JPH01239475A - Electronic watthour meter - Google Patents

Electronic watthour meter

Info

Publication number
JPH01239475A
JPH01239475A JP6572888A JP6572888A JPH01239475A JP H01239475 A JPH01239475 A JP H01239475A JP 6572888 A JP6572888 A JP 6572888A JP 6572888 A JP6572888 A JP 6572888A JP H01239475 A JPH01239475 A JP H01239475A
Authority
JP
Japan
Prior art keywords
waveform
data
proportional
area
current
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
JP6572888A
Other languages
Japanese (ja)
Inventor
Osamu Kajiya
梶家 治
Katsutaro Matsumoto
松本 勝太郎
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.)
Takaoka Toko Co Ltd
Tokyo Electric Power Co Holdings Inc
Original Assignee
Tokyo Electric Power Co Inc
Takaoka Electric Mfg 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 Tokyo Electric Power Co Inc, Takaoka Electric Mfg Co Ltd filed Critical Tokyo Electric Power Co Inc
Priority to JP6572888A priority Critical patent/JPH01239475A/en
Publication of JPH01239475A publication Critical patent/JPH01239475A/en
Pending legal-status Critical Current

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  • Measurement Of Current Or Voltage (AREA)

Abstract

PURPOSE:To simplify a computation and to make a microcomputer, etc., usable by taking signals proportional to a load voltage and a load current of a feeder into an arithmetic part after they are rectified with a half-wave and converted to the digital values, and making the computation on the data in the most common with an adding. CONSTITUTION:By an auxiliary transformer 1, the signal proportional to the load voltage of the feeder is supplied to an input terminal 9a on a rectifier circuit 9, and by an auxiliary current transformer 2, the signal proportional to the load current of the feeder is supplied to the input terminal 10a on the rectifier circuit 10. In each rectifier circuit 9, 10, the inputted signals are rectified with the half-wave and inputted to 1st and 2nd channels 15a, 15b of an A/D converter circuit 15. In this converter circuit 15, each signal inputted by means of receiving a channel number and a command from the arithmetic part 17 are converted to digital values, and these converted data are supplied to the arithmetic part 17. Then in the arithmetic part 17, the data written are made to compute in the most common with the adding, and the computed results are displayed on a display part 8.

Description

【発明の詳細な説明】 「産業上の利用分野」 本発明はマイクロコンピュータを採用した電子式電力量
計の改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION "Field of Industrial Application" The present invention relates to an improvement in an electronic watt-hour meter employing a microcomputer.

「従来の技術」 第8図はマイクロコンピュータを採用した従来技術の電
子式電力量計のブロック図である。同図にあ゛いて、1
は補助変圧器、2は補助変流器で、それぞれ給電線の負
荷電圧に比例した信号および給電線の負荷電流に比例し
た信号をサンプルホールド回路3.4に供給する。サン
プルホールド回路3.4では、入力信号の周期よりも早
い周期で入力信号の瞬時値がサンプルホールドされる。
"Prior Art" FIG. 8 is a block diagram of a conventional electronic watt-hour meter employing a microcomputer. In the same figure, 1
2 is an auxiliary transformer, and 2 is an auxiliary current transformer, which respectively supply a signal proportional to the load voltage of the power supply line and a signal proportional to the load current of the power supply line to the sample and hold circuit 3.4. The sample and hold circuit 3.4 samples and holds the instantaneous value of the input signal at a cycle faster than the cycle of the input signal.

サンプルホールドされた入力信号はA/D変挽回路5.
6でそれぞれデジタル値に変換された後、演算部7に取
込まれ所定の演算処理が施されて、表示部8に表示され
る。
The sampled and held input signal is sent to an A/D conversion circuit 5.
After each of the signals is converted into a digital value in step 6, it is taken into a calculation section 7, subjected to predetermined calculation processing, and displayed on a display section 8.

「発明が解決しようとする課題」 上述のごとき従来技術においては、A/D変換回路5.
6でデジタル変換されて演算部7に取込まれるデータは
、交流瞬時値データであるため、電圧データと電流デー
タの乗算とその結果の加算を一定回数繰り返して電力量
が得られる。そのため、演算部7には高速乗算を主体と
する複雑な演算処理が要求される。
"Problem to be Solved by the Invention" In the prior art as described above, the A/D conversion circuit 5.
Since the data digitally converted in step 6 and taken into the calculation unit 7 is AC instantaneous value data, the electric energy can be obtained by repeating the multiplication of the voltage data and the current data and the addition of the results a certain number of times. Therefore, the arithmetic unit 7 is required to perform complex arithmetic processing mainly consisting of high-speed multiplication.

本発明はこの点に鑑み、簡単な演算処理ですませるよう
にしたものである。
In view of this point, the present invention is designed to allow simple arithmetic processing.

「課題を解決するための手段」 給電線の負荷電圧に比例した信号および給電線の負荷電
流に比例した信号を半波整流した上で、デジタル値に変
換する。
"Means for Solving the Problem" A signal proportional to the load voltage of the power supply line and a signal proportional to the load current of the power supply line are half-wave rectified and then converted into digital values.

「作用」 本発明によれば、デジタル値に変換されて演算部に取込
まれたデータからは加算を主体とした演算を施すことに
よって電力量が演算でき、高速乗算を必要としないので
、安価なマイクロコンピュータを採用することができる
"Operation" According to the present invention, the amount of electric power can be calculated by performing calculations mainly based on addition from data converted to digital values and taken into the calculation section, and high-speed multiplication is not required, so it is inexpensive. A microcomputer can be used.

「実施例」 以下本発明の実施例を図面に基づいて詳細に説明する。"Example" Embodiments of the present invention will be described in detail below based on the drawings.

なお、上記実施例と同一部分には同一番号を付し、その
説明は省略する。
Note that the same parts as those in the above embodiment are given the same numbers, and the explanation thereof will be omitted.

第1図は本発明の一実施例を示す電子式電力量計のブロ
ック図でおる。この図において、9は補助変圧器1から
入力端子9aに供給された信号を半波整流する整流回路
、10は補助変流器2から入力端子10aに供給された
信号を半波整流する整流回路である。また15は前記整
流回路9および10からの信号をそれぞれ第1チヤンネ
ル15aおよび第2チヤンネル15bに供給されるA/
D変換回路、17はこのA/D変換回路15から取込ま
れたデジタルデータに所定の演算処理を施して電力量を
演算する演算部でおる。
FIG. 1 is a block diagram of an electronic watt-hour meter showing one embodiment of the present invention. In this figure, 9 is a rectifier circuit that half-wave rectifies the signal supplied from the auxiliary transformer 1 to the input terminal 9a, and 10 is a rectifier circuit that half-wave rectifies the signal supplied from the auxiliary transformer 2 to the input terminal 10a. It is. Further, reference numeral 15 denotes an A/R which supplies the signals from the rectifying circuits 9 and 10 to the first channel 15a and the second channel 15b, respectively.
The D conversion circuit 17 is a calculation section that performs predetermined calculation processing on the digital data taken in from the A/D conversion circuit 15 to calculate the amount of electric power.

次に上記実施例の動作を説明する。Next, the operation of the above embodiment will be explained.

補助変圧器1は給電線の負荷電圧に比例した信号を整流
回路90入力端子9aに供給する。補助変流器2は給電
線の負荷電流に比例した信号を整流回路10の入力端子
10aに供給する。
The auxiliary transformer 1 supplies a signal proportional to the load voltage of the power supply line to the rectifier circuit 90 input terminal 9a. The auxiliary current transformer 2 supplies a signal proportional to the load current of the power supply line to the input terminal 10a of the rectifier circuit 10.

整流回路9および10は入力端子9aおよび1Qaに供
給された信号をそれぞれ半波整流し、それぞれA/D変
換回路15の第1チヤンネル15aおよび第2チヤンネ
ル15bに供給する。
Rectifier circuits 9 and 10 half-wave rectify the signals supplied to input terminals 9a and 1Qa, respectively, and supply them to first channel 15a and second channel 15b of A/D conversion circuit 15, respectively.

A/D変換回路15は演算部17から図示されない制御
線を通して、チャンネル番号とコマンドを受(ブて入力
端子15a、15bに供給された信号を順次A/D変換
し、データが演算部17に取込まれる。
The A/D conversion circuit 15 receives a channel number and a command from the calculation section 17 through a control line (not shown), and sequentially A/D converts the signals supplied to the input terminals 15a and 15b, and the data is sent to the calculation section 17. be taken in.

演算部17は取込まれたデータに所定の演算処理を施し
て電力量を演算し、表示部8に表示する。
The arithmetic unit 17 performs predetermined arithmetic processing on the captured data to calculate the amount of power and displays it on the display unit 8 .

ここで、演算部17で実施する演算処理の内容について
説明する。
Here, the content of the calculation process performed by the calculation unit 17 will be explained.

第2図は演算原理を説明するために示した一般的な交流
波形で、11は電圧波形を、12は電流波形をそれぞれ
示しており、電流波形12が電圧波形11より位相角φ
だけ遅れている状態を示している。電圧波形11および
電流波形12の半周期の時間をTとし、電圧波形11を
ysrnωtとすると、半周期弁の平均値は となって、電圧波形11の大きさVに比例した値が得ら
れる。また電流波形12についても、半周期弁の平均値
は、電流波形12をl5in(ωを一φ)とすると =KICO3φ       ・・・・・・(2〉とな
って、有効分に比例した(直が得られる。なお、(1)
、(2)式中、Kは比例定数でおる。
FIG. 2 shows general AC waveforms shown to explain the calculation principle, 11 shows the voltage waveform, 12 shows the current waveform, and the current waveform 12 has a phase angle φ from the voltage waveform 11.
This indicates that there is a delay. If the half-cycle time of the voltage waveform 11 and the current waveform 12 is T, and the voltage waveform 11 is ysrnωt, then the average value of the half-cycle valve is , and a value proportional to the magnitude V of the voltage waveform 11 is obtained. Also, regarding the current waveform 12, the average value of the half-period valve is proportional to the effective component (directly is obtained.In addition, (1)
, (2), where K is a proportionality constant.

(2)式の意味は、第2図において電流波形12の符号
03 A204で囲まれた部分の面積の半周期の平均値
02h1から符号Q2A103で囲まれた負の部分の面
積の半周期の平均l!l02h2を差引いた値がIC0
6φに比例することを示すものである。
The meaning of equation (2) is from the average half-cycle of the area of the part surrounded by the code 03 A204 of the current waveform 12 in FIG. l! The value after subtracting l02h2 is IC0
This shows that it is proportional to 6φ.

電流波形12は正弦波であるから、符号02A103で
囲まれた波形部の面積は、符号04A?0、で囲まれた
部分の面積に等しい。よって符号03A204で囲まれ
た波形部の面積から符号04A205で囲まれた波形部
の面積を差引けば、ICO3φに比例した値が得られる
。また符@03A204で囲まれた波形部の面積と符号
04A205で囲まれた波形部の面積を加算すれば、電
流の大きさIに比例した値が得られる。
Since the current waveform 12 is a sine wave, the area of the waveform portion surrounded by 02A103 is 04A? It is equal to the area of the part surrounded by 0. Therefore, by subtracting the area of the waveform portion surrounded by the symbol 04A205 from the area of the waveform portion surrounded by the symbol 03A204, a value proportional to ICO3φ is obtained. Further, by adding the area of the waveform portion surrounded by the symbol @03A204 and the area of the waveform portion surrounded by the symbol 04A205, a value proportional to the magnitude I of the current is obtained.

第3図は電流波形12が電圧波形11より位相角φだけ
進んでいる場合を示している。電流波形12について符
号o2A103で囲まれた波形部の面積から符号03A
204で囲まれた波形部の面積を差引けば、lCo5φ
に比例した値が得られ、また符号03A204で囲まれ
た波形部の面積は符号05A306で囲まれた波形部の
面積に等しいため、lCo8φに比例した値は、符@0
2A103で囲まれた波形部の面積から符号05A3 
o6で囲まれた波形部の面積を差引くことによって得ら
れる。また、符号02A1Q3で囲まれた波形部の面積
に符号05A306で囲まれた波形部の面積を加えれば
、電流の大きさ■に比例した値が得られる。
FIG. 3 shows a case where the current waveform 12 leads the voltage waveform 11 by a phase angle φ. Regarding current waveform 12, code 03A is obtained from the area of the waveform portion surrounded by code o2A103.
By subtracting the area of the waveform surrounded by 204, lCo5φ
Since the area of the waveform surrounded by the code 03A204 is equal to the area of the waveform surrounded by the code 05A306, the value proportional to lCo8φ is obtained by the sign @0
Code 05A3 from the area of the waveform surrounded by 2A103
It is obtained by subtracting the area of the waveform portion surrounded by o6. Further, by adding the area of the waveform portion surrounded by the symbol 05A306 to the area of the waveform portion surrounded by the symbol 02A1Q3, a value proportional to the magnitude of the current ■ can be obtained.

第4図も演算原理の説明図で、交流波形の半周期をn区
分してサンプリングを行い、al、a2・・a、の順に
n個のデータが得られる様子を示している。このように
して得られたn1ljilのデータを加算することによ
って、交流波形の大きざに比例した値が与えられること
は、面積法と呼ばれるアルゴリズムとして周知の通りで
おる。
FIG. 4 is also an explanatory diagram of the calculation principle, and shows how sampling is performed by dividing a half period of an AC waveform into n sections, and n pieces of data are obtained in the order of al, a2, . . . a. By adding the n1ljil data obtained in this way, a value proportional to the size of the AC waveform is given, as is well known as an algorithm called the area method.

このような手法で第4図の交流波のうち、符号OAO2
で囲まれた波形部の面積を求めるには、単にal、a 
・・akのに個のデータを加算しだのでは誤差が大きく
不可能であるが、ざらに半周期の終りから数えたに個の
データa。、an−1・・an+に+1を加算して平均
値を取ることにより、誤差を小ざくすることができる。
Using this method, the code OAO2 of the alternating current waves in Fig. 4 is
To find the area of the waveform surrounded by , simply al, a
Although it would be impossible to add data of ak to ak, the error would be large, but it would be impossible to add data of ak to ak, but it would be impossible to add data of ak to ak. , an-1 . . . an+ and take the average value, the error can be reduced.

第4図の交流波形の大きざを1とし、a1〜aHについ
ては01を基準に位相角を表わすことにし、θをサンプ
リング間隔の位相角、θ0を各サンプリング区間内にあ
けるサンプリング位相角とすれば、a1=s:00g、
a2=s!n(θ十θ0 ) 、 a3 =S1n(2
θ十00)・・で表わされ、an−、−arl−に+1
については01を基準に位相角を表すと、a、=sin
(θ−θ ) 、a n−1=s i n (2θ〇 一θ。)・・どなるので、 al +82 +” ”+aH+an 十an−1+’
 ・十an−に+1 ・・・・・・・・・(4) となって、誤差はθ。がO〜θ/2の範囲に変動するこ
とにより生ずることがわかるので、半周期の区分数nを
大きくすれば誤差を小さくできることは明らかでおる。
The size difference of the AC waveform in Fig. 4 is assumed to be 1, and the phase angles for a1 to aH are expressed based on 01. Let θ be the phase angle of the sampling interval, and θ0 be the sampling phase angle within each sampling interval. If, a1=s:00g,
a2=s! n(θ+θ0), a3=S1n(2
It is expressed as θ100)..., +1 for an-, -arl-
Expressing the phase angle based on 01, a,=sin
(θ-θ), a n-1=s i n (2θ〇1θ.)...so, al +82 +""+aH+an 10 an-1+'
・+1 to 10 an- (4), and the error is θ. Since it can be seen that this is caused by fluctuations in the range of O to θ/2, it is clear that the error can be reduced by increasing the number of half-cycle divisions n.

第5図は面積法のアルゴリズムを位相情報の演算に適用
する場合の説明図である。第5図は交流波形が第にサン
プリング区間内の符@03において負から正に変化し、
同区間での正のサンプリングデータakが得られた場合
を示している。上述の手法を用いて符号Q、A204で
囲まれた部分の面積を求めると、実際の波形は符号03
で負から正へと変化しているのに、第に区間の始まりで
ある符号O−3で負から正に変化した場合と同一結果が
得られ、符号02A103で囲まれた負の波形部の面積
を符号Q2A10′3で囲まれた面積に過小評価するこ
とになる。その結果、実際の位相情報はφであるのにφ
−と評価することになる。ψとφ−の差の最大は、サン
プリング間隔の位相角θになり得る。この位相差は交流
波形の大きざを求めるだけなら無視できる値であっても
、位相情報を含んだ演算には大きな誤差の原因となり得
るものである。言いかえれば、サンプリング周波数を高
めることによって位相誤差を小ざく精度よく演算を行う
ことができる訳である。
FIG. 5 is an explanatory diagram when the area method algorithm is applied to calculation of phase information. FIG. 5 shows that the AC waveform first changes from negative to positive at mark @03 within the sampling interval,
This shows a case where positive sampling data ak in the same interval is obtained. When the area of the part surrounded by the code Q and A204 is calculated using the above method, the actual waveform is the code 03.
Although it changes from negative to positive at , the same result as when it changes from negative to positive at code O-3, which is the start of the second interval, is obtained, and the negative waveform part surrounded by code 02A103 The area will be underestimated to the area surrounded by the symbol Q2A10'3. As a result, even though the actual phase information is φ, φ
It will be evaluated as −. The maximum difference between ψ and φ- may be the phase angle θ of the sampling interval. Although this phase difference is a value that can be ignored when only determining the magnitude of the AC waveform, it can cause a large error in calculations that include phase information. In other words, by increasing the sampling frequency, it is possible to reduce the phase error and perform calculations with high accuracy.

さて、第6図および第7図は上述の如く考慮して演算部
17に取込まれた給電線の負荷電圧に比例した信号11
と給電線の負荷電流に比例した信号12の各−周期分の
データを示したものである。
Now, FIG. 6 and FIG. 7 show the signal 11 proportional to the load voltage of the feeder line taken into the calculation unit 17 in consideration as described above.
This shows data for each period of the signal 12 which is proportional to the load current of the power supply line.

第6図においては、電流位相が遅れφ、第7図では電流
位相が進みφであることを示している。
6 shows that the current phase is delayed φ, and FIG. 7 shows that the current phase is advanced φ.

第6図において、電圧波形11の面積法で得られた値を
ΣV、電流波形12の符号02AO3で囲まれた波形部
の面積法で得られた値をΣ■6、符@03AO4で囲ま
れた波形部について同様に得られた値をΣIBとすれば
、 給電線の消費電力−にΣ■(ΣIA  n1B)・・・
・・・(5) (ここでKは比例定数である) で得られることは上述した通りでおる。
In Fig. 6, the value obtained by the area method of the voltage waveform 11 is ΣV, the value obtained by the area method of the waveform portion of the current waveform 12 surrounded by the symbol 02AO3 is Σ■6, and the value surrounded by the symbol @03AO4. If the value similarly obtained for the waveform part is ΣIB, then the power consumption of the feeder line - is Σ■(ΣIA n1B)...
...(5) (Here, K is a proportionality constant) What can be obtained is as described above.

また、第7図においては、電流波形12の符号02A1
03で囲まれた波形部の面積法で得られた値をΣIA、
符号04A205で囲まれた波形部の同様にして得られ
た値をΣIBとすれば、給電線の消費電力は(5)式で
得られることも上述した通りでおる。
In addition, in FIG. 7, the code 02A1 of the current waveform 12 is
The value obtained by the area method of the waveform part surrounded by 03 is ΣIA,
As mentioned above, if the similarly obtained value of the waveform portion surrounded by the symbol 04A205 is ΣIB, the power consumption of the feeder line can be obtained by equation (5).

このようにして得られた給電線の電力に所定の演算を実
施して電力量を演算し、表示部8に表示する。
A predetermined calculation is performed on the power of the feeder line obtained in this manner to calculate the amount of power, and the amount of power is displayed on the display unit 8.

「発明の効果」 以上詳述したごとく、本発明によれば加算を主体とした
簡単な演算を施すことによって電力量が演算できる電子
式電力量計を提供できる。
"Effects of the Invention" As detailed above, according to the present invention, it is possible to provide an electronic watt-hour meter that can calculate the amount of power by performing simple calculations mainly consisting of addition.

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

第1図は本発明の一実施例を示す電子式電力量計のブロ
ック図、第2図、第3図、第4図および第5図は原理説
明のための交流波形図、第6図、第7図は演算部に取込
まれたデータの関係図、第8図は従来技術による電子式
電力計のブロック図である。 図において 9.10は整流回路 15はA/D変換回路 17は演算部         でおる。
FIG. 1 is a block diagram of an electronic watt-hour meter showing an embodiment of the present invention; FIGS. 2, 3, 4, and 5 are AC waveform diagrams for explaining the principle; FIG. 7 is a relationship diagram of data taken into the calculation section, and FIG. 8 is a block diagram of an electronic wattmeter according to the prior art. In the figure, 9.10 indicates the rectifier circuit 15 and the A/D conversion circuit 17 as an arithmetic unit.

Claims (1)

【特許請求の範囲】[Claims] 給電線の負荷電圧に比例した信号と給電線の負荷電流に
比例した信号とをそれぞれ個別に半波整流する整流回路
と、該整流回路から出力される信号をデジタル変換する
A/D変換回路と、このA/D変換回路から取込まれた
デジタルデータに所定の演算処理を施して電力量を演算
する演算部とを備えたことを特徴とする電子式電力量計
A rectifier circuit that separately performs half-wave rectification of a signal proportional to the load voltage of the power supply line and a signal proportional to the load current of the power supply line, and an A/D conversion circuit that digitally converts the signal output from the rectification circuit. An electronic watt-hour meter comprising: a calculation unit that performs predetermined calculation processing on the digital data taken in from the A/D conversion circuit to calculate the amount of electric power.
JP6572888A 1988-03-22 1988-03-22 Electronic watthour meter Pending JPH01239475A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6572888A JPH01239475A (en) 1988-03-22 1988-03-22 Electronic watthour meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6572888A JPH01239475A (en) 1988-03-22 1988-03-22 Electronic watthour meter

Publications (1)

Publication Number Publication Date
JPH01239475A true JPH01239475A (en) 1989-09-25

Family

ID=13295369

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6572888A Pending JPH01239475A (en) 1988-03-22 1988-03-22 Electronic watthour meter

Country Status (1)

Country Link
JP (1) JPH01239475A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5903145A (en) * 1992-02-21 1999-05-11 Abb Power T & D Company Inc. Universal electronic energy meter for use with 4-wire standard services

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5903145A (en) * 1992-02-21 1999-05-11 Abb Power T & D Company Inc. Universal electronic energy meter for use with 4-wire standard services
US6229295B1 (en) 1992-02-21 2001-05-08 Abb Power T&D Company Inc. Apparatus for metering at least one type of electrical power over a predetermined range of service voltages
US6940268B2 (en) 1992-02-21 2005-09-06 Elster Electricity, Llc Apparatus for metering at least one type of electrical power over a predetermined range of service voltages

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