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JPH0668516B2 - AC effective value detection method - Google Patents
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JPH0668516B2 - AC effective value detection method - Google Patents

AC effective value detection method

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Publication number
JPH0668516B2
JPH0668516B2 JP13277987A JP13277987A JPH0668516B2 JP H0668516 B2 JPH0668516 B2 JP H0668516B2 JP 13277987 A JP13277987 A JP 13277987A JP 13277987 A JP13277987 A JP 13277987A JP H0668516 B2 JPH0668516 B2 JP H0668516B2
Authority
JP
Japan
Prior art keywords
effective value
sampling data
frequency
alternating current
zero
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
JP13277987A
Other languages
Japanese (ja)
Other versions
JPS63295971A (en
Inventor
隆之 小野
健 竹村
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
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP13277987A priority Critical patent/JPH0668516B2/en
Publication of JPS63295971A publication Critical patent/JPS63295971A/en
Publication of JPH0668516B2 publication Critical patent/JPH0668516B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は交流の実効値検出方法にかかり、詳しくは、出
力の大幅な周波数変化を伴う発電機等をディジタル保護
継電装置により保護する場合において、保護継電装置に
入力される任意周波数の変流電圧・電流の実効値を正確
に検出可能とした交流の実効値検出方法に関する。
The present invention relates to a method for detecting an effective value of alternating current, and more specifically, in the case of protecting a generator or the like with a large frequency change in output by a digital protective relay device. In the above, it relates to a method of detecting an AC effective value capable of accurately detecting an effective value of a current-transforming voltage / current of an arbitrary frequency input to a protective relay device.

(従来の技術) 発電機等の交流電力系統を構成する機器を保護する場
合、系統の電圧・電流の瞬時値をアナログ量で検出した
後、ディジタル量に変換し、これらのディジタル量から
電圧・電流の波高値・実効値を求め、これらの波高値等
が一定値を越えた場合にディジタル保護継電装置を動作
させて機器を保護する方法が採用されている。
(Prior Art) When protecting a device that constitutes an AC power system such as a generator, the instantaneous values of the system voltage and current are detected as analog quantities, then converted to digital quantities, and the voltage and current are converted from these digital quantities. A method is adopted in which the crest value and effective value of the current are obtained, and when the crest value or the like exceeds a certain value, the digital protection relay device is operated to protect the device.

この場合、ディジタル保護継電装置への交流入力の波高
値等を検出する方法として、従来から以下に示す方法が
知られている。
In this case, as a method for detecting the peak value of AC input to the digital protective relay device, the following method has been conventionally known.

すなわち、従来では波高値等を検出するべき定格周波数
(50Hzまたは60Hz)の交流に対して、例えば600Hzまた
は720Hzの周波数にてサンプリングを行い、その結果得
られたサンプリングデータのうち、電気角90゜相当の位
相差を有する任意の2点または任意の連続する8点にお
けるサンプリングデータを2乗してこれらを加算し、こ
の加算値の平方根を算出することにより交流の波高値を
求め、次いで実効値を求めている。
That is, in the past, sampling was performed at a frequency of, for example, 600 Hz or 720 Hz with respect to an alternating current having a rated frequency (50 Hz or 60 Hz) for which a peak value or the like should be detected, and among the resulting sampling data, an electrical angle of 90 ° Squared the sampling data at arbitrary two points or arbitrary continuous eight points having a considerable phase difference, add these, and calculate the square root of this added value to obtain the peak value of the alternating current, and then the effective value. Are seeking.

例えば、正弦波交流の電圧の波高値Vを求める方法は
以下のとおりである。前記電気角90゜相当の位相差を有
する任意の2点におけるサンプリングデータをそれぞれ
υ,υとし、υ=Vsin(ωt+φ)とすると
(φはυの位相角)、υはυsin(ωt+φ
+90゜)で表される。υ,υの2乗の和の平方根を
求めると、 [{Vsin(ωt+φ)} +{Vsin(ωt+φ+90゜}1/2 =V{sin2(ωt+φ)+cos2(ωt+φ)}1/2 =V ………………………………(1) となり、波高値を検出することができる。
For example, the method of obtaining the peak value V m of the sinusoidal AC voltage is as follows. Let υ 1 and υ 2 be sampling data at arbitrary two points having a phase difference corresponding to the electrical angle of 90 °, and let υ 1 = V m sin (ωt + φ) (φ is a phase angle of υ 1 ), υ 2 Is υ 2 = m sin (ωt + φ
+ 90 °). When the square root of the sum of squares of υ 1 and υ 2 is calculated, [{V m sin (ωt + φ)} 2 + {V m sin (ωt + φ + 90 °} 2 ] 1/2 = V m {sin 2 (ωt + φ) + cos 2 (ωt + φ)} 1/2 = V m ………………………… (1), and the peak value can be detected.

このように、電気角90゜相当の位相差を有する2点であ
れば常に(1)式が成立するので、上記の関係にある任意
のサンプリングデータを採用しても波高値Vひいては
実効値V/▲√▼を正確に検出することができ、デ
ィジタル保護継電装置によって機器を適切に保護するこ
とが可能となる。
As described above, since the formula (1) is always satisfied at two points having a phase difference corresponding to an electrical angle of 90 °, the peak value V m and thus the effective value can be obtained even if arbitrary sampling data having the above relationship is adopted. V m / ▲ √ ▼ can be accurately detected, and the device can be appropriately protected by the digital protective relay device.

(発明が解決しようとする問題点) しかしながら、発電機の如く出力周波数の変化を伴う機
器の保護においては、以下のような不都合が生ずる。
(Problems to be Solved by the Invention) However, the following inconvenience arises in the protection of a device such as a generator that involves a change in output frequency.

すなわち、発電機ではその周波数が起動時(約20Hz)か
ら負荷遮断時(約100Hz)まで広範囲に変化するため、
ディジタル保護継電装置としても交流の広い周波数領域
にわたって小さな誤差で実効値を検出することが要求さ
れる。しかるに、前述した従来の方法では、いかなる周
波数の交流に対してもサンプリングデータは定格周波数
における電気角90゜間隔のものを採用するため、定格以
外の周波数では電気角90゜間隔でのサンプリングデータ
を採用したことにはならず、上記(1)式により演算した
波高値ないし実効値と実際の各値との間に誤差を生ずる
ことになる。
In other words, the frequency of the generator varies over a wide range from startup (about 20 Hz) to load shedding (about 100 Hz).
Even as a digital protective relay device, it is required to detect an effective value with a small error over a wide frequency range of alternating current. However, in the above-mentioned conventional method, since the sampling data for the alternating current of any frequency has an electrical angle of 90 ° at the rated frequency, the sampling data at the electrical angle of 90 ° is used for frequencies other than the rated frequency. This is not adopted, and an error occurs between the peak value or effective value calculated by the above equation (1) and each actual value.

ここで、第3図は、誤差={(検出値)−(真値)}×
100/真値[%]としてサンプリング周波数600[Hz]で定格
周波数における電気角90゜間隔相当のサンプリングデー
タを採用した場合の誤差の周波数特性を、交流の周波数
[Hz]を横軸に、誤差[%]を縦軸にとって示した図で
あり、同図(イ)は前述した連続2点によるサンプリン
グデータを採用した場合を、また同図(ロ)は連続8点
によるサンプリングデータを採用した場合をそれぞれ示
している。
Here, in FIG. 3, error = {(detection value) − (true value)} ×
The frequency characteristic of the error when the sampling data corresponding to the electrical angle 90 ° interval at the rated frequency with the sampling frequency 600 [Hz] as 100 / true value [%] is adopted is the AC frequency.
The horizontal axis represents [Hz] and the vertical axis represents error [%]. The figure (a) shows the case where the sampling data by the continuous two points described above is adopted, and the figure (b) shows the continuous case. The case where sampling data by 8 points is adopted is shown.

同図(イ)において、例えば交流の周波数が100[Hz]で
ある場合、2点のサンプリングデータの採り方によって
誤差や約+41.4[%]から−100[%]の範囲で生じることに
なり、従来の検出方法では定格周波数以外の周波数での
演算誤差がこのように大きいため交流の実効値を正確に
検出することができず、ディジタル保護継電装置による
発電機等の保護には不適当なものであった。
In the figure (a), for example, when the frequency of the alternating current is 100 [Hz], the error may occur in the range of about +41.4 [%] to -100 [%] depending on how the sampling data of two points is taken. However, the conventional detection method cannot accurately detect the effective value of AC due to such a large calculation error at frequencies other than the rated frequency, and is not suitable for protection of generators, etc. by the digital protective relay device. It was suitable.

本発明はこのような問題点を解決するべく提案されたも
ので、その目的とするところは、交流の周波数が大幅に
変化してもその実効値を高精度で検出することができる
交流の実効値検出方法を提供することにある。
The present invention has been proposed in order to solve such a problem, and an object of the present invention is to detect the effective value of an alternating current that can detect its effective value with high accuracy even if the frequency of the alternating current changes significantly. It is to provide a value detection method.

(問題点を解決するための手段) 上記目的を達成するため、本発明は、交流の複数の零交
差点間のすべてのサンプリングデータと、零交差点間の
時間から求めた交流の周期等を用いて実効値を検出する
ものであり、交流周波数がどのように変動しようともそ
の周期を実効値演算に加味することによって高精度に実
効値を検出しようとするものである。
(Means for Solving Problems) In order to achieve the above object, the present invention uses all sampling data between a plurality of alternating zero-crossing points, the cycle of the alternating current obtained from the time between the zero-crossing points, and the like. This is to detect the effective value, and to detect the effective value with high accuracy by adding the period to the effective value calculation no matter how the AC frequency changes.

すなわち本発明は、実効値を検出するべき交流の瞬時値
を一定周波数でサンプリングして、そのサンプリングデ
ータの正負の符号変化から交流の2つの零交差点の存在
を確認し、次いで、これらの零交差点間の複数のサンプ
リングデータの2乗の和を算出すると共に、前記零交差
点間のサンプリング回数,サンプリング周期及び前記零
交差点の直前・直後のサンプリングデータから前記零交
差点間の時間を求め、この時間にて前記零交差点間の複
数のサンプリングデータの2乗の和を除算した値に前記
サンプリング周期を乗じたものの平方根を算出して交流
の実効値を求めることを特徴とする (作用) 本発明によれば、サンプリングデータの符号変化から交
流の1周期または1/2周期に相当する2つの零交差点の
存在を確認する。そして、これらの零交差点間のすべて
のサンプリングデータと、交流の周期及びサンプリング
周期を用いて実効値の定義に基づき実効値を演算する。
That is, according to the present invention, the instantaneous value of the alternating current for which the effective value is to be detected is sampled at a constant frequency, the presence of two zero-crossing points of the alternating current is confirmed from the positive and negative sign changes of the sampling data, and then these zero-crossing points are detected. The sum of squares of a plurality of sampling data between the zero crossing points is calculated, and the time between the zero crossing points is obtained from the sampling frequency between the zero crossing points, the sampling period, and the sampling data immediately before and after the zero crossing point. Then, a square root of a value obtained by dividing the sum of squares of a plurality of sampling data between the zero crossing points by the sampling period is calculated to obtain the effective value of the alternating current. (Operation) According to the present invention For example, from the sign change of the sampling data, the existence of two zero crossing points corresponding to one cycle or half cycle of the alternating current is confirmed. Then, the effective value is calculated based on the definition of the effective value using all the sampling data between these zero crossing points, the alternating current cycle and the sampling cycle.

(実施例) 以下、図面に沿って本発明の実施例を説明する。まず、
第1図は本発明の一実施例を説明するためのもので、周
波数inの正弦波交流のほぼ1周期の波形及びこの波
形をサンプリング周波数でサンプリングしたときの
サンプリングデータを、時間(t)を横軸、交流の電圧ま
たは電流の振幅Xを縦軸として表したものである。
(Examples) Examples of the present invention will be described below with reference to the drawings. First,
FIG. 1 is for explaining one embodiment of the present invention, in which a waveform of a sinusoidal wave AC having a frequency in of approximately one cycle and sampling data when this waveform is sampled at a sampling frequency s are shown as time (t). Is represented by the horizontal axis, and the amplitude X of the AC voltage or current is represented by the vertical axis.

図中、A,B,Cは以下のサンプリングデータの符号の
反転により検出される、交流波形の振幅が零となる点
(零交差点)を、Xa1,Xa2、Xb1,Xb2、X
c1,Xc2は各零交差点A,B,Cにそれぞれ隣り合
うサンプリングデータを、ta1,ta2、tb1,t
b2、tc1,tc2は各零交差点A,B,Cからこれ
らの直前、直後のサンプリング点までの時間をそれぞえ
れ示している。また、tはサンプリング周期、T
A−C間の時間で交流の1周期に相当し、またTはA
−B間の時間で交流の1/2周期に相当している。
In the figure, A, B, and C represent points (zero crossing points) at which the amplitude of the AC waveform becomes zero, which are detected by the following inversion of the sign of the sampling data, X a1 , X a2 , X b1 , X b2 , and X.
c1 and X c2 are sampling data adjacent to the zero crossing points A, B and C, respectively, and are represented by t a1 , t a2 , t b1 and t
b2 , t c1 , and t c2 indicate the times from the respective zero-crossing points A, B, C to the sampling points immediately before and after these zero-crossing points, respectively. Further, t s is a sampling cycle, T 1 is a time between A and C, which corresponds to one cycle of alternating current, and T 2 is A.
The time between −B corresponds to 1/2 cycle of alternating current.

ここで、サンプリング周期tとサンプリング周波数
との関係は、 t=1/ ……………………………(2) となる。また、T及びTは、 T=1/in …………………………(3) T=T/2 ……………………………(4) によって表される。
Here, the sampling period t s and the sampling frequency
the relationship between the s is a t s = 1 / s ................................. ( 2). Further, T 1 and T 2, the T 1 = 1 / in .............................. ( 3) T 2 = T 1/2 ................................. (4) expressed.

次に、交流の1周期Tにおけるサンプリング回数をN
,1/2周期Tにおけるサンプリング回数をNとす
ると、T,Tはそれぞれ以下のように表される。
Next, the number of samplings in one cycle T 1 of alternating current is set to N
1, the 1/2 the number of sampling times in the period T 2 and N 2, T 1, T 2 are respectively represented as follows.

=(N−1)×t+ta1+tc2………………(5) T=(N−1)×t+ta1+tb2………………(6) また、零交差点A,B,C近傍の波形を直線近似する
と、ta1,tb2,tc2はそれぞれ以下のように表
される。
T 1 = (N 1 -1) × t s + t a1 + t c2 .................. (5) T 2 = (N 2 -1) × t s + t a1 + t b2 .................. (6) Further, when the waveforms near the zero crossing points A, B, and C are linearly approximated, ta1 , tb2 , and tc2 are respectively expressed as follows.

a1=|Xa1|×t/(|Xa1|+|Xa2|)………(7) tb2=|Xb2|×t/(|Xb1|+|Xb2|)………(8) tc2=|Xc2|×t/(|Xc1|+|Xc2|)………(9) この場合、inに比べて大きくなるほど、直線
近似の度合いが強くなる。
t a1 = | X a1 | × t s / (| X a1 | + | X a2 |) ... (7) t b2 = | X b2 | × t s / (| X b1 | + | X b2 |) ……… (8) t c2 = | X c2 | × t s / (| X c1 | + | X c2 |)… (9) In this case, as s becomes larger than in , the degree of linear approximation Becomes stronger.

ここで、交流の実効値の定義を考慮すると、第1図の場
合の実効値Xrmsは、以下のように近似される。
Here, considering the definition of the effective value of the alternating current, the effective value X rms in the case of FIG. 1 is approximated as follows.

まず、交流の1周期Tについて(以下「方式1」とい
う)は、 また、交流の1/2周期Tについて(以下「方式2」と
いう)は、 となる。なお、Xは零交差点間のサンプリングデータ
であり、方式1の場合においては周期Tにおけるi番
目の、あるいは方式2の場合においては1/2周期T
おけるi番目のサンプリングデータを示している。
First, regarding one cycle T 1 of alternating current (hereinafter referred to as “method 1”), Also, for the 1/2 cycle T 2 of AC (hereinafter referred to as “method 2”), Becomes Note that X i is the sampling data between the zero crossing points, and indicates the i-th sampling data in the period T 1 in the case of method 1, or the i-th sampling data in the 1/2 cycle T 2 in the case of method 2. There is.

ここで、Ns1,Ns2は Ns1in=T×=T/t…………(12) Ns2/(in×2)=(T/2)× =T×=T/t……………………(13) となる。この近似では、inより充分大きくと
れば、実際の交流の実効値とみなすことができる。
Here, N s1, N s2 is N s1 = s / in = T 1 × s = T 1 / t s ............ (12) N s2 = s / (in × 2) = (T 1/2) X s = T 2 x s = T 2 / t s (13) In this approximation, if s is made sufficiently larger than in , it can be regarded as the actual effective value of the alternating current.

次に、(5),(7),(9)式から (6),(7),(8)式から (12),(14)式から (13,(15))式から となる。Next, from equations (5), (7), and (9) From Eqs. (6), (7), and (8) From equations (12) and (14) From equation (13, (15)) Becomes

これにより、交流の実効値Xrmsは、方式1については
(10),(16)式により、方式2については(11),(17)式によ
り求めることができる。
As a result, the effective value X rms of AC is
From Formulas (10) and (16), Formula 2 can be obtained from Formulas (11) and (17).

第2図(イ)は方式1により検出した実効値の誤差の周
波数特性を、同図(ロ)は同じく方式2による誤差の周
波数特性をそれぞれ示したものでありサンプリング周波
=600[Hz]の場合であり、方式2は方式1に比べ
て誤差が若干大きい反面、1/2周期毎に演算が可能であ
るから、応答性が良くなる。また、これらの特性から、
本発明では広い周波数範囲にわたって交流の実効値を精
度良く検出できることが明らかである。
FIG. 2 (a) shows the frequency characteristic of the error of the effective value detected by the method 1, and FIG. 2 (b) shows the frequency characteristic of the error by the method 2, respectively. Sampling frequency s = 600 [Hz] In the case of Method 2, the error is slightly larger than that of Method 1, but the responsiveness is improved because the calculation can be performed every 1/2 cycle. Also, from these characteristics,
It is apparent that the present invention can accurately detect the effective value of AC over a wide frequency range.

なお、本発明は上記実施例の如くディジタル保護継電装
置の交流入力ばかりでなく、その他一般の交流実効値の
検出にも適用できることは言うまでもない。
Needless to say, the present invention can be applied not only to the AC input of the digital protective relay device as in the above embodiment, but also to the detection of other general AC effective values.

(発明の効果) 以上のように本発明によれば、交流の零交差点間の複数
のサンプリングデータと交流の周期等を用い、定義に基
づいて実効値を直接検出するようにしたため、交流周波
数が広範囲にわたって変化するような場合でもその実効
値を少ない誤差で高精度に検出することができる。
(Effect of the invention) As described above, according to the present invention, the effective value is directly detected based on the definition by using a plurality of sampling data between AC zero-crossing points and the AC cycle. Even in the case of changing over a wide range, the effective value can be detected with high accuracy and with a small error.

従って、本発明は、交流周波数が大幅に変動する発電機
等の機器をディジタル保護継電装置により保護する場合
に極めて有用であり、高精度の保護を期待することがで
きる。
Therefore, the present invention is extremely useful when a device such as a generator whose AC frequency fluctuates greatly is protected by a digital protective relay device, and high-precision protection can be expected.

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

第1図及び第2図は本発明の一実施例を示すもので、第
1図は本発明が適用される交流波形及びサンプリングデ
ータを示す図、第2図(イ),(ロ)はそれぞれ本発明
により検出された実効値誤差の周波数特性を示す図、第
3図(イ),(ロ)はそれぞれ従来例による実効値誤差
の周波数特性を示す図である。 A,B,C……零交差点 Xa1,Xa2,Xb1,Xb2,Xc1,Xc2……
サンプリングデータ T……零交差点A−C間の時間 T……零交差点A−B間の時間 t……サンプリング周期
1 and 2 show an embodiment of the present invention. FIG. 1 is a diagram showing an AC waveform and sampling data to which the present invention is applied, and FIGS. 2 (A) and 2 (B) respectively. FIGS. 3A and 3B are diagrams showing the frequency characteristic of the effective value error detected by the present invention, and FIGS. 3A and 3B are diagrams showing the frequency characteristic of the effective value error according to the conventional example. A, B, C ... Zero crossing points Xa1 , Xa2 , Xb1 , Xb2 , Xc1 , Xc2 ...
Time t s ...... sampling period between time T 2 ...... zero crossing point A-B between the sampled data T 1 ...... zero crossing point A-C

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】交流の瞬時値を一定周波数でサンプリング
し、そのサンプリングデータの正負の符号変化から前記
交流の2つの零交差点の存在を確認し、次いで、前記零
交差点間の複数のサンプリングデータの2乗の和を算出
すると共に、前記零交差点間のサンプリング回数,サン
プリング周期及び前記各零交差点の直前・直後のサンプ
リングデータから前記零交差点間の時間を求め、この時
間にて前記零交差点間の複数のサンプリングデータの2
乗の和を除算した値に前記サンプリング周期を乗じたも
のの平方根を算出して前記交流の実効値を求めることを
特徴とする交流の実効値検出方法。
1. An instantaneous value of alternating current is sampled at a constant frequency, the existence of two zero-crossing points of the alternating current is confirmed from positive and negative sign changes of the sampling data, and then a plurality of sampling data between the zero-crossing points are sampled. The sum of squares is calculated, and the time between the zero crossings is calculated from the number of samplings between the zero crossings, the sampling period, and the sampling data immediately before and after each zero crossing. 2 of multiple sampling data
A method of detecting an AC effective value, characterized in that a square root of a value obtained by dividing a sum of powers by the sampling period is calculated to obtain the AC effective value.
JP13277987A 1987-05-28 1987-05-28 AC effective value detection method Expired - Fee Related JPH0668516B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13277987A JPH0668516B2 (en) 1987-05-28 1987-05-28 AC effective value detection method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13277987A JPH0668516B2 (en) 1987-05-28 1987-05-28 AC effective value detection method

Publications (2)

Publication Number Publication Date
JPS63295971A JPS63295971A (en) 1988-12-02
JPH0668516B2 true JPH0668516B2 (en) 1994-08-31

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Application Number Title Priority Date Filing Date
JP13277987A Expired - Fee Related JPH0668516B2 (en) 1987-05-28 1987-05-28 AC effective value detection method

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Country Link
JP (1) JPH0668516B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011053054A (en) * 2009-09-01 2011-03-17 Hioki Ee Corp Apparatus and method for measuring electric characteristics
CN112782460A (en) * 2019-11-04 2021-05-11 江苏莱提电气股份有限公司 Method for calculating effective value of alternating voltage
CN116840544A (en) * 2023-06-12 2023-10-03 北京科荣达航空科技股份有限公司 Method and device for acquiring effective value of alternating current signal

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Publication number Publication date
JPS63295971A (en) 1988-12-02

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