JPS6059974A - Converter - Google Patents

Converter

Info

Publication number
JPS6059974A
JPS6059974A JP58166068A JP16606883A JPS6059974A JP S6059974 A JPS6059974 A JP S6059974A JP 58166068 A JP58166068 A JP 58166068A JP 16606883 A JP16606883 A JP 16606883A JP S6059974 A JPS6059974 A JP S6059974A
Authority
JP
Japan
Prior art keywords
winding
output
series
output voltage
voltage
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
JP58166068A
Other languages
Japanese (ja)
Other versions
JPH0465636B2 (en
Inventor
Mitsuo Kurihara
栗原 美津雄
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.)
Tokai University
Original Assignee
Tokai University
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 Tokai University filed Critical Tokai University
Priority to JP58166068A priority Critical patent/JPS6059974A/en
Publication of JPS6059974A publication Critical patent/JPS6059974A/en
Publication of JPH0465636B2 publication Critical patent/JPH0465636B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02MAPPARATUS FOR CONVERSION BETWEEN AC AND AC, BETWEEN AC AND DC, OR BETWEEN DC AND DC, AND FOR USE WITH MAINS OR SIMILAR POWER SUPPLY SYSTEMS; CONVERSION OF DC OR AC INPUT POWER INTO SURGE OUTPUT POWER; CONTROL OR REGULATION THEREOF
    • H02M5/00Conversion of ac power input into ac power output, e.g. for change of voltage, for change of frequency, for change of number of phases
    • H02M5/02Conversion of ac power input into ac power output, e.g. for change of voltage, for change of frequency, for change of number of phases without intermediate conversion into dc
    • H02M5/04Conversion of ac power input into ac power output, e.g. for change of voltage, for change of frequency, for change of number of phases without intermediate conversion into dc by static converters
    • H02M5/10Conversion of ac power input into ac power output, e.g. for change of voltage, for change of frequency, for change of number of phases without intermediate conversion into dc by static converters using transformers
    • H02M5/16Conversion of ac power input into ac power output, e.g. for change of voltage, for change of frequency, for change of number of phases without intermediate conversion into dc by static converters using transformers for conversion of frequency

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  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Ac-Ac Conversion (AREA)

Abstract

PURPOSE:To enable to vary the secondary side voltage while the phase difference is held when the primary side voltage is constant by winding a positively connected input side winding, reversely connected output side sinding, and a control winding on two annular cores. CONSTITUTION:U-shaped cores A1, A2 and B1, B2 are opposed t form annular cores A, B, the primary windings n1, n1' are positively connected in series, connected to an input power source Ei, the secondary windings n2, n2' are reversely connected in series to obtain an output voltage V2 through a capacitor C1, control windings n3, n3' are reversely connected in series, connected through a variable resistor R to a control power source Ed to form a converter. Accordingly, the magnetic resistance of the output winding Nb is modulated by an input side magnetic flux phia to generate parametric oscillation by a capacitor C1 to establish an output voltage V having a phase difference of 90 deg., and a magnetic flux phib is controlled by the resistor R to vary the output voltage V2.

Description

【発明の詳細な説明】 し産業上の利用分野〕 立を磁心、直交磁心あるいは平面回路における2鉄心形
で構成された変換器は、パラメ) IJソック振によっ
て位相差を有し、定電圧回路、逓信器、分周器として数
多く利用されていることは周知の事実である。
[Detailed Description of the Invention] Industrial Field of Use] A converter configured with a vertical magnetic core, an orthogonal magnetic core, or a two-core type in a planar circuit has a phase difference due to IJ sock vibration, and is used in a constant voltage circuit. It is a well-known fact that they are widely used as transmitters, transmitters, and frequency dividers.

本発明は、2鉄心形でパラメトリック回路と鉄共振回路
を同時に併せ持った変換器に係り、特に制御巻線を有し
、1次側の単相入力電圧を一定としたとき、制御巻線に
流す直流電流を変えることによって、位相差を保持した
まま2次側の単相出力電圧を自由に可変できる変換器に
関する。
The present invention relates to a two-iron core type converter having both a parametric circuit and a fero-resonant circuit at the same time, and in particular, it has a control winding, and when the single-phase input voltage on the primary side is constant, the voltage flowing through the control winding is The present invention relates to a converter that can freely vary the single-phase output voltage on the secondary side while maintaining the phase difference by changing the direct current.

〔従来技術〕[Prior art]

本発明者らは磁気立体回路を用いた相数変換器として、
単相−二相、および単相−三相用で、能動体素子を用い
ずに出力電圧を自由に可変できる変換器を特願昭58−
030399号、特願昭58−094445号として既
に提案した。
The present inventors have developed a phase number converter using a magnetic three-dimensional circuit.
A patent application filed in 1983 for a converter for single-phase to two-phase and single-phase to three-phase use, which can freely vary the output voltage without using active elements.
030399 and Japanese Patent Application No. 58-094445.

〔発明の目的〕[Purpose of the invention]

本発明は単相交流を単相交流に周波数も変えて変換する
ことができ、かつ1次側の単相入力電圧を一定としたと
き、2次側の単相出力電圧を位相差を保持した!ま自由
に可変できる変換器を提供することを目的としたもので
ある。
The present invention can convert single-phase AC to single-phase AC by changing the frequency, and when the single-phase input voltage on the primary side is constant, the single-phase output voltage on the secondary side can maintain the phase difference. ! The purpose of this invention is to provide a converter that can be freely varied.

〔発明の構成〕[Structure of the invention]

上記の目的を達成する本発明は第1.第2図示のように
2つの環状磁心A、Hにそれぞれ施こした同一巻数n1
= n、’の2つの巻線を直列に正接続して単相入力電
圧Vinが印加される入力側巻線Nとし、同じく2つの
環状磁心A、Bにそれぞれ施こした同一巻数n、””n
2’の2つの巻線を直列に逆接続して出力側巻線Nとし
、この出力側巻線NbにはコンデンサC1を並列に接続
して該コンデンサC1の両端を出力端子とすると共に、
更に2つの環状磁心A、Bに同一巻数n3”’ n3’
の2つの巻線を直列に逆接続して直流制御電流idが流
される制御巻線Nとして構成する。
The present invention which achieves the above objects is the first. As shown in the second diagram, the same number of turns n1 are applied to the two annular magnetic cores A and H, respectively.
= n, ' are connected positively in series to form the input side winding N to which the single-phase input voltage Vin is applied, and the same number of turns n, applied to the two annular magnetic cores A and B, respectively. ”n
The two windings 2' are reversely connected in series to form an output winding N, and a capacitor C1 is connected in parallel to this output winding Nb, with both ends of the capacitor C1 serving as output terminals.
Furthermore, the same number of turns n3'''n3' on the two annular magnetic cores A and B
The two windings are connected in reverse in series to form a control winding N through which a DC control current id flows.

〔実施例の構成〕[Configuration of Example]

以下図面によって本発明の一実施例の構成を詳細に駅間
する。
The configuration of one embodiment of the present invention will be explained in detail below with reference to the drawings.

第1図はその構成説明図、第2図はその回路図、第3図
は実施例で使用するU形磁心の形状寸法を示す説明図で
ある。
FIG. 1 is an explanatory diagram of its configuration, FIG. 2 is a circuit diagram thereof, and FIG. 3 is an explanatory diagram showing the shape and dimensions of the U-shaped magnetic core used in the embodiment.

U形磁心ん、A2.B1.B2は長さt−107簡1幅
W=20椙、高さh=58慎、厚さt=8瓢、アーム間
の距離f=92wnの積層鉄心で、フェライトコアでも
よい。
U-shaped magnetic core, A2. B1. B2 is a laminated iron core with length t-107mm, width W=20mm, height h=58mm, thickness t=8mm, and distance between arms f=92wn, and may be a ferrite core.

2つのU形磁心に1+ A2の両端を互いに接合させて
1つの環状磁心Aを形成する。同様にしてもう1つの環
状磁心Bを形成する。環状磁心A、Bけ2つのU形磁心
で形成し々くてもよく、0形磁心を用いることができる
One annular magnetic core A is formed by joining two U-shaped magnetic cores at both ends of 1+ A2 to each other. Another annular magnetic core B is formed in the same manner. The annular magnetic cores A and B may be formed of two U-shaped magnetic cores, and a 0-shaped magnetic core can be used.

この2つの環状磁心A、Bにそれぞれ直径05■の7オ
ルマール線を用いた同一巻数11 =11’ =250
回の2つの巻線を施こし、これらを直列に正接続して入
力側巻線塊とし、これに単相入力電源E1を接続する。
For these two annular magnetic cores A and B, 7 Ormar wires with a diameter of 05 cm are used, and the same number of turns is 11 = 11' = 250
Two windings are made, and these are positively connected in series to form an input-side winding block, and a single-phase input power source E1 is connected to this.

同じく2つの環状磁心A、Bにそれぞれ直径0.5諭の
フォルマール線を用いた同一4数n2 = n2’ =
250回の2つの巻線を施とし、これらを直列に逆接続
して出力側巻線為とし、この出力側巻線凡にはコンデン
サC1を並列に接続して該コンデンサCIの両端を出力
端子とする。
Similarly, the same four numbers n2 = n2' = using Formal wires with a diameter of 0.5 for each of the two annular magnetic cores A and B.
Two windings of 250 turns are connected, and these are connected in reverse in series to form the output side winding.A capacitor C1 is connected in parallel to this output side winding, and both ends of the capacitor CI are connected to the output terminals. shall be.

更に2つの環状磁心A、Bにそれぞれ直径0.5咽のフ
ォルマール線を用いた同一巻数n3 g n3’=27
0回の2つの巻線を施こし、これらを直列に逆接続して
制御巻線Naとし、この制御巻線Naに直列に直流制御
電流脆と可変抵抗Rの直列回路を接続する。
Furthermore, the same number of turns n3 g n3' = 27 using Formal wires with a diameter of 0.5 mm for the two annular magnetic cores A and B, respectively.
Two windings with zero turns are made, and these are reversely connected in series to form a control winding Na, and a series circuit of a DC control current and a variable resistor R is connected in series to this control winding Na.

〔実施例の作用〕[Effect of the embodiment]

次にその作用を説明する。入力側巻線N、に単相入力電
源E、によって単相入力電圧Vlnを印加し交流電流を
流すと、環状磁心A、Bにそれぞれ入力側巻線艮、出力
側巻線Nbによって第1図の矢印方向に磁束φ6.φb
が発生する。この磁束φ1.φbは磁気的に結合し寿い
でそれぞれ独立磁路と表っている。
Next, its effect will be explained. When a single-phase input voltage Vln is applied to the input-side winding N by the single-phase input power supply E and an alternating current is caused to flow, the input-side winding and the output-side winding Nb are applied to the annular magnetic cores A and B, respectively, as shown in FIG. Magnetic flux φ6. φb
occurs. This magnetic flux φ1. φb is magnetically coupled and represents an independent magnetic path.

換言すれば通常の変圧器は1次、2次側共に変圧器作用
、すなわち誘導電圧が生じるわけであるが、これは1次
、2次り11の磁気的な結合でもって生じ、1次側、2
次側の磁束は同相である。従って、その電圧も当然、同
相と女るのであるが、本発明の場合は出力側を逆接続し
であるので、2次側の変圧器誘導作用が打ち消し合うの
で磁気的な結合を考えなくてもよいから1次側と2次側
の磁束φ1.φbは90度の位相差を有しているために
磁路としては、独立と考えられる。
In other words, in a normal transformer, transformer action, that is, induced voltage is generated on both the primary and secondary sides, but this is caused by magnetic coupling between the primary and secondary 11, and the primary side ,2
The magnetic flux on the next side is in phase. Therefore, the voltage is naturally in phase, but in the case of the present invention, the output side is connected in reverse, so the induced effects of the transformer on the secondary side cancel each other out, so there is no need to consider magnetic coupling. Since it is good, the magnetic flux φ1 on the primary side and the secondary side. Since φb has a phase difference of 90 degrees, it is considered that the magnetic paths are independent.

しかし、使用している環状磁心は共有であるため、入力
側磁束φaによって出力側巻線Nbの磁気抵抗が変調す
るために、それに伴なって出力側インダクタンスも変調
し、その結果、出力側巻線凡とコンデンサC!によって
パラメトリック発振が生じ、単相入力電圧Vinに対し
90度の位相差を持った出力電圧■2が確立する。この
90度の位相差を保持した捷ま出力電圧v2の値のみを
加減させるには独立している出力側の磁路、すなわち、
磁束φbを加減すればよく、そのためには、逆接続した
制御巻線Ndに直流制御電流胸により直流制御電流1d
を流し、との直流制御電流1dを可変抵抗Rによって加
減することによって、環状磁心A、Hにそれぞれ発生す
る磁束φdを変化させればよい。乙のようにすると、あ
る半周期では環状磁心Aの磁束は第1図の矢印で示すよ
うにφbとφdの差となって未飽和となり環状磁心Bの
磁束はφbとφdの和となって飽和する、寸だ、次の半
周期ではこれと逆に環状磁心Aが飽和し、環状磁心Bが
未飽和とたす、以下半周期毎にこれを繰り返し寿から、
磁束が制御されることにより、出力電圧v2が制御され
ることになる。
However, since the annular magnetic core used is shared, the magnetic resistance of the output winding Nb is modulated by the input magnetic flux φa, and the output inductance is also modulated accordingly. Line fan and capacitor C! As a result, parametric oscillation occurs, and an output voltage 2 having a phase difference of 90 degrees with respect to the single-phase input voltage Vin is established. To adjust only the value of the twisted output voltage v2 that maintains this 90 degree phase difference, an independent magnetic path on the output side, that is,
It is only necessary to adjust the magnetic flux φb, and for that purpose, a DC control current 1d is applied to the reversely connected control winding Nd by a DC control current source.
The magnetic flux φd generated in each of the annular magnetic cores A and H can be changed by controlling the DC control current 1d with and through the variable resistor R. If we do as shown in B, in a certain half cycle, the magnetic flux of the annular magnetic core A becomes the difference between φb and φd, as shown by the arrow in Figure 1, and becomes unsaturated, and the magnetic flux of the annular magnetic core B becomes the sum of φb and φd. In the next half cycle, on the contrary, the annular magnetic core A is saturated and the annular magnetic core B is unsaturated.This is repeated every half cycle from now on,
By controlling the magnetic flux, the output voltage v2 is controlled.

次に直流制御電流id対出力電圧v2の関係について述
べる。
Next, the relationship between the DC control current id and the output voltage v2 will be described.

第1.第2図の入力側巻線凡の両端に単相入力電圧Vj
 nを印加し、出力側巻線Nbの両端にコンデンサCt
 = 275μFを接続する。次に単相入力電圧Vin
を徐々に増加していくと、鳩。=34V付近でパラメト
リック発振が生じ単相入力電圧Vl nに対して90度
の位相差を有した正弦波の出力電圧v2が確立する。第
4図及び第5図はそれぞれ入力電圧Vinと出力電圧■
の波形図及びベクトル図である。
1st. The single-phase input voltage Vj is applied to both ends of the input winding in Figure 2.
n is applied, and a capacitor Ct is connected across the output winding Nb.
= Connect 275μF. Next, the single-phase input voltage Vin
Gradually increase the dove. Parametric oscillation occurs near =34V, and a sinusoidal output voltage v2 having a phase difference of 90 degrees with respect to the single-phase input voltage Vln is established. Figures 4 and 5 show the input voltage Vin and output voltage, respectively.
FIG. 2 is a waveform diagram and a vector diagram of FIG.

また、第6図は入力−圧Vin対出力電圧■2の関係を
示す特性線図である。この第6図からも判るように本発
明は、定電圧性を有した変換器であり、入力電圧が歪波
形でも出力電圧波形は正弦波(第4図参照)となり、更
に過負槽に対する保護や垂下特性を有している。そのた
めに出力側を短絡しても発振が停止するだけで回路には
全々さしつかえが無い等の優れた特徴を持っている。
Further, FIG. 6 is a characteristic diagram showing the relationship between the input voltage Vin and the output voltage 2. As can be seen from Fig. 6, the present invention is a converter with constant voltage characteristics, and even if the input voltage is a distorted waveform, the output voltage waveform is a sine wave (see Fig. 4), and it is further protected against overload tanks. It has drooping characteristics. Therefore, even if the output side is short-circuited, the oscillation will simply stop and there will be no problem with the circuit.

本発明は、これらの利点を生かした上で、環状磁心A、
Hに制御巻線Naを施こしその両端に直流制御電源ガと
可変抵抗Rの直列回路を接続し可変抵抗Rを徐々に変え
ながら直流制御電流1dを変化することにより、出力電
圧v2を順次変動させるものである。第7図はそのとき
の特性を示したもので、v1□−35V一定時における
直流制御電流1d対出力電圧v2の関係である。第7図
からも明らかなようにldが0.4〜1.75Atで変
化した場合、出力電圧v2は35V〜6vまで変動して
いく様子が理解できヨウ。第8図1d Vln = 3
5V一定、 Id=1.2Aにした場合の入力電圧波形
対出力電圧波形を示したものであるが、位相差が90度
を保持したまま出力電圧が変動していく状態が理解でき
よう。
The present invention takes advantage of these advantages and provides annular magnetic cores A,
A control winding Na is connected to H, a series circuit of a DC control power source and a variable resistor R is connected to both ends of the control winding Na, and the DC control current 1d is varied while gradually changing the variable resistor R, thereby sequentially varying the output voltage V2. It is something that makes you FIG. 7 shows the characteristics at that time, which is the relationship between the DC control current 1d and the output voltage v2 when v1□-35V is constant. As is clear from FIG. 7, it can be seen that when ld changes from 0.4 to 1.75 At, the output voltage v2 changes from 35V to 6V. Figure 8 1d Vln = 3
This shows the input voltage waveform versus output voltage waveform when the voltage is constant at 5V and Id = 1.2A, and it can be understood that the output voltage fluctuates while the phase difference is maintained at 90 degrees.

また、2倍周波数時の出力電圧も制御電流を駆使するこ
とによって変動が可能であることが実験によって確認で
きた。
Furthermore, it was confirmed through experiments that the output voltage at double frequency can also be varied by making full use of the control current.

〔発明の効果〕〔Effect of the invention〕

以上の説明より明らかなように本発明によれば次のよう
な効果を奏する。
As is clear from the above description, the present invention provides the following effects.

■、出力電圧を位相差を保持し九オま、自由に変えるこ
とができる。■、入力側巻線と出力側巻線に二相サーボ
・モータを接続することによりその回転ならびに回転制
御ができる。■、同一磁心を用いて構成できるため、構
造が安価である。■。
■The output voltage can be changed freely by 9 degrees while maintaining the phase difference. ■By connecting a two-phase servo motor to the input and output windings, the rotation and rotation can be controlled. (2) The structure is inexpensive because it can be constructed using the same magnetic core. ■.

能動体素子は一切使用してない。■、過負荷保護や垂下
特性を有しているため、出力側を短絡しても発振が停止
するだけで回路には全く影響が無い。
No active elements are used. (2) Since it has overload protection and drooping characteristics, even if the output side is shorted, oscillation will simply stop and the circuit will not be affected at all.

■、出力電圧波形は良好である。■The output voltage waveform is good.

【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の構成説明図、第2図はその
回路図、第3図は実施例で使用するU形磁心の形状寸法
を示す説明図、第4図及び第5図はそれぞれ入力電圧と
出力電圧の波形図及びベクトル図、第6図は入力電圧対
出力電圧の関係を示す特性線図、第7図は入力電圧を一
定としたときの直流制御電流対出力電圧の特性線図、第
8図は入力電圧及び直流制御電流を一定とした時の入力
電圧と出力電圧の波形図である。 A、B ・・・・・環状磁心、凡・・・・・入力側巻線
、Nb・・・・・出力側巻線、Nd・・・・・制御巻線
、EI・・・・・・単相入力電源、C1・・・・・コン
デンサ、Ed・・・・・・直流制御電源、R・・・・・
可変抵抗。
Fig. 1 is an explanatory diagram of the configuration of an embodiment of the present invention, Fig. 2 is its circuit diagram, Fig. 3 is an explanatory diagram showing the shape and dimensions of the U-shaped magnetic core used in the embodiment, Figs. 4 and 5. are waveform diagrams and vector diagrams of input voltage and output voltage, respectively, Figure 6 is a characteristic line diagram showing the relationship between input voltage and output voltage, and Figure 7 is a diagram of DC control current vs. output voltage when the input voltage is constant. The characteristic diagram, FIG. 8, is a waveform diagram of the input voltage and output voltage when the input voltage and DC control current are constant. A, B......Annular magnetic core, General...Input side winding, Nb...Output side winding, Nd...Control winding, EI...... Single phase input power supply, C1...Capacitor, Ed...DC control power supply, R...
Variable resistance.

Claims (1)

【特許請求の範囲】[Claims] 2つの環状磁心A、Hにそれぞれ施こした同一巻数n1
=nl’の2つの巻線を直列に正接続して単相入力電圧
vi nが印加される入力側巻線Naとし、同じく2つ
の環状磁心A、Bにそれぞれ施とした同一巻数n2=n
2′の26の巻線を直列に逆接続して出力側巻線凡とじ
、この出力側巻線凡にはコンデンサC1を並列に接続し
て該コンデンサCIの両端を出力端子とすると共に、更
□に2つの環状磁心A、Hに同一巻数n3 ”’ n3
の2つの巻線を直列に逆接続して直流制御電流1dが流
される制御巻線Naとして構成した変換器。
The same number of turns n1 applied to the two annular magnetic cores A and H, respectively.
The two windings of =nl' are positively connected in series to form the input side winding Na to which the single-phase input voltage vin is applied, and the same number of turns n2 = n applied to the two annular magnetic cores A and B respectively.
The 26 windings of 2' are connected in reverse in series to form an output side winding, and a capacitor C1 is connected in parallel to this output side winding, with both ends of the capacitor CI serving as output terminals. □ has two annular magnetic cores A, H has the same number of turns n3 ”' n3
A converter configured by connecting two windings in series in reverse order to form a control winding Na through which a DC control current 1d flows.
JP58166068A 1983-09-09 1983-09-09 Converter Granted JPS6059974A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58166068A JPS6059974A (en) 1983-09-09 1983-09-09 Converter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58166068A JPS6059974A (en) 1983-09-09 1983-09-09 Converter

Publications (2)

Publication Number Publication Date
JPS6059974A true JPS6059974A (en) 1985-04-06
JPH0465636B2 JPH0465636B2 (en) 1992-10-20

Family

ID=15824378

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58166068A Granted JPS6059974A (en) 1983-09-09 1983-09-09 Converter

Country Status (1)

Country Link
JP (1) JPS6059974A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011151934A1 (en) * 2010-06-01 2011-12-08 中央産業株式会社 Auto voltage regulator for charge
WO2013039415A1 (en) * 2011-09-02 2013-03-21 ХОРЬЯКОВ, Владимир Владимирович Resonant transducer
JP2015034135A (en) * 2013-08-08 2015-02-19 宇部興産株式会社 Method for producing high purity aromatic compound, and high purity aromatic compound

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011151934A1 (en) * 2010-06-01 2011-12-08 中央産業株式会社 Auto voltage regulator for charge
WO2013039415A1 (en) * 2011-09-02 2013-03-21 ХОРЬЯКОВ, Владимир Владимирович Resonant transducer
JP2015034135A (en) * 2013-08-08 2015-02-19 宇部興産株式会社 Method for producing high purity aromatic compound, and high purity aromatic compound

Also Published As

Publication number Publication date
JPH0465636B2 (en) 1992-10-20

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