JPH0666844A - Digital estimating operating method for ac input amplitude - Google Patents

Digital estimating operating method for ac input amplitude

Info

Publication number
JPH0666844A
JPH0666844A JP4221848A JP22184892A JPH0666844A JP H0666844 A JPH0666844 A JP H0666844A JP 4221848 A JP4221848 A JP 4221848A JP 22184892 A JP22184892 A JP 22184892A JP H0666844 A JPH0666844 A JP H0666844A
Authority
JP
Japan
Prior art keywords
value
sampling
point
input
amplitude
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
JP4221848A
Other languages
Japanese (ja)
Other versions
JP3099542B2 (en
Inventor
Seiji Uebu
誠二 上蔀
Kenji Arai
健司 新井
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.)
Fuji Electric Co Ltd
Fuji Facom Corp
Original Assignee
Fuji Electric Co Ltd
Fuji Facom 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 Fuji Electric Co Ltd, Fuji Facom Corp filed Critical Fuji Electric Co Ltd
Priority to JP04221848A priority Critical patent/JP3099542B2/en
Publication of JPH0666844A publication Critical patent/JPH0666844A/en
Application granted granted Critical
Publication of JP3099542B2 publication Critical patent/JP3099542B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To provide an estimated value of amplitude of an AC input signal with less frequency fluctuation error from the sampling value of the AC input signal. CONSTITUTION:Among AC input sampling values, the sampling value just before O-cross point in a O-cross point part ZP is a1, the sampling value just after it is a2, and the sampling value situated ahead by the time interval corresponding to the phase difference 90 deg. of a standard frequency from the sampling point of the value a1 is b1, and the sampling value situated ahead by the time interval corresponding to the phase difference 90 deg. of the standard frequency from the sampling point of the value a2 is b2. The 90 deg. 2-point arithmetic value m2 is determined from the values a2, b2. When the corresponding value Em' of the 90 deg. 2-point arithmetic value of the O-cross point is determined by the linear interpolation of the arithmetic values m1, m2, this value gives an ZC input estimated value close to an AC input true value Em.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は交流入力信号をサンプリ
ングしてA/D変換し、この変換されたデジタルデータ
から交流入力信号の振巾を推定演算する方法、特に入力
周波数の変動時にも高精度が得られる交流入力振巾のデ
ジタル推定演算方法に関する。なお以下各図において同
一の符号は同一もしくは相当部分を示す。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention is a method for sampling an AC input signal, performing A / D conversion, and estimating and calculating the amplitude of the AC input signal from the converted digital data. The present invention relates to a digital estimation calculation method of an AC input amplitude that can obtain accuracy. In the drawings below, the same reference numerals indicate the same or corresponding parts.

【0002】[0002]

【従来の技術】例えば60Hzの交流入力信号を電気角
15°に相当する固定のサンプリング周期(換言すれば
交流入力信号の周期1/60(sec)の15/36
0)でサンプリングしてA/D変換し、このデジタル変
換されたサンプリング値のうち電気角90°の時間間隔
(つまり(1/60)×1/4(sec))を持つサン
プリング値をa,bとしたときその交流入力信号の振巾
Emは
2. Description of the Related Art For example, an AC input signal of 60 Hz has a fixed sampling period corresponding to an electrical angle of 15 ° (in other words, 15/36 of the period 1/60 (sec) of the AC input signal).
0) sampling and A / D conversion, and among the digitally converted sampling values, a sampling value having a time interval of an electrical angle of 90 ° (that is, (1/60) × 1/4 (sec)) is a, When b, the amplitude Em of the AC input signal is

【0003】[0003]

【数1】Em=(a2 +b2 1/2 ………(1) として求められる。なお便宜上、この演算法を90°2
点演算法といい、この演算で求めた演算値、つまり式
(1)のEmに相当する値を90°2点演算値と呼ぶ。
しかしこの方法では交流入力周波数が変動すると誤差が
大きく出てしまうのが普通である。
## EQU1 ## Em = (a 2 + b 2 ) 1/2 (1) For convenience, this calculation method is 90 ° 2.
This is called a point operation method, and the operation value obtained by this operation, that is, the value corresponding to Em in Expression (1) is called a 90 ° 2-point operation value.
However, this method usually causes a large error when the AC input frequency fluctuates.

【0004】図6は基準周波数を60Hzとした前記の
固定サンプリング周期で周波数が57Hzに変化した交
流入力信号をサンプリングした場合のサンプリング値
(上段)と、このサンプリング値を用い90°2点演算
法により求めた交流入力信号の振巾推定値(つまり90
°2点演算値)の真値に対する誤差(下段)との関係を
示す。この場合、式(1)に用いるサンプリング値a,
bの位相によって誤差も大きく変化し、最大約4%の誤
差となる。
FIG. 6 shows a sampling value (upper row) when an AC input signal whose frequency has changed to 57 Hz is sampled at the fixed sampling cycle with the reference frequency of 60 Hz, and a 90 ° two-point arithmetic method using this sampling value. The estimated amplitude of the AC input signal obtained by
Shows the relationship between the true value of the two-point calculation value) and the error (lower row). In this case, the sampling value a used in equation (1),
The error greatly changes depending on the phase of b, and the maximum error is about 4%.

【0005】ただし、この誤差は半周期分の90°2点
演算値を平均とするとほぼ“0”になるという特性が有
り、従来は前述のサンプリング値を用いて基準周波数の
電気角30°の時間間隔ごとに90°2点演算を6点で
行い、その演算値を平均化することで誤差を最小化して
いた。図7は図6に対応する図で、図7の下段は図6の
90°2点演算値にこの30°6点平均を施した際の誤
差の減少状態を示し、この場合、最大約0.2%の誤差
となる。
However, this error has a characteristic that it is almost "0" when the 90 ° 2-point calculation value for a half cycle is averaged. Conventionally, using the above-mentioned sampling value, the electrical angle of the reference frequency of 30 ° The error was minimized by performing 2-point calculation of 90 ° at 6 points at each time interval and averaging the calculated values. FIG. 7 is a diagram corresponding to FIG. 6, and the lower part of FIG. 7 shows a state of error reduction when the 30 ° 6-point average is applied to the 90 ° 2-point calculated value of FIG. There is an error of 2%.

【0006】[0006]

【発明が解決しようとする課題】しかしながら、図7の
ように6点の演算値を求めるには処理時間がかかり、ま
た演算時点により結果が変動し、交流入力信号の振巾を
高精度で求めたい場合には、なお無視できない誤差が出
るという問題がある。そこでこの発明の課題は、周波数
変動時にも高精度が得られるような交流入力振巾のデジ
タル推定演算方法を提供することにある。
However, as shown in FIG. 7, it takes a long processing time to obtain the calculated values of the six points, and the result fluctuates depending on the time of the calculation, so that the amplitude of the AC input signal can be obtained with high accuracy. If you want to, you still have the problem that there are errors that cannot be ignored. Therefore, an object of the present invention is to provide a digital estimation calculation method of an AC input amplitude that can obtain high accuracy even when the frequency changes.

【0007】[0007]

【課題を解決するための手段】前記の課題を解決するた
めに、請求項1のデジタル推定演算方法では、基準周波
数の前後に周波数が変動し得る交流入力信号をこの基準
周波数の周期1/4n(但しnは2以上の所定の整数と
する)の固定サンプリング周期でサンプリングしてA/
D変換し、このデジタル変換されたサンプリング値から
前記交流入力信号の振巾(Emなど)を推定する方法で
あって、前記交流入力信号の0クロス点の直前のサンプ
リング値(a1など)を用いた90°2点演算値(m1
など)と、該0クロス点の直後のサンプリング値(a2
など)を用いた90°2点演算値(m2など)との直線
補間により、この0クロス点の90°2点演算値に相当
する値(Em’など)を求め、該値を前記交流入力信号
の振巾の推定値とする。
In order to solve the above-mentioned problems, in the digital estimation calculation method according to the first aspect, an AC input signal whose frequency can fluctuate before and after the reference frequency is set to a period ¼n of this reference frequency. (Where n is a predetermined integer of 2 or more) is sampled at a fixed sampling period and A /
A method of D-converting and estimating the amplitude (Em, etc.) of the AC input signal from the digitally converted sampling value, using a sampling value (a1, etc.) immediately before the 0 cross point of the AC input signal. 90 ° 2-point calculated value (m1
Etc.) and the sampling value immediately after the 0 cross point (a2
, Etc.) is used to obtain a value (Em ′, etc.) corresponding to the 90 ° two-point calculated value of this 0 cross point by linear interpolation with the 90 ° two-point calculated value (m2, etc.), and the value is input to the AC input. Estimate the amplitude of the signal.

【0008】また請求項2のデジタル推定演算方法で
は、請求項1の記載の推定演算方法において、さらに前
記交流入力信号の周波数(fなど)を求め、この周波数
と前記固定サンプリング周期とを用いて前記交流入力信
号の振巾の推定値に所定の(式(6)の)補正を施した
値を改めて前記交流入力信号の振巾の推定値(Em”な
ど)とする。
According to the digital estimation calculation method of claim 2, in the estimation calculation method according to claim 1, the frequency (f, etc.) of the AC input signal is further obtained, and this frequency and the fixed sampling period are used. A value obtained by subjecting the estimated value of the amplitude of the AC input signal to predetermined (formula (6)) correction is again used as the estimated value of the amplitude of the AC input signal (Em ″ or the like).

【0009】[0009]

【作用】この発明では、演算アルゴリズム上、最も誤差
の小さい時点(0クロス点)を検出し、その直前,直後
のサンプリング値を用いて夫々90°2点演算を行い、
その二つの90°2点演算値に直線補間を施して近似的
に0クロス点での90°2点演算値に相当する値を求
め、この値を交流入力信号の振巾の推定値とすることに
より、周波数変動時の誤差を最小化する。また必要に応
じさらにこのときの周波数を検出し、その周波数を用い
た補正式により前記の推定値に補正を施し、より誤差の
少ない推定値を得る。
According to the present invention, the point at which the error is smallest (0 cross point) is detected in the calculation algorithm, and the 90 ° two-point calculation is performed using the sampling values immediately before and immediately after that,
By linearly interpolating the two 90 ° two-point calculated values, a value approximately corresponding to the 90 ° two-point calculated value at the 0 cross point is obtained, and this value is used as the estimated value of the amplitude of the AC input signal. This minimizes the error when the frequency changes. If necessary, the frequency at this time is further detected, and the estimated value is corrected by a correction equation using the frequency to obtain an estimated value with less error.

【0010】この方法により90°2点演算は2回でよ
く、図2のように安定した演算結果が得られ、さらに周
波数誤差補正を行うことにより高精度な演算結果とな
る。
With this method, the 90 ° two-point calculation only needs to be performed twice, and a stable calculation result can be obtained as shown in FIG. 2. Further, by performing frequency error correction, a highly accurate calculation result can be obtained.

【0011】[0011]

【実施例】90°2点演算アルゴリズムにおいて、周波
数変動時、誤差が最小になるのは、図6に示したように
交流入力瞬時値が“0”及び“最大値”の時である。従
って本来なら、入力瞬時値が“0”の時点で90°2点
演算を行えば誤差は最小となるが、サンプリングは交流
入力と非同期であるため、サンプリング時点が0クロス
点と一致するとは限らない。このため本発明では入力瞬
時値の“0クロス点”をサンプリング値の符号が反転す
る点として検出し、その0クロス点の直前,直後の2つ
のサンプリング時点のサンプリングデータa1,a2
と、このサンプリングデータに対し夫々、基準周波数の
電気角90°に相当する時間間隔で以前にサンプリング
されたデータb1,b2とを用いて90°2点演算を二
回行い、この二つの演算データに直線補間を施すことに
より、近似的に入力瞬時値が“0”の時点の90°2点
演算値を推定している。図1はこの演算方法の説明図
で、同図(A)は上記のサンプリングデータを示し、同
図(B)は同図(A)の0クロス点部(丸の領域)ZP
の拡大図である。また同図(C)は直線補間の方法を示
す。次に図1を参照しつつ本発明の演算方法の詳細を説
明する。
EXAMPLE In the 90 ° two-point calculation algorithm, the error is minimized when the frequency fluctuates when the AC input instantaneous value is "0" and "maximum" as shown in FIG. Therefore, originally, the error is minimized if the 90 ° 2-point calculation is performed when the input instantaneous value is “0”, but since the sampling is asynchronous with the AC input, the sampling time does not always coincide with the 0 cross point. Absent. Therefore, in the present invention, the "0 cross point" of the input instantaneous value is detected as a point at which the sign of the sampling value is inverted, and the sampling data a1 and a2 at two sampling points immediately before and after the 0 cross point are detected.
90 ° two-point calculation is performed twice using the data b1 and b2 previously sampled at a time interval corresponding to the electrical angle 90 ° of the reference frequency, and the two calculated data By linearly interpolating with, the 90 ° two-point calculated value at the time when the input instantaneous value is “0” is approximately estimated. FIG. 1 is an explanatory diagram of this calculation method. FIG. 1A shows the above sampling data, and FIG. 1B shows the 0 cross point portion (circle area) ZP of FIG.
FIG. Further, FIG. 3C shows a linear interpolation method. Next, the details of the calculation method of the present invention will be described with reference to FIG.

【0012】サンプリングデータa1,b1を用いた9
0°2点演算値m1は次式(2)で表される。
9 using sampling data a1 and b1
The 0 ° 2-point calculation value m1 is expressed by the following equation (2).

【0013】[0013]

【数2】m1=(a12 +b12 1/2 ………(2) 同様にサンプリングデータa2,b2を用いた90°2
点演算値m2は次式(3)で表される。
## EQU2 ## m1 = (a1 2 + b1 2 ) 1/2 (2) Similarly, 90 ° 2 using the sampling data a2 and b2
The point calculation value m2 is expressed by the following equation (3).

【0014】[0014]

【数3】m2=(a22 +b22 1/2 ………(3) この2つの90°2点演算値m1,m2に直線補間を行
って真の0クロス点における90°2点演算値に相当す
る値としての交流入力振巾推定値Em’を求めると、此
の値は真の交流入力振巾Emに極めて近似した値とな
り、
## EQU3 ## m2 = (a2 2 + b2 2 ) 1/2 (3) The two 90 ° two-point calculation values m1 and m2 are linearly interpolated to calculate the 90 ° two-point calculation at the true 0 cross point. When the AC input amplitude estimated value Em 'as a value corresponding to the value is obtained, this value becomes a value extremely close to the true AC input amplitude Em,

【0015】[0015]

【数4】 Em≒Em’=m1+(m2−m1)・|a1/(a2−a1)|……(4) によって与えられる。次にさらに交流入力周波数fを測
定して上記式(4)で求めた交流入力振巾推定値Em’
から、より高精度に交流入力振巾推定値Em”を求める
方法を述べる。なお入力周波数fの測定は0クロス点の
検出を複数回行ってその時間間隔を求めることにより、
高精度に行うことができる。
[Equation 4] Em≈Em ′ = m1 + (m2-m1) · | a1 / (a2-a1) | ... (4) Next, the AC input frequency f is further measured, and the AC input amplitude estimated value Em ′ obtained by the above equation (4) is obtained.
From here, the method of obtaining the AC input amplitude estimated value Em ″ with higher accuracy will be described. The measurement of the input frequency f is performed by detecting the 0 cross point a plurality of times and obtaining the time interval thereof.
It can be performed with high precision.

【0016】理想的に0クロス点と、この点に対し基準
周波数の電気角90°相当分の時間間隔を持つ点とでサ
ンプリングが行われた場合における、90°2点演算法
における周波数変動時の誤差は理論上算出することがで
きる。なお図3はこの誤差の説明図で、同図(A)は交
流入力周波数fが基準の60(Hz)である場合を示
し、このとき0クロス点から基準周波数60Hzの電気
角90°に相当する時間間隔
Ideally, when sampling is performed at a zero cross point and a point having a time interval corresponding to an electrical angle of 90 ° of the reference frequency with respect to this point, when the frequency changes in the 90 ° two-point arithmetic method. The error of can be theoretically calculated. FIG. 3 is an explanatory diagram of this error. FIG. 3A shows a case where the AC input frequency f is the reference frequency of 60 (Hz), and at this time, it corresponds to an electrical angle of 90 ° from the 0 cross point to the reference frequency of 60 Hz. Time interval

【0017】[0017]

【数5】t=(1/60)×90/360(sec) を置いてサンプリングされた値bは正しく交流入力振巾
Emに一致することを示している。一方図3(B)は交
流入力周波数f=60+α(Hz)と周波数が増加側に
変動した場合を示し、この場合、固定サンプリング時間
tは変わらないので0クロス点からこの時間間隔tを置
いてサンプリングされた値bは、時間間隔tに対応する
電気角が90°より増加するので真の交流入力振巾Em
より若干分ΔEだけ小さな値となる。ところで式(1)
に示した90°2点演算値は理想的に0クロス点でサン
プリングが行われた場合、a=0であるから、
## EQU00005 ## The value b sampled with t = (1/60) .times.90 / 360 (sec) is shown to exactly match the AC input amplitude Em. On the other hand, FIG. 3B shows a case where the frequency fluctuates to the increasing side with the AC input frequency f = 60 + α (Hz). In this case, since the fixed sampling time t does not change, this time interval t is set from the 0 cross point. The sampled value b has a true AC input amplitude Em because the electrical angle corresponding to the time interval t increases from 90 °.
The value is slightly smaller by ΔE. By the way, formula (1)
The 90 ° two-point calculated value shown in is ideally a = 0 when sampling is performed at the 0 cross point,

【0018】[0018]

【数6】(a2 +b2 1/2 =|b| であり、一方このbの値は図3から判るように交流入力
周波数をfとすると、
## EQU6 ## (a 2 + b 2 ) 1/2 = | b |, on the other hand, the value of this b is, assuming that the AC input frequency is f, as can be seen from FIG.

【0019】[0019]

【数7】b=Em・Sin(2πf・t) =Em・Sin(2πf・(1/60)・90/36
0) で与えられる。従って
[Formula 7] b = Em · Sin (2πf · t) = Em · Sin (2πf · (1/60) · 90/36
0) is given. Therefore

【0020】[0020]

【数8】 Em=b/Sin(2πf・(1/60)・90/360)………(5) 一方このbの値は図1の演算で求められたEm’に相当
するものであるから、この式(5)は下式(6)のよう
に書換えることができる。
[Equation 8] Em = b / Sin (2πf · (1/60) · 90/360) (5) On the other hand, the value of b corresponds to Em ′ obtained by the calculation of FIG. Therefore, this equation (5) can be rewritten as the following equation (6).

【0021】[0021]

【数9】 Em”=Em’/Sin(2πf・(1/60)・90/360)……(6) 但しここで式(6)の左辺をEmの代わりにEm”とし
たのは式(5)の関係を用い、式(6)の右辺で求めた
値は交流入力信号の振巾の推定値であって、交流入力信
号の振巾の真値Emとは異なるためである。
[Equation 9] Em ″ = Em ′ / Sin (2πf · (1/60) · 90/360) (6) However, it is the equation that the left side of the equation (6) is Em ″ instead of Em. This is because the value obtained from the right side of the equation (6) using the relationship of (5) is an estimated value of the amplitude of the AC input signal and is different from the true value Em of the amplitude of the AC input signal.

【0022】つまりこの式(6)を用いて交流入力周波
数fと、0クロス点での90°2点演算値の相当値E
m’とから、より誤差の少ない交流入力信号の振巾推定
値Em”を求めることができる。図4は入力周波数f=
55Hz(即ち基準周波数60Hzに対し−5Hzの周
波数変動がある場合)、振巾Em=10Vの交流入力に
対し本発明の演算を行って推定された交流入力振巾推定
値(ここでは補正値と呼んでいる)を示す。即ち同図の
左端の縦1列の1〜7の数値は0クロス点の番号を、2
番目の縦1列の数値は0クロス点の直前のサンプリング
値に基づく90°2点演算値m1とその誤差%を、3番
目の縦1列の数値は0クロス点の直後のサンプリング値
に基づく90°2点演算値m2とその誤差%を、4番目
の縦1列の数値は上記演算値m1,m2から式(4)の
直線近似(直線補間)で推定した交流入力振巾推定値E
m’とその誤差%を、5番目の縦1列の数値は上記の推
定値Em’に更に式(6)の周波数補正を行って推定し
た交流入力振巾推定値Em”とその誤差%を夫々示す。
なおここで誤差%は交流入力レベルの真値Em=10V
に対する値を表し、また検出された周波数fは55.0
367Hzである。
That is, using this equation (6), the AC input frequency f and the equivalent value E of the 90 ° two-point calculated value at the 0 cross point are obtained.
The amplitude estimation value Em ″ of the AC input signal with a smaller error can be obtained from m ′. In FIG. 4, the input frequency f =
An AC input swing estimated value (here, a correction value) estimated by performing the operation of the present invention on an AC input having a swing Em = 10V at 55 Hz (that is, a frequency variation of -5 Hz with respect to a reference frequency of 60 Hz). Calling). That is, the numbers 1 to 7 in the vertical 1 column at the left end of FIG.
The numerical value in the 1st vertical column is based on the sampling value immediately before the 0-cross point, and the 90 ° 2-point calculated value m1 and its error%. The numerical value in the 3rd vertical 1-column is based on the sampling value immediately after the 0 cross point. The AC input amplitude estimated value E obtained by estimating the 90 ° 2-point calculated value m2 and its error% by the linear approximation (linear interpolation) of the equation (4) from the calculated values m1 and m2 in the fourth vertical one-column numerical value
m ′ and its error% are the AC input amplitude estimated value Em ″ estimated by performing the frequency correction of the equation (6) on the above-mentioned estimated value Em ′ and the error% thereof. Show each.
Here, the error% is the true value of the AC input level Em = 10V
And the detected frequency f is 55.0.
It is 367 Hz.

【0023】図5は入力周波数65Hz(即ち基準周波
数60Hzに対し+5Hzの周波数変動がある場合)の
図4と同様な演算結果を示す。このように基準周波数6
0Hzに対しほぼ10%の変動があっても本発明の式
(4)による直線補間により1%以下の誤差で交流入力
信号振巾の推定ができ、さらにこの推定値に式(6)周
波数補正を施せばこの誤差は1桁以上小さくなることが
判る。
FIG. 5 shows the same calculation result as in FIG. 4 for an input frequency of 65 Hz (that is, when there is a frequency variation of +5 Hz with respect to a reference frequency of 60 Hz). Thus, the reference frequency 6
Even if there is a variation of about 10% with respect to 0 Hz, the AC input signal amplitude can be estimated with an error of 1% or less by the linear interpolation according to the equation (4) of the present invention, and the estimated value is corrected by the equation (6) frequency correction. It can be seen that this error is reduced by one digit or more by applying.

【0024】[0024]

【発明の効果】本発明によれば0クロス点の直前,直後
のサンプリング値から得られる2つの90°2点演算値
に直線補間を行って交流入力信号の振巾を推定し、さら
に必要に応じてこの推定値に周波数補正を施して交流入
力信号の振巾を推定するようにしたので、90°2点演
算は二回行えば良く、しかも安定した演算結果が得られ
る。更に周波数値により補正を行うことにより、より高
精度な演算結果が得られる。
According to the present invention, the amplitude of the AC input signal is estimated by linearly interpolating two 90 ° two-point calculated values obtained from the sampling values immediately before and after the zero crossing point, and further if necessary. Accordingly, since the estimated value is frequency-corrected to estimate the amplitude of the AC input signal, the 90 ° two-point calculation may be performed twice, and a stable calculation result can be obtained. Furthermore, by performing correction with the frequency value, a more accurate calculation result can be obtained.

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

【図1】請求項1の発明に関わる演算方法の説明図FIG. 1 is an explanatory diagram of a calculation method according to the invention of claim 1.

【図2】請求項1の発明に関わる演算に基づく周波数変
動誤差の特性例を示す図
FIG. 2 is a diagram showing a characteristic example of a frequency fluctuation error based on a calculation according to the invention of claim 1;

【図3】請求項2の発明に関わる周波数補正方法の説明
FIG. 3 is an explanatory diagram of a frequency correction method according to the invention of claim 2;

【図4】入力周波数の減少時における本発明の演算結果
の具体例を示す図
FIG. 4 is a diagram showing a specific example of a calculation result of the present invention when the input frequency is reduced.

【図5】入力周波数の増加時における本発明の演算結果
の具体例を示す図
FIG. 5 is a diagram showing a specific example of a calculation result of the present invention when the input frequency is increased.

【図6】90°2点演算方法における周波数変動誤差の
特性例を示す図
FIG. 6 is a diagram showing a characteristic example of a frequency fluctuation error in a 90 ° two-point calculation method.

【図7】従来の30°6点平均の演算方法による周波数
変動誤差の特性例を示す図
FIG. 7 is a diagram showing a characteristic example of a frequency fluctuation error by a conventional 30 ° 6-point average calculation method.

【符号の説明】[Explanation of symbols]

ZP 0クロス点部 a1 0クロス点の直前のサンプリング値 a2 0クロス点の直後のサンプリング値 b1 サンプリング値a1に対し基準周波数の90°
位相差に相当する時間間隔を持つサンプリング値 b2 サンプリング値a2に対し基準周波数の90°
位相差に相当する時間間隔を持つサンプリング値 m1 サンプリング値a1,b1から得られる90°
2点演算値 m2 サンプリング値a2,b2から得られる90°
2点演算値 Em’ 90°2点演算値m1,m2から直線補間によ
って得られる0クロス点の90°2点演算値に相当する
値(=交流入力振巾推定値) Em” Em’に周波数補正を施して推定した交流入力
振巾推定値 Em 交流入力振巾の真値
ZP 0 Cross point part a1 0 Sampling value immediately before cross point a2 0 Sampling value immediately after cross point b1 90 ° of reference frequency with respect to sampling value a1
Sampling value b2 having a time interval corresponding to the phase difference 90 ° of the reference frequency with respect to the sampling value a2
Sampling value m1 having a time interval corresponding to the phase difference 90 ° obtained from sampling values a1 and b1
2-point calculation value m2 90 ° obtained from sampling values a2 and b2
2-point calculation value Em '90 ° 2-point calculation value obtained by linear interpolation from 0 cross point 90 ° 2-point calculation value (= AC input amplitude estimated value) Em "Em' frequency Estimated value of AC input amplitude estimated with correction Em True value of AC input amplitude

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】基準周波数の前後に周波数が変動し得る交
流入力信号をこの基準周波数の周期の1/4n(但しn
は2以上の所定の整数とする)の固定サンプリング周期
でサンプリングしてA/D変換し、このデジタル変換さ
れたサンプリング値から前記交流入力信号の振巾を推定
する方法であって、 前記交流入力信号の0クロス点の直前のサンプリング値
を用いた90°2点演算値と、該0クロス点の直後のサ
ンプリング値を用いた90°2点演算値との直線補間に
より、この0クロス点の90°2点演算値に相当する値
を求め、該値を前記交流入力信号の振巾の推定値とする
ことを特徴とする交流入力振巾のデジタル推定演算方
法。
1. An AC input signal whose frequency can fluctuate before and after a reference frequency is set to 1 / 4n (where n
Is a predetermined integer greater than or equal to 2), performs A / D conversion by sampling at a fixed sampling period, and estimates the amplitude of the AC input signal from the digitally converted sampling value. By linearly interpolating the 90 ° 2-point calculation value using the sampling value immediately before the 0-cross point of the signal and the 90 ° 2-point calculation value using the sampling value immediately after the 0-cross point, this 0-cross point A digital estimation calculation method for an AC input amplitude, wherein a value corresponding to a 90 ° two-point calculated value is obtained and the value is used as an estimated value of the amplitude of the AC input signal.
【請求項2】請求項1に記載の推定演算方法において、
さらに前記交流入力信号の周波数を求め、この周波数と
前記固定サンプリング周期とを用いて前記交流入力信号
の振巾の推定値に所定の補正を施した値を改めて前記交
流入力信号の振巾の推定値とすることを特徴とする交流
入力振巾のデジタル推定演算方法。
2. The estimation calculation method according to claim 1,
Further, the frequency of the AC input signal is obtained, and a value obtained by applying a predetermined correction to the estimated value of the amplitude of the AC input signal using this frequency and the fixed sampling period is used to estimate the amplitude of the AC input signal again. A method for digitally estimating an AC input amplitude, which is characterized by setting a value.
JP04221848A 1992-08-21 1992-08-21 Digital input amplitude calculation method for AC input amplitude Expired - Fee Related JP3099542B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP04221848A JP3099542B2 (en) 1992-08-21 1992-08-21 Digital input amplitude calculation method for AC input amplitude

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP04221848A JP3099542B2 (en) 1992-08-21 1992-08-21 Digital input amplitude calculation method for AC input amplitude

Publications (2)

Publication Number Publication Date
JPH0666844A true JPH0666844A (en) 1994-03-11
JP3099542B2 JP3099542B2 (en) 2000-10-16

Family

ID=16773137

Family Applications (1)

Application Number Title Priority Date Filing Date
JP04221848A Expired - Fee Related JP3099542B2 (en) 1992-08-21 1992-08-21 Digital input amplitude calculation method for AC input amplitude

Country Status (1)

Country Link
JP (1) JP3099542B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007263758A (en) * 2006-03-28 2007-10-11 Hioki Ee Corp Measuring device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007263758A (en) * 2006-03-28 2007-10-11 Hioki Ee Corp Measuring device

Also Published As

Publication number Publication date
JP3099542B2 (en) 2000-10-16

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