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JPH0126029B2 - - Google Patents
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JPH0126029B2 - - Google Patents

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Publication number
JPH0126029B2
JPH0126029B2 JP58071596A JP7159683A JPH0126029B2 JP H0126029 B2 JPH0126029 B2 JP H0126029B2 JP 58071596 A JP58071596 A JP 58071596A JP 7159683 A JP7159683 A JP 7159683A JP H0126029 B2 JPH0126029 B2 JP H0126029B2
Authority
JP
Japan
Prior art keywords
phase
circuit
power
voltage
axis
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
Application number
JP58071596A
Other languages
Japanese (ja)
Other versions
JPS59195165A (en
Inventor
Hidenori Kawaomo
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP7159683A priority Critical patent/JPS59195165A/en
Publication of JPS59195165A publication Critical patent/JPS59195165A/en
Publication of JPH0126029B2 publication Critical patent/JPH0126029B2/ja
Granted legal-status Critical Current

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  • Measurement Of Current Or Voltage (AREA)
  • Control Of Electrical Variables (AREA)

Description

【発明の詳細な説明】 この発明は、3相交流電源の各種特性を把握す
るために必要な3相交流電源の電力計測装置に関
するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a power measuring device for a three-phase AC power supply, which is necessary for grasping various characteristics of the three-phase AC power supply.

第1図〜第3図は従来の計測回路の原理を説明
するための回路図であり、第1図は有効電力を計
測する有効電力計測回路、第2図は無効電力を計
測する無効電力計測回路、第3図は力率を計測す
る力率計測回路である。
Figures 1 to 3 are circuit diagrams for explaining the principle of conventional measurement circuits. Figure 1 is an active power measurement circuit that measures active power, and Figure 2 is a reactive power measurement circuit that measures reactive power. Circuit FIG. 3 is a power factor measuring circuit that measures the power factor.

図において、1,2は電力計素子を示し、電流
コイル(固定コイル)3と、電圧コイル(可動コ
イル)4とで構成され、電力計素子1,2は同一
軸に取り付けられている。
In the figure, numerals 1 and 2 indicate wattmeter elements, which are composed of a current coil (fixed coil) 3 and a voltage coil (movable coil) 4, and the wattmeter elements 1 and 2 are attached to the same axis.

5は電力率素子、6は3相負荷を示す。 5 is a power factor element, and 6 is a three-phase load.

次に、動作について説明する。 Next, the operation will be explained.

第1図の有効電力計測回路は、3相負荷6に見
合つたU相電流IUが矢印方向へ流れるとき、電圧
コイル4に線間電圧EEVとU相電流IUとに見合つ
たトルクが発生する。
In the active power measurement circuit shown in FIG. 1, when a U-phase current I U corresponding to a three-phase load 6 flows in the direction of the arrow, a torque corresponding to a line voltage E EV and a U-phase current I U is applied to the voltage coil 4. Occur.

また、W相についても同様で、電力計素子2に
トルクが発生し、電力計素子1,2を取り付けた
軸のトルクの掛り具合で有効電力量を指示するよ
うに構成されている。
The same applies to the W phase, where torque is generated in the wattmeter element 2, and the amount of active power is indicated by the amount of torque applied to the shaft to which the wattmeter elements 1 and 2 are attached.

第2図の無効電力計測回路は、U相電流IUによ
つて電流コイル3に磁界が発生し、U相電圧EU
からπ/2だけ遅れた線間電圧EVWによつて電圧
コイル4にトルクが発生する。このトルクの作用
によつて有効電力からπ/2ずれた量、つまり無
効電力が計測される。
In the reactive power measurement circuit shown in Fig. 2, a magnetic field is generated in the current coil 3 by the U-phase current I U , and the U-phase voltage E U
Torque is generated in the voltage coil 4 by the line voltage E VW delayed by π/2 from the line voltage E VW . Due to the action of this torque, an amount deviated from active power by π/2, that is, reactive power is measured.

しかし、無効電力が得られるのは、3相平衡状
態の時に限られる。
However, reactive power can only be obtained in a three-phase balanced state.

第3図は力率計測回路で、電力率素子5は互い
に機械的に60度の角度で位置付けられた2組のコ
イル、すなわち線間電圧EUV,EUWに接続された
電圧コイル4A,4Bと、U相電流IUに接続され
た2組の電流コイル3A,3Bとで構成され、力
率に見合つたトルクがそれぞれの電圧コイル4
A,4Bに作用し、力率を指示する。
Figure 3 shows a power factor measuring circuit, in which the power factor element 5 consists of two sets of coils mechanically positioned at an angle of 60 degrees to each other, namely voltage coils 4A and 4B connected to line voltages E UV and E UW . and two sets of current coils 3A and 3B connected to the U-phase current IU , and the torque corresponding to the power factor is applied to each voltage coil 4.
It acts on A and 4B and indicates the power factor.

なお、電力計素子1,2および電力率素子5を
各コイル3,3A,3B,4,4A,4Bで構成
した各計測回路を示したが、ホール素子で構成し
た各計測回路も在存する。
Note that although each measurement circuit is shown in which the wattmeter elements 1 and 2 and the power factor element 5 are constructed from the respective coils 3, 3A, 3B, 4, 4A, and 4B, there are also measurement circuits constructed from Hall elements.

従来の3相交流電源の電力計測装置は以上のよ
うに構成されているので、有効電力、無効電力、
力率等を測定しようとする場合、個々の計測器が
必要となる。
The conventional power measurement device for three-phase AC power supply is configured as described above, so it can measure active power, reactive power,
When attempting to measure power factor, etc., individual measuring instruments are required.

また、電力の検出には可動コイル、あるいはホ
ール素子が採用されていたので、商用周波数程度
の低い周波数の計測しかできず、インバータ周波
数のような電流、電圧波形の瞬時電力、瞬時力率
等の計測が不可能であつた。
In addition, since a moving coil or a Hall element was used to detect power, it was only possible to measure frequencies as low as commercial frequencies. It was impossible to measure.

さらに、3相不平衡の場合には計測できないな
どの問題点があつた。
Furthermore, there were other problems such as the inability to measure in the case of three-phase unbalance.

この発明は、上記のような問題点を解消するた
めになされたもので、計測サンプル値としては瞬
時の電圧値および瞬時の電流値をd,q変換理論
に基づく演算回路へ与えることにより、瞬時の電
力および瞬時の力率、あるいは3相不平衡の電力
等が計測できる3相交流電源の電力計測装置を得
ることを目的とする。
This invention was made in order to solve the above-mentioned problems.As measurement sample values, instantaneous voltage values and instantaneous current values are given to an arithmetic circuit based on the d,q conversion theory. An object of the present invention is to obtain a power measuring device for a three-phase AC power supply that can measure the power, instantaneous power factor, or three-phase unbalanced power.

以下、この発明の一実施例を図について説明す
る。
An embodiment of the present invention will be described below with reference to the drawings.

第4図において、7は3相交流の電圧値、電流
値をd,q軸変換理論に基づいてd軸、q軸の電
圧値、電流値に変換するd,q軸変換回路、8A
〜8Dはd軸、q軸の電圧値と電流値とを掛算す
る掛算回路、9Aは掛算回路8A,8Dの演算結
果を加算する加算回路、10は掛算回路8Cの演
算結果から掛算回路8Bの演算結果を減算する減
算回路、8E,8Fは掛算回路、9Bは掛算回路
8E,8Fの演算結果を加算する加算回路、11
は加算回路9Bの演算結果を開平演算するルート
演算回路、12は力率演算回路としての割算回路
を示し、加算回路9Aの演算結果をルート演算回
路11の演算結果で割算するものである。
In Fig. 4, 7 is a d- and q-axis conversion circuit that converts three-phase AC voltage and current values into d- and q-axis voltage and current values based on the d- and q-axis conversion theory, and 8A.
~8D is a multiplication circuit that multiplies the voltage value and current value of the d-axis and q-axis, 9A is an addition circuit that adds the calculation results of multiplication circuits 8A and 8D, and 10 is a multiplication circuit that adds the calculation results of multiplication circuit 8C to the calculation result of multiplication circuit 8B. 11 is a subtraction circuit that subtracts the calculation results; 8E and 8F are multiplication circuits; 9B is an addition circuit that adds the calculation results of the multiplication circuits 8E and 8F;
Reference numeral 12 indicates a root arithmetic circuit that performs a square root calculation of the arithmetic result of the adder circuit 9B, and 12 a division circuit as a power factor arithmetic circuit, which divides the arithmetic result of the adder circuit 9A by the arithmetic result of the root arithmetic circuit 11. .

なお、d,q軸変換回路7は2相、例えばU、
W相電流IU,IWおよび線間電圧EUV,EWVから下記
のように、d軸、q軸の電流Id,Iqと、電圧Ed
Eqとをアナログ演算回路または中央処理装置
CPUを用いたデイジタル演算回路で演算する。
Note that the d and q axis conversion circuit 7 has two phases, for example, U,
From the W-phase currents I U , I W and the line voltages E UV , E WV , the d-axis and q-axis currents I d , I q and the voltages E d ,
E q and the analog arithmetic circuit or central processing unit
Calculations are performed using a digital arithmetic circuit using a CPU.

Id=√32・IU Iq=−√2/2(IU+2IW) Ed=√23(VUV−0.5VWV) Eq=−√2・VWV/2 次に、動作について説明するが、その前に原理
について説明する。
Id=√32・I U Iq=−√2/2(I U +2I W ) Ed=√23(V UV −0.5V WV ) Eq=−√2・V WV /2 Next, I will explain the operation. ,Before that, I will explain the principle.

3相交流の相電圧および相電流の実効値をV,
I、位相差をθとすると、有効電力Wおよび無効
電力Qは下記の第1.1式、第2.2式で表わされる。
The effective values of the phase voltage and phase current of three-phase AC are V,
When I is the phase difference and θ is the phase difference, the active power W and the reactive power Q are expressed by the following equations 1.1 and 2.2.

W=3VIcosθ ……1.1 Q=3VIsinθ ……1.2 また、角周波数をωとすると、各相電圧および
相電流の瞬時値には下記の第2.1式〜第3.3式で表
わされる。
W=3VIcosθ...1.1 Q=3VIsinθ...1.2 Furthermore, when the angular frequency is ω, the instantaneous values of each phase voltage and phase current are expressed by the following equations 2.1 to 3.3.

VU=√2Vcosωt ……2.1 VV=√2Vcos(ωt−2π/3) ……2.2 VW=√2Vcos(ωt+2π/3) ……2.3 IU=√2Icos(ωt−θ) ……3.1 IV=√2Iccs(ωt−θ−2π/3) ……3.2 IW=√2Icos(ωt−θ+2π/3) ……3.3 ここで、上記第2.1式〜第3.3式で表わされる瞬
間電圧および瞬時電流をd,q軸変換理論に基づ
いてd軸、q軸の電圧、電流に変換すると、下記
の第4.1式〜第5.2式が得られる。
V U =√2Vcosωt ……2.1 V V =√2Vcos(ωt−2π/3) ……2.2 V W =√2Vcos(ωt+2π/3) ……2.3 I U =√2Icos(ωt−θ) ……3.1 I V = √2Iccs (ωt−θ−2π/3) …3.2 I W =√2Icos (ωt−θ+2π/3) …3.3 Here, the instantaneous voltage and instantaneous current expressed by Equations 2.1 to 3.3 above When converted into d-axis and q-axis voltages and currents based on the d- and q-axis conversion theory, the following equations 4.1 to 5.2 are obtained.

Vd=√3Vcosωt ……4.1 Vq=√3Vsinωt ……4.2 Id=√3Icos(ωt−θ) ……5.1 Ip=√3Isin(ωt−θ) ……5.2 そこで、このd,q軸の電圧および電流を用い
て有効電力および無効電力を求めると、下記の第
6.1式、第6.2式が得られる。
V d = √3Vcosωt …4.1 V q =√3Vsinωt …4.2 I d =√3Icos (ωt−θ) …5.1 I p =√3Isin (ωt−θ) …5.2 Therefore, the d and q axes When calculating the active power and reactive power using voltage and current, the following equation is obtained.
Equations 6.1 and 6.2 are obtained.

W=Vd・Id+Vq・Iq ……6.1 Q=−Vd・Iq+Vq・Id ……6.2 また、力率cosθは第1.1式、第1.2式の有効電力
W、無効電力Qを用いて下記の第7式で表わすこ
とができる。
W=V d・I d +V q・I q ……6.1 Q=−V d・I q +V q・I d ……6.2 In addition, the power factor cos θ is the active power W and the reactive power in equations 1.1 and 1.2. It can be expressed by the following equation 7 using the power Q.

cosθ=W/√22 ……(7) したがつて、上記の論理式を回路式を回路構成
することにより、有効電力、無効電力、力率の瞬
時値を求めることが可能となる。
cosθ=W/√ 2 + 2 (7) Therefore, by configuring the circuit formula from the above logical formula, it becomes possible to obtain the instantaneous values of active power, reactive power, and power factor.

第4図は上記の論理式を具体化した一実施例で
あり、相電流および線間電圧をd軸、q軸の電
流、電圧に変換するために、d,q軸変換回路7
でId,Iq,Vd,Vqを演算して求める。
FIG. 4 shows an example embodying the above logical formula. In order to convert phase currents and line voltages into d-axis and q-axis currents and voltages, a d- and q-axis conversion circuit 7 is used.
Calculate I d , I q , V d , and V q using .

次に、変換した電圧および電流値を掛算回路8
A〜8D、加算回路9A、減算回路10で第6.1
式、第6.2式に示した有効電力W、無効電力Qの
演算を実行する。
Next, the converted voltage and current values are multiplied by a multiplication circuit 8.
A to 8D, addition circuit 9A, subtraction circuit 10, No. 6.1
The active power W and reactive power Q shown in Equation 6.2 are calculated.

そして、有効電力Wおよび無効電力Qがそれぞ
れ得られたら第7式にしたがい、掛算回路8E,
8F、加算回路9Bおよびルート演算回路11で
諸演算処理を行ない、最終的に割算回路12で力
率を算出する。
Then, when the active power W and the reactive power Q are obtained, the multiplication circuit 8E,
8F, an addition circuit 9B, and a route calculation circuit 11 perform various calculation processes, and finally a division circuit 12 calculates the power factor.

なお、上記実施例では3相が平衡した状態の電
力を考慮した例で説明したが、この実施例に限定
されるものではなく、3相が不平衡の状態の電力
であつても全く同様に成立する。
In addition, although the above embodiment has been explained using an example in which power is taken into account when the three phases are balanced, the present invention is not limited to this example, and the same applies even when the power is when the three phases are unbalanced. To establish.

また、演算回路をアナログ回路で構成したもの
を示したが、デイジタル回路で構成することによ
り、温度ドリフト等の影響のない高精度の計測回
路を構成することもできる。
Further, although the arithmetic circuit has been shown to be configured with an analog circuit, by configuring it with a digital circuit, it is also possible to configure a highly accurate measurement circuit that is free from the effects of temperature drift and the like.

以上のように、この発明によれば、3相交流電
源の電力、力率をd、q軸変換理論に基づく、演
算回路で変換したたと、電気的四則演算回路によ
つて演算処理する構成としたので、3相交流の平
衡、不平衡に拘らず有効電力、無効電力及び力率
の瞬時値を高速、高精度で計測できるという優れ
た効果がある。
As described above, according to the present invention, if the power and power factor of a three-phase AC power source are converted by an arithmetic circuit based on the d- and q-axis conversion theory, the configuration is such that the electrical four arithmetic arithmetic circuits perform arithmetic processing. Therefore, there is an excellent effect that the instantaneous values of active power, reactive power, and power factor can be measured at high speed and with high accuracy regardless of whether the three-phase alternating current is balanced or unbalanced.

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

第1図は従来の有効電力を計測する有効電力計
測回路、第2図は従来の無効電力を計測する無効
電力計測回路、第3図は従来の力率を計測する力
率計測回路、第4図はこの発明の一実施例による
3相交流電源の電力計測装置を示すブロツク図で
ある。 図において、1,2は電力計素子、3,3A,
3Bは電流コイル、4,4A,44Bは電圧コイ
ル、5は電力率素子、6は3相負荷、7はd,q
軸変換回路、8A〜8Fは掛算回路、9A,9B
は加算回路、10は減算回路、11はルート演算
回路、12は割算回路を示す。なお、図中、同一
符号は同一、または相当部分を示す。
Figure 1 shows a conventional active power measurement circuit that measures active power, Figure 2 shows a conventional reactive power measurement circuit that measures reactive power, Figure 3 shows a conventional power factor measurement circuit that measures power factor, and Figure 4 shows a conventional power factor measurement circuit that measures power factor. The figure is a block diagram showing a power measuring device for a three-phase AC power supply according to an embodiment of the present invention. In the figure, 1 and 2 are wattmeter elements, 3 and 3A,
3B is a current coil, 4, 4A, 44B are voltage coils, 5 is a power factor element, 6 is a 3-phase load, 7 is d, q
Axis conversion circuit, 8A to 8F are multiplication circuits, 9A, 9B
10 is an addition circuit, 10 is a subtraction circuit, 11 is a root calculation circuit, and 12 is a division circuit. In addition, in the figures, the same reference numerals indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] 1 3相交流電源の線間電圧及び相電流を入力と
して2相の電圧及び電流に変換する3相/2相変
換回路と、この3相/2相変換回路によつて変換
されたd軸の電圧及びd軸の電流の乗算結果と上
記3相/2相変換回路によつて変換されたq軸の
電圧及びq軸の電流の乗算結果とを加算する有効
電力演算回路と、上記3相/2相変換回路によつ
て変換されたq軸の電圧及びd軸の電流の乗算結
果から上記3相/2相変換回路によつて変換され
たd軸の電圧及びq軸の電流の乗算結果を減算す
る無効電力演算回路と、上記有効電力演算回路で
求めた有効電力を2乗した値と上記無効電力演算
回路で求めた無効電力を2乗した値との平方根に
より上記有効電力を除算する力率演算回路とを備
えた3相交流電源の電力計測装置。
1. A 3-phase/2-phase conversion circuit that converts the line voltage and phase current of a 3-phase AC power supply into 2-phase voltage and current as input, and the d-axis converted by this 3-phase/2-phase conversion circuit. an active power calculation circuit that adds the multiplication result of the voltage and the d-axis current to the multiplication result of the q-axis voltage and the q-axis current converted by the 3-phase/2-phase conversion circuit; From the multiplication result of the q-axis voltage and d-axis current converted by the 2-phase conversion circuit, the multiplication result of the d-axis voltage and q-axis current converted by the 3-phase/2-phase conversion circuit is calculated. A reactive power calculation circuit to subtract, and a power to divide the above active power by the square root of the value obtained by squaring the active power obtained by the above active power calculation circuit and the value obtained by squaring the reactive power obtained by the above reactive power calculation circuit. A power measurement device for a three-phase AC power supply, which is equipped with a rate calculation circuit.
JP7159683A 1983-04-20 1983-04-20 Electric power measuring device for three-phase ac power source Granted JPS59195165A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7159683A JPS59195165A (en) 1983-04-20 1983-04-20 Electric power measuring device for three-phase ac power source

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7159683A JPS59195165A (en) 1983-04-20 1983-04-20 Electric power measuring device for three-phase ac power source

Publications (2)

Publication Number Publication Date
JPS59195165A JPS59195165A (en) 1984-11-06
JPH0126029B2 true JPH0126029B2 (en) 1989-05-22

Family

ID=13465199

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7159683A Granted JPS59195165A (en) 1983-04-20 1983-04-20 Electric power measuring device for three-phase ac power source

Country Status (1)

Country Link
JP (1) JPS59195165A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2776951B2 (en) * 1990-03-29 1998-07-16 マツダ株式会社 Rotary atomizing electrostatic coating equipment

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0230787Y2 (en) * 1980-03-03 1990-08-20

Also Published As

Publication number Publication date
JPS59195165A (en) 1984-11-06

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