JPS58167969A - Measurement of effective value - Google Patents

Measurement of effective value

Info

Publication number
JPS58167969A
JPS58167969A JP4888182A JP4888182A JPS58167969A JP S58167969 A JPS58167969 A JP S58167969A JP 4888182 A JP4888182 A JP 4888182A JP 4888182 A JP4888182 A JP 4888182A JP S58167969 A JPS58167969 A JP S58167969A
Authority
JP
Japan
Prior art keywords
frequency
value
effective value
sampling
input
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.)
Granted
Application number
JP4888182A
Other languages
Japanese (ja)
Other versions
JPH037072B2 (en
Inventor
Hiroshi Igawa
博 井川
Shigeru Taniguchi
茂 谷口
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
Tokyo Shibaura 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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP4888182A priority Critical patent/JPS58167969A/en
Publication of JPS58167969A publication Critical patent/JPS58167969A/en
Publication of JPH037072B2 publication Critical patent/JPH037072B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R19/00Arrangements for measuring currents or voltages or for indicating presence or sign thereof
    • G01R19/02Measuring effective values, i.e. root-mean-square values

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Current Or Voltage (AREA)

Abstract

PURPOSE:To enable accurate measurement of effective values with limited errors in the computation accompanied by frequency variations in the waveform of the AC input by correcting a sampling value of the AC input waveform with a deviation between the actual frequency and the reference frequency. CONSTITUTION:An AC input waveform obtained through a potential transformer 1 undergoes an A/D conversion detecting two sampling values having a fixed phase difference pi/2 in the reference frequency f0 with an A/D converter 2. A frequency transducer 3, outputs a level signal proportional to the frequency f0 of the AC input waveform to be fed the A/D converter 2. The A/D conversion outputs thus obtained is sent to an effective value arithmetic unit 4 and one of sampling data is corrected by a phase pi DELTAf0/2f0 according to a variation value DELTAf0 of an actual frequency f0' from the reference frequency f0 to form a data with a relative phase difference separated just by pi/2 whereby an effective value is calculated. This enables the correction of errors in the computation of a digital effective value accompanied by variations in the AC input frequency.

Description

【発明の詳細な説明】 仕術分針の数例。[Detailed description of the invention] A few examples of sajutsu minute needles.

本妬明は交流入力波形を所定のサンプリング周波数です
ンプリングしそのサンプリング値を用いてla瀝演算鳳
虐により交流人力実効値を算出する実効値測定方法に係
り、交流入力の周波数変動に伴なう誤差をなくすための
補正子IRに関するものである。
This paper relates to an effective value measurement method in which an AC input waveform is sampled at a predetermined sampling frequency, and the sampled value is used to calculate the AC human power effective value by LA calculation. This relates to a corrector IR for eliminating errors.

発明の技術め背景およびその間馳点 父流入力波形な加定のサンプリング周波数でサンプリン
グし、そのテンプリング値を用いて交流人力実効値を算
出する方法は各sあるが、その中で「横形演算原理」と
呼ばえる実効値演jl原塊が良く用いられている。
There are various methods of sampling the current input waveform at an additional sampling frequency and calculating the AC human power effective value using the Tempering value. The effective value calculation jl original block, which can be called "principle", is often used.

このam演3!原塩とは、交流入力波形から祷られるT
離れ次任意の2つの竺ンプリング値から、実効値を算出
するテイジタル夾効蝋演算手法である。例えは’(%)
 = Vs&+2g10tなる交流入力波形があつ友場
合、Vの値は任意の時刻tlに計るサンプ甑t(tl−
−L−)から 4f。
This AM performance 3! Raw salt is T determined from the AC input waveform.
This is a digital additive calculation method that calculates an effective value from two arbitrary sampling values. An example is '(%)
= Vs&+2g10t, the value of V is the sample t(tl-
-L-) to 4f.

V” ” r”(11) + r”(tl −」−) 
−−−−−−−−−(L)10 と求めることがで自、この計算式を用いれは、原塩的−
二−ll!!l#i生じない。
V""r" (11) + r" (tl -" -)
−−−−−−−−−(L)10 can be calculated as follows.Using this calculation formula, it is possible to calculate
Two-ll! ! l#i does not occur.

ここで通常、サンプリング周期はあらかじめ決まってお
り、ちょうど位相が丁離れたデータをフンブリング出来
るような時間間隔でサンプリングを何なっている。もし
、交流入力波形のmaaが当初予定の1拳となる周波数
f0からΔjOたVIずれて(/、十Δf、 ) Cな
ると、正しいVはy” = y”($1) + v” 
(il −4(fcl+mf6))・・・(2)にて求
めるべきところである。しかし%笑除6二は上記(1)
式を計算しているため、多少のw4*が生じる。す・な
わち、サンプリングデータとして、位相鵬波数の変動に
伴ない、相対的位相差かiより多少ずれたデータを使用
せざるを得ないために誤差が尭生する。
Normally, the sampling period is predetermined, and sampling is performed at such time intervals that it is possible to humbulate data whose phases are exactly apart. If maa of the AC input waveform deviates from the originally planned frequency f0 of 1 fist by ΔjO VI (/, 1Δf, )C, the correct V is y” = y”($1) + v”
(il -4(fcl+mf6))...This should be found in (2). However, %lol excluding 62 is above (1)
Since we are calculating the formula, some amount of w4* occurs. That is, as sampling data, it is necessary to use data that is slightly shifted from the relative phase difference i due to fluctuations in the phase and wave numbers, resulting in errors.

上述の通り、横形演算原理を用いて、交流入力波形の実
効値を算出する場合、従来、交流入力波形の周波数変動
に伴ない、算出した実効値t: i14*が生じていた
As described above, when calculating the effective value of an AC input waveform using the horizontal calculation principle, conventionally, the calculated effective value t: i14* occurs as the frequency of the AC input waveform changes.

角−の目的 本尭−のl的は、横形演算原理を用いて交流入力波形の
サンプリング値より実効値な算出する一一際し、その交
流入力波形のjlIla畝変動礁;伴なう撫Jl−差が
少なく正伽な実効値を得ることができる実効値調定方法
を提供することC″−ある。
The purpose of the corner is to calculate the effective value from the sampling value of the AC input waveform using the horizontal calculation principle, and then calculate the jlIla ridge fluctuation reef of the AC input waveform; - To provide an effective value adjustment method that can obtain accurate effective values with little difference.

尭1i[)飢賛 本角−はある基準となる周FIL a 10の交流入力
波形を所定周波数でサンプすると共舊;、上記&隼とな
るj[数I・−二おける一定の位相差iを有する2つの
サンプリング値を検出し、かつ前記交流入力波形の実際
の周rILajを検出し、前記基準となる周波数fo4
二対する偏差Δf、か、らこれ−二対応する位分、II
II記実際の周波数fの、前記基準となるJthllr
IL畝foc対する増または減方向g:ずれた位相のサ
ンプリング値となるように袖正し、この補正した一万の
値と残りのサン1リンダ値と6二よりi形演算原塩礁ユ
よって実効値を求め為こと6二よ01交流人力a形1;
よる周波数変動を補正し、この周波数置11g11区−
伴なう演算誤差を少なくした実効値測定方法6二ある。
孭1i[) 扭子本斯- is a certain reference frequency FIL a When the 10 AC input waveforms are sampled at a predetermined frequency, the above &Hayabusi j [a constant phase difference i in the number I・-2 , detect two sampling values having the reference frequency fo4, detect the actual frequency rILaj of the AC input waveform,
Two deviations Δf, or from this - two corresponding digits, II
II. The reference Jthllr of the actual frequency f
Increase or decrease direction g with respect to IL ridge foc: Correct the sleeve so that it becomes a sampling value with a shifted phase, and from this corrected value of 10,000, the remaining Sun 1 Linda value, and 6 2, the i-type calculation is To find the effective value, 62 yo 01 AC human power a form 1;
Correct the frequency fluctuation due to this frequency position 11g11 section -
There are six effective value measurement methods that reduce the accompanying calculation errors.

発明の実施例 −以下、図面な参踏して本%明の一実施例を簡単6二祝
−する。
Embodiments of the Invention Hereinafter, one embodiment of the present invention will be briefly described with reference to the drawings.

II I NIL本軸明方法を実行する装線代表的な#
l4Ilt例を示す。第1図に於て−j定対象となる交
流電圧波形を信号レベル4:下げるための計鯵用変圧番
lを設ける。この計暢用変圧器lを逃して得られた交流
入力波形Fi、ム/D変換62 により、所定のサンプ
リング周期−二でサンプリングされ、かつアナログディ
ジタル変換される。又、周波数トランスデユー?(Fテ
D)3は、上記交流入力波形の周波数6二比例したレベ
ル信号を出力し、前記A/D質換器2を通じて周波数を
表わすディジタル麺4二変換される。
II I NIL Typical wire installation # to carry out the main axis clearing method
An l4Ilt example is shown. In FIG. 1, a measuring transformer number 1 is provided for lowering the signal level 4 of the AC voltage waveform to be subjected to -j constant. The AC input waveform Fi obtained by passing through the measuring transformer l is sampled at a predetermined sampling period of -2 by the M/D conversion 62, and is converted into an analog-to-digital signal. Also, frequency transdue? (FteD) 3 outputs a level signal proportional to the frequency 6 of the AC input waveform, which is converted into a digital signal 42 representing the frequency through the A/D converter 2.

上記のようにして得られ゛たム/D f換勧出力#′i
、実効値演算装置4I−送られ、こζで、前記交流入力
サンプリング愉を周波数入力により補止した値を用いて
、槍形演3!腺1llI:より、実効値演算するよう5
ニして構成する。
The sum/D f exchanged output #'i obtained as above
, is sent to the effective value calculation device 4I, and this ζ uses the value obtained by supplementing the AC input sampling value with the frequency input to calculate the spear shape 3! Gland 1llI: From 5 to calculate the effective value.
and configure it.

交流電流#1.形1:IIL、ても、信号レベル感二下
げるための変#l餘5を通じて得られた交流入力波形を
前記交流電圧波形と゛Pi様−二処履すること1二より
、周波数軸圧な竹なった実効値演算が可能である〇次C
1本妬−の原理的動作I:ついて帛2図を参゛) 照して説明する。絽1&Aで示した針慟用変圧輪lC二
より得られる交流入力波形の実線の周flL欽が尚初子
定されてい***となる交流入力JIil披数がIoか
ら例えばj、cj、+Δf、 > l:変動した場合%
纂2−5;示す通す、実際にサンプリングされる二つの
サンプリングデータの相対的位相差は、尚初子足由する
AC current #1. Form 1: IIL, by processing the AC input waveform obtained through the change #l function 5 to lower the signal level with the AC voltage waveform, it is possible to obtain the frequency axis pressure. It is possible to calculate the effective value of
The principle operation of Ippon envy (I) will be explained with reference to Figure 2. If the circumference flL of the solid line of the AC input waveform obtained from the transformer wheel lC2 shown in 甽1&A is still determined first, the AC input JIil and the number from Io to, for example, j, cj, +Δf, > l: % if fluctuated
Essay 2-5: As shown, the relative phase difference between the two actually sampled data is still the same.

そこで、前記実効値演算(ロ)路の入力と1て、このフ
ンプリンダデータ≦;加えて周波数トランスデューデー
から0jli1波数゛信波数入信り、、−s この周波
数mm11甑Δj、 t=応じて、サンプリングデータ
の一方桶正して相対的位相差がちょうど6離れたデータ
となるようにした後、*誰演鼻原塩5二て1[其するよ
う1二すれri′%交流入力周波数変動に伴なうディジ
タル央矯値演算−差を補正することができる。
Therefore, with the input of the effective value calculation (b) path, this frequency transducer data ≦; In addition, from the frequency transducer, 0jli1 wave number ゛signal wave number input, -s This frequency mm11 Δj, t=depending After correcting one side of the sampling data so that the relative phase difference is exactly 6 apart, Digital median correction due to fluctuations - differences can be corrected.

次に本発明の具体的手法を第31の70−チャートな参
蝋して鋭−する。
Next, the specific method of the present invention will be explained with reference to the 31st 70-chart.

1ず纂1嫡で示したム/D変換餘2から交流入力荻形の
1周期分のサンプリングデータな夾5cb値演%俟@4
へ入力する(ステップa)。但しこのサンプリング周波
数は、、互の数倍以上(費数倍)とする。そしてこのサ
ンプリングデータがマイナスからプ□ラス又祉プラスか
らマイ矢スヘ極性変化する部分や二つのサンプリングデ
ータ例えば壓4凶のサンプリングデータV(sx)及び
、V(ts)を艶出する(ステップ’b)。上述した極
性変化部分1i、波形の直線性が蛾も保良れている部分
である0次g;、周a数トランスデエーナ−(PTD)
より5eR入力波形の実際の周波数f・′を入力しくス
テップC)%蟲初子定の基準となる周波数f0との大き
さを比較する(ステップa)。このfo’とj、の大き
さt−Fifo > fo o場合と10’< /a 
o場合の二基りが考えられるが、どちらかを判断して、
下記のように演算処塩する。
Sampling data for one period of AC input ogiform from the Mu/D conversion unit 2 shown in 1st line 1st order 5cb value performance @ 4
(step a). However, this sampling frequency shall be several times higher than each other (multiple times the cost). Then, the part where the polarity of this sampling data changes from negative to positive or positive to positive or negative, or two sampling data, for example, the sampling data V(sx) and V(ts) of 壓 4 evil are polished (step' b). The above-mentioned polarity change part 1i is a part where the linearity of the waveform is well maintained, which is the 0th order g;, a frequency transducer (PTD).
Step C) Input the actual frequency f·' of the 5eR input waveform and compare the magnitude with the frequency f0, which is the standard for determining the percentage of insects (Step a). The size of fo' and j is t-Fifo > fo o and 10'< /a
There are two possibilities for case o, but decide which one,
Perform calculations as shown below.

■f−’>joの場合(九′=1.÷ムj0と仮足する
)第4鵬に示す通りサン1りンlデータ V(tl)とV($1)の間の波形の@lll1性が1
111保ft−レテイbコトをill!j:V(sl)
とV(Im)のデーzかbmnJlc!す、1m正デー
タV($1″)を下木儂;より算出する(ステツ゛プ・
)。この補正データV(%え′)は、サンプリングデー
タV(t、)との位相差が周波数1.’=1.+ΔfC
;於露 て、丁RT を二相幽する補正データである0そしてこ
のサンプリングデータV(S、)及び−正量V(11’
)を用いて検形演其鳳急により実効値演算を行なえは(
ステップノ)、周波数による一#iのほとんどない実効
値が算出できる。
■ In the case of f-'> jo (temporarily add 9' = 1. ÷ m j0) As shown in the 4th section, the @ of the waveform between Sun 1 Rin l data V (tl) and V ($1) lll1 sex is 1
111 ft-Ill tell you what to do! j:V(sl)
And V(Im) day z or bmnJlc! Then, calculate the 1m positive data V ($1″) from the lower tree (step
). This correction data V (%e') has a phase difference with the sampling data V (t,) of frequency 1. '=1. +ΔfC
; 0, which is the correction data that suppresses the two-phase RT, and this sampling data V(S,) and -positive amount V(11'
) can be used to calculate the effective value according to the test method.
Step no), it is possible to calculate almost no effective value of #i depending on the frequency.

V(t1’) = 1(IT(tIN+1v(sl月)
Δj。
V(t1') = 1(IT(tIN+1v(sl month)
Δj.

x (4i。(7゜。4j、)/(、;))−1v(s
1川/s:をンプリング周獣数 ■i、’<i、の場合(九′=j0−Δ九と仮足する)
継5−−−示す過り、上記■項とニジ」祿にしてサンプ
リングデータV(tl)とV($3)から袖関fkl二
より、循正データv<s@’>を下式により算出する(
ステップg)。この補正データV(Ss’)$1ナング
リングデータV($4)との位相差が、胸波数九′=j
0−Δjに於て丁簾五に相幽するデータである。そして
このサンプリングデータV($4)及び補正値V(ml
’)を用いて槓形演″I/#創引:、より実効値演算を
行なえは(ステップh)s周波数によるI#4差のtl
とんとない実効値が算出できる。
x (4i.(7°.4j,)/(,;))−1v(s
1 river/s: Sample the cycle animal number ■i, if '<i, (temporarily add 9' = j0 - Δ9)
Continuation 5---As shown above, from the sampling data V(tl) and V($3), the circulation data v<s@'> is calculated by the following formula from the sampling data V(tl) and V($3). calculate(
Step g). The phase difference between this correction data V (Ss') $1 and the nangling data V ($4) is the chest wave number 9' = j
This is the data that corresponds to the length of the curtain at 0-Δj. Then, this sampling data V ($4) and correction value V (ml
') is used to calculate the effective value of ``I/# creation:'' (Step h) tl of I#4 difference depending on s frequency
An incredible effective value can be calculated.

V(tg’)=  1(IV($1月+IV(1,)l
)j、:サンプリングlll4tIL数 尚、110項及び■積でIVI述した通り九′〉joの
場酋;サンプリングデ―りV($1)及びV($9)i
o’<1.の場合;サンプリングデーfi V(%s)
 JILU V($43を用いること1二より%胸fI
L数変動によるm−に対する。サンプリングデータの補
正を厘1ml性の蝋も保たれている部分(tXとtsQ
関)で竹なう仁とができる。
V(tg')=1(IV($1 month+IV(1,)l
)j, : Sampling lll4tIL number As mentioned in IVI in terms of 110 and ■ product, the case of 9′〉jo; sampling date V($1) and V($9)i
o'<1. In the case of; sampling data fi V (%s)
JILU V (Using $43 12% Breast fI
For m- due to L number variation. The sampling data was corrected for the part where 1 ml of wax was also preserved (tX and tsQ).
Seki) and Takenaujin is established.

総合的な効果 以上、本尭明感二よれは横形演31!鳳珈C二より交流
人力夷5wl値を算出する場合、交流人力6二胸畝数変
動があっても、はとんど−艷のない実効fIi演舞が実
現できる。
More than the overall effect, Motoya Akira Kanjiyore is 31 horizontal performances! When calculating the AC human force 5wl value from the AC human force C2, even if there is a change in the number of AC human force 62 pectoral ridges, an effective fli performance without any fIi can be realized.

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

第1図は本発明方法な実行するディジタル実効憧演鼻回
路のII地例を示すプルツク回路図、謝2図は本発明の
atm的動作を説明する波形図、絽3凶は本発明による
実効値掬定方法の一実施例な示すフローチャート、第4
図および第5凶は第3図で示した方法における動作を説
明するための波形図である。 1・・・計−用変圧− 2・・・アナ關ダデイジタル変換器 5−saIILトランスデユーサ− 4・・・実効値演算装置 5・・・変tlL鯵(7J1
17)代珈人 弁膣士 則 釘 麿 佑 (#盆か1名
)第1図 第2図 第4図 第51!1
Fig. 1 is a pull circuit diagram showing an example of a digital effective performance circuit executed by the method of the present invention, Fig. 2 is a waveform diagram explaining the ATM-like operation of the present invention, and Fig. Flowchart showing an embodiment of the value estimation method, No. 4
Figure 5 and Figure 5 are waveform diagrams for explaining the operation in the method shown in Figure 3. 1... Meter transformer 2... Analog digital converter 5-saIIL transducer 4... Effective value arithmetic device 5... Transformer tlL mackerel (7J1
17) Daikajin Ben-vagina Nori Kugi Maro Yu (#Bon or 1 person) Figure 1 Figure 2 Figure 4 Figure 51!1

Claims (1)

【特許請求の範囲】[Claims] (1)  ある基準となる0周波*jtso交流入力液
形を所定周液倣でナングすると共−二、上記基準と唸る
周f11.象l・1:おける一定の位相差)を有する3
つのサンプリング値を検出し、かつ前記交流入方波y#
O貴−〇周波数ftを検出し、前記基準となる周波数j
ot二対する偏差Δ/、からこれε:対応する位相前記
seem波数への、前記基準となる周披軌I:対する増
または滅方向葛:ずれた位相のサンプリング値となるよ
う6二補正し、この補正し九一方の値とmeOt、ング
リンl値と6−より積形演算厚層によって実効″値を求
める*拳値1m15i!方法・(1)  6る基準とな
る周波II/・の交流周IIIL数を所定周tILII
kl・でナングリンlすると共c:、この交流入力波形
の、液形の直S性かはぼ保たれる@性反転点WN懐の2
つのサンプリング値V($1)、v(tg)およびこれ
ら2つのサンプリング* V($1)+V(til)1
二対しそれぞれ基準となる周波数ムにおける一定の位相
差iを有するサンプリング値V($11)IT(s4)
を検出し、かつ前記交流入力波形の実際の属波数1−を
検出して前記基準となる周波*i、に対する大小間係を
判定すると共6:その偏差ΔI0を求め、その結果j’
、 > joでI;冨j0+Δj0の場合は、前記2つ
のサンプリングmV(sx)、V(tm)から−閣法に
より補正値v(を白を 11V(S8)と蓄:より横形演算鳳W効値を求め。 f′o<joで八=/、−Δf0の場合は同じく袖閣法
−二より補正値’V(l’)を 1二て求め、この補正値V($11’)と前記サン1リ
ング愉V(4番)とにより横形演算原理にて実効値を釆
める実効値測定方法。
(1) When the 0 frequency *jtso AC input liquid type, which is a certain reference, is numbered by copying the predetermined frequency, the frequency f11. 3 with a certain phase difference)
and detect the AC incoming wave y#
Detect the frequency ft and use the reference frequency j
ot2 deviation Δ/, from this ε: corresponding phase to the seem wave number, the reference circumferential trajectory I: increase or decrease relative to it: 62 correction so that the sampling value of the shifted phase is obtained, and this correction The effective value is determined by the product calculation thickness layer from the one value, meOt, and the ring l value. The number of cycles tILII
When we do nangrin l with kl, c:, the directness of the liquid form of this AC input waveform is almost maintained, and the inversion point of WN is 2.
two sampling values V($1), v(tg) and these two samplings *V($1)+V(til)1
Two pairs of sampling values V($11)IT(s4) each having a constant phase difference i at the reference frequency m
and detect the actual dependent wave number 1- of the AC input waveform to determine the magnitude relationship with respect to the reference frequency *i.
, > I in jo; If the value is j0 + Δj0, from the two samplings mV (sx) and V (tm), the correction value v (white is stored as 11 V (S8)) according to the Cabinet method: From the horizontal calculation, the effective value of W is calculated. If f′o<jo and 8=/, -Δf0, calculate the correction value 'V(l') by 12 from the Sokaku method-2, and combine this correction value V($11') with the above sample. An effective value measurement method in which the effective value is determined using the horizontal calculation principle using the 1-ring V (No. 4).
JP4888182A 1982-03-29 1982-03-29 Measurement of effective value Granted JPS58167969A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4888182A JPS58167969A (en) 1982-03-29 1982-03-29 Measurement of effective value

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4888182A JPS58167969A (en) 1982-03-29 1982-03-29 Measurement of effective value

Publications (2)

Publication Number Publication Date
JPS58167969A true JPS58167969A (en) 1983-10-04
JPH037072B2 JPH037072B2 (en) 1991-01-31

Family

ID=12815620

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4888182A Granted JPS58167969A (en) 1982-03-29 1982-03-29 Measurement of effective value

Country Status (1)

Country Link
JP (1) JPS58167969A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008029107A (en) * 2006-07-20 2008-02-07 Mels Corp Sine wave rms value detector and sine wave power supply device using the same
CN105891585A (en) * 2016-04-01 2016-08-24 许继集团有限公司 Effective value calculating method and device in sine wave frequency slow change process

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008029107A (en) * 2006-07-20 2008-02-07 Mels Corp Sine wave rms value detector and sine wave power supply device using the same
CN105891585A (en) * 2016-04-01 2016-08-24 许继集团有限公司 Effective value calculating method and device in sine wave frequency slow change process

Also Published As

Publication number Publication date
JPH037072B2 (en) 1991-01-31

Similar Documents

Publication Publication Date Title
US4210022A (en) Method for the inductive measurement of fluid flow
EP2027475A1 (en) Method and device for demodulation of signals
CN103344825A (en) Electric energy measuring system based on alternating-current sampling
JPS58167969A (en) Measurement of effective value
CN110763915B (en) Method for calculating voltage included angle and zero line current and three-phase electric energy meter
JPS5920534A (en) Fuel feeder for internal combustion engine
SU1755070A1 (en) Apparatus for temperature measuring and checking
SU951358A1 (en) Shaft rotation angle to voltage convertion method
JP3075319B2 (en) Electromagnetic flow meter
JP2522532B2 (en) Fuzzy controller
SU978061A1 (en) Inductor power measuring device
SU752244A1 (en) Device for proportioning flows
Fitzenreiter et al. Velocity-space synthesis of ISEE-1 measurements of the three dimensional electron distribution function
RU2093841C1 (en) Measuring transducer for current and voltage harmonic components
SU477361A1 (en) Method for converting current value of voltage to gain
SU964453A2 (en) Electromagnetic flowmeter
SU466465A1 (en) Measurement method of alternating voltage
RU2161772C2 (en) Angle determination device
JP3598521B2 (en) Data table processing device
SU443259A1 (en) The method of controlling the level of liquid in the yeast growth tank
SU808776A1 (en) Method of automatic control of recirculating flue gas flowrate in steam generator with steam reheater
JPS5763459A (en) Reactive power meter
SU746336A1 (en) Three-phase network asymmetry digital meter
SU738141A1 (en) Method and device for converting differential transformer output signal into pulse-width signal
SU506035A1 (en) Method of converting the rotation angle