Vby ··· (3)

【0013】このVrx、Vryを使用して、負荷電流Ir
は、 Ir =Vr /r=Vrx/r+jVry/r ・・・(4) であるから、負荷電力Pl は Pl =Vl ×Ir =Vl Vrx/r+jVl Vry/r ・・・(5) で、複素電力を算出する。
Using the Vrx and Vry, the load current Ir
Is Ir = Vr / r = Vrx / r + jVry / r (4), and the load power Pl is Pl = Vl.times.Ir = V1 Vrx / r + jV1 Vry / r (5), and the complex power is Is calculated.

【0014】具体例として、設定値を Ra1=1(k
Ω)、Ra2=49(kΩ)、Rb =1(kΩ) 、1/ωCb
=30(kΩ)、r=0.1(Ω)、Vl =50(V)、
負荷インピーダンスZl =−4−j3(Ω)(実際には
Zlの素子値は未知であるが、理論の妥当性を示すため
既知とする)として、複素電力を算出する。なお、理論
値として有効電力は−400(W)、無効電力は進み3
00(Var)で、 Pl =−400+j300 であ
る。
As a specific example, when the set value is Ra1 = 1 (k
Ω), R a2 = 49 (kΩ), Rb = 1 (kΩ), 1 / ωCb
= 30 (kΩ), r = 0.1 (Ω), Vl = 50 (V),
The complex power is calculated as a load impedance Zl = −4−j3 (Ω) (actually, the element value of Zl is unknown, but is assumed to indicate the validity of the theory). The theoretical power is -400 (W) and the reactive power is 3
At 00 (V ar ), Pl = −400 + j300.

【0015】各電圧の実効値を有効数字4桁とすると、
次の値となる。 Va =1.000(V)、Vb =1.666(V)、V
bx=0.0555(V)、Vby=1.665(V)、V
r =1.000(V)、Vsa=0.6325(V)、V
sb=2.384(V) (1)式から Vrx=−0.7999(V) (2)式から Vry=0.5996(V) (5)式から 複素電力 Pl =−399.95+j2
99.8 となる。
If the effective value of each voltage is four significant digits,
It has the following values: Va = 1.000 (V), Vb = 1.666 (V), V
bx = 0.0555 (V), Vby = 1.665 (V), V
r = 1.000 (V), Vsa = 0.6325 (V), V
sb = 2.384 (V) From equation (1) Vrx = −0.7999 (V) From equation (2) Vry = 0.5996 (V) From equation (5) Complex power Pl = −399.95 + j2
99.8.

【0016】[0016]

【発明の効果】上述のように、簡単な回路で、しかも実
効値電圧の測定のみで複素電力の算出が可能で、例えば
熱電対形計器を利用することにより、等価複素電力の測
定が可能で、電力測定を必要とする分野での使用効果は
極めて大きい。
As described above, it is possible to calculate the complex power with a simple circuit and only by measuring the effective value voltage. For example, by using a thermocouple type instrument, it is possible to measure the equivalent complex power. The effect of use in fields requiring power measurement is extremely large.

【0017】モータの駆動電源として常用されている低
周波インバータ電源から供給される電力の測定において
は、電流波形及び電圧波形が高調波を含み、波形歪が大
きいが、従来の電力計のような大きな誤差はない。
In the measurement of power supplied from a low-frequency inverter power supply commonly used as a drive power supply for a motor, a current waveform and a voltage waveform include harmonics and waveform distortion is large. There is no big error.

【0018】三相リニアモータの三相等価回路のパラメ
ータ値算定並びに運転制御におけるリアルタイムの電力
測定が容易である。
It is easy to calculate parameter values of a three-phase equivalent circuit of a three-phase linear motor and measure power in real time in operation control.

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

【図1】本発明の複素電力の計測方法を実施する回路構
成図である。
FIG. 1 is a circuit configuration diagram for implementing a method for measuring complex power according to the present invention.

【図2】電圧のベクトル図である。FIG. 2 is a voltage vector diagram.

【符号の説明】[Explanation of symbols]

E 電源電圧(V) Vl 負荷の実効値電圧(V) Zl 負荷インピーダンス(Ω) r 既知抵抗(Ω) Ra1 既知抵抗(Ω) Ra2 既知抵抗(Ω) Rb 既知抵抗(Ω) Cb コンデンサ(μF) Vr 実効値電圧(V) Va 実効値電圧(V) Vb 実効値電圧(V) Vsa 実効値電圧(V) Vsb 実効値電圧(V) p、q、a、b、s 端子記号 Vr 、Va 、Vb 、Vsa、Vsb 電圧ベクトル E Power supply voltage (V) Vl Load effective value voltage (V) Zl Load impedance (Ω) r Known resistance (Ω) Ra1 Known resistance (Ω) Ra2 Known resistance (Ω) Rb Known resistance (Ω) Cb capacitor (μF) Vr RMS voltage (V) Va RMS voltage (V) Vb RMS voltage (V) Vsa RMS voltage (V) Vsb RMS voltage (V) p, q, a, b, s Terminal symbols Vr, Va, Vb, Vsa, Vsb voltage vector

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 電源から供給される有効電力と無効電力
よりなる複素電力を計測するために、負荷Zl と並列に
抵抗Ra1とRa2の第一直列回路、及び抵抗Rb とコンデ
ンサCb の第二直列回路を接続し、前記負荷Zl と前記
第一、及び第二直列回路の抵抗Ra1及びRb 側の接続点
pと前記電源の一端sとの間に抵抗rを接続し、前記負
荷Zl の両端子間の実効値電圧Vl 、前記抵抗Ra1の実
効値電圧Va 、前記抵抗Rb の実効値電圧Vb 、前記抵
抗rの実効値電圧Vr 、前記電源の一端sと前記抵抗R
a1とRa2との接続点a間の実効値電圧Vsa、及び前記電
源の一端sと前記抵抗Rb とコンデンサCb との接続点
b間の実効値電圧Vsbを測定し、Vl 値から既知の第二
直列回路のRb 及びCb を使用してVbx及びVbyを算出
しておき、これらの実測値及び算出値から(1)式より
Vrxを算出し、 Vrx=(Vsa2 −Vr 2 −Va 2 )/2Va ・・・(1) 次に2個の電圧Vr 、Vb の実部、虚部とVsbについ
て、 (Vrx+Vbx)2 +(Vry+Vby)2 =Vsb2 ・・・(2) が成り立ち、Vr の虚部Vryは(3)式より算出し、 Vry={(Vsb2 −Vr 2 −Vb 2 )/2−VrxVbx}/Vby ・・・(3) このVrx、Vryを使用して、負荷電流Ir は、 Ir =Vr /r=Vrx/r+jVry/r ・・・(4) であるから、負荷電力Pl は Pl =Vl ×Ir =Vl Vrx/r+jVl Vry/r ・・・(5) で、複素電力を算出することを特徴とする複素電力の計
測方法。
To 1. A for measuring the complex power consisting of active and reactive power supplied from the power source, a first series circuit in parallel with the load Zl resistor R a1 and R a2, and the resistor Rb and capacitor Cb A second series circuit is connected, and a resistor r is connected between the load Zl and a connection point p on the resistors R a1 and Rb sides of the first and second series circuits and one end s of the power supply. effective voltage Vl between both terminals of zl, the effective voltage Va of the resistor R a1, effective voltage Vb of the resistor Rb, the effective value voltage Vr of the resistance r, the one end s of the source resistance R
effective voltage Vsa between the connection point between a1 and R a2 a, and the effective voltage Vsb between the connection point b between the end s and the resistor Rb and capacitor Cb of the power supply is measured, the from Vl value known Vbx and Vby are calculated using Rb and Cb of the two-series circuit, and Vrx is calculated from the measured value and the calculated value according to the equation (1). Vrx = (Vsa 2 −Vr 2 −Va 2 ) / 2Va (1) Next, for the real part, imaginary part and Vsb of the two voltages Vr and Vb, (Vrx + Vbx) 2 + (Vry + Vby) 2 = Vsb 2 . imaginary part Vry is calculated from equation (3), Vry = {(Vsb 2 -Vr 2 -Vb 2) / 2-VrxVbx} / Vby ··· (3) this Vrx, using Vry, load current Ir Is: Ir = Vr / r = Vrx / r + jVry / r (4) Therefore, the load power Pl is Pl = Vl.times.Ir = V1 Vrx / r + jVl Vr. y / r (5) A complex power measurement method, wherein the complex power is calculated as follows.
JP32639894A 1994-12-27 1994-12-27 How to measure complex power Expired - Fee Related JP3326763B2 (en)

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JP3326763B2 true JP3326763B2 (en) 2002-09-24

Family

ID=18187357

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Country Link
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Also Published As

Publication number Publication date
JPH08184617A (en) 1996-07-16

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